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<identifier>HZDR:PUBLDB:588-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Pavlenko, O. P.]]></dc:creator>
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<dc:title><![CDATA[Thermal dilepton and open charm signals versus hard initial yields in heavy-ion collisions at RHIC and LHC energies]]></dc:title>
<dc:source><![CDATA[Physics Letters B 391 (1997) pp. 185-190]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Abstract
The hard initial production of open charm and dileptons is compared with possible thermal signals in heavy-ion collisions at RHIC and LHC energies. Our approach is based on the perturbative QCD mini-jet mechanism of quark-gluon matter formation. The thermal dilepton signal is found to rise much stronger as compared to the hard Drell - Yan background with increasing collider energy and clearly dominates at LHC energy. Oppositely, open charm stems from initial hard production. A possible rnanifestation of gluon shadowing at RHIC and LHC energies is discussed.]]></dc:description>
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<identifier>HZDR:PUBLDB:588-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Pavlenko, O. P.]]></dc:creator>
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<dc:title><![CDATA[Thermal dilepton and open charm signals versus hard initial yields in heavy-ion collisions at RHIC and LHC energies]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-144 Preprint]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Abstract
The hard initial production of open charm and dileptons is compared with possible thermal signals in heavy-ion collisions at RHIC and LHC energies. Our approach is based on the perturbative QCD mini-jet mechanism of quark-gluon matter formation. The thermal dilepton signal is found to rise much stronger as compared to the hard Drell - Yan background with increasing collider energy and clearly dominates at LHC energy. Oppositely, open charm stems from initial hard production. A possible rnanifestation of gluon shadowing at RHIC and LHC energies is discussed.]]></dc:description>
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<identifier>HZDR:PUBLDB:589-1</identifier>
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<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Vorst, K.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-589-1</dc:identifier>
<dc:title><![CDATA[Anwendung neuronaler Netze zur Identifizierung gefährlicher Betriebszustände in Chemieanlagen]]></dc:title>
<dc:source><![CDATA[Preprint - GVC / VDI Fachtagung in Köthen, 7. - 8. November 1996, S. 141-147]]></dc:source>
<dc:date>1996</dc:date>
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<identifier>HZDR:PUBLDB:593-1</identifier>
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<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Steffen, H. J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-593-1</dc:identifier>
<dc:title><![CDATA[Plasma source ion implantation of oxygen and nitrogen in aluminum]]></dc:title>
<dc:source><![CDATA[Journal of Vacuum Science and Technology Part B 12 (1994) 2]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:596-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Dittes, F.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-596-1</dc:identifier>
<dc:title><![CDATA[Optimization on Rugged Landscapes: A New General Purpose Monte Carlo Approach]]></dc:title>
<dc:source><![CDATA[Physical Review Letters 76 (1996) 25 pp. 4651-55]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:603-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Müller, W. F. J.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:creator><![CDATA[Bassini, R.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:creator><![CDATA[Blaich, T.]]></dc:creator>
<dc:creator><![CDATA[Immé, G.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:creator><![CDATA[Kunze, W. D.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:creator><![CDATA[Möhlenkamp, T.]]></dc:creator>
<dc:creator><![CDATA[Seidel, W.]]></dc:creator>
<dc:creator><![CDATA[Trzcinski, A.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-603-1</dc:identifier>
<dc:title><![CDATA[Determination of critical exponents in nuclear systems]]></dc:title>
<dc:source><![CDATA[GSI-Preprint-96-29]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/preprint</dc:type>
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<identifier>HZDR:PUBLDB:606-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Plass, M.]]></dc:creator>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Kolitsch, A.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-606-1</dc:identifier>
<dc:title><![CDATA[Layered structure diagnostic and optical modelling of c-BN]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 127/128 (1997) 857]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:607-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Wüst, F.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-607-1</dc:identifier>
<dc:title><![CDATA[Synthesis of "3+1"-mixed-ligand oxorhenium(V) complexes containing modified 3,17ß-Estradiol]]></dc:title>
<dc:source><![CDATA[Bioorganic and Medicinal Chemistry Letters 6 (1996) 22 pp.2729-2734]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:608-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Chudoba, T.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-608-1</dc:identifier>
<dc:title><![CDATA[Modifizierung mechanischer und korrosiver Oberflächeneigenschaften von Magnesium durch Ionenimplantation]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-143 (Dissertation an der Fakultät Mathematik und Naturwissenschaften der TU Dresden)]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
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<header>
<identifier>HZDR:PUBLDB:28455-1</identifier>
<datestamp>2025-06-05</datestamp>
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</header>
<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Wu, X.]]></dc:creator>
<dc:creator><![CDATA[Hong, D.]]></dc:creator>
<dc:creator><![CDATA[Ghamisi, P.]]></dc:creator>
<dc:creator><![CDATA[Li, W.]]></dc:creator>
<dc:creator><![CDATA[Tao, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-28455-1</dc:identifier>
<dc:title><![CDATA[MsRi-CCF: Multi-Scale and Rotation-Insensitive Convolutional Channel Features for Geospatial Object Detection]]></dc:title>
<dc:source><![CDATA[Remote Sensing 10(2018)12, 1990]]></dc:source>
<dc:date>2018</dc:date>
<dc:description><![CDATA[Geospatial object detection is a fundamental but challenging problem in the remote sensing community. Although deep learning has shown its power in extracting discriminative features, there is still room for improvement in its detection performance, particularly for objects with large ranges of variations in scale and direction. To this end, a novel approach, entitled multi-scale and rotation-insensitive convolutional channel features (MsRi-CCF), is proposed for geospatial object detection by integrating robust low-level feature generation, classifier generation with outlier removal, and detection with a power law. The low-level feature generation step consists of rotation-insensitive and multi-scale convolutional channel features, which were obtained by learning a regularized convolutional neural network (CNN) and integrating multi-scaled convolutional feature maps, followed by the fine-tuning of high-level connections in the CNN, respectively. Then, these generated features were fed into AdaBoost (chosen due to its lower computation and storage costs) with outlier removal to construct an object detection framework that facilitates robust classifier training. In the test phase, we adopted a log-space sampling approach instead of fine-scale sampling by using the fast feature pyramid strategy based on a computable power law. Extensive experimental results demonstrate that compared with several state-of-the-art baselines, the proposed MsRi-CCF approach yields better detection results, with 90.19% precision with the satellite dataset and 81.44% average precision with the NWPU VHR-10 datasets. Importantly, MsRi-CCF incurs no additional computational cost, which is only 0.92 s and 0.7 s per test image on the two datasets. Furthermore, we determined that most previous methods fail to gain an acceptable detection performance, particularly when they face several obstacles, such as deformations in objects (e.g., rotation, illumination, and scaling). Yet, these factors are effectively addressed by MsRi-CCF, yielding a robust geospatial object detection method.]]></dc:description>
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<identifier>HZDR:PUBLDB:611-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Mahamid, A.]]></dc:creator>
<dc:creator><![CDATA[Bryan, J. C.]]></dc:creator>
<dc:creator><![CDATA[Bucher, J. J.]]></dc:creator>
<dc:creator><![CDATA[Burrell, A. K.]]></dc:creator>
<dc:creator><![CDATA[Edelstein, N. M.]]></dc:creator>
<dc:creator><![CDATA[Hudson, E. A.]]></dc:creator>
<dc:creator><![CDATA[Kaltsoyannis, N.]]></dc:creator>
<dc:creator><![CDATA[Lukens, W. W.]]></dc:creator>
<dc:creator><![CDATA[Shuh, D. K.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-611-1</dc:identifier>
<dc:title><![CDATA[Electronic and Structural Investigations of Technetium Compounds by X-ray Absorption Spectroscopy]]></dc:title>
<dc:source><![CDATA[Inorganic Chemistry 34 (1995) pp. 193]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:description><![CDATA[Channeling profile analysis is simulated using the dynamic binary collision code Crystal-TRIM. A good agreement between theoretical and experimental data is found for silicon targets which were predamaged by Si+ ions of different energies and analyzed by 140 keV B+ ions. For each example the depth profile of the defects relevant for the dechanneling of the analyzing ions is given. An estimation on the annealing of such defects is obtained by comparison of results for as-implanted and annealed samples.]]></dc:description>
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<dc:title><![CDATA[Computer Simulation of Channeling Profile Analysis of Implantation Damage]]></dc:title>
<dc:source><![CDATA[MRS Symposium Proceedings, Mat. Res. Soc. Symp. Proc. Vol. 532, pp. 133-140, 1998 Materials Research Society]]></dc:source>
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<dc:description><![CDATA[Channeling profile analysis is simulated using the dynamic binary collision code Crystal-TRIM. A good agreement between theoretical and experimental data is found for silicon targets which were predamaged by Si+ ions of different energies and analyzed by 140 keV B+ ions. For each example the depth profile of the defects relevant for the dechanneling of the analyzing ions is given. An estimation on the annealing of such defects is obtained by comparison of results for as-implanted and annealed samples.]]></dc:description>
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<dc:title><![CDATA[Experimentelle Untersuchung turbulenter Flüssigmetall- und Flüssigmetall-Gas-Strömungen in einem äußeren Magnetfeld]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-219]]></dc:source>
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<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Gallmeister, K.]]></dc:creator>
<dc:creator><![CDATA[Pavlenko, O. P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1177-1</dc:identifier>
<dc:title><![CDATA[Thermal Dilepton Signal and Dileptons from Correlated Open Charm and Bottom Decays in Ultrarelativistic Heavy-Ion Collisions]]></dc:title>
<dc:source><![CDATA[Advances in Nuclear Dynamics 4, Edited by W. Bauer and H.-G. Ritter, Plenum Press, New York, 1998, p. 163]]></dc:source>
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<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Geipel, G.]]></dc:creator>
<dc:creator><![CDATA[Denecke, M. A.]]></dc:creator>
<dc:creator><![CDATA[Allen, P. G.]]></dc:creator>
<dc:creator><![CDATA[Bucher, J. J.]]></dc:creator>
<dc:creator><![CDATA[Edelstein, N. M.]]></dc:creator>
<dc:creator><![CDATA[Shuh, D. K.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
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<dc:title><![CDATA[Structural Investigation of the System Ca<SUP>2+</SUP>/UO<SUB>2</SUB><SUP>2+</SUP>/CO<SUB>3</SUB><SUP>2-</SUP> by EXAFS]]></dc:title>
<dc:source><![CDATA[1997 SSRL Annual Activity Report]]></dc:source>
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<dc:creator><![CDATA[Engelmann, H.-J.]]></dc:creator>
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<dc:identifier>https://www.hzdr.de/publications/Publ-1182-1</dc:identifier>
<dc:title><![CDATA[Institute of Radiochemistry; Annual Report 1997]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-218]]></dc:source>
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<datestamp>2023-05-03</datestamp>
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<dc:creator><![CDATA[Markwitz, A.]]></dc:creator>
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<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Hofmeister, H.]]></dc:creator>
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<dc:title><![CDATA[Homogeneously Size Distributed Ge Nanoclusters Embedded in SiO<SUB>2</SUB> Layers Produced by Ion Beam Synthesis]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 147 (1999) 361-366]]></dc:source>
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<dc:title><![CDATA[Homogeneously Size Distributed Ge Nanoclusters Embedded in SiO<SUB>2</SUB> Layers Produced by Ion Beam Synthesis]]></dc:title>
<dc:source><![CDATA[E-MRS ´98, Strasbourg, June 16 - 19, 1998]]></dc:source>
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<identifier>HZDR:PUBLDB:1187-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Misiuk, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1187-1</dc:identifier>
<dc:title><![CDATA[Enhancement of the Intensity of the Short-Wavelength Visible Photoluminescence from Silicon-Implanted Silicon-Dioxide Films Caused by Hydrostatic Pressure During Annealing]]></dc:title>
<dc:source><![CDATA[Applied Physics Letters, Vol. 73, H. 10, 7. Sept. 1998   S. 1418 - 1420]]></dc:source>
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<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1189-1</identifier>
<datestamp>2023-05-03</datestamp>
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<dc:creator><![CDATA[Vahle, A.]]></dc:creator>
<dc:creator><![CDATA[Eichler, B.]]></dc:creator>
<dc:creator><![CDATA[Funke, H.]]></dc:creator>
<dc:creator><![CDATA[Hübener, S.]]></dc:creator>
<dc:creator><![CDATA[Jost, D. T.]]></dc:creator>
<dc:creator><![CDATA[Türler, A.]]></dc:creator>
<dc:creator><![CDATA[Brüchle, W.]]></dc:creator>
<dc:creator><![CDATA[Jäger, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1189-1</dc:identifier>
<dc:title><![CDATA[Gas Chromatographic Studies of Oxide and Hydroxide Species of Tungsten - Model Experiments with Respect to the Physico-Chemical Characterization of Seaborgium (Element 106)]]></dc:title>
<dc:source><![CDATA[Radiochimica Acta 84, 43-51 (1999)]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1008-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Schauer, W.]]></dc:creator>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:creator><![CDATA[Brentano, P.]]></dc:creator>
<dc:creator><![CDATA[Eberth, J.]]></dc:creator>
<dc:creator><![CDATA[Enders, J.]]></dc:creator>
<dc:creator><![CDATA[Egidy, T.]]></dc:creator>
<dc:creator><![CDATA[Grinberg, M.]]></dc:creator>
<dc:creator><![CDATA[Herzberg, R.-D.]]></dc:creator>
<dc:creator><![CDATA[Huxel, N.]]></dc:creator>
<dc:creator><![CDATA[Käubler, L.]]></dc:creator>
<dc:creator><![CDATA[Neumann-Cosel, P.]]></dc:creator>
<dc:creator><![CDATA[Nicolay, N.]]></dc:creator>
<dc:creator><![CDATA[Ott, J.]]></dc:creator>
<dc:creator><![CDATA[Pietralla, N.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Raman, S.]]></dc:creator>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:creator><![CDATA[Richter, A.]]></dc:creator>
<dc:creator><![CDATA[Schlegel, C.]]></dc:creator>
<dc:creator><![CDATA[Schnare, H.]]></dc:creator>
<dc:creator><![CDATA[Servene, T.]]></dc:creator>
<dc:creator><![CDATA[Skoda, S.]]></dc:creator>
<dc:creator><![CDATA[Stoyanov, C.]]></dc:creator>
<dc:creator><![CDATA[Thomas, H. G.]]></dc:creator>
<dc:creator><![CDATA[Wiedenhöver, I.]]></dc:creator>
<dc:creator><![CDATA[Zilges, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1008-1</dc:identifier>
<dc:title><![CDATA[Dipole excitations in <SUP>122</SUP>Te, <SUP>126</SUP>Te and <SUP>130</SUP>Te]]></dc:title>
<dc:source><![CDATA[Zeitschrift für Physik A 358, H.2, 197-198 (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Excited states of the nuclei <SUP>122</SUP>Te, <SUP>126</SUP>Te and <SUP>130</SUP>Te
were populated via the (gamma,gamma') reaction at endpoint energies of
the bremsstrahlung between 4.5 and 5.5 MeV. Gamma rays were detected with
a EUROBALL-CLUSTER detector and a single detector. In all nuclei several
dipole transitions were identified at energies around 3 MeV. The lowest
corresponding J = 1 states are interpreted as two-phonon excitations. Quasiparticle-phonon-model
calculations predict one 1<SUP>-</SUP> state arising from the coupling
of the first quadrupole and the first octupole phonon and one 1<SUP>+</SUP>
state arising from the coupling of the first and the isovector second quadrupole
phonon at about 3 MeV. The calculated transition strengths are compatible
with experimental one.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1008-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:752-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:creator><![CDATA[Brentano, P.]]></dc:creator>
<dc:creator><![CDATA[Eberth, J.]]></dc:creator>
<dc:creator><![CDATA[Enders, J.]]></dc:creator>
<dc:creator><![CDATA[Herzberg, R.-D.]]></dc:creator>
<dc:creator><![CDATA[Huxel, N.]]></dc:creator>
<dc:creator><![CDATA[Käubler, L.]]></dc:creator>
<dc:creator><![CDATA[Neumann-Cosel, P.]]></dc:creator>
<dc:creator><![CDATA[Nicolay, N.]]></dc:creator>
<dc:creator><![CDATA[Pietralla, N.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, A.]]></dc:creator>
<dc:creator><![CDATA[Schlegel, C.]]></dc:creator>
<dc:creator><![CDATA[Schnare, H.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Servene, T.]]></dc:creator>
<dc:creator><![CDATA[Skoda, S.]]></dc:creator>
<dc:creator><![CDATA[Thomas, H. G.]]></dc:creator>
<dc:creator><![CDATA[Wiedenhöver, I.]]></dc:creator>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:creator><![CDATA[Zilges, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-752-1</dc:identifier>
<dc:title><![CDATA[Resonant photon scattering on the semi-magic nucleus <SUP>89</SUP>Y up to 7 MeV* Account Nr.: 00269871]]></dc:title>
<dc:source><![CDATA[Nuclear Physics A 620 (1997) 1-15]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The semi-magic nucleus <SUP>89</SUP>Y has been investigated in a (gamma,gamma')
experiment at an endpoint energy of the bremsstrahlung of E<SUB>0</SUB>=
7 MeV. The scattered photons have been detected with a EUROBALL Cluster
detector. The observed excitations are discussed in the framework of the
shell model and a coupling of the unpaired proton to milti-phonon structures
in the doubly even neighbours. Transitions above 4.7 MeV are considered
to have E1 character. Around 6.3 MeV an unusually large concentration of
E1 strength is found. Its origin is likely to correspond to similar structures
in the <SUP>88</SUP>Sr and <SUP>90</SUP>Zr isotones which can be interpreted
to result from the constructive interference of strong two-phonon amplitudes
with weak admixtures from the low-energy tail of the giant dipole resonance.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-752-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:844-1</identifier>
<datestamp>2022-11-11</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schnare, H.]]></dc:creator>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:creator><![CDATA[Käubler, L.]]></dc:creator>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-844-1</dc:identifier>
<dc:title><![CDATA[Resolution-enhanced spectroscopy of <SUP>81</SUP>Y]]></dc:title>
<dc:source><![CDATA[Physical Review C Volume 56, Number 2, 729-743]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The fusion-evaporation reaction <SUP>58</SUP>Ni(<SUP>32</SUP>S,2 alpha
p ) has been used to study the neutron-deficient isotope <SUP>81</SUP>Y.
Multiple particle gamma-ray coincidences have been detected by the GAMMASPHERE
array combined with the MICROBALL chrged-particle detector system. Gamma-ray
spectra with an improved resolution have been achieved from an event-by-event
determination of the nucleus recoil momentum, thus allowing a precise Doppler-shift
correction. In this way a resolution enhancement by a factor 2 was obtained
for a 1 MeV gamma line. During the analysis an E<SUB>gamma</SUB> - E<SUB>gamma</SUB>
matrix as well as an E<SUB>gamma</SUB> - E<SUB>gamma</SUB> - E<SUB>gamma</SUB>
cube have been used to extend the previously known level scheme to higher
spin ( I ca. 57/2 ) and excitation energy ( E<SUB>x</SUB> ca. 17 MeV ).
More than 100 new gamma rays and 80 new levels have been added to the level
scheme and six new bands have been established. The interpretation of these
bands in terms of the cranking model and their comparison with similar
bands in neighboring nuclei is discussed.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevC.56.729]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-844-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:995-1</identifier>
<datestamp>2023-04-27</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Lane, G. J.]]></dc:creator>
<dc:creator><![CDATA[Fossan, D. B.]]></dc:creator>
<dc:creator><![CDATA[Thorslund, I.]]></dc:creator>
<dc:creator><![CDATA[Vaska, P.]]></dc:creator>
<dc:creator><![CDATA[Allatt, R. G.]]></dc:creator>
<dc:creator><![CDATA[Paul, E. S.]]></dc:creator>
<dc:creator><![CDATA[Käubler, L.]]></dc:creator>
<dc:creator><![CDATA[Schnare, H.]]></dc:creator>
<dc:creator><![CDATA[Hibbert, I. M.]]></dc:creator>
<dc:creator><![CDATA[O'Brien, N.]]></dc:creator>
<dc:creator><![CDATA[Wadsworth, R.]]></dc:creator>
<dc:creator><![CDATA[Andrejtscheff, W.]]></dc:creator>
<dc:creator><![CDATA[Graaf, J.]]></dc:creator>
<dc:creator><![CDATA[Simpson, J.]]></dc:creator>
<dc:creator><![CDATA[Lee, I. Y.]]></dc:creator>
<dc:creator><![CDATA[Macchiavelli, A. O.]]></dc:creator>
<dc:creator><![CDATA[Blumenthal, D. J.]]></dc:creator>
<dc:creator><![CDATA[Davids, C. N.]]></dc:creator>
<dc:creator><![CDATA[Lister, C. J.]]></dc:creator>
<dc:creator><![CDATA[Seweryniak, D.]]></dc:creator>
<dc:creator><![CDATA[Afanasjev, A. V.]]></dc:creator>
<dc:creator><![CDATA[Ragnarsson, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-995-1</dc:identifier>
<dc:title><![CDATA[Identification of Excited States in Doubly Odd <SUP>110</SUP>Sb: Smooth Band Termination]]></dc:title>
<dc:source><![CDATA[Physical Review C, Nuclear Physics, 3rd Series, Volume 55, Number 5]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Excited states in <SUP>110</SUP>Sb have been identified for the first time
in a series of gamma-spectroscopy experiments using both thin and backed
targets, including neutron-fold and recoil-mass measurements to provide
unambiguous channel identification. The three decoupled intruder bands
observed in <SUP>110</SUP>Sb are based upon configurations involving 2p-2h
excitations across the Z=50 shell gap and show the features of smooth band
termination. The yrast intruder band, which has been connected to the low-spin
levels, is tentatively identified up to its predicted termination at I<SUP>Pi</SUP>=45<SUP>+</SUP>.
Excellent agreement with configuration-dependent cranked Nilsson-Strutinsky
calculations is obtained for the high-spin states near termination.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevC.55.R2127]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-995-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:595-1</identifier>
<datestamp>2020-10-29</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brentano, P.]]></dc:creator>
<dc:creator><![CDATA[Eberth, J.]]></dc:creator>
<dc:creator><![CDATA[Enders, J.]]></dc:creator>
<dc:creator><![CDATA[Esser, L.]]></dc:creator>
<dc:creator><![CDATA[Herzberg, R.-D.]]></dc:creator>
<dc:creator><![CDATA[Huxel, N.]]></dc:creator>
<dc:creator><![CDATA[Meise, H.]]></dc:creator>
<dc:creator><![CDATA[Neumann-Cosel, P.]]></dc:creator>
<dc:creator><![CDATA[Nicolay, N.]]></dc:creator>
<dc:creator><![CDATA[Pietralla, N.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:creator><![CDATA[Richter, A.]]></dc:creator>
<dc:creator><![CDATA[Schlegel, C.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Skoda, S.]]></dc:creator>
<dc:creator><![CDATA[Thomas, H. G.]]></dc:creator>
<dc:creator><![CDATA[Wiedenhöver, I.]]></dc:creator>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:creator><![CDATA[Zilges, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-595-1</dc:identifier>
<dc:title><![CDATA[First Observation of the Scissors Mode in a Gamma-Soft Nucleus: The Case of 196Pt]]></dc:title>
<dc:source><![CDATA[Physical Review Letters 76 (1996) 12 pp. 2029-32]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[A nuclear resonance fluorescence experiment with one of the newly developed
highly efficient EUROBALL cluster detectors has been performed on the gamma-soft
nucleus <SUP>196</SUP>Pt. Magnetic dipole excitations were observed between
2 and 3.5 MeV excitation energiy. They are interpreted as the main fragments
of the scissors mode based on the measured excitation strengths and branching
ratios. A strong gamma decay, which we believe to be an E2 decay of the
scissors mode to the 2<SUB>1</SUB><SUP>+ </SUP>state, is observed. It allows
an extraction of the effective boson quadrupole charges in the interacting
boson model.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevLett.76.2029]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-595-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:713-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Radermacher, E.]]></dc:creator>
<dc:creator><![CDATA[Wilhelm, M.]]></dc:creator>
<dc:creator><![CDATA[Albers, S.]]></dc:creator>
<dc:creator><![CDATA[Eberth, J.]]></dc:creator>
<dc:creator><![CDATA[Nicolay, N.]]></dc:creator>
<dc:creator><![CDATA[Thomas, H. G.]]></dc:creator>
<dc:creator><![CDATA[Brentano, P.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Skoda, S.]]></dc:creator>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:creator><![CDATA[Maier, K. H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-713-1</dc:identifier>
<dc:title><![CDATA[The gamma-decay of particle-hole states in 208Pb using the Euroball Cluster detector]]></dc:title>
<dc:source><![CDATA[Nuclear Physics A 597 (1996) pp. 408-426]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Neutron particle-hole states in the doubly magic nucleus <SUP>208</SUP>Pb
were investigated using a Euroball Cluster detector and five usual HPGe
detectors at the Osiris cube spectrometer in Cologne. 126 gamma-ray transitions
with energies up to 7.2 MeV could be detected, 14 of those for the first
time. The states were excited with the <SUP>208</SUP>Pb (p,p'gamma)<SUP>208</SUP>Pb
reaction via isobaric analogue resonances in <SUP>209</SUP>Bi at E<SUB>p</SUB>=16.5,
17, 17.45, 17.5 and 18.5 MeV and through the subcoulomb <SUP>207</SUP>Pb(d,pgamma)<SUP>208</SUP>Pb
reaction at E<SUB>d</SUB>=10 MeV. For most of the excited states assignments
for the particle and/or the hole component of the configuration could be
made, 22 of these are new.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-713-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:14325-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Sytcheva, A.]]></dc:creator>
<dc:creator><![CDATA[Löw, U.]]></dc:creator>
<dc:creator><![CDATA[Yasin, S.]]></dc:creator>
<dc:creator><![CDATA[Wosnitza, J.]]></dc:creator>
<dc:creator><![CDATA[Zherlitsyn, S.]]></dc:creator>
<dc:creator><![CDATA[Thalmeier, P.]]></dc:creator>
<dc:creator><![CDATA[Goto, T.]]></dc:creator>
<dc:creator><![CDATA[Wyder, P.]]></dc:creator>
<dc:creator><![CDATA[Lüthi, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14325-1</dc:identifier>
<dc:title><![CDATA[Acoustic Faraday effect in Tb<sub>3</sub>Ga<sub>5</sub>O<sub>12</sub>]]></dc:title>
<dc:source><![CDATA[Physical Review B 81(2010), 214415]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The transverse acoustic wave propagating along the [100] axis of the cubic Tb<sub>3</sub>Ga<sub>5</sub>O<sub>12</sub> (acoustic c<sub>44</sub> mode) is doubly degenerate. A magnetic field applied in the direction of propagation lifts this degeneracy and leads to the rotation of the polarization vector - the magnetoacoustic Faraday rotation. Here, we report on the observation and analysis of the magnetoacoustic Faraday effect in Tb<sub>3</sub>Ga<sub>5</sub>O<sub>12</sub> in static and pulsed magnetic fields. We present also a theoretical model based on magnetoelastic coupling of 4f electrons to both, acoustic and optical phonons and an effective coupling between them. This model explains the observed linear frequency dependence of the Faraday rotation angle.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14325-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:14277-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Tsushima, S.]]></dc:creator>
<dc:creator><![CDATA[Brendler, V.]]></dc:creator>
<dc:creator><![CDATA[Fahmy, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14277-1</dc:identifier>
<dc:title><![CDATA[Aqueous coordination chemistry and photochemistry of uranyl(VI) oxalate revisited: a density functional theory study]]></dc:title>
<dc:source><![CDATA[Dalton Transactions 39(2010)45, 10953-10958]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Using density functional theory (DFT) calculations, we revisited a classical problem of uranyl(VI) oxalate photochemical decomposition. Photoreactivities of uranyl(VI) oxalate complexes are found to correlate largely with ligand-structural arrangements. Importantly, the intramolecular photochemical reaction is inhibited when oxalate is bound to uranium exclusively in chelate binding mode. Previously proposed mechanisms involving a UO<sub>2</sub>(C<sub>2</sub>O<sub>4</sub>)<sub>2</sub><sup>2-</sup> (1:2) complex as the main photoreactive species are thus unlikely to apply, because the two oxalic acids are bound to uranium in a chelating binding mode. Our DFT results suggest that the relevant photoreactive species are UO<sub>2</sub>(C<sub>2</sub>O<sub>4</sub>)<sub>3</sub><sup>4-</sup> (1:3) and (UO<sub>2</sub>)<sub>2</sub>(C<sub>2</sub>O<sub>4</sub>)<sub>5</sub><sup>6-</sup> (2:5) complexes binding uranium in an unidentate fashion. These species go through decarboxylation upon excitation to the triplet state, which ensues the release of CO<sub>2</sub> and reduction of U(VI) to U(V). The calculations also suggest an alternative intermolecular pathway at low pH via an electron transfer between the excited state *UO<sub>2</sub><sup>2+</sup> and hydrogen oxalate (HC<sub>2</sub>O<sub>4</sub><sup>-</sup>) which eventually leads to the production of CO and OH<sup>-</sup> with no net reduction of U(VI). The calculated results are consistent with previous experimental findings that CO is only detected at low pH while U(IV) is detected only at high pH.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1039/C0DT00974A]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14277-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:209-1</identifier>
<datestamp>2020-12-07</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Käubler, L.]]></dc:creator>
<dc:creator><![CDATA[Wirowski, R.]]></dc:creator>
<dc:creator><![CDATA[Nicolay, N.]]></dc:creator>
<dc:creator><![CDATA[Albers, S.]]></dc:creator>
<dc:creator><![CDATA[Esser, S.]]></dc:creator>
<dc:creator><![CDATA[Brentano, P.]]></dc:creator>
<dc:creator><![CDATA[Andrejtscheff, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-209-1</dc:identifier>
<dc:title><![CDATA[Particle excitations and collectivity in the N=48 nuclei <SUP>83</SUP>Br and <SUP>85</SUP>Rb]]></dc:title>
<dc:source><![CDATA[Nuclear Physics A 584 (1995) pp. 159]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Excited states of the nuclei <SUP>83</SUP>Br and <SUP>85</SUP>Rb were populated
in the reaction <SUP>82</SUP>Se(<SUP>7</SUP>Li,alpha2n) and <SUP>82</SUP>Se(<SUP>7</SUP>Li,4n),
respectively, using the <SUP>7</SUP>Li beams of the FN tandem accelerator
in Cologne (E=32 MeV) and of the 120 cm cyclotron in Rossendorf (E=35 MeV).Gamma-gamma-particle
coincidences were measured with six Ge and fourteen Si detectors installed
at the detector array Cologne OSIRIS CUBE. This technique enabled a reaction
channel selection. Multipole orders of the gamma-rays were derived from
directional correlations of coincident gamma-rays and from angular distributions.
Mean lifetimes were deduced for seven levels in <SUP>83</SUP>Br and two
levels in <SUP>85</SUP>Rb using the Doppler-shift-attenuation method. The
level scheme of <SUP>83</SUP>Br has been extended up to (21<SUP>+</SUP>/2)
and 15<SUP>-</SUP>/2 states. In <SUP>85</SUP>Rb a level sequence built
on the ground state has been established up to 15<SUP>(-)</SUP>/2 and a
new cascade of fast M1 transitions starting with a 17<SUP>(-)</SUP>/2 state
at 3198.2 keV has been found. Furthermore, several medium-spin states have
been newly introduced. The level sequences inboth nuclei have been interpreted
in terms of the shell model. The calculations performed in the model space
pi(0g<SUB>9/2</SUB>, 1p<SUB>1/2</SUB>, 1p<SUB>3/2</SUB>, 0f<SUB>5/2</SUB>)
v(0g<SUB>9/2,</SUB> 1p<SUB>1/2</SUB>) reproduce single-particle characteristics
as well as collective properties of the level sequences.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/0375-9474(94)00488-9]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-209-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:642-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Käubler, L.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:creator><![CDATA[Grawe, H.]]></dc:creator>
<dc:creator><![CDATA[Heese, J.]]></dc:creator>
<dc:creator><![CDATA[Kluge, H.]]></dc:creator>
<dc:creator><![CDATA[Maier, K. H.]]></dc:creator>
<dc:creator><![CDATA[Schubart, R.]]></dc:creator>
<dc:creator><![CDATA[Spohr, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-642-1</dc:identifier>
<dc:title><![CDATA[In-Beam Study of <SUP>109</SUP>Sn]]></dc:title>
<dc:source><![CDATA[Physica Scripta T56 (1995) pp. 266]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[In-beam spectroscopic investigations of <SUP>109</SUP>Sn have been performed
using the reactions <SUP>55</SUP>Mn(<SUP>58</SUP>Ni,3pn) and <SUP>106</SUP>Cd(alpha,n)
with E<SUB>58Ni</SUB>= 240 MeV and E<SUB>alpha</SUB>=23 MeV, respectively.
An extended level scheme of <SUP>109</SUP>Sn is presemted showing high-spin
states up to E<SUB>x </SUB>ca. 8 MeV with J<SUP>pi</SUP>=(41/2<SUP>+</SUP>).
The problem of the <SUP>109</SUP>Sn ground state has been solved identifying
a 12.8 keV transition deexciting the 7/2<SUP>+</SUP> state to the 5/2<SUP>+
</SUP>g.s. A half-life of T<SUB>1/2</SUB>=7(1) ns has been measured for
the 17/2<SUP>+ </SUP>state at E<SUB>x</SUB>=2114 keV. The experimental
data are compared with the predictions of shell-model calculations.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-642-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:237-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Grawe, H.]]></dc:creator>
<dc:creator><![CDATA[Schubart, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-237-1</dc:identifier>
<dc:title><![CDATA[Neutron-Core Excitations in <SUB>36</SUB><SUP>86</SUP>Kr<SUB>50</SUB>]]></dc:title>
<dc:source><![CDATA[Physica Scripta T56 (1995) pp. 303]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Shell-model calculations for the N=50 nucleus <SUP>86</SUP>Kr are presented
and compared toresults of recent in-beam experiments. Two model spaces
are considered: a pure proton configuration space containing the 0f<SUB>5/2</SUB>,
1p<SUB>3/2</SUB>, 1p<SUB>1/2</SUB>, 0g<SUB>9/2 </SUB>orbitals and a model
space including additionally the particlehole&nbsp; excitation generated
by one neutron lifted from the 0g<SUB>9/2</SUB> orbital across the shell
gap to the 1d<SUB>5/2 </SUB>orbital. The predictions of the shell-model
using various sets of residual interactions and based on pure proton excitations
are comparable with the experimental findings for the states of positive
parity below 4 MeV and for the negative-parity states with spins up to
7<SUP>-</SUP>. The inclusion of neutron-core excitations causes an improved
agreement between experimental and calculated level energies for the positive-parity
yrast states with spins 7, 9 and 10. The interpretation of neutron-core
excited high-spin states is supported by the comparision of the level structure
of <SUB>36</SUB><SUP>86</SUP>Kr<SUB>50 </SUB>to the experimental levels
of the valence-mirror nucleus <SUB>28</SUB><SUP>64</SUP>Ni<SUB>36</SUB>.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-237-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1192-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Käubler, L.]]></dc:creator>
<dc:creator><![CDATA[Schnare, H.]]></dc:creator>
<dc:creator><![CDATA[Fossan, D. B.]]></dc:creator>
<dc:creator><![CDATA[Afanasjev, A. V.]]></dc:creator>
<dc:creator><![CDATA[Andrejtscheff, W.]]></dc:creator>
<dc:creator><![CDATA[Allatt, R. G.]]></dc:creator>
<dc:creator><![CDATA[Graaf, J.]]></dc:creator>
<dc:creator><![CDATA[Grawe, H.]]></dc:creator>
<dc:creator><![CDATA[Hibbert, I. M.]]></dc:creator>
<dc:creator><![CDATA[Lee, I. Y.]]></dc:creator>
<dc:creator><![CDATA[Macchiavelli, A. D.]]></dc:creator>
<dc:creator><![CDATA[O'Brien, N.]]></dc:creator>
<dc:creator><![CDATA[Maier, K. H.]]></dc:creator>
<dc:creator><![CDATA[Paul, E. S.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Ragnarsson, I.]]></dc:creator>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:creator><![CDATA[Schubart, R.]]></dc:creator>
<dc:creator><![CDATA[Thorslund, I.]]></dc:creator>
<dc:creator><![CDATA[Vaska, P.]]></dc:creator>
<dc:creator><![CDATA[Wadsworth, R.]]></dc:creator>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1192-1</dc:identifier>
<dc:title><![CDATA[Collective structures and smooth band termination in <SUP>109</SUP>Sn]]></dc:title>
<dc:source><![CDATA[Z. Phys. A356 (1996) 235-237]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Six rotational bands up to energies E<SUB>x</SUB>=24.7 MeV and spins J<SUP>pi</SUP>=(79/2<SUP>-</SUP>)
have been identified in <SUP>109</SUP>Sn using the GAMMASPHERE gamma-detector
array. Four of the bands show smoothly decreasing dynamic moments of inertia
at rotational frequencies hv > 0.6 MeV. The bands arise at medium spins
from coupling of a valence d<SUB>5/2</SUB>, g<SUB>7/2</SUB> or h<SUB>11/2</SUB>
neutron to the deformed 2p2h proton excitation of the Z=50 core <SUP>108</SUP>Sn.
At very high hv these bands show the typical behaviour of smoothly terminating
bands, i.e. a gradual alignment of the angular momenta of the valence particles
and holes corresponding to a transition from high collectivity to noncollective
states.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1192-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1193-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Frauendorf, S.]]></dc:creator>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1193-1</dc:identifier>
<dc:title><![CDATA[Magnetic dipole bands in odd indium isotopes built on the pig<SUB>9/2</SUB><SUP>-1</SUP>vh<SUB>11/2</SUB><SUP>2</SUP> configuration]]></dc:title>
<dc:source><![CDATA[Nuclear Physics A 621 (1997) 736-744]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The structure of the magnetic dipole bands is studied by means of shell-modell
calculations. The calculations correlate with the data, showing a transition
from irregular sequences in the light isotopes to regular bands in the
heavy ones. The analysis of the wave functions reveals a more complex mechanism
of angular momentum generation than in the Pb isotopes: the shears mechanism
of the intruder orbitals and the normal parity neutrons make comparable
contributions.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1193-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1290-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Coleman, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1290-1</dc:identifier>
<dc:title><![CDATA[Characterization of vacancy-type defects in Al<SUP>+</SUP> and N<SUP>+</SUP> ion implanted SiC by slow positron implantation spectroscopy]]></dc:title>
<dc:source><![CDATA[Applied Surface Science 149 (1999) 140-143]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1290-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1291-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Coleman, P. G.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1291-2</dc:identifier>
<dc:title><![CDATA[Characterization of Defects in Ion Implanted SiC by Slow Positron Implantation Spectroscopy and Rutherford Backscattering]]></dc:title>
<dc:source><![CDATA[8th Int. Workshop on Slow Positron Beam Techniques for Solids and Surfaces (SLOPOS-8), Cape Town, Sept. 6 - 12, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1291-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1291-3</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Coleman, P. G.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
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<dc:description><![CDATA[Die durchgeführten Untersuchungen an 50 netzgekoppelten PV-Anlagen (Leistungsbereich < 5 kWp) ermöglichten eine vergleichende Analyse der eingesetzten Hauptkomponenten sowie eine Beurteilung der gewählten Anlagenkonzepte. Danach steht bei den Modulen -neben dem Übergang zu Großmodulen- die Erhöhung der Qualität (STC-Leistung !) eindeutig im Vordergrund. Als brauchbarstes Wandlungskonzept in den Wechselrichtern hat sich die Pulsweiten-Modulation erwiesen. Neben hohen Jahresnutzungsgraden (94 %) sollten künftige Modelle durch einen hohen Eingangsspannungsbereich (bis 600 V) die Installation von Einstrang-Anlagen ermöglichen. Durch die Integration von Komponenten zur Anlagendiagnose (etwa PR-Überwachung) und Erhöhung der Zuverlässigkeit können weitere Ertragspotentiale erschlossen werden. Jahreserträge von deutlich über 800 kWh/kWp sind damit bei gut ausgerichteten Anlagen auch im hier untersuchten Leistungsbereich erreichbar.
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]]></dc:description>
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<dc:title><![CDATA[Corrosion Protection of Titanium by Deposition of Niobium Thin Films]]></dc:title>
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<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
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<dc:title><![CDATA[Corrosion Protection of Titanium by Deposition of Niobium Thin Films]]></dc:title>
<dc:source><![CDATA[Surface & Coatings Technology 116-119 (1999) 1107-1110]]></dc:source>
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<dc:creator><![CDATA[Baraniak, L.]]></dc:creator>
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<dc:title><![CDATA[Sorption Behaviour of Radium on Sandy and Clayey Sediments of the Upper Saxon Elbe River Valley]]></dc:title>
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<dc:description><![CDATA[With the background of uranium mine restoration the adsorption of radium on different kinds of sandstone, claystone and lime marl was studied in dependence on such parameters as water composition, acidity, phase contact time and the concentration of radium, barium and sulfate by static batch experiments at the mine temperature of 14°C.]]></dc:description>
<dc:subject><![CDATA[Environmental Radioactivity]]></dc:subject>
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<dc:subject><![CDATA[Distribution Ratio]]></dc:subject>
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<dc:title><![CDATA[Cold quark stars from hot lattice QCD: a comparison]]></dc:title>
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<dc:description><![CDATA[Based on a quasiparticle model for \beta stable and electrically neutral deconfined matter we address the possibility of pure quark stars. The model is adjusted to recent hot lattice QCD results for 2+1 flavors with almost physical quark masses. Using stability and binding arguments general statements can be made concerning the existence of such compact stellar objects.]]></dc:description>
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<dc:title><![CDATA[Toward a soft x-ray fourier-transform spectrometer]]></dc:title>
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<dc:title><![CDATA[Structural Investigations on Pyrolysed Polycarbosilanes]]></dc:title>
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<dc:creator><![CDATA[Neu, M. P.]]></dc:creator>
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<dc:title><![CDATA[Comparison of chemical extractions and laser photoacoustic spectroscopy for the determination of plutonium species in carbonate solution]]></dc:title>
<dc:source><![CDATA[Radiochimica Acta 66/67 (1994) pp. 251]]></dc:source>
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<dc:title><![CDATA[Long term plutonium solubility and speciation studies in a synthetic brine]]></dc:title>
<dc:source><![CDATA[Radiochimica Acta 66/67 (1994) pp. 3]]></dc:source>
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<dc:title><![CDATA[The effects of radiolysis upon speciation and solubility of neptunium in brine solutions]]></dc:title>
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<dc:title><![CDATA[Degradation of 3,3',4,4'-Tetrachlorobiphenyl by selected white rot fungi]]></dc:title>
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<dc:title><![CDATA[The Hydrothermal Chromate Treatment of Carbon Steel. The Electrochemical and Surface Analytical Characterisation of Protecting Oxide Layers]]></dc:title>
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<dc:title><![CDATA[Transformation of Titanium Carbide Precipitations under Hydrothermal Conditions]]></dc:title>
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<identifier>HZDR:PUBLDB:633-1</identifier>
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<dc:creator><![CDATA[Thieme, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-633-1</dc:identifier>
<dc:title><![CDATA[Characterisation of Oxide Layers Formed by Hydrothermal Chromate Treatment]]></dc:title>
<dc:source><![CDATA[Corros. Sci. 34 (1993) pp. 1557]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:634-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Baraniak, L.]]></dc:creator>
<dc:creator><![CDATA[Mende, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-634-1</dc:identifier>
<dc:title><![CDATA[Mining Relics as Sources of Natural Radioactivity - Release of Radon from Uranium Mill Tailings]]></dc:title>
<dc:source><![CDATA[Hrsg.: Winter, M., Wicke, A., "Umweltradioaktivität, Radioökologie und Strahleneinwirkungen" Verlag TÜV Rheinland, 1 (1993) pp. 76]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:635-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Baldsiefen, G.]]></dc:creator>
<dc:creator><![CDATA[Maagh, P.]]></dc:creator>
<dc:creator><![CDATA[Hübel, H.]]></dc:creator>
<dc:creator><![CDATA[Korten, W.]]></dc:creator>
<dc:creator><![CDATA[Chmel, S.]]></dc:creator>
<dc:creator><![CDATA[Neffgen, M.]]></dc:creator>
<dc:creator><![CDATA[Pohler, W.]]></dc:creator>
<dc:creator><![CDATA[Grawe, H.]]></dc:creator>
<dc:creator><![CDATA[Maier, K. H.]]></dc:creator>
<dc:creator><![CDATA[Spohr, K.]]></dc:creator>
<dc:creator><![CDATA[Schubart, R.]]></dc:creator>
<dc:creator><![CDATA[Frauendorf, S.]]></dc:creator>
<dc:creator><![CDATA[Maier, H. J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-635-1</dc:identifier>
<dc:title><![CDATA[Shears bands in 201Pb and 202Pb]]></dc:title>
<dc:source><![CDATA[Nuclear Physics A 592 (1995) pp. 365]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:637-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Deleplanque, M. A.]]></dc:creator>
<dc:creator><![CDATA[Frauendorf, S.]]></dc:creator>
<dc:creator><![CDATA[Clark, D. L.]]></dc:creator>
<dc:creator><![CDATA[Diamond, R. M.]]></dc:creator>
<dc:creator><![CDATA[Stephens, F. S.]]></dc:creator>
<dc:creator><![CDATA[Becker, J. A.]]></dc:creator>
<dc:creator><![CDATA[Brinkmann, M. J.]]></dc:creator>
<dc:creator><![CDATA[Cederwall, B.]]></dc:creator>
<dc:creator><![CDATA[Fallon, P.]]></dc:creator>
<dc:creator><![CDATA[Farris, L. P.]]></dc:creator>
<dc:creator><![CDATA[Henry, E. A.]]></dc:creator>
<dc:creator><![CDATA[Hubel, H.]]></dc:creator>
<dc:creator><![CDATA[Hughes, J. R.]]></dc:creator>
<dc:creator><![CDATA[Korten, W.]]></dc:creator>
<dc:creator><![CDATA[Lee, I. Y.]]></dc:creator>
<dc:creator><![CDATA[Macchiavelli, A. O.]]></dc:creator>
<dc:creator><![CDATA[Stoyer, M. A.]]></dc:creator>
<dc:creator><![CDATA[Willsau, P.]]></dc:creator>
<dc:creator><![CDATA[Draper, J. E.]]></dc:creator>
<dc:creator><![CDATA[Duyar, C.]]></dc:creator>
<dc:creator><![CDATA[Rubel, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-637-1</dc:identifier>
<dc:title><![CDATA[Low-spin termination of the superdeformed band in 135Nd]]></dc:title>
<dc:source><![CDATA[Physical Review C 52 (1995) pp. R2302]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:638-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Dzelalija, M.]]></dc:creator>
<dc:creator><![CDATA[Kotte, R.]]></dc:creator>
<dc:creator><![CDATA[Mösner, J.]]></dc:creator>
<dc:creator><![CDATA[Neubert, W.]]></dc:creator>
<dc:creator><![CDATA[Wohlfarth, D.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-638-1</dc:identifier>
<dc:title><![CDATA[Entropy in central Au + Au reactions beetween 100 and 400 A MeV]]></dc:title>
<dc:source><![CDATA[Physical Review C 52 (1995) pp. 346]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:639-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gorelik, G.]]></dc:creator>
<dc:creator><![CDATA[Rotter, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-639-1</dc:identifier>
<dc:title><![CDATA[Matwej Bronstein und die Anfänge der Quantengravitation]]></dc:title>
<dc:source><![CDATA[Physikalische Blätter 51 (1995) pp. 423]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
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<header>
<identifier>HZDR:PUBLDB:640-1</identifier>
<datestamp>2019-03-04</datestamp>
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</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Käubler, L.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:creator><![CDATA[Grawe, H.]]></dc:creator>
<dc:creator><![CDATA[Heese, J.]]></dc:creator>
<dc:creator><![CDATA[Kluge, H.]]></dc:creator>
<dc:creator><![CDATA[Maier, K. H.]]></dc:creator>
<dc:creator><![CDATA[Schubart, R.]]></dc:creator>
<dc:creator><![CDATA[Spohr, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-640-1</dc:identifier>
<dc:title><![CDATA[High-spin states in <SUP>109</SUP>Sn and their decay to the ground state]]></dc:title>
<dc:source><![CDATA[Zeitschrift für Physik A 351 (1995) pp. 123]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[An extended level scheme of <SUP>109</SUP>Sn is presented showing high-spin
states up to E<SUB>x </SUB>ca. 8 MeV and spins up to Jpi=(41/2<SUP>+</SUP>).
Their decay to the 5/2<SUP>+</SUP> ground state has been observed identifying
a 12.8 keV 7/2<SUP>+</SUP> -> 5/2<SUP>+</SUP> transition. A half life of
T<SUB>1/2</SUB>=7(1) ns has been measured for the 17/2<SUP>+</SUP> state
at E<SUB>x</SUB>=2114 keV. The experimental data are compared with the
predictions of shell-model calculations.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:format><![CDATA[application/pdf]]></dc:format>
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<header>
<identifier>HZDR:PUBLDB:649-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pochodzalla, J.]]></dc:creator>
<dc:creator><![CDATA[Möhlenkamp, T.]]></dc:creator>
<dc:creator><![CDATA[Rubehn, T.]]></dc:creator>
<dc:creator><![CDATA[Schüttauf, A.]]></dc:creator>
<dc:creator><![CDATA[Wörner, A.]]></dc:creator>
<dc:creator><![CDATA[Zude, E.]]></dc:creator>
<dc:creator><![CDATA[Begemann-Blaich, M.]]></dc:creator>
<dc:creator><![CDATA[Blaich, T.]]></dc:creator>
<dc:creator><![CDATA[Emling, H.]]></dc:creator>
<dc:creator><![CDATA[Ferrero, A.]]></dc:creator>
<dc:creator><![CDATA[Gross, C. J.]]></dc:creator>
<dc:creator><![CDATA[Immé, G.]]></dc:creator>
<dc:creator><![CDATA[Iori, I.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-649-1</dc:identifier>
<dc:title><![CDATA[Probing the nuclear liquid-gas phase transition]]></dc:title>
<dc:source><![CDATA[Physical Review Letters 75 (1995) pp. 1040]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-649-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:653-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ritman, J. L.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-653-1</dc:identifier>
<dc:title><![CDATA[The FOPI Detector at SIS/GSI]]></dc:title>
<dc:source><![CDATA[Nuclear Physics B (Proc. Suppl.) 44 (1995) pp. 708]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-653-1</dc:relation>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:656-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schult, O. W. B.]]></dc:creator>
<dc:creator><![CDATA[Sistemich, K.]]></dc:creator>
<dc:creator><![CDATA[Koptev, V.]]></dc:creator>
<dc:creator><![CDATA[Müller, H.]]></dc:creator>
<dc:creator><![CDATA[Cassing, W.]]></dc:creator>
<dc:creator><![CDATA[Jarczyk, L.]]></dc:creator>
<dc:creator><![CDATA[Komarov, V. I.]]></dc:creator>
<dc:creator><![CDATA[Sibirtsev, A.]]></dc:creator>
<dc:creator><![CDATA[Ernst, J.]]></dc:creator>
<dc:creator><![CDATA[Santo, R.]]></dc:creator>
<dc:creator><![CDATA[Nioradze, M.]]></dc:creator>
<dc:creator><![CDATA[Kulikov, A. V.]]></dc:creator>
<dc:creator><![CDATA[Hardt, A.]]></dc:creator>
<dc:creator><![CDATA[Dshemuchadse, S.]]></dc:creator>
<dc:creator><![CDATA[Leege, K.-W.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-656-1</dc:identifier>
<dc:title><![CDATA[Plans for investigations of subthreshold K<SUP>+</SUP> production in p<SUP>+</SUP>A collisions]]></dc:title>
<dc:source><![CDATA[Nuclear Physics A 583 (1995) pp. 629]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[We plan to investigate sub-threshold K<SUP>+</SUP> production in proton bombardment of atomic nuclei in order to study the reaction mechanism through a measurement of the double differential cross section and of K<SUP>+</SUP> p and K<SUP>+</SUP> d coincides. The status of the theoretical studies is summarized, and the spectrometer to be installed in the COSY ring is briefly described.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-656-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1330-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Preusche, S.]]></dc:creator>
<dc:creator><![CDATA[Füchtner, F.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1330-1</dc:identifier>
<dc:title><![CDATA[The Rossendorf PET Cyclotron "CYCLONE 18/9" Facility-Two Years of Operation]]></dc:title>
<dc:source><![CDATA["IBA PET CYCLONE USERS, Second Workshop", Eds. KU Leuven and IBA,
Leuven, Belgium, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[An overview of the two years of operation of the Rossendorf CYCLONE 18/9 facility is given. Datas of the radionuclide production are presented and improvements at the cyclotron and our experience in operation and maintenance of the CYCLONE 18/9 are described.]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1331-1</dc:identifier>
<dc:title><![CDATA[Introduction to X-Ray Diffraction at Synchrotron Light Sources]]></dc:title>
<dc:source><![CDATA[Actinide-XAS-98 Conference, Grenoble Oct. 4-6 , 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1331-2</dc:identifier>
<dc:title><![CDATA[Introduction to X-Ray Diffraction at Synchrotron Light Sources]]></dc:title>
<dc:source><![CDATA[Proceedings Actinide-XAS-98 Conference, Grenoble Oct. 4-6 , 1998, p. 40-49]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1333-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Dönau, F.]]></dc:creator>
<dc:creator><![CDATA[Zhang, J. Y.]]></dc:creator>
<dc:creator><![CDATA[Riedinger, L. L.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1333-1</dc:identifier>
<dc:title><![CDATA[Restorationof the Broken D2-Symmetry in the Mean Field Description of Rotating Nuclei]]></dc:title>
<dc:source><![CDATA[Physics Letters B 450 (1999) 313-319]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1334-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1334-2</dc:identifier>
<dc:title><![CDATA[Messung von Gasgehalt, Gasgeschwindigkeit und Volumenstrom mit Gittersensoren]]></dc:title>
<dc:source><![CDATA[1. Chemnitzer Verfahrenstechnisches Kolloquium / Strömungen in der Verfahrenstechnik, 25.-26. Nov. 1998, TU Chemnitz]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Mit Hilfe neuartiger Gittersensoren können  Gasgehaltsverteilungen in einer Zweiphasenströmung im Strömungsquerschnitt mit einer Zeitauflösung von über 1000 Hz gemessen werden. Die Sensoren beruhen auf einer elektrischen Leitfähigkeitsmessung. Zwei hintereinander angeordnete Sensoren erlauben die Ermittlung von Geschwindigkeitsverteilungen der Gasphase. Hierzu werden die Zeitverläufe des Gasgehalts an den einzelnen Meßpunkten der beiden Sensoren individuell durch Berechnung von Kreuzkorrelationsfunktionen ausgewertet. Die erhaltenen Geschwindigkeitsverteilungen können mit den ebenfalls gemessenen Gasgehalten multipliziert und über dem Querschnitt integriert werden. Dadurch erhält man den Gesamtvolumenstrom der Gasphase. Tests an einer mit Wasser-Luft-Gemisch betriebenen Versuchsschleife zeigen die Funktionsfähigkeit dieses Verfahrens. ]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
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<identifier>HZDR:PUBLDB:1334-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1334-1</dc:identifier>
<dc:title><![CDATA[Messung von Gasgehalt, Gasgeschwindigkeit und Volumenstrom mit Gittersensoren]]></dc:title>
<dc:source><![CDATA[1. Chemnitzer Verfahrenstechnisches Kolloquium / Strömungen in der Verfahrenstechnik, 25.-26. Nov. 1998, TU Chemnitz]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Mit Hilfe neuartiger Gittersensoren können  Gasgehaltsverteilungen in einer Zweiphasenströmung im Strömungsquerschnitt mit einer Zeitauflösung von über 1000 Hz gemessen werden. Die Sensoren beruhen auf einer elektrischen Leitfähigkeitsmessung. Zwei hintereinander angeordnete Sensoren erlauben die Ermittlung von Geschwindigkeitsverteilungen der Gasphase. Hierzu werden die Zeitverläufe des Gasgehalts an den einzelnen Meßpunkten der beiden Sensoren individuell durch Berechnung von Kreuzkorrelationsfunktionen ausgewertet. Die erhaltenen Geschwindigkeitsverteilungen können mit den ebenfalls gemessenen Gasgehalten multipliziert und über dem Querschnitt integriert werden. Dadurch erhält man den Gesamtvolumenstrom der Gasphase. Tests an einer mit Wasser-Luft-Gemisch betriebenen Versuchsschleife zeigen die Funktionsfähigkeit dieses Verfahrens. ]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:8918-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Popov, I.]]></dc:creator>
<dc:creator><![CDATA[Gemming, S.]]></dc:creator>
<dc:creator><![CDATA[Seifert, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-8918-1</dc:identifier>
<dc:title><![CDATA[Structural and Electronic Properties of a Mo6S8 Cluster deposited on a Au(111) Surface]]></dc:title>
<dc:source><![CDATA[Physical Review B 75(2007), 245436]]></dc:source>
<dc:date>2007</dc:date>
<dc:description><![CDATA[Atomic and electronic properties of the Mo6S8 cluster are investigated using DFT band structure calculations with pseudopotentials and a plane-wave basis set. The calculations showed that these clusters can be well bound on the surface in a potential well with degenerate local energy minima, despite a negligible net electron transfer between the two subsystems. The cluster may move freely inside this well on the surface. The cluster-surface binding is via S-Au bonds, with additional contributions of the Mo atom in the vicinity of the surface.]]></dc:description>
<dc:subject><![CDATA[adsorption]]></dc:subject>
<dc:subject><![CDATA[DFT]]></dc:subject>
<dc:subject><![CDATA[density-functional theory]]></dc:subject>
<dc:subject><![CDATA[cluster]]></dc:subject>
<dc:subject><![CDATA[metal surface]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:language>eng</dc:language>
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<header>
<identifier>HZDR:PUBLDB:1352-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Baraniak, L.]]></dc:creator>
<dc:creator><![CDATA[Jelen, K.]]></dc:creator>
<dc:creator><![CDATA[Schiene, R.]]></dc:creator>
<dc:creator><![CDATA[Fischer, K.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1352-1</dc:identifier>
<dc:title><![CDATA[Influence of Mine Wood Degradation Products on the Adsorption of Uranium, Thorium, Iron and Lead on ore Mountain Rocks and Elbe Valley Sediments]]></dc:title>
<dc:source><![CDATA[Vortragstagung der Fachgruppe Nuklearchemie der Gesellschaft Deutscher Chemiker, Dresden 7.-9. September 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The influence of mine-wood leachates on the adsorption of U(VI), Th(IV), Fe(III) and Pb(II)   (1) on typical rocks and minerals of the mining sites in the German Erzgebirge and  (2) on sediments of the Königstein mine (Saxony) and its near field was studied under aerobic condition.

The wood was decomposed by reflux boiling of wood shavings with water.  The leachates were analysed for DOC, phenolic and saccharic compounds, molecular weight distribution and content of carboxylic and phenolic hydroxyl groups.  The adsorption experiments were carried out equilibrating the geomaterial with the aqueous phase in the presence of U(VI) and DOC for 4-6 weeks.  The uranium concentration ranged from 3.2 10-6 to 3.2 10-5 mol/L (0.76-7.62 mg/L) and the DOC content was 8.3-166 mg/L.  The distribution ratio (Rs [mL/g]) was determined by liquid scintillation counting of an added 234U tracer (10-40 Bq/sample) after distribution and a careful phase separation.

Uranium adsorption on rocks and minerals from the Erzgebirge: The adsorption from a DOC-free synthetic mine water takes mainly place on diabase and on calcite; about 80% of the uranium is bound on these minerals.  The influence of the wood degradation products and pine wood lignin increases the adsorption to 90-95 %.  Granite and basalt adsorb from DOC-free mine water 50-60% of the uranium.  In the presence of the wood leachate and lignin, the adsorption increases to about 80%.  The effect of the wood leachate and lignin is insignificant for gneiss. Very little uranium adsorbs on phyllite.  From all solutions practically no uranium is bound ( 2%).

Uranium adsorption on Königstein sediments:  It is evident that uranium is preferentially bound to sandstone (91-97%); especially with a high distribution ratio to the limonithe-rich turonian sandstone (142 mL/g). Even under the influence of the organic compounds the sorption ranges from 68 to 93%.  Wood leachate and lignin (2-4%) decrease the sorption. The adsorption o ...]]></dc:description>
<dc:subject><![CDATA[Uranium]]></dc:subject>
<dc:subject><![CDATA[Thorium]]></dc:subject>
<dc:subject><![CDATA[Iron]]></dc:subject>
<dc:subject><![CDATA[Lead]]></dc:subject>
<dc:subject><![CDATA[Adsorption]]></dc:subject>
<dc:subject><![CDATA[Distribution Ratio]]></dc:subject>
<dc:subject><![CDATA[Metamorphic Rocks]]></dc:subject>
<dc:subject><![CDATA[Phyllite]]></dc:subject>
<dc:subject><![CDATA[Granite]]></dc:subject>
<dc:subject><![CDATA[Basalt]]></dc:subject>
<dc:subject><![CDATA[Calcite]]></dc:subject>
<dc:subject><![CDATA[Gneiss]]></dc:subject>
<dc:subject><![CDATA[Diabase]]></dc:subject>
<dc:subject><![CDATA[Sediments]]></dc:subject>
<dc:subject><![CDATA[Sandstone]]></dc:subject>
<dc:subject><![CDATA[Claystone]]></dc:subject>
<dc:subject><![CDATA[Wood Degradation Products]]></dc:subject>
<dc:subject><![CDATA[Lignin]]></dc:subject>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:935-1</identifier>
<datestamp>2022-11-09</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Betzl, M.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-935-1</dc:identifier>
<dc:title><![CDATA[Alloying by High Dose Ion Implantation of Iron into Magnesium and Aluminium]]></dc:title>
<dc:source><![CDATA[Hyperfine Interactions 113 (1998) 391-401]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1023/A:1012648321780]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-935-1</dc:relation>
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<header>
<identifier>HZDR:PUBLDB:1354-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Wang, X.]]></dc:creator>
<dc:creator><![CDATA[Kolitsch, A.]]></dc:creator>
<dc:creator><![CDATA[Prokert, F.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1354-2</dc:identifier>
<dc:title><![CDATA[Ion Beam Assisted Deposition of AlN Monolithic Films and Al/AlN Multilayers: a Comparative Study]]></dc:title>
<dc:source><![CDATA[SMMIB 97, Gatlinburg, TE, USA, Sept. 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1354-1</identifier>
<datestamp>2023-05-04</datestamp>
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<dc:source><![CDATA[Physical Review C, Volume 56, Number 2, S.1031-1043]]></dc:source>
<dc:date>1997</dc:date>
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Using a phenomenological schematic model of multipole giant resonances we consider the effects of overlapping of their doorway components. The conccpt of the partial widths of a giant resonance becomes ambiguous when the escape widths get comparable with the spacings between the components. In such a case, the partial widths determined in terms of the K- and S-matrices differ from each othcr. The mixing of the doorway components due to the interaction via the common decay channels influences significantly their multipole strengths, widths and positions in energy.]]></dc:description>
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Using a phenomenological schematic model of multipole giant resonances we consider the effects of overlapping of their doorway components. The conccpt of the partial widths of a giant resonance becomes ambiguous when the escape widths get comparable with the spacings between the components. In such a case, the partial widths determined in terms of the K- and S-matrices differ from each othcr. The mixing of the doorway components due to the interaction via the common decay channels influences significantly their multipole strengths, widths and positions in energy.]]></dc:description>
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ion beam (FIB) have been measured. The experiments were performed with
Ga+ ions of 35 keV at a current of 3 nA and variable chopping frequency
up to 10 MHz. The acoustic signals were detected by means of a piezoelectric
sensor with integrated pre-amplifier. A dependence on the sample material
was found. The results suggest that the ion-acoustic effect can be utilized
for imaging and material characterization of surface and subsurface structures
in FIB systems.]]></dc:description>
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<dc:title><![CDATA[Blue photoluminescence from high-dose Si+ - and Ge+ - implanted silicon dioxide layers]]></dc:title>
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<identifier>HZDR:PUBLDB:1405-7</identifier>
<datestamp>2025-02-17</datestamp>
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<dc:title><![CDATA[Positron emission tomography for quality assurance of cancer therapy with light ion beams.]]></dc:title>
<dc:source><![CDATA[Abstracts of the Int. Nuclear Physics Conference, Paris, 24-28 Aug(1998)823]]></dc:source>
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<identifier>HZDR:PUBLDB:1407-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
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<dc:title><![CDATA[Anwendung des Master-Curve-Konzeptes zur bruchmechanischen Charakterisierung von Reaktordruckbehälterstählen]]></dc:title>
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<identifier>HZDR:PUBLDB:1407-7</identifier>
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<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
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<dc:title><![CDATA[Anwendung des Master-Curve-Konzeptes zur bruchmechanischen Charakterisierung von Reaktordruckbehälterstählen]]></dc:title>
<dc:source><![CDATA[Deutscher Verband für Materialprüfung und -forschung e.V., Tagung Werkstoffprüfung 1998, Bad Nauheim, Dez. 98, Tagungsberichte Werkstoffprüfung 1998", S. 353]]></dc:source>
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<identifier>HZDR:PUBLDB:1745-1</identifier>
<datestamp>2023-05-05</datestamp>
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<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Nitzsche, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1745-1</dc:identifier>
<dc:title><![CDATA[SANS Investigations of the Irradiation-Caused Structural Damages in VVER-440-Type Reactor Pressure Vessel Steels]]></dc:title>
<dc:source><![CDATA[1st European Conference on Neutron Scattering, Interlaken (Switzerland), Oct. 1996]]></dc:source>
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<dc:description><![CDATA[Small-angle neutron scattering (SANS) experiments were performed at KWS2 facility of the KFA Jülich for investigating the defect structures, which are produced by neutron irradiation in Russian Cr-Mo-V alloyed reactor pressure vessel steel. Irradiation and post-irradiation annealing considerably change both SANS intensity and its course in the Guinier plot, which was analysed by the Glatter method. As a rule, bimodal size distribution functions were found with a first maximum at a radius of 1-2 nm and a second maximum at 6-8 nm. Irradiation increases the first maximum annealing reduces it. 
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:559-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Nitzsche, P.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-559-1</dc:identifier>
<dc:title><![CDATA[Investigation of the Development of Irradiation - Induced Precipitates in VVER-440-Type Reactor Pressure Vessel Steels and Weld Metals During Irradiation and Annealing]]></dc:title>
<dc:source><![CDATA[18th International Symposium "Effects of Radiation in Materials", Hyannis (USA), June 25 - 27, 1996, ASTM STP 1325]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The development of irradiation-induced precipitates in VVER-440 type reactor pressure vessel steels 15Kh2MFA and weld metals SV-10KhMFT during irradiation and post-irradiation annealing is studied by small angle neutron and X-ray scattering. The kinetic conditions for the precipitation of particles, which already exist in the unirradiated state, seem to be improved at temperatures of about 270 °C due to the irradiation. The size distribution of the irradiation-induced precipitates depends on the copper content and differs between weld and base metal. A strong correlation between the formation of irradiation-induced precipitates and the irradiation hardening is found. The hardness nearly linearly depends on the number of these precipitates. 
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1208-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Moormann, R.]]></dc:creator>
<dc:creator><![CDATA[Alberici, S.]]></dc:creator>
<dc:creator><![CDATA[Hinssen, H.-K.]]></dc:creator>
<dc:creator><![CDATA[Krüssenberg, A.-K.]]></dc:creator>
<dc:creator><![CDATA[Wu, C. H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1208-1</dc:identifier>
<dc:title><![CDATA[Oxidation Behaviour of Carbon-Based Materials Used for High-Temperature Gas-Cooled Reactors and Fusion Reactors]]></dc:title>
<dc:source><![CDATA[9th CIMTEC (International Conference on Modern Materials & Technologies)
14.-19.06.1998, Florence, Italy]]></dc:source>
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<dc:description><![CDATA[Kinetic formula describing oxidation of several innovative Cbased HTR and fusion reactor materials in oxygen, steam and CO2 are reported for use in computer codes for safety analyses (air/steam ingress accidents). Most data deal with oxidation regime II (in-pore diffusion control) but some information on regime I and III are added, too. The data situation on oxidation of pure graphites and CFCs in O2 and H2O seems to be sufficient but for mixed materials, particularly Si/C composites to be used in fusion reactors, additional experiments are necessary.]]></dc:description>
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<dc:title><![CDATA[Oxidation Behaviour of Carbon-Based Materials Used for High-Temperature Gas-Cooled Reactors and Fusion Reactors]]></dc:title>
<dc:source><![CDATA[Advances in Science and Technology, Vol 24 (1999) 331-8]]></dc:source>
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<dc:description><![CDATA[Kinetic formula describing oxidation of several innovative Cbased HTR and fusion reactor materials in oxygen, steam and CO2 are reported for use in computer codes for safety analyses (air/steam ingress accidents). Most data deal with oxidation regime II (in-pore diffusion control) but some information on regime I and III are added, too. The data situation on oxidation of pure graphites and CFCs in O2 and H2O seems to be sufficient but for mixed materials, particularly Si/C composites to be used in fusion reactors, additional experiments are necessary.]]></dc:description>
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<dc:title><![CDATA[Theoretische Grundlagen der Ionenstrahlsynthese: Computersimulationen auf atomarer Ebene]]></dc:title>
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<dc:title><![CDATA[Thermal Dilepton Signal Versus Dileptons from Open Charm and Bottom Decays in Heavy-Ion Collisions]]></dc:title>
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<dc:source><![CDATA[Physical Review C, Vol. 57 (1998) pp. 3276-3283]]></dc:source>
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<dc:creator><![CDATA[Rath, H. J.]]></dc:creator>
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<dc:title><![CDATA[Thermocapillary bubble migration at high Reynolds and Marangoni numbers under low gravity]]></dc:title>
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<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Beyer, M.]]></dc:creator>
<dc:creator><![CDATA[Lifante, C.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14280-1</dc:identifier>
<dc:title><![CDATA[Steam bubble condensation in polydispersed flow - Experiments and CFD simulations]]></dc:title>
<dc:source><![CDATA[7th International Conference on Multiphase Flow, ICMF 2010, 30.05.-04.06.2010, Tampa, USA]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Many activities were done in the last years to improve the modeling of adiabatic bubbly flows in the frame of CFD. In this case models for momentum transfer between the phases are most important. Usually they are expressed as so-called bubble forces. Experimental investigation as well as Direct Numerical Simulations (DNS) showed, that these bubble forces strongly depend on the bubble size. In addition to the well known drag force also virtual mass, lift, turbulent dispersion and wall forces have to be considered. The lift force even changes its sign in dependence of the bubble size (Tomiyama, 1989). In consequence large bubbles are pushed to the opposite direction than small bubbles if a gradient of the liquid velocity perpendicular to the relative bubble velocity exists (Lucas et al. 2001, Prasser et al. 2007). To simulate the separation of small and large bubbles more than one momentum equation is required (Krepper et al. 2005). For this reason recently so-called Inhomogeneous-MUSIG (MUlti SIze Group) model was implemented into the ANSYS-CFX code (Frank et al. 2008, Krepper et al. 2008). It allows the consideration of a number of bubble classes independently for the mass balance (for a proper modeling of bubble coalescence and breakup a large number of bubble groups is required) and for the momentum balance (only very few classes can be considered due to the high computational effort, criteria for the classification can be derived from the dependency of the bubble forces on the bubble size, e.g. the change of the sign of the lift force). In the presently implemented version of the Inhomogeneous MUSIG model only transfers between the bubble classes due to bubble coalescence and breakup can be modeled. In case of flows with phase transfer additional transfers between the single classes and the liquid and transfers between bubble classes caused by growth or shrinking of bubbles have to be considered. The equations for the extension of the MUSIG models are derived in Section 2. of this paper (see also Lucas et al. 2009). They were recently implemented into the CFX code and are presently verified (see Section 4).]]></dc:description>
<dc:subject><![CDATA[CFD-simulations]]></dc:subject>
<dc:subject><![CDATA[population balance models]]></dc:subject>
<dc:subject><![CDATA[heat and mass transfer]]></dc:subject>
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<dc:title><![CDATA[EXAFS Investigations on the Interaction of Uranium(VI) with Natural and Synthetic Humic Acids]]></dc:title>
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<dc:title><![CDATA[Structural Analysis of Uranium(VI) Complexes by X-ray Absorption Spectroscopy]]></dc:title>
<dc:source><![CDATA[Surface Investigations 13, 557 (1998)]]></dc:source>
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<dc:title><![CDATA[Structural Analysis of Uranium(VI) Complexes by X-ray Absorption Spectroscopy]]></dc:title>
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<dc:title><![CDATA[Determination of relative arsenite and arsenate Concentrations in aqueous mixtures by XANES]]></dc:title>
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<dc:title><![CDATA[Direktmessung alpha-aktiver Nuklide]]></dc:title>
<dc:source><![CDATA[6. Sitzg. Arbeitskreis "Freimessg. v. Anlageteilen u. Bauschutt aus dem Abbau kerntechn. Anlagen des Brennstoffkreislaufes" Rossendorf, 6.11.96]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-808-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:814-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-814-1</dc:identifier>
<dc:title><![CDATA[In-situ Investigation of Ion Driff Processes in Glass ...]]></dc:title>
<dc:source><![CDATA[EUROSENSORS XI, Warshaw, 21.-24.9.1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-814-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:815-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brenscheidt, F.]]></dc:creator>
<dc:creator><![CDATA[Oswald, S.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-815-1</dc:identifier>
<dc:title><![CDATA[Wear mechanisms in titanium implanted silicon nitride ceramics]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 129 (1997) 483-486]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The wear of silicon nitride ceramics is reduced by titanium
implantation albeit the friction coefficient is slightly increased. X-ray
excited photoelectron spectroscopy indicates that silicon oxide is formed
in the wear track while possible lubricating titanium oxides are not found.
Therefore we attribute the observed wear reduction to the amorphization
of the surface as proved by transmission electron microscopy.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:820-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Kolomeitsev, E. E.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-820-1</dc:identifier>
<dc:title><![CDATA[Kaonen in Kernmaterie]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-167]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-820-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:822-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:creator><![CDATA[Seifert, S.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-822-1</dc:identifier>
<dc:title><![CDATA[Institute of Bioinorganic and Radiopharmaceutical Chemistry; Annual Report 1996]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-165]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-822-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:823-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Biegansky, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-823-1</dc:identifier>
<dc:title><![CDATA[Ladungsverteilungen und kollektives Verhalten in 197Au + 197Au - Stößen bei Eprog = 150 bis 1000 A MeV]]></dc:title>
<dc:source><![CDATA[Dissertation]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-823-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1236-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Dumaz, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1236-1</dc:identifier>
<dc:title><![CDATA[Post Test Calculations of NOKO Experiments within the Framework of a European Research Program]]></dc:title>
<dc:source><![CDATA[Kerntechnik Vol. 63, No. 3, Mai 1998, S. 113-119, ISSN 0932-3902]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[In the frame of a European program (EU BWR R&D Cluster), six
test series with an emergency condenser test bundle were
performed in 1996. Within the Physics and Thermalhydraulics
Complementary Action to the BWR Cluster (BWR/CA) the German
Forschungszentrum Rossendorf (FZR) e.V. and the French Com
missariat a l'Energie Atomique (CEA/DRN) have calculated 9
tests and an additional blind test of NOKO bundle experiments
in 1997. These post test calculations were carried out using
the ATHLET computer code (FZR) and the CATHARE2 computer code
(CEA DRN).
The comparison of the experimental and computational results
(e.g. for mass flows, temperatures, capacities, pressure
drops) show an excellent agreement. Despite the good
prediction of global parameters, a variation of local
parameters (e.g. film velocity, void fraction, heat flux) can
be observed. This can be explained by the significant effect
of the tube wall conduction in controlling the heat transfer.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1236-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:963-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Hicken, E. F.]]></dc:creator>
<dc:creator><![CDATA[Jaegers, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-963-1</dc:identifier>
<dc:title><![CDATA[Test and Calculation of the Emergency Condenser of the SWR 1000]]></dc:title>
<dc:source><![CDATA[Post-SMIRT 14 International Seminar "Passive Safety Features in Nuclear Installations", S B2.27-B2.35, 25.-27. August 1997, Pisa, Italien]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The Siemens AG is developing the new innovative boiling water reactor
concept SWR1000. New features are the passive safety systems (e.g.
emergency condensers, building condensers, passive pressure pulse
transmitters, gravitydriven core flooding lines).

For the experimental investigation of the emergency condenser effectiveness,
the NOKO test facility has been constructed at the Forschungszentrum Jülich
in cooperation with Siemens. This test facility has an operating pressure of
10 MPa and a maximum power of 4 MW for steam production. The emergency
condenser bundle consists of eight tubes and is fabricated with planned
geometry and material of the SWR1000. In more than 200 experiments, the
emergency condenser capacity was tested as a function of pressure, water
level and concentration of noncondensables in the pressure vessel as well
of pressure, water level and temperature in the condenser.

Post test calculations of NOKO experiments were performed with an improved
version of ATHLET. To calculate the heat transfer coefficients during
condensation in horizontal tubes the module KONWAR has been developed
and implemented in ATHLET. KONWAR is based on the flow regime map of
Tandon and includes several semiempirical correlations for the determination
of the heat transfer coefficients. The comparison between calculations and
experiments shows a good agreement.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-963-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:963-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Hicken, E. F.]]></dc:creator>
<dc:creator><![CDATA[Jaegers, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-963-7</dc:identifier>
<dc:title><![CDATA[Test and Calculation of the Emergency Condenser of the SWR 1000]]></dc:title>
<dc:source><![CDATA[Post-SMIRT 14 International Seminar "Passive Safety Features in Nuclear Installations", S B2.27-B2.35, 25.-27. August 1997, Pisa, Italien]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The Siemens AG is developing the new innovative boiling water reactor
concept SWR1000. New features are the passive safety systems (e.g.
emergency condensers, building condensers, passive pressure pulse
transmitters, gravitydriven core flooding lines).

For the experimental investigation of the emergency condenser effectiveness,
the NOKO test facility has been constructed at the Forschungszentrum Jülich
in cooperation with Siemens. This test facility has an operating pressure of
10 MPa and a maximum power of 4 MW for steam production. The emergency
condenser bundle consists of eight tubes and is fabricated with planned
geometry and material of the SWR1000. In more than 200 experiments, the
emergency condenser capacity was tested as a function of pressure, water
level and concentration of noncondensables in the pressure vessel as well
of pressure, water level and temperature in the condenser.

Post test calculations of NOKO experiments were performed with an improved
version of ATHLET. To calculate the heat transfer coefficients during
condensation in horizontal tubes the module KONWAR has been developed
and implemented in ATHLET. KONWAR is based on the flow regime map of
Tandon and includes several semiempirical correlations for the determination
of the heat transfer coefficients. The comparison between calculations and
experiments shows a good agreement.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:968-1</identifier>
<datestamp>2023-04-28</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krüssenberg, A.-K.]]></dc:creator>
<dc:creator><![CDATA[Moormann, R.]]></dc:creator>
<dc:creator><![CDATA[Hinssen, H.-K.]]></dc:creator>
<dc:creator><![CDATA[Hofmann, M.]]></dc:creator>
<dc:creator><![CDATA[Wu, C. H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-968-1</dc:identifier>
<dc:title><![CDATA[Investigation of Oxidation Resistance of Carbon Based First-Wall Liner Material Aerolor AO5]]></dc:title>
<dc:source><![CDATA[Journal of Nuclear Materials 258-263 (1998) 770-776]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Minimizing the consequences of loss of vacuum and loss of coolant into vacuum accidents with respect to fusion reactor design requires the choice of materials as oxidation resistant as possible. In continuation to the testing of carbon candidate materials under oxidizing conditions (oxygen and steam) in collaboration with NET the carbon compound Aerolor AO5 of Carbone Lorraine has been examined in detail in the test facilities INDEX 2 and SPALEX at Forschungszentrum Jülich. The parameters for these oxidation experiments in the in-pore diffusion controlled regime are temperature (from 973 K up to 1173 K for oxygen, from 1173 K up to 1423 K for steam) and reaction gas concentration (1 vol.-% - 20 vol.% oxygen in argon, 5 vol.% - 100 vol.% steam in argon). The deducted equations for the primary oxidation reactions consider the dependence of the reaction rate on temperature, partial pressure and burn-off of the material.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0022-3115(98)00256-6]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-968-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:968-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krüssenberg, A.-K.]]></dc:creator>
<dc:creator><![CDATA[Moormann, R.]]></dc:creator>
<dc:creator><![CDATA[Hinssen, H.-K.]]></dc:creator>
<dc:creator><![CDATA[Hofmann, M.]]></dc:creator>
<dc:creator><![CDATA[Wu, C. H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-968-2</dc:identifier>
<dc:title><![CDATA[Investigation of Oxidation Resistance of Carbon Based First-Wall Liner Material Aerolor AO5]]></dc:title>
<dc:source><![CDATA[Posterbeitrag während 8th International Conference Fusion Reactor Materials, 26.10 - 31.10.1997, Sendai, Japan]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Minimizing the consequences of loss of vacuum and loss of coolant into vacuum accidents with respect to fusion reactor design requires the choice of materials as oxidation resistant as possible. In continuation to the testing of carbon candidate materials under oxidizing conditions (oxygen and steam) in collaboration with NET the carbon compound Aerolor AO5 of Carbone Lorraine has been examined in detail in the test facilities INDEX 2 and SPALEX at Forschungszentrum Jülich. The parameters for these oxidation experiments in the in-pore diffusion controlled regime are temperature (from 973 K up to 1173 K for oxygen, from 1173 K up to 1423 K for steam) and reaction gas concentration (1 vol.-% - 20 vol.% oxygen in argon, 5 vol.% - 100 vol.% steam in argon). The deducted equations for the primary oxidation reactions consider the dependence of the reaction rate on temperature, partial pressure and burn-off of the material.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
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<dc:creator><![CDATA[Nikitin, A. N.]]></dc:creator>
<dc:creator><![CDATA[Sukhoparov, W. A.]]></dc:creator>
<dc:creator><![CDATA[Heinitz, J.]]></dc:creator>
<dc:creator><![CDATA[Walther, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-885-1</dc:identifier>
<dc:title><![CDATA[Investigations of texture formation in geomaterials by neutron diffraction with high pressure chambers]]></dc:title>
<dc:source><![CDATA[High Pressure Research 14 (1995) pp. 155-162]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:886-1</identifier>
<datestamp>2022-11-10</datestamp>
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<dc:creator><![CDATA[Nomura, K.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Ujihira, Y.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-886-1</dc:identifier>
<dc:title><![CDATA[CEMS study on magnetic structure of Fe-Si-Al films implanted with Al and N ions]]></dc:title>
<dc:source><![CDATA[ICAME '95, Conference Proceedings Vol. 50, Ed.: I. Ortalli, SIF Bologna, 1996, pp. 703-706]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:887-1</identifier>
<datestamp>2022-11-10</datestamp>
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</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Fröb, H.]]></dc:creator>
<dc:creator><![CDATA[Böhme, T.]]></dc:creator>
<dc:creator><![CDATA[Leo, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-887-1</dc:identifier>
<dc:title><![CDATA[Room-temperature, sorth-wavelength (400-500 nm) photoluminescence from silicon-implanted silicon dioxide films]]></dc:title>
<dc:source><![CDATA[Applied Physics Letters 68 (1996) 17 pp. 2410-2412]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:888-1</identifier>
<datestamp>2022-11-10</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pham, T.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:creator><![CDATA[Hüller, J.]]></dc:creator>
<dc:creator><![CDATA[Albrecht, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-888-1</dc:identifier>
<dc:title><![CDATA[Coimplantation of silver and halogens in thin SiO<SUB>2</SUB> films]]></dc:title>
<dc:source><![CDATA[Journal of Applied Physics 79 (1996) 8 pp. 3915-3920]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:889-1</identifier>
<datestamp>2022-11-10</datestamp>
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<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pham, T.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:creator><![CDATA[Hüller, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-889-1</dc:identifier>
<dc:title><![CDATA[Ion beam sensitized SiO<SUB>2</SUB> surface for halide ions]]></dc:title>
<dc:source><![CDATA[Analytica Chimica Acta 320 (1996) pp. 289-291]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/0003-2670(95)00537-4]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-889-1</dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:891-1</identifier>
<datestamp>2022-11-10</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Keudell, A.]]></dc:creator>
<dc:creator><![CDATA[Jacob, W.]]></dc:creator>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-891-1</dc:identifier>
<dc:title><![CDATA[Role of hydrogen ions in plasma-enhanced chemical vapor deposition of hydrocarbon films, investigated by in situ ellipsometry]]></dc:title>
<dc:source><![CDATA[Applied Physics Letters 66 (1995) 11 pp. 1322-1324]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1063/1.113229]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-891-1</dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:893-1</identifier>
<datestamp>2022-11-10</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Henke, D.]]></dc:creator>
<dc:creator><![CDATA[Tyrroff, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-893-1</dc:identifier>
<dc:title><![CDATA[Ion optical system for transport and deceleration of highly charged ions]]></dc:title>
<dc:source><![CDATA[Review of Scientific Instruments 67 (1996) 3 pp. 1070-1072]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1063/1.1146761]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-893-1</dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:542-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Albe, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-542-1</dc:identifier>
<dc:title><![CDATA[Theoretical study of boron nitride modifications at hydrostatic pressures]]></dc:title>
<dc:source><![CDATA[Physical Review B 55 (1997) 10 pp. 6203-6210]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[This paper presents a detailed study of boron nitrides
at hydrostatic pressures. Cohesive properties of zincblende (c-BN), wurtzite
(w-BN), hexagonal (h-BN), rhombohedral (r-BN) and rocksalt structure are
calculated by systematic optimization of unit cell parameters using total-energy
DFT techniques. With focus on the very rarely discussed layered modifications
the p - V equation of states are derived. It is confirmed taht the isothermal
bulk modulus of the sp2 bonded phases is more than ten times smaller in
comparison to the dense phases. Additionally the equilibrium line of c-BN
and h-BN in the phase p, T diagram is estimated. According to recent experimental
reports c-BN is predicted as stable modification at standard conditions.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
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<record>
<header>
<identifier>HZDR:PUBLDB:687-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Albe, K.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-687-1</dc:identifier>
<dc:title><![CDATA[Computer Simulation and Boron Nitride]]></dc:title>
<dc:source><![CDATA[Rad. Eff. Def. Solids 142 (1997) 85]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[This paper presents computer simulation studies of boron
nitride using ab initio and empirical methods. Results of self-consistent
DFT-LDA calculations are shown, which were performed to characterize static
ground-state properties of the different BN modifications. With help of
these calculations the cubic phase is predicted as stable modification
under standard conditions. Furthermore an empirical interatomic potential
is introduced, which was parameterized by means of ab initio results and
allows a reliable description of structures and energies of Bn, Nm and
BnNm clusters and solid modifications. Finally, using this classical forcefield
a MD-simulation of N2 impact on a h-BN target is presented.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-687-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:14479-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Götz, C.]]></dc:creator>
<dc:creator><![CDATA[Geipel, G.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14479-1</dc:identifier>
<dc:title><![CDATA[The Influence of the temperature on the carbonate complexation of Uranium(VI) - a spectroscopic study]]></dc:title>
<dc:source><![CDATA[Journal of Radioanalytical and Nuclear Chemistry 287(2011)3, 961-969]]></dc:source>
<dc:date>2011</dc:date>
<dc:description><![CDATA[The interaction of uranium(VI) with carbonate ions was studied with absorption spectroscopy and time resolved laser induced fluorescence spectroscopy due to the importance of these complexes in environmental relevant waters. In the pH range from 2 to 11 the influence of the temperature on the spectra was studied to check changes in the abundances of several binding forms. It was found that several binding forms are predominant at different temperatures and pH values. This observation can be explained by speciation changes due to the dependence of chemical equilibria on the temperature. 
Furthermore photoluminescence spectra of aqueous solutions of uranyl carbonate complexes were observed at ambient temperatures for the first time and single component absorption spectra of the uranyl carbonate complexes UO2(CO3)34- and UO2(CO3)22- were derived.]]></dc:description>
<dc:subject><![CDATA[Uranium(VI)]]></dc:subject>
<dc:subject><![CDATA[carbonate complexation]]></dc:subject>
<dc:subject><![CDATA[absorption spectroscopy]]></dc:subject>
<dc:subject><![CDATA[time resolved laser induced fluorescence spectroscopy]]></dc:subject>
<dc:subject><![CDATA[temperature]]></dc:subject>
<dc:subject><![CDATA[chemical equilibrium]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1007/s10967-010-0854-4]]></dc:relation>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1372-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Lauckner, K.]]></dc:creator>
<dc:creator><![CDATA[Enghardt, W.]]></dc:creator>
<dc:creator><![CDATA[Hinz, R.]]></dc:creator>
<dc:creator><![CDATA[Pawelke, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1372-1</dc:identifier>
<dc:title><![CDATA[Fully 3D PET image reconstruction for a spatially-varying system response and very low counting statistics.]]></dc:title>
<dc:source><![CDATA[IEEE Medical Imaging Conference, November 8-14, 1998, Toronto, Canada
<br>
Book of Abstracts(1998)84]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[A dedicated PET-system has been integrated into the heavy ion tumour facility at the Gesellschaft für Schwerionenforschung (GSI) in  Darmstadt in order to monitor and control the applied dose distribution during the irradiation. The positron camera has strongly spatially-varying system behaviour due to its limited angle design and the presence of detector gaps. Furthermore, the expected counting statistics are limited by the doses applied per therapy fraction. 
A three-dimensional Maximum-Likelihood Estimator algorithm has been adapted to this imaging situation. Corrections for activity outside of the field of view, parallax errors, randoms as well as normalization factors have been implemented. The algorithm has been validated using <SUP>22</SUP>Na reference sources. Resolution, edge detectability, geometrical fidelity of size and position have been chosen as figures of merit. Results of the performance studies as well as an example of the algorithm's application to patient data are presented.]]></dc:description>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1372-1</dc:relation>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<dc:creator><![CDATA[Lauckner, K.]]></dc:creator>
<dc:creator><![CDATA[Enghardt, W.]]></dc:creator>
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<dc:title><![CDATA[Fully 3D PET image reconstruction for a spatially-varying system response and very low counting statistics.]]></dc:title>
<dc:source><![CDATA[IEEE Medical Imaging Conference, November 8-14, 1998, Toronto, Canada
<br>
Book of Abstracts(1998)84]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[A dedicated PET-system has been integrated into the heavy ion tumour facility at the Gesellschaft für Schwerionenforschung (GSI) in  Darmstadt in order to monitor and control the applied dose distribution during the irradiation. The positron camera has strongly spatially-varying system behaviour due to its limited angle design and the presence of detector gaps. Furthermore, the expected counting statistics are limited by the doses applied per therapy fraction. 
A three-dimensional Maximum-Likelihood Estimator algorithm has been adapted to this imaging situation. Corrections for activity outside of the field of view, parallax errors, randoms as well as normalization factors have been implemented. The algorithm has been validated using <SUP>22</SUP>Na reference sources. Resolution, edge detectability, geometrical fidelity of size and position have been chosen as figures of merit. Results of the performance studies as well as an example of the algorithm's application to patient data are presented.]]></dc:description>
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<dc:creator><![CDATA[Albe, K.]]></dc:creator>
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<dc:identifier>https://www.hzdr.de/publications/Publ-1259-1</dc:identifier>
<dc:title><![CDATA[Computersimulationen zu Struktur und Wachstum von Bornitrid]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-228 Dissertation TU Dresden; April 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Dünne Filme aus kubischem Bornitrid (<I>c</I>-BN) sind aufgrund ihrer herausragenden thermomechanischen, chemischen und elektronischen Eigenschaften von besonderem Interesse für die Materialforschung. Bornitrid in der kubischen Phase ist das nach Diamant härteste bekannte Material. Anders als Kohlenstoff verhält es sich gegenüber ferrithaltigen Metallen chemisch inert und zeigt auch bei hohen Temperaturen eine vergleichsweise geringere Oxidationsneigung. Wegen seiner hohen thermischen Stabilität und der Möglichkeit, dünne Schichten bei niedrigen Temperaturen zu synthetisieren, ist Bornitrid&nbsp; als&nbsp; <I>Hard-Coating</I>-Material für Werkzeuge besonders geeignet. Mögliche Anwendungen für mikroelelektronische Hochleistungsbauelemente ergeben sich aus der hohen Wärmeleitfähigkeit und der weiten Bandlücke (E<SUB>g</SUB> ~ 6 eV). Bornitrid kann mit Beryllium und Silizium n- bzw. p-Typ dotiert werden und läßt sich mit einer Oxidschicht passivieren. Die optische Transparenz im sichtbaren und Infrarotbereich macht das Material zudem für die Oberflächenvergütung optischer Bauelemente geeignet. ...]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Albe, K.]]></dc:creator>
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<dc:title><![CDATA[Computersimulationen zu Struktur und Wachstum von Bornitrid]]></dc:title>
<dc:source><![CDATA[Workshop "Molekulare Dynamik" des SFB 438 der Universität Augsburg, Herrsching, April 24, 1998 (invited lecture)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Dünne Filme aus kubischem Bornitrid (<I>c</I>-BN) sind aufgrund ihrer herausragenden thermomechanischen, chemischen und elektronischen Eigenschaften von besonderem Interesse für die Materialforschung. Bornitrid in der kubischen Phase ist das nach Diamant härteste bekannte Material. Anders als Kohlenstoff verhält es sich gegenüber ferrithaltigen Metallen chemisch inert und zeigt auch bei hohen Temperaturen eine vergleichsweise geringere Oxidationsneigung. Wegen seiner hohen thermischen Stabilität und der Möglichkeit, dünne Schichten bei niedrigen Temperaturen zu synthetisieren, ist Bornitrid&nbsp; als&nbsp; <I>Hard-Coating</I>-Material für Werkzeuge besonders geeignet. Mögliche Anwendungen für mikroelelektronische Hochleistungsbauelemente ergeben sich aus der hohen Wärmeleitfähigkeit und der weiten Bandlücke (E<SUB>g</SUB> ~ 6 eV). Bornitrid kann mit Beryllium und Silizium n- bzw. p-Typ dotiert werden und läßt sich mit einer Oxidschicht passivieren. Die optische Transparenz im sichtbaren und Infrarotbereich macht das Material zudem für die Oberflächenvergütung optischer Bauelemente geeignet. ...]]></dc:description>
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<dc:creator><![CDATA[Kuhn, N.]]></dc:creator>
<dc:creator><![CDATA[Kotowski, H.]]></dc:creator>
<dc:creator><![CDATA[Maichle-Mößmer, C.]]></dc:creator>
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<dc:title><![CDATA[Synthese und Kristallstruktur von [Fe(MeCN)<SUB>6</SUB>][Fe<SUB>2</SUB>OCl<SUB>6</SUB>]]]></dc:title>
<dc:source><![CDATA[Zeitschrift für anorganische und allgemeine Chemie 624 (1998) 1653-1656]]></dc:source>
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<dc:creator><![CDATA[Repp, T.]]></dc:creator>
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<dc:title><![CDATA[Fluiddynamic Waterhammer Simulations with Consideration of Fluid-Structure Interaction]]></dc:title>
<dc:source><![CDATA[Sammelband Workshop Kompetenzerhalt Kerntechnik, Jahrestagung Kerntechnik, 18.-21. Mai 1999, Karlsruhe; Haag, G. (Ed.), 2000]]></dc:source>
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<identifier>HZDR:PUBLDB:896-1</identifier>
<datestamp>2022-11-10</datestamp>
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<dc:creator><![CDATA[Friedlein, R.]]></dc:creator>
<dc:creator><![CDATA[Tyrroff, H.]]></dc:creator>
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<dc:creator><![CDATA[Zippe, C.]]></dc:creator>
<dc:creator><![CDATA[Zschornack, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-896-1</dc:identifier>
<dc:title><![CDATA[Hot and warm electron energy distribution at different electron cyclotron resonance ion source operation regimes]]></dc:title>
<dc:source><![CDATA[Review of Scientific Instruments 67 (1996) 3 pp. 1322-1324]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Friedlein, R.]]></dc:creator>
<dc:creator><![CDATA[Herpich, S.]]></dc:creator>
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<dc:title><![CDATA[Experimental study of the hot and warm electron populations in an electron cyclotron resonance argon-oxygen-hydrogen plasma]]></dc:title>
<dc:source><![CDATA[Physics of Plasmas 2 (1995) 6 pp. 2138-2140]]></dc:source>
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<dc:creator><![CDATA[Friedlein, R.]]></dc:creator>
<dc:creator><![CDATA[Küchler, D.]]></dc:creator>
<dc:creator><![CDATA[Zippe, C.]]></dc:creator>
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<dc:creator><![CDATA[Tyrroff, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-898-1</dc:identifier>
<dc:title><![CDATA[Energy dispersive X-ray spectroscopy for ECR plasma diagnostics]]></dc:title>
<dc:source><![CDATA[Hyperfine Interactions 99 (1996) pp. 225-234]]></dc:source>
<dc:date>1996</dc:date>
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<identifier>HZDR:PUBLDB:899-1</identifier>
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<dc:creator><![CDATA[Friedlein, R.]]></dc:creator>
<dc:creator><![CDATA[Herpich, S.]]></dc:creator>
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<dc:creator><![CDATA[Tyrroff, H.]]></dc:creator>
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<dc:creator><![CDATA[Zippe, C.]]></dc:creator>
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<dc:identifier>https://www.hzdr.de/publications/Publ-899-1</dc:identifier>
<dc:title><![CDATA[X-ray spectroscopy on ECR plasmas]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 98 (1995) pp. 585-588]]></dc:source>
<dc:date>1995</dc:date>
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<identifier>HZDR:PUBLDB:900-1</identifier>
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<dc:creator><![CDATA[Grunwald, G.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-900-1</dc:identifier>
<dc:title><![CDATA[Theoretische Untersuchungen zur Fluid-Struktur-Wechselwirkung in zweiphasig durchströmten Schwingungsmodellen]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-178 April 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Kurzfassung
Ausgehend von den Grundgleichungen für Kontinuität, Impuls und Energie einer Zweiphasenströmung werden Beziehungen für ein Ersatzfluid des Gas- Flüssigkeits- Gemisches mit orts- und zeitabhängiger Dichte und Geschwindigkeit aufgestellt und anhand eines Siedemodells geprüft. Es folgen Anwendungen auf ein 1D- und ein 2D- Schwingungsmodell (Pendel im Zweiphasenstrom) unter Berücksichtigung der Fluid-Struktur- Wechselwirkung und die Berechnung von Eigenfrequenzen und Dämpfungen.]]></dc:description>
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We evaluate corrected meson fields in the region 300 <= <I>M</I> <= 600 of constituent quark masses <I>M</I> and compare them with the uncorrected fields. We study the effect of the corrections on various expectation values of nuclear observables such as the root-mean square radius, the axial-vector coupling constant, magnetic moments and the delta-nucleon mass splitting.]]></dc:description>
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<dc:identifier>https://www.hzdr.de/publications/Publ-490-1</dc:identifier>
<dc:title><![CDATA[A 100 kV 10 A high-voltage pulse generator for plasma immersion ion implantation]]></dc:title>
<dc:source><![CDATA[Review of Scientific Instruments 67 (1996) 7 pp. 2621-2625]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The design of a high voltage pulsing system for a plasma immersion ion implantation (PIII)
facility is presented. A list of requirements, which have to be fulfilled by a high voltage pulse
generator to get best results and a optimum operation of the PIII system, is given. A simple
electrical model of the plasma is presented which describes the plasma as a capacitive-resistive
load. The model parameters are determined to fit experimental results. The requirements for the
pulse generator can be fulfilled well using a pulse generator design which employs a hard tube
switch. A pulse generator design is presented which is especially optimized for PIII systems.
Especially the hard tube control is optimized for obtaining voltage rise times as short as possible.<p>

Comments or further questions to:  brutscher@fz-rossendorf.de]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-490-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:701-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barradas, N.]]></dc:creator>
<dc:creator><![CDATA[Maas, A. S. H.]]></dc:creator>
<dc:creator><![CDATA[Mändl, S.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-701-1</dc:identifier>
<dc:title><![CDATA[Short pulse plasma immersion ion implantation of oxygen into silicon: determination of the energy distribution]]></dc:title>
<dc:source><![CDATA[Surface & Coatings Technology 93 (1997) 238-241]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Plasma immersion ion implantation was used to implant
oxygen ions into silicon with applied voltage pulses of 40 kV and 2.5 ms
total lenght. Positive ions from the plasma O2+ and O+, with a continuous
energy distribution between 0 and 40 keV were implanted with nominal doses
between 2x1016 and 2x1017/cm2. The resulting oxygen depth profiles were
measured with elastic recoil detection using 13.4 MeV a particles. The
obtained depth profiles were simulated using a linear superposition of
single-energy profiles calculated with TRIM, in order to determine relevant
parameters of the accelerated ions. The energy distribution of the incident
ions is derived from the results obtained and compared with theoretical
models. The agreement found is very good. The plasma found to be composed
of 35(8)% O2+ and 65(8)% O+ ions. An Fe contamination in the plasma is
observed using Rutherford backscattering.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-701-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:701-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barradas, N.]]></dc:creator>
<dc:creator><![CDATA[Maas, A. S. H.]]></dc:creator>
<dc:creator><![CDATA[Mändl, S.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-701-2</dc:identifier>
<dc:title><![CDATA[Short pulse plasma immersion ion implantation of oxygen into silicon: determination of the energy distribution]]></dc:title>
<dc:source><![CDATA[3rd International Workshop on Plasma - Based Ion Implantation (PBII), Dresden, Germany, Sept. 16-18, 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Plasma immersion ion implantation was used to implant
oxygen ions into silicon with applied voltage pulses of 40 kV and 2.5 ms
total lenght. Positive ions from the plasma O2+ and O+, with a continuous
energy distribution between 0 and 40 keV were implanted with nominal doses
between 2x1016 and 2x1017/cm2. The resulting oxygen depth profiles were
measured with elastic recoil detection using 13.4 MeV a particles. The
obtained depth profiles were simulated using a linear superposition of
single-energy profiles calculated with TRIM, in order to determine relevant
parameters of the accelerated ions. The energy distribution of the incident
ions is derived from the results obtained and compared with theoretical
models. The agreement found is very good. The plasma found to be composed
of 35(8)% O2+ and 65(8)% O+ ions. An Fe contamination in the plasma is
observed using Rutherford backscattering.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-701-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:994-1</identifier>
<datestamp>2023-04-27</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barradas, N.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Betzl, M.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-994-1</dc:identifier>
<dc:title><![CDATA[Influence of the Ion Irradiation on the Properties of ß-FeSi<SUB>2</SUB> Layers Prepared by Ion Beam Assisted Deposition]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 127/128(1997) 316-320]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[ß-FeSi2 was produced by ion beam assisted deposition
(IBAD). The influence of the deposition parameters on the structure was
studied by Rutherford backscattering, X-ray diffraction, cross section
transmission electron microscopy, and scanning electron microscopy. The
samples grow in a columnar way with pin-holes and their surface is rough.
A soft IBAD process with low Ar energy (EAr = 200 eV) and low Ar ion to
Fe atom ratio (IAr/AFe = 0.16) improves the layer structure in comparison
to samples prepared without Ar irradiation. Less pin-holes are formed,
and the roughness shows a minimum. The roughness increases for larger EAr
and larger IAr/AFe. All samples are polycrystalline but with a pronounced
texture. The preferential orientation is also enhanced by the IBAD process.
The electrical properties of the layers were characterized by Hall effect
measurements and measurements of the I-V characteristics of simple diode
structures. The results are discussed in relation with the influence of
the ion beam.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0168-583X(96)00947-0]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-994-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:868-1</identifier>
<datestamp>2022-11-11</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kubátová, A.]]></dc:creator>
<dc:creator><![CDATA[Matucha, M.]]></dc:creator>
<dc:creator><![CDATA[Bubner, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-868-1</dc:identifier>
<dc:title><![CDATA[Application of <SUP>13</SUP>C-labelled polychlorinated biphenyl congener 153 as internal standard in the gas chromatogrophic-mass spectrometric analysis of polychlorinated biphenyls]]></dc:title>
<dc:source><![CDATA[Journal of Chromatography A 750 (1996) pp. 245-251]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/0021-9673(96)00282-8]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-868-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:678-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brenscheidt, F.]]></dc:creator>
<dc:creator><![CDATA[Mändl, S.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:creator><![CDATA[Fischer, W.]]></dc:creator>
<dc:creator><![CDATA[Herrmann, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-678-1</dc:identifier>
<dc:title><![CDATA[Tribological Properties of Silicon Nitride Ceramics Modified by Titanium and subsequent Oxygen Implantation]]></dc:title>
<dc:source><![CDATA[Surface & Coatings Technology 97 (1997) 675-679]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[A silicon nitride based ceramic was implanted with 150
keV titanium to a fluence of 1017 ions/cm2. Subsequently the samples were
implanted with oxygen using plasma immersion ion implantation (PIII) and
conventional beam-line implantation to stimulate the formation of lubricating
oxides in the surface. The wear is reduced for all implanted samples. The
friction coefficient is slightly higher than in the non-implanted case
for all implantation conditions investigated although oxide formation in
the wear track is suggested by detection of a relatively high amount of
oxygen in the wear track as indicated by energy-dispersive X-ray spectroscopy
(EDX). We discuss the possible mechanisms that lead to the observed tribological
behaviour.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-678-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1043-1</identifier>
<datestamp>2023-05-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brenscheidt, F.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1043-1</dc:identifier>
<dc:title><![CDATA[Annealing studies of chromium implanted silicon nitride ceramics]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 127/128 (1997) 677-680]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The effect of chromium implantation and subsequent annealing
on the hardness and wear behaviour of a silicon nitride-based ceramic is
investigated. Implantation energies were 200, 400, 1000 and 2000 keV, the
fluence was 1017 Cr+ ions cm-2 in all cases. The annealing temperatures
were 800 C, 1000 C and 1200 C. The phase composition was determined with
X-ray diffraction. Annealing at 800 C does not affect the crystal structure.
At 1000 C the -Si3N4-phase is formed for 1 and 2 MeV implantation energy.
At 1200 C, Cristobalite and Keiviite are formed at the lower implantation
energies; at higher energies -Si3N4 is formed. We discuss the phase formation
for the different implantation energies and annealing temperatures and
the relationship with the observed hardness and wear.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0168-583X(96)01154-8]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1043-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:702-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brutscher, J.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-702-2</dc:identifier>
<dc:title><![CDATA[Plasma immersion implantation using pulsed plasma with DC and pulsed high voltages]]></dc:title>
<dc:source><![CDATA[Surf. Coati. Technol. 93 (1997) 197]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[New experiments in plasma immersion ion implantation (PIII)
have been performed to explore the extended operation regimes available
with pulsed plasmas. A pulsed extraction voltage and a synchronized pulsed
plasma show a further reduction of thermal load, more stable operation
and improved implantation results. It was even possible to run PIII in
a mode with pulsed plasma and a DC voltage; in this way omitting the costly
high voltage modulating unit. Time resolved measurements of plasma density
and electron temperature have been made to get information about the plasma
buildup and decay process. In all cases a space charge sheath forms around
the sample where the ions are accelerated. The extension of the sheath
has been measured using time resolved Langmuir probe measurements. Iron
and aluminium samples were implanted with nitrogen using a DC plasma and
pulsed extraction voltage, pulsed plasma and pulsed extraction voltage,
and pulsed plasma and a DC extraction voltage. Analysis showed that in
all cases nitrogen could be implanted.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-702-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:702-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brutscher, J.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-702-1</dc:identifier>
<dc:title><![CDATA[Plasma immersion implantation using pulsed plasma with DC and pulsed high voltages]]></dc:title>
<dc:source><![CDATA[3rd International Workshop on Plasma - Based Ion Implantation (PBII), Dresden, Germany, Sept. 16-18, 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[New experiments in plasma immersion ion implantation (PIII)
have been performed to explore the extended operation regimes available
with pulsed plasmas. A pulsed extraction voltage and a synchronized pulsed
plasma show a further reduction of thermal load, more stable operation
and improved implantation results. It was even possible to run PIII in
a mode with pulsed plasma and a DC voltage; in this way omitting the costly
high voltage modulating unit. Time resolved measurements of plasma density
and electron temperature have been made to get information about the plasma
buildup and decay process. In all cases a space charge sheath forms around
the sample where the ions are accelerated. The extension of the sheath
has been measured using time resolved Langmuir probe measurements. Iron
and aluminium samples were implanted with nitrogen using a DC plasma and
pulsed extraction voltage, pulsed plasma and pulsed extraction voltage,
and pulsed plasma and a DC extraction voltage. Analysis showed that in
all cases nitrogen could be implanted.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-702-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1194-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bubner, M.]]></dc:creator>
<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:creator><![CDATA[Meyer, M.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1194-1</dc:identifier>
<dc:title><![CDATA[Isotopically Labelled Humic Acids for Heavy Metal Complexation]]></dc:title>
<dc:source><![CDATA[Vortrag, Joint European IIS Conference, 24.-26.Juni 1998, Bad Soden]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
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<dc:title><![CDATA[Kinetics of an expanding pion gas and low-mass dilepton emission]]></dc:title>
<dc:source><![CDATA[Int. Workshop on Nuclei + Nuclear Excitations, Hirschegg 1993, vom 3.11.93]]></dc:source>
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<dc:title><![CDATA[High-resolution spectroscopy of fission fragments, neutrons and gamma-rays]]></dc:title>
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<dc:creator><![CDATA[Thieme, M.]]></dc:creator>
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<dc:title><![CDATA[In-situ-Charakterisierung von Retentionsprozessen an Gesteinen mittels SWV]]></dc:title>
<dc:source><![CDATA[ELACH 1, Elektroanalyt. Tagung, Feldberg, 2.-4.6.1993]]></dc:source>
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<dc:creator><![CDATA[Geipel, G.]]></dc:creator>
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<dc:title><![CDATA[Untersuchungen zu natürlich-radioaktiven Inhaltsstoffen in Berghalden des Wismutbergbaus in Schlema]]></dc:title>
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<dc:creator><![CDATA[Hübener, S.]]></dc:creator>
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<dc:title><![CDATA[Modellexperimente zur gaschemischen Charakterisierung des Elementes 106]]></dc:title>
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<dc:creator><![CDATA[Winter, G.]]></dc:creator>
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<dc:title><![CDATA[A study of exicted states in 85 Kr and 86Kr: Evidence for neutron-core excitations in the N=50 nucleus 86Kr]]></dc:title>
<dc:source><![CDATA[Physical Review C, Vol. 48, No. 3, September 1993, p. 1010-1019]]></dc:source>
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<dc:creator><![CDATA[Bubner, M.]]></dc:creator>
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<dc:title><![CDATA[Ein Einstufenverfahren zur Synthese von [1,2 14c] Trichloressigsäure, ausgehend von [1,2 14c] Natriumacetat]]></dc:title>
<dc:source><![CDATA[3. Arbeitstagung des IIS, Bad Soden 1993]]></dc:source>
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<dc:creator><![CDATA[Kumpf, H.]]></dc:creator>
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<dc:title><![CDATA[Neutronic Problems of a Compact 14 MeV Plasma Neutron Source]]></dc:title>
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<dc:description><![CDATA[Neutronic problems connected with the design of a compact 14MeV neutron source for fusion material research based on a plasma mirror are treated. In particular it has been demonstrated, that further construction efforts are necessary to comply with the established radiation limits for the magnetic system. Further it ist not possible to raise the useful high energy flux by arranging reflectors. If one of the source areas of the machine is equipped with a moderator, a thermal neutron source with a flux of about 5 1014 n cm-2  s-1 can be achieved.]]></dc:description>
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<dc:creator><![CDATA[Funke, H.]]></dc:creator>
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<dc:title><![CDATA[Theoretische Probleme bei der Auswertung von Thermochromatographie-Experimenten]]></dc:title>
<dc:source><![CDATA[2. Workshop, Chemie schwerster Elemente, 25.-27.5.1993, Solothurn, Schweiz]]></dc:source>
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<dc:title><![CDATA[Ein modernes technisches System zur verbesserten betrieblichen Überwachung des ukrainischen Kernkraftwerks Saporoshje]]></dc:title>
<dc:source><![CDATA[Atomwirtschaft Atomtechnik 4 April 1998, S. 230-234]]></dc:source>
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<dc:description><![CDATA[Die zu Beginn der neunziger Jahre in der Ukraine praktizierte KKW-Überwachung ermöglichte der Aufsichtsbehörde nur einen unzureichenden Zugang zu Informationen über den jeweils aktuellen betrieblichen Sicherheitszustand. Im Zusammenhang mit den Ergebnissen von Sicherheitsanalysen für Kernkraftwerke war es daher erforderlich, die Möglichkeiten der betrieblichen Überwachung dieser KKW durch die ukrainische Behörde zu verbessern. Für das KKW Saporoshje wurde vom Forschungszentrum Rossendorf im Verbund mit dem TÜV Rheinland ein modernes Überwachungssystem als Pilotprojekt konzipiert, eingerichtet und Ende 1995 in den Probebetrieb überführt. Es ergänzt die vorhandenen betrieblichen Kontroll- und Überwachungseinrichtungen durch Einbeziehung moderner Informations- und Rechentechnik. Das System ermöglicht eine kontinuierliche Beobachtung des Zustandes der Anlage im Normalbetrieb und bei Betriebsstörungen bzw. Störfällen, so daß bei erkennbaren Abweichungen vom bestimmungsgemäßen Betrieb frühzeitig durch Anfrage und Anordnung darauf reagiert werden kann.]]></dc:description>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Wüst, F.]]></dc:creator>
<dc:creator><![CDATA[Scheller, D.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-999-1</dc:identifier>
<dc:title><![CDATA[Synthesis of Oxorhenium(V) Complexes Derived from 7-alpha-Functionalized Testosterone: First Rhenium-Containing Testosterone Derivatives]]></dc:title>
<dc:source><![CDATA[Eur. J. Inorg. Chem. 1998, 789-793]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1002/(SICI)1099-0682(199806)1998:6<789::AID-EJIC789>3.0.CO;2-Z]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-999-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:28460-2</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Matschiavelli, N.]]></dc:creator>
<dc:creator><![CDATA[Kluge, S.]]></dc:creator>
<dc:creator><![CDATA[Podlech, C.]]></dc:creator>
<dc:creator><![CDATA[Standhaft, D.]]></dc:creator>
<dc:creator><![CDATA[Grathoff, G.]]></dc:creator>
<dc:creator><![CDATA[Ikeda-Ohno, A.]]></dc:creator>
<dc:creator><![CDATA[Warr, L.]]></dc:creator>
<dc:creator><![CDATA[Chukharkina, A.]]></dc:creator>
<dc:creator><![CDATA[Arnold, T.]]></dc:creator>
<dc:creator><![CDATA[Cherkouk, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-28460-2</dc:identifier>
<dc:title><![CDATA[The year-long development of microorganisms in uncompacted Bavarian bentonite slurries at 30 °C and 60 °C]]></dc:title>
<dc:source><![CDATA[Environmental Science & Technology 53(2019)17, 10514-10524]]></dc:source>
<dc:date>2019</dc:date>
<dc:description><![CDATA[In the multi-barrier concept for the deep geological disposal of high-level radioactive waste (HLW), bentonite is proposed as a potential barrier and buffer material for sealing the space between the steel-canister containing the HLW and the surrounding host rock. In order to broaden the spectra of appropriate bentonites, we investigated the metabolic activity and diversity of naturally occurring microorganisms as well as their time-dependent evolution within the industrial B25 Bavarian bentonite under repository-relevant conditions. We conducted anaerobic microcosm-experiments containing the B25 bentonite and a synthetic Opalinus Clay pore water solution, which were incubated for one year at 30 °C and 60 °C. Metabolic activity was only stimulated by the addition of lactate, acetate or H2. The majority of lactate- and H2-containing microcosms at 30 °C were dominated by strictly anaerobic, sulfate-reducing and spore-forming microorganisms. The subsequent generation of hydrogen sulfide led to the formation of iron-sulfur precipitations. Independent from the availability of substrates, thermophilic bacteria dominated microcosms that were incubated at 60 °C. However, in the respective microcosms, no significant metabolic activity occurred and there was no change in the analyzed bio-geochemical parameters.]]></dc:description>
<dc:subject><![CDATA[high-level radioactive waste repository]]></dc:subject>
<dc:subject><![CDATA[sulfate-reduction]]></dc:subject>
<dc:subject><![CDATA[spores]]></dc:subject>
<dc:subject><![CDATA[thermophiles]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1021/acs.est.9b02670]]></dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:753-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Weishart, H.]]></dc:creator>
<dc:creator><![CDATA[Schöneich, J.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Renkewitz, S.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-753-1</dc:identifier>
<dc:title><![CDATA[Conductive Tungsten-Based Layers Synthesized by Ion Implantation into 6H-Silicon Carbide]]></dc:title>
<dc:source><![CDATA[Materials Research Society symposium proceeding 438 (1997) pp. 283-288 (MRS 1996 Fall Mtg)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[We studied high dose implantation of tungsten into 6H-silicon carbide in order to synthesize an electrically conductive layer. Implantation was performed at 200 keV with a dose of 1.2×10(17) W(+)cm(-2) at temperatures between 200°C and 400°C. The influence of implantation temperature on the distribution of W in SiC was investigated and compared to results obtained earlier from room temperature (RT) and 500°C implants. Rutherford backscattering spectrometry (RBS) was employed to study the structure and composition of the implanted layers. Implantation at temperatures between RT and 300°C did not influence the depth distribution of C, Si and W. The W depth profile shows a conventional Gaussian shape. Implanting at higher temperatures led to a more confined W rich layer in the SiC. This confinement is explained by Ostwald ripening which is enabled during implantation at temperatures above 300°C. The depth of the implantation induced damage decreases slightly with increasing implantation temperature, except for 400°C implantation. The amount of damage, however, is significantly reduced only for implantation at 500°C.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-753-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1000-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Zessin, J.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1000-1</dc:identifier>
<dc:title><![CDATA[<SUP>11</SUP>C-Labelling of Heterocyclic Aromatic Compounds in Ring Positions: Synthesis of 2-<SUP>11</SUP>C Indole]]></dc:title>
<dc:source><![CDATA[Journal of Labelled Compounds and Radiopharmaceuticals XLI, 669-676 (1998)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1000-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1001-1</identifier>
<datestamp>2023-04-27</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Michel, P.]]></dc:creator>
<dc:creator><![CDATA[Möller, K.]]></dc:creator>
<dc:creator><![CDATA[Naumann, B.]]></dc:creator>
<dc:creator><![CDATA[Naumann, L.]]></dc:creator>
<dc:creator><![CDATA[Schamlott, A.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, G.]]></dc:creator>
<dc:creator><![CDATA[Schülke, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1001-1</dc:identifier>
<dc:title><![CDATA[MARS: A Start Detector System for the Cosy Time-of-Flight Spectrometer TOF]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research A 408 (1998) 453-467]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0168-9002(98)00220-4]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1001-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:513-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Henkel, T.]]></dc:creator>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:creator><![CDATA[Kögler, R.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Seibt, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-513-1</dc:identifier>
<dc:title><![CDATA[The Temperature Dependence of the Ion Beam Induced Interfacial Amorphization in Silicon]]></dc:title>
<dc:source><![CDATA[Applied Physics Letters 68 (1996) 24 pp. 34253427]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The temperature dependence of the ion beam induced interfacial amorphization process (IBIIA) in silicon has been investigated at temperatures above 80 K using Rutherford Backscattering Spectroscopy/Channeling (RBS/C) and Cross-Sectional Transmission Electron Microscopy (XTEM). Three regimes are observed. Above temperatures of about 320 K there is strong temperature dependence of the IBIIA rate (thermal regime). At lower temperatures the rate moves towards a saturation value (transition regime). Below approximately 150 K IBIIA is nearly temperature independent (ballistic regime). This low temperataure regime can be explained by an athermal transport of point defects like in ballistic mixing processes.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-513-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:482-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Jäger, H.-U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-482-1</dc:identifier>
<dc:title><![CDATA[An explanation of trap-limited self-interstitial diffusion and enhanced boron clustering in boron doped silicon superlattices]]></dc:title>
<dc:source><![CDATA[Proceedings of the Fourth International Symposium on Process Physics and Modeling in Semiconductor Technology, edited by G. R. Srinivasan, C. S. Murthy and S. T. Dunham, pp. 210-215]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Boron doped crystalline superlattices grown by low-temperature molecular beam epitaxy have been used by Stolk et al.  to study the diffusion of self-interstitials I in Si. After 40 keV Si+ ion implantation and subsequent annealing, stationary interstitial profiles are found at 670 °C for periods t ~1 h, demonstrating that the penetration depth of interstitials is limited by trapping at hitherto unidentified impurities. In addition, the high
interstitial supersaturation causes B de-activation in the near-surface region. We show that both these effects, the trap-limited interstitial diffusion and the enhanced B clustering, can be explained, if the transient de-activation of boron is modeled by the first-order reaction I + B_s ->B_i. Boron atomic and electrical profiles as well as self-interstitial profiles are computed which are in good agreement with the experimental results.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-482-1</dc:relation>
<dc:audience>Researchers</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:482-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Jäger, H.-U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-482-7</dc:identifier>
<dc:title><![CDATA[An explanation of trap-limited self-interstitial diffusion and enhanced boron clustering in boron doped silicon superlattices]]></dc:title>
<dc:source><![CDATA[Proceedings of the Fourth International Symposium on Process Physics and Modeling in Semiconductor Technology, edited by G. R. Srinivasan, C. S. Murthy and S. T. Dunham, pp. 210-215]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Boron doped crystalline superlattices grown by low-temperature molecular beam epitaxy have been used by Stolk et al.  to study the diffusion of self-interstitials I in Si. After 40 keV Si+ ion implantation and subsequent annealing, stationary interstitial profiles are found at 670 °C for periods t ~1 h, demonstrating that the penetration depth of interstitials is limited by trapping at hitherto unidentified impurities. In addition, the high
interstitial supersaturation causes B de-activation in the near-surface region. We show that both these effects, the trap-limited interstitial diffusion and the enhanced B clustering, can be explained, if the transient de-activation of boron is modeled by the first-order reaction I + B_s ->B_i. Boron atomic and electrical profiles as well as self-interstitial profiles are computed which are in good agreement with the experimental results.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-482-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:403-1</identifier>
<datestamp>2020-12-09</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Mathar, R. J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-403-1</dc:identifier>
<dc:title><![CDATA[Influence of the first-order polarization on the stopping power for bare charges in the jellium model]]></dc:title>
<dc:source><![CDATA[Physical Review A 53 (1996) 4 pp.2873-2876]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Adding the contribution of the next higher order of the density parameter to the random-phase approximation (the zeroth-order, noninteracting approximation to the subceptibility) improves the calculation of the linear dielectric function of the jellium model. In this paper, the corresponding results by Holas, Aravind, and Singwi (Phys. Rev. B20 (1979) 4912) are picked up to extend the Lindhard-Winter theory of the electronic energy loss in a straightforward manner. As known from static approximations to the local-field correction, the electronic stopping at low ion velocities is enhanced. Above the stopping-power maximum, the first-order dynamic dielectric function delivers a correction of the opposite sign.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevA.53.2873]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-403-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:2539-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Lange, K.]]></dc:creator>
<dc:creator><![CDATA[Harz, M.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2539-1</dc:identifier>
<dc:title><![CDATA[Schlußbericht: Anwendungsgerechte Systemintegration und Zuverlässigkeit für die intelligente mikro-mechanische Sensorik (AN-SYS), Teilvorhaben: Silizium-Glas- und Silizium-Silizium-Bonden]]></dc:title>
<dc:source><![CDATA[BMBF-Verbundprojekt, Förderkennzeichen 13 MV 0266, Mai 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2539-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:1143-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
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<dc:title><![CDATA[Focused Ion Beam Sputtering of Silicon and Related Materials]]></dc:title>
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<dc:description><![CDATA[The impressive development of focused ion beam (FIB) systems from the laboratory level to high performance industrial machines during the last twenty years is briefly reported. The design and the functional principle of a liquid metal ion source as well as a FIB column are described. Main application fields of the FIB technology are stoichiometric writing implantation or ion milling which are dominated by the sputtering effect.  The FIB is a very suitable tool for sputtering of well defined holes which can easily be analysed by surface profiling. By applying this volume loss method the sputtering yields and milling rates of crystalline, amorphous, and poly-silicon, as well as SiO2, CVD- and high pressure (HP) - diamond and 6H:SiC were investigated for 35 and 70 keV Co, Ga, Ge, Nd and Au ions. For crystalline silicon and 6H:SiC targets, the sputtering yield was determined as a function of the incident angle of the ions and the substrate temperature. In addition, the influence of the pixel dwell time on the erosion process in the case of high dose cobalt implantation was investigated. The experimental obtained yield data are compared with calculated values using different known models.]]></dc:description>
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<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Voigt, A.]]></dc:creator>
<dc:creator><![CDATA[Kirmse, R.]]></dc:creator>
<dc:creator><![CDATA[Ortner, K.]]></dc:creator>
<dc:creator><![CDATA[Hübener, R.]]></dc:creator>
<dc:creator><![CDATA[Carballho Rias, R.]]></dc:creator>
<dc:creator><![CDATA[Vasquez-Lopez, E.]]></dc:creator>
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<dc:title><![CDATA[Darstellung, Strukturen und EPR-Spektren der Rhenium(II)-Nitrosylkomplexe [Re(NO)Cl<SUB>2</SUB>(PPh<SUB>3</SUB>)(OPPh<SUB>3</SUB>)(OReO<SUB>3</SUB>)], [Re(NO)Cl<SUB>2</SUB>(OPPh<SUB>3</SUB>)<SUB>2</SUB>(OReO<SUB>3</SUB>)] und [Re(NO)Cl...]]></dc:title>
<dc:source><![CDATA[Z. anorg. Allg. Chem. 624 (1998) 1662-1668]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1205-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Voigt, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1205-1</dc:identifier>
<dc:title><![CDATA[Synthesis, Structure and EPR Spectra of (Bu<SUB>4</SUB>N)<SUB>2</SUB>-[(OH<SUB>2</SUB>)Br<SUB>4</SUB>ReNReBr<SUB>4</SUB>NReBr<SUB>4</SUB>(OH<SUB>2</SUB>)]]]></dc:title>
<dc:source><![CDATA[Inorganic Chemistry Communications 1 (1998) 213-216]]></dc:source>
<dc:date>1998</dc:date>
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<dc:type>info:eu-repo/semantics/article</dc:type>
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<identifier>HZDR:PUBLDB:121-3</identifier>
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<dc:creator><![CDATA[Fraysse, L.]]></dc:creator>
<dc:creator><![CDATA[Frolov, S.]]></dc:creator>
<dc:creator><![CDATA[Gobbi, A.]]></dc:creator>
<dc:creator><![CDATA[Grigorian, Y.]]></dc:creator>
<dc:creator><![CDATA[Guillaume, G.]]></dc:creator>
<dc:creator><![CDATA[Herrmann, N.]]></dc:creator>
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<dc:creator><![CDATA[Houari, A.]]></dc:creator>
<dc:creator><![CDATA[Jeong, S. C.]]></dc:creator>
<dc:creator><![CDATA[Jorio, M.]]></dc:creator>
<dc:creator><![CDATA[Jundt, F.]]></dc:creator>
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<dc:creator><![CDATA[Koncz, P.]]></dc:creator>
<dc:creator><![CDATA[Korchagin, Y.]]></dc:creator>
<dc:creator><![CDATA[Krämer, M.]]></dc:creator>
<dc:creator><![CDATA[Kuhn, C.]]></dc:creator>
<dc:creator><![CDATA[Legrand, I.]]></dc:creator>
<dc:creator><![CDATA[Lebedev, A.]]></dc:creator>
<dc:creator><![CDATA[Maguire, C.]]></dc:creator>
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<dc:creator><![CDATA[Reisdorf, W.]]></dc:creator>
<dc:creator><![CDATA[Sadchikov, A.]]></dc:creator>
<dc:creator><![CDATA[Schüll, D.]]></dc:creator>
<dc:creator><![CDATA[Seres, Z.]]></dc:creator>
<dc:creator><![CDATA[Sikora, B.]]></dc:creator>
<dc:creator><![CDATA[Simion, V.]]></dc:creator>
<dc:creator><![CDATA[Smolyankin, S.]]></dc:creator>
<dc:creator><![CDATA[Sodan, U.]]></dc:creator>
<dc:creator><![CDATA[Teh, K.]]></dc:creator>
<dc:creator><![CDATA[Tezkratt, R.]]></dc:creator>
<dc:creator><![CDATA[Trzaska, M.]]></dc:creator>
<dc:creator><![CDATA[Vasiliev, M. A.]]></dc:creator>
<dc:creator><![CDATA[Wagner, P.]]></dc:creator>
<dc:creator><![CDATA[Wessels, J. P.]]></dc:creator>
<dc:creator><![CDATA[Wienold, T.]]></dc:creator>
<dc:creator><![CDATA[Wilhelmi, Z.]]></dc:creator>
<dc:creator><![CDATA[Zhilin, A. L.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
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<dc:title><![CDATA[Velocity correlations of intermediate mass fragments produced in central collisions of Au + Au at E = 150 A MeV]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR 93-14 Preprint]]></dc:source>
<dc:date>1993</dc:date>
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<identifier>HZDR:PUBLDB:121-1</identifier>
<datestamp>2020-11-03</datestamp>
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<dc:creator><![CDATA[Trzaska, M.]]></dc:creator>
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<dc:creator><![CDATA[Wagner, P.]]></dc:creator>
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<dc:title><![CDATA[Velocity correlations of intermediate mass fragments produced in central collisions of Au + Au at E = 150 A MeV]]></dc:title>
<dc:source><![CDATA[Physical Review C, 48, (1993)  pp. R955-R959]]></dc:source>
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<dc:title><![CDATA[Nuclear structure funktion F<SUB>2</SUB><SUP>A</SUP>:Moments Mn(F<SUB>2</SUB><SUP>A</SUP>) and kinematics beyond x=1]]></dc:title>
<dc:source><![CDATA[Physical Review D 47 (1993) 3804]]></dc:source>
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<record>
<header>
<identifier>HZDR:PUBLDB:169-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Titov, A. I.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Bratkovskaya, E. L.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-169-1</dc:identifier>
<dc:title><![CDATA[Dielectron production in pp and pd collisions at 1-5 GeV]]></dc:title>
<dc:source><![CDATA[Physical Review C 51 (1995) pp. 227]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-169-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:169-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Titov, A. I.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Bratkovskaya, E. L.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-169-2</dc:identifier>
<dc:title><![CDATA[Dielectron production in pp and pd collisions at 1-5 GeV]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-34 Preprint]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/preprint</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-169-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:173-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:creator><![CDATA[Kirch, S.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-173-1</dc:identifier>
<dc:title><![CDATA[Institute of Ion Beam Physics and Materials Research; Annual Report 1993]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-36]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-173-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:174-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Frauendorf, S.]]></dc:creator>
<dc:creator><![CDATA[Pashkevich, V. V.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-174-2</dc:identifier>
<dc:title><![CDATA[General Axial Shapes of Sodium Clusters]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-37 Preprint]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/preprint</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-174-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:174-3</identifier>
<datestamp>2020-12-08</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Frauendorf, S.]]></dc:creator>
<dc:creator><![CDATA[Pashkevich, V. V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-174-3</dc:identifier>
<dc:title><![CDATA[General Axial Shapes of Sodium Clusters]]></dc:title>
<dc:source><![CDATA[Annals of Physics 5 (1996) pp. 34-56]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1002/andp.2065080105]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-174-3</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:175-1</identifier>
<datestamp>2020-12-08</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pausch, G.]]></dc:creator>
<dc:creator><![CDATA[Bohne, W.]]></dc:creator>
<dc:creator><![CDATA[Hilscher, D.]]></dc:creator>
<dc:creator><![CDATA[Ortlepp, H.-G.]]></dc:creator>
<dc:creator><![CDATA[Polster, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-175-1</dc:identifier>
<dc:title><![CDATA[Particle identification in a wide dynamic range based on pulse-shape analysis with solid-state detectors]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research A 349 (1994) 2/3 pp. 281-284]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/0168-9002(94)90634-3]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-175-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:175-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Pausch, G.]]></dc:creator>
<dc:creator><![CDATA[Bohne, W.]]></dc:creator>
<dc:creator><![CDATA[Hilscher, D.]]></dc:creator>
<dc:creator><![CDATA[Ortlepp, H.-G.]]></dc:creator>
<dc:creator><![CDATA[Polster, D.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-175-2</dc:identifier>
<dc:title><![CDATA[Particle identification in a wide dynamic range based on pulse-shape analysis with solid-state detectors]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-38]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-175-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:177-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Seidel, W.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-177-1</dc:identifier>
<dc:title><![CDATA[Double-grid avalanche counters with large dynamic range]]></dc:title>
<dc:source><![CDATA[Fa. ALTIUM, USA, Buch über P-CAD]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/book</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:book</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-177-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:180-2</identifier>
<datestamp>2020-12-07</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kolomeitsev, E. E.]]></dc:creator>
<dc:creator><![CDATA[Voskresensky, D. N.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-180-2</dc:identifier>
<dc:title><![CDATA[Kaon Polarization in Nuclear Matter]]></dc:title>
<dc:source><![CDATA[Nuclear Physics A 588 (1995) pp. 889]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/0375-9474(95)00084-E]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-180-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:180-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Kolomeitsev, E. E.]]></dc:creator>
<dc:creator><![CDATA[Voskresensky, D. N.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-180-1</dc:identifier>
<dc:title><![CDATA[Kaon Polarization in Nuclear Matter]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-40 Preprint]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/preprint</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-180-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:683-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Nakamura, K.]]></dc:creator>
<dc:creator><![CDATA[Mändl, S.]]></dc:creator>
<dc:creator><![CDATA[Brutscher, J.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-683-1</dc:identifier>
<dc:title><![CDATA[Incident Ion Monitoring during Plasma Immersion Ion Implantation by Direct Measurements of High Energy Secondary Electrons]]></dc:title>
<dc:source><![CDATA[3rd International Workshop on Plasma - Based Ion Implantation (PBII), Dresden, Germany, Sept. 16-18 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The present paper investigated time-resolved incident ion monitoring during PIII processes on the basis of high energy secondary electron measurements with scintillation technique. Taking into consideration the sheath geometry and a secondary electron emission coefficient of the target material, the experimental data were in a good agreement with theoretical predictions for dependences on target-voltage, pressure and plasma density.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-683-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:861-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Strobel, M.]]></dc:creator>
<dc:creator><![CDATA[Reiß, S.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-861-1</dc:identifier>
<dc:title><![CDATA[Evolution of nanocluster ensembler: Computer simulation of diffusion and reaction controlled Ostwald ripening]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 120 (1996) pp. 216-220]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The Ion Beam Synthesis (IBS) of nanoclusters can be controlled by the flux and the fluence of ions as well as by the implantation and/or annealing temperature. The evolution of the precipitates, mainly described by their particle radius distribution (PRD), the number of remaining particles and the critical radius, depends on these parameters. However, the evolution is expected to behave different for systems like SiO2 and CoSi2 clusters in Si, because they are characterized by quite different ratios of diffusion to reaction constants. Here we present an unified model of Ostwald ripening of nanoclusters, which describes the pure diffusion and reaction controlled limits as well as all intermediate, mixed processes. Expressing the exact solution of the adiabatic diffusion equation by multipole moments we derive the governing equation for the evolution of an ensemble of nanoclusters in the leading monopole approximation. Whereas in the diffusion controlled regime we have the well known infinite range 1/r interaction among the nanoclusters, 1/r2 interactions come into play in the reaction limited regime. Computer simulations for ensembles of several thousands of nanoclusters demonstrate the evolution for typical cases.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:title><![CDATA[N.C.A. <SUP>11</SUP>C-labelling of aromatic compounds in the ring-position: synthesis of nitro-[1-<SUP>11</SUP>C]benzene and [1-<SUP>11</SUP>C]aniline]]></dc:title>
<dc:source><![CDATA[Journal of Labelled Compounds and Radiopharmaceuticals 36 (1994) 1 pp. 33]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:title><![CDATA[Institute of Bioinorganic and Radiopharmaceutical Chemistry; Annual Report 1993]]></dc:title>
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<dc:title><![CDATA[Institute of Nuclear and Hadron Physics; Annual Report 1993]]></dc:title>
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<dc:title><![CDATA[Effects of flow on intermediate mass fragments in central gold on gold collisions]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-41 Preprint]]></dc:source>
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<dc:title><![CDATA[Effects of flow on intermediate mass fragments in central gold on gold collisions]]></dc:title>
<dc:source><![CDATA[Physics Letters B 337 (1994) pp. 53]]></dc:source>
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<dc:title><![CDATA[Effects of flow on intermediate mass fragments in central gold on gold collisions]]></dc:title>
<dc:source><![CDATA[Physics Letters B 340 (1994) pp. 267 (Erratum)]]></dc:source>
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<dc:title><![CDATA[Buried (fe 2-x Co x) Si2 layers with variable band gap formed in silicon by ion beam synthesis (IBS)]]></dc:title>
<dc:source><![CDATA[Journal of Applied Physics A 62 (1996), 155]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Fietz, T.]]></dc:creator>
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<dc:title><![CDATA[Synthesis and molecular structure of chlore(3-thiapentane-1.5-dithiolato)oxorhenium(V)]]></dc:title>
<dc:source><![CDATA[Inorganica Chimica Acta 231 (1995) pp. 233-236]]></dc:source>
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<dc:title><![CDATA[Thermocapillary bubble migration in a drop tower experiment]]></dc:title>
<dc:source><![CDATA[und Proceedings: 45th IAF Congress, Jerusalem, 9.-14.10.1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:193-1</identifier>
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<dc:creator><![CDATA[Mittag, S.]]></dc:creator>
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<dc:identifier>https://www.hzdr.de/publications/Publ-193-1</dc:identifier>
<dc:title><![CDATA[Recherche zu Gruppendatenbibliotheken für die Anwendung des Programmes DYN3D auf Reaktoren vom Typ WWER]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-46]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Für die Berechnung des Reaktorverhaltens mit Kernmodellen (wie DYN3D) werden sog. Weniggruppen-Neutronendaten benötigt. Es wird eine Übersicht zu entsprechenden Datenbibliotheken für die Spaltzonen von russischen WWER-Reaktoren aufgestellt. Die Informationen über verwendete Primärdaten und die Genauigkeit der Zellcodes für die Gruppendatengenerierung werden im wesentlichen in Tabellenform gegeben. Zur Beurteilung der Qualität der Daten werden Vergleiche zwischen gemessenen und berechneten Reaktorparametern zusammengestellt. Die verfügbaren Informationen ergeben keine signifikanten Qualitätsunterschiede zwischen den einzelnen Datenbibliotheken.]]></dc:description>
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<dc:creator><![CDATA[Große, M.]]></dc:creator>
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<dc:creator><![CDATA[Eichhorn, F.]]></dc:creator>
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<dc:creator><![CDATA[Goerigk, G.]]></dc:creator>
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<dc:title><![CDATA[ASAXS and SANS investigations of the chemical composition of irradiation-induced precipitates in nuclear pressure vessel steels]]></dc:title>
<dc:source><![CDATA[1st European Conference on Synchrotron Radiation in Material Science, Chester UK, 2.-8.7.1994]]></dc:source>
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<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
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<dc:title><![CDATA[Writing implantation with a high current Focused Ion Beam to form CoSi2 - Microstructures]]></dc:title>
<dc:source><![CDATA[EIPB '94, New Orleans, 31.5.-3.6.1994]]></dc:source>
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<identifier>HZDR:PUBLDB:1018-1</identifier>
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<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:creator><![CDATA[Hatzopoulos, N.]]></dc:creator>
<dc:creator><![CDATA[Armour, D. G.]]></dc:creator>
<dc:creator><![CDATA[Berg, J. A.]]></dc:creator>
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<dc:title><![CDATA[Ellipsometric Investigation of Damage Distribution in Low Energy Boron Implantation of Silicon]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 127/128 (1997) 879-883]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[As the scaling of silicon devices to 100 nm channel length requires the formation of ultra-shallow (< 60 nm) junctions, high depth resolution analytical techniques become necessary for the  characterization of the dopant and damage distributions. In situ single wavelength Ellipsometric
Etch Depth Profiling (EEDP) and non-destructive Variable Angle of incidence Spectroscopic Ellipsometry (VASE) have been used to obtain accurate and quantitative information on the depth profiles of radiation damage produced by low energy, room temperature ion implantation of B<SUP>+</SUP> into Si.]]></dc:description>
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<identifier>HZDR:PUBLDB:1021-2</identifier>
<datestamp>2023-04-26</datestamp>
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<dc:creator><![CDATA[Kaptari, L. P.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Dorkin, S. M.]]></dc:creator>
<dc:creator><![CDATA[Semikh, S. S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1021-2</dc:identifier>
<dc:title><![CDATA[Elastic Proton-Deuteron Backward Scattering: Relativistic Effets and Polarization Observables]]></dc:title>
<dc:source><![CDATA[Physical Review C Vol. 57 (1998) 1097-1111]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Abstract
The elastic proton-deuteron backward reaction is analyzed within a covariant approach based on the Bethe-Salpeter equation with realistic meson-exchange interaction. Lorentz boost and other relativistic effects in the cross section and spin correlation observables, like tensor analyzing power and polarization transfer etc., are investigated in explicit form. Results of numerical calculations for a compbte set of polarization observables are presented.]]></dc:description>
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<identifier>HZDR:PUBLDB:1021-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kaptari, L. P.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Dorkin, S. M.]]></dc:creator>
<dc:creator><![CDATA[Semikh, S. S.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
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<dc:title><![CDATA[Elastic Proton-Deuteron Backward Scattering: Relativistic Effets and Polarization Observables]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-194]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Abstract
The elastic proton-deuteron backward reaction is analyzed within a covariant approach based on the Bethe-Salpeter equation with realistic meson-exchange interaction. Lorentz boost and other relativistic effects in the cross section and spin correlation observables, like tensor analyzing power and polarization transfer etc., are investigated in explicit form. Results of numerical calculations for a compbte set of polarization observables are presented.]]></dc:description>
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<identifier>HZDR:PUBLDB:1023-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kamanin, D. V.]]></dc:creator>
<dc:creator><![CDATA[Wagner, W.]]></dc:creator>
<dc:creator><![CDATA[Ortlepp, H.-G.]]></dc:creator>
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<dc:title><![CDATA[A Method for the Intrinsic Calibration of CsI(Tl) Detectors]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-197]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Abstract
A method for the intrinsic energy calibration of photomultiplier-coupled CsI(Tl) detectors is described. A simple empirical model of the scintillation light pulse-shape of CsI(Tl) crystals for light charged particles has been applied to simulate the particle identification matrix as it follows from the pulse-shape analysis method. The calibration procedure for the large-area CsI(Tl) detectors of the scintillator shell of the 4 π - array FOBOS for ions with Z < 4 at energies below 100 AMeV is based on the energies of the particle punch-through points.]]></dc:description>
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<dc:creator><![CDATA[Kamanin, D. V.]]></dc:creator>
<dc:creator><![CDATA[Wagner, W.]]></dc:creator>
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<dc:title><![CDATA[A Method for the Intrinsic Calibration of CsI(Tl) Detectors]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research A 413 (1998) 127-137]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Abstract
A method for the intrinsic energy calibration of photomultiplier-coupled CsI(Tl) detectors is described. A simple empirical model of the scintillation light pulse-shape of CsI(Tl) crystals for light charged particles has been applied to simulate the particle identification matrix as it follows from the pulse-shape analysis method. The calibration procedure for the large-area CsI(Tl) detectors of the scintillator shell of the 4 π - array FOBOS for ions with Z < 4 at energies below 100 AMeV is based on the energies of the particle punch-through points.]]></dc:description>
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<identifier>HZDR:PUBLDB:1028-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Brückner, J.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1028-1</dc:identifier>
<dc:title><![CDATA[Metal Plasma Immersion Ion Implantation and Deposition (MPIIID): Chromium on Magnesium]]></dc:title>
<dc:source><![CDATA[Konferenz SMMIB 97, Gatlinburg, TE, USA, Sept. 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1028-2</identifier>
<datestamp>2023-04-26</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brückner, J.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
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<dc:title><![CDATA[Metal Plasma Immersion Ion Implantation and Deposition (MPIIID): Chromium on Magnesium]]></dc:title>
<dc:source><![CDATA[Surface and Coatings Technology 103-104 (1998) 227-230]]></dc:source>
<dc:date>1998</dc:date>
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<identifier>HZDR:PUBLDB:1030-1</identifier>
<datestamp>2023-04-26</datestamp>
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<dc:creator><![CDATA[Taut, S.]]></dc:creator>
<dc:creator><![CDATA[Hübener, S.]]></dc:creator>
<dc:creator><![CDATA[Eichler, B.]]></dc:creator>
<dc:creator><![CDATA[Türler, A.]]></dc:creator>
<dc:creator><![CDATA[Gäggeler, H. W.]]></dc:creator>
<dc:creator><![CDATA[Timokhin, S. N.]]></dc:creator>
<dc:creator><![CDATA[Zvara, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1030-1</dc:identifier>
<dc:title><![CDATA[Thermochromatography of Heavy Actinides - Adsorption of No-259 on Ti, V, Nb, Ta and Mo]]></dc:title>
<dc:source><![CDATA[Journal of Alloys and Compounds 271-273 (1998) 316-321]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:creator><![CDATA[Taut, S.]]></dc:creator>
<dc:creator><![CDATA[Hübener, S.]]></dc:creator>
<dc:creator><![CDATA[Eichler, B.]]></dc:creator>
<dc:creator><![CDATA[Türler, A.]]></dc:creator>
<dc:creator><![CDATA[Gäggeler, H. W.]]></dc:creator>
<dc:creator><![CDATA[Timokhin, S. N.]]></dc:creator>
<dc:creator><![CDATA[Zvara, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1030-2</dc:identifier>
<dc:title><![CDATA[Thermochromatography of Heavy Actinides - Adsorption of No-259 on Ti, V, Nb, Ta and Mo]]></dc:title>
<dc:source><![CDATA[J. Less-Common Met. 271-273, 316 (1998)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1213-1</identifier>
<datestamp>2023-05-03</datestamp>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Kohl, F. J.]]></dc:creator>
<dc:creator><![CDATA[Öfele, K.]]></dc:creator>
<dc:creator><![CDATA[Herrmann, W. A.]]></dc:creator>
<dc:creator><![CDATA[Voigt, A.]]></dc:creator>
<dc:creator><![CDATA[Kirmse, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1213-1</dc:identifier>
<dc:title><![CDATA[(Bu<SUB>4</SUB>N)[Re{NB(C<SUB>6</SUB>F<SUB>5</SUB>)<SUB>3</SUB>}CI<SUB>4</SUB>(OH<SUB>2</SUB>)] - Struktur und EPR-Spektren]]></dc:title>
<dc:source><![CDATA[Zeitschrift für anorganische und allgemeine Chemie 624 (1998) 934-936]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:547-2</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Brutscher, J.]]></dc:creator>
<dc:creator><![CDATA[Mändl, S.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-547-2</dc:identifier>
<dc:title><![CDATA[The use of plasma source ion implantation for wear protection]]></dc:title>
<dc:source><![CDATA[Y. Pauleau and P. B. Barna (eds), Protective Coatings and Thin Films, pp. 635-647, c 1997 Kluwer Academic Publishers, Printed in the Netherlands]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Plasma source ion implantation (PSII) has been developed
as an alternative technique to circumvent the limitations of conventional
ion implantation, like the requirements of a complicated target handling
and beam raster system for a uniform ion implantation of 3-dimensional
samples. In this method, a plasma sheath conformably surrounds the target.
By applying negative high voltage pulses, positively charged ions are accelerated
from the plasma trough the sheath and implanted into the target. Critical
parameters for the further development of this implantation process are
the ion implantation current and the sheath expansion characteristics.]]></dc:description>
<dc:type>info:eu-repo/semantics/book</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:book</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-547-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:547-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Brutscher, J.]]></dc:creator>
<dc:creator><![CDATA[Mändl, S.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-547-1</dc:identifier>
<dc:title><![CDATA[The use of plasma source ion implantation for wear protection]]></dc:title>
<dc:source><![CDATA[NATO-ARW, Portimao, Portugal, 30.5.-5.6.1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Plasma source ion implantation (PSII) has been developed
as an alternative technique to circumvent the limitations of conventional
ion implantation, like the requirements of a complicated target handling
and beam raster system for a uniform ion implantation of 3-dimensional
samples. In this method, a plasma sheath conformably surrounds the target.
By applying negative high voltage pulses, positively charged ions are accelerated
from the plasma trough the sheath and implanted into the target. Critical
parameters for the further development of this implantation process are
the ion implantation current and the sheath expansion characteristics.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-547-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1040-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Enghardt, W.]]></dc:creator>
<dc:creator><![CDATA[Debus, J.]]></dc:creator>
<dc:creator><![CDATA[Hasch, B.-G.]]></dc:creator>
<dc:creator><![CDATA[Hinz, R.]]></dc:creator>
<dc:creator><![CDATA[Haberer, T.]]></dc:creator>
<dc:creator><![CDATA[Jäkel, O.]]></dc:creator>
<dc:creator><![CDATA[Lauckner, K.]]></dc:creator>
<dc:creator><![CDATA[Pawelke, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1040-1</dc:identifier>
<dc:title><![CDATA[Quality assurance of heavy ion tumour therapy by means of positron emission tomography.]]></dc:title>
<dc:source><![CDATA[IEEE Nuclear Science Symposium and Medical Imaging Conference, Albuquerque, New Mexico, 9-15 Nov, 1997
<br>
Book of Abstracts(1997)102]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1040-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1040-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Enghardt, W.]]></dc:creator>
<dc:creator><![CDATA[Debus, J.]]></dc:creator>
<dc:creator><![CDATA[Hasch, B.-G.]]></dc:creator>
<dc:creator><![CDATA[Hinz, R.]]></dc:creator>
<dc:creator><![CDATA[Haberer, T.]]></dc:creator>
<dc:creator><![CDATA[Jäkel, O.]]></dc:creator>
<dc:creator><![CDATA[Lauckner, K.]]></dc:creator>
<dc:creator><![CDATA[Pawelke, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1040-7</dc:identifier>
<dc:title><![CDATA[Quality assurance of heavy ion tumour therapy by means of positron emission tomography.]]></dc:title>
<dc:source><![CDATA[IEEE Nuclear Science Symposium and Medical Imaging Conference, Albuquerque, New Mexico, 9-15 Nov, 1997
<br>
Book of Abstracts(1997)102]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1040-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1071-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hennig, C.]]></dc:creator>
<dc:creator><![CDATA[Denecke, M. A.]]></dc:creator>
<dc:creator><![CDATA[Roßberg, A.]]></dc:creator>
<dc:creator><![CDATA[Zahn, G.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1071-1</dc:identifier>
<dc:title><![CDATA[Uranium L<SUB>III</SUB> XANES and EXAFS on the Uranyl Unit in a Single Crystal with Linear Polarized Synchrotron Radiation]]></dc:title>
<dc:source><![CDATA[HASYLAB Jahresbericht 1997, 823 (1998)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1071-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:877-1</identifier>
<datestamp>2022-11-10</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-877-1</dc:identifier>
<dc:title><![CDATA[Ion implantation and annealing effects in silicon carbide]]></dc:title>
<dc:source><![CDATA[Materials Research Society symposium proceeding 438 (1997) pp. 241-252, MRS]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[SiC is a promising semiconductor material for high-power/high-frequency
and high-temperature electronic applications. For selective doping of SiC
ion implantation is the only possible process. However, relatively little
is known about ion implantation and annealing effects in SiC. Compared
to ion implantation into Si there is a number of specific features which
have to be considered for successful ion beam processing of SiC. A brief
review is given on some aspects of ion implantation in and annealing of
SiC. The ion implantation effects in SiC are discussed in direct comparison
to Si. The following issues are addressed: ion ranges, radiation damage,
amorphization, high temperature implantation, ion beam induced crystallization
and surface erosion.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1557/PROC-438-241]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-877-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:831-1</identifier>
<datestamp>2022-11-11</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:creator><![CDATA[Prokert, F.]]></dc:creator>
<dc:creator><![CDATA[Schell, N.]]></dc:creator>
<dc:creator><![CDATA[Seifarth, H.]]></dc:creator>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-831-1</dc:identifier>
<dc:title><![CDATA[Density and structural changes of SiC after amorphization and annealing]]></dc:title>
<dc:source><![CDATA[Applied Physics Letters 70(26), 3531]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The density of amorphous SiC layers formed by 2 MeV Si<SUP>+</SUP> implantation into single crystalline 6H-SiC was measured by X-ray reflectometry and compared with the resultts of step height measurements. Reactive ion
etching was used to investigate the density as function of depth. The density of the as-amorphized SiC is about 12 % less than that of the crystalline material. Within the experimental accuracy the density reduction is homogeneous
over the whole layer thickness. Low temperature annealing leads to the formation of relaxed amorphous SiC with a density about 7 % below the crystalline one. These large density changes are in contrast to results in amorphous
Si. They can be explained by the high atomic density of SiC and the chemical disorder in the amorphous state of SiC.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1063/1.119223]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-831-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:232-1</identifier>
<datestamp>2020-12-03</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Glaser, M.]]></dc:creator>
<dc:creator><![CDATA[Hahn, F. E.]]></dc:creator>
<dc:creator><![CDATA[Lügger, T.]]></dc:creator>
<dc:creator><![CDATA[Scheller, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-232-1</dc:identifier>
<dc:title><![CDATA[Synthesis and characterization of isocyanide containing rhenium(III) complexes trans-[ReCl<SUB>3</SUB>(CNR)(PPh<SUB>3</SUB>)<SUB>2</SUB>] and crystal structure of trans-[ReCl<SUB>3</SUB>(CN-t-C<SUB>4</SUB>H<SUB>9</SUB>)(PPh<SUB>3</SUB>)<SUB>2</SUB>]]]></dc:title>
<dc:source><![CDATA[Inorganica Chimica Acta 232 (1995) 235-239]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/0020-1693(94)04373-4]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-232-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:235-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Leibnitz, P.]]></dc:creator>
<dc:creator><![CDATA[Reck, G.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-235-1</dc:identifier>
<dc:title><![CDATA[Technetium and Rhenium Complexes with Multidentale Thioether Ligands]]></dc:title>
<dc:source><![CDATA[4th Intern. Sympos. on Tc in Chemistry and Nuclear Medicine, Brixen, in: Technetium and Rhenium in Chemistry and Nuclear Medicine, Edited by Nicolini, M.u.a., SGEDITORIALI Padova 4 (1995) 231-234]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-235-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:235-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Leibnitz, P.]]></dc:creator>
<dc:creator><![CDATA[Reck, G.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-235-7</dc:identifier>
<dc:title><![CDATA[Technetium and Rhenium Complexes with Multidentale Thioether Ligands]]></dc:title>
<dc:source><![CDATA[4th Intern. Sympos. on Tc in Chemistry and Nuclear Medicine, Brixen, in: Technetium and Rhenium in Chemistry and Nuclear Medicine, Edited by Nicolini, M.u.a., SGEDITORIALI Padova 4 (1995) 231-234]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:bookPart</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-235-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:236-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Seifert, S.]]></dc:creator>
<dc:creator><![CDATA[Syhre, R.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
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<dc:creator><![CDATA[Gabriel, F.]]></dc:creator>
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<dc:title><![CDATA[Bericht der Herbsttagung der Studiengruppe für Elektronische Instrumentierung vom 29. September bis 1. Oktober an der Universität in Frankfurt am Main]]></dc:title>
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<dc:creator><![CDATA[Titov, A. I.]]></dc:creator>
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<dc:title><![CDATA[Polarization Observables in the Reaction NN -> NN O|]]></dc:title>
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<dc:description><![CDATA[Abstract:
We study the reaction NN → NNΦ slightly above the threshold within an extended one-boson exchange model which also accounts for uud knock-out. It is shown that  olarization observables, like the beam-target asymmetry, are sensible quantities for identifying a ss admixture in the nucleon wave function on the few per cent level.]]></dc:description>
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<dc:creator><![CDATA[Peshier, A.]]></dc:creator>
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<dc:title><![CDATA[Thermodynamics of the PHI<SUP>4</SUP> Theory in Tadpole Approximation]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-208]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Abstract
Relying on the Luttinger-Ward theorem we derive a thermodynamically selfconsistent and scale independent approximation of the thermodynamic potential for the scalar Φ<sup>4</sup> theory in the tadpole approximation. The resulting thermodynamic potential as a function of the temperature is similar to the one of the recently proposed screened perturbation theory.]]></dc:description>
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<dc:creator><![CDATA[Peshier, A.]]></dc:creator>
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<dc:title><![CDATA[Thermodynamics of the PHI<SUP>4</SUP> Theory in Tadpole Approximation]]></dc:title>
<dc:source><![CDATA[Europhysics Letters 43 (4), pp. 381-385 (1998)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Abstract
Relying on the Luttinger-Ward theorem we derive a thermodynamically selfconsistent and scale independent approximation of the thermodynamic potential for the scalar Φ<sup>4</sup> theory in the tadpole approximation. The resulting thermodynamic potential as a function of the temperature is similar to the one of the recently proposed screened perturbation theory.]]></dc:description>
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<dc:creator><![CDATA[Frauendorf, S.]]></dc:creator>
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<dc:title><![CDATA[Evaporation Rates for Liquid Clusters]]></dc:title>
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<dc:title><![CDATA[Evaporation Rates for Liquid Clusters]]></dc:title>
<dc:source><![CDATA[Zeitschrift für Physik D 35 (1995) pp. 191]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:description><![CDATA[Es  wird ein Ultraschall-Meßverfahren für Zweiphasenströmungen vorgestellt, das die simultane Messung der Volumenstromdichte der Gas- und der Flüssigphase in einer Rohrleitung ermöglicht. Ein Prototyp wurde in Zusammenarbeit mit der Universität Nishny Novgorod (Rußland) aufgebaut. Es realisiert einen gepulsten Transmissions- und Reflexionsbetrieb mit Wellenleitersensoren, die auch an heiße Rohrleitungen bis zu 350°C direkt angekoppelt werden können. Kernstück der Meßmethode ist ein Mustererkennungsverfahren, das in bestimmten Volumenstrombereichen nach einer umfangreichen Kalibrierung (Trainingsprozeß) einen Meßfehler von kleiner 10 % besitzt, wenn die thermodynamischen und geometrischen Randbedingungen nahezu konstant bleiben. Durch die Erweiterung der Trainingsmatrizen um einen, die thermodynamischen Eigenschaften determinierenden Parameter (z. B. Temperatur, Druck) kann das Klassifizierungsverfahren auch auf Fälle mit veränderlichen Stoffwerten angewandt werden. Das Mustererkennungsverfahren und die Ultraschalltechnik wurden experimentell optimiert und erprobt. Die Ultraschallsignale wurden außerdem mit Hilfe der Methode des unüberwachten Lernens klassifiziert. Die gefundenen Gruppen von Signalmustern weisen eine deutliche Ähnlichkeit zu bekannten Strömungskarten auf. Es wird gezeigt, daß das Verfahren des unüberwachten Lernens sich für die objektive Aufstellung von Strömungskarten eignet. In einem speziellen Kapitel werden die Ergebnisse von Tests zur Füllstandsmessung in einem Segment der Hauptumwälzleitung von Druckwasserreaktoren vorgestellt.]]></dc:description>
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<dc:title><![CDATA[Anwendung der Entscheidungsanalyse bei der Sanierung von Altlasten]]></dc:title>
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<dc:title><![CDATA[Dynamic in situ Diagnostics Using High-Energy Ion Beam Analysis]]></dc:title>
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1093-1</dc:identifier>
<dc:title><![CDATA[Workshop "Meßtechnik für stationäre und transiente Mehrphasenströmungen" , 6.-7. November 1997 in Rossendorf]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-204, Dezember 1997 (Tagungsband)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
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<identifier>HZDR:PUBLDB:1096-1</identifier>
<datestamp>2023-05-02</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:creator><![CDATA[Schnare, H.]]></dc:creator>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:creator><![CDATA[Servene, T.]]></dc:creator>
<dc:creator><![CDATA[Käubler, L.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Wilhelm, M.]]></dc:creator>
<dc:creator><![CDATA[Fitzler, A.]]></dc:creator>
<dc:creator><![CDATA[Kasemann, S.]]></dc:creator>
<dc:creator><![CDATA[Radermacher, E.]]></dc:creator>
<dc:creator><![CDATA[Brentano, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1096-1</dc:identifier>
<dc:title><![CDATA[States of Seniority 3 and 5 in the N=48 Nucleus <SUP>87</SUP>Y<SUP></SUP>]]></dc:title>
<dc:source><![CDATA[Physical Review C Volume 57, Number 6, pp. 2892-2902]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1109-1</identifier>
<datestamp>2023-05-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Friebe, M.]]></dc:creator>
<dc:creator><![CDATA[Jankowsky, R.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Seichter, W.]]></dc:creator>
<dc:creator><![CDATA[Papadopoulos, M.]]></dc:creator>
<dc:creator><![CDATA[Chiotillis, E.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1109-1</dc:identifier>
<dc:title><![CDATA[A Mixed-Ligand P,S,N-cis-Dioxorhenium(V) Complex by Ligand Exchange Reaction on trans-monooxo-trichloro-bis(triphenylphosphine)rhenium(V): Formation and Structural Studies]]></dc:title>
<dc:source><![CDATA[Polyhedron Vol. 17, No. 21, pp. 3711-3720, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0277-5387(98)00169-7]]></dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:1065-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Werner, M.]]></dc:creator>
<dc:creator><![CDATA[Willschütz, H.-G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1065-2</dc:identifier>
<dc:title><![CDATA[Finite Element Based Stress Analysis of BWR Internals Exposed to Accident Loads]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik98, München, 26.-28. Mai 1998, Tagungsbericht S. 721-724]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[During a hypothetical accident the reactor pressure vessel internals of boiling water reactors can be exposed to considerable loads resulting from temperature gradients and pressure waves. The finite element (FE) analysis is an efficient tool to evaluate the consequences of those loads by computing the maximum mechanical stresses in the components. 3 dimensional FE models were developed for the core shroud, the upper and the lower core supporting structure, the steam separator pipes and the feed water distributor. The models of core shroud, upper core support structure and lower core support structure were coupled by means of the substructure technique. All FE models can be used for thermal and for structural mechanical analyses. As an example the FE analysis for the case of a station black-out scenario (loss of power supply for the main circulating pumps) with subsequent emergency core cooling is demonstrated. The transient temperature distributions within the core shroud and within the steam dryer pipes as well were calculated based on the fluid temperatures and the heat transfer coefficients provided by thermo-hydraulic codes. At the maximum temperature gradients in the core shroud, the mechanical stress distribution was computed in a static analysis with the actual temperature field being the load. It could be shown that the maximum resulting material stresses do not exceed the permissible thresholds fixed in the appropriate regulations. Another scenario which was investigated is the break of a feed water line leading to a non-symmetric subpressure wave within the reactor pressure vessel. The dynamic structural response of the core shroud was assessed in a tranisient analysis. Even for this load case the maximum resulting stresses remain within the allowed limits at any time.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1065-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Werner, M.]]></dc:creator>
<dc:creator><![CDATA[Willschütz, H.-G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1065-7</dc:identifier>
<dc:title><![CDATA[Finite Element Based Stress Analysis of BWR Internals Exposed to Accident Loads]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik98, München, 26.-28. Mai 1998, Tagungsbericht S. 721-724]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[During a hypothetical accident the reactor pressure vessel internals of boiling water reactors can be exposed to considerable loads resulting from temperature gradients and pressure waves. The finite element (FE) analysis is an efficient tool to evaluate the consequences of those loads by computing the maximum mechanical stresses in the components. 3 dimensional FE models were developed for the core shroud, the upper and the lower core supporting structure, the steam separator pipes and the feed water distributor. The models of core shroud, upper core support structure and lower core support structure were coupled by means of the substructure technique. All FE models can be used for thermal and for structural mechanical analyses. As an example the FE analysis for the case of a station black-out scenario (loss of power supply for the main circulating pumps) with subsequent emergency core cooling is demonstrated. The transient temperature distributions within the core shroud and within the steam dryer pipes as well were calculated based on the fluid temperatures and the heat transfer coefficients provided by thermo-hydraulic codes. At the maximum temperature gradients in the core shroud, the mechanical stress distribution was computed in a static analysis with the actual temperature field being the load. It could be shown that the maximum resulting material stresses do not exceed the permissible thresholds fixed in the appropriate regulations. Another scenario which was investigated is the break of a feed water line leading to a non-symmetric subpressure wave within the reactor pressure vessel. The dynamic structural response of the core shroud was assessed in a tranisient analysis. Even for this load case the maximum resulting stresses remain within the allowed limits at any time.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1069-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Stephan, I.]]></dc:creator>
<dc:creator><![CDATA[Gawlik, D.]]></dc:creator>
<dc:creator><![CDATA[Gatschke, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1069-1</dc:identifier>
<dc:title><![CDATA[Bestimmung der Neutronenflußdichten in den Bestrahlungseinrichtungen des BER II bei der HEU-LEU Umstellung]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik 1998, Tagungsbericht, Mannheim 1998, S. 631 ff.]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1069-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Stephan, I.]]></dc:creator>
<dc:creator><![CDATA[Gawlik, D.]]></dc:creator>
<dc:creator><![CDATA[Gatschke, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1069-7</dc:identifier>
<dc:title><![CDATA[Bestimmung der Neutronenflußdichten in den Bestrahlungseinrichtungen des BER II bei der HEU-LEU Umstellung]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik 1998, Tagungsbericht, Mannheim 1998, S. 631 ff.]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1070-1</identifier>
<datestamp>2023-05-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Mäding, P.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1070-1</dc:identifier>
<dc:title><![CDATA[N.C.A.<SUP>11</SUP>C-Labelling of Benzenoid Compounds in Ring Positions: Synthesis of 3-Nitro-/ 3-<SUP>11</SUP>C/ Toluene and 4-Nitro-/ 4-<SUP>11</SUP>C/ Toluene and Their Corresponding Toluidines]]></dc:title>
<dc:source><![CDATA[Journal of Labelled Compounds and Radiopharmaceuticals XLI, 647-656 (1998)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1002/(SICI)1099-1344(199807)41:7<647::AID-JLCR114>3.0.CO;2-5]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1070-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:562-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kögler, R.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Romano-Rodriguez, A.]]></dc:creator>
<dc:creator><![CDATA[Perez-Rodriguez, A.]]></dc:creator>
<dc:creator><![CDATA[Serre, C.]]></dc:creator>
<dc:creator><![CDATA[Calvo-Barrio, L.]]></dc:creator>
<dc:creator><![CDATA[Morante, J. R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-562-1</dc:identifier>
<dc:title><![CDATA[Ion Beam Synthesis of SiC in Silicon-on-Insulator]]></dc:title>
<dc:source><![CDATA[IIT '96, Austin, Texas, USA; Proc. 11th Int. Conf. Ion Implantation Technology; The Inst. of Electrical and Electronics Eng., Piscataway, USA, 1997, p. 709]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Ion beam synthesis of ß-SiC in the top-Si-layer of a SIMOX (Separation by Implantation of OXygen) substrate is reported.
All the implanted C is captured inside the 200 nm top-Si-layer and is accumulated preferentially at the Si/SiO2-interface during annealing. A Si/SiC/SiO2-structure is obtained by C implantation at high temperature (T&gt;500 °C) and subsequent annealing treatment (T=1250 °C). It consists of a crystalline Si overlayer, a Si layer with a high density of perfectly aligned ß-SiC grains and a buried oxide layer. Implantation at elevated temperatures is crucial for the quality of the SiC layer. However, the use of such implantation  temperatures is limited by the dissolution of the buried oxide layer.]]></dc:description>
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<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1135-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Dumaz, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1135-1</dc:identifier>
<dc:title><![CDATA[Post-Test Calculations of NOKO Emergency Condenser Experiments]]></dc:title>
<dc:source><![CDATA[ICONE 6 - 6th International Conference on Nuclear Engineering , 10.-14. Juni 1998, San Diego, Californien, Beitrag 6382]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The SWR1000 is a new innovative boiling water reactor concept,
which is developed by Siemens AG. This concept is characterized
in particular by passive safety systems (e.g., four emergency
condensers, four building condensers, eight passive pressure
pulse transmitters, six gravitydriven core flooding lines).
Passive safety systems need no external energy sources. The
function is directly based on the physical phenomena:
gravity, natural convection and/or evaporation. Therefore the
effectiveness is independent of operator actions and smaller
failure rates are assigned to passive safety systems.
For the experimental investigation of the operation mode and
the effectiveness of these passive safety systems the multipurpose
thermohydraulic test facility NOKO (NOKO is an abbreviation for
the German translation of emergency condenser) was constructed
at the Forschungszentrum Jülich (FZJ). The facility has a maximum
power of 4 MW for steam production and a maximum operating pressure
of 10 MPa.

In the frame of an European Union programme (EU BWR R&D Cluster),
six test series with an emergency condenser test bundle were
performed in 1996. Within the Physics and Thermalhydraulics
Complementary Actions (BWR/CA) to the EU BWR R&D Cluster the
German Forschungszentrum Rossendorf (FZR) e.V. and the French
Commisariat a'l Energie Atomique (CEA/DRN) have calculated 9 tests
and an additional blind test of the NOKO bundle experiments. These
posttest calculations were carried out using ATHLET (FZR) and
CATHARE2 (CEA/DRN). The results of these calculations are presented
in this paper.

Detailed comparisons of ATHLET and CATHARE results show that despite
the good prediction of global parameters for both codes, the variations
of local parameters calculated (e.g., film velocity and temperature)
are not in such a good agreement. This can be explained by some
compensating errors in computer codes (e.g., an overestimation of
the condensing film velocity can hide an error in the condensation
correlation) and the significant effect of the tube wall conduction
in controlling the heat transfer. The emergency condenser test bundle
of the available and considered experiments were not instrumented.
Therefore a deeper analysis (including a detailed comparison of local
parameters) is not possible. New test series released in the frame of
a new European union action will be analyzed in 1998.
]]></dc:description>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1135-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1135-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Dumaz, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1135-7</dc:identifier>
<dc:title><![CDATA[Post-Test Calculations of NOKO Emergency Condenser Experiments]]></dc:title>
<dc:source><![CDATA[ICONE 6 - 6th International Conference on Nuclear Engineering , 10.-14. Juni 1998, San Diego, Californien, Beitrag 6382]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The SWR1000 is a new innovative boiling water reactor concept,
which is developed by Siemens AG. This concept is characterized
in particular by passive safety systems (e.g., four emergency
condensers, four building condensers, eight passive pressure
pulse transmitters, six gravitydriven core flooding lines).
Passive safety systems need no external energy sources. The
function is directly based on the physical phenomena:
gravity, natural convection and/or evaporation. Therefore the
effectiveness is independent of operator actions and smaller
failure rates are assigned to passive safety systems.
For the experimental investigation of the operation mode and
the effectiveness of these passive safety systems the multipurpose
thermohydraulic test facility NOKO (NOKO is an abbreviation for
the German translation of emergency condenser) was constructed
at the Forschungszentrum Jülich (FZJ). The facility has a maximum
power of 4 MW for steam production and a maximum operating pressure
of 10 MPa.

In the frame of an European Union programme (EU BWR R&D Cluster),
six test series with an emergency condenser test bundle were
performed in 1996. Within the Physics and Thermalhydraulics
Complementary Actions (BWR/CA) to the EU BWR R&D Cluster the
German Forschungszentrum Rossendorf (FZR) e.V. and the French
Commisariat a'l Energie Atomique (CEA/DRN) have calculated 9 tests
and an additional blind test of the NOKO bundle experiments. These
posttest calculations were carried out using ATHLET (FZR) and
CATHARE2 (CEA/DRN). The results of these calculations are presented
in this paper.

Detailed comparisons of ATHLET and CATHARE results show that despite
the good prediction of global parameters for both codes, the variations
of local parameters calculated (e.g., film velocity and temperature)
are not in such a good agreement. This can be explained by some
compensating errors in computer codes (e.g., an overestimation of
the condensing film velocity can hide an error in the condensation
correlation) and the significant effect of the tube wall conduction
in controlling the heat transfer. The emergency condenser test bundle
of the available and considered experiments were not instrumented.
Therefore a deeper analysis (including a detailed comparison of local
parameters) is not possible. New test series released in the frame of
a new European union action will be analyzed in 1998.
]]></dc:description>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1135-7</dc:relation>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1155-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Voigt, A.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Kirmse, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1155-1</dc:identifier>
<dc:title><![CDATA[The existence of [ReNF<SUB>4</SUB>]<SUP>-</SUP> - an EPR study]]></dc:title>
<dc:source><![CDATA[Inorg. Chem. Communications  1 (1998) 141-142]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1155-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1166-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Puers, C.]]></dc:creator>
<dc:creator><![CDATA[Kampf, G.]]></dc:creator>
<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1166-2</dc:identifier>
<dc:title><![CDATA[Investigation of Bacterial Diversity in Soil of a Depleted Saxonian Uranium Mine via 16S rRNA Gene and 16S/23S Intergenic Spacer Analyses]]></dc:title>
<dc:source><![CDATA[International Symposium on Microbial Ecology ISME-8, Halifax, Kanada, 9.-14.8.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1166-2</dc:relation>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1166-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Puers, C.]]></dc:creator>
<dc:creator><![CDATA[Kampf, G.]]></dc:creator>
<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1166-1</dc:identifier>
<dc:title><![CDATA[Investigation of Bacterial Diversity in Soil of a Depleted Saxonian Uranium Mine via 16S rRNA Gene and 16S/23S Intergenic Spacer Analyses]]></dc:title>
<dc:source><![CDATA[International Symposium on Microbial Ecology ISME-8, Halifax, Kanada, 9.-14.8.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
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<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1166-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1042-1</identifier>
<datestamp>2023-05-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pham, M. T.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Seifarth, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1042-1</dc:identifier>
<dc:title><![CDATA[Surface Roughness with Nanometer-Scale Ag Particles Generated by Ion Implantation]]></dc:title>
<dc:source><![CDATA[Analytica Chimica Acta 350 (1997) 209-220]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Surfaces of SiO2, Si3N4, Ta2O5 and glass were implanted
with Ag+ ions. Studies using X-ray diffraction (XRD) and atomic force microscopy
(AFM) show that the surface morphology is dominated by metallic silver
features consisting of regularly shaped, mostly spherical, Ag particles
spanning a size range from some nanometers to some 100 nm in diameter.
The particle size metrics, distribution, shape, and their density are shown
to be controlled by the process paramters ion dose, dose rate, and ion
energy. Adjusting the energy of the incident ions results in various degrees
of submerging into the substrate including exposed Ag features anchored
onto the surface or buried Ag particles overcoated by a thin layer of the
matrix material. The substrate material differs by its ability of stabilizing
the dispersion and blocking the Ag movement. Ta2O5 and glass substrates
provide more homogeneously dispersed Ag particles, much smaller in size
and regularly shaped compared to SiO2 and Si3N4 substrate systems. Potential
application refers to surface enhanced Raman scattering.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0003-2670(97)00294-8]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1042-1</dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:299-1</identifier>
<datestamp>2020-12-11</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heide, B.]]></dc:creator>
<dc:creator><![CDATA[Barz, H.-W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-299-1</dc:identifier>
<dc:title><![CDATA[Collective Effects and Multifragmentation in Heavy Ion Collisions at Intermediate Energies within a Hybrid Model]]></dc:title>
<dc:source><![CDATA[Nuclear Physics A 588 (1995) pp. 918]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/0375-9474(95)00131-J]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-299-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:299-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Heide, B.]]></dc:creator>
<dc:creator><![CDATA[Barz, H.-W.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-299-2</dc:identifier>
<dc:title><![CDATA[Collective Effects and Multifragmentation in Heavy Ion Collisions at Intermediate Energies within a Hybrid Model]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-71 Preprint]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/preprint</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-299-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:300-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Treuner, M.]]></dc:creator>
<dc:creator><![CDATA[Langbein, D.]]></dc:creator>
<dc:creator><![CDATA[Galindo, V.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-300-1</dc:identifier>
<dc:title><![CDATA[Thermocapillary Bubble and Drop Migration in a Drop Tower Experiment]]></dc:title>
<dc:source><![CDATA[9th European Aymposium "Gravity Dependent Phenomena", Berlin, May 1995]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-300-1</dc:relation>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:301-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Priede, J.]]></dc:creator>
<dc:creator><![CDATA[Thess, A.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-301-1</dc:identifier>
<dc:title><![CDATA[Oblique hydrothermal wave instability of thermocapillary driven convection in a coplanar magnetic field]]></dc:title>
<dc:source><![CDATA[9th European Symposium "Gravity Dependet Phenomena", Berlin, May 1995 und MAHID 95 - Konferenz, Riga, August 1995]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-301-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:302-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Langenbrunner, H.]]></dc:creator>
<dc:creator><![CDATA[Witke, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-302-1</dc:identifier>
<dc:title><![CDATA[Heat transfer experiments in a turbulent sodium MHD channel flow]]></dc:title>
<dc:source><![CDATA[MAHID 95 - Konferenz, August 1995, Riga]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-302-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:303-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:description><![CDATA[The goal of this work was to evaluate the potential of small YAP:Ce crystals, especially designed for a high-resolution PET system. We directly compared the scintillator properties of 3x3x20 mm<SUP>3</SUP> crystals YAP with those of BGO. The light output, energy resolution, detection efficiency and timing properties for the irradiation using <SUP>137</SUP>Cs and <SUP>22</SUP>Na sources were investigated. Special consideration was given to the influence of the reflector coating on the light output as well as on the overall performance of the quality of the studied crystals.]]></dc:description>
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<dc:title><![CDATA[Computer Simulation of Ion-Assisted Thin Film Deposition]]></dc:title>
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<dc:title><![CDATA[Ion Beam Synthesis of Gold Nanoclusters in SiO<SUB>2</SUB>: Computer Simulations versus Experiments]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 147 (1999) 343-349]]></dc:source>
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<dc:title><![CDATA[Ion Beam Synthesis of Gold Nanoclusters in SiO<SUB>2</SUB>: Computer Simulations versus Experiments]]></dc:title>
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<dc:description><![CDATA[The further miniaturization of silicon micromechanical
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at the mm- and sub-mm level will lead to a new generation of microdevices.
A modern technique to fabricate three dimensional micromechanical structures
is the combination of high concentration p+-doping by writing ion implantation
using a focused ion beam (FIB) and subsequent anisotropic and selective
wet chemical etching. FIB patterned and chemical etched 3D structures have
been fabricated using 35 keV Ga+-ion implantation and subsequent anisotropic
etching in KOH/H2O-solution. The Ga+-FIB patterned test structures were
characterized by scanning electron microscopy.]]></dc:description>
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<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-688-1</dc:identifier>
<dc:title><![CDATA[Writing FIB Implantation an Subsequent Anisotropic Wet Chemical Etching for Fabrication of 3D Structures in Silicon]]></dc:title>
<dc:source><![CDATA[EUROSENSORS X, 8.-11.9.1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The further miniaturization of silicon micromechanical
structures in combination with the high developed microelectronic technology
at the mm- and sub-mm level will lead to a new generation of microdevices.
A modern technique to fabricate three dimensional micromechanical structures
is the combination of high concentration p+-doping by writing ion implantation
using a focused ion beam (FIB) and subsequent anisotropic and selective
wet chemical etching. FIB patterned and chemical etched 3D structures have
been fabricated using 35 keV Ga+-ion implantation and subsequent anisotropic
etching in KOH/H2O-solution. The Ga+-FIB patterned test structures were
characterized by scanning electron microscopy.]]></dc:description>
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<dc:creator><![CDATA[Pacaud, Y.]]></dc:creator>
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<dc:identifier>https://www.hzdr.de/publications/Publ-553-2</dc:identifier>
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<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 120 (1996) 114-120]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[A short review is presented concerning problems of ion beam processing of single crystalline silicon carbide. Emphasis is given
to recent results on point defect, extended defects, amorphization and recrystallization, electrical activation of dopant atoms, and metallization.]]></dc:description>
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<dc:creator><![CDATA[Voigt, A.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Kirmse, R.]]></dc:creator>
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<dc:title><![CDATA[Zur Existenz von [ReNCl<SUB>4-n</SUB>F<SUB>n</SUB>]<SUP>-</SUP> (n=1-3) Nitridorhenat(VI)-Gemischtligandenkomplexen - eine EPR-Untersuchung]]></dc:title>
<dc:source><![CDATA[Zeitschrift für Naturforschung 53b, 1183-1187 (1998)]]></dc:source>
<dc:date>1998</dc:date>
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<dc:creator><![CDATA[Strieder, F.]]></dc:creator>
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<dc:creator><![CDATA[Imbriani, G.]]></dc:creator>
<dc:creator><![CDATA[Junker, M.]]></dc:creator>
<dc:creator><![CDATA[Becker, H. W.]]></dc:creator>
<dc:creator><![CDATA[Bemmerer, D.]]></dc:creator>
<dc:creator><![CDATA[Best, A.]]></dc:creator>
<dc:creator><![CDATA[Bonetti, R.]]></dc:creator>
<dc:creator><![CDATA[Broggini, C.]]></dc:creator>
<dc:creator><![CDATA[Caciolli, A.]]></dc:creator>
<dc:creator><![CDATA[Corvisiero, P.]]></dc:creator>
<dc:creator><![CDATA[Costantini, H.]]></dc:creator>
<dc:creator><![CDATA[Dileva, A.]]></dc:creator>
<dc:creator><![CDATA[Elekes, Z.]]></dc:creator>
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<dc:title><![CDATA[New experimental study of low-energy (p,gamma) resonances in magnesium isotopes]]></dc:title>
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<dc:date>2010</dc:date>
<dc:description><![CDATA[Proton captures on Mg isotopes play an important role in the Mg-Al cycle active in stellar H shell burning. In particular, the strengths of low-energy resonances with E < 200 keV in 25Mg(p,gamma)26Al determine the production of 26Al and a precise knowledge of these nuclear data is highly desirable. Absolute measurements at such low-energies are often very difficult and hampered by gamma-ray background as well as changing target stoichiometry during the measurements. The latter problem can be partly avoided using higher energy resonances of the same reaction as a normalization reference. Hence the parameters of suitable resonances have to be studied with adequate precision. In the present work we report on new measurements of the resonance strengths omega_gamma of the E = 214, 304, and 326 keV resonances in the reactions 24Mg(p,gamma)25Al, 25Mg(p,gamma)26Al, and 26Mg(p,gamma)27Al, respectively. These studies were performed at the LUNA facility in the Gran Sasso underground laboratory using multiple experimental techniques and provided results with a higher accuracy than previously achieved.]]></dc:description>
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<dc:creator><![CDATA[Limata, B.]]></dc:creator>
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<dc:creator><![CDATA[Lemut, A.]]></dc:creator>
<dc:creator><![CDATA[Marta, M.]]></dc:creator>
<dc:creator><![CDATA[Mazzocchi, C.]]></dc:creator>
<dc:creator><![CDATA[Menegazzo, R.]]></dc:creator>
<dc:creator><![CDATA[Prati, P.]]></dc:creator>
<dc:creator><![CDATA[Roca, V.]]></dc:creator>
<dc:creator><![CDATA[Rolfs, C.]]></dc:creator>
<dc:creator><![CDATA[Rossi Alvarez, C.]]></dc:creator>
<dc:creator><![CDATA[Salvo, C.]]></dc:creator>
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<dc:creator><![CDATA[Straniero, O.]]></dc:creator>
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<dc:title><![CDATA[New experimental study of low-energy (p,gamma) resonances in magnesium isotopes]]></dc:title>
<dc:source><![CDATA[Physical Review C 82(2010), 015801]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Proton captures on Mg isotopes play an important role in the Mg-Al cycle active in stellar H shell burning. In particular, the strengths of low-energy resonances with E < 200 keV in 25Mg(p,gamma)26Al determine the production of 26Al and a precise knowledge of these nuclear data is highly desirable. Absolute measurements at such low-energies are often very difficult and hampered by gamma-ray background as well as changing target stoichiometry during the measurements. The latter problem can be partly avoided using higher energy resonances of the same reaction as a normalization reference. Hence the parameters of suitable resonances have to be studied with adequate precision. In the present work we report on new measurements of the resonance strengths omega_gamma of the E = 214, 304, and 326 keV resonances in the reactions 24Mg(p,gamma)25Al, 25Mg(p,gamma)26Al, and 26Mg(p,gamma)27Al, respectively. These studies were performed at the LUNA facility in the Gran Sasso underground laboratory using multiple experimental techniques and provided results with a higher accuracy than previously achieved.]]></dc:description>
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<dc:creator><![CDATA[Zotti, L. A.]]></dc:creator>
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<dc:description><![CDATA[A combined experimental and theoretical study is presented revealing the influence of metal-molecule coupling on electronic transport through single-molecule junctions. Transport experiments through tolane molecules attached to gold electrodes via thiol, nitro, and cyano anchoring groups are performed. By fitting the experimental current-voltage characteristics to a single-level tunneling model, we extract both the position of the molecular orbital closest to the Fermi energy and the strength of the metal-molecule coupling. The values found for these parameters are rationalized with the help of density-functional-theory-based transport calculations. In particular, these calculations show that the anchoring groups determine the junction conductance by controlling not only the strength of the coupling to the metal but also the position of the relevant molecular energy levels.]]></dc:description>
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<dc:title><![CDATA[Ion Drift Behaviour in Borosilicate Glasses during Anodic Bonding to Silicon or Metals]]></dc:title>
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<dc:title><![CDATA[Speziation des Urans- Bestimmung und Berechnung unter natürlichen Bedingungen]]></dc:title>
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<dc:title><![CDATA[Determination of Molecular-Level Structural Information of Uranium in Environmentally Relevant Samples by EXAFS]]></dc:title>
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<dc:title><![CDATA[Determination of Molecular-Level Structural Information of Uranium in Environmentally Relevant Samples by EXAFS]]></dc:title>
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<dc:creator><![CDATA[Rettig, D.]]></dc:creator>
<dc:creator><![CDATA[Merker, P.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1122-1</dc:identifier>
<dc:title><![CDATA[Particle emission from UV-irradiated silica surfaces]]></dc:title>
<dc:source><![CDATA[Journal of Aerosol Science Vol.29, Suppl.1, pp. S921-S922 (1998)]]></dc:source>
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<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:creator><![CDATA[Rettig, D.]]></dc:creator>
<dc:creator><![CDATA[Merker, P.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1122-2</dc:identifier>
<dc:title><![CDATA[Particle emission from UV-irradiated silica surfaces]]></dc:title>
<dc:source><![CDATA[5th International Aerosol Conference, Edinburgh, 12-18.Sept.,1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1123-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Griffith, D. V.]]></dc:creator>
<dc:creator><![CDATA[Parrott, J.]]></dc:creator>
<dc:creator><![CDATA[Togrou, M.]]></dc:creator>
<dc:creator><![CDATA[Dilworth, J. R.]]></dc:creator>
<dc:creator><![CDATA[Zheng, Y.]]></dc:creator>
<dc:creator><![CDATA[Ritter, S.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1123-1</dc:identifier>
<dc:title><![CDATA[Synthesis and Crystal Structure of Novel Tetrameric Nitrido Complexes]]></dc:title>
<dc:source><![CDATA[Zeitschrift für anorganische und allgemeine Chemie 624 (1998) 1409-1414]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1124-1</identifier>
<datestamp>2023-05-02</datestamp>
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<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Brutscher, J.]]></dc:creator>
<dc:creator><![CDATA[Mändl, S.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1124-1</dc:identifier>
<dc:title><![CDATA[Utilization of Plasma Source Ion Implantation for Tribological Applications]]></dc:title>
<dc:source><![CDATA[Surface & Coatings Technology 96 (1997) pp. 16-21]]></dc:source>
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<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1126-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Schleif, M.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1126-1</dc:identifier>
<dc:title><![CDATA[Solitonische Feldkonfigurationen des Nambu & Jona-Lasinio-Modells im Medium]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-211]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/doctoralThesis</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1127-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Dobler, M.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1127-1</dc:identifier>
<dc:title><![CDATA[Untersuchung der Bildung der Eisensilizide während der Ionenstrahlsynthese und der ionenstrahlinduzierten Phasenbildung]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-214; TU Dresden, 23. 01. 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/doctoralThesis</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
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<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:698-1</identifier>
<datestamp>2022-05-24</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Weishart, H.]]></dc:creator>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-698-1</dc:identifier>
<dc:title><![CDATA[Ion Beam Assisted Deposition of a tungsten Compound Layer on 6H-Silicon Carbide]]></dc:title>
<dc:source><![CDATA[Diamond and Related Materials 6 (1997) 1432-1435]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Ion beam assisted deposition (IBAD) as a means of synthesizing
a tungsten carbide layer on top of SiC is investigated by Rutherford Backscattering
(RBS), X-ray diffraction (XRD) and four point probe measurements. Evaporation
of tungsten and subsequent implantation of carbon leads to a crystalline
layer of tungsten carbide whose resistivity is 1554 mWcm. At an implantation
dose of 5x1017C+cm-2 enhanced surface erosion occurs. Simultaneous evaporation
of tungsten and implantation of carbon procedures a layer of crystalline
W2C mixed with tungsten. The resistivity of this layer is 400 mWcm, i.e.
only a factor of 5 higher than that of single crystal W2C.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:698-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Weishart, H.]]></dc:creator>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-698-2</dc:identifier>
<dc:title><![CDATA[Ion Beam Assisted Deposition of a tungsten Compound Layer on 6H-Silicon Carbide]]></dc:title>
<dc:source><![CDATA[1. Europ. Conf. "Selicon carbide and related materials", Heraclion/Crete, Greece, Oct. 6-9, 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Ion beam assisted deposition (IBAD) as a means of synthesizing
a tungsten carbide layer on top of SiC is investigated by Rutherford Backscattering
(RBS), X-ray diffraction (XRD) and four point probe measurements. Evaporation
of tungsten and subsequent implantation of carbon leads to a crystalline
layer of tungsten carbide whose resistivity is 1554 mWcm. At an implantation
dose of 5x1017C+cm-2 enhanced surface erosion occurs. Simultaneous evaporation
of tungsten and implantation of carbon procedures a layer of crystalline
W2C mixed with tungsten. The resistivity of this layer is 400 mWcm, i.e.
only a factor of 5 higher than that of single crystal W2C.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1222-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Barz, H.-U.]]></dc:creator>
<dc:creator><![CDATA[Böhmer, B.]]></dc:creator>
<dc:creator><![CDATA[Konheiser, J.]]></dc:creator>
<dc:creator><![CDATA[Stephan, I.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1222-1</dc:identifier>
<dc:title><![CDATA[Entwicklung einer fortgeschrittenen Methodik zur Bestimmung der Neutronenbelastung des Druckbehältermaterials vom Reaktor des Typs WWER-1000]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-222 Mai 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[In diesem Projekt wurden für die WWER-1000-Reaktoren Balakovo-3 und Rovno-3 die Parameter der Neutronenbelastung experimentell und theoretisch bestimmt. 
Der vorliegende Bericht beschreibt das methodische Vorgehen, welches aus dem reinen Berechnungsteil, der gammaspektrometrischen Analyse der Aktivierungsdetektoren und dem Vergleich der gemessenen und berechneten Werte einschließliche der Spektrumsjustierung besteht. Dieses Instrumentarium, welches allgemein bei der Bestimmung der Neutronenfluenz anwendbar ist, wurde im Projektzeitraum weiter verbessert. 
]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
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<dc:type>doc-type:report</dc:type>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1225-1</identifier>
<datestamp>2023-05-03</datestamp>
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</header>
<metadata>
<oai_dc:dc
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barz, H.-W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1225-1</dc:identifier>
<dc:title><![CDATA[Combined Effects of Nuclear Coulomb Field, Radial Flow and Opaqueness on Two-Pion Correlations]]></dc:title>
<dc:source><![CDATA[Physical Review C, Volume 59, Number 4, April 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevC.59.2214]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1225-1</dc:relation>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1227-1</identifier>
<datestamp>2023-05-03</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Wüst, F.]]></dc:creator>
<dc:creator><![CDATA[Carlson, K. E.]]></dc:creator>
<dc:creator><![CDATA[Katzenellenbogen, J. A.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1227-1</dc:identifier>
<dc:title><![CDATA[Synthesis and Binding Affinities of New 17a-Substituted Estradiol-Rhenium n+1 Mixed-Ligand and Thioether-Carbonyl Complexes]]></dc:title>
<dc:source><![CDATA[Steroids 63:665-671, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0039-128X(98)00079-8]]></dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:984-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Hicken, E. F.]]></dc:creator>
<dc:creator><![CDATA[Jaegers, H.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-984-1</dc:identifier>
<dc:title><![CDATA[Experimentelle Ergebnisse mit der NOKO-Versuchsanlage]]></dc:title>
<dc:source><![CDATA[VGB-Kraftwerkstechnik 78 (1998), Heft 5, ISSN 0372-5715, S. 90-96]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[On the NOKO (emergency condenser) test station constructed at Jülich Research Centre, the operating performance and effectiveness of the emergency condenser of the boiling water reactor 1000 have been determined in well over 200 tests. It has been possible to check that the tests were in close agreement with a modified version of ATHLET ]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:436-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-436-1</dc:identifier>
<dc:title><![CDATA[Übersicht zu Arbeiten des Institutes für Sicherheitsforschung des FZR]]></dc:title>
<dc:source><![CDATA[Seminarvortrag, Institut für Reaktorsicherheit im FZK, Karlsruhe, 23. Februar 1995]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:438-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-438-1</dc:identifier>
<dc:title><![CDATA[Akustische Lecküberwachung mit Neuronalen Netzen an Druckanlagen komplizierter Topologie]]></dc:title>
<dc:source><![CDATA[DECHEMA-Jahrestagung '95, Wiesbaden, 30.5.-1.6.1995, Band 3, S. 227-228]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:441-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Valko, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-441-1</dc:identifier>
<dc:title><![CDATA[Identification of Topics for Cooperation between the European Community and Eastern European Countries in the Field of Nuclear Reactor Safety, Radioactive Waste and Site Restoration]]></dc:title>
<dc:source><![CDATA[Study accomplished by order of EU DG XII, Rossendorf, 1995]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
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<identifier>HZDR:PUBLDB:443-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Steiff, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-443-1</dc:identifier>
<dc:title><![CDATA[Anwendungsmöglichkeiten neuartiger EDV-gestützter Erkennungsmethoden zur Identifikation gefährlicher Betriebszustände in Chemieanlagen]]></dc:title>
<dc:source><![CDATA[Preprints des Workshops "Reaktionsführung bei chem. Synthesen im techn. Maßstab mit Unterstützung durch moderne Methoden der EDV", Bonn, 24.5.95, S. 67 - 75]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
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<header>
<identifier>HZDR:PUBLDB:445-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Müller, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-445-1</dc:identifier>
<dc:title><![CDATA[Hadron Production in pBe interactions at 14.6 GeV/c]]></dc:title>
<dc:source><![CDATA[Zeitschrift für Physik A 353 (1995) pp. 237]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Invariant cross sections for the production of π<sup>±</sup>, <i>K</i><sup>±</sup>,  <i>p</i> and <i>d</i> in <i>p</i>Be interactions at 14.6 GeV/c are well reproduced by calculations carried out in the framework of the Rossendorf collision model.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-445-1</dc:relation>
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<header>
<identifier>HZDR:PUBLDB:447-1</identifier>
<datestamp>2021-11-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Hempel, A.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Eichhorn, F.]]></dc:creator>
<dc:creator><![CDATA[Riekel, C.]]></dc:creator>
<dc:creator><![CDATA[Engstroem, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-447-1</dc:identifier>
<dc:title><![CDATA[SAXS Investigation of the Structural Changes in the Plastic Zone Ahead of a Crack Tip in Ductile Metals]]></dc:title>
<dc:source><![CDATA[Journal of Molecular Structure 383 (1996) pp. 267-270]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0022-2860(96)09297-6]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:449-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:date>1998</dc:date>
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<dc:title><![CDATA[Annealing and Recrystallization of Amorphous Silicon Carbide Produced by Ion Implantation]]></dc:title>
<dc:source><![CDATA[ECSCRM '98 (2nd European Conf. on Silicon Carbide and Related Materials), Montpellier, Sept. 2 - 4, 1998]]></dc:source>
<dc:date>1998</dc:date>
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<dc:title><![CDATA[Annealing and Recrystallization of Amorphous Silicon Carbide Produced by Ion Implantation]]></dc:title>
<dc:source><![CDATA[Journal of Applied Physics Vol. 84, Number 9, 1. Nov. 1998, pp. 4769-4774]]></dc:source>
<dc:date>1998</dc:date>
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<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Abram, S.]]></dc:creator>
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<dc:title><![CDATA[Synthesis, Characterization and Structure of bis{2-[1-(thiosemicarbazono)ethyl]pyridinium}hexanitratothorate(IV)]]></dc:title>
<dc:source><![CDATA[J. Chem. Cryst.]]></dc:source>
<dc:date>1998</dc:date>
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<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Mack, J.]]></dc:creator>
<dc:creator><![CDATA[Ortner, K.]]></dc:creator>
<dc:creator><![CDATA[Müller, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1151-1</dc:identifier>
<dc:title><![CDATA[Reactions of Dichloro[2-(dimethylaminomethyl)phenyl-C<SUP>1</SUP>,N]gold(III), [Au(damp-C<SUP>1</SUP>,N)Cl<SUB>2</SUB>], with heterocyclic thiols. Evidence for Au-N bond cleavage and protonation of the dimethylamino group]]></dc:title>
<dc:source><![CDATA[J. Chem. Soc. Dalton Trans. 1998, Pages 1011-1019]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Schulz-Lang, E.]]></dc:creator>
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<dc:title><![CDATA[Tris(selenophenyl)methane]]></dc:title>
<dc:source><![CDATA[Acta Crystallographica (1998) C55, 1010-1011]]></dc:source>
<dc:date>1998</dc:date>
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<dc:creator><![CDATA[Schulz-Lang, E.]]></dc:creator>
<dc:creator><![CDATA[Vasquez-Lopez, E.]]></dc:creator>
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<dc:title><![CDATA[Synthesis and Crystal Structures of [TeI<SUB>3</SUB>][GaI<SUB>4</SUB>] and [TeI<SUB>3</SUB>][InI<SUB>4</SUB>]]]></dc:title>
<dc:source><![CDATA[Z. anorg. allg. Chem. 624 (1998) 999-102]]></dc:source>
<dc:date>1998</dc:date>
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<dc:creator><![CDATA[Lindau, B.]]></dc:creator>
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<dc:title><![CDATA[Anwendung wissensbasierter Methoden auf der Grundlage von Insitu-Messung und qualitativer Modellierung zur Optimierung von Schüttguthandhabungstechniken am Beispiel des Dosierens]]></dc:title>
<dc:source><![CDATA[49.Berg- und Hüttenmännischer Tag 1998 in Freiberg, S. 325-333]]></dc:source>
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<dc:title><![CDATA[Anwendung wissensbasierter Methoden auf der Grundlage von Insitu-Messung und qualitativer Modellierung zur Optimierung von Schüttguthandhabungstechniken am Beispiel des Dosierens]]></dc:title>
<dc:source><![CDATA[Freiberger Forschungshefte A 841 Grundstoff-Verfahrenstewchnik 1998, Technische Universität Bergakademie Freiberg Partikeltechnologie: Vorträge und Poster zum 49.Berg-und Hüttenmännischen Tag 1998 in Freiberg, S. 325-333]]></dc:source>
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
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<dc:title><![CDATA[Theoretische Modellierung des Druckbehälters und der Druckbehältereinbauten eines Siedewasserreaktors (SWR), Abschlußbericht]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-147 (nur für den internen dienstlichen Gebrauch), August 1996]]></dc:source>
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<identifier>HZDR:PUBLDB:1156-1</identifier>
<datestamp>2023-05-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Jankowsky, R.]]></dc:creator>
<dc:creator><![CDATA[Friebe, M.]]></dc:creator>
<dc:creator><![CDATA[Noll, B.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1156-1</dc:identifier>
<dc:title><![CDATA[Determination of Dissociation Constants of <sup>99m</sup>Technetium Radiopharmaceuticals by Capillary Electrophoresis]]></dc:title>
<dc:source><![CDATA[Journal Chromatography A, 833 (1999) 83-96]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Capillary electrophoresis was applied to investigate pK<sub>a</sub> values of <sup>99m</sup>Tc radiotracers used in nuclear medicine. Therefore, the protonation equilibria of the carboxyl groups of <sup>99m</sup>Tc- mercaptoacetylglycylglycylglycine (<sup>99m</sup>Tc-MAG<sub>3</sub>) and <sup>99m</sup>Tc-ethylenecysteine dimer (<sup>99m</sup>Tc-EC) were studied by pH-dependent determination of electrophoretical velocities. <sup>99m</sup>ethylenecysteine dimer diethyl ester (<sup>99m</sup>Tc-ECD) was used as a non-protonable standard. The capillary electrophoresis system was equipped with a radioactivity detector. Measurements were performed using a pressure-driven capillary zone electrophoresis which allowed runs even in the low pH range. For the determination of pK<sub>a</sub> values, the electrophoretical velocities of the analytes were referred to the electrophoretical velocities of tetraphenyle arsonium chloride as a positively charged marker. Calculation of pK<sub>a</sub> values was accomplished by non-linear curve fitting of both structure-based equilibria equations and sigmoidal decay functions to the experimental data. <sup>99m</sup>Tc-MAG<sub>3</sub> was shown to have a carboxyl group pK<sub>a</sub> value of 4.22. the value for the carboxyl groups of <sup>99m</sup>Tc-EC is 2.90 (determined by structure-based equilibria equations), which represents a common value for both carboxyl groups. By the use of sigmoidal functions, similar values were elucidated. As expected, <sup>99m</sup>Tc-ECD shows no protonation step.]]></dc:description>
<dc:subject><![CDATA[Dissociation constants]]></dc:subject>
<dc:subject><![CDATA[Pharmaceutical analysis]]></dc:subject>
<dc:subject><![CDATA[Technetium]]></dc:subject>
<dc:subject><![CDATA[Metal complexes]]></dc:subject>
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<identifier>HZDR:PUBLDB:1160-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Förster, E.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1160-1</dc:identifier>
<dc:title><![CDATA[Anodic Oxidation of the Carbon-14-labelled Organic Waste]]></dc:title>
<dc:source><![CDATA[13th Radiochemical Conference, Marianske Lazne, 19.-24.4.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Barium carbonate is a widely accepted stable chemical form for the safe disposal of carbon-14. This requires, however, oxidation of carbon-14-containing organic waste to carbon dioxide. We habe developed a method for the mineralization of organic compounds by anodic oxidation in silver-sulfate-containing sulfuric-chromic acid. This process can also be used for complete oxidation of "difficult" organic wastes, such as hydrophobic substances like hydrocarbons, plastics, activated carbon, etc. The generation of additional chromium-containing hazardous wastes are avoided in this process by electrolytically regenerating chromium(III) to chromium(VI). The degradation of C-14 labeled organic compounds during the process is monitored by on-line measurement the β-radiation of the produced <sup>14</sup>CO<sub>2</sub>]]></dc:description>
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<dc:title><![CDATA[Investigations of the Structural Changes Ahead of a Crack Tip in Ductile Aluminium Using Scanning Micro-Beam Small Angle X-Ray Scattering]]></dc:title>
<dc:source><![CDATA[J. Material Science Letters 17 (1998) 1631]]></dc:source>
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<dc:creator><![CDATA[Wober, J.]]></dc:creator>
<dc:creator><![CDATA[Flemming, K.]]></dc:creator>
<dc:creator><![CDATA[Hard, B. C.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, K.]]></dc:creator>
<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1162-1</dc:identifier>
<dc:title><![CDATA[Comparison of Desulfovibrio Isolates Recovered from a Uranium Waste Heap and Other Environments]]></dc:title>
<dc:source><![CDATA[Uranium Mining and Hydrogeology II, Freiberg, Germany, 15.-17.09.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Pietzsch, K.]]></dc:creator>
<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
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<dc:title><![CDATA[Comparison of Desulfovibrio Isolates Recovered from a Uranium Waste Heap and Other Environments]]></dc:title>
<dc:source><![CDATA[Uranium Mining and Hydrogeology II, Freiberg, Germany, 15.-17.09.1998]]></dc:source>
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<dc:creator><![CDATA[Wober, J.]]></dc:creator>
<dc:creator><![CDATA[Flemming, K.]]></dc:creator>
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<dc:creator><![CDATA[Pietzsch, K.]]></dc:creator>
<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1162-3</dc:identifier>
<dc:title><![CDATA[Comparison of Desulfovibrio Isolates Recovered from a Uranium Waste Heap and Other Environments]]></dc:title>
<dc:source><![CDATA[Euroconference: Bacterial-Metal/Radionuclide Interaction, Rossendorf/Dresden, Germany, 02.-04.12.1998]]></dc:source>
<dc:date>1998</dc:date>
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<identifier>HZDR:PUBLDB:1163-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kutschke, S.]]></dc:creator>
<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:creator><![CDATA[Otto, A.]]></dc:creator>
<dc:creator><![CDATA[Panak, P.]]></dc:creator>
<dc:creator><![CDATA[Geipel, G.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1163-1</dc:identifier>
<dc:title><![CDATA[Molecular Characterization of Thiobacillus Strains Recovered from Uranium Waste Piles]]></dc:title>
<dc:source><![CDATA[Uranium Mining and Hydrology II, Freiberg, Germany, 15.-17.9.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1233-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Enghardt, W.]]></dc:creator>
<dc:creator><![CDATA[Haberer, T.]]></dc:creator>
<dc:creator><![CDATA[Hasch, B.-G.]]></dc:creator>
<dc:creator><![CDATA[Hinz, R.]]></dc:creator>
<dc:creator><![CDATA[Jäkel, O.]]></dc:creator>
<dc:creator><![CDATA[Krämer, M.]]></dc:creator>
<dc:creator><![CDATA[Lauckner, K.]]></dc:creator>
<dc:creator><![CDATA[Pawelke, J.]]></dc:creator>
<dc:creator><![CDATA[Sobiella, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1233-1</dc:identifier>
<dc:title><![CDATA[Positronen Emissions Tomographie für die Qualitätskontrolle der Strahlentherapie mit <SUP>12</SUP>C-Ionen.]]></dc:title>
<dc:source><![CDATA[29. Tagung der Deutschen Gesellschaft für Medizinische Physik, Dresden, 14-17 Okt, 1998
<br>
L. Voigtmann, P. Geyer (Eds.), Tagungsband (1998) 125-126]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1233-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Enghardt, W.]]></dc:creator>
<dc:creator><![CDATA[Haberer, T.]]></dc:creator>
<dc:creator><![CDATA[Hasch, B.-G.]]></dc:creator>
<dc:creator><![CDATA[Hinz, R.]]></dc:creator>
<dc:creator><![CDATA[Jäkel, O.]]></dc:creator>
<dc:creator><![CDATA[Krämer, M.]]></dc:creator>
<dc:creator><![CDATA[Lauckner, K.]]></dc:creator>
<dc:creator><![CDATA[Pawelke, J.]]></dc:creator>
<dc:creator><![CDATA[Sobiella, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1233-7</dc:identifier>
<dc:title><![CDATA[Positronen Emissions Tomographie für die Qualitätskontrolle der Strahlentherapie mit <SUP>12</SUP>C-Ionen.]]></dc:title>
<dc:source><![CDATA[29. Tagung der Deutschen Gesellschaft für Medizinische Physik, Dresden, 14-17 Okt, 1998
<br>
L. Voigtmann, P. Geyer (Eds.), Tagungsband (1998) 125-126]]></dc:source>
<dc:date>1998</dc:date>
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<identifier>HZDR:PUBLDB:1234-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Geipel, G.]]></dc:creator>
<dc:creator><![CDATA[Rutsch, M.]]></dc:creator>
<dc:creator><![CDATA[Brendler, V.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1234-1</dc:identifier>
<dc:title><![CDATA[Laserspektroskopische Untersuchungen zur Bestimmung der Speziation von Schwermetallionen in Abwässern von Aufbereitungsprozessen]]></dc:title>
<dc:source><![CDATA[GDCh Umwelttagung Karlsruhe Sept. 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1235-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Römer, J.]]></dc:creator>
<dc:creator><![CDATA[Füchtner, F.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1235-1</dc:identifier>
<dc:title><![CDATA[Automated Production of the PET Tracer 16 alpha-[<SUP>18</SUP>F] Fluoroestradiol for Breast Cancer Imaging]]></dc:title>
<dc:source><![CDATA[Nucl. Med. Biol. 26 (1999) 473-479]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<identifier>HZDR:PUBLDB:1240-1</identifier>
<datestamp>2023-05-03</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gong, M.]]></dc:creator>
<dc:creator><![CDATA[Reddy, C. V.]]></dc:creator>
<dc:creator><![CDATA[Beling, C. D.]]></dc:creator>
<dc:creator><![CDATA[Fung, S.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Wirth, H.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1240-1</dc:identifier>
<dc:title><![CDATA[Deep Level Traps in the Extended Tail Region of Boron-Implanted n-Type 6H-SiC]]></dc:title>
<dc:source><![CDATA[Applied Physics Letters, Volume 72, Number 21, pp. 2739-2741]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Deep traps in the boron extended tail region of ion implanted 6HSiC pn junctions formed during annealing have been studied
using deep level transient spectroscopy. Dramatically high concentrations of ~ 1016 cm3 of the D center have been observed
through the unusual appearance of minority peaks in the majority carrier spectra. No evidence is found for any shallow boron
acceptor in this region, but an induced hole trap Ih at EV + 0.46 eV is found under cold implantation conditions. These results
support the picture of the extended tail, rich in boron-vacancy complexes such as the D center, which forms as a result of vacancy
enhanced indiffusion. The dominance of the electrically active D center in the depletion layer of the technologically important SiC
pn junction diode suggests the need for further research in this area. © 1998 American Institute of Physics.]]></dc:description>
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<identifier>HZDR:PUBLDB:1232-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:title><![CDATA[Defect Production and Evolution During and After Ion Implantation Studied by a Combination of Time-Ordered BCA and MD Simulations]]></dc:title>
<dc:source><![CDATA[12th International Conference on Ion Implantation Technology, June 22-26, 1998, Kyoto/Japan]]></dc:source>
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<dc:description><![CDATA[A novel method is applied to investigate the as-implanted defect structure formed during keV implantation into Si. It uses a combination of time-ordered computer simulations based on the binary collision approximation (BCA) and classical molecular dynamics (MD) simulations.The as-implanted damage created in 30 keV P+, 15 keV  As+, and 15 keV B+ implants is analyzed and depth profiles of different defect species are given.]]></dc:description>
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<dc:title><![CDATA[The Canonical Form of the Transition Matrix Elements]]></dc:title>
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<dc:title><![CDATA[Bericht der Frühjahrstagung der Studiengruppe für Elektronische Instrumentierung vom 30. März bis 1. April 1998 bei DESY in Hamburg]]></dc:title>
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<dc:title><![CDATA[Tribological Properties and Hardness of Silicon Nitride Ceramics after Ion Implantation and Subsequent Annealing]]></dc:title>
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<dc:title><![CDATA[Crystallization and Surface Erosion of SiC by Ion Irradiation at Elevated Temperatures]]></dc:title>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
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<dc:title><![CDATA[Anwendung von Kleinwinkelstreuverfahren zum Nachweis verformungsbedingter Strukturschädigung]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-229]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Der Einfluß plastischer Verformung nach einsinniger Zug- und Biegebelastung auf die Kleinwinkelstreuintensität wurde an technischen Al-Legierungen untersucht.
Bei geeigneter Versuchstechnik lassen sich sowohl mit Röntgenstrahlung als auch mit Neutronen verformungsbedingte Effekte nachweisen. Sie sind im Einschnürbereich einer Zugprobe als Porenstreuung und im Bereich vor der Rißspitze von biegeverformtem, hochduktilem Aluminium als Streuung an Versetzungsstrukturen zu interpretieren. Durch punktförmiges Abtasten mit einem stark fokussierten Synchrotron-Röntgenstrahl können inhomogene Schädigungsstrukturen mit hoher Ortsauflösung nachgewiesen werden. Diese mit SM-SAXS (Scanning Microbeam - Small Angle X-ray Scattering) bezeichnete Technik ist ein Schritt zur Entwicklung eines
Kleinwinkelstreu-Mikroskops.

Small Angle Scattering Characterization of deformation-damaged microstructure
The microstructural changes preceding the ductile fracture were investigated by small angle scattering methods at commercial Al alloys. Within the necking region of tensile deformed specimens additional small angle scattering effects can be measured. They are in agreement with the assumption of pore scattering. The inhomogeneous deformation field ahead the crack tip of a bended and precracked specimen can be monitored by scanning with a highly focussed X-ray beam of a Synchrotron source. In this case the scattering intensity decreases with increasing distance from the crack tip. The effect can be interpreted as scattering at the dislocation arrangements. The used scanning microbeam small angle X-ray scattering technique is a first step to the development of a "small angle scattering microscope".]]></dc:description>
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<dc:creator><![CDATA[Skoda, S.]]></dc:creator>
<dc:creator><![CDATA[Fiedler, B.]]></dc:creator>
<dc:creator><![CDATA[Becker, F.]]></dc:creator>
<dc:creator><![CDATA[Eberth, J.]]></dc:creator>
<dc:creator><![CDATA[Freund, S.]]></dc:creator>
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<dc:creator><![CDATA[Stuch, O.]]></dc:creator>
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<dc:creator><![CDATA[Jungclaus, A.]]></dc:creator>
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<dc:creator><![CDATA[Lieb, K. P.]]></dc:creator>
<dc:creator><![CDATA[Teich, C.]]></dc:creator>
<dc:creator><![CDATA[Ender, C.]]></dc:creator>
<dc:creator><![CDATA[Härtlein, T.]]></dc:creator>
<dc:creator><![CDATA[Köck, F.]]></dc:creator>
<dc:creator><![CDATA[Schwalm, D.]]></dc:creator>
<dc:creator><![CDATA[Baumann, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1261-1</dc:identifier>
<dc:title><![CDATA[Identification of Excited States in the <SUP>68</SUP>Se with Cluster Detectors]]></dc:title>
<dc:source><![CDATA[Physical Review C Volume 58 Number 1 July 1998 PRC 58 R5-R9]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1263-1</identifier>
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<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1263-1</dc:identifier>
<dc:title><![CDATA[Bakterielle Diversität in uranhaltigen Abraumhalden und Absetzbecken]]></dc:title>
<dc:source><![CDATA[WGL-Tagung: Biodiversität; 17.-19.11.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1265-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Panda, B.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1265-1</dc:identifier>
<dc:title><![CDATA[Positron affinities and deformation potentials in cubic]]></dc:title>
<dc:source><![CDATA[Acta Physica Polonica A 95 (1999) 641-646]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1266-1</identifier>
<datestamp>2023-05-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gallmeister, K.]]></dc:creator>
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<dc:creator><![CDATA[Pavlenko, O. P.]]></dc:creator>
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<dc:title><![CDATA[Can One Discriminate the Thermal Dilepton Signal Against the Open Charm and Bottom Decay Background in Ultrarelativistic Heavy-Ion Collisions?]]></dc:title>
<dc:source><![CDATA[European Physical Journal C 8 (1999) 473-478]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Abstract
In ultrarelativistic heavy-ion collisions at √s > 20 (120) A GeV a copious production of charm (bottom) production sets in which, via correlated semileptonic DD (BB) decays, gives rise to a dilepton yield at invariant mass M ≈ 2 - 3 GeV in excess of the Drell-Yan yield and the thermal dilepton signal from deconfined matter as well. We show that appropriate single-electron transverse momentum cuts (suitable for ALICE at LHC) cause a threshold like behavior of the dilepton spectra from heavy-quark meson decays and the Drell-Yan process and can allow to observe a thermal dilepton signal from hot deconfined matter.]]></dc:description>
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<identifier>HZDR:PUBLDB:1266-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Gallmeister, K.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Pavlenko, O. P.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1266-2</dc:identifier>
<dc:title><![CDATA[Can One Discriminate the Thermal Dilepton Signal Against the Open Charm and Bottom Decay Background in Ultrarelativistic Heavy-Ion Collisions?]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-235]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Abstract
In ultrarelativistic heavy-ion collisions at √s > 20 (120) A GeV a copious production of charm (bottom) production sets in which, via correlated semileptonic DD (BB) decays, gives rise to a dilepton yield at invariant mass M ≈ 2 - 3 GeV in excess of the Drell-Yan yield and the thermal dilepton signal from deconfined matter as well. We show that appropriate single-electron transverse momentum cuts (suitable for ALICE at LHC) cause a threshold like behavior of the dilepton spectra from heavy-quark meson decays and the Drell-Yan process and can allow to observe a thermal dilepton signal from hot deconfined matter.]]></dc:description>
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<identifier>HZDR:PUBLDB:1268-1</identifier>
<datestamp>2023-05-04</datestamp>
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<dc:creator><![CDATA[Markwitz, A.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
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<dc:title><![CDATA[Phase Formation in Ion Beam Bombarded Al-Au Multilayers Using High-Current 2.0 MeV <SUP>4</SUP>He<SUP>+</SUP> Ions]]></dc:title>
<dc:source><![CDATA[Surface and Interface Analysis, Vol. 26 No 9, pp. 650-658 (1998)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:509-1</identifier>
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<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Pavlenko, O. P.]]></dc:creator>
<dc:creator><![CDATA[Peshier, A.]]></dc:creator>
<dc:creator><![CDATA[Hentschel, M.]]></dc:creator>
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<dc:title><![CDATA[Estimates of Electromagnetic Signals from Deconfined Matter Produced in Ultrarelativistic Heavy-Ion Collisions]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-128]]></dc:source>
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<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
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<dc:creator><![CDATA[Peshier, A.]]></dc:creator>
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<dc:title><![CDATA[Estimates of Electromagnetic Signals from Deconfined Matter Produced in Ultrarelativistic Heavy-Ion Collisions]]></dc:title>
<dc:source><![CDATA[Advances in Nuclear Dynamics 2, Edited by Bauer and Westfall, Plenum Press, New York, 1996, p. 285]]></dc:source>
<dc:date>1996</dc:date>
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<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:creator><![CDATA[Engelmann, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-511-1</dc:identifier>
<dc:title><![CDATA[Institute of Radiochemistry; Annual Report 1995]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-123]]></dc:source>
<dc:date>1996</dc:date>
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<dc:creator><![CDATA[Kolitsch, A.]]></dc:creator>
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<dc:title><![CDATA[Herstellung, Charakterisierung und Ionenstrahlmodofizierung amopher Kohlenstoffschichten]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-127]]></dc:source>
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<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
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<dc:description><![CDATA[The report gives an overview on the scientific work of the Institute of Safety Research in 1994. ]]></dc:description>
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<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
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<dc:title><![CDATA[Einfluß bestrahlungsindizierter Ausscheidungen auf die Zähigkeit von Cr-Mo-V-legierten Reaktordruckbehälterstählen]]></dc:title>
<dc:source><![CDATA[28. Tagung DVM-Arbeitskreises Bruchvorgänge, Bremen, 26. - 27. Februar 1996, DVM-Bericht 228, S. 173 - 182]]></dc:source>
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<dc:creator><![CDATA[Große, M.]]></dc:creator>
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<dc:creator><![CDATA[Engstroem, P.]]></dc:creator>
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<dc:title><![CDATA[SAXS Investigation of Structural Changes in the Plastic Zone Ahead of the Crack Tip in Ductile Metals]]></dc:title>
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<dc:creator><![CDATA[Müller, H.]]></dc:creator>
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<dc:title><![CDATA[Are missing-mass measurements the key for understanding subthreshold particle production]]></dc:title>
<dc:source><![CDATA[Zeitschrift für Physik A 355 (1996) pp. 223-224]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[By measuring the fast particles emerging from a proton-nucleus interaction the number of participants can be determined. This might be the key quantity for understanding subthreshold particle production.]]></dc:description>
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<identifier>HZDR:PUBLDB:526-1</identifier>
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<dc:creator><![CDATA[Henke, D.]]></dc:creator>
<dc:creator><![CDATA[Tyrroff, H.]]></dc:creator>
<dc:creator><![CDATA[Wirth, H.]]></dc:creator>
<dc:creator><![CDATA[Zschornack, G.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-526-1</dc:identifier>
<dc:title><![CDATA[Output Maximization of a 7.25 GHz ECR Ion Source]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-131 Preprint]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:527-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Schleif, M.]]></dc:creator>
<dc:creator><![CDATA[Wünsch, R.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-527-1</dc:identifier>
<dc:title><![CDATA[Inertial Mass of the Chiral Quark-Loop Soliton in the Nambu & Jona-Lasinio Model at Finite Temperature and Density]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-132 Preprint]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Abstract
We consider the mass of the one-loop hedgehog soliton of the bosonized SU(2) Nambu & Jona-Lasinio model embedded in hot nuclear matter mimiced by a gas of constituent quarks. We prove that the proper-time regularized and self-consistently determined soliton in a heat bath obeys Poincare's invariance up order V<sup>2</sup>. At ifinite temperature and chemical potential, we show that the inertial mass obtained in the perturbative pushing approach coincides with the total internal energy of the soliton.]]></dc:description>
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<dc:creator><![CDATA[Glaser, M.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Berger, R.]]></dc:creator>
<dc:creator><![CDATA[Hahn, F. E.]]></dc:creator>
<dc:creator><![CDATA[Lügger, T.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-528-1</dc:identifier>
<dc:title><![CDATA[Unexpected formation of the new oxorhenium (V) complex [ReO(NH(CH<SUB>2</SUB>CH<SUB>2</SUB>S)<SUB>2</SUB>)(SC<SUB>6</SUB>H<SUB>5</SUB>)] obtained by N-C cleavage of the tripodal ligand N(CH<SUB>2</SUB>CH<SUB>2</SUB>SH)<SUB>3</SUB>]]></dc:title>
<dc:source><![CDATA[Inorganica Chimica Acta 257 (1997) 143-147]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:532-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-532-1</dc:identifier>
<dc:title><![CDATA[Institute of Ion Beam Physics and Materials Research; Annual Report 1995]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-129]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
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<identifier>HZDR:PUBLDB:533-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Dönau, F.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Enghardt, W.]]></dc:creator>
<dc:creator><![CDATA[Möller, K.]]></dc:creator>
<dc:creator><![CDATA[Mösner, J.]]></dc:creator>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:creator><![CDATA[Wünsch, R.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-533-1</dc:identifier>
<dc:title><![CDATA[Institute of Nuclear and Hadron Physics; Annual Report 1995]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-130]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:536-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Peshier, A.]]></dc:creator>
<dc:creator><![CDATA[Hentschel, M.]]></dc:creator>
<dc:creator><![CDATA[Soff, G.]]></dc:creator>
<dc:creator><![CDATA[Pavlenko, O. P.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-536-2</dc:identifier>
<dc:title><![CDATA[Electromagnetic signals from deconfined matter resulting from ultrarelativistic heavy-ion collisions]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-136]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Peshier, A.]]></dc:creator>
<dc:creator><![CDATA[Hentschel, M.]]></dc:creator>
<dc:creator><![CDATA[Soff, G.]]></dc:creator>
<dc:creator><![CDATA[Pavlenko, O. P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-536-1</dc:identifier>
<dc:title><![CDATA[Electromagnetic signals from deconfined matter resulting from ultrarelativistic heavy-ion collisions]]></dc:title>
<dc:source><![CDATA[World Scientific, Singapore: Structure of Vacuum and Elementary Matter, World Scientific 1997, New Jersy, London, Hongkong,  (Eds.) H. Stoecker, A. Gallmann, J. H. Hamilton, p. 483]]></dc:source>
<dc:date>1997</dc:date>
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<dc:title><![CDATA[Aufnahme und Verteilung von Trichloressigsäure in Trieben Norwegischer Fichte]]></dc:title>
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<dc:creator><![CDATA[Geipel, G.]]></dc:creator>
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<dc:title><![CDATA[Laser and X-ray spectroscopic studies of uranium-calcite interface phenomena]]></dc:title>
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<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Hatzopoulos, N.]]></dc:creator>
<dc:creator><![CDATA[Danilin, A.]]></dc:creator>
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<dc:title><![CDATA[Proximity gettering of Fe in SIMOX structures]]></dc:title>
<dc:source><![CDATA[IIT '96, Austin, Texas, USA; Proc. 11th Int. Conf. Ion Implantation Technology; The Inst. of Electrical and Electronics Eng., Piscataway, USA, 1997, p. 737]]></dc:source>
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<dc:title><![CDATA[Proximity gettering of copper in separation-by-implanted-oxygen structures]]></dc:title>
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<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
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<dc:creator><![CDATA[Danilin, A.]]></dc:creator>
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<dc:title><![CDATA[Proximity gettering of copper in separation-by-implanted-oxygen structures]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 120 (1996) 60]]></dc:source>
<dc:date>1996</dc:date>
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<identifier>HZDR:PUBLDB:568-1</identifier>
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<dc:creator><![CDATA[Enghardt, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-568-1</dc:identifier>
<dc:title><![CDATA[Positronen-Emissions-Tomographie bei der Schwerionentherapie. Ein Verfahren zur in-situ Kontrolle der Tumorbehandlung mit Strahlen schwerer Ionen]]></dc:title>
<dc:source><![CDATA[Physikalische Blätter 52 (1996) 9 pp. 874-875]]></dc:source>
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<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Pham, T.]]></dc:creator>
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<dc:title><![CDATA[Nanometre-sized Silver Halides Entrapped in SiO<sub>2</sub> Matrices]]></dc:title>
<dc:source><![CDATA[Journal of Materials Science 33 (1998) 155-159]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The formation of nanocrystals after implantation of silver
alone as well as together with the halogen ions Cl, Br, and I into a SiO2
layer of about 100 nm was studied by X-ray diffraction and transmission
electron microscopy. The co-implantation of Ag and Cl/Br results in the
formation of cubic AgX-crystals which are stable in size under annealing.
The co-implantation of Ag and I as well as single Ag implantation result
in Ag crystallites, which grow under annealing. The annealing procedure
causes a redistribution of the particles within the layer.]]></dc:description>
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<identifier>HZDR:PUBLDB:572-1</identifier>
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<dc:creator><![CDATA[Moll, H.]]></dc:creator>
<dc:creator><![CDATA[Geipel, G.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Brendler, V.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-572-1</dc:identifier>
<dc:title><![CDATA[Interaction of Uranium (VI) with Silicon Species in aqueous Solutions]]></dc:title>
<dc:source><![CDATA[NRC4-Konferenz in St. Malo (Frankreich) 8.-13.9.1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:594-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Gabriel, F.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-594-1</dc:identifier>
<dc:title><![CDATA[Bericht der Frühjahrstagung der Studiengruppe für Elektronische Instrumentierung vom 25. bis 27. März 1996 in Karlsruhe]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-141]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
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<dc:audience>Researchers</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:599-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Bauer, R.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Walter, B.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Füchtner, F.]]></dc:creator>
<dc:creator><![CDATA[Will, E.]]></dc:creator>
<dc:creator><![CDATA[Linnemann, H.]]></dc:creator>
<dc:creator><![CDATA[Obert, M.]]></dc:creator>
<dc:creator><![CDATA[Zwiener, U.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-599-1</dc:identifier>
<dc:title><![CDATA[Measurement of the cerebral uptake and meta-bolism of L-6-[18F]Fluoro-3,4-dihydroxyphenylalanine (18FDOPA) in newborn piglets]]></dc:title>
<dc:source><![CDATA[Neurochemistry: Cellular, Molecular, and Clinical Aspects, Book Article, Plenum Publishing Cooperation, Section 43: PET Imaging of Receptors;1149-1155]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1881-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Alemany, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1881-1</dc:identifier>
<dc:title><![CDATA[Magnetohydrodynamic Flow Around a Circular Cylinder]]></dc:title>
<dc:source><![CDATA[Bluff Body Wakes Dynamics and Instabilities, p. 51 - 54, Berlin, Heidelberg, New York, Springer 1993, pp. 51 - 54]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The flow around a circular cylinder is considered for the following particular configuration: The fluid is electrically conducting and the whole system is inside an external magnetic field. This magnetohydrodynamic (MHD) flow is of interest for various applications but also for basic fluiddynamic research.
As an introduction to typical MHD effects a simple model system is considered: Fluid flow parallel to the cylinder axis. It allows an analytical solution of the combined system of Navier-Stokes- and Maxwell-equations. The results clearly show the development of the typical shear-layers resulting from the electromagnetic and viscous forces: Boundary layer at the cylinder surface, tangential layers at the cylinder poles, deep core and outer core of the wake. 
Analytical and experimental results will be summarized concerning the more interesting standard geometry of a flow perpendicular to the cylinder axis. 
The experimental results include turbulence intensities and the induced magnetic field at different locations in the up- and downstream wakes, as well as the pressure at the cylinder surface.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1882-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1882-1</dc:identifier>
<dc:title><![CDATA[New results on MHD drag coefficients]]></dc:title>
<dc:source><![CDATA[Progress in Astronautics and Aeronautics, Ed. H. Branover, Y. Unger, Washington 148 (1993), S. 551 - 565]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[Theoretical and experimental results of MHD drag coefficients are summarized. Special attention is paid to Stokes flow, where a typical error has been found in the literature. This situation is clarified here, and correct results are presented. Numerical calculations are performed for the MHD Stokes flow around a cylinder in a transverse magnetic field, yielding qualitative agreement for the drag with both measurement as well as a rough asymptotic analysis. The MHD drag coefficient of the cylinder in a transverse magnetic field increases proportionally to M . lnM if  M >> 1 (where M is the Hartmann number). Finally, the deflection of a rising bubble in a liquid metal is determined if the direction of the magnetic field is inclined relative to the vertical line.]]></dc:description>
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<identifier>HZDR:PUBLDB:1592-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Häfele, W.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1592-1</dc:identifier>
<dc:title><![CDATA[Energy Problems of the United Germany]]></dc:title>
<dc:source><![CDATA[Paper presented at the SEC IFPA Meeting "Energy Strategy of the Countries with Transitional Economics", held at Moscow, June 24 - 25, 1993, Perspectives in Energy 2 (1993), p. 369]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[After the reunification of Germany, the energy situation in Germany has changed and particularly so in eastern Germany. There the demand for electric energy has suddenly decreased owing to industrial closures and accordingly, for this and for environmental reasons, the production of lignite has decreased as well. All nuclear capacity was shut down. Instead, a number of very modern high-performance coal-fired plants are being installed that also allow a sharp reduction of air pollution. Naturally, a modernisation and integration of the electrical grid is under way.]]></dc:description>
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<identifier>HZDR:PUBLDB:1592-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Häfele, W.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1592-2</dc:identifier>
<dc:title><![CDATA[Energy Problems of the United Germany]]></dc:title>
<dc:source><![CDATA[Paper presented at the SEC IFPA Meeting "Energy Strategy of the Countries with Transitional Economics", held at Moscow, June 24 - 25, 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[After the reunification of Germany, the energy situation in Germany has changed and particularly so in eastern Germany. There the demand for electric energy has suddenly decreased owing to industrial closures and accordingly, for this and for environmental reasons, the production of lignite has decreased as well. All nuclear capacity was shut down. Instead, a number of very modern high-performance coal-fired plants are being installed that also allow a sharp reduction of air pollution. Naturally, a modernisation and integration of the electrical grid is under way.]]></dc:description>
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<identifier>HZDR:PUBLDB:1526-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Hübener, S.]]></dc:creator>
<dc:creator><![CDATA[Brüchle, W.]]></dc:creator>
<dc:creator><![CDATA[Dressler, R.]]></dc:creator>
<dc:creator><![CDATA[Eichler, B.]]></dc:creator>
<dc:creator><![CDATA[Gäggeler, H. W.]]></dc:creator>
<dc:creator><![CDATA[Grantz, M.]]></dc:creator>
<dc:creator><![CDATA[Heyne, H.]]></dc:creator>
<dc:creator><![CDATA[Jäger, E.]]></dc:creator>
<dc:creator><![CDATA[Jost, D. T.]]></dc:creator>
<dc:creator><![CDATA[Kirbach, U. u. a.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1526-1</dc:identifier>
<dc:title><![CDATA[Physico-chemical characterization of Seaborgium as oxide hydroxide]]></dc:title>
<dc:source><![CDATA[I. Intern. Conference in the Chemistry and Physics of the Transactinide Elements TAV 99]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[
The physico-chemical characterization of seaborgium as oxide hydroxide, performed in 1998 at the GSI accelerator UNILAC, continues earlier gas chromatographic studies of seabor-gium oxychlorides [1, 2]. In our former studies seaborgium behaved like a typical group 6 element despite the relativistic effects, which are increasing with the nuclear charge and cause unexpected chemical properties of the lighter transactinide elements rutherfordium and dubnium [3, 4]. To characterize seaborgium its properties have to be compared with those of other elements, first of all its homologues molybdenum and tungsten. The clear gra-dation of their chemical properties favors the oxides of the group 6 elements for studies of the influence of relativistic effects on the chemical properties of seaborgium. All the more as gas chromatographic studies of oxides or oxide hydroxides, respectively, provide high selec-tivity with regard to the lighter transactinides and interfering actinides. But on the other hand, the surface reactions dissociative adsorption and associative desorption governing the reac-tion  ...]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:14302-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Fähnemann, S.]]></dc:creator>
<dc:creator><![CDATA[Stephan, H.]]></dc:creator>
<dc:creator><![CDATA[Walther, M.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Haaf, C.]]></dc:creator>
<dc:creator><![CDATA[Comba, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14302-1</dc:identifier>
<dc:title><![CDATA[Very stable copper(II) complexes of bispidines and their radiopharmaceutical behavior]]></dc:title>
<dc:source><![CDATA[International Symposium on Technetium and other Radiometals in Chemistry and Medicine, 08.-11.09.2010, Bressanone, Italy]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The three bispidine-derived ligands L1 - L3 (bispidine = 3,7-diazabicyclo[3.3.1]-nonane) have been labeled with <SUP>64</SUP>Cu, and the radioactive copper(II) complexes have been investigated for potential radiopharmaceutical applications. The thermodynamic stability of copper(II) complexes with the 2<SUP>nd</SUP> generation bispidines L2 and L3 is significantly higher than with L1 as a 1<SUP>st</SUP> generation bispidine. Despite this, labeling kinetics and challenge experiments indicate that  L1 has advantages as a ligand for radiocopper(II) applications over the new ligands L2 and L3. The copper(II) complexes of all three bispidine ligands were found to be rather hydrophilic (log D<SUB>o/w</SUB> at pH = 7.4: <SUP>64</SUP>Cu-L1 = -2.88, <SUP>64</SUP>Cu-L2 = -1.45, <SUP>64</SUP>Cu-L3 = -1.94). In vitro experiments with rat plasma give evidence that the <SUP>64</SUP>Cu complexes of L1  L3 are very stable.]]></dc:description>
<dc:subject><![CDATA[bispidine]]></dc:subject>
<dc:subject><![CDATA[coordination geometry]]></dc:subject>
<dc:subject><![CDATA[stability]]></dc:subject>
<dc:subject><![CDATA[copper-64]]></dc:subject>
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<identifier>HZDR:PUBLDB:14302-2</identifier>
<datestamp>2025-06-05</datestamp>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Fähnemann, S.]]></dc:creator>
<dc:creator><![CDATA[Stephan, H.]]></dc:creator>
<dc:creator><![CDATA[Walther, M.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Haaf, C.]]></dc:creator>
<dc:creator><![CDATA[Comba, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14302-2</dc:identifier>
<dc:title><![CDATA[Very stable copper(II) complexes of bispidines and their radiopharmaceutical behavior]]></dc:title>
<dc:source><![CDATA[Nuclear Medicine and Biology 37(2010)6, 678-679]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The three bispidine-derived ligands L1 - L3 (bispidine = 3,7-diazabicyclo[3.3.1]-nonane) have been labeled with <SUP>64</SUP>Cu, and the radioactive copper(II) complexes have been investigated for potential radiopharmaceutical applications. The thermodynamic stability of copper(II) complexes with the 2<SUP>nd</SUP> generation bispidines L2 and L3 is significantly higher than with L1 as a 1<SUP>st</SUP> generation bispidine. Despite this, labeling kinetics and challenge experiments indicate that  L1 has advantages as a ligand for radiocopper(II) applications over the new ligands L2 and L3. The copper(II) complexes of all three bispidine ligands were found to be rather hydrophilic (log D<SUB>o/w</SUB> at pH = 7.4: <SUP>64</SUP>Cu-L1 = -2.88, <SUP>64</SUP>Cu-L2 = -1.45, <SUP>64</SUP>Cu-L3 = -1.94). In vitro experiments with rat plasma give evidence that the <SUP>64</SUP>Cu complexes of L1  L3 are very stable.]]></dc:description>
<dc:subject><![CDATA[bispidine]]></dc:subject>
<dc:subject><![CDATA[coordination geometry]]></dc:subject>
<dc:subject><![CDATA[stability]]></dc:subject>
<dc:subject><![CDATA[copper-64]]></dc:subject>
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<identifier>HZDR:PUBLDB:14302-3</identifier>
<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Fähnemann, S.]]></dc:creator>
<dc:creator><![CDATA[Stephan, H.]]></dc:creator>
<dc:creator><![CDATA[Walther, M.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Haaf, C.]]></dc:creator>
<dc:creator><![CDATA[Comba, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14302-3</dc:identifier>
<dc:title><![CDATA[Very stable copper(II) complexes of bispidines and their radiopharmaceutical behavior]]></dc:title>
<dc:source><![CDATA[Ulderico Mazzi, William V. Eckelman, Wynn A. Volkert: Technetium and Other Radiometals in Chemistry and Medicine, Padova: SGEditoriali, 2010, 51-56]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The three bispidine-derived ligands L1 - L3 (bispidine = 3,7-diazabicyclo[3.3.1]-nonane) have been labeled with <SUP>64</SUP>Cu, and the radioactive copper(II) complexes have been investigated for potential radiopharmaceutical applications. The thermodynamic stability of copper(II) complexes with the 2<SUP>nd</SUP> generation bispidines L2 and L3 is significantly higher than with L1 as a 1<SUP>st</SUP> generation bispidine. Despite this, labeling kinetics and challenge experiments indicate that  L1 has advantages as a ligand for radiocopper(II) applications over the new ligands L2 and L3. The copper(II) complexes of all three bispidine ligands were found to be rather hydrophilic (log D<SUB>o/w</SUB> at pH = 7.4: <SUP>64</SUP>Cu-L1 = -2.88, <SUP>64</SUP>Cu-L2 = -1.45, <SUP>64</SUP>Cu-L3 = -1.94). In vitro experiments with rat plasma give evidence that the <SUP>64</SUP>Cu complexes of L1  L3 are very stable.]]></dc:description>
<dc:subject><![CDATA[bispidine]]></dc:subject>
<dc:subject><![CDATA[coordination geometry]]></dc:subject>
<dc:subject><![CDATA[stability]]></dc:subject>
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<dc:creator><![CDATA[Ferse, W.]]></dc:creator>
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<dc:title><![CDATA[Möglichkeiten und Grenzen der Entscheidungsanalyse bei der Unterstützung von öffentlichen Entscheidungen]]></dc:title>
<dc:source><![CDATA[Workshop "Nachhaltigkeit - Leitbild für die Wirtschaft", Zentrum für Interdisziplinäre Technikforschung der Technischen Universität Dresden, Dresden, 24. - 26. September 1997]]></dc:source>
<dc:date>1997</dc:date>
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<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1660-1</dc:identifier>
<dc:title><![CDATA[The Dresden Innovationskolleg on Magnetofluiddynamics]]></dc:title>
<dc:source><![CDATA[Int. Workshop "The use fo magnetic fields in metallurgy and metals processing", Frankfurt/Main, Oct. 1 - 2, 1997]]></dc:source>
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<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1661-1</dc:identifier>
<dc:title><![CDATA[Destabilizing actions of staedy magnetic fields]]></dc:title>
<dc:source><![CDATA[3rd Int. Conference on Transfer Phenomena in Magnetohydrodynamic & Eletroconducting Flows, Aussois, France, Sept. 22 - 26, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Usually the action of steady magnetic fields on electrically conducting flows is a damping one. But several examples exist where additional instabilities are due to the magnetic field influence. Such examples will be listed up based on a classification of the various MHD actions. The physical reason for these phenomena and possible applications will be discussed.]]></dc:description>
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<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1663-1</dc:identifier>
<dc:title><![CDATA[Kleinwinkelstreuexperimente mit Neutronen- und Synchrotronstrahlung zur Untersuchung der strukturellen Mechanismen der Neutronenversprödung]]></dc:title>
<dc:source><![CDATA[Paul Scherrer Institut Villingen, 21. 10. 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1667-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1667-1</dc:identifier>
<dc:title><![CDATA[Proposal on Dynamic Benchmark Problem for Coupled Thermohydraulic/3D Hexagonal Neutron Kinetic Codes]]></dc:title>
<dc:source><![CDATA[AER Working Group D Meeting, Budapest, 5 - 7 May, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1668-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1668-1</dc:identifier>
<dc:title><![CDATA[Development of an ATHLET Input Data Check for the Dodewaard Reactor]]></dc:title>
<dc:source><![CDATA[Status Report BWRCA-Meeting, Rossendorf, 27 - 28 October, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
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<dc:title><![CDATA[Eine Frischdampfleitungsleckanalyse für den WWER-440 mit dem gekoppelten Programmkomplex DYN3D/ATHLET]]></dc:title>
<dc:source><![CDATA[4th ATHLET-User Group Meeting, Garching, 11/12 June, 1997]]></dc:source>
<dc:date>1997</dc:date>
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1670-1</dc:identifier>
<dc:title><![CDATA[Simulation von Erwärmungsprozessen in großen Behältern mit dem Code CFX]]></dc:title>
<dc:source><![CDATA[CFX-Anwendertreffen, Bad Dürkheim, 16./17. September 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kyrki-Rajamäki, R.]]></dc:creator>
<dc:creator><![CDATA[Mittag, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1671-1</dc:identifier>
<dc:title><![CDATA[Guidelines for the Collection of NPP Measurement Data to be Used in Transient Code Validation]]></dc:title>
<dc:source><![CDATA[1st Meeting on the CEC PHARE project SRR1-95, Rossendorf, September 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Collecting measurement data of NPP transients will be of key importance for the validation of coupled thermohydraulics / neutron kinetics codes. The transient data should cover relevant effects caused by the interaction between 3D neutron kinetics and thermohydraulics. Data will be collected for both VVER types (VVER­440 and VVER­1000).]]></dc:description>
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<identifier>HZDR:PUBLDB:1672-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Manturov, G.]]></dc:creator>
<dc:creator><![CDATA[Böhmer, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1672-1</dc:identifier>
<dc:title><![CDATA[Covariance Matrices for the Calculated Spectra at the VVER-1000 Cavity]]></dc:title>
<dc:source><![CDATA[International Workshop on the Balakovo-3 Interlaboratory Pressure Vessel Dosimetry Experiment, Rossendorf, 2 - 5 September 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Neumann, J.]]></dc:creator>
<dc:creator><![CDATA[Schlüter, S.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Vorst, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1673-1</dc:identifier>
<dc:title><![CDATA[Zustandserkennung in Chemieanlagen mit neuronalen Netzen]]></dc:title>
<dc:source><![CDATA[DECHEMA-Fachausschuß "Sicherheitsgerechtes Auslegen von Chemieapparaten", Oberhausen, 26./27. November, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Priede, J.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1674-1</dc:identifier>
<dc:title><![CDATA[Magnetic stabilization of thermocapillary driven convection]]></dc:title>
<dc:source><![CDATA[Int. Workshop on Hydrodynamic Aspects of Electron Beam Technologies, Dresden, March 16 -18, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1678-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schäfer, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1678-1</dc:identifier>
<dc:title><![CDATA[ATHLET Calculations of Selected Experiments at PMK-2]]></dc:title>
<dc:source><![CDATA[GRS-Project Metting PHARE 4.2.6b, Berlin, 15. 06. 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The report deals with results of ATHLET calculations for the Hungarian test facility PMK-2. The test facilty is a 1:2070 scaled
down model of a VVER-440 reactor. The calculated experiments includes a inadvertent opening of the pressurizer safety valve"
and a pressurizer surge line break". Both experiments were carried out within the PHARE 4.2.6b project. For the calculations
the code ATHLET mod1.1 Cycle C was used. The results of the calculations were compared with the experimental data.
]]></dc:description>
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<dc:language>eng</dc:language>
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<header>
<identifier>HZDR:PUBLDB:214-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Eichhorn, F.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-214-1</dc:identifier>
<dc:title><![CDATA[Characterization of Irradiation-induced Precipitates by Small Angle X-ray and Neutron Scattering Experiments Effects of Radiation on Materials]]></dc:title>
<dc:source><![CDATA[17th Volume, ASTM STP 1270, D.S. Gelles, R.K. Nanstadt, A.S. Kumar, E.A. Little, Eds., American Society for Testing and Materials, Philadelphia, p. 1123]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The nature of the irradiation-induced precipitates in the VVER-440-type steel 15Kh2MFA has been investigated by the combination of small angle neutron scattering and anomalous small angle X-ray scattering. By the method of contrast variation information about the chemical composition of the irradiation-induced precipitates was obtained. ASAXS experiments with variation of the X-ray energy near to the energy of the vanadium K-absorption edge prove the content of vanadium within the irradiation-induced precipitates. The scattering density of the precipitates is lower than the scattering density of the iron matrix. The chemical shift of the vanadium-K -absorption-edge and the results of the variation of the contribution of the magnetic scattering in the SANS experiment show, that vanadium does not precipitate in an elementary state. By assuming the precipitates being vanadium carbide these results can be explained in the best way.]]></dc:description>
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<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:214-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Eichhorn, F.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-214-7</dc:identifier>
<dc:title><![CDATA[Characterization of Irradiation-induced Precipitates by Small Angle X-ray and Neutron Scattering Experiments Effects of Radiation on Materials]]></dc:title>
<dc:source><![CDATA[17th Volume, ASTM STP 1270, D.S. Gelles, R.K. Nanstadt, A.S. Kumar, E.A. Little, Eds., American Society for Testing and Materials, Philadelphia, p. 1123]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The nature of the irradiation-induced precipitates in the VVER-440-type steel 15Kh2MFA has been investigated by the combination of small angle neutron scattering and anomalous small angle X-ray scattering. By the method of contrast variation information about the chemical composition of the irradiation-induced precipitates was obtained. ASAXS experiments with variation of the X-ray energy near to the energy of the vanadium K-absorption edge prove the content of vanadium within the irradiation-induced precipitates. The scattering density of the precipitates is lower than the scattering density of the iron matrix. The chemical shift of the vanadium-K -absorption-edge and the results of the variation of the contribution of the magnetic scattering in the SANS experiment show, that vanadium does not precipitate in an elementary state. By assuming the precipitates being vanadium carbide these results can be explained in the best way.]]></dc:description>
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<dc:type>doc-type:bookPart</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-214-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:148-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Eichhorn, F.]]></dc:creator>
<dc:creator><![CDATA[Haubold, H.-G.]]></dc:creator>
<dc:creator><![CDATA[Goerigk, G.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-148-1</dc:identifier>
<dc:title><![CDATA[Characterisation of Nanoscale Precipitates in Reactor Pressure Vessel Steel 15Kh2MFA by Small Angle Scattering Experiments]]></dc:title>
<dc:source><![CDATA[und Proceeding EUROMAT 94, Balatonszeplak, Hungaria, 30. Mai bis 01. Juni 1994, p. 448]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The deterioration of the mechanical properties of reactor pressure vessel (RPV) steels during their irradiation in a nuclear power plant is known as neutron embrittlement. The microscopic mechanisms of the neutron embrittlement of low alloy RPV steel are not fully understood.
These mechanisms were investigated at the RPV steel of Russian and Czech type 15Kh2MFA. This steel differs from ASTM type A503 or A533 steels mainly in its contents of the carbide forming elements Cr and V. Neutron small angle scattering (SANS) using the SANS-2 facility at the FRG-1 reactor in Geesthacht and anomalous X-ray small angle scattering (ASAXS) using the JUSIFA facility at the HASYLAB in Hamburg were employed.
The difference between the scattering intensities from irradiated and unirradiated specimens give the small angle scattering effect of the radiation damages. Irradiation induced precipitates were found with a mean diameter of   = 1...2 nm. The defect volume fraction is depending from the neutron fluence.
From the magnetic scattering contrast (SANS) and the anomalous scattering contrast (ASAXS) information about the chemical composition were got. This results are compared with the idea that the irradiation induced precipitates in 15Kh2MFA steel are carbides.]]></dc:description>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-148-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:99-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-99-1</dc:identifier>
<dc:title><![CDATA[3-Dimensional Analysis of a Baron Dilution Accident by Using the Code DYN3D/M2]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[An incorrect startup of a pump in an isolated loop containing a plug of diluted absorber can initiate a reactivity accident in a VVER-440. It is assumed that the main gate valve is opened after starting the main coolant pump. When the plug enters the core, it gives rise to a positive reactivity. An asymmetric distribution of diluted water in the core is expected which requires a 3-dimensional analysis for a more correct description of this accident.
The code DYN3D/M2 developed for investigations of reactivity initiated accidents in thermal reactors with hexagonal fuel elements is used for analysis. A model describing the mixing of water from the different loops in the lower plenum of a VVER-440 reactor gives the boron concentration at the inlet of each fuel element. The two limiting cases, ideal mixing and no mixing, are investigated for comparisons.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-99-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:291-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-291-1</dc:identifier>
<dc:title><![CDATA[Results of Second Kinetic AER-Benchmark]]></dc:title>
<dc:source><![CDATA[und Vortrag, 4th AER Symposium, Sozopol, Bulgaria, October 10 - 13, 1994, pp. 397 - 415]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Mathematical benchmark are widely used and accepted means of verifying the reliability of numerical simulations. The present benchmark is aimed at assessing the discrepancies between three-dimensional core models used for transient calculations in VVER-reactor cores.
The second AER benchmark problem was defined at the 3nd AER Symposium in Pietany (1993). The problem and the complete set of input data for a control rod ejection accident in a VVER-440 was described. An asymmetric control rod with a worth approximately 2 ßeff was ejected at hot zero power (HZP). The Doppler effect being the main feedback effect for this type of transients is the only feedback taken into account by an adiabatic model of fuel temperature. Therefore it was possible to calculate this type of transient with codes which do not contain a complete thermo-hydraulic model.
Results of the four codes BIPR-8 (RRI Moskau), DYN3D/M2 (RCR Rossendorf), HEXTRAN (VVT Espoo) and KOKO3D (KFKI-AERI Budapest) were obtained and analyzed by comparisons. The agreement of the results is quite satisfactory, however there exist some discrepancies.]]></dc:description>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-291-1</dc:relation>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:108-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hirsch, W.]]></dc:creator>
<dc:creator><![CDATA[Lischke, R.]]></dc:creator>
<dc:creator><![CDATA[Matthäi, J.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-108-1</dc:identifier>
<dc:title><![CDATA[Untersuchungen zur Windenergienutzung in Sachsen]]></dc:title>
<dc:source><![CDATA[Kongreß "TERRATEC" 9.-12.3.1994, Leipzig, Tagungsband S. 144]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Im Rahmen eines umfangreichen Programmes wurden Untersuchungen zur Anwendbarkeit der Windatlas-Methode (WASP) zur Ermittlung des Windenergiepotentials in Sachsen durchgeführt. Das Ziel der Untersuchungen bestand darin, die erwarteten Grenzen bei der Nutzung von WASP in orografisch gegliedertem Gelände genauer zu ermitteln. Grundlage der Berechnungen waren Messungen von vier Stationen des sächsischen Windmeßprogrammes. Es konnte gezeigt werden, daß in großen Gebieten der Oberlausitz die Windatlas-Methode genutzt werden kann. In den Kammregionen des Erzgebirges wurden widersprüchliche Ergebnisse gefunden, so daß eine Nutzung hier praktisch nur in sehr kleinen Repräsentationsgebieten in der Umgebung einer Meßstation möglich ist.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-108-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<header>
<identifier>HZDR:PUBLDB:108-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hirsch, W.]]></dc:creator>
<dc:creator><![CDATA[Lischke, R.]]></dc:creator>
<dc:creator><![CDATA[Matthäi, J.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-108-7</dc:identifier>
<dc:title><![CDATA[Untersuchungen zur Windenergienutzung in Sachsen]]></dc:title>
<dc:source><![CDATA[Kongreß "TERRATEC" 9.-12.3.1994, Leipzig, Tagungsband S. 144]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Im Rahmen eines umfangreichen Programmes wurden Untersuchungen zur Anwendbarkeit der Windatlas-Methode (WASP) zur Ermittlung des Windenergiepotentials in Sachsen durchgeführt. Das Ziel der Untersuchungen bestand darin, die erwarteten Grenzen bei der Nutzung von WASP in orografisch gegliedertem Gelände genauer zu ermitteln. Grundlage der Berechnungen waren Messungen von vier Stationen des sächsischen Windmeßprogrammes. Es konnte gezeigt werden, daß in großen Gebieten der Oberlausitz die Windatlas-Methode genutzt werden kann. In den Kammregionen des Erzgebirges wurden widersprüchliche Ergebnisse gefunden, so daß eine Nutzung hier praktisch nur in sehr kleinen Repräsentationsgebieten in der Umgebung einer Meßstation möglich ist.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-108-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2361-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Albe, K.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2361-1</dc:identifier>
<dc:title><![CDATA[Computersimulationen zur Schichtabscheidung von Bornitrid]]></dc:title>
<dc:source><![CDATA[Frühjahrstagung der DPG, AK: Festkörperphysik, FB: Dünne Schichten,
Münster, Germany, March 17-21, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2361-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2362-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Albe, K.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2362-1</dc:identifier>
<dc:title><![CDATA[Molecular-dynamics simulations on boron nitride thin film deposition]]></dc:title>
<dc:source><![CDATA[10th Int. Conference on Surface Modification of Metals by Ion Beams, 
Gatlinburg, USA, September 22-26, 1997 (invited lecture)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2362-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:2363-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Albe, K.]]></dc:creator>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2363-1</dc:identifier>
<dc:title><![CDATA[Atomic scale simulations based on classical molecular-dynamics and ab initio-methods: advantageous tools for understanding growth and properties of boron nitride]]></dc:title>
<dc:source><![CDATA[Int. Workshop on Challenges in Predictive Process Simulation (ChiPPS '97), Wandlitz, Germany, Aug. 17 - 20, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2364-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Antons, A.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Mantl, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2364-1</dc:identifier>
<dc:title><![CDATA[Process simulation of sub-µm pattern formation by local oxidation of CoSi<SUB>2</SUB>/Si heterostructures]]></dc:title>
<dc:source><![CDATA[Int. Workshop on Challenges in Predictive Process Simulation (ChiPPS '97), Wandlitz, Germany, Aug. 17 - 20, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:1885-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Josserand, J.]]></dc:creator>
<dc:creator><![CDATA[Marty, P.]]></dc:creator>
<dc:creator><![CDATA[Alemany, A.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1885-1</dc:identifier>
<dc:title><![CDATA[MHD Flow Around a Cylinder in a Aligned Magnetic Field]]></dc:title>
<dc:source><![CDATA[Progress in Astronautics and Aeronautics, Ed. H. Branover, Y. Unger, Washington 148 (1993), S. 519 - 534]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[Recent results on the study of a liquid metal flow around an insulating cylinder with constant aligned magnetic field are presented. From the experimental point of view, a special type of differential pressure transducer using strain gauges is described. The results obtained with mercury as liquid metal are presented for an interaction parameter N ranging from O to approximately 8. The stabilizing effect of the magnetic field on the boundary layer separation is shown. Pressure distribution around the cylinder as well as the overall pressure drag coefficient CD are given for different values of N. The last section presents analytical calculations of the flow distribution of an inviscid fluid when N << 1. The theoretical results are in good agreement with these experimental results.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1887-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Popp, K.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, U.]]></dc:creator>
<dc:creator><![CDATA[Bergner, F.]]></dc:creator>
<dc:creator><![CDATA[Hampe, E.]]></dc:creator>
<dc:creator><![CDATA[Leonhardt, W.-D.]]></dc:creator>
<dc:creator><![CDATA[Schützler, H.-P.]]></dc:creator>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1887-1</dc:identifier>
<dc:title><![CDATA[Irradiation and Annealing Behaviour of 15Kh2MFA Reactor Pressure Vessel Steel]]></dc:title>
<dc:source><![CDATA[in L.E. Steele (ed.): Radiation Embrittlement of Nuclear Reactor Pressure Vessel Steels: An International Review, ASTM-STP 1170, Philadelphia, 1993, pp. 344 - 368, Vol. 4]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[Usually the assessment of the irradiation sensitivity and annealing behavior of reactor pressure vessel (RPV) steels is performed by means of destructive test methods, mainly impact and tension tests. In this paper a new kind of search for an efficient temperature-time regime for postirradiation thermal heat treatment is presented using nondestructive test methods like positron annihilation (Doppler broadening parameter S) and hardness (Vickers hardness HV 10).
Samples of Cr-Mo-V RPV steels (Soviet type 15Kh2MFA) were irradiated to different fluence levels of fast neutrons at temperatures T < 156 °C in a test reactor (base metal) and T = 265 °C in a pressurized water reactor (base as well as weld metal). From isochronal and isothermal annealing curves of HV 10 and S, favorable temperature-time regimes for each type of irradiated material were estimated. The data obtained from tension and impact tests indicate that sufficiently large recoveries took place by application of these regimes. 
The new approach presented is especially useful in such cases where only the smallest amounts of irradiated materials are available-a case often met for RPV surveillance specimens.]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1890-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Thess, A.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Marty, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1890-1</dc:identifier>
<dc:title><![CDATA[Electromgnetically Induced Flow Around a Cylinder]]></dc:title>
<dc:source><![CDATA[Progress in Astronautics and Aeronautics, Ed. H. Branover, Y. Unger, Washington 148 (1993), S. 535 - 550]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The unidirectional flow of an electrically conducting fluid around a cylinder of arbitrary electrical conductivity, which is driven by the interaction of a homogeneous electric current with a homogeneous magnetic field and the resulting force on the cylinder are calculated numerically without any approximation in a large range of parameters. Asymptotic solutions are derived for the case of very strong and very weak magnetic fields respectively. A comparison with experimental results on insulating and highly conducting cylinders leads to a partial agreement although inertial forces are not taken into account in the model. Finally, confinement effects are considered leading to a better agreement between theory and experiment.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1890-1</dc:relation>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1891-1</identifier>
<datestamp>2023-05-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Popp, K.]]></dc:creator>
<dc:creator><![CDATA[Rintamaa, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1891-1</dc:identifier>
<dc:title><![CDATA[Measurement of Dynamic Elastic-Plastic Fracture Toughness Parameters Using Various Methods]]></dc:title>
<dc:source><![CDATA[Int. J. Pres. Ves. and Piping 5 (1993), p. 233 - 241]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[Two improved impact testing facilities are used for the dynamic fracture toughness evaluation of precracked Charpy V-notch specimens. The methods of single specimen acoustic emission and crack mouth opening displacement testing are assumed to indicate the initiation points of stable crack growth. Thus, the dynamic ductile initiation J integral JId can be derived. It was shown that the toughness JId of the heat-resistant steel 10CrMo9.10 cannot be approximated by the J value at the maximum of the load deflection curve.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/0308-0161(93)90031-N]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1891-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:14305-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ruffani, A.]]></dc:creator>
<dc:creator><![CDATA[Stephan, H.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, J.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Graham, B.]]></dc:creator>
<dc:creator><![CDATA[Spiccia, L.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14305-1</dc:identifier>
<dc:title><![CDATA[Novel <SUP>64</SUP>Cu-labeled bombesins capable of GRP receptor-targeted tumor imaging]]></dc:title>
<dc:source><![CDATA[International Symposium on Technetium and other Radiometals in Chemistry and Medicine, 08.-11.09.2010, Bressanone, Italy]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[A new macrocyclic ligand, 2-[4,7-bis(2-pyridylmethyl)-1,4,7-triazacyclononan-1-yl]acetic acid (1), binds copper strongly and the resulting radiocopper(II)-ligand complex exhibits high in vivo stability. The pendant carboxylic group enables this derivative to be conjugated to the N-terminal amino acid residues of peptides. Exploiting this, two stabilized bombesin derivatives have been coupled to 1 and radiolabeled with the positron emitter copper-64.
In vitro binding characteristics of the [64Cu]CuII-labeled bombesin conjugates in gastrinreleasing peptide receptor (GRPR) overexpressing prostate cancer (PC-3) cells have been evaluated. Biodistribution studies performed in Wistar rats indicate a specific uptake in the GRPR-rich pancreas and rapid renal elimination. Small animal PET imaging studies confirmed a high extent of tumor accumulation in NMRI nu/nu mice bearing the human prostate tumor PC-3. Incorporation of one additional glutamic acid residue within the spacer between bombesin and the radiolabeled complex leads to a higher tumor-to-muscle uptake ratio.]]></dc:description>
<dc:subject><![CDATA[TACN]]></dc:subject>
<dc:subject><![CDATA[bombesin]]></dc:subject>
<dc:subject><![CDATA[copper-64]]></dc:subject>
<dc:subject><![CDATA[prostate cancer]]></dc:subject>
<dc:subject><![CDATA[small animal positron emission tomography]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:14305-2</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ruffani, A.]]></dc:creator>
<dc:creator><![CDATA[Stephan, H.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, J.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Graham, B.]]></dc:creator>
<dc:creator><![CDATA[Spiccia, L.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14305-2</dc:identifier>
<dc:title><![CDATA[Novel <SUP>64</SUP>Cu-labeled bombesins capable of GRP receptor-targeted tumor imaging]]></dc:title>
<dc:source><![CDATA[Nuclear Medicine and Biology 37(2010)6, 692-693]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[A new macrocyclic ligand, 2-[4,7-bis(2-pyridylmethyl)-1,4,7-triazacyclononan-1-yl]acetic acid (1), binds copper strongly and the resulting radiocopper(II)-ligand complex exhibits high in vivo stability. The pendant carboxylic group enables this derivative to be conjugated to the N-terminal amino acid residues of peptides. Exploiting this, two stabilized bombesin derivatives have been coupled to 1 and radiolabeled with the positron emitter copper-64.
In vitro binding characteristics of the [64Cu]CuII-labeled bombesin conjugates in gastrinreleasing peptide receptor (GRPR) overexpressing prostate cancer (PC-3) cells have been evaluated. Biodistribution studies performed in Wistar rats indicate a specific uptake in the GRPR-rich pancreas and rapid renal elimination. Small animal PET imaging studies confirmed a high extent of tumor accumulation in NMRI nu/nu mice bearing the human prostate tumor PC-3. Incorporation of one additional glutamic acid residue within the spacer between bombesin and the radiolabeled complex leads to a higher tumor-to-muscle uptake ratio.]]></dc:description>
<dc:subject><![CDATA[TACN]]></dc:subject>
<dc:subject><![CDATA[bombesin]]></dc:subject>
<dc:subject><![CDATA[copper-64]]></dc:subject>
<dc:subject><![CDATA[prostate cancer]]></dc:subject>
<dc:subject><![CDATA[small animal positron emission tomography]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/j.nucmedbio.2010.04.093]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:14305-3</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ruffani, A.]]></dc:creator>
<dc:creator><![CDATA[Stephan, H.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, J.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Graham, B.]]></dc:creator>
<dc:creator><![CDATA[Spiccia, L.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14305-3</dc:identifier>
<dc:title><![CDATA[Novel <SUP>64</SUP>Cu-labeled bombesins capable of GRP receptor-targeted tumor imaging]]></dc:title>
<dc:source><![CDATA[U. Mazzi, W. C. Eckelman, W. A. Volkert: Technetium and Other Radiometals in Chemistry and Medicine, Padova: SGEditoriali Padova, 2010, 217-220]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[A new macrocyclic ligand, 2-[4,7-bis(2-pyridylmethyl)-1,4,7-triazacyclononan-1-yl]acetic acid (1), binds copper strongly and the resulting radiocopper(II)-ligand complex exhibits high in vivo stability. The pendant carboxylic group enables this derivative to be conjugated to the N-terminal amino acid residues of peptides. Exploiting this, two stabilized bombesin derivatives have been coupled to 1 and radiolabeled with the positron emitter copper-64.
In vitro binding characteristics of the [64Cu]CuII-labeled bombesin conjugates in gastrinreleasing peptide receptor (GRPR) overexpressing prostate cancer (PC-3) cells have been evaluated. Biodistribution studies performed in Wistar rats indicate a specific uptake in the GRPR-rich pancreas and rapid renal elimination. Small animal PET imaging studies confirmed a high extent of tumor accumulation in NMRI nu/nu mice bearing the human prostate tumor PC-3. Incorporation of one additional glutamic acid residue within the spacer between bombesin and the radiolabeled complex leads to a higher tumor-to-muscle uptake ratio.]]></dc:description>
<dc:subject><![CDATA[TACN]]></dc:subject>
<dc:subject><![CDATA[bombesin]]></dc:subject>
<dc:subject><![CDATA[copper-64]]></dc:subject>
<dc:subject><![CDATA[prostate cancer]]></dc:subject>
<dc:subject><![CDATA[small animal positron emission tomography]]></dc:subject>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
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<header>
<identifier>HZDR:PUBLDB:14355-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Sharma, M.]]></dc:creator>
<dc:creator><![CDATA[Kanjilal, A.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Kanjilal, D.]]></dc:creator>
<dc:creator><![CDATA[Chatterjee, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14355-1</dc:identifier>
<dc:title><![CDATA[Room temperature ferromagnetism in Ni-doped HfO2 thin films]]></dc:title>
<dc:source><![CDATA[Journal of Physics D: Applied Physics 43(2010)30]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[In this paper detailed studies on modification of structural and magnetic properties of Ni-doped hafnium oxide (HfO2) thin films are reported. We used 200 keV Ni beam for doping of Ni. For homogeneous dispersion and activation of doped Ni ions, 120 MeV Ni swift heavy ions (SHI) irradiation was used. This unique combination of Ni doping by ion beam and dispersing and activating by Ni SHI irradiation of HfO2 films is reported for the first time. The origin of ferromagnetism in the Ni-doped HfO2 thin films is investigated. We demonstrate the cluster free nature of our film using cross-sectional high resolution transmission microscopy and magnetization versus temperature data. Rutherford backscattering data are used to establish that Ni ions are implanted in the HfO2 matrix at the predicted location. Dispersion of implanted Ni and lattice defects such as oxygen vacancies are attributed to be the main source of ferromagnetism.]]></dc:description>
<dc:subject><![CDATA[magnetic clusters]]></dc:subject>
<dc:subject><![CDATA[Ni-doped hafnium oxide (HfO2)]]></dc:subject>
<dc:subject><![CDATA[swift heavy ion irradiation]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1088/0022-3727/43/30/305003]]></dc:relation>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1529-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schulz Lang, E.]]></dc:creator>
<dc:creator><![CDATA[Dahmer, M.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1529-1</dc:identifier>
<dc:title><![CDATA[Tetraphenylphosphonium tetrakis(1-methyl-1,2,3,4-tetrazole-5-thiolato-S)- aurate(III) hemihydrate]]></dc:title>
<dc:source><![CDATA[Acta Crystallographica C (1999), C55, 854-856]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The tetraphenylphosphonium salt of tetra(1-methyl-1,2,3,4-tetrazole-5-thiolato)aurate(III) crystallizes as H2O solvate in the monoclinic space group C2/c with the gold atom situated on an inversion centre. The tetrazole rings are arranged almost orthogonally to the square coordination sphere. Au-S-C angles of 106.16(11) and 107.14(12)° have been found.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<record>
<header>
<identifier>HZDR:PUBLDB:1531-1</identifier>
<datestamp>2025-01-15</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Stephan, H.]]></dc:creator>
<dc:creator><![CDATA[Berger, R.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:creator><![CDATA[Schmidtchen, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1531-1</dc:identifier>
<dc:title><![CDATA[Efficient phase transfer of pertechnetate with bicyclic guanidinium compounds]]></dc:title>
<dc:source><![CDATA[Journal of Radioanalytical and Nuclear Chemistry 242 (2) (1999) 399-403]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Extraction of pertechnetate with bicyclic guanidinium compounds has been studied in the system KTcO<SUB>4</SUB>-buffer-H<SUB>2</SUB>O/ligand-trichloromethane. Extraction data of guanidinium ligands have been compared with trialkylmethylammonium (Aliquat 336), tetraphenylphosphonium and tetraphenylarsonium chloride. The lipophilicity of extractants investigated was determined by RP-HPLC. The efficiency of pertechnetate extraction correlates with the lipophilicity of the guanidinium compounds. 1:1 complex formation in the organic phase was observed. The influence of hydroxide, chloride and bicarbonate on the pertechnetate extraction has been investigated. Pertechnetate is extracted with great preference over OH<SUP>-</SUP>, Cl<SUP>-</SUP> and HCO<SUB>3</SUB><SUP>-</SUP>.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1007/BF02345569]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1531-1</dc:relation>
<dc:audience>Researchers</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1679-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Stephan, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1679-1</dc:identifier>
<dc:title><![CDATA[Rossendorf Activation Measurements for the Balakovo-3 Experiment]]></dc:title>
<dc:source><![CDATA[International Workshop on the Balakovo-3 Interlaboratory Pressure Vessel Dosimetry Experiment, Rossendorf, 2 - 5 September, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1679-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1680-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1680-1</dc:identifier>
<dc:title><![CDATA[Report on Contribution of the Forschungszentrum Rossendorf e. V. to the Project Reconstitution Techniques Qualification & Evaluation to Study Aging Phenomena of Nuclear Pressure Vessel Materials (RESQUE)]]></dc:title>
<dc:source><![CDATA[European Atomic Energy Community, Nuclear Fission Safety, 1st Progress Meeting, Erlangen, Germany, October 14-15, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1680-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1681-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1681-1</dc:identifier>
<dc:title><![CDATA[Anwendung des Master-Curve-Konzeptes]]></dc:title>
<dc:source><![CDATA[Vortrag auf der Sitzung der DVM Arbeitsgruppe "Instrumentierter Kerbschlagbiegeversuch", Staatliche Materialprüfanstalt MPA der Universität Stuttgart, 26. September 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1681-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:1682-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1682-1</dc:identifier>
<dc:title><![CDATA[Report on Contribution of the Forschungszentrum Rossendorf e. V. to IAEA Coordinated Research Programme "Assuring Structural Integrity of Reactor Pressure Vessel - CPR Phase IV"]]></dc:title>
<dc:source><![CDATA[IAEA Coordinated Research Programme Meeting, Vienna, Austria, October 8 - 10, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1682-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1684-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Weier, T.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Lielausis, O.]]></dc:creator>
<dc:creator><![CDATA[Platacis, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1684-1</dc:identifier>
<dc:title><![CDATA[Cylinder wake control by means of electromagnetic forces]]></dc:title>
<dc:source><![CDATA[Int. Workshop on Electromagnetic Boundary Layer Control for Saltwater Flows , Dresden, July 7 - 8, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1684-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1687-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bouziotis, P.]]></dc:creator>
<dc:creator><![CDATA[Papadopoulos, M.]]></dc:creator>
<dc:creator><![CDATA[Pirmettis, I.]]></dc:creator>
<dc:creator><![CDATA[Pelecanou, M.]]></dc:creator>
<dc:creator><![CDATA[Raptopoulou, C. P.]]></dc:creator>
<dc:creator><![CDATA[Terzis, A.]]></dc:creator>
<dc:creator><![CDATA[Stassinopoulou, C.]]></dc:creator>
<dc:creator><![CDATA[Friebe, M.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1687-1</dc:identifier>
<dc:title><![CDATA[Synthesis and characterization of two P,S,N-coordinated cis-dioxorhenium (V) complexes]]></dc:title>
<dc:source><![CDATA[Technetium, Rhenium and Other Metals in Chemistry and Nuclear Medicine
(Edited by Nicolini M., Mazzi U.) SGE Editoriali Padova (1999) pp. 203-208]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[In the course of our investigations into mixed ligand systems containing thiol residues, we have examined, among others, the reactions of bidentate aminethiols with monodentate thiols, as well as tridentate/monodentate mixed ligand systems in the presence of ReOCl3(PPh3)2. Mixed ligand complexes of the general type "2+1+1" and "3+1" have been isolated. Surprisingly, in our synthetic attempts to clarify the mechanism of such reactions, we revceived two unexpected cis-dioxorhenium(V) P,S,N-coordinated complexes, where the aminethiol acts as a bidentate ligand over the Re(V) precursor. The two novel complexes of the general formula ReO2[R2NCH2CH2S][PPh3] where NR2=NEt2 (Complex 1) and NR2=N(CH2CH2)2C(OCH2)2 (Complex 2) are presented below. Both complexes have been characterized by elemental analysis and spectroscopic methods. Crystallographic studies show that the coordination geometry around rhenium is trigonal bipyramidal with the two cis-oxo groups and the sulfur atom of the ligand occupying the basal plane, while the nitrogen of the ligand and the phosphorus occupy the apical positions.  ]]></dc:description>
<dc:type>info:eu-repo/semantics/book</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:book</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1687-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1689-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Zimmermann, T.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1689-1</dc:identifier>
<dc:title><![CDATA[Ring Transformations of Heterocyclic Compounds. XVIII [1]. Spiro[cyclohexadiene-indolines] with Three Stereocenters from Pyrylium Salts and Chiral Methyleneindolines - An Example of a High Diastereoselektive Ring Transformation]]></dc:title>
<dc:source><![CDATA[Communication in "Anorganische allgemeine Chemie",
"J. Heterocylic Chemie"]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[ The diastereoselective synthesis of 6-aroyl-3,5-diarylspiro[cyclohexa-2,4-diene-1,2´-indolines] 4 possessing three stereocenters from 2,4,6-triaryl-pyrylium perchlorates 1 and chiral methyleneindolines 3, generated in situ by deprotonation of the corresponding 3H-indolium perchlorates 2, in the presence of triethylamine/acetic acid in ethanol by a 2,5-[C4+C2] pyrylium ring transformation is reported. Structure elucidation is performed by  X-ray structure determinations of the spiro[cyclohexadiene-indolines] 4a, 4p and 4t. The influence of various substituents at C-3 of the methyleneindolines 3 on the stereochemistry of the transformation, mechanistic details as well as spectroscopic data of the products 4 are discussed.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1689-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1690-1</identifier>
<datestamp>2023-05-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Eichhorn, F.]]></dc:creator>
<dc:creator><![CDATA[Schell, N.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Kögler, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1690-1</dc:identifier>
<dc:title><![CDATA[Strain and SiC particle formation in silicon implanted with carbon ions of medium fluence studied by synchrotron X-ray diffraction]]></dc:title>
<dc:source><![CDATA[J. Appl. Phys.Vol. 86 No. 8 (1999) 4184 - 4187]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1693-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Stefani, F.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1693-1</dc:identifier>
<dc:title><![CDATA[Velocity reconstruction in conducting Fluids from magnetic field and electric potential measurements]]></dc:title>
<dc:source><![CDATA[Inverse Problems, 15 (1999), pp. 771-786]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[A possibility for the determination of velocity fields in conducting fluids is presented. Applying a magnetic field from outside, electric and magnetic fields are induced by the fluid motion. These fields can be measured at the walls and outside the fluid volume respectively. The inverse problem of reconstructing the velocity from the measured electric and magnetic fields is solved using Tikhonov regularization.
]]></dc:description>
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<identifier>HZDR:PUBLDB:1694-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:creator><![CDATA[Langenbuch, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1694-1</dc:identifier>
<dc:title><![CDATA[Gekoppelte Berechnungen von Thermohydraulik und Neutronenkinetik]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik, 18. - 20. Mai 1999, Karlsruhe, Sammelband "Neue Ergebnisse aus F+E zur Fluiddynamik und Reaktorphysik", Inforum Verlagsgesellschaft, Bonn, Juni 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Es wird ein Überblick über den Entwicklungsstand und die Anwendung von Computercodes mit Kopplung von thermohydraulischen Anlagenmodellen von Kernkraftwerken und 3D Neutronenkinetik gegeben. Insbesondere wird auf die Ankopplung von Neutronenkinetikmoduln an den Thermohydraulikcode ATHLET eingegangen. Es werden Arbeiten zur Validierung der Codekomplexe durch Nachrechnung von transienten Prozessen in Kernkraftwerken und internationale Programmvergleiche beschrieben. Die Anwendung von ATHLET mit gekoppelter 3D Neutronenkinetik für Störfallanalysen wird an 2 Beispielen demonstriert. Mit den gekoppelten Programmsystemen sind erstmals konsistente Störfallanalysen ohne zusätzliche konservative Annahmen möglich. Entwicklungsbedarf besteht noch bei der Berücksichtigung von 3D Temperatur- und Borkonzentrationsverteilungen innerhalb des Reaktors,
die den hypothetischen Störfallablauf wesentlich beeinflussen können.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1694-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:creator><![CDATA[Langenbuch, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1694-7</dc:identifier>
<dc:title><![CDATA[Gekoppelte Berechnungen von Thermohydraulik und Neutronenkinetik]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik, 18. - 20. Mai 1999, Karlsruhe, Sammelband "Neue Ergebnisse aus F+E zur Fluiddynamik und Reaktorphysik", Inforum Verlagsgesellschaft, Bonn, Juni 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Es wird ein Überblick über den Entwicklungsstand und die Anwendung von Computercodes mit Kopplung von thermohydraulischen Anlagenmodellen von Kernkraftwerken und 3D Neutronenkinetik gegeben. Insbesondere wird auf die Ankopplung von Neutronenkinetikmoduln an den Thermohydraulikcode ATHLET eingegangen. Es werden Arbeiten zur Validierung der Codekomplexe durch Nachrechnung von transienten Prozessen in Kernkraftwerken und internationale Programmvergleiche beschrieben. Die Anwendung von ATHLET mit gekoppelter 3D Neutronenkinetik für Störfallanalysen wird an 2 Beispielen demonstriert. Mit den gekoppelten Programmsystemen sind erstmals konsistente Störfallanalysen ohne zusätzliche konservative Annahmen möglich. Entwicklungsbedarf besteht noch bei der Berücksichtigung von 3D Temperatur- und Borkonzentrationsverteilungen innerhalb des Reaktors,
die den hypothetischen Störfallablauf wesentlich beeinflussen können.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2103-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Fontaine, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2103-1</dc:identifier>
<dc:title><![CDATA[Holes in Boron-Doped Diamond: Comparison Between Experiment and a New Model]]></dc:title>
<dc:source><![CDATA[10th European Conference on Diamond, Diamond-Like Materials, Carbon Nanotubes, Nitrides & Silicon Carbides, nPrague, CZ, Sept. 12-17, 1999]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[We present a model for the calculation of the hole concentration in boron-doped diamond. It is based on details of the structure of the valence band and on a careful energy balance around the valence band edge. The effect of a variable hole effective mass is first examined. It is found that both the hole concentration and its activation energy increase with increasing hole effective mass. The calculations are then compared to some available experimental data. Good agreement between experiment and calculation is reached. It is concluded that the model rightly describes the thermal generation of the holes from the acceptor levels to the valence band. The difficulty to determine the acceptor and donor concentration independently from the hole effective mass is finally discussed.]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:1700-1</identifier>
<datestamp>2023-05-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Bauer, R.]]></dc:creator>
<dc:creator><![CDATA[Vorieger, G.]]></dc:creator>
<dc:creator><![CDATA[Walter, B.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Füchtner, F.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Zwiener, U.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1700-1</dc:identifier>
<dc:title><![CDATA[Upregulation of the Aromatic Amino Acid Decarboxylase under Neonatal Asphyxia]]></dc:title>
<dc:source><![CDATA[Neurobiology of Disease 6, (1999) 131-139]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Perinatal hypoxic-ischemic cerebral injury is a major determinant of neurologic morbidity and mortality in the neonatal period and later in childhood. There is evidence that the dopaminergic system is sensitive to asphyxia. However, the respective enzyme activities have not yet been measured in the living neonatal brain. In this study, we hav used F18-labeled 6-fluoro-L-3,4-dihydroxyphenylalanine (FDOPA) together with positron-emission tomography l(PET) to estimate the activity of the aromatic amino acid decarboxylase (AADC), the ultimate enzyme in the synthesis of dopamine (DA), in the brain of newborn piglets. Simultaneously, the cerebral blood flow (CBF) was measured with colored microspheres. Asphyxia elicited an up to threefold increase of the CBF. Despite this, the blood-brdain transfer of FDOPA as well as the clearance rate constants from brain were unchanged. However, the synthesis rate of FDA from FDOPA was significantly increased in frontal cortex, striatum, and midbrain. The increase of the AADC activity and the decrease of monoamine oxidase activity may contribute to the increase of extracellular DA during asphyxia which is expected to be involved in severe disturbances of neuronal metabolism, e.g., by generating free radicals.]]></dc:description>
<dc:subject><![CDATA[asphyxia]]></dc:subject>
<dc:subject><![CDATA[aromatic amino acid decarboxylase]]></dc:subject>
<dc:subject><![CDATA[DOPA]]></dc:subject>
<dc:subject><![CDATA[dopamine metabolism]]></dc:subject>
<dc:subject><![CDATA[neonatal pigs]]></dc:subject>
<dc:subject><![CDATA[positron-emission tomography]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1006/nbdi.1998.0232]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:1702-1</identifier>
<datestamp>2019-03-04</datestamp>
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</header>
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            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Horche, W.]]></dc:creator>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Schäfer, F.]]></dc:creator>
<dc:creator><![CDATA[Trostel, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1702-1</dc:identifier>
<dc:title><![CDATA[Summary Technical Report of PMK-2 Test No. 2:Pressuriser Surge Line Break Verifikation Report]]></dc:title>
<dc:source><![CDATA[Gesellschaft für Anlagen- und Reaktorsicherheit mbH, Garching, Nov. 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The report deals with the results of ATHLET post-test calculations for an experiment at the Hungarian integral test facility PMK-2. The experiment pressurizer surge line break" was carried out within the PHARE 4.2.6b project. The primary objective of this test was to provid data for the phenomena associated with a pressurizer surge line break transient. The post-test analyses were performed with ATHLET mod1.1 Cycle C by the Forschungszentrum Rossendorf (FZR) and with ATHLET mod1.1 Cycle D by the Atomic Research Institute Budapest (KFKI) and the Gesellschaft für Anlagen- und Reaktorsicherheit (GRS).
]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<record>
<header>
<identifier>HZDR:PUBLDB:1704-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Mittag, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1704-1</dc:identifier>
<dc:title><![CDATA[Dodewaard core - Reactor physical modelling and neutron kinetic computer simulations. Progress report on the application of the coupled code DYN3D-ATHLET.]]></dc:title>
<dc:source><![CDATA[BWRCA report 4.1.6-2, August 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:2156-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kachurin, G. A.]]></dc:creator>
<dc:creator><![CDATA[Leier, A. F.]]></dc:creator>
<dc:creator><![CDATA[Zhuravlev, K. S.]]></dc:creator>
<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Gutakovsky, A. K.]]></dc:creator>
<dc:creator><![CDATA[Volodin, V. A.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2156-2</dc:identifier>
<dc:title><![CDATA[Effect of ion dose and annealing mode on the photoluminescence from SiO<SUB>2</SUB>-layers implanted with Si-ions]]></dc:title>
<dc:source><![CDATA[11th Int. Conf. on Ion Beam Modification of Materials, Amsterdam,The Netherlands,
Aug. 31 - Sept. 4, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:2156-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kachurin, G. A.]]></dc:creator>
<dc:creator><![CDATA[Leier, A. F.]]></dc:creator>
<dc:creator><![CDATA[Zhuravlev, K. S.]]></dc:creator>
<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Gutakovsky, A. K.]]></dc:creator>
<dc:creator><![CDATA[Volodin, V. A.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2156-1</dc:identifier>
<dc:title><![CDATA[Effect of ion dose and annealing mode on the photoluminescence from SiO<SUB>2</SUB>-layers implanted with Si-ions]]></dc:title>
<dc:source><![CDATA[Phys. Techn. Semiconductors (in Russian) 32 (1998) 1371]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2156-1</dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:1938-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1938-1</dc:identifier>
<dc:title><![CDATA[ATHLET-Rechnungen zum IAEA-Standardproblem SPE-4]]></dc:title>
<dc:source><![CDATA[3. ATHLET-Anwendertreffen, Garching, Oktober 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The experiment to the IAEA standard problem exercise No. 4 was a 3.2 mm break on the downcomer head. The high pressure injection cooling was assumed to be not available. As an accident management measure, bleed and feed on the secondary side of the steam generator was applied. Research Center Rossendorf contributed to the experiment of SPE-4 by supplying needle shaped conductivity probes for the measurement of local void fractions in the primary circuit of the PMK-II test facility. In the course of the standard problem exercise No. 4 RCR contributed with post-test calculations using the thermalhydraulic code ATHLET.

The calculations showed, that the code was suitable to reproduce the main events of the test. Reasons for some deviations and modelling problems were discussed.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:100-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-100-1</dc:identifier>
<dc:title><![CDATA[Natural Circulation Instabilities During a Loca of VVER-Type Reactors]]></dc:title>
<dc:source><![CDATA[und Proceedings: International Conference New Trends in Nuclear System Thermohydraulics, Pisa, 30.5.-2.6.1994, pp. 793 - 797]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[In the Research Centre Rossendorf pre- and posttest calculations to the OECD/NEA/CSNI International Standard Problem No. 33 were carried out with the GRS code ATHLET. This Problem was a natural circulation experiment with stepwise reduced primary coolant inventory. In the ATHLET calculations after a drainage of about 50% of the primary inventory cyclic oscillations of the mass flows and the void fractions were observed. These are found in the experimental results also. A simple analytical model was developed to distinguish physically caused oscillations from numerically caused ones. The oscillations observed could be interpreted as density wave instability in the local recirculation loop core- bypass.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1892-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Beyer, M.]]></dc:creator>
<dc:creator><![CDATA[Carl, H.]]></dc:creator>
<dc:creator><![CDATA[Langer, L.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Seidel, A.]]></dc:creator>
<dc:creator><![CDATA[Zschau, J.]]></dc:creator>
<dc:creator><![CDATA[Nowak, K.]]></dc:creator>
<dc:creator><![CDATA[Tolksdorf, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1892-1</dc:identifier>
<dc:title><![CDATA[Aufbau eines technischen Systems zur Verbesserung der betrieblichen Überwachung der KKW durch die staatlichen Aufsichtsbehörden (Saporoshje)]]></dc:title>
<dc:source><![CDATA[Abschlußbericht im Rahmen eines BMU-Projektes in 3 Teilen: Kurzfassung, Anlage A: Textteil, Anlage B: Materialsammlung, Rossendorf; Köln, Dezember 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[In order to improve operational surveillance of a WWER-1000 unit of the Ukrainian nuclear power plant Saporoshje a technical monitoring system has been specified. The system shall enable the state regulatory and supervisory bodies to survey the unit operation independently of operators, to assess its safety status, and to impose appropriate conditions. By its up-to-date configuration the system provides early indication of any operational incident and emission of radioactive materials connected. Based on the system an immediate warning in emergency situations is possible as well as an effective emergency management. For this purpose 49 operational parameters of the unit, 18 radiological parameters of the unit and the plant site and 6 meteorological parameters are monitored. The costs of establishing the technical system in its minimal size are estimated to about 1.3 Million DM (without expenses for installation of the system and of the data networks). Additionally about 650 000 DM are required for most necessary backfitting of measuring channels. Including another unit into the monitoring system implies further costs of about 200 000 DM.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:51-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-51-1</dc:identifier>
<dc:title><![CDATA[Acoustic Leak Detection at Complicated Geometrical Structures Using Fuzzy Logic and Neural Networks]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR 93-21 October 1993, pp 1-14]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[Methods of acoustic leak monitoring are of great practical interest for the safety of pressure vessels and pipe lines not only at the primary circuit of nuclear power plants. In this report some aspects of acoustic leak localization at complicated three-dimensional topologies for the case of leakage monitoring at the reactor vessel head of a  VVER-440 are discussed.
An acoustic method based on pattern recognition is being developed. During the learning phase, the localization classifier is trained with sound patterns that are generated with simulated leaks at all locations endangered by leak. After training unknown leak positions can be recognized through comparison with the training patterns.
The sound patterns of the simulated leaks are simultaneously detected with an AE-sensor array and with high frequency microphones measuring structureborne sound and airborne noise, respectively.
The initial results show the used classifiers principally to be capable of detecting and locating leaks, but they also show that further investigations are necessary to develop a reliable method. ]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:1895-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Zschau, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1895-1</dc:identifier>
<dc:title><![CDATA[Konzeption zur Ausgestaltung des technischen Systems für das BMU-Projekt "Spezifikation Fernübertragung Saporoshje"]]></dc:title>
<dc:source><![CDATA[Fachbericht FWSF-20/93, Juni 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[In the report the boundary conditions and the resulting technical possibilities are described for the construction of a technical system for remote monitoring of the nuclear power plant Zaporosh`ye, unit 5, available for the supervision by the state regulatory body. The general structure of the system and especially different technical solutions for the remote data transfer are discussed in more detail.]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:402-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Fülle, R.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-402-1</dc:identifier>
<dc:title><![CDATA[Forschungszentrum Rossendorf; Jahresbericht 1993/94]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-100]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-402-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:412-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bojarevics, A.]]></dc:creator>
<dc:creator><![CDATA[Gelfgat, Y. M.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-412-1</dc:identifier>
<dc:title><![CDATA[Testing of a new experimental technique to study MHD-Associated phenomena with free liquid metal surface]]></dc:title>
<dc:source><![CDATA[Int. Riga Conference on MHD, August 1995, Riga]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:format><![CDATA[application/pdf]]></dc:format>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:457-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Scheffler, M.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-457-1</dc:identifier>
<dc:title><![CDATA[Theoretische Modellierung des Druckbehälters und der Druckbehältereinbauten eines Siedewasserreaktors (SWR)]]></dc:title>
<dc:source><![CDATA[Institutsbericht]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1943-1</identifier>
<datestamp>2023-05-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Eckert, K.]]></dc:creator>
<dc:creator><![CDATA[Grahn, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1943-1</dc:identifier>
<dc:title><![CDATA[Plume and finger regimes driven by an exothermic interfacial reaction]]></dc:title>
<dc:source><![CDATA[Physical Review Letters 82, 31 May 1999, Number22, 4436-4439]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[We study the pattern formation in a chemical two-layer system, placed in a Hele-Shaw cell. The upper layer is an organic solvent in which a carboxylic acid is  dissolved. The lower layer consists of water containing an inorganic base. We report on a novel instability type which is driven by an exothermic neutralisation reaction in vicinity to the interface. This instability combines plume and finger regimes and gives rise to a self-sustained dynamics.]]></dc:description>
<dc:subject><![CDATA[hydrodynamic instability]]></dc:subject>
<dc:subject><![CDATA[plume regime]]></dc:subject>
<dc:subject><![CDATA[finger regime]]></dc:subject>
<dc:subject><![CDATA[interfacial reaction]]></dc:subject>
<dc:subject><![CDATA[interfacial instability]]></dc:subject>
<dc:subject><![CDATA[pattern formation]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevLett.82.4436]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1943-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1532-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:creator><![CDATA[Danilin, S.]]></dc:creator>
<dc:creator><![CDATA[Kyrki-Rajamäki, R.]]></dc:creator>
<dc:creator><![CDATA[Hadek, J.]]></dc:creator>
<dc:creator><![CDATA[Kereszturi, A.]]></dc:creator>
<dc:creator><![CDATA[Siltanen, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1532-1</dc:identifier>
<dc:title><![CDATA[A Benchmark for Coupled 3D Neutron Kinetics/Thermohydraulics System Codes - Main Steam Header Break in a NPP with VVER-440 Reactor]]></dc:title>
<dc:source><![CDATA[Proc. International Conference on Mathematics and Computation, Reactor Physics and Environmental Analysis in Nuclear Applications (MC '99), vol. 1, pp. 359-368, Senda Editorial, S.A., Madrid (Spain)]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Recently 3D neutron kinetics core models have been coupled to advanced thermohydraulics system codes. These coupled codes can be used for the analysis of the whole reactor system. In the framework of the international  "Atomic Energy Research" (AER) association on VVER Reactor Physics and Reactor Safety, a benchmark for these code systems was defined. The reference reactor is the Russian VVER-440. The response of the reactor core to a main steam header break should be investigated. Solutions were received from the following five organizations: Kurchatov Institute Moscow (Russia), VTT Energy Espoo (Finland), Nuclear Research Institute Rez (Czech Republic), KFKI AEKI Budapest (Hungary) and Forschungszentrum Rossendorf (Germany). The paper presents an overview of the results of the benchmark. A good agreement in the thermohydraulic behaviour can be observed, the main differences between the solutions arise from the use of different nuclear data.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1532-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1532-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:creator><![CDATA[Danilin, S.]]></dc:creator>
<dc:creator><![CDATA[Kyrki-Rajamäki, R.]]></dc:creator>
<dc:creator><![CDATA[Hadek, J.]]></dc:creator>
<dc:creator><![CDATA[Kereszturi, A.]]></dc:creator>
<dc:creator><![CDATA[Siltanen, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1532-7</dc:identifier>
<dc:title><![CDATA[A Benchmark for Coupled 3D Neutron Kinetics/Thermohydraulics System Codes - Main Steam Header Break in a NPP with VVER-440 Reactor]]></dc:title>
<dc:source><![CDATA[Proc. International Conference on Mathematics and Computation, Reactor Physics and Environmental Analysis in Nuclear Applications (MC '99), vol. 1, pp. 359-368, Senda Editorial, S.A., Madrid (Spain)]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Recently 3D neutron kinetics core models have been coupled to advanced thermohydraulics system codes. These coupled codes can be used for the analysis of the whole reactor system. In the framework of the international  "Atomic Energy Research" (AER) association on VVER Reactor Physics and Reactor Safety, a benchmark for these code systems was defined. The reference reactor is the Russian VVER-440. The response of the reactor core to a main steam header break should be investigated. Solutions were received from the following five organizations: Kurchatov Institute Moscow (Russia), VTT Energy Espoo (Finland), Nuclear Research Institute Rez (Czech Republic), KFKI AEKI Budapest (Hungary) and Forschungszentrum Rossendorf (Germany). The paper presents an overview of the results of the benchmark. A good agreement in the thermohydraulic behaviour can be observed, the main differences between the solutions arise from the use of different nuclear data.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1534-1</identifier>
<datestamp>2025-01-15</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Mäding, P.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1534-1</dc:identifier>
<dc:title><![CDATA[Synthesis of [1-<SUP>11</SUP>C]phenol]]></dc:title>
<dc:source><![CDATA[J. Labelled Cpd. Radiopharm. 43 (2000) 557-563]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The synthesis of n.c.a. [1-<SUP>11</SUP>C]phenol (3) which is a further important aromatic <SUP>11</SUP>C unit for potential PET radiotracers is decribed for the first time. [1-<SUP>11</SUP>C]aniline (1) was diazotized and the [1-<SUP>11</SUP>C]benzenediazonium bromide (2) formed was concentrated in situ to give 3. Before diazotization, 1 had to be purified twice by means of an adsorber resin and a cation exchange resin. Starting from the purified 1, 3 was obtained in a radiochemical purity of about 79 % within 10 min. Related to crude 1 from the one-pot process, thereproducible radiochemical yield of 3 was about 16 % (decay-corrected). <SUP>13</SUP>C/<SUP>11</SUP>C Co-labelling experiments were carried out in order to confirm the identity of 3 and the position of the label.]]></dc:description>
<dc:subject><![CDATA[PET]]></dc:subject>
<dc:subject><![CDATA[<SUP>11</SUP>C-ring labelling]]></dc:subject>
<dc:subject><![CDATA[diazotization]]></dc:subject>
<dc:subject><![CDATA[[1-<SUP>11</SUP>C]aniline]]></dc:subject>
<dc:subject><![CDATA[[1-<SUP>11</SUP>C]phenol]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:14525-1</identifier>
<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Krause, M.]]></dc:creator>
<dc:creator><![CDATA[Abrasonis, G.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Kolitsch, A.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14525-1</dc:identifier>
<dc:title><![CDATA[Carbon:Vanadium (C:V) nanocomposite filmsfor tribological applications]]></dc:title>
<dc:source><![CDATA[12th International conference on Plasma Surface Engineering, 13.-17.09.2010, Garmisch-Partenkirchen, Deutschland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Nanocomposites are heterogeneous materials wherein the lateral extension of at least one component is lower than 100 nm.[1] They represent a new class of functional materials, whose properties cannot be predicted from those of their constituents alone. Among the various classes of nanocomposites, metal-containing nano-particles embedded in a carbon matrix have recently attracted considerable interest regarding their structure and properties.[2,3] 
This study focuses on the structure and the mechanical properties of C:V nanocomposites. A series of C:V films with a varying vanadium concentration of 2 at.% ≤ xv ≤ 50 at.% was grown on silicon by DC dual magnetron sputtering. Depending on the metal concentration, significant structural variations were observed within both phases (dispersed phase and matrix) of the nanocomposite. At low vanadium concentrations, an amorphous metal rich and an amorphous carbon phase are formed. An increasing metal content promotes the formation of cubic VC and a graphitic carbon phase. With optimized deposition parameters, the hardness of the C:V nanocomposite films is higher then 10 GPa, and the elastic modulus achieves values of about 130 GPa. The friction coefficients for sliding conditions are as good as 0.1. 

[1]	P. M. Ajayan, L.S. Schadler, P.V. Braun, Nanocomposites Science and Technology, Wiley, 2005
[2]	T. Hayashi, S. Hirono, M. Tomita, S. Umemura, Nature 381, 772-774 (1996)
[3]	M. Krause et al., Phys. Stat. Sol. (B), 244, 4236-4239 (2007); G. Abrasonis et al. Carbon, 45, 2995-3006 (2007); M. Berndt et al., Plasma Process. Polym. 6, S902S906 (2009); C. Adelhelm et al., J. Appl. Phys. 105, 033522 (2009); M. Magnuson et al. Phys. Rev. B, 80, 235108 (2009).]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:14210-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:creator><![CDATA[Joseph, C.]]></dc:creator>
<dc:creator><![CDATA[Schmeide, K.]]></dc:creator>
<dc:creator><![CDATA[Sachs, S.]]></dc:creator>
<dc:creator><![CDATA[Brendler, V.]]></dc:creator>
<dc:creator><![CDATA[Geipel, G.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14210-1</dc:identifier>
<dc:title><![CDATA[Sorption of uranium(VI) onto Opalinus Clay in the absence and presence of humic acid in Opalinus Clay pore water]]></dc:title>
<dc:source><![CDATA[Chemical Geology 284(2011), 240-250]]></dc:source>
<dc:date>2011</dc:date>
<dc:description><![CDATA[The U(VI) sorption onto Opalinus Clay (OPA), a natural clay rock from Mont Terri, Switzerland, was investigated in the absence and presence of humic acid under aerobic conditions using synthetic OPA pore water (I = 0.34 M, pH 7.6) as background electrolyte. The results show that the U(VI) sorption onto OPA is low and not influenced by humic acid. This can be attributed to the dissolution of calcite, a mineral constituent of the clay. The resulting calcium ions (up to 25 mM) in the pore water influence both the U(VI) speciation and the speciation of humic acid. In OPA pore water the U(VI) speciation is dominated by the neutral complex Ca2UO2(CO3)3(aq) both in the absence and presence of humic acid. Its predominance was verified by time-resolved laser-induced fluorescence spectroscopy (TRLFS). Speciation estimations for humic acid show that calcium ions saturate the humic acid binding sites almost completely. Thus, only few humic acid binding sites are available for U(VI) complexation at pH 7.6. For the sorption of U(VI) and humic acid onto OPA distribution coefficients, Kd, were determined and amount to (0.0222 ± 0.0004) m3/kg and (0.129 ± 0.006) m3/kg, respectively. In conclusion, calcium ions determine the interaction processes of U(VI) and humic acid in the OPA system.]]></dc:description>
<dc:subject><![CDATA[uranium(VI)]]></dc:subject>
<dc:subject><![CDATA[humic acid]]></dc:subject>
<dc:subject><![CDATA[sorption]]></dc:subject>
<dc:subject><![CDATA[speciation]]></dc:subject>
<dc:subject><![CDATA[Opalinus Clay]]></dc:subject>
<dc:subject><![CDATA[calcium]]></dc:subject>
<dc:subject><![CDATA[Ca2UO2(CO3)3(aq)]]></dc:subject>
<dc:subject><![CDATA[TRLFS]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:14338-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:creator><![CDATA[Abrasonis, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14338-1</dc:identifier>
<dc:title><![CDATA[(i)PVD growth of carbon-transition metal nanocomposites: from energetic condensation to periodic precipitation patterns]]></dc:title>
<dc:source><![CDATA[Nanofair 2010, 06.-07.07.2010, Dresden, Germany]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[(i)PVD growth of carbon-transition metal nanocomposites: from energetic condensation to periodic precipitation patterns]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<header>
<identifier>HZDR:PUBLDB:292-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Mittag, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-292-2</dc:identifier>
<dc:title><![CDATA[Solution of AER Benchmark Problem on Control Rod Worth of Paks VVER-440 by the Code DYN3D]]></dc:title>
<dc:source><![CDATA[Proc. 4th AER Symposium, Sozopol, Bulgaria, October 10 - 13, 1994, pp. 443 - 461]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[This paper presents a solution of the AER benchmark problem specified for the 7th cycle of the Paks-2 VVER-440 reactor. The problem concerns control rod worth for both the beginning and the end of burnup cycle states. The burnup distribution of cycle 7 was calculated starting from the burnup values of the third cycle. The calculations were carried out by using the burnup option of the DNYN3D code and a MAGRU group data library. The results are compared with calculations published by other authors on AER meetings. Furthermore the influence on reactivity of some control rod properties typical for VVER-440 was studied.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:292-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:creator><![CDATA[Mittag, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-292-1</dc:identifier>
<dc:title><![CDATA[Solution of AER Benchmark Problem on Control Rod Worth of Paks VVER-440 by the Code DYN3D]]></dc:title>
<dc:source><![CDATA[4th AER Symposium in Sozopol, Bulgaria, Oct. 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[This paper presents a solution of the AER benchmark problem specified for the 7th cycle of the Paks-2 VVER-440 reactor. The problem concerns control rod worth for both the beginning and the end of burnup cycle states. The burnup distribution of cycle 7 was calculated starting from the burnup values of the third cycle. The calculations were carried out by using the burnup option of the DNYN3D code and a MAGRU group data library. The results are compared with calculations published by other authors on AER meetings. Furthermore the influence on reactivity of some control rod properties typical for VVER-440 was studied.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:14203-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Vinnichenko, M.]]></dc:creator>
<dc:creator><![CDATA[Cornelius, S.]]></dc:creator>
<dc:creator><![CDATA[Gago, R.]]></dc:creator>
<dc:creator><![CDATA[Krause, M.]]></dc:creator>
<dc:creator><![CDATA[Shevchenko, N.]]></dc:creator>
<dc:creator><![CDATA[Rogozin, A.]]></dc:creator>
<dc:creator><![CDATA[Munnik, F.]]></dc:creator>
<dc:creator><![CDATA[Kolitsch, A.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14203-1</dc:identifier>
<dc:title><![CDATA[Effect of secondary phase formation on electrical and optical properties of Al-doped ZnO]]></dc:title>
<dc:source><![CDATA[EFDS-Workshop Transparente leitfähige Oxide - Festkörperphysikalische Grundlagen und Technologie, 01.-02.06.2010, Dresden, Germany]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[It has been shown that increasing substrate temperature above its optimum value leads to an increase of Al concentration in the AZO films, which exceeds the solubility limit and triggers the formation of an insulating metastable homologous (ZnO)3Al2O3 phase. The formation of (ZnO)3Al2O3 is established for the AZO films grown in a given range of deposition conditions, while the films grown at substantially different conditions may show formation of other secondary phases (e.g. aluminium oxide or spinel). This (ZnO)3Al2O3 impedes crystal growth and causes a significant increase of free electron scattering. In turn, it leads to an increase of electrical resistivity of the films. This phase has been observed by XANES even in the films with the lowest Al concentration and the best crystallinity. Increase of this phase volume fraction with increasing Al concentration correlates with observed changes in the film Raman and optical constants spectra.]]></dc:description>
<dc:subject><![CDATA[Al-doped ZnO]]></dc:subject>
<dc:subject><![CDATA[homologous metastable phase]]></dc:subject>
<dc:subject><![CDATA[(ZnO)3Al2O3]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:14204-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Conroy, D. J. R.]]></dc:creator>
<dc:creator><![CDATA[Millner, P. A.]]></dc:creator>
<dc:creator><![CDATA[Stewart, D. I.]]></dc:creator>
<dc:creator><![CDATA[Pollmann, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14204-1</dc:identifier>
<dc:title><![CDATA[Biosensing for the Environment and Defence: Aqueous Uranyl Detection Using Bacterial Surface Layer Proteins]]></dc:title>
<dc:source><![CDATA[Sensors 10(2010), 4739-4755]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The fabrication of novel uranyl (UO2 2+) binding protein based sensors is reported. The new biosensor responds to picomolar levels of aqueous uranyl ions within minutes using Lysinibacillus sphaericus JG-A12 S-layer protein tethered to gold electrodes. In comparison to traditional self assembled monolayer based biosensors the porous bioconjugated layer gave greater stability, longer electrode life span and a denser protein layer. Biosensors responded specifically to UO2 2+ ions and showed minor interference from Ni2+, Cs+, Cd2+ and Co2+. Chemical modification of JG-A12 protein phosphate and carboxyl groups prevented UO2 2+ binding, showing that both moieties are involved in the recognition to UO2 2+.]]></dc:description>
<dc:subject><![CDATA[S-layer]]></dc:subject>
<dc:subject><![CDATA[surface layer]]></dc:subject>
<dc:subject><![CDATA[protein biosensor]]></dc:subject>
<dc:subject><![CDATA[uranium]]></dc:subject>
<dc:subject><![CDATA[uranyl]]></dc:subject>
<dc:subject><![CDATA[metal ion]]></dc:subject>
<dc:subject><![CDATA[sequestering]]></dc:subject>
<dc:subject><![CDATA[impedance spectroscopy]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<identifier>HZDR:PUBLDB:14221-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
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            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Knüpfer, A.]]></dc:creator>
<dc:creator><![CDATA[Bussmann, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14221-1</dc:identifier>
<dc:title><![CDATA[PiC on GPGPUs]]></dc:title>
<dc:source><![CDATA[CiHPC Competence in High Performance Computing HPC Status Conference of Gauß-Allianz e.V., 22.-24.06.2010, Schwetzingen, Deutschland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Implementation of a modular Particle-in-Cell Algorithm for GPGPU Clusters]]></dc:description>
<dc:subject><![CDATA[gpu]]></dc:subject>
<dc:subject><![CDATA[gpgpu]]></dc:subject>
<dc:subject><![CDATA[graphic card]]></dc:subject>
<dc:subject><![CDATA[algorithm]]></dc:subject>
<dc:subject><![CDATA[simulation]]></dc:subject>
<dc:subject><![CDATA[particle-in-cell]]></dc:subject>
<dc:subject><![CDATA[pic]]></dc:subject>
<dc:subject><![CDATA[cuda]]></dc:subject>
<dc:subject><![CDATA[mpi]]></dc:subject>
<dc:subject><![CDATA[parallel]]></dc:subject>
<dc:subject><![CDATA[high-performance]]></dc:subject>
<dc:subject><![CDATA[computing]]></dc:subject>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14221-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1944-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Noetzel, J.]]></dc:creator>
<dc:creator><![CDATA[Handstein, A.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Prokert, F.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Thomas, J.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1944-1</dc:identifier>
<dc:title><![CDATA[Co/Cu solid solution prepared by ion implantation]]></dc:title>
<dc:source><![CDATA[Journal of Magnetism and Magnetic Materials, 205 (1999) 177-185]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[A Co/Cu solid solution is prepared by direct implantation of 200 keV Co ions into Cu targets. The maximum concentration at this ion energy is limited to 25 at.% Co due to sputtering. Magnetic measurements show a spin-glass behaviour, as expected for a
solid solution of Co in Cu. At about 630 K the solid solution starts to decompose into
clusters. After heat treatment, the sample shows ferro- and superparamagnetic behaviour, indicating that the size of the clusters is broadly distributed.]]></dc:description>
<dc:subject><![CDATA[Co/Cu]]></dc:subject>
<dc:subject><![CDATA[impantation]]></dc:subject>
<dc:subject><![CDATA[spin-glass]]></dc:subject>
<dc:subject><![CDATA[spinodal decomposition]]></dc:subject>
<dc:type>info:eu-repo/semantics/preprint</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1944-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:1945-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Peshier, A.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1945-1</dc:identifier>
<dc:title><![CDATA[Quasiparticle description of deconfined matter at finite mu and T]]></dc:title>
<dc:source><![CDATA[Proceedings of the ECT* workshop "Understanding Deconfinement in QCD", Trento, March 1-13, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[An effective quasiparticle description of deconfined QCD thermodynamics compatible with both finite temperature nonperturbative lattice data and the asymptotic limit is generalized to finite chemical potential.
 Implications for the N <SUB>f</SUB> = 4 flavor lattice data extended to mu > 0 as well as for deconfined matter with realistic quark masses are considered.]]></dc:description>
<dc:subject><![CDATA[QCD]]></dc:subject>
<dc:subject><![CDATA[thermodynamics]]></dc:subject>
<dc:subject><![CDATA[quasiparticle]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1945-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:534-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-534-1</dc:identifier>
<dc:title><![CDATA[A Neural-Network Approach for Acoustic Leak Monitoring in Pressurized Plants with Complicated Topologies]]></dc:title>
<dc:source><![CDATA[Control Engineering Practice, Vol. 4, No. 9, pp. 1271-1276, 1996, pp. 1271 - 1276]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[A neural-network approach has been developed for localizing leakages and estimating the leak rate in pressurized plants with complicated three-dimensional structures. Results are presented from experiments with simulated leaks at a VVER-440 reactor vessel head. As features for characterizing the occurrence and the location of a leak, RMS values of acoustic emission sensors and coherence values and power spectra of microphone signals were used. Three-layer perceptron networks were found to be best suited for leak localization and for estimation of leak rates. However, the estimation of leak rates required an additional neural network because a different normalization procedure was necessary for extracting features from the RMS values of the acoustic emission sensors. Perceptron networks with continuously valued outputs corresponding to the coordinates of the leak positions were useful for classifying even positions which had not been offered during training.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-534-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:3091-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hennig, C.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Roßberg, A.]]></dc:creator>
<dc:creator><![CDATA[Funke, H.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3091-1</dc:identifier>
<dc:title><![CDATA[EXAFS as a tool for bond length determination in the environment of heavy atoms]]></dc:title>
<dc:source><![CDATA[J. Synchrotron Rad. 8, 695-697 (2001)]]></dc:source>
<dc:date>2001</dc:date>
<dc:description><![CDATA[The scattering amplitude of a heavy atom structure is generated mainly by the contribution of the heavy scatterers, because the scattering amplitude is proportional to the electron density. In the case of a low scattering part of light atoms this may lead to incorrect calculation of atomic coordinates. Is the structure model similar to correct structure, then it is very difficult to find an independent criterion for the accuracy of the bond lengths.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-3091-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:1535-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kern, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1535-1</dc:identifier>
<dc:title><![CDATA[Void fraction measurement in foams using needle shaped conductivity probes]]></dc:title>
<dc:source><![CDATA[The Second European Congress on Chemical Engineering: "Chemical Engineering for competitiveness and employment in process industries", 5-7 October 1999, Montpellier, France, proceedings on CD-ROM, 09010004.pdf.]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Needle Shaped Conductivity Probes have been applied to measure the properties of aqueous alcohol foams. Simultaneous usage of gamma densitometry and video imaging should allow a calibration and prove the values of the probe. The results show that the conductivity probes are able to measure in the foam zone as well as in the bubbly flow whereas the geometry of the foam causes some problems to detect reliably the foam bubbles.]]></dc:description>
<dc:subject><![CDATA[Conductivity Probes]]></dc:subject>
<dc:subject><![CDATA[Foam]]></dc:subject>
<dc:subject><![CDATA[Void Fraction]]></dc:subject>
<dc:subject><![CDATA[Bubble Size]]></dc:subject>
<dc:subject><![CDATA[Coalescence]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1535-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:1535-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kern, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1535-7</dc:identifier>
<dc:title><![CDATA[Void fraction measurement in foams using needle shaped conductivity probes]]></dc:title>
<dc:source><![CDATA[The Second European Congress on Chemical Engineering: "Chemical Engineering for competitiveness and employment in process industries", 5-7 October 1999, Montpellier, France, proceedings on CD-ROM, 09010004.pdf.]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Needle Shaped Conductivity Probes have been applied to measure the properties of aqueous alcohol foams. Simultaneous usage of gamma densitometry and video imaging should allow a calibration and prove the values of the probe. The results show that the conductivity probes are able to measure in the foam zone as well as in the bubbly flow whereas the geometry of the foam causes some problems to detect reliably the foam bubbles.]]></dc:description>
<dc:subject><![CDATA[Conductivity Probes]]></dc:subject>
<dc:subject><![CDATA[Foam]]></dc:subject>
<dc:subject><![CDATA[Void Fraction]]></dc:subject>
<dc:subject><![CDATA[Bubble Size]]></dc:subject>
<dc:subject><![CDATA[Coalescence]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1535-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:1536-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1536-1</dc:identifier>
<dc:title><![CDATA[Measurement of Gas Fraction, Gas Velocity and Volume Flow by Electrode Mesh Sensors]]></dc:title>
<dc:source><![CDATA[ECCE 2 - Second European Congress of Chemical Engineering - Montpellier 05.-07.10.1999, paper CDROM 11280001.pdf.]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[A new wire-mesh sensor for gas-liquid flows is presented. Air-water mixtures in a vertical pipe were studied in a wide range of superficial ve-locities. Gas fraction and gas velocity profiles as well as a high resolution imaging of the flow structure are obtained. A volume flow rate measure-ment is feasible.]]></dc:description>
<dc:subject><![CDATA[gas-liquid flow]]></dc:subject>
<dc:subject><![CDATA[flow visualisation]]></dc:subject>
<dc:subject><![CDATA[gas fraction]]></dc:subject>
<dc:subject><![CDATA[gas velocity]]></dc:subject>
<dc:subject><![CDATA[gas flow rate]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1536-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:1536-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1536-7</dc:identifier>
<dc:title><![CDATA[Measurement of Gas Fraction, Gas Velocity and Volume Flow by Electrode Mesh Sensors]]></dc:title>
<dc:source><![CDATA[ECCE 2 - Second European Congress of Chemical Engineering - Montpellier 05.-07.10.1999, paper CDROM 11280001.pdf.]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[A new wire-mesh sensor for gas-liquid flows is presented. Air-water mixtures in a vertical pipe were studied in a wide range of superficial ve-locities. Gas fraction and gas velocity profiles as well as a high resolution imaging of the flow structure are obtained. A volume flow rate measure-ment is feasible.]]></dc:description>
<dc:subject><![CDATA[gas-liquid flow]]></dc:subject>
<dc:subject><![CDATA[flow visualisation]]></dc:subject>
<dc:subject><![CDATA[gas fraction]]></dc:subject>
<dc:subject><![CDATA[gas velocity]]></dc:subject>
<dc:subject><![CDATA[gas flow rate]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1536-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1537-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Dudlik, A.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Schlüter, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1537-1</dc:identifier>
<dc:title><![CDATA[Visualization of cavitating liquid flow behind fast acting valve]]></dc:title>
<dc:source><![CDATA[ECCE 2 - Second European Congress of Chemical Engineering - Montpellier 05.-07.10.1999, paper CDROM 11270003.pdf.]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The paper presents high speed measurements of the transient void fraction distribution in the cavitating flow behind fast acting butterfly valves. A new electrode mesh sensor with a time resolution of 1024 frames per second was used. As a result, a new method to avoid cavitational water hammers was found.]]></dc:description>
<dc:subject><![CDATA[Plant safety]]></dc:subject>
<dc:subject><![CDATA[pipelines]]></dc:subject>
<dc:subject><![CDATA[water hammers]]></dc:subject>
<dc:subject><![CDATA[cavitation collapses]]></dc:subject>
<dc:subject><![CDATA[fast two-phase flow visualisation]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1537-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1537-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Dudlik, A.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Schlüter, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1537-7</dc:identifier>
<dc:title><![CDATA[Visualization of cavitating liquid flow behind fast acting valve]]></dc:title>
<dc:source><![CDATA[ECCE 2 - Second European Congress of Chemical Engineering - Montpellier 05.-07.10.1999, paper CDROM 11270003.pdf.]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The paper presents high speed measurements of the transient void fraction distribution in the cavitating flow behind fast acting butterfly valves. A new electrode mesh sensor with a time resolution of 1024 frames per second was used. As a result, a new method to avoid cavitational water hammers was found.]]></dc:description>
<dc:subject><![CDATA[Plant safety]]></dc:subject>
<dc:subject><![CDATA[pipelines]]></dc:subject>
<dc:subject><![CDATA[water hammers]]></dc:subject>
<dc:subject><![CDATA[cavitation collapses]]></dc:subject>
<dc:subject><![CDATA[fast two-phase flow visualisation]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1537-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1415-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Rother, A.]]></dc:creator>
<dc:creator><![CDATA[Knieß, T.]]></dc:creator>
<dc:creator><![CDATA[Pütz, M.]]></dc:creator>
<dc:creator><![CDATA[Jungclas, H.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1415-1</dc:identifier>
<dc:title><![CDATA[Nicotinamide-substituted complexes as redox markers 2. Synthesis of a <SUP>99</SUP>Tc dihydropyridine mixed-ligand complex and investigation of the stability in tissue homogenates]]></dc:title>
<dc:source><![CDATA[J. Labelled Cpd. Radiopharm. 42 (1999) 673-681]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[For developing a dihydropyridine/pyridinium salt redox delivery system that could be useful for SPECT investigations by <SUP>99m</SUP>Tc compounds  the synthesis of a mixed-ligand complex of the long-lived isotope <SUP>99</SUP>Tc is described. The new compound bearing a pyridinium salt moiety was characterised by NMR-spectrometry and X-ray structure analysis. By reduction with sodium dithionite the corresponding 1,4-dihydropyridine complex was prepared and the stability in buffer, tissue homogenates, blood plasma and cerebrospinal fluid was investigated by UV-VIS spectrometry.]]></dc:description>
<dc:subject><![CDATA[redox delivery system]]></dc:subject>
<dc:subject><![CDATA[pyridinium salt]]></dc:subject>
<dc:subject><![CDATA[1,4-dihydropyridine]]></dc:subject>
<dc:subject><![CDATA[<SUP>99</SUP>Tc-complexes]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1470-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Römer, J.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Kasch, H.]]></dc:creator>
<dc:creator><![CDATA[Scheller, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1470-1</dc:identifier>
<dc:title><![CDATA[Herstellung und Charakterisierung der Sulfamate von Estra-3,17xi-diolen. Schnelle Umsetzung von 16alpha-Fluorestradiol zum 16alpha-Fluorestradiol-3,17beta-disulfamat (Preparation and Characterization of the sulphamates of estra-3,17xi-diols. Rapid conversion of 16alpha-fluoroestradiol into 16alpha-fluoroestradiol-3,17beta-disulfamate)]]></dc:title>
<dc:source><![CDATA[J. Prakt. Chem. 341 (1999) 574-587]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Estradiols are able to form two monosulphamates and one disulphamate. In the present work all the sulphamates of 17alpha-estradiol, 17beta-estradiol and 16alpha-fluoroestradiol were synthesized and characterized. For characterization NMR spectroscopy was used first of all. Because of its high sulphatase inhibitory efficiency and 16alpha-fluoroestradiol-3,17beta-disulphamate found a special interest among the new sulphamates. Just the binding between sulphamate and sulphatase favoured 16alpha-[<SUP>18</SUP>F]fluorestradiol-3,17beta-disulphamate to a new radiopharmaceutical which should be appropriate to image the active sites of sulphatase by positron emission tomography. The preparation of  16alpha[<SUP>18</SUP>F]fluoroestradiol-3,17beta-disulphamate requires a simple and rapid procedure. The conditions for such a procedure were also elaborated using non-radioactive substances.]]></dc:description>
<dc:subject><![CDATA[Fluorine]]></dc:subject>
<dc:subject><![CDATA[Steroids]]></dc:subject>
<dc:subject><![CDATA[Synthetic methods]]></dc:subject>
<dc:subject><![CDATA[Estradiols]]></dc:subject>
<dc:subject><![CDATA[Sulfamate]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>ger</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<header>
<identifier>HZDR:PUBLDB:1640-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barz, H.-U.]]></dc:creator>
<dc:creator><![CDATA[Konheiser, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1640-1</dc:identifier>
<dc:title><![CDATA[Rossendorf Monte Carlo Calculations for the Balakovo-3 Experiment and Comparison to Experimental Results]]></dc:title>
<dc:source><![CDATA[International Workshop on the Balakovo-3 Interlaboratory Pressure Vessel Dosimetry Experiment, Rossendorf, 2. - 5. September 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[In this report is described the theoretical and experimental determination of all needed parameters  for the neutron exposure of the different specimens that were irradiated in the Rheinsberg reactor within the period from 1984 until 1988 to obtain data for neutron embrittlement studies.
The methodical approach is represented, possible sources of errors are discussed and all the needed results are collected. The work can be divided into a pure calculation part, into the description of the extraction of the monitors and their gamma spectrometric analysis and into the discussion of the spectrum adjustment procedure which combines experimental and theoretical results. Therefore, this representation deals not only with this special task but gives also a survey about the methodical approach and the state of art in Rossendorf for the general problem of determination of neutron fluences, because the developed methods are generally applicable and not limited to the special problem of neutron embrittlement. Different  problems with respect of neutron fluences exist also in Germany.
The calculation of fluences is based on an accurate description of the history of the reactor for all irradiation periods, i.e. the time and space dependence of burn up, power and fisson sources. This information was given for a time and space grid of all fuel elements. 
For the calculation of the fluences were not used time dependent fluxes, but at first  integral sources of fission neutrons are calculated for different fissionable isotopes. Using these given integral source distributions the fluences were calculated and the results from the different fissionable source were composed. For the improvement of the comparison between experimental and theoretical results a special method was used calculating special integral sources for the given detector, because each detector according to its decay notes another integral source resp. flux distribution, which has to be theoretically corrected. 
The basis of all transport calculations was the Monte Carlo method in a special problem adjusted kind.  Special procedures were developed and successfully applicated for the reduction of statistical errors. Therefore, also for single specimens results with small statistical errors were obtained. It is remarkable that this accurate method which allows a realistic 3-dimensional description of the system reactor-surroundings could be applied with reasonable calculation times for the great number of needed calculations.
To reduce the uncertainties connected by using of group cross sections some calculations with different group sets are performed. It could be shown, that for the Russian ABBN-78 group data (10 groups within the relevant energy range) and the group data on the base of JEF-1 (123 energy groups) a very good agreement could be realized. Also the application of the known code MCNP with a further independent data base gave the same results  within the statistical errors. Furthermore we have used for tests the newest Russian group data MULTIK-90, which we have obtained from the Phys. Energetic Institute Obninsk.
Besides the standard CT1-, Charpy- and tension-specimens were irradiated  CTX-, CT05- and CT5-specimens, too. The usual positions of these irradiations were the so-called Target channels. For some cases  the Irradiation or Surveillance channels have been used, too.
The experimental determination of the neutron fluences was performed by the gamma spectrometric analysis of the used activation detectors. For the Russian detectors the elements Fe, Cu and Nb were used. For some measurements detectors from Rossendorf were applied. The contents of these detectors are Ti, Fe, Ni, Co, Cu, and Ag. Additionally  103Rh was used, too.
All the methods for the analysis of experiments have been enlarged and improved, because many difficulties beginning with the extraction of detectors and their bad consistency had to be overcome. An essential problem was the est ...]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:2352-1</identifier>
<datestamp>2025-04-16</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Jenkins, D. G.]]></dc:creator>
<dc:creator><![CDATA[Wadsworth, R.]]></dc:creator>
<dc:creator><![CDATA[Cameron, J. A.]]></dc:creator>
<dc:creator><![CDATA[Clark, R. M.]]></dc:creator>
<dc:creator><![CDATA[Fossan, D. B.]]></dc:creator>
<dc:creator><![CDATA[Hibbert, I. M.]]></dc:creator>
<dc:creator><![CDATA[Janzen, V. P.]]></dc:creator>
<dc:creator><![CDATA[Krücken, R.]]></dc:creator>
<dc:creator><![CDATA[Lane, G. J.]]></dc:creator>
<dc:creator><![CDATA[Lee, I. Y.]]></dc:creator>
<dc:creator><![CDATA[Macchiavelli, A. O.]]></dc:creator>
<dc:creator><![CDATA[Parry, C. M.]]></dc:creator>
<dc:creator><![CDATA[Sears, J. M.]]></dc:creator>
<dc:creator><![CDATA[Smith, J. F.]]></dc:creator>
<dc:creator><![CDATA[Frauendorf, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2352-1</dc:identifier>
<dc:title><![CDATA[Confirmation of the Shears Mechanism in Near-Spherical Tin Nuclei]]></dc:title>
<dc:source><![CDATA[Physical Review Letters, Volume 83, Number 3, 19 July 1999, 500-503]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevLett.83.500]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2352-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2357-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Werner, P.]]></dc:creator>
<dc:creator><![CDATA[Eichler, S.]]></dc:creator>
<dc:creator><![CDATA[Mariani, G.]]></dc:creator>
<dc:creator><![CDATA[Kögler, R.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2357-1</dc:identifier>
<dc:title><![CDATA[TEM investigation of CxSi defects in C implanted silicon]]></dc:title>
<dc:source><![CDATA[Appl. Phys. Lett. 70 (1997) 252]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2357-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2442-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pham, M. T.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Steiner, G.]]></dc:creator>
<dc:creator><![CDATA[Oswald, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2442-1</dc:identifier>
<dc:title><![CDATA[Ion beam sensitizing of titanium surfaces to hydroxyapatite formation]]></dc:title>
<dc:source><![CDATA[Proceedings of the Eleventh International Conference on Surface Modification of Metals by Ion Beams (SMMIB'99), Sept. 19-14, 1999, Beijing, P.R. China.]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[CaO and P2O5 containing Ti surfaces were prepared and examined for their bioactivity. The preparation involved the incorporation of Ca and P into Ti by ion implantation to a total dose of up to 8 x 1017 ions/cm² with a 1.7 Ca/P ratio and a subsequent oxidation at 500 °C in O2 for 40 min. The model surfaces were examined for their reactivity toward hydroxyapatite formation by microscopically recording the mineralization in a simulated body fluid. The ion implantation modified surfaces were shown to exhibit enhanced mineralization by inducing heterogeneous nucleation, growth, and proliferation of hydroxyapatite, relative to a control sample of pure Ti. The surface induced reactivity was shown to relate to the enhanced provision of the ionic mineral components Ca2+ and HPO42- directly supplied from the surface and the substrate-mediated nucleation by hydroxylated surface TiO2.]]></dc:description>
<dc:subject><![CDATA[biomaterials]]></dc:subject>
<dc:subject><![CDATA[ion implantation]]></dc:subject>
<dc:subject><![CDATA[surface coatings]]></dc:subject>
<dc:subject><![CDATA[Ti]]></dc:subject>
<dc:subject><![CDATA[hydroxyapatite]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2442-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2442-2</identifier>
<datestamp>2025-04-16</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pham, M. T.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Steiner, G.]]></dc:creator>
<dc:creator><![CDATA[Oswald, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2442-2</dc:identifier>
<dc:title><![CDATA[Ion beam sensitizing of titanium surfaces to hydroxyapatite formation]]></dc:title>
<dc:source><![CDATA[Surface & Coatings Technology 128-129 (2000) 313-319]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[CaO and P2O5 containing Ti surfaces were prepared and examined for their bioactivity. The preparation involved the incorporation of Ca and P into Ti by ion implantation to a total dose of up to 8 x 1017 ions/cm² with a 1.7 Ca/P ratio and a subsequent oxidation at 500 °C in O2 for 40 min. The model surfaces were examined for their reactivity toward hydroxyapatite formation by microscopically recording the mineralization in a simulated body fluid. The ion implantation modified surfaces were shown to exhibit enhanced mineralization by inducing heterogeneous nucleation, growth, and proliferation of hydroxyapatite, relative to a control sample of pure Ti. The surface induced reactivity was shown to relate to the enhanced provision of the ionic mineral components Ca2+ and HPO42- directly supplied from the surface and the substrate-mediated nucleation by hydroxylated surface TiO2.]]></dc:description>
<dc:subject><![CDATA[biomaterials]]></dc:subject>
<dc:subject><![CDATA[ion implantation]]></dc:subject>
<dc:subject><![CDATA[surface coatings]]></dc:subject>
<dc:subject><![CDATA[Ti]]></dc:subject>
<dc:subject><![CDATA[hydroxyapatite]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0257-8972(00)00593-4]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2442-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<header>
<identifier>HZDR:PUBLDB:14363-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Cramer, A.]]></dc:creator>
<dc:creator><![CDATA[Landgraf, S.]]></dc:creator>
<dc:creator><![CDATA[Beyer, E.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14363-1</dc:identifier>
<dc:title><![CDATA[Marangoni convection in molten salts - physical modelling toward lower Prandtl numbers]]></dc:title>
<dc:source><![CDATA[Experiments in Fluids 50(2011)2, 479-490]]></dc:source>
<dc:date>2011</dc:date>
<dc:description><![CDATA[Marangoni convection is involved in many technological processes. The substances of industrial interest are often governed by diffusive heat transport and their physical modelling is limited with respect to the Prandtl number Pr. The present paper addresses this deficiency. Studies were made on molten salts having Pr values in an intermediate range well below that of the typically employed organics. Since some of the selected species have a relatively high melting point, a high-temperature facility which allows studying thermocapillary convection at temperatures in excess of 1000°C was built. The results presented here were obtained in a cylindrical geometry, although the equipment that was built is not restricted to this configuration because of its modular construction. Modelled after some applications, the fluid was heated centrically on top. The bulk was embedded in a large thermostatically controlled reservoir so as to establish the lower ambient reference temperature. A characteristic size of the experimental cell was chosen such that, on the one hand, the dynamic Bond number Bo did not become too high; on the other hand, the liquid had to have a certain depth to allow particle image velocimetry. The complicated balance between body forces and thermocapillary forces in the case of intermediate Bo was found to result in a distinct local separation into a bulk motion governed by natural convection with a recirculating Marangoni flow on top. In contrast to low viscosity organics, the vapour pressure of which increases considerably with decreasing Pr, high values of the Marangoni number can be reached. Comparisons of the topology of Marangoni vortices between molten salts with 2.3 <= Pr <= 6.4 and a silicone oil with Pr typically one order of magnitude higher suggest that the regime of non-negligible heat diffusion is entered.]]></dc:description>
<dc:subject><![CDATA[Marangoni convection]]></dc:subject>
<dc:subject><![CDATA[surface tension driven flow]]></dc:subject>
<dc:subject><![CDATA[molten salts]]></dc:subject>
<dc:subject><![CDATA[Prandtl number]]></dc:subject>
<dc:subject><![CDATA[physical modelling]]></dc:subject>
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<identifier>HZDR:PUBLDB:1538-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Taut, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1538-1</dc:identifier>
<dc:title><![CDATA[Cora - a new control program for the roma detection system]]></dc:title>
<dc:source><![CDATA[1. Internationale Conference on the Chemistry and Physics of the Transactinide Elements TAN 99]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[A new computer program has been developed for the control of the GSI Rotating Wheel Multi Detector Apparatus (ROMA) running under the Windows 95 and Windows NT 4.0 operating systems. It can be fitted to a lot of detection tasks in a highly flexible way.

The ROMA apparatus [1] has been used successfully for a lot of chemical investiga-tions of transactinide elements. In preparation of our seaborgium experiment at GSI in sum-mer 1998 [2] we developed a new control program. This was necessary because the old control code was running on an ATARI computer. In case of a damage of this computer, there would not have been the possibility of a replacement, which could possibly cancel the experiment.
The new program was designed to fulfill our special experimental requirements. A second feature is its support of the usual working conditions in a long running beam time. That means, persons without a deep understanding of a computer should be able to use this program without any difficulties, even if the programmer is not available. Thirdly, it should be highly flexible in order to adapt it to new experimental demands. Finally, the program should be to a great extent independent of the experiment hardware in order to be usable for similar apparatuses.
The program is written entire-ly in the C++ language using the Borland C++ Builder 1.0 programming environment based on the object oriented Virtual Component Library.

The program has to carry out the following tasks:

· control of the ROMA wheel movements according to the actual experiment;
· enabling and disabling the nuclear spectros-copy data acquisition;
· sending information about the actual ROMA status to the data acquisition hardware;
· processing requests of the acquisition hardware (e. g. switching in "daughter mode" [3]);
· processing user input (e. g. experiment and wheel setup dialog boxes).

The program is a Microsoft Windows applicatio ...]]></dc:description>
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<identifier>HZDR:PUBLDB:1539-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Stephan, H.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Berger, R.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:creator><![CDATA[Schmidtchen, F. P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1539-1</dc:identifier>
<dc:title><![CDATA[Complexation and phase transfer of perrhenate and pertechnetate with guanidium hosts]]></dc:title>
<dc:source><![CDATA[XXIV. International Symposium on Macrocyclic Chemistry, 18-23 July 1999, Barcelona]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Noncovalent binding of pertechnetate may be of considerable interest as a new approach to labelling organic compounds with technetium without any reduction step, and for removal of pertechnetate as an environmental contaminant. Effective and selective complexation of pertechnetate should be realisable on the basis of molecular assembled supramolecular receptors that can provide multi-point fixation of tetrahedral anion pertechnetate as shown in the figure.

This paper reports on complexation experiments of pertechnetate and its nonradioactive congener perrhenate using different guanidinium compounds. The characterisation of these Tc(VII) and Re(VII) complexes are supported by X-ray crystal structures, TLC, infrared and NMR spectra. Liquid-liquid extraction studies are performed in order to monitor the influence of competition anions on phase transfer and to evaluate the stoichiometry  of the complexes extracted. Lipophilicity and ionisation properties of guanidinium hosts and their Tc(VII)/Re(VII) complexes are determined by RP-HPLC. Molecular modeling calculations are used for the interpretation of the experimental results.
]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Stephan, H.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Berger, R.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:creator><![CDATA[Schmidtchen, F. P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1539-7</dc:identifier>
<dc:title><![CDATA[Complexation and phase transfer of perrhenate and pertechnetate with guanidium hosts]]></dc:title>
<dc:source><![CDATA[XXIV. International Symposium on Macrocyclic Chemistry, 18-23 July 1999, Barcelona]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Noncovalent binding of pertechnetate may be of considerable interest as a new approach to labelling organic compounds with technetium without any reduction step, and for removal of pertechnetate as an environmental contaminant. Effective and selective complexation of pertechnetate should be realisable on the basis of molecular assembled supramolecular receptors that can provide multi-point fixation of tetrahedral anion pertechnetate as shown in the figure.

This paper reports on complexation experiments of pertechnetate and its nonradioactive congener perrhenate using different guanidinium compounds. The characterisation of these Tc(VII) and Re(VII) complexes are supported by X-ray crystal structures, TLC, infrared and NMR spectra. Liquid-liquid extraction studies are performed in order to monitor the influence of competition anions on phase transfer and to evaluate the stoichiometry  of the complexes extracted. Lipophilicity and ionisation properties of guanidinium hosts and their Tc(VII)/Re(VII) complexes are determined by RP-HPLC. Molecular modeling calculations are used for the interpretation of the experimental results.
]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Misiuk, A.]]></dc:creator>
<dc:creator><![CDATA[Kachurin, G. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2107-2</dc:identifier>
<dc:title><![CDATA[The effect of annealing under hydrostatic pressure on the visible photoluminescence from Si<SUP>+</SUP>--implanted SiO<SUB>2</SUB> films]]></dc:title>
<dc:source><![CDATA[E-MRS´98, Strasbourg, June 16-19, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2107-1</identifier>
<datestamp>2025-12-02</datestamp>
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<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Misiuk, A.]]></dc:creator>
<dc:creator><![CDATA[Kachurin, G. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2107-1</dc:identifier>
<dc:title><![CDATA[The effect of annealing under hydrostatic pressure on the visible photoluminescence from Si<SUP>+</SUP>--implanted SiO<SUB>2</SUB> films]]></dc:title>
<dc:source><![CDATA[Journal of Luminescence 80 (1999) 229-233]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1706-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Richter, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1706-1</dc:identifier>
<dc:title><![CDATA[Verifizierungsuntersuchungen zur Detektion von Rißinitiierung bei duktilem Materialverhalten unter schlagartiger Belastung]]></dc:title>
<dc:source><![CDATA[Abschlußbericht zum Forschungsaufenthalt am VTT Espoo (Finland) an die Deutsche Akademie der Naturforscher Leopoldina, Juli 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2514-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Chudoba, T.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2514-1</dc:identifier>
<dc:title><![CDATA[Verschleißschutz von Alumnium- und Magnesiumlegierungen durch Ionenimplantation]]></dc:title>
<dc:source><![CDATA[Innovative Verfahren der Oberflächenvergütung von Leichtmetallen, Essen, June 5, 1997]]></dc:source>
<dc:date>1997</dc:date>
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<identifier>HZDR:PUBLDB:2321-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kachurin, G. A.]]></dc:creator>
<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Zhuravlev, K. S.]]></dc:creator>
<dc:creator><![CDATA[Pazdnikov, N. A.]]></dc:creator>
<dc:creator><![CDATA[Volodin, V. A.]]></dc:creator>
<dc:creator><![CDATA[Gutakovsky, A. K.]]></dc:creator>
<dc:creator><![CDATA[Leier, A. F.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2321-1</dc:identifier>
<dc:title><![CDATA[Visible and near-infrared luminescence from Si nanostructures formed by ion implantation and pulse annealing]]></dc:title>
<dc:source><![CDATA[Nucl. Instr. Meth. B122 (1997) 571]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2319-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Huber, H.]]></dc:creator>
<dc:creator><![CDATA[Assmann, W.]]></dc:creator>
<dc:creator><![CDATA[Karamian, S. A.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Prusseit, W.]]></dc:creator>
<dc:creator><![CDATA[Gazis, E.]]></dc:creator>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:creator><![CDATA[Kokkoris, M.]]></dc:creator>
<dc:creator><![CDATA[Kossionidis, E.]]></dc:creator>
<dc:creator><![CDATA[Mieskes, H. D.]]></dc:creator>
<dc:creator><![CDATA[Vlastou, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2319-1</dc:identifier>
<dc:title><![CDATA[Void formation in Ge induced by high energy heavy ion irradiation]]></dc:title>
<dc:source><![CDATA[Nucl. Instr. Meth. B122 (1997) 542]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1708-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Fethke, M.]]></dc:creator>
<dc:creator><![CDATA[Ringel, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1708-1</dc:identifier>
<dc:title><![CDATA[Experimentelle Untersuchungen zur Wirksamkeit passiver Komponenten für den SWR1000]]></dc:title>
<dc:source><![CDATA[atomwirtschaft - atomtechnik 44 (1999)1, S. 35-36]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Am 29. Oktober 1998 veranstaltete die Ortssektion Sachsen der Kerntechnischen Gesellschaft e.V. an der TU Dresden ein Seminar zum Thema "Experimentelle Untersuchungen zur Wirksamkeit passiver Komponenten für den SWR1000". Diese Thematik erhielt u.a. durch das von Siemens beantragte standortunabhänige Prüfverfahren (vgl. atw 43 (1998), Nr. 10, S. 650) sowie der am 5. November in Königswinter durchgeführten KTG-Tagung "SWR1000 - ein zukunftsweisendes Reaktorkonzept" eine besondere Aktualität. In dem derzeit von der Siemens AG entwickelten innovativen Siedewasserreaktor SWR1000 werden zur Erhöhung der Sicherheit und der Wirtschaftlichkeit aktive Sicherheitssysteme weitestgehend durch passive ersetzt oder mit diesen kombiniert. Hierzu zählen die nachfolgend im Detail beschriebenen Systeme Notkondensator, Gebäudekondensator sowie Passiver Impulsgeber.

]]></dc:description>
<dc:subject><![CDATA[SWR1000]]></dc:subject>
<dc:subject><![CDATA[passive Sicherheitssysteme]]></dc:subject>
<dc:subject><![CDATA[Notkondensator]]></dc:subject>
<dc:subject><![CDATA[Gebäudekondensator]]></dc:subject>
<dc:subject><![CDATA[passiver Impulsgeber]]></dc:subject>
<dc:subject><![CDATA[Kerntechnische Gesellschaft]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1708-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Fethke, M.]]></dc:creator>
<dc:creator><![CDATA[Ringel, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1708-2</dc:identifier>
<dc:title><![CDATA[Experimentelle Untersuchungen zur Wirksamkeit passiver Komponenten für den SWR1000]]></dc:title>
<dc:source><![CDATA[Seminar "Experimentelle Untersuchungen zur Wirksamkeit passiver Komponenten für den SWR1000", TU Dresden, 29. Oktober 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Am 29. Oktober 1998 veranstaltete die Ortssektion Sachsen der Kerntechnischen Gesellschaft e.V. an der TU Dresden ein Seminar zum Thema "Experimentelle Untersuchungen zur Wirksamkeit passiver Komponenten für den SWR1000". Diese Thematik erhielt u.a. durch das von Siemens beantragte standortunabhänige Prüfverfahren (vgl. atw 43 (1998), Nr. 10, S. 650) sowie der am 5. November in Königswinter durchgeführten KTG-Tagung "SWR1000 - ein zukunftsweisendes Reaktorkonzept" eine besondere Aktualität. In dem derzeit von der Siemens AG entwickelten innovativen Siedewasserreaktor SWR1000 werden zur Erhöhung der Sicherheit und der Wirtschaftlichkeit aktive Sicherheitssysteme weitestgehend durch passive ersetzt oder mit diesen kombiniert. Hierzu zählen die nachfolgend im Detail beschriebenen Systeme Notkondensator, Gebäudekondensator sowie Passiver Impulsgeber.

]]></dc:description>
<dc:subject><![CDATA[SWR1000]]></dc:subject>
<dc:subject><![CDATA[passive Sicherheitssysteme]]></dc:subject>
<dc:subject><![CDATA[Notkondensator]]></dc:subject>
<dc:subject><![CDATA[Gebäudekondensator]]></dc:subject>
<dc:subject><![CDATA[passiver Impulsgeber]]></dc:subject>
<dc:subject><![CDATA[Kerntechnische Gesellschaft]]></dc:subject>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<header>
<identifier>HZDR:PUBLDB:1709-1</identifier>
<datestamp>2023-05-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Hicken, E. F.]]></dc:creator>
<dc:creator><![CDATA[Jaegers, H.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1709-1</dc:identifier>
<dc:title><![CDATA[Experimental and Analytical Investigation of the Operation Mode of the Emergency Condenser of the SWR1000]]></dc:title>
<dc:source><![CDATA[Nuclear Technology 126 (1999), May 1999, p. 123-142]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The Siemens AG is developing the new innovative boiling water reactor concept SWR1000. New features are the passive safety systems (e.g. emergency condensers, building condensers, passive pressure pulse transmitters, gravity-driven core flooding lines).

For the experimental investigation of the emergency condenser effectiveness, the NOKO test facility has been constructed at the Forschungszentrum Jülich in cooperation with Siemens. This test facility has an operating pressure of 10 MPa and a maximum power of 4 MW for steam production. The emergency condenser bundle consists of eight tubes and is fabricated with planned geometry and material of the SWR1000. In more than 200 experiments, the emergency condenser power was determined as a function of pressure, water level and concentration of noncondensables in the pressure vessel as well of pressure, water level and temperature in the condenser. 

Post test calculations of NOKO experiments were performed with an improved version of ATHLET. To calculate the heat transfer coefficients during condensation in horizontal tubes it was necessary to develop the module KONWAR and to implement it in ATHLET. KONWAR is based on the flow regime map of Tandon and includes several semiempirical correlations for the determination of the heat transfer coefficients. The comparison bet-ween calculations and experiments shows good agreement.
]]></dc:description>
<dc:subject><![CDATA[SWR1000]]></dc:subject>
<dc:subject><![CDATA[emergency condenser]]></dc:subject>
<dc:subject><![CDATA[ATHLET]]></dc:subject>
<dc:subject><![CDATA[KONWAR]]></dc:subject>
<dc:subject><![CDATA[condensation inside horizontal and slightly inclinde tubes]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:244-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-244-1</dc:identifier>
<dc:title><![CDATA[Control of the Cylinder Wake Instabilities by an External Magnetic Field]]></dc:title>
<dc:source><![CDATA[and Proceedings: 1994 Meetingof the Division of Fluid Dynamics (APS/DFD), Atlanta, 20-22 November 1994, Bulletin of the American Physical Society, Series II, 39 (1994) 9, p. 1979]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The standard cylinder wake is considered for the magnetohydrodynamic (MHD) case: The fluid is electrically conducting and exposed to an external uniform magnetic field of different directions. In general, the magnetic field stabilizes the flow, the vortex street can be suppressed for each Re. A numerical simulation of the time-dependent flow as well as a simple analytical stability analysis will be presented and compared with available and own experiments. The experimentally found tendency of an increasing level of low-frequency perturbations for an increasing magnetic field will be discussed and compared with the analytical stability analysis. Typical features of the MHD case will be presented: Drag increase, up- and downstream wakes, surface pressure redistribution, recirculation bubbles at high Re, etc.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:105-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Zippe, W.]]></dc:creator>
<dc:creator><![CDATA[Baldauf, D.]]></dc:creator>
<dc:creator><![CDATA[Szabados, L.]]></dc:creator>
<dc:creator><![CDATA[Ézsöl, G.]]></dc:creator>
<dc:creator><![CDATA[Baranyai, G.]]></dc:creator>
<dc:creator><![CDATA[Nagy, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-105-2</dc:identifier>
<dc:title><![CDATA[Two-phase flow behaviour during a medium size cold leg test on PMK-II (SPE-4)]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik 1994, 17.-19. Mai 1994, Stuttgart, Tagungsbericht, ISSN 0720-9207, S. 77-80]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The Hungarian integral test rig PMK of the KFKI Atomic Energy Research Institute was used as a source of experimental data for the IAEA Standard Problem Exercise SPE-4, a Medium size cold leg Loca with a secondary Bleed-and-feed procedure. The needle shaped conductivity probes developed by the Research Center Rossendorf have been applied in order to obtain information about the void fraction and the structure of the two-phase flow. The primary circuit of the PMK-II test facility was practically fully equipped with probes (with exception of the core simulator and the downcomer). An overview of the signals of all probes and the general chronology of characteristic events are discussed. As a main result the mechanism of the hot leg loop-seal clearing was clarified in detail.]]></dc:description>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:105-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Zippe, W.]]></dc:creator>
<dc:creator><![CDATA[Baldauf, D.]]></dc:creator>
<dc:creator><![CDATA[Szabados, L.]]></dc:creator>
<dc:creator><![CDATA[Ézsöl, G.]]></dc:creator>
<dc:creator><![CDATA[Baranyai, G.]]></dc:creator>
<dc:creator><![CDATA[Nagy, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-105-1</dc:identifier>
<dc:title><![CDATA[Two-phase flow behaviour during a medium size cold leg test on PMK-II (SPE-4)]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik 1994, Stuttgart, 17.-19.5.1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The Hungarian integral test rig PMK of the KFKI Atomic Energy Research Institute was used as a source of experimental data for the IAEA Standard Problem Exercise SPE-4, a Medium size cold leg Loca with a secondary Bleed-and-feed procedure. The needle shaped conductivity probes developed by the Research Center Rossendorf have been applied in order to obtain information about the void fraction and the structure of the two-phase flow. The primary circuit of the PMK-II test facility was practically fully equipped with probes (with exception of the core simulator and the downcomer). An overview of the signals of all probes and the general chronology of characteristic events are discussed. As a main result the mechanism of the hot leg loop-seal clearing was clarified in detail.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
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<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-105-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:144-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Hensel, F.]]></dc:creator>
<dc:creator><![CDATA[Schütz, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-144-1</dc:identifier>
<dc:title><![CDATA[Messung der Volumenströme von Gas und Flüssigkeit in einer Zweikomponentenströmung mit Ultraschall und Mustererkennung]]></dc:title>
<dc:source><![CDATA[ACHEMA '94, Internationales Treffen für Chemische Technik und Biotechnologie, Frankfurt am Main, 5.-11.06.1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The state-of art of ultrasonic two-phase flow measurements is characterised by a number of different approaches commonly based on the identification and characterisation of individual voids (bubbles, plugs etc.) applying the techniques of ultrasonic testing. The recorded individual events are integrated to extract parameters as void fraction or volume flow rates. The main limitation of these methods arises from the complicated structure of two-phase flow at higher void fractions which leads to multiple diffractions of the sound beam. The measurement is therefore limited to low void fractions or an easy flow structure.
The main idea of the present work was to overcome these limitations by means of pattern recognition. An ultrasonic beam crossing the two-phase flow is modulated by the changing structure of the voids passing by and therefore the through-transmission signal must contain information about the parameters of the two-phase flow even if  information about individual flow effects cannot be derived. Therefore it was supposed that a pattern recognition algorithm trained with signals obtained at known conditions is able to identify the set of the flow parameters (flow rates, void fraction etc.) in an unknown situation.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-144-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:3184-1</identifier>
<datestamp>2025-12-09</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Pécz, B.]]></dc:creator>
<dc:creator><![CDATA[Dobos, L.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3184-1</dc:identifier>
<dc:title><![CDATA[Ion beam synthesis of graphite and diamond in silicon carbide]]></dc:title>
<dc:source><![CDATA[Applied Physics Letters Vol. 76, Nr. 20, 15 May 2000, 2847-2849]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[A high dose of 1x1018 cm-2,  60 keV carbon ions was implanted into single crystalline 6H silicon carbide (SiC) at elevated temperatures. The formation of  carbon phases in the crystalline SiC lattice was investigated by cross sectional transmission electron microscopy. An amorphous, carbon rich phase was produced at 300oC. Precipitates of graphite were obtained at 600oC, whereas at 900oC small diamond grains were produced. These grains are in perfect epitaxial relation with the surrounding SiC lattice. ]]></dc:description>
<dc:subject><![CDATA[Ion implantation]]></dc:subject>
<dc:subject><![CDATA[Ion beam synthesis]]></dc:subject>
<dc:subject><![CDATA[carbon]]></dc:subject>
<dc:subject><![CDATA[silicon carbide]]></dc:subject>
<dc:subject><![CDATA[diamond]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1063/1.126493]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-3184-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:163-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Priede, J.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Thess, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-163-1</dc:identifier>
<dc:title><![CDATA[Thermocapillary Instabilities in Liquid Metals: Hartmann Number Versus Prandtl-Number]]></dc:title>
<dc:source><![CDATA[Magnetohydrodynamics, Proc. Energy Transfer in MHD Flows, Conference, Aussois, France, Sept. 1994, pp. 571 - 580]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The technical need for instability postponement, turbulence suppression and flow control in material processing as well as the seek for low-cost alternatives to space-technologies for crystal growth are currently leading to an increased interest in the interaction between thermocapillary flows in electrically conducting fluids and magnetic fields. While the interplay between isothermal flows and magnetic fields is well understood, our physical understanding of the influence of magnetic fields on thermocapillary flow phenomena, i.e. flows driven by surface tension gradients, leaves still much to be desired.
The goal of the püresent communication is to demonstrate that a magnetic field acting on the thermocapillary flow of a low Prandtl number fluid causes the fluid to behave like a high Prandtl number fluid. This important feature is exemplified by considering the linear stability of a unidirectional thermocapillary flow set up by a temperature gradient parallel to the free surface of an unbounded planar fluid layer. The magnetic field is supposed to be normal to the free surface. Our problem is the magnetic counterpart to the work of Smith & Davis. We report results of a comprehensive study of the critical Marangoni number for the onset of hydrothermal waves as a function of the Hartmann number and of the Prandtl number. For weak magnetic field the instability mechanism in liquid metals is found to be the same as in the nonmagnetic case for low Prandtl numbers. For sufficiently strong magnetic field the basic flow and the most unstable perturbation are confined to a thin Hartmann boundary layer below the free surface which leads to a decrease of the effective viscous diffusion time-scale as Ha-2. Our Computations reveal that at a certain value of the Hartmann number, when the effective viscous time equals the thermal diffusion time, the character of the instability changes discontinously. The new type of instability is reminiscent of the instability mechanism w ...]]></dc:description>
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<identifier>HZDR:PUBLDB:163-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Priede, J.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Thess, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-163-2</dc:identifier>
<dc:title><![CDATA[Thermocapillary Instabilities in Liquid Metals: Hartmann Number Versus Prandtl-Number]]></dc:title>
<dc:source><![CDATA["Energy Transfer in MHD Flows", Sept. 1994, Aussois, Frankreich, pp. 571 - 580]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The technical need for instability postponement, turbulence suppression and flow control in material processing as well as the seek for low-cost alternatives to space-technologies for crystal growth are currently leading to an increased interest in the interaction between thermocapillary flows in electrically conducting fluids and magnetic fields. While the interplay between isothermal flows and magnetic fields is well understood, our physical understanding of the influence of magnetic fields on thermocapillary flow phenomena, i.e. flows driven by surface tension gradients, leaves still much to be desired.
The goal of the püresent communication is to demonstrate that a magnetic field acting on the thermocapillary flow of a low Prandtl number fluid causes the fluid to behave like a high Prandtl number fluid. This important feature is exemplified by considering the linear stability of a unidirectional thermocapillary flow set up by a temperature gradient parallel to the free surface of an unbounded planar fluid layer. The magnetic field is supposed to be normal to the free surface. Our problem is the magnetic counterpart to the work of Smith & Davis. We report results of a comprehensive study of the critical Marangoni number for the onset of hydrothermal waves as a function of the Hartmann number and of the Prandtl number. For weak magnetic field the instability mechanism in liquid metals is found to be the same as in the nonmagnetic case for low Prandtl numbers. For sufficiently strong magnetic field the basic flow and the most unstable perturbation are confined to a thin Hartmann boundary layer below the free surface which leads to a decrease of the effective viscous diffusion time-scale as Ha-2. Our Computations reveal that at a certain value of the Hartmann number, when the effective viscous time equals the thermal diffusion time, the character of the instability changes discontinously. The new type of instability is reminiscent of the instability mechanism w ...]]></dc:description>
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<dc:creator><![CDATA[Priede, J.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Thess, A.]]></dc:creator>
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<dc:title><![CDATA[Thermocapillary Instabilities in Liquid Metals: Hartmann Number Versus Prandtl-Number]]></dc:title>
<dc:source><![CDATA["Energy Transfer in MHD Flows", Sept. 1994, Aussois, Frankreich, pp. 571 - 580]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The technical need for instability postponement, turbulence suppression and flow control in material processing as well as the seek for low-cost alternatives to space-technologies for crystal growth are currently leading to an increased interest in the interaction between thermocapillary flows in electrically conducting fluids and magnetic fields. While the interplay between isothermal flows and magnetic fields is well understood, our physical understanding of the influence of magnetic fields on thermocapillary flow phenomena, i.e. flows driven by surface tension gradients, leaves still much to be desired.
The goal of the püresent communication is to demonstrate that a magnetic field acting on the thermocapillary flow of a low Prandtl number fluid causes the fluid to behave like a high Prandtl number fluid. This important feature is exemplified by considering the linear stability of a unidirectional thermocapillary flow set up by a temperature gradient parallel to the free surface of an unbounded planar fluid layer. The magnetic field is supposed to be normal to the free surface. Our problem is the magnetic counterpart to the work of Smith & Davis. We report results of a comprehensive study of the critical Marangoni number for the onset of hydrothermal waves as a function of the Hartmann number and of the Prandtl number. For weak magnetic field the instability mechanism in liquid metals is found to be the same as in the nonmagnetic case for low Prandtl numbers. For sufficiently strong magnetic field the basic flow and the most unstable perturbation are confined to a thin Hartmann boundary layer below the free surface which leads to a decrease of the effective viscous diffusion time-scale as Ha-2. Our Computations reveal that at a certain value of the Hartmann number, when the effective viscous time equals the thermal diffusion time, the character of the instability changes discontinously. The new type of instability is reminiscent of the instability mechanism w ...]]></dc:description>
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<identifier>HZDR:PUBLDB:1844-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Richter, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1844-1</dc:identifier>
<dc:title><![CDATA[Bewertung von akustischen Emissionssignalen, aufgenommen mit einer hammerfinnenintegrierten AE-Sonde]]></dc:title>
<dc:source><![CDATA[Arbeitskreis "Instrumentierter Kerbschlagbiegeversuch" des DVM Berlin, 19. September 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Anhand von Beispielen wurden elastische low blow's und deren komplexes akustisches Verhalten an einer ungekerbten hochfesten Stahlprobe unter Ausschluß von plastischer  Deformation und Rißbildung diskutiert. Störsignale, die durch verschiedene Prozesse generiert werden, sollen somit besser verstanden und letztlich von Nutzsignal separiert  werden. Die Korrelation der gemessenen Störsignale zu charakteristischen Ereignissen, wie Reibungsquellen und mechanischer Kontakt, gelang noch nicht. Deshalb wird eine zusätzliche AE-Instrumentierung von Probe und Widerlager in Betrach gezogen,  die bei der Störquelleninterpretation hilfreich sein wird.
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:189-1</identifier>
<datestamp>2019-03-04</datestamp>
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</header>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Richter, H.]]></dc:creator>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Winkler, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-189-1</dc:identifier>
<dc:title><![CDATA[Ermittlung dynamischer Rißeinleitungszähigkeiten mit dem instrumentierten Kerbschlagbiegeversuch bei elastisch-plastischem Werkstoffverhalten]]></dc:title>
<dc:source><![CDATA[Tagungsband der 26. Vortragsveranstaltung des DVM-AK "Bruchvorgänge", Magdeburg, 22. - 23. Februar 1994, S. 373 - 383]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Rißwiderstandskurven sind zum unentbehrlichen Instrumentarium zur Beschreibung des Versagens rißbehafteter Komponenten bei elastisch-plastischem Werkstoffverhalten geworden. Die Abhängigkeit der R-Kurve von der Dicke der jeweiligen Proben gestattet aber nur bedingt die Übertragung der Versuchsergebnisse auf das Bauteilverhalten. In der Literatur wird gezeigt, daß der Beginn der stabilen Rißeinleitung einen echten, geometrieunabhängigen Werkstoffkennwert darstellt. Als anerkannte Methode zur Bestimmung kritischer Rißeinleitungsparameter wird die Messung der Stretchzonenbreite vor der Rißspitze (SZW) verwendet. In quasistatischen Einproben (EPT)- oder in Mehrprobentechniken (MPT) lassen sich mit Hilfe von kritschen SZW gültige Rißeinleitungszähigkeiten auf J-Integralbasis bestimmen.
Noch ungelöst ist das Problem der Ermittlung von dynamischen Rißeinleitungszähigkeiten in EPT mit Hilfe des instrumentierten Kerbschlagbiegeversuches. Hierfür muß durch Messung physikalischer Größen, die mit dem Rißeinleitungsprozeß in Verbindung stehen, der Zeitpunkt der Rißeinleitung detektiert werden. Derartige physikalische Detektionsverfahren sind beispielsweise akustische Emission, elektrische und magnetische Emission. Man erkennt, daß alle drei Verfahren nur indirekt auf Rißbildungsprozesse reagieren. Erste Experimente mit einer Instrumentierung des Kerbschlagbiegeversuchs werden vorgestellt, wobei neben der Schlagkraft gleichzeitig akustische, magnetische und elektrische Emission erfaßt werden.
Durch die simultane Erfassung der Signale verschiedener Methoden in Zusammenhang mit hochauflösender Meßtechnik und mathematisch-numerischen Verfahren der Signalauswertung kann erwartet werden, daß die charakteristischen Zeitpunkte für Rißeinleitung und stabilen Rißfortschritt zuverlässig detektiert werden können.]]></dc:description>
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<identifier>HZDR:PUBLDB:142-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-142-1</dc:identifier>
<dc:title><![CDATA[Erfahrungen und Ergebnisse des 1000-Dächer-Photovoltaik-Programms in Sachsen]]></dc:title>
<dc:source><![CDATA[9. Nationales Symposium Photovoltaische Solarenergie, Staffelstein, 16.-18.3.1994, Tagungsband S. 149]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Die Ergebnisse aus dem einjährigen Betrieb von  43 netzgekoppelten PV-Anlagen in Sachsen werden dargestellt. Schwerpunkte bilden die architektonische Einbindung der Generatoren in die Gebäude, die mögliche Synchronisation zwischen solarer Stromerzeugung und dem Verbrauch von Elektroenergie sowie Erfahrungen bei der Installation und dem Betrieb von netzgekoppelten PV-Anlagen.
Hervorhebenswert sind die Ergebnisse zum möglichen Eigenverbrauch des solar erzeugten Stromes. Es konnte gezeigt werden, daß gerade energiesparende Haushalte stark auf die "Zwischenspeicherung" im öffentlichen Netz angewiesen sind (Eigenverbrauch 20 %). Maximal wird ein Eigenverbrauch von ca. 50 % erreicht.
Die erreichten jährlichen Energieerträge betragen im Mittel 680 kWh/kWp, wobei große Unterschiede zwischen den einzelnen Anlagen gefunden wurden. Als Hauptursache für die unterschiedlichen energetischen Ergebnisse werden Abweichungen der Modulparameter von den Datenblattangaben der Hersteller vermutet.]]></dc:description>
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<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-142-7</dc:identifier>
<dc:title><![CDATA[Erfahrungen und Ergebnisse des 1000-Dächer-Photovoltaik-Programms in Sachsen]]></dc:title>
<dc:source><![CDATA[9. Nationales Symposium Photovoltaische Solarenergie, Staffelstein, 16.-18.3.1994, Tagungsband S. 149]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Die Ergebnisse aus dem einjährigen Betrieb von  43 netzgekoppelten PV-Anlagen in Sachsen werden dargestellt. Schwerpunkte bilden die architektonische Einbindung der Generatoren in die Gebäude, die mögliche Synchronisation zwischen solarer Stromerzeugung und dem Verbrauch von Elektroenergie sowie Erfahrungen bei der Installation und dem Betrieb von netzgekoppelten PV-Anlagen.
Hervorhebenswert sind die Ergebnisse zum möglichen Eigenverbrauch des solar erzeugten Stromes. Es konnte gezeigt werden, daß gerade energiesparende Haushalte stark auf die "Zwischenspeicherung" im öffentlichen Netz angewiesen sind (Eigenverbrauch 20 %). Maximal wird ein Eigenverbrauch von ca. 50 % erreicht.
Die erreichten jährlichen Energieerträge betragen im Mittel 680 kWh/kWp, wobei große Unterschiede zwischen den einzelnen Anlagen gefunden wurden. Als Hauptursache für die unterschiedlichen energetischen Ergebnisse werden Abweichungen der Modulparameter von den Datenblattangaben der Hersteller vermutet.]]></dc:description>
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<identifier>HZDR:PUBLDB:356-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Brünig, D.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-356-1</dc:identifier>
<dc:title><![CDATA[Betriebserfahrungen mit einer 100-m2-Solaranlage zur Trinkwasserbereitung und Fernwärmeeinspeisung]]></dc:title>
<dc:source><![CDATA[5. Symposium Thermische Solarenergie, Staffelstein, 21.-26. Juni 1995, Tagungsband S.133]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Die Ergebnisse des ersten zehn Betriebsmonate der Solaranlage Freital werden vorgestellt. Bei einem Kollektornutzungsgrad von 29% wurde ein Ertrag von 264 kWh/m² erreicht. Für das erste volle Betriebsjahr wird ein Wert von 327 kWh/m² erwartet. Mehr als 2/3 der erzeugten Solarwärme wurde in das Fernwärmenetz eingespeist, der Rest diente der Warmwasserbereitung einer Schule.]]></dc:description>
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<dc:creator><![CDATA[Brünig, D.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
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<dc:title><![CDATA[Betriebserfahrungen mit einer 100-m2-Solaranlage zur Trinkwasserbereitung und Fernwärmeeinspeisung]]></dc:title>
<dc:source><![CDATA[5. Symposium Thermische Solarenergie, Staffelstein, 21.-26. Juni 1995, Tagungsband S.133]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Die Ergebnisse des ersten zehn Betriebsmonate der Solaranlage Freital werden vorgestellt. Bei einem Kollektornutzungsgrad von 29% wurde ein Ertrag von 264 kWh/m² erreicht. Für das erste volle Betriebsjahr wird ein Wert von 327 kWh/m² erwartet. Mehr als 2/3 der erzeugten Solarwärme wurde in das Fernwärmenetz eingespeist, der Rest diente der Warmwasserbereitung einer Schule.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:3092-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3092-1</dc:identifier>
<dc:title><![CDATA[[Au(Et2dtc)2][TcNCl4] - Synthesis and Structure]]></dc:title>
<dc:source><![CDATA[Anorganische allg. Chemie]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[ [Au(Et2dtc)2][TcNCl4] (Et2dtc- = N,N-diethyldithiocarbamate) is formed by the reaction of [Au(CO)Cl] with [TcN(Et2dtc)2] in dichloromethane.  The solid state structure of the compound is characterized by a large triclinic unit cell (a = 9.422(2), b = 22.594(5), c = 32.153(7) Å, a = 72.64(1), b = 85.19(1), g = 86.15(1)°,  Z = 12)  and shows an unusual arrangement due to long-range interactions between the technetium atoms and sulfur atoms of the [Au(Et2dtc)2]+ units (3.45 - 3.56 Å ) which assemble two anions and one cation to {[TcNCl4][Au(Et2dtc)2][TcNCl4]}- moieties. 






]]></dc:description>
<dc:subject><![CDATA[Technetium complexes]]></dc:subject>
<dc:subject><![CDATA[Gold complexes]]></dc:subject>
<dc:subject><![CDATA[Nitrido compounds]]></dc:subject>
<dc:subject><![CDATA[X-ray structure]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1948-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Seifert, S.]]></dc:creator>
<dc:creator><![CDATA[Syhre, R.]]></dc:creator>
<dc:creator><![CDATA[Gupta, A.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1948-1</dc:identifier>
<dc:title><![CDATA[Stability studies on "3+1" mixed-ligand technetium and rhenium complexes]]></dc:title>
<dc:source><![CDATA[Technetium, Rhenium and Other Metals in Chemistry and Nuclear Medicine
(Edited by Nicolini M., Mazzi U.) SGE Editoriali Padova (1999) pp 687-690]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The stability and reactivity of "3+1" <SUP>99m</SUP>Tc mixed-ligand complexes were investigated in vitro and in vivo in the blood of rats. Surprisingly, in whole blood the complexes, which proved to be stable in saline, PBS of pH 7.4 and mostly in plasma, were converted into more hydrophilic metabolites. Small structural differences in the complex molecule have a profound influence on the rate of metabolism of the complexes. Transchelation reactions with glutathione (GSH) were hypothesized and this hypothesis substantiated by challenge experiments. Structural parameters influencing the stability of the complexes and consequences for the radiopharmaceutical design are discussed.  ]]></dc:description>
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<identifier>HZDR:PUBLDB:1949-1</identifier>
<datestamp>2023-05-05</datestamp>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Pavlenko, O. P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1949-1</dc:identifier>
<dc:title><![CDATA[The Ter-Mikaelian and Landau-Pomeranchuk effects for induced soft gluon radiation in a QCD medium]]></dc:title>
<dc:source><![CDATA[Physics Letters B 477 (2000) 171-177 web: hep-ph]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The polarization of a surrounding QCD medium 
modifies the induced gluon radiation spectrum
of a high-energy parton at small transverse momenta
for a single interaction and for multiple scatterings as well.
This effect is an analogue of the Ter-Mikaelian effect in QED,
superimposed to the Landau--Pomeranchuk effect,
however it appears in QCD in a different phase space region.]]></dc:description>
<dc:subject><![CDATA[Landau-Pomeranchuk effect]]></dc:subject>
<dc:subject><![CDATA[gluon radiation]]></dc:subject>
<dc:subject><![CDATA[Ter-Mikaelian effect]]></dc:subject>
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<identifier>HZDR:PUBLDB:1950-1</identifier>
<datestamp>2023-05-10</datestamp>
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<dc:creator><![CDATA[Peshier, A.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Soff, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1950-1</dc:identifier>
<dc:title><![CDATA[Equation of State of Deconfined Matter at Finite Chemical Potential in a Quasiparticle Description]]></dc:title>
<dc:source><![CDATA[Physical Review C, Volume 61 (2000) 045203]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[An effective quasiparticle description of the thermodynamics  of deconfined matter, compatible with both finite-temperature  lattice data and the perturbative limit, is generalized to  finite chemical potential.
 Within this approach, the available 4-flavor lattice equation of  state is extended to finite baryon density, and implications for  cold, charge-neutral deconfined matter in β-equilibrium  in compact stars are considered.]]></dc:description>
<dc:subject><![CDATA[deconfined matter]]></dc:subject>
<dc:subject><![CDATA[equation of state]]></dc:subject>
<dc:subject><![CDATA[QCD]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevC.61.045203]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1950-1</dc:relation>
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<header>
<identifier>HZDR:PUBLDB:1712-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Aszodi, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1712-1</dc:identifier>
<dc:title><![CDATA[Simulation der transienten Naturkonvektion in einem seitlich beheizten Behälter]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik '96, Mannheim, 21. - 23. Mai 1996, Tagungsbericht S. 106 - 109]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1713-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bergner, F.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, U.]]></dc:creator>
<dc:creator><![CDATA[Fleischer, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1713-1</dc:identifier>
<dc:title><![CDATA[Das Konzept des Ultraschall-Laufzeit-Prozeßablauf-Bildes]]></dc:title>
<dc:source><![CDATA[Seminar für zerstörungsfreie Materialcharakterisierung, Jena, Oktober 1996, Berichtsband 54, DGZfP, S. 253 - 258]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1713-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Bergner, F.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, U.]]></dc:creator>
<dc:creator><![CDATA[Fleischer, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1713-7</dc:identifier>
<dc:title><![CDATA[Das Konzept des Ultraschall-Laufzeit-Prozeßablauf-Bildes]]></dc:title>
<dc:source><![CDATA[Seminar für zerstörungsfreie Materialcharakterisierung, Jena, Oktober 1996, Berichtsband 54, DGZfP, S. 253 - 258]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1717-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bojarevics, A.]]></dc:creator>
<dc:creator><![CDATA[Gelfgat, Y.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Simanowskis, S.]]></dc:creator>
<dc:creator><![CDATA[Mankis, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1717-1</dc:identifier>
<dc:title><![CDATA[Procedure and method of MHD phenomena investigation on juvenile surfaces of liquid metal]]></dc:title>
<dc:source><![CDATA[8th Beer-Sheva Int. Seminar on MHD flows and turbulence, Jerusalem, February 1996, to appear in: Progress in Astronautics and Aeronautics, Ed.: Branover, H.; Unger, Y.; Washington]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1721-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ferse, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1721-1</dc:identifier>
<dc:title><![CDATA[A Computer System for Evaluation of Contamined Sites]]></dc:title>
<dc:source><![CDATA[NATO ASI Series: Environment - Vol. 8, Kluver Academie Publishers, 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
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<identifier>HZDR:PUBLDB:1722-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ferse, W.]]></dc:creator>
<dc:creator><![CDATA[Reitz, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1722-1</dc:identifier>
<dc:title><![CDATA[A Risk Evaluation System for Contamined Sites]]></dc:title>
<dc:source><![CDATA[Proc. of the FOURTH INTERNATIONAL WORKSHOP on real-time computing of the environmental consequence of an accident release from a nuclear installation, Aronsborg, Sweden, Oct. 7 - 11, 1996, Paper N ...]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1723-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Galindo, V.]]></dc:creator>
<dc:creator><![CDATA[Teuner, M.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Langbein, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1723-1</dc:identifier>
<dc:title><![CDATA[Drop tower experiments on the thermocapillary drop migration]]></dc:title>
<dc:source><![CDATA[Proceedings Drop Tower Days, Bremen, July 8 - 11, 1996, pp. 2 - 10]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1724-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:title><![CDATA[Influence of the Irradiation Temperature on the Formation of Defects in Reactor Pressure Vessel Steels]]></dc:title>
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<dc:title><![CDATA[Anwendungsmöglichkeiten neuronaler Netze zur Früherkennung in Chemieanlagen]]></dc:title>
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<dc:description><![CDATA[The preliminary results of the activation measurements and calculations in the different points of the irradiation facility KORPUS are shortly described and analyzed. The tasks  of these investigations are the dosimetry characterization of the facility and creation of the international dosimetry benchmark.]]></dc:description>
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<dc:title><![CDATA[Experiences with the parallel version of MCNP-4A on a SUN workstation network and on the CONVEX SPP-1000system]]></dc:title>
<dc:source><![CDATA[Proc. of the International Conference on Computation Modelling and Computing in Physics, Dubna, Russia, Sept. 16 - 21, 1996, p. 52]]></dc:source>
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<dc:source><![CDATA[Proc. of the International Conference on Computation Modelling and Computing in Physics, Dubna, Russia, Sept. 16 - 21, 1996, p. 52]]></dc:source>
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<dc:title><![CDATA[On the role of thermal boundary conditions in the instability of thermocapillary driven low-Prandtl-number convection]]></dc:title>
<dc:source><![CDATA[Proc. of the Second European Symposium Fluids in Space, Neapel, April 22 - 26, 1996, pp. 508 - 511]]></dc:source>
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<dc:title><![CDATA[Sichere Bewertung des Materialzustandes in Altanlagen durch Probenkonstitution]]></dc:title>
<dc:source><![CDATA[INNOMATA 1996, 2. Ausstellungstagung für Materialtechnologie und Werkstoffanwendung, Dresden, Mai 1996, Comp. S. 323]]></dc:source>
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<dc:title><![CDATA[Sichere Bewertung des Materialzustandes in Altanlagen durch Probenkonstitution]]></dc:title>
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
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<dc:title><![CDATA[Ein FE-Schwingungsmodell zur Unterstützung der Diagnose von Reaktoren des Typs WWER]]></dc:title>
<dc:source><![CDATA[IV. Kolloquium "Technische Diagnostik", Dresden, 15. März 1996]]></dc:source>
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<dc:title><![CDATA[A novel experimental technique to study different phenomena at a free liquid metal surface]]></dc:title>
<dc:source><![CDATA[The 125th TMS meeting, Experimental methods in Microgravity, Anaheim (USA), February 4 - 8, 1996]]></dc:source>
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<dc:creator><![CDATA[Bojarevics, A.]]></dc:creator>
<dc:creator><![CDATA[Gelfgat, Y.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Cramer, A.]]></dc:creator>
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<dc:title><![CDATA[Second Experimental studies on diefferent phenomena at freee metal surface]]></dc:title>
<dc:source><![CDATA[European Symposium Fluids in Space, Neapel, April 22 - 26, 1996]]></dc:source>
<dc:date>1996</dc:date>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Ferse, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1746-1</dc:identifier>
<dc:title><![CDATA[Die Struktur des wissensbasierten Systems XUMA-GEFA]]></dc:title>
<dc:source><![CDATA[Seminar der Anwenderländer des Baden-Württemberger Altlastenbewertungssystems, Bad Schandau, August 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Ferse, W.]]></dc:creator>
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<dc:title><![CDATA[Die Anwendung der Entscheidungsanalyse zur Unterstützung öffentlicher Entscheidungen]]></dc:title>
<dc:source><![CDATA[KOVERS-Seminar, ETH Zürich, 28. November 1996]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Galindo, V.]]></dc:creator>
<dc:creator><![CDATA[Teuner, M.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1748-1</dc:identifier>
<dc:title><![CDATA[Experiments on thermocapillary migration of drops in a drop tower]]></dc:title>
<dc:source><![CDATA[Escuela de Fisico-Quimica de Fluidos: Drops, bubbles and film, Santander, September 9 - 13, 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kruber, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1751-1</dc:identifier>
<dc:title><![CDATA[Die Praxis-Anwendung der Entscheidungsanalyse für die Bewertung und Auswahl optimaler Sanierungskonzepte]]></dc:title>
<dc:source><![CDATA[KOVERS-Seminar, ETH Zürich, 28. September 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1752-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Langenbuch, S.]]></dc:creator>
<dc:creator><![CDATA[Lizorkin, M.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:creator><![CDATA[Velkov, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1752-1</dc:identifier>
<dc:title><![CDATA[3D Neutronic Codes coupled with Thermal-hydraulic System Codes for PWR, BWR and VVER reactors]]></dc:title>
<dc:source><![CDATA[OECD/CSNI Workshop on Transient Themal-Hydraulics and Neutronic codes Requirements, Annapolis, Md (USA), November 5 - 8, 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1753-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Meyer, K.]]></dc:creator>
<dc:creator><![CDATA[Hollstein, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1753-1</dc:identifier>
<dc:title><![CDATA[Analytical Model to Calculate the Transfer Functions of Neutron Noise coused by Random Pendulum Motions of a VVER-440 Control Element]]></dc:title>
<dc:source><![CDATA[IMORN-26, Piestany, May 27 - 29, 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2866-1</identifier>
<datestamp>2025-12-04</datestamp>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Fitz, C.]]></dc:creator>
<dc:creator><![CDATA[Kolitsch, A.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2866-1</dc:identifier>
<dc:title><![CDATA[In situ measurement of stress during deposition of boron nitride films]]></dc:title>
<dc:source><![CDATA[Material Science Forum, Proceedings of the 5th European Conference on Residual Stress, 28-30 September 1999, Noorwijkerhout, The Netherlands, Vol. 347-349 (2000) pp. 156-160]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[A two-beam laser deflection system has been setup for real-time measurement of the stress in thin films during processing. The curvature of a Si-cantilever, laser reflectivity and real time spectroscopic ellipsometry data are recorded simultaneously. Reliable real time film thickness data are essential for the calculation of the instantaneous stress from the bending force per unit width measured. Instantaneous stress data with a depth resolution in the nanometer range provide detailed information on growth processes. It is demonstrated that force per unit width or global stress data, as calculated by applying the simple form of Stoney's equation, are not appropriate for the analysis of the stress in layered structures like boron nitride films.
The depth distribution of the instantaneous stress in boron nitride films recorded during growth by ion beam assisted deposition has been analyzed. The layer sequence of interfacial turbostratic BN layer / mixed (t-BN+c-BN) transition layer / cubic BN can be clearly identified in the instantaneous stress data. The instantaneous stress has been found to depend sensitively upon fluctuations in the boron deposition rate which in turn cause variations in the ion/atom arrival ratio. Real time global stress data recorded during ion implantation into c-BN films have revealed for the first time two mechanisms being involved.
]]></dc:description>
<dc:subject><![CDATA[instantaneous stress]]></dc:subject>
<dc:subject><![CDATA[laser deflection]]></dc:subject>
<dc:subject><![CDATA[ellipsometry]]></dc:subject>
<dc:subject><![CDATA[boron nitride]]></dc:subject>
<dc:subject><![CDATA[ion implantation]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:14288-1</identifier>
<datestamp>2025-06-05</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Höhne, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14288-1</dc:identifier>
<dc:title><![CDATA[Extention of the AIAD model - The free surface drag model]]></dc:title>
<dc:source><![CDATA[CFD-network meeting, 21.-22.07.2010, Jülich, Deutschland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Problem: Different models necessary for dispersed particles and separated continuous phases (interfacial drag etc.)]]></dc:description>
<dc:subject><![CDATA[AIAD]]></dc:subject>
<dc:subject><![CDATA[CFX]]></dc:subject>
<dc:subject><![CDATA[CFD]]></dc:subject>
<dc:subject><![CDATA[horizontal flow]]></dc:subject>
<dc:subject><![CDATA[surface drag]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:1755-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Polte, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1755-1</dc:identifier>
<dc:title><![CDATA[Diskusion eines Kriteriensystems zur Bewertung der Ansiedlung von Industrie in urbanen Gebieten]]></dc:title>
<dc:source><![CDATA[KOVERS-Seminar, ETH Zürich, 28. November 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1756-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1756-1</dc:identifier>
<dc:title><![CDATA[BLDN - Modell zur Berechnung der axialen Dampfgehaltsverteilung bei der Druckentlastung]]></dc:title>
<dc:source><![CDATA[42. Sitzung des DECHEMA/GVC-Arbeitsausschusses "Sicherheitsgerechtes Auslegen von Chemieapparaten", Rossendorf, 15. - 16.10. 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Das Programm BLDN (BLow-DowN) basiert auf einem eindimensionalen Strömungsmodell zur Beschreibung der axialen Dampfgehaltsverteilung in einem stehenden zylindrischen Druckbehälter bei einem Abblasevorgang unter Beschränkung auf eine Komponente. Zur Beschreibung der axialen Dampfgehaltsverteilung werden für Dampf und Flüssigkeit die gemeinsamen Massen- und Energieerhaltungsgleichungen gelöst. Es wird von thermodynamischem Gleichgewicht ausgegangen. Die zum Abschluß des Systems notwendige Phasendriftbeziehung wird in Form einer Phasendifferenzgeschwindigkeit als Funktion vom Dampfgehalt und den Stoffwerten verwendet. Mit Hilfe dieser Beziehung werden die Geschwindigkeiten beider Phasen gekoppelt. Der Impuls des Strömungsmediums wird vernachlässigt. Die Impulsgleichungen bleiben deshalb unberücksichtigt. Im Druckgefäß wird lediglich ein hydrostatisches Druckprofil berechnet, mit dessen Hilfe die Meßwerte von Differenzdruckgebern simuliert werden können. Die Anwendbarkeit des Modells ist wegen der fehlenden Impulsgleichungen auf kleine Lecks beschränkt. Der trägheitsbedingte Druckimpuls, der auf die Differenzdruckgeber in den ersten Zehntelsekunden des Aufsiedens wirkt, wird nicht nachgebildet. Die Verbindung zwischen Leckmassenstrom und Druckabfallgeschwindigkeit wird durch integrale Massen- und Energiebilanzen hergestellt, die über den gesamten Behälter gebildet werden. Je nach Option wird der Druckabfall aus dem Leckmassenstrom (BLDN) oder umgekehrt (BLDN_PV) berechnet. Der Wärmestrom, der von den Behälterwänden infolge des Absinkens der Fluidtemperatur während des Druckentlastungsvorgangs ausgeht, wird mit einer Wärmeübergangszahl für gesättigtes Sieden berechnet. Die momentane Temperatur an der Behälterinnenwand wird durch analytische Lösung der Wärmeleitungsgleichung in der Wand bestimmt. Der Verlauf des Massenhöhenstands (collapsed level) wird durch Integration des Leckmassenstroms bestimmt. Der Gemischspiegel wird unter Vorgabe des jeweiligen Massenhöhenstands aus der axialen Dampfgehaltsverteilung ermittelt. Bei der Berechnung des Dampfgehalts am Leckort wird die Lage des Gemischspiegels und die Höhe der Sprudelschicht (Schaumzone) berücksichtigt. Letztere bildet sich am Übergang von der Blasenströmung zum Dampfraum heraus.]]></dc:description>
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<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Richter, H.]]></dc:creator>
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<dc:title><![CDATA[Determination of Fracture Mechanical Values Using Charpy Size SENB Specimes and Correlation with Charpy-V Impact Test Results]]></dc:title>
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<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
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<dc:title><![CDATA[Herstellung und Prüfung von Charpy-V-Verbundproben]]></dc:title>
<dc:source><![CDATA[Jahressitzung 1996 der DVM-Arbeitsgruppe "Instrumentierter Kerbschlagbiegeversuch", Merseburg, 13.09. 1996]]></dc:source>
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<dc:creator><![CDATA[Ferse, W.]]></dc:creator>
<dc:creator><![CDATA[Kruber, S.]]></dc:creator>
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<dc:title><![CDATA[ECON - Ein System zur Lastmodellierung]]></dc:title>
<dc:source><![CDATA[Bericht Forschungszentrum Rossendorf, Institut für Sicherheitsforschung, 1996]]></dc:source>
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<dc:creator><![CDATA[Ferse, W.]]></dc:creator>
<dc:creator><![CDATA[Geiger, W.]]></dc:creator>
<dc:creator><![CDATA[Reitz, T.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1761-1</dc:identifier>
<dc:title><![CDATA[Spezifikation und Struktur der Altlastenbewertung mit dem Programmsystem XUMA-GEFA]]></dc:title>
<dc:source><![CDATA[Bericht Forschungszentrum Rossendorf, Institut für Sicherheisforschung, 1996]]></dc:source>
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<identifier>HZDR:PUBLDB:1418-1</identifier>
<datestamp>2025-02-17</datestamp>
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<dc:creator><![CDATA[Schnare, H.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Frauendorf, S.]]></dc:creator>
<dc:creator><![CDATA[Dönau, F.]]></dc:creator>
<dc:creator><![CDATA[Käubler, L.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Jungclaus, A.]]></dc:creator>
<dc:creator><![CDATA[Lieb, K. P.]]></dc:creator>
<dc:creator><![CDATA[Lingk, C.]]></dc:creator>
<dc:creator><![CDATA[Skoda, S.]]></dc:creator>
<dc:creator><![CDATA[Eberth, J.]]></dc:creator>
<dc:creator><![CDATA[Angelis, G.]]></dc:creator>
<dc:creator><![CDATA[Lo Bianco, G.]]></dc:creator>
<dc:creator><![CDATA[Gadea, A.]]></dc:creator>
<dc:creator><![CDATA[Farnea, E.]]></dc:creator>
<dc:creator><![CDATA[Napoli, D. R.]]></dc:creator>
<dc:creator><![CDATA[Ur, C. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1418-1</dc:identifier>
<dc:title><![CDATA[First evidence of magnetic rotation in the A=80 region]]></dc:title>
<dc:source><![CDATA[Physical Review Letters Vol 82, Number 22, 31 May 1999, 4408-4411]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevLett.82.4408]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:1420-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Gabriel, F.]]></dc:creator>
<dc:creator><![CDATA[Gippner, P.]]></dc:creator>
<dc:creator><![CDATA[Grosse, E.]]></dc:creator>
<dc:creator><![CDATA[Janssen, D.]]></dc:creator>
<dc:creator><![CDATA[Michel, P.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Schamlott, A.]]></dc:creator>
<dc:creator><![CDATA[Seidel, W.]]></dc:creator>
<dc:creator><![CDATA[Steegmueller, U.]]></dc:creator>
<dc:creator><![CDATA[Wenzel, M.]]></dc:creator>
<dc:creator><![CDATA[Wolf, A.]]></dc:creator>
<dc:creator><![CDATA[Wünsch, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1420-1</dc:identifier>
<dc:title><![CDATA[The FEL Projects at the Rossendorf Radiation Source ELBE.]]></dc:title>
<dc:source><![CDATA[20th Int.Free Electron Laser Conference, Williamsburg USA, Aug.1998]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Abstract: The status of the ELBE FEL projects is reviewed. ü]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:14200-1</identifier>
<datestamp>2025-06-05</datestamp>
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<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pagowska, K.]]></dc:creator>
<dc:creator><![CDATA[Ratajczak, R.]]></dc:creator>
<dc:creator><![CDATA[Stonert, A.]]></dc:creator>
<dc:creator><![CDATA[Turos, A.]]></dc:creator>
<dc:creator><![CDATA[Nowicki, L.]]></dc:creator>
<dc:creator><![CDATA[Sathish, N.]]></dc:creator>
<dc:creator><![CDATA[Jozwik, P.]]></dc:creator>
<dc:creator><![CDATA[Muecklich, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14200-1</dc:identifier>
<dc:title><![CDATA[RBS\channeling and TEM study of damage buildup in ion bombarded GaN]]></dc:title>
<dc:source><![CDATA[VIII-th International Conference Ion Implantation and Other Applications of Ions and Electrons, 14.-17.06.2010, Kazimierz Dolny, Poland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[A systematic study on structural defect buildup in 320 keV Ar-ion bombarded GaN epitaxial layers has been reported, by varying ion fluences ranged from 5x10<SUP>12</SUP> to 1x10<SUP>17</SUP> at/cm<SUP>2</SUP>. 1μm thick GaN epitaxial layers were grown on sapphire substrates using the MOVPE technique. RBS\channeling with 1.7 MeV <SUP>4</SUP>He beam was applied for analysis. As a complementary method High Resolution Transmission Electron Microscopy (HRTEM) has been used. The later has revealed the presence of extended defects like dislocations, faulted loops and stacking faults. New version of the Monte Carlo simulation code McChasy has been developed that makes it possible to analyze such defects on the basis of the Bent Channel (BC) model. Damage accumulation curves for two distinct types of defects, i.e. Randomly Displaced Atoms (RDA) and extended defects (i.e BC) have been determined. They were evaluated in the frame of the MultiStep Damage Accumulation (MSDA) model, allowing numerical parameterization of defect transformations occurring upon ion bombardment. Displaced atoms buildup is a three step process for GaN and whereas extended defect buildup is always a two step process.]]></dc:description>
<dc:subject><![CDATA[GaN]]></dc:subject>
<dc:subject><![CDATA[ion bombardment]]></dc:subject>
<dc:subject><![CDATA[ion channeling]]></dc:subject>
<dc:subject><![CDATA[TEM]]></dc:subject>
<dc:subject><![CDATA[defect transformations]]></dc:subject>
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<identifier>HZDR:PUBLDB:1423-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Zänker, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, W.]]></dc:creator>
<dc:creator><![CDATA[Brendler, V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1423-1</dc:identifier>
<dc:title><![CDATA[Charakterisierung der Kolloidpartikel im Hauptentwässerungsstollen des Freiberger Bergbaureviers (Rothschönberger Stolln)]]></dc:title>
<dc:source><![CDATA[GDCh-Fachtagung, FG Nuklearchemie, Dresden, Germany, 07.-09.09.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Der Rothschönberger Stolln ist der Hauptentwässerungsstollen des aufgelassenen Freiberger Bergbaureviers. An seinem Mundloch enthält sein Wasser etwa 1 mg/l an kolloidalen Partikeln des Größenbereichs 75 bis 300 nm. Die Partikel bestehen vor allem aus Eisen- und Aluminiumoxidhydroxid, tragen aber auch Spurenelemente (Pb, As, Cu, Y, La). Die Schadstoffe Pb und As z.B. sind im Rothschönberger Stolln  nahezu vollständig an Kolloide gebunden. Das Uranium dagegen liegt in nichtkolloidaler Form (echt gelöst) vor; wahrscheinlich sind dafür Karbonatkomplexe des Uranylions verantwortlich. Nach Absenken des pH-Wertes auf etwa 5 (Zerstörung der Karbonatkomplexe) waren erhebliche Mengen des Uraniums an Kolloide gebunden. Letzteres besitzt Bedeutung für die Beurteilung des Verhaltens von Uranium in  sauren Grubenwässern, wie z. B. in Wässern der Urangrube Königstein. Speziationsrechnungen mit Hilfe des thermodynamischen Geochemie-Rechenprogramms EQ6 stimmen zunächst schlecht mit den experimentellen Befunden überein. Die vom Experiment abweichenden Rechenergebnisse können jedoch leicht aus einer unzureichenden Berücksichtigung der Kinetik im chemischen Modell erklärt werden. Die Versuche zeigen Wege auf, wie Modellrechnungen mit EQ6 "praxisnäher" gemacht werden können.]]></dc:description>
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<identifier>HZDR:PUBLDB:1424-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
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<dc:title><![CDATA[Institute of Radiochemistry; Annual Report 1998]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-247 Januar 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Annual Report 1998
Institute of Radiochemistry]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1425-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Uglov, V. V.]]></dc:creator>
<dc:creator><![CDATA[Khodasevich, V. V.]]></dc:creator>
<dc:creator><![CDATA[Kuleshov, A. K.]]></dc:creator>
<dc:creator><![CDATA[Fedotova, J. A.]]></dc:creator>
<dc:creator><![CDATA[Rusalsky, D. P.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1425-2</dc:identifier>
<dc:title><![CDATA[Plasma immersion ion implantation for improvement of mechanical properties of ANSI M2 steel]]></dc:title>
<dc:source><![CDATA[4th Int. Workshop on PBII, Dearborn, June 2-4, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Khodasevich, V. V.]]></dc:creator>
<dc:creator><![CDATA[Kuleshov, A. K.]]></dc:creator>
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<dc:title><![CDATA[Plasma immersion ion implantation for improvement of mechanical properties of ANSI M2 steel]]></dc:title>
<dc:source><![CDATA[Journal of Vacuum Science and Technology B 17(2), Mar/Apr 1999, 836-839]]></dc:source>
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<dc:creator><![CDATA[Reich, T.]]></dc:creator>
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<dc:title><![CDATA[Euroconference and NEA Workshop Actinide-XAS-98]]></dc:title>
<dc:source><![CDATA[ESRF Newsletter]]></dc:source>
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<dc:description><![CDATA[Euroconference and NEA Workshop Actinide-XAS-98]]></dc:description>
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<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
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<dc:title><![CDATA[Photoluminescence and electroluminescence investigations at Ge-rich SiO<SUB>2</SUB> layers]]></dc:title>
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<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
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<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Fröb, H.]]></dc:creator>
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<dc:title><![CDATA[Photoluminescence and electroluminescence investigations at Ge-rich SiO<SUB>2</SUB> layers]]></dc:title>
<dc:source><![CDATA[Journal of Luminescence 80 (1999) 275-279]]></dc:source>
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<dc:creator><![CDATA[Iskra, W.]]></dc:creator>
<dc:creator><![CDATA[Rotter, I.]]></dc:creator>
<dc:creator><![CDATA[Dittes, F.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2108-1</dc:identifier>
<dc:title><![CDATA[Hierarchical trapping of resonance states at high level density]]></dc:title>
<dc:source><![CDATA[Physical Review C 47, (1993), 1086-1090]]></dc:source>
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<dc:creator><![CDATA[Beyer, M.]]></dc:creator>
<dc:creator><![CDATA[Carl, H.]]></dc:creator>
<dc:creator><![CDATA[Langer, L.]]></dc:creator>
<dc:creator><![CDATA[Nowak, K.]]></dc:creator>
<dc:creator><![CDATA[Seidel, A.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Tolksdorf, P.]]></dc:creator>
<dc:creator><![CDATA[Zschau, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1767-1</dc:identifier>
<dc:title><![CDATA[Aufbau eines technischen Systems zur Verbesserung der betrieblichen Überwachung des KKW Saporoshje durch die staatliche Aufsichtsbehörde der Ukraine (in Russisch)]]></dc:title>
<dc:source><![CDATA[Atomnaja Technika sa Rubeshom, Heft 3 (1995), S.3]]></dc:source>
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<dc:description><![CDATA[Es wird die Struktur eines technischen Computersystems zur betrieblichen Überwachung der Zuverlässigkeit und Sicherheit ukrainischer KKW durch die staatlichen Aufsichtsbehörden beschrieben. Nach Auffassung der Autoren führt der Aufbau eines solchen Überwachungssystems, unabhängig von den Kontrollsystemen des Betreibers, zu einer schnellen, signifikanten und kostengünstigen Sicherheitserhöhung beim Betrieb der Reaktoranlagen vom Typ WWER-1000.]]></dc:description>
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<dc:creator><![CDATA[Schuhmann, P.]]></dc:creator>
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<dc:title><![CDATA[Bestimmung eines repräsentativen Wertes aus einer Folge von Meßwerten]]></dc:title>
<dc:source><![CDATA[Fachbericht FWSF 02/96, August 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1764-1</identifier>
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<dc:creator><![CDATA[Mäding, P.]]></dc:creator>
<dc:creator><![CDATA[Scheunemann, M.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Iterbeke, K.]]></dc:creator>
<dc:creator><![CDATA[Tourwe, D.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1764-1</dc:identifier>
<dc:title><![CDATA[Development of potential tumour imaging agents by 4-[<SUP>18</SUP>F]]]></dc:title>
<dc:source><![CDATA[8<SUP>th</SUP> Conference of Central European Division of International Isotope Society, Bad Soden, 10.-11.6.1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The 4-[<SUP>18</SUP>F]fluorobenzoyl compounds of Neurotensin(8-13) (NT(8-13)) as well as [Arg<SUP>8</SUP>pseudo(CH<SUB>2</SUB>NH)Arg<SUP>9</SUP>]NT(8-13) were obtained by reaction of N-succinimidyl 4-[<SUP>18</SUP>F]fluorobenzoate ([<SUP>18</SUP>F]SFB) with these peptides in aqueous buffered solutions at pH 8.3 in r.c.y. of up to 43 % (related to [<SUP>18</SUP>F]SFB; decay-corrected) within 80 min (including HPLC purification). This is the first example for the specific radiolabelling of the alpha-amino group at the N-terminal arginine unit of peptides using [<SUP>18</SUP>F]SFB.]]></dc:description>
<dc:subject><![CDATA[Neurotensin(8-13)]]></dc:subject>
<dc:subject><![CDATA[<SUP>18</SUP>F-labelling]]></dc:subject>
<dc:subject><![CDATA[[<SUP>18</SUP>F]SFB]]></dc:subject>
<dc:subject><![CDATA[neurotensin receptor]]></dc:subject>
<dc:subject><![CDATA[pseudopeptide]]></dc:subject>
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<dc:creator><![CDATA[Mäding, P.]]></dc:creator>
<dc:creator><![CDATA[Scheunemann, M.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
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<dc:creator><![CDATA[Tourwe, D.]]></dc:creator>
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<dc:title><![CDATA[Development of potential tumour imaging agents by 4-[<SUP>18</SUP>F]]]></dc:title>
<dc:source><![CDATA[J. Labelled Compd. Radiopharm. 42 (1999) 987-1022]]></dc:source>
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<dc:description><![CDATA[The 4-[<SUP>18</SUP>F]fluorobenzoyl compounds of Neurotensin(8-13) (NT(8-13)) as well as [Arg<SUP>8</SUP>pseudo(CH<SUB>2</SUB>NH)Arg<SUP>9</SUP>]NT(8-13) were obtained by reaction of N-succinimidyl 4-[<SUP>18</SUP>F]fluorobenzoate ([<SUP>18</SUP>F]SFB) with these peptides in aqueous buffered solutions at pH 8.3 in r.c.y. of up to 43 % (related to [<SUP>18</SUP>F]SFB; decay-corrected) within 80 min (including HPLC purification). This is the first example for the specific radiolabelling of the alpha-amino group at the N-terminal arginine unit of peptides using [<SUP>18</SUP>F]SFB.]]></dc:description>
<dc:subject><![CDATA[Neurotensin(8-13)]]></dc:subject>
<dc:subject><![CDATA[<SUP>18</SUP>F-labelling]]></dc:subject>
<dc:subject><![CDATA[[<SUP>18</SUP>F]SFB]]></dc:subject>
<dc:subject><![CDATA[neurotensin receptor]]></dc:subject>
<dc:subject><![CDATA[pseudopeptide]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:creator><![CDATA[Bergner, F.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, U.]]></dc:creator>
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<dc:title><![CDATA[Punktquelle-Punktempfänger-Modell zur Rißfortschrittsmessung mit Ultraschall]]></dc:title>
<dc:source><![CDATA[DVM Arbeitsgemeinschaft Werkstoffe, Tagung "Werkstoffprüfung", Bad Nauheim, 5. - 6. Dezember 1995, Proc. S. 419]]></dc:source>
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<identifier>HZDR:PUBLDB:1768-1</identifier>
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<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1768-1</dc:identifier>
<dc:title><![CDATA[Detection of Irradiation-Inducted Microstructures Changes of VVER-Type RPV Steel by Small Angle Scattering Methods]]></dc:title>
<dc:source><![CDATA[Proc. International Topical Meeting on VVER-Safety, Prague, Sept. 1995, Session III, paper 7]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1770-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Eichhorn, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1770-1</dc:identifier>
<dc:title><![CDATA[ASAXS-Investigations of Irradiation - Induced Precipitates in VVER-440-Type Reactor Pressure Vessel Steel with High Cu Content]]></dc:title>
<dc:source><![CDATA[HASYLAB-Jahresbericht 1994, Hamburg, Januar 1995, S. 535]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1773-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1773-1</dc:identifier>
<dc:title><![CDATA[Acoustic Leak Monitoring Using Neural Networks]]></dc:title>
<dc:source><![CDATA[Proc. Annual Meeting on Nuclear Technology '95, Nürnberg, May 16 - 18 1995, pp. 231 - 234]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1774-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Hollstein, F.]]></dc:creator>
<dc:creator><![CDATA[Meyer, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1774-1</dc:identifier>
<dc:title><![CDATA[Calculation of Neutron Noise Due to Control Rod Vibrations Using Nodal Methods for Hexagonal-Z-Geometry]]></dc:title>
<dc:source><![CDATA[Proc. Specialists Meeting on Reactor Noise, SMORN VII, Avignon, France, 19 - 23 June, 1995, Vol. 2, 12.1]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:226-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Galindo, V.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Treuner, M.]]></dc:creator>
<dc:creator><![CDATA[Langbein, D.]]></dc:creator>
<dc:creator><![CDATA[Rath, H. J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-226-1</dc:identifier>
<dc:title><![CDATA[Thermocapillary bubble migration -Drop tower experiments-]]></dc:title>
<dc:source><![CDATA["Drop Tower Days 94", Bremen, Juli 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Experiments on the thermocapillary bubble migration are presently carried out in the Drop Tower Bremen. After a heating period of about two hours, a sufficiently linear temperature gradient is established with paraffin liquids in a cavity. For the moment of drop of the capsule two bubbles with diameters of up to 2 mm are generated and the injection needles are retracted. During 4.74 s under strongly reduced gravity the speed of the bubble migration is observed with video camera, the temperature field by Pt 100 temperature gauges and the use of a differential interferometer. First experimental results with a liquid characterized by the Prandtl number Pr = 10 (n-decane) agree very well with theoretical data available both from literature as well as with numerical simulations. The correspoding Reynolds numbers are in the range between 20 < Re < 160. The experimental setup, the measuring technique and the evaluation method will be presented as well as comparison between experimental and theoretical results.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1845-1</identifier>
<datestamp>2019-03-04</datestamp>
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            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Barz, H.-U.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, U.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, U.]]></dc:creator>
<dc:creator><![CDATA[Konheiser, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1845-1</dc:identifier>
<dc:title><![CDATA[Characterization of the Initial State of the Reactor Pressure Vessel Steels of the Rheinsberg Irradiation Programme - Survey on Mechanical Testing including Fracture Mechanics and Fluence Investigation in the Research Centre Rossendorf]]></dc:title>
<dc:source><![CDATA[5th Specialists Meeting of Scientific and Engineering Cooperation Agreement - Safety of Components, Stuttgart, 04. - 07. 10. 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[A German/Russian irradiation programme was performed in the high flux irradiation channels of the PWR VVER-2 Rheinsberg from 1984 to 1987. Within the programme Charpy-V-, COD-, 0,5-CT-, X-CT- and 1-CT specimens of reactor pressure vessel (RPV) steels 15Kh2MFA and 15Kh2NMFA(A) and RPV weld metal 10KhMFT, 10Kh2MFA(U) and 10KhNMA(A) were irradiated. These materials are used in the pressurized water reactor of Russian type VVER-440 and VVER-1000. The irradiation of one series of experiments took one year. In this paper the unirradiated initial state of the material is characterized. The mechanical properties measured at different temperatures include instrumented Charpy-V notch- and quasistatic fracture toughness data. Furthermore the neutronfluence of the specimens were calculated in dependence of the position in the high flux irradiation channels of the PWR VVER-2 Rheinsberg.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:160-1</identifier>
<datestamp>2019-03-04</datestamp>
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</header>
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<oai_dc:dc
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<dc:creator><![CDATA[Weier, T.]]></dc:creator>
<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Alemany, A.]]></dc:creator>
<dc:creator><![CDATA[Pilaud, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-160-1</dc:identifier>
<dc:title><![CDATA[On Stability of MHD flow around a cylinder in an aligned magnetic fields]]></dc:title>
<dc:source><![CDATA[Magnitnaya gidrodinamika 1997 Vol. 33, No. 1, p. 14-22 (in Russian)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The hydromagnetic stability of the flow of an incompressible conducting fluid around a circular cyliner in a uniform magnetic field parallel to the mean flow is investigated with different approaches:
 	Experiments for 1000 < Re < 9000
 	a simple analytical model
 	numerical simulation for Re < 1000.
Main goal of the investigations is to find the stability curce inthe (Re, N)-plane, and to distinguish between 2D and 3D instabilities.
Experimental results will be presented based on hot-wire measurements in the down-stream cylinder wake. The suppression of the vortex street by increasing magnetic fields is clearly identified.
Parallel to the disappearance of the typical Kármán frequency an increase of low frequency fluctuations is observed in the spectrum. This will be discussed in therms of theoretical predictions for long-wave MHD instabilities.
More physical insight into the stability behaviour is obtained by a simple Kolmogorov flow modelling of the cylinder wake and the corresponding stability analysis. Theoretical results will be presented for the 2D case: critical Reynolds number, wave number and Strouhal number as function of the magnetic field.
The critical wave number jumbs form the region of the typical Kármán value to very low values at a distinct magnetic field strength. The simple model is extended to include 3D instabilities in the flow. Limitations of the model and the comparison to experiments will be discussed.
Finally the 2D case for Re < 1000 will be compared with results of a full numerical simulation.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:160-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Weier, T.]]></dc:creator>
<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Alemany, A.]]></dc:creator>
<dc:creator><![CDATA[Pilaud, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-160-2</dc:identifier>
<dc:title><![CDATA[On Stability of MHD flow around a cylinder in an aligned magnetic fields]]></dc:title>
<dc:source><![CDATA["Energy Transfer in MHD Flows", Sept. 1994, Aussois, Frankreich]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The hydromagnetic stability of the flow of an incompressible conducting fluid around a circular cyliner in a uniform magnetic field parallel to the mean flow is investigated with different approaches:
 	Experiments for 1000 < Re < 9000
 	a simple analytical model
 	numerical simulation for Re < 1000.
Main goal of the investigations is to find the stability curce inthe (Re, N)-plane, and to distinguish between 2D and 3D instabilities.
Experimental results will be presented based on hot-wire measurements in the down-stream cylinder wake. The suppression of the vortex street by increasing magnetic fields is clearly identified.
Parallel to the disappearance of the typical Kármán frequency an increase of low frequency fluctuations is observed in the spectrum. This will be discussed in therms of theoretical predictions for long-wave MHD instabilities.
More physical insight into the stability behaviour is obtained by a simple Kolmogorov flow modelling of the cylinder wake and the corresponding stability analysis. Theoretical results will be presented for the 2D case: critical Reynolds number, wave number and Strouhal number as function of the magnetic field.
The critical wave number jumbs form the region of the typical Kármán value to very low values at a distinct magnetic field strength. The simple model is extended to include 3D instabilities in the flow. Limitations of the model and the comparison to experiments will be discussed.
Finally the 2D case for Re < 1000 will be compared with results of a full numerical simulation.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:14381-1</identifier>
<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Timmel, K.]]></dc:creator>
<dc:creator><![CDATA[Galindo, V.]]></dc:creator>
<dc:creator><![CDATA[Miao, X.]]></dc:creator>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14381-1</dc:identifier>
<dc:title><![CDATA[Physikalische Modellierung des Stranggussprozesses mit niedrig schmelzenden Legierungen]]></dc:title>
<dc:source><![CDATA[Symposium Stranggießen, 15.-17.11.2010, Neu-Ulm, Deutschland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Die Strömung in der Metallschmelze hat einen wesentlichen Einfluss auf die Produktqualität beim Stranggießen. Probleme entstehen beispielsweise durch Einschlüsse von Oxiden, intermetallischen Verbindungen oder Gasblasen, die durch eine unkontrollierte Strömung in die Erstarrungszone gelangen. Die Optimierung dieser Strömung basierte bisher vor allem auf numerischen Simulationen und Modellexperimenten mit Wasser. Obwohl die Strömungsuntersuchungen an diesen Wassermodellen signifikante Erkenntnisgewinne über die Strömung und die optimale Auslegung z.B. des Tauchrohrs oder der Eintauchtiefe des Tauchrohrs gebracht haben, stoßen diese Modelle für eine Reihe von Fragestellungen an ihre physikalischen Grenzen, da Flüssigmetalle z.B. sehr hohe Oberflächenspannungen und sehr kleine Prandtl-Zahl besitzen, und Wasser offensichtlich für Untersuchungen des Einflusses von Magnetfeldern völlig ungeeignet ist.
In den vergangenen Jahren wurden am Forschungszentrum Dresden-Rossendorf experimentelle Versuchsanlagen mit niedrig schmelzenden Legierungen für die physikalische Modellierung des Stranggussprozesses aufgebaut. Ziel ist die systematische Untersuchung der Flüssigmetallströmungen und Transportprozesse in Verteiler, Tauchrohr und Kokille. Dabei steht insbesondere die Wirkung elektromagnetischer Felder, wie sie in Form von elektromagnetischen Bremsen oder Rührern bereits im industriellen Einsatz sind, im Mittelpunkt. Außerdem bieten die Versuchsanlagen gute Bedingungen für die Erprobung neuer Messtechniken und Anlagenkomponenten. Die Versuchsanlage CONCAST-LMM (Continuous Casting Liquid Metal Model) ist 2009 fertig gestellt worden und arbeitet mit einer Sn60Bi40-Legierung als Modellfluid im Temperaturbereich von 200°C bis 400°C. Ein kleineres Modell mit der eutektischen GaInSn-Legierung wird bei Raumtemperatur betrieben. Die Strömungseigenschaften werden mit Hilfe lokaler Sonden sowie modernen Ultraschall und elektromagnetischen Methoden vermessen. 
Im Rahmen dieses Beitrages werden Strömungsmessungen in einer einphasigen Flüssigmetallströmung in der Kokille unter Einwirkung eines statischen Magnetfeldes vorgestellt und mit entsprechenden numerischen Simulationen verglichen. Es zeigt sich, dass das Magnetfeld den aus dem Tauchrohr in die Kokille austretenden Jet ablenkt und lokale Rezirkulationsgebiete verstärkt. Die bremsende Wirkung des Magnetfeldes stellt sich als äußerst komplex dar. Eine gleichmäßige Reduktion der Strömungsgeschwindigkeit im gesamten Volumen wird nicht beobachtet.]]></dc:description>
<dc:subject><![CDATA[continuous casting]]></dc:subject>
<dc:subject><![CDATA[liquid metal model]]></dc:subject>
<dc:subject><![CDATA[magnetic field]]></dc:subject>
<dc:subject><![CDATA[mould flow]]></dc:subject>
<dc:subject><![CDATA[Ultrasound Doppler Method]]></dc:subject>
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<identifier>HZDR:PUBLDB:14381-2</identifier>
<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Timmel, K.]]></dc:creator>
<dc:creator><![CDATA[Galindo, V.]]></dc:creator>
<dc:creator><![CDATA[Miao, X.]]></dc:creator>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14381-2</dc:identifier>
<dc:title><![CDATA[Physikalische Modellierung des Stranggussprozesses mit niedrig schmelzenden Legierungen]]></dc:title>
<dc:source><![CDATA[Symposium Stranggießen, 15.-17.11.2010, Neu-Ulm, Deutschland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Die Strömung in der Metallschmelze hat einen wesentlichen Einfluss auf die Produktqualität beim Stranggießen. Probleme entstehen beispielsweise durch Einschlüsse von Oxiden, intermetallischen Verbindungen oder Gasblasen, die durch eine unkontrollierte Strömung in die Erstarrungszone gelangen. Die Optimierung dieser Strömung basierte bisher vor allem auf numerischen Simulationen und Modellexperimenten mit Wasser. Obwohl die Strömungsuntersuchungen an diesen Wassermodellen signifikante Erkenntnisgewinne über die Strömung und die optimale Auslegung z.B. des Tauchrohrs oder der Eintauchtiefe des Tauchrohrs gebracht haben, stoßen diese Modelle für eine Reihe von Fragestellungen an ihre physikalischen Grenzen, da Flüssigmetalle z.B. sehr hohe Oberflächenspannungen und sehr kleine Prandtl-Zahl besitzen, und Wasser offensichtlich für Untersuchungen des Einflusses von Magnetfeldern völlig ungeeignet ist.
In den vergangenen Jahren wurden am Forschungszentrum Dresden-Rossendorf experimentelle Versuchsanlagen mit niedrig schmelzenden Legierungen für die physikalische Modellierung des Stranggussprozesses aufgebaut. Ziel ist die systematische Untersuchung der Flüssigmetallströmungen und Transportprozesse in Verteiler, Tauchrohr und Kokille. Dabei steht insbesondere die Wirkung elektromagnetischer Felder, wie sie in Form von elektromagnetischen Bremsen oder Rührern bereits im industriellen Einsatz sind, im Mittelpunkt. Außerdem bieten die Versuchsanlagen gute Bedingungen für die Erprobung neuer Messtechniken und Anlagenkomponenten. Die Versuchsanlage CONCAST-LMM (Continuous Casting Liquid Metal Model) ist 2009 fertig gestellt worden und arbeitet mit einer Sn60Bi40-Legierung als Modellfluid im Temperaturbereich von 200°C bis 400°C. Ein kleineres Modell mit der eutektischen GaInSn-Legierung wird bei Raumtemperatur betrieben. Die Strömungseigenschaften werden mit Hilfe lokaler Sonden sowie modernen Ultraschall und elektromagnetischen Methoden vermessen. 
Im Rahmen dieses Beitrages werden Strömungsmessungen in einer einphasigen Flüssigmetallströmung in der Kokille unter Einwirkung eines statischen Magnetfeldes vorgestellt und mit entsprechenden numerischen Simulationen verglichen. Es zeigt sich, dass das Magnetfeld den aus dem Tauchrohr in die Kokille austretenden Jet ablenkt und lokale Rezirkulationsgebiete verstärkt. Die bremsende Wirkung des Magnetfeldes stellt sich als äußerst komplex dar. Eine gleichmäßige Reduktion der Strömungsgeschwindigkeit im gesamten Volumen wird nicht beobachtet.]]></dc:description>
<dc:subject><![CDATA[continuous casting]]></dc:subject>
<dc:subject><![CDATA[liquid metal model]]></dc:subject>
<dc:subject><![CDATA[magnetic field]]></dc:subject>
<dc:subject><![CDATA[mould flow]]></dc:subject>
<dc:subject><![CDATA[Ultrasound Doppler Method]]></dc:subject>
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<identifier>HZDR:PUBLDB:3096-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Matys, S.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Scheunemann, M.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3096-1</dc:identifier>
<dc:title><![CDATA[Rhenium- und Technetiumverbindungen als potentielle Substrate und Modulatoren von P-Glykoprotein: Untersuchungen an Hirnzellen in vitro]]></dc:title>
<dc:source><![CDATA[Intern. Jahrestagung DGN, Kassel, 16.-19.04.1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Die mit <SUP>99m</SUP>Tc-MIBI und ähnlichen Verbindungen nachweisbare Expression von P-Glykoproteinen (Pgp), z.B. In Tumoren, ist auch für den Transport von Substanzen durch die Blut-Hirn-Schranke (BHS) von Bedeutung. Die Pgp sind eine Komponente der multidrug resistance. In der BHJS bilden sie ein funktionelle Barriere zum Schutz des Gehirns vor toxischen Substanzen, indem sie die Pgp-Substrate in einem ATP-abhängigen Prozess vom Gehirn in das Blut transportieren. In RT-PCR Studien an amortalisierten Endothelzellen von Rattenhirnkapillaren (RBE4) wurde die Expression der Genprodukte  von mdr1a und verstärkt von mdr1b, ähnlich den Verhältnissen bei frisch präparierten Rattenhirnmikrogefäßen, nachgewiesen.  Zur Beurteilung von Transportvorgängen durch die Pgp an der BHS wurden deshalb in-vitro-Studien mit RBE-4-Zellen durchgeführt. Funktionell wurde die Pgp-Aktivität charakterisiert durch die Zellaufnahme und den Efflux von [<SUP>99m</SUP>Tc]MIBI, [<SUP>3</SUP>H]Colchicin und [<SUP>3</SUP>H]Vinblastin unter Standardbedingungen und bei Hemmung der Pgp. Da die Akkumulation dieser Tracer ganz wesentlich von der metabolistischen Lage der Zellen abhängt wurden in ausgewählten Experimenten Simultanmessungen mit [<SUP>18</SUP>F]FDG und anderen Stoffwechseltracern durchgeführt.  Mit dem so etablierten Modell konnte der Einfluss von mehr als 20 neuen <SUP>99</SUP>Tc- bzw. Re-Komplexen  auf die Pgp Aktivität untersucht werden. Es zeigt sich, dass verschiedene Substanzen zu Veränderungen der Tracerakkumulation in den RBE4-Zellen führen. So wurden Komplexe identifiziert, deren Wirkung mit der des Pgp-Inhibitors Verapamil vergleichbar ist. So erhöht sich z.B. spezifisch die nach 1 h in den Zellen verbleibende [<SUP>99m</SUP>Tc]MIBI Aktivität bei der Applikation von einer <SUP>99</SUP>Tc- oder analogen Re-Substanz auf 1157±72% bzw. 1117±56% und von Verapamil (je 10 µM) auf 859±103% der Kontrolle.
Die Ergebnisse lassen erwarten, dass Tc- oder Re-Komplexe nicht nur Substrate, sondern auch Modulatoren der Pgp sein können. 
]]></dc:description>
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<identifier>HZDR:PUBLDB:3096-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Matys, S.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Scheunemann, M.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3096-2</dc:identifier>
<dc:title><![CDATA[Rhenium- und Technetiumverbindungen als potentielle Substrate und Modulatoren von P-Glykoprotein: Untersuchungen an Hirnzellen in vitro]]></dc:title>
<dc:source><![CDATA[Nuklearmedizin 36 (1997) A34]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Die mit <SUP>99m</SUP>Tc-MIBI und ähnlichen Verbindungen nachweisbare Expression von P-Glykoproteinen (Pgp), z.B. In Tumoren, ist auch für den Transport von Substanzen durch die Blut-Hirn-Schranke (BHS) von Bedeutung. Die Pgp sind eine Komponente der multidrug resistance. In der BHJS bilden sie ein funktionelle Barriere zum Schutz des Gehirns vor toxischen Substanzen, indem sie die Pgp-Substrate in einem ATP-abhängigen Prozess vom Gehirn in das Blut transportieren. In RT-PCR Studien an amortalisierten Endothelzellen von Rattenhirnkapillaren (RBE4) wurde die Expression der Genprodukte  von mdr1a und verstärkt von mdr1b, ähnlich den Verhältnissen bei frisch präparierten Rattenhirnmikrogefäßen, nachgewiesen.  Zur Beurteilung von Transportvorgängen durch die Pgp an der BHS wurden deshalb in-vitro-Studien mit RBE-4-Zellen durchgeführt. Funktionell wurde die Pgp-Aktivität charakterisiert durch die Zellaufnahme und den Efflux von [<SUP>99m</SUP>Tc]MIBI, [<SUP>3</SUP>H]Colchicin und [<SUP>3</SUP>H]Vinblastin unter Standardbedingungen und bei Hemmung der Pgp. Da die Akkumulation dieser Tracer ganz wesentlich von der metabolistischen Lage der Zellen abhängt wurden in ausgewählten Experimenten Simultanmessungen mit [<SUP>18</SUP>F]FDG und anderen Stoffwechseltracern durchgeführt.  Mit dem so etablierten Modell konnte der Einfluss von mehr als 20 neuen <SUP>99</SUP>Tc- bzw. Re-Komplexen  auf die Pgp Aktivität untersucht werden. Es zeigt sich, dass verschiedene Substanzen zu Veränderungen der Tracerakkumulation in den RBE4-Zellen führen. So wurden Komplexe identifiziert, deren Wirkung mit der des Pgp-Inhibitors Verapamil vergleichbar ist. So erhöht sich z.B. spezifisch die nach 1 h in den Zellen verbleibende [<SUP>99m</SUP>Tc]MIBI Aktivität bei der Applikation von einer <SUP>99</SUP>Tc- oder analogen Re-Substanz auf 1157±72% bzw. 1117±56% und von Verapamil (je 10 µM) auf 859±103% der Kontrolle.
Die Ergebnisse lassen erwarten, dass Tc- oder Re-Komplexe nicht nur Substrate, sondern auch Modulatoren der Pgp sein können. 
]]></dc:description>
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<identifier>HZDR:PUBLDB:3153-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3153-1</dc:identifier>
<dc:title><![CDATA[Synthesis of new materials by ion beams]]></dc:title>
<dc:source><![CDATA[CSNSM, ORSAY Campus, France, May 3, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:3154-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3154-1</dc:identifier>
<dc:title><![CDATA[Atomistische Simulation der Ionenimplantation und ihre Anwendung in der Si-Technologie]]></dc:title>
<dc:source><![CDATA[Institut für Physik der Universität Augsburg, January 28,1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1426-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Baraniak, L.]]></dc:creator>
<dc:creator><![CDATA[Mack, B.]]></dc:creator>
<dc:creator><![CDATA[Abraham, A.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1426-1</dc:identifier>
<dc:title><![CDATA[Untersuchung des Einflusses der in Grubenwässern gelösten organischen Verbindungen auf den Valenzzustand von Radionukliden und Schwermetallen im Hinblick auf den Flutungsprozess der sächsischen Uranbergwerke]]></dc:title>
<dc:source><![CDATA[Abschlußbericht zum Förderprojekt des Ministeriums für Wissenschaft und Kunst des Freistaates Sachsen (Förderkennzeichen: 4-7541.83-FZR/512) Juni 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Mit Bezug auf die Flutung von Bergwerken im sächsischen Raum wurden die Redoxeigenschaften von natürlichen Polyelektrolyten, wie Holzabbauprodukten, Lignin und Huminsäuren und die Reduktion von Eisen(III) und Uran(VI) durch diese Polyelektrolyte untersucht. Außerdem wurde die Adsorption von Eisen(II,III) und Uran(IV,VI) aus Flutungswässern an grubentypischen Gesteinen und Sedimenten unter anaeroben Bedingungen bei Anwesenheit der organischen Substanzen untersucht. (Juni 1998)]]></dc:description>
<dc:subject><![CDATA[Umweltchemie]]></dc:subject>
<dc:subject><![CDATA[Bergbausanierung]]></dc:subject>
<dc:subject><![CDATA[Uranium]]></dc:subject>
<dc:subject><![CDATA[Eisen]]></dc:subject>
<dc:subject><![CDATA[Redoxchemie]]></dc:subject>
<dc:subject><![CDATA[Polyelektrolyte]]></dc:subject>
<dc:subject><![CDATA[Holzabbauprodukte]]></dc:subject>
<dc:subject><![CDATA[Lignin]]></dc:subject>
<dc:subject><![CDATA[Huminsäure]]></dc:subject>
<dc:subject><![CDATA[Potentiometrie]]></dc:subject>
<dc:subject><![CDATA[Voltammetrie]]></dc:subject>
<dc:subject><![CDATA[Spektrophotometrie]]></dc:subject>
<dc:subject><![CDATA[Adsorption]]></dc:subject>
<dc:subject><![CDATA[Radiotracer]]></dc:subject>
<dc:subject><![CDATA[Flüssigszintillationsmessung]]></dc:subject>
<dc:type>info:eu-repo/semantics/other</dc:type>
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<identifier>HZDR:PUBLDB:1428-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1428-1</dc:identifier>
<dc:title><![CDATA[Bacterial-Metal/Radionuclide Interaction: Basic Research and Bioremediation-Extendet Abstracts, Eurokonference, Forschungszentrum Rossendorf, December 2-4, 1998]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-252 Februar 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:14516-2</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Zhang, C.]]></dc:creator>
<dc:creator><![CDATA[Grants, I.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14516-2</dc:identifier>
<dc:title><![CDATA[Quantitative characterization of melt flows in AC magnetic fields]]></dc:title>
<dc:source><![CDATA[4th Asian Workshop on Electromagnetic Processing of Materials, 03.-06.10.2010, Jeju, South Korea, 172-175]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[This presentation considers various situations where the flow inside a liquid metal column is driven by different configurations of AC magnetic fields. The ultrasonic Doppler method has been used to determine profiles of the fluid velocity in the ternary alloy GaInSn. The azimuthal and vertical velocity components have been measured allowing for an analysis of both a swirling flow in the horizontal planes and the flow pattern in the radial-meridional plane. In particular, we consider here transient liquid metal flows generated inside a cylindrical container by the superposition of a rotating magnetic field (RMF) and a travelling magnetic field (TMF). The application of the magnetic body forces can be used to create a tornado-like vortex in a closed volume of liquid metal. Moreover, the case of an RMF-driven flow will be discussed which is influenced by an oxide layer at the free surface of the metallic melt. The oxide layer feels the effect of the viscous force arising from the moving liquid beneath and the friction force from the side walls. A complex interaction occurs if the both forces are in the same order of magnitude. In that case, our measurements demonstrate that the occurrence of the oxide layer may lead to an unexpected oscillating behaviour of the bulk flow.]]></dc:description>
<dc:subject><![CDATA[liquid metal]]></dc:subject>
<dc:subject><![CDATA[electromagnetic stirring]]></dc:subject>
<dc:subject><![CDATA[rotating magnetic field]]></dc:subject>
<dc:subject><![CDATA[ultrasound Doppler velocimetry]]></dc:subject>
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<datestamp>2025-06-05</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Zhang, C.]]></dc:creator>
<dc:creator><![CDATA[Grants, I.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14516-1</dc:identifier>
<dc:title><![CDATA[Quantitative characterization of melt flows in AC magnetic fields]]></dc:title>
<dc:source><![CDATA[4th Asian Workshop on Electromagnetic Processing of Materials, 03.-06.10.2010, Jeju, South Korea]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[This presentation considers various situations where the flow inside a liquid metal column is driven by different configurations of AC magnetic fields. The ultrasonic Doppler method has been used to determine profiles of the fluid velocity in the ternary alloy GaInSn. The azimuthal and vertical velocity components have been measured allowing for an analysis of both a swirling flow in the horizontal planes and the flow pattern in the radial-meridional plane. In particular, we consider here transient liquid metal flows generated inside a cylindrical container by the superposition of a rotating magnetic field (RMF) and a travelling magnetic field (TMF). The application of the magnetic body forces can be used to create a tornado-like vortex in a closed volume of liquid metal. Moreover, the case of an RMF-driven flow will be discussed which is influenced by an oxide layer at the free surface of the metallic melt. The oxide layer feels the effect of the viscous force arising from the moving liquid beneath and the friction force from the side walls. A complex interaction occurs if the both forces are in the same order of magnitude. In that case, our measurements demonstrate that the occurrence of the oxide layer may lead to an unexpected oscillating behaviour of the bulk flow.]]></dc:description>
<dc:subject><![CDATA[liquid metal]]></dc:subject>
<dc:subject><![CDATA[electromagnetic stirring]]></dc:subject>
<dc:subject><![CDATA[rotating magnetic field]]></dc:subject>
<dc:subject><![CDATA[ultrasound Doppler velocimetry]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1429-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Rutsch, M.]]></dc:creator>
<dc:creator><![CDATA[Geipel, G.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1429-1</dc:identifier>
<dc:title><![CDATA[Zeitaufgelöste Laserinduzierte Fluoreszenzspektroskopie mit ultrakurzen Pulsen: Experimentelles Setup und Anwendungsbeispiele]]></dc:title>
<dc:source><![CDATA[Poster, GDCh-Tagung-Anakon]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[
Die zeitaufgelöste laserinduzierte Fluoreszenzspektroskopie (TRLFS) wird schon seit längerem als äußerst sensitive Methode zur Untersuchung der Komplexbildung von Radionukliden mit organischen und anorganischen Liganden eingesetzt. Hier sind insbesondere Untersuchungen an Uran(VI) und Cm(III) mit Huminsäuren zu nennen.  Jedoch sind die bisher angewandte TRLFS-Techniken mit Anregungspulsen im Nanosekundenbereich nur auf Radionuklide mit Fluoreszenzeigenschaften beschränkt /1/. Die
Entwicklung und Anwendung einer TRLFS mit ultrakurzen Anregungspulsen, d.h. mit Pulsen im Pico- und  emtosekundenbereich, eröffnet die Möglichkeit die Komplexbildung von nichtfluoreszierenden, umweltrelevanten Radionukliden, wie z. B. Neptunium, mit organischen Liganden über die Veränderung der Fluoreszenz-eigenschaften der Liganden zu untersuchen.
Ein erster Schritt für die Anwendung der TRLFS mit ultrakurzen Pulsen besteht im Aufbau eines solchen Lasersystem. Das neue Rossendorfer Lasersystem nutzt einen zweifach verstärkten Puls mit einer Pulsdauer von 130 fs eines mode-locked Ti:Sapphire Oszillators als Anregungspuls /2/. Die Auswahl der optimalen Anregungswellenlänge erfolgt über ein durchstimmbares  estkörperlasersystem (OPA-System) zwischen 250 nm und 10 µm. Das Fluoreszenzlicht der Probe wird direkt in einen
Gitterspektrographen eingekoppelt, die Detektion des Fluoreszenzsignals erfolgt mit einer intensivierten CCD Kamera. 
Zuerst wurden die Fluoreszenzeigenschaften (Fluoreszenzlebensdauer, Fluoreszenzintensität und -spektrum) von verschiedenen Huminsäuren untersucht. Dabei wurden die Probenparameter (pH-Wert, Konzentration,Ionenstärke) und verschiedene Systemparameter, wie z.B. Anregungswellenlänge, variiert. Das mit der bisherigen Lasertechnik sehr gut charakterisierte Komplexsystem Uran(VI) und Huminsäure /3/ wurde für eine Validierung des Femtosekunden-Lasersystems verwendet. Die
Ergebnisse der vergleichenden Messungen werden diskutiert.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1431-2</identifier>
<datestamp>2025-02-13</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kaptari, L. P.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Dorkin, S. M.]]></dc:creator>
<dc:creator><![CDATA[Semikh, S. S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1431-2</dc:identifier>
<dc:title><![CDATA[Pion Exchange Effects in Elastic Backward Proton-Deuteron Scattering]]></dc:title>
<dc:source><![CDATA[Few-Body Systems 27, 189-206 (1999)]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Abstract. 
The elastic backward proton-deuteron scattering is analyzed within a covariant approach based on the Bethe-Salpeter equation with realistic meson-exchange interaction. Contributions of the one-nucleon and one-pion exchange mechanisms to the cross section and polarization observables are investigated in explicit form. Results of numerical calculations for the cross section, tensor analyzing power and spin transfers are presented. The one-pion exchange contribution is essential for describing the spin averaged cross section, while in polarization observables it is found to be less important.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1007/s006010050129]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1431-2</dc:relation>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<header>
<identifier>HZDR:PUBLDB:1431-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Kaptari, L. P.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Dorkin, S. M.]]></dc:creator>
<dc:creator><![CDATA[Semikh, S. S.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1431-1</dc:identifier>
<dc:title><![CDATA[Pion Exchange Effects in Elastic Backward Proton-Deuteron Scattering]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-246 Januar 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Abstract. 
The elastic backward proton-deuteron scattering is analyzed within a covariant approach based on the Bethe-Salpeter equation with realistic meson-exchange interaction. Contributions of the one-nucleon and one-pion exchange mechanisms to the cross section and polarization observables are investigated in explicit form. Results of numerical calculations for the cross section, tensor analyzing power and spin transfers are presented. The one-pion exchange contribution is essential for describing the spin averaged cross section, while in polarization observables it is found to be less important.]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1431-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:14297-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Melikhova, O.]]></dc:creator>
<dc:creator><![CDATA[Cizek, J.]]></dc:creator>
<dc:creator><![CDATA[Kuriplach, J.]]></dc:creator>
<dc:creator><![CDATA[Prochazka, I.]]></dc:creator>
<dc:creator><![CDATA[Cieslar, M.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14297-1</dc:identifier>
<dc:title><![CDATA[Positron annihilation study of vacancies in FeAl based alloys]]></dc:title>
<dc:source><![CDATA[Intermetallics 18(2010)-598]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[In the present contribution, high-resolution positron lifetime and coincidence Doppler broadening spectroscopies are used to characterize defects in Fe76Al24 and Fe72Al28 alloys. In order to facilitate defect identification, we also perform a theoretical study of basic vacancy-like defects in three phases of the FeAl system: ordered, short-range ordered, and disordered. Positron characteristics, like positron lifetime, positron binding energy to defects, high-momentum parts of Doppler broadening curves and specific trapping rates, are calculated for various defect configurations. The results are discussed in the context of experimental data obtained here and available in literature.]]></dc:description>
<dc:subject><![CDATA[Iron aluminides, based on Fe3Al]]></dc:subject>
<dc:subject><![CDATA[Point defects]]></dc:subject>
<dc:subject><![CDATA[Ab-initio calculations]]></dc:subject>
<dc:subject><![CDATA[Non-destructive evaluation]]></dc:subject>
<dc:subject><![CDATA[Positron characteristics]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14297-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:2109-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Herzberg, R.-D.]]></dc:creator>
<dc:creator><![CDATA[Brentano, P.]]></dc:creator>
<dc:creator><![CDATA[Rotter, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2109-1</dc:identifier>
<dc:title><![CDATA[Evidence for trapping and collectivization of resonances at strong coupling]]></dc:title>
<dc:source><![CDATA[Nuclear Physics A 556, (1993), 107-114]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2109-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2110-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Rotter, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2110-1</dc:identifier>
<dc:title><![CDATA[Selforganization and chaos in the nuclear system]]></dc:title>
<dc:source><![CDATA[in: Dynamical Systems and Chaos, Vol. 2 (Physics), ed. By Y. Aizawa, S. Saito and K. Shiraiwa, World Scientific 1995, pp. 550-553]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/book</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:book</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2110-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:3076-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kliem, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3076-1</dc:identifier>
<dc:title><![CDATA[3D flow simulation for a reactor core modelled as porous body by CFX - 4.2 code]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik 2000, Bonn, 23.-25. Mai 2000, Tagungsbericht S. 69-73]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[In this paper, the 3D flow simulation in a reactor core with asymmetrical power distribution and low mass flow rate carried out by CFX - 4.2 code is presented.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:3076-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kliem, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3076-7</dc:identifier>
<dc:title><![CDATA[3D flow simulation for a reactor core modelled as porous body by CFX - 4.2 code]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik 2000, Bonn, 23.-25. Mai 2000, Tagungsbericht S. 69-73]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[In this paper, the 3D flow simulation in a reactor core with asymmetrical power distribution and low mass flow rate carried out by CFX - 4.2 code is presented.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-3076-7</dc:relation>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1545-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Mönch, I.]]></dc:creator>
<dc:creator><![CDATA[Stephan, I.]]></dc:creator>
<dc:creator><![CDATA[Köthe, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1545-2</dc:identifier>
<dc:title><![CDATA[High-purity niobium for neutron activation detectors]]></dc:title>
<dc:source><![CDATA[Tagung Ultra High Purity Base 1999 Metals, Sendai, Japan]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[High-purity niobium has successfully been used as neutron detector material in advanced neutron dosimetry. Reliable and accurate neutron dosimetry measurements  are needed to control the neutron load of the reactor pressure vessel (RPV) during its operation. Neutrons-irradiation of the RPV material causes an embrittlement of the ferritic steel. The effect is highly safety-relevant and must, thus, be monitored. It is standard to use a set of several materials with different neutron activation or spallation reactions. An cases of the niobium detectors the nuclear reaction one makes use of 93Nb(n,n`)93mNb reaction. It is specially favourable because the energy dependence of this reaction is similar to the  energy dependence of the damage function of the RPV material. Furthermore, the half-life is long (16.1 years) and results in a nearly constant weighting over the reactor cycle. Therefore, the decay correction is only small in comparison with other detectors.
Niobium of low purity is not appropriate for this purpose. Impurities can affect additional activation reactions. Especially detrimental is tantalum. The neutron capture of 181Ta leads to 182Ta resulting in high energy gamma lines (1121,1122 keV) and  added excitation of the detected 16 and 18 keV niobium lines. The correction of these effects is difficult and yields additional errors.
The requirements of the purity are strict: a good niobium detector must not have a Ta concentration of more than 1 ppm.
The niobium was produced by a technology which consists of an electrolytic refining, melting processes and mechanical treatment. In the cathodic niobium (electrolysis conditions: T = 750°C, j=0.4 mA/mm²) the so-called "problematic element" Ta could not be detected by instrumental neutron-activation analysis (cTa <<1 at.ppm). 
With the niobium produced in this way, the neutron fluence at the VVER-type RPVs of the nuclear power plants in Greifswald (Germany), Rovno, and Balakovo (Russia) were determined. Int ...]]></dc:description>
<dc:subject><![CDATA[High purity niobium]]></dc:subject>
<dc:subject><![CDATA[neutron detector]]></dc:subject>
<dc:subject><![CDATA[electrolytic refining]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1545-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1545-3</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Mönch, I.]]></dc:creator>
<dc:creator><![CDATA[Stephan, I.]]></dc:creator>
<dc:creator><![CDATA[Köthe, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1545-3</dc:identifier>
<dc:title><![CDATA[High-purity niobium for neutron activation detectors]]></dc:title>
<dc:source><![CDATA[Material Transactions JIM Vol. 41, 1 (2000) 1ff]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[High-purity niobium has successfully been used as neutron detector material in advanced neutron dosimetry. Reliable and accurate neutron dosimetry measurements  are needed to control the neutron load of the reactor pressure vessel (RPV) during its operation. Neutrons-irradiation of the RPV material causes an embrittlement of the ferritic steel. The effect is highly safety-relevant and must, thus, be monitored. It is standard to use a set of several materials with different neutron activation or spallation reactions. An cases of the niobium detectors the nuclear reaction one makes use of 93Nb(n,n`)93mNb reaction. It is specially favourable because the energy dependence of this reaction is similar to the  energy dependence of the damage function of the RPV material. Furthermore, the half-life is long (16.1 years) and results in a nearly constant weighting over the reactor cycle. Therefore, the decay correction is only small in comparison with other detectors.
Niobium of low purity is not appropriate for this purpose. Impurities can affect additional activation reactions. Especially detrimental is tantalum. The neutron capture of 181Ta leads to 182Ta resulting in high energy gamma lines (1121,1122 keV) and  added excitation of the detected 16 and 18 keV niobium lines. The correction of these effects is difficult and yields additional errors.
The requirements of the purity are strict: a good niobium detector must not have a Ta concentration of more than 1 ppm.
The niobium was produced by a technology which consists of an electrolytic refining, melting processes and mechanical treatment. In the cathodic niobium (electrolysis conditions: T = 750°C, j=0.4 mA/mm²) the so-called "problematic element" Ta could not be detected by instrumental neutron-activation analysis (cTa <<1 at.ppm). 
With the niobium produced in this way, the neutron fluence at the VVER-type RPVs of the nuclear power plants in Greifswald (Germany), Rovno, and Balakovo (Russia) were determined. Int ...]]></dc:description>
<dc:subject><![CDATA[High purity niobium]]></dc:subject>
<dc:subject><![CDATA[neutron detector]]></dc:subject>
<dc:subject><![CDATA[electrolytic refining]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:14201-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Vinnichenko, M.]]></dc:creator>
<dc:creator><![CDATA[Cornelius, S.]]></dc:creator>
<dc:creator><![CDATA[Rogozin, A.]]></dc:creator>
<dc:creator><![CDATA[Shevchenko, N.]]></dc:creator>
<dc:creator><![CDATA[Gago, R.]]></dc:creator>
<dc:creator><![CDATA[Kolitsch, A.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14201-1</dc:identifier>
<dc:title><![CDATA[Properties, structure and phase composition of transparent conductive oxide thin films grown by magnetron sputtering]]></dc:title>
<dc:source><![CDATA[Invited talk during visit to "Next Energy" EWE-Forschungszentrum für Energietechnologie e.V., 10.-11.02.2010, Oldenburg, Germany]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Understanding of the mechanisms of donor impurity incorporation, its electrical activation and charge carrier transport in transparent conducting oxides (TCO) is required for further improvement of functionality of this class of materials. The present work focuses on investigation of indium oxide (IO), Sn-doped indium oxide (ITO), ZnO, and ZnO:Al (AZO) films grown by reactive pulsed magnetron sputtering (RPMS) with a precise control of the oxygen partial pressure at substrate temperatures, Ts, ranging from RT to 550°C. In order to explore potential advantages of RPMS, the relationship between the deposition parameters and structure, phase composition and physical properties of these TCOs was investigated. The films were characterized by spectroscopic ellipsometry, Hall effect measurements, X-ray diffraction (XRD) and, in case of ZnO and AZO films, by X-ray absorption near edge structures (XANES). The Sn concentration in ITO was determined by Auger analysis, while the Al concentration in ZnO matrix was estimated by elastic recoil detection analysis and Rutherford back scattering.
The comparison of the real-time behavior of the IO and ITO film structure and electrical properties during annealing provides a direct evidence of Sn donor activation (with an estimated efficiency of 40%) in ITO due to amorphous-to-crystalline transition. The ITO film crystallinity always improves with increasing substrate temperature or during isothermal annealing, with the electrical resistivity decreasing. In contrast, the electrical resistivity of AZO films shows a clear minimum at an optimum substrate temperature (200-400 °C), which depends on metal/oxygen flux ratio and correlates with a maximum in crystallinity (grain size). In this case, the highest mobility value of 46 cm2 V-1 s-1 is comparable to the best values achieved in AZO films grown by less cost-efficient techniques. This value is achieved at the free electron density of 6x10<sup>20</sup> cm-3 which corresponds to maximum ~30% electrical activation of Al impurity. At higher temperatures, the AZO electrical properties and crystalline quality deteriorate abruptly according to the following mechanism. Increasing Ts above its optimum value leads to a higher Al concentration in the AZO films, which exceeds the solubility limit and triggers the formation of an insulating metastable homologous (ZnO)3Al2O3 phase. This phase impedes crystal growth and causes a significant increase of free electron scattering both at grain boundaries and inclusions of this phase. In order to enable the growth of low-resistivity AZO films in a wider range of TS, lower metal/oxygen flux ratios should be used. The proposed approach to minimizing the influence of this undesirable phase may also be applied to other deposition methods of AZO involving high-energy particle bombardment.]]></dc:description>
<dc:subject><![CDATA[Al-doped ZnO]]></dc:subject>
<dc:subject><![CDATA[transparent conductive oxides]]></dc:subject>
<dc:subject><![CDATA[electrical properties]]></dc:subject>
<dc:subject><![CDATA[optical properties]]></dc:subject>
<dc:subject><![CDATA[phase composition]]></dc:subject>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:1549-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schneider, C.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1549-1</dc:identifier>
<dc:title><![CDATA[Two-phase flow in the anode chamber of alkaline chloride electrolysis cells]]></dc:title>
<dc:source><![CDATA[ECCE 2 - Second European Congress of Chemical Engineering - Montpellier 05.-07.10.1999, paper CDROM 09170010.pdf.]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[In membrane electrolysis cells a layer of spherical foam was found grow-ing with increasing performance. At the top a transition to cell foam oc-curs. Near the cell bottom the boundary layer of gas fraction and velocity at the electrode was measured. The velocity boundary layer changes from laminar to turbulent.]]></dc:description>
<dc:subject><![CDATA[gas fraction distribution]]></dc:subject>
<dc:subject><![CDATA[foam]]></dc:subject>
<dc:subject><![CDATA[bubble size]]></dc:subject>
<dc:subject><![CDATA[liquid circulation]]></dc:subject>
<dc:subject><![CDATA[hydrogen peroxide decomposition]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1549-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1549-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schneider, C.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1549-7</dc:identifier>
<dc:title><![CDATA[Two-phase flow in the anode chamber of alkaline chloride electrolysis cells]]></dc:title>
<dc:source><![CDATA[ECCE 2 - Second European Congress of Chemical Engineering - Montpellier 05.-07.10.1999, paper CDROM 09170010.pdf.]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[In membrane electrolysis cells a layer of spherical foam was found grow-ing with increasing performance. At the top a transition to cell foam oc-curs. Near the cell bottom the boundary layer of gas fraction and velocity at the electrode was measured. The velocity boundary layer changes from laminar to turbulent.]]></dc:description>
<dc:subject><![CDATA[gas fraction distribution]]></dc:subject>
<dc:subject><![CDATA[foam]]></dc:subject>
<dc:subject><![CDATA[bubble size]]></dc:subject>
<dc:subject><![CDATA[liquid circulation]]></dc:subject>
<dc:subject><![CDATA[hydrogen peroxide decomposition]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1549-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1550-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1550-1</dc:identifier>
<dc:title><![CDATA[[Re(NBH2SBH3)(Me2PhP)(Et2dtc)]2 - A novel rhenium dimer with the unusual bridging (NBH2SBH3)4- ligand]]></dc:title>
<dc:source><![CDATA[Communication in Inorg. Chem. Communications]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[
The title compound is formed during the reaction of [ReN(Me2PhP)(Et2dtc)2] (Me2PhP = dimethylphenylphosphine, Et2dtc- = diethyldithiocarbamate) with excess BH3 in tetrahydrofurane. Two ReV atoms are linked by two (NBH2SBH3)4- units which act as three-dentate ligand via N, S and H forming an 8-membered metallacycle with additional co-ordination of a hydrido H atom trans to the nitrogen atom. The ReN multiple bond length is 1.70(1) Å which is only slightly longer than in the starting compound [ReN(Me2PhP)(Et2dtc)2] (1.666(6) Å).]]></dc:description>
<dc:subject><![CDATA[Keywords: Rhenium complexes]]></dc:subject>
<dc:subject><![CDATA[Nitrido bridges]]></dc:subject>
<dc:subject><![CDATA[Diborinyl sulfide]]></dc:subject>
<dc:subject><![CDATA[Crystal structure]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1550-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:1560-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hennig, C.]]></dc:creator>
<dc:creator><![CDATA[Nolze, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1560-1</dc:identifier>
<dc:title><![CDATA[Characterization of the preferred orientation in EXAFS-samples]]></dc:title>
<dc:source><![CDATA[NEA-Conference, Genoble 1998, NEA-Report]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Preferred orientation in powder samples influences extendet  X-ray absorption fine structure (EXAFS) measurements due to the polarization of synchrotron radiation. The polarization effect at the uranium LIII edge EXAFS and the analysis of preferred orientation is demonstrated using the natural mineral metatorbernite. For simple textures an X-ray diffraction measurement in Bragg-Brentano geometry allows to determine the crystallite orientation basing on a full pattern refinement including a preferred orientation model according to March-Dollase.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1560-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:1564-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pham, M. T.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Steiner, G.]]></dc:creator>
<dc:creator><![CDATA[Oswald, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1564-1</dc:identifier>
<dc:title><![CDATA[Surface sensitivity of ion implanted titanium to hydroxyapatite formation]]></dc:title>
<dc:source><![CDATA[Journal of Materials Science Letters  19 (2000) 313]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Titanium surfaces containing CaO and P2O5 were prepared by ion implantation of Ca and P and subsequent oxidation. Their reactivity to form hydroxyapatite was examined by in situ microscopically recording the surface mineralization in a simulated body fluid. The ion implanted surfaces exhibit enhanced mineralization by inducing heterogeneous nucleation, growth, and proliferation of hydroxyapatite, relative to a control sample of pure Ti. The surface induced reactivity was shown to relate to the mineral precursors Ca2+ and (HPO4)2- directly supplied from the surface and the substrate-mediated nucleation by hydroxylated surface TiO2.]]></dc:description>
<dc:subject><![CDATA[biomaterials]]></dc:subject>
<dc:subject><![CDATA[titanium]]></dc:subject>
<dc:subject><![CDATA[hydroxyapatite]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1564-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1564-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pham, M. T.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Steiner, G.]]></dc:creator>
<dc:creator><![CDATA[Oswald, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1564-2</dc:identifier>
<dc:title><![CDATA[Surface sensitivity of ion implanted titanium to hydroxyapatite formation]]></dc:title>
<dc:source><![CDATA[Mater. Sci. Lett. 19 (2000) 443-445]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Titanium surfaces containing CaO and P2O5 were prepared by ion implantation of Ca and P and subsequent oxidation. Their reactivity to form hydroxyapatite was examined by in situ microscopically recording the surface mineralization in a simulated body fluid. The ion implanted surfaces exhibit enhanced mineralization by inducing heterogeneous nucleation, growth, and proliferation of hydroxyapatite, relative to a control sample of pure Ti. The surface induced reactivity was shown to relate to the mineral precursors Ca2+ and (HPO4)2- directly supplied from the surface and the substrate-mediated nucleation by hydroxylated surface TiO2.]]></dc:description>
<dc:subject><![CDATA[biomaterials]]></dc:subject>
<dc:subject><![CDATA[titanium]]></dc:subject>
<dc:subject><![CDATA[hydroxyapatite]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1564-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:14544-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Planer‐Friedrich, B.]]></dc:creator>
<dc:creator><![CDATA[Suess, E.]]></dc:creator>
<dc:creator><![CDATA[Scheinost, A. C.]]></dc:creator>
<dc:creator><![CDATA[Wallschläger, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14544-1</dc:identifier>
<dc:title><![CDATA[Arsenic speciation in sulfidic waters: Consolidation of contradictory spectroscopic and chromatographic evidence]]></dc:title>
<dc:source><![CDATA[Analytical Chemistry 82(2010)24, 10228-10235]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[In recent years, analytical methods have been developed that have demonstrated that soluble arsenic‐sulfur species constitute a major fraction of dissolved arsenic in sulfidic waters. However, an intense debate is going on about the exact chemical nature of these compounds, since X‐ray absorption spectroscopy (XAS) data generated at higher (mmol/L) concentrations suggest the presence of (oxy)thioarsenites in such waters, while ion chromatographic (IC) and mass spectroscopic data at lower (μmol/L to nmol/L) concentrations indicate the presence of (oxy)thioarsenates. In this contribution, we connect and explain these two apparently different types of results. We show by XAS that thioarsenites are the primary reaction products of arsenite and sulfide in geochemical model experiments in the complete absence of oxygen. However, thioarsenites are extremely instable towards oxidation, and convert rapidly into thioarsenates when exposed to atmospheric oxygen, e.g. while waiting for analysis on the chromatographic autosampler. This problem can only be eliminated when the entire chromatographic process is conducted inside a glove box. We also show that thioarsenites are instable towards sample dilution, which is commonly employed prior to chromatographic analysis when ultra‐sensitive detectors like ICP‐MS are used. This instability has two main reasons: if pH changes during dilution, then equilibria between individual arsenic‐sulfur species rearrange rapidly due to their different stability regions within the pH range, and if pH is kept constant during dilution, then this changes the ratio between OH‐ and SH‐ in solution, which in turn shifts the underlying speciation equilibria. This problem is avoided by analyzing samples undiluted. Our studies show that thioarsenites appear as thioarsenates in IC analyses if oxygen is not excluded completely, and as arsenite if samples are diluted in alkaline anoxic medium. This also points out that thioarsenites are necessary intermediates in the formation of thioarsenates.]]></dc:description>
<dc:subject><![CDATA[arsenic]]></dc:subject>
<dc:subject><![CDATA[XAFS]]></dc:subject>
<dc:subject><![CDATA[IC-ICP-MS]]></dc:subject>
<dc:subject><![CDATA[speciation]]></dc:subject>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Weier, T.]]></dc:creator>
<dc:creator><![CDATA[Fey, U.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Lielausis, O.]]></dc:creator>
<dc:creator><![CDATA[Platacis, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1553-1</dc:identifier>
<dc:title><![CDATA[Electromagnetic flow control for drag reduction and separation prevention]]></dc:title>
<dc:source><![CDATA[Proceedings of the 11th European Drag Reduction Working Meeting, Prague, Sept. 15-17 1999, pp.84-85]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The flow of an electrically conducting fluid like sea-water can be 
controlled by electromagnetic forces, i.e.~Lorentz-forces. These forces 
may be generated by an appropriate chosen arrangement of permanent 
magnets and electrodes. A strip like geometry as shown in fig. 1  
produces a Lorentz-force with a streamwise component only. In a first 
approximation this force is independent of the spanwise coordinate z and
decays exponentially with increasing wall distance y [1]. The successful 
application of a surface parallel Lorentz force in streamwise direction
to control the flow around a cylinder has been demonstrated in 
[2]. We consider here the action of such a force on a flat plate
boundary layer up to Re=9*10^5 and the flow around a NACA-0017-like
hydrofoil with Re<8*10^4. The experiments were carried out in a
saltwater facility and accompanied by flow visualizations in an open
channel with sodium hydroxide as the working fluid.

>From the boundary layer equations with the Lorentz-force term one gains
a characteristic parameter Z (Tsinober--Shtern parameter [1]) describing 
the ratio of electromagnetic to viscous forces. If this parameter equals 
one, the boundary layer equations have a solution with an exponential 
flow profile similar to the asymptotic suction profile. A considerable 
transition delay and therefore drastic drag reduction should be expected 
from such a boundary layer [3], because the exponential profile has 
proven to be much more stable than the Blasius one. Force balance 
measurements on a flat plate show indeed the reduction of total drag by 
more than 80\% (see fig. 2). However, this drag reduction is due to the 
momentum added to the flow by the body force. The skin friction on the 
contrary is even slightly increased, as can be concluded from the 
velocity profiles in fig. 2. The reason for this behavior
lies in the real force distribution and probably the high turbulence level
of the environment. It is  ...]]></dc:description>
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<dc:creator><![CDATA[Weier, T.]]></dc:creator>
<dc:creator><![CDATA[Fey, U.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Lielausis, O.]]></dc:creator>
<dc:creator><![CDATA[Platacis, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1553-7</dc:identifier>
<dc:title><![CDATA[Electromagnetic flow control for drag reduction and separation prevention]]></dc:title>
<dc:source><![CDATA[Proceedings of the 11th European Drag Reduction Working Meeting, Prague, Sept. 15-17 1999, pp.84-85]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The flow of an electrically conducting fluid like sea-water can be 
controlled by electromagnetic forces, i.e.~Lorentz-forces. These forces 
may be generated by an appropriate chosen arrangement of permanent 
magnets and electrodes. A strip like geometry as shown in fig. 1  
produces a Lorentz-force with a streamwise component only. In a first 
approximation this force is independent of the spanwise coordinate z and
decays exponentially with increasing wall distance y [1]. The successful 
application of a surface parallel Lorentz force in streamwise direction
to control the flow around a cylinder has been demonstrated in 
[2]. We consider here the action of such a force on a flat plate
boundary layer up to Re=9*10^5 and the flow around a NACA-0017-like
hydrofoil with Re<8*10^4. The experiments were carried out in a
saltwater facility and accompanied by flow visualizations in an open
channel with sodium hydroxide as the working fluid.

>From the boundary layer equations with the Lorentz-force term one gains
a characteristic parameter Z (Tsinober--Shtern parameter [1]) describing 
the ratio of electromagnetic to viscous forces. If this parameter equals 
one, the boundary layer equations have a solution with an exponential 
flow profile similar to the asymptotic suction profile. A considerable 
transition delay and therefore drastic drag reduction should be expected 
from such a boundary layer [3], because the exponential profile has 
proven to be much more stable than the Blasius one. Force balance 
measurements on a flat plate show indeed the reduction of total drag by 
more than 80\% (see fig. 2). However, this drag reduction is due to the 
momentum added to the flow by the body force. The skin friction on the 
contrary is even slightly increased, as can be concluded from the 
velocity profiles in fig. 2. The reason for this behavior
lies in the real force distribution and probably the high turbulence level
of the environment. It is  ...]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Knigth, M. P.]]></dc:creator>
<dc:creator><![CDATA[Brohan, P.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:creator><![CDATA[Finnemann, H.]]></dc:creator>
<dc:creator><![CDATA[Hüsken, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1775-1</dc:identifier>
<dc:title><![CDATA[Comparsion of Rod-Ejection Transient Calculations in Hexagonal-Z Geometry]]></dc:title>
<dc:source><![CDATA[International Conference on Mathematics and Computations, Reactor Physics and Environment Analysis, Portland, Oregon/USA, April 30 - May 5, 1995, Proc. Vol. 2, pp. 1248 - 1258]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[This Paper proposes a set of 3-dimensional benchmark rod ejection problems for a VVER reactor, based on the wellknown NEACRP PWR rod-ejection problems defined by Siemens/KWU. Predictions for these benchmarks deriving using three hexagonal-z nodal transient codes, the PANTER code of Nuclear Electric, the HEXTIME code of Siemens/KWU and the DYN3D code of FZ-Rossendorf are presented and compared.]]></dc:description>
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<dc:creator><![CDATA[Knigth, M. P.]]></dc:creator>
<dc:creator><![CDATA[Brohan, P.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:creator><![CDATA[Finnemann, H.]]></dc:creator>
<dc:creator><![CDATA[Hüsken, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1775-7</dc:identifier>
<dc:title><![CDATA[Comparsion of Rod-Ejection Transient Calculations in Hexagonal-Z Geometry]]></dc:title>
<dc:source><![CDATA[International Conference on Mathematics and Computations, Reactor Physics and Environment Analysis, Portland, Oregon/USA, April 30 - May 5, 1995, Proc. Vol. 2, pp. 1248 - 1258]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[This Paper proposes a set of 3-dimensional benchmark rod ejection problems for a VVER reactor, based on the wellknown NEACRP PWR rod-ejection problems defined by Siemens/KWU. Predictions for these benchmarks deriving using three hexagonal-z nodal transient codes, the PANTER code of Nuclear Electric, the HEXTIME code of Siemens/KWU and the DYN3D code of FZ-Rossendorf are presented and compared.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1777-1</identifier>
<datestamp>2019-03-04</datestamp>
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</header>
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1777-1</dc:identifier>
<dc:title><![CDATA[Post Test Calculations to 11% Break LOCA Experiments in the Integral Test Facility ISB-VVER Using the Thermalhydraulic Code ATHLET]]></dc:title>
<dc:source><![CDATA[Proc. Jahrestagung Kerntechnik, Nürnberg, 16. - 18. Mai 1995, pp. 83 - 87]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[The considered test was a break on the upper plenum with different modes of emergency core cooling. The reference case was the non-availability of emergency cooling. Injecting the emergency coolant into the cold leg, no increasing of rod cladding temperatures was observed, but natural circulation instabilities occurred. Injecting the cooling into the hot leg, the cooling situation was getting worse. Due to the injected cold emergency coolant, the fluid density in the discharge volume was enhanced and the break mass flow increased. The observed events in the test were reproduced by the code with good agreement

]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1777-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1777-2</dc:identifier>
<dc:title><![CDATA[Post Test Calculations to 11% Break LOCA Experiments in the Integral Test Facility ISB-VVER Using the Thermalhydraulic Code ATHLET]]></dc:title>
<dc:source><![CDATA[Conference "Thermopysical Aspects of WWER-Type Reactor Safety", Obninsk, Russia, Nov. 1995, Proc. Vol. 2, pp. 150 - 154]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[The considered test was a break on the upper plenum with different modes of emergency core cooling. The reference case was the non-availability of emergency cooling. Injecting the emergency coolant into the cold leg, no increasing of rod cladding temperatures was observed, but natural circulation instabilities occurred. Injecting the cooling into the hot leg, the cooling situation was getting worse. Due to the injected cold emergency coolant, the fluid density in the discharge volume was enhanced and the break mass flow increased. The observed events in the test were reproduced by the code with good agreement

]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Maletti, R.]]></dc:creator>
<dc:creator><![CDATA[Ulrich, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1778-1</dc:identifier>
<dc:title><![CDATA[105 Mio. DM Zuschüsse - Energie-Förderung durch das SMWA]]></dc:title>
<dc:source><![CDATA[IHK Wirtschaftsdienst 6 (1995), H. 6, S. 20]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Maletti, R.]]></dc:creator>
<dc:creator><![CDATA[Ulrich, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1779-1</dc:identifier>
<dc:title><![CDATA[Energie-Förderung durch das Sächsische Staatsministerium für Wirschaft und Arbeit im Jahre 1994]]></dc:title>
<dc:source><![CDATA[Energieanwendung 44 (1995), H. 4, S. 50]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Maletti, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1780-1</dc:identifier>
<dc:title><![CDATA[Solaranlagen in Sachsen: eine Zwischenbilanz]]></dc:title>
<dc:source><![CDATA[Sonnenenergie und Wärmetechnik 1995, H. 5, S. 21]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Kolevzon, V.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
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<dc:title><![CDATA[Ligth scattering by different liquid surfaces]]></dc:title>
<dc:source><![CDATA[Lecture at: Fachtagung "Lasermethoden in der Strömungsmeßtechnik", Rostock, September 1995]]></dc:source>
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<dc:creator><![CDATA[Hatzopoulos, N.]]></dc:creator>
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<dc:creator><![CDATA[Siapkas, D. I.]]></dc:creator>
<dc:creator><![CDATA[Hemment, P. L. F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-894-1</dc:identifier>
<dc:title><![CDATA[Electrical and optical characterisation of double SIMOX structures formed by sequential high energy oxygen implantation into silicon]]></dc:title>
<dc:source><![CDATA[Microelectronic Engineering 28 (1995) pp.415-418]]></dc:source>
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<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
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<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1797-1</dc:identifier>
<dc:title><![CDATA[Prozeß- und Anlagendiagnostik]]></dc:title>
<dc:source><![CDATA[Ein Überblick über die Arbeiten des Institutes für Sicherheitsforschung, FZR, März 1995]]></dc:source>
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<dc:title><![CDATA[Einfluß von Orographie und Rauhigkeit auf das Windenergiepotential in ausgewählten Gebieten Sachsens]]></dc:title>
<dc:source><![CDATA[Diplomarbeit Technische Universität Dresden, Fakultät Maschinenwesen, Nr. 1549, 28.09.1995]]></dc:source>
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<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Eichhorn, F.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Henrion, W.]]></dc:creator>
<dc:creator><![CDATA[Albrecht, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-50-1</dc:identifier>
<dc:title><![CDATA[Electrical and Optical Properties of ß-FeSi2 after Co Implantation and Annealing]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods B 84 (1994), 172]]></dc:source>
<dc:date>1994</dc:date>
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<dc:creator><![CDATA[Nicht, E.-M.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Vostry, P.]]></dc:creator>
<dc:creator><![CDATA[Cieslar, M.]]></dc:creator>
<dc:creator><![CDATA[Blazek, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2337-1</dc:identifier>
<dc:title><![CDATA[Electrical resistivity and positron lifetime studies of the Cu-Mn system]]></dc:title>
<dc:source><![CDATA[Nukleonika 42 (1997) 175]]></dc:source>
<dc:date>1997</dc:date>
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<identifier>HZDR:PUBLDB:1799-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Beyer, M.]]></dc:creator>
<dc:creator><![CDATA[Carl, H.]]></dc:creator>
<dc:creator><![CDATA[Nowak, K.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Seidel, A.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1799-1</dc:identifier>
<dc:title><![CDATA[Unterstützung der ukrainischen Genehmigungsbehörde NARU beim Aufbau eines technischen Systems zur verbesserten betrieblichen Überwachung des KKW Saporoshje (4. Realisierungsstufe)]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-259 Mai 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Das vor zwei Jahren im KKW Saporoshje in Betrieb genommene System zur verbesserten betrieblichen Überwachung wurde an die Kiewer Zentrale der ukrainischen Aufsichtsbehörde angeschlossen. Dazu wurden die für den Anschluß und die Ausstattung dieser Zentrale in der ersten Ausbaustufe unbedingt erforderlichen technischen Mittel einvernehmlich spezifiziert, in Deutschland beschafft, im notwendigen Umfang erprobt, in die Ukraine überführt und dem Partner am Einsatzort unentgeltlich überlassen. Bei der Erprobung des Informationstransfers aus dem KKW Saporoshje in die Kiewer Zentrale wurde nachgewiesen, daß die von der ukrainischen Behörde gemietete Standleitung die notwendigen technischen Anforderungen erfüllt. Bei Funktionstests Mitte Januar 1998 wurden On-line-Daten aus dem Saporoger System der verbesserten betrieblichen Überwachung fehlerfrei nach Kiew übertragen. 
Ferner sind der ukrainischen Seite zum Anschluß des KKW Rovno an die Kiewer Zentrale die gleichen technischen Mittel zur Verfügung gestellt worden.]]></dc:description>
<dc:subject><![CDATA[betriebliche Überwachung]]></dc:subject>
<dc:subject><![CDATA[KKW Saporoshje]]></dc:subject>
<dc:subject><![CDATA[KKW Rovno]]></dc:subject>
<dc:subject><![CDATA[ukrainische Kernkraftwerke]]></dc:subject>
<dc:subject><![CDATA[Schutzziele]]></dc:subject>
<dc:subject><![CDATA[Kontrollaufgaben]]></dc:subject>
<dc:subject><![CDATA[Betriebssicherheit von Kernkraftwerken]]></dc:subject>
<dc:subject><![CDATA[WWER-1000/W-320]]></dc:subject>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
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<identifier>HZDR:PUBLDB:1800-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Beyer, M.]]></dc:creator>
<dc:creator><![CDATA[Carl, H.]]></dc:creator>
<dc:creator><![CDATA[Kriks, J.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1800-1</dc:identifier>
<dc:title><![CDATA[Unterstützung der ukrainischen Genehmigungs- und Aufsichtsbehörde bei der Einrichtung einer verbesserten betrieblichen Überwachung für das KKW Rovno (5. Realisierungsstufe)]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-260 Mai 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[In Analogie zum Pilotprojekt für den 5. Block vom KKW Saporoshje - WWER-1000/W-320 - wurde für die beiden WWER-440/W-213 Blöcke vom KKW Rovno eine verbesserte betriebliche Überwachung eingerichtet. Dazu werden dem Vor-Ort-Inspektor am KKW Standort und der Aufsichtsbehörde in Kiew einmal pro Minute 55 aktuelle sicherheitsrelevante Parameter pro Block und 7 standortspezifische Parameter zur Erfassung und Bewertung mittels moderner technischer Mittel on-line zur Verfügung gestellt. Die zur Ausstattung des Arbeitsplatzes des Vor-Ort-Inspektors unbedingt benötigten Ausrüstungen wurden unter Berücksichtigung der aktuellen Anforderungen des KKW Rovno spezifiziert, beschafft und der ukrainischen Seite unentgeltlich überlassen. Bei Funktionstests Ende 1998/Anfang 1999 wurden Datensätze aus dem lokalen Rechnernetz des KKW Rovno fehlerfrei nach Kiew übertragen und auf einem Rechner im Informations- und Krisenzentrum in Form von Tabellen, Grafiken und Schemata dargestellt.]]></dc:description>
<dc:subject><![CDATA[betriebliche Überwachung von Kernkraftwerken]]></dc:subject>
<dc:subject><![CDATA[KKW Saporoshje]]></dc:subject>
<dc:subject><![CDATA[KKW Rovno]]></dc:subject>
<dc:subject><![CDATA[WWER-1000/W-320]]></dc:subject>
<dc:subject><![CDATA[WWER-440/W-213]]></dc:subject>
<dc:type>info:eu-repo/semantics/report</dc:type>
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<header>
<identifier>HZDR:PUBLDB:14318-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Helm, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14318-1</dc:identifier>
<dc:title><![CDATA[The basic physics of intersubband transitions  from the simple to the subtle]]></dc:title>
<dc:source><![CDATA[International Quantum Cascade Lasers School & Workshop, 30.08.-03.09.2010, Florenz, Italien]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[I will describe the basic properties of intersubband transitions in quantum wells, partly along the lines of the now ten-years-old review paper [1]. I will proceed from the very basic to the discussion of some more specific systems, like superlattices or transitions within the valence band, and to some recently discovered, rather subtle effects.
 An interesting interplay is found with transitions between shallow impurity states, which becomes particularly striking in superlattices and coupled quantum wells [2]. Based on a calculation that treats the heterostructure potential and the random-impurity potential on the same footing [3], we can successfully explain or re-interpret some old, hitherto poorly understood data (see Fig. 1). 
Another subtle effect emerges, if intersubband spectra are recorded using time-domain terahertz spectroscopy, i.e. fully resolving the phase of the electric field. We show that transmission and absorption spectra are not equivalent, and whereas the absorption line has a standard Lorentzian shape, the transmission spectrum exhibits a Fano-type lineshape (see Fig. 2). This has been explained with the influence of the so-called ponderomotive current [4].
Most of the more recent experimental work discussed here was performed mainly by Dominik Stehr and Martin Wagner (both FZD), most of the samples used were provided by Gottfried Strasser (TU Vienna) and his group, and for part of this work the collaboration with the theory group of Univ. Marburg (D. Golde, M. Kira, S. W. Koch) was indispensable.
[1] M. Helm, The basic physics of intersubband transitions, in Semiconductors and Semimetals, Vol. 62, p. 1-99 (2000). 
[2] D. Stehr, C. Metzner, M. Helm, T. Roch, and G. Strasser, Resonant impurity bands in semiconductor superlattices, Phys. Rev. Lett. 95, 257401 (2005). 
[3] D. Stehr, M. Helm, C. Metzner, and M. C. Wanke, Microscopic theory of impurity states in coupled quantum wells and superlattices, Phys. Rev. B 74, 085311 (2006).
[4] D. Golde, M. Wagner, D. Stehr, H. Schneider, M. Helm, A.M. Andrews, T. Roch, G. Strasser, M. Kira, and S.W. Koch: Fano signatures in the intersubband terahertz response of optically excited semiconductor quantum wells, Phys. Rev. Lett. 102, 127403 (2009).]]></dc:description>
<dc:subject><![CDATA[intersubband]]></dc:subject>
<dc:subject><![CDATA[quantum wells]]></dc:subject>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<dc:type>doc-type:lecture</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1432-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Hoppe, D.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1432-1</dc:identifier>
<dc:title><![CDATA[Modellbildung durch Auswertung von Fehlerdimensionen]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-244]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[
Betrachtet werden Prozesse, in denen Teilprozesse voneinander abgrenzbar sind, die unabhängig voneinander zur Komplexität des Prozeßmodellfehlers beitragen. Auf der Grundlage von Dimensionsbetrachtungen wird versucht, die zu den Teilprozessen gehörenden Teilmodelle, d.h. die Elemente der Modellstruktur des Prozesses einzeln zu bestimmen. Ein Gesamtmodell des Prozesses soll auf diese Weise zielgerichteter als mit herkömmlichen Methoden gebildet werden können. Zur qualitativen Erfassung des Modellfehlers wird anhand von Ansätzen aus der Dimensionsanalyse, einem Bestandteil der Ähnlichkeitstheorie, ein Fehlermodell definiert. Zur quantitativen Erfassung der Komplexität des Modellfehlers werden dimensionsähnliche Kenngrößen eingeführt, die von einer Variante der fraktalen Dimension, der Zirkel- oder Liniendimension ausgehen.


]]></dc:description>
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<identifier>HZDR:PUBLDB:1434-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Gabriel, F.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1434-1</dc:identifier>
<dc:title><![CDATA[Bericht der Herbsttagung der Studiengruppe für Elektronische Instrumentierung vom 28.-30. September 1998 im Forschungszentrum Jülich]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-242]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1436-1</dc:identifier>
<dc:title><![CDATA[Workshop Meßtechnik für stationäre und transiente Mehrphasenströmungen, 24.-25. September 1998 in Rossendorf]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-241]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1437-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1437-1</dc:identifier>
<dc:title><![CDATA[Institute of Safety Research; Annual Report 1997]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-238 October 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The report gives an overview on the scientific work of the Institute of Safety Research in 1997. ]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1448-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Leib, J.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1448-1</dc:identifier>
<dc:title><![CDATA[Forschungszentrum Rossendorf; Jahresbericht 1997]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-240]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:1555-1</identifier>
<datestamp>2025-01-15</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kotte, R.]]></dc:creator>
<dc:creator><![CDATA[Barz, H. W.]]></dc:creator>
<dc:creator><![CDATA[Neubert, W.]]></dc:creator>
<dc:creator><![CDATA[Plettner, C.]]></dc:creator>
<dc:creator><![CDATA[Wohlfarth, D.]]></dc:creator>
<dc:creator><![CDATA[Alard, J. P.]]></dc:creator>
<dc:creator><![CDATA[Andronic, A.]]></dc:creator>
<dc:creator><![CDATA[Averbeck, R.]]></dc:creator>
<dc:creator><![CDATA[Basrak, Z.]]></dc:creator>
<dc:creator><![CDATA[Bastid, N.]]></dc:creator>
<dc:creator><![CDATA[Bendarag, N.]]></dc:creator>
<dc:creator><![CDATA[Berek, G.]]></dc:creator>
<dc:creator><![CDATA[Caplar, R.]]></dc:creator>
<dc:creator><![CDATA[Cindro, N.]]></dc:creator>
<dc:creator><![CDATA[Crochet, P.]]></dc:creator>
<dc:creator><![CDATA[Devismes, A.]]></dc:creator>
<dc:creator><![CDATA[Dupieux, P.]]></dc:creator>
<dc:creator><![CDATA[Dzelalija, M.]]></dc:creator>
<dc:creator><![CDATA[Eskef, M.]]></dc:creator>
<dc:creator><![CDATA[Fodor, Z.]]></dc:creator>
<dc:creator><![CDATA[Gobbi, A.]]></dc:creator>
<dc:creator><![CDATA[Grishkin, Y.]]></dc:creator>
<dc:creator><![CDATA[Herrmann, N.]]></dc:creator>
<dc:creator><![CDATA[Hildenbrand, K. D.]]></dc:creator>
<dc:creator><![CDATA[Hong, B.]]></dc:creator>
<dc:creator><![CDATA[Kecskemeti, J.]]></dc:creator>
<dc:creator><![CDATA[Kim, Y. J.]]></dc:creator>
<dc:creator><![CDATA[Kirejczyk, M.]]></dc:creator>
<dc:creator><![CDATA[Korolija, M.]]></dc:creator>
<dc:creator><![CDATA[Kowalczyk, M.]]></dc:creator>
<dc:creator><![CDATA[Kress, T.]]></dc:creator>
<dc:creator><![CDATA[Kutsche, R.]]></dc:creator>
<dc:creator><![CDATA[Lebedev, A.]]></dc:creator>
<dc:creator><![CDATA[Lee, K. S.]]></dc:creator>
<dc:creator><![CDATA[Leifels, Y.]]></dc:creator>
<dc:creator><![CDATA[Manko, V.]]></dc:creator>
<dc:creator><![CDATA[Merlitz, H.]]></dc:creator>
<dc:creator><![CDATA[Moisa, D.]]></dc:creator>
<dc:creator><![CDATA[Nianine, A.]]></dc:creator>
<dc:creator><![CDATA[Pelte, D.]]></dc:creator>
<dc:creator><![CDATA[Petrovici, M.]]></dc:creator>
<dc:creator><![CDATA[Rami, F.]]></dc:creator>
<dc:creator><![CDATA[Reisdorf, W.]]></dc:creator>
<dc:creator><![CDATA[Schauenburg, B.]]></dc:creator>
<dc:creator><![CDATA[Schüll, D.]]></dc:creator>
<dc:creator><![CDATA[Seres, Z.]]></dc:creator>
<dc:creator><![CDATA[Sikora, B.]]></dc:creator>
<dc:creator><![CDATA[Sim, K. S.]]></dc:creator>
<dc:creator><![CDATA[Simion, V.]]></dc:creator>
<dc:creator><![CDATA[Siwek-Wilczynska, K.]]></dc:creator>
<dc:creator><![CDATA[Somov, A.]]></dc:creator>
<dc:creator><![CDATA[Stoicea, G.]]></dc:creator>
<dc:creator><![CDATA[Vasiliev, M. A.]]></dc:creator>
<dc:creator><![CDATA[Wagner, P.]]></dc:creator>
<dc:creator><![CDATA[Wisniewski, K.]]></dc:creator>
<dc:creator><![CDATA[Yang, J. T.]]></dc:creator>
<dc:creator><![CDATA[Yushmanov, Y.]]></dc:creator>
<dc:creator><![CDATA[Zhilin, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1555-1</dc:identifier>
<dc:title><![CDATA[On the Space-Time Difference of Proton and Composite Particle Emission in Central Heavy-Ion Reactions at 400 AMeV]]></dc:title>
<dc:source><![CDATA[The European Physical Journal A 6 (1999) 185-195]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Small-angle correlations of pairs of nonidentical light charged particles 
produced in central collisions of heavy ions 
in the A=100 mass region at a beam energy of 400 AMeV are investigated with the FOPI detector system at GSI Darmstadt. The difference of longitudinal correlation functions with the 
relative velocity parallel and anti-parallel to the center-of-mass velocity of the pair in the central source frame is studied. This method allows extracting the apparent 
space-time differences of the emission of the charged particles. Comparing the correlations with results of a final-state interaction model delivers quantitative estimates of these asymmetries. Time delays as short as 1 fm/c or - alternatively - source radius differences of a few tenth fm are resolved. 
The strong collective expansion of the participant zone introduces not only an apparent reduction of the source radius 
but also a modification of the emission times. After correcting for both effects a complete sequence of space-time emission points of p, d, t, 3He, alpha particles is presented for the first time.
]]></dc:description>
<dc:subject><![CDATA[Nuclear physics]]></dc:subject>
<dc:subject><![CDATA[Intermediate energy heavy-ion reactions]]></dc:subject>
<dc:subject><![CDATA[Multifragmentation]]></dc:subject>
<dc:subject><![CDATA[Fragment-fragment correlation]]></dc:subject>
<dc:subject><![CDATA[Final-state interaction]]></dc:subject>
<dc:subject><![CDATA[Radial flow]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.48550/arXiv.nucl-ex/9904007]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:1016-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Baraniak, L.]]></dc:creator>
<dc:creator><![CDATA[Thieme, M.]]></dc:creator>
<dc:creator><![CDATA[Funke, H.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1016-1</dc:identifier>
<dc:title><![CDATA[Verhalten des Radiums im Flutungsprozeß des Uranbergwerks Königstein]]></dc:title>
<dc:source><![CDATA[Wissenschaftliche Zeitschrift der TU-Dresden 46 (1997) Heft 6, S. 90-94]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The interaction of radium with characteristic sediments of the upper Saxon Elbe river valley was investigated with the
aim to provide key data for transport modelling within the framework of mining site restoration. Adsorption
measurements therefore were carried out on site-specific sediments (different kinds of sandstone, claystone and lime
marl) using (1) acidic mine water coming from sulfuric acid residues of the former in-situ leaching process, (2)
groundwater that is inflowing into the mine and (3) mixtures of both which simulates certain stages of the mine flooding process. The distribution ratios were determined by batch experiments using an eight-week equilibration at aquifer temperature (14 °C). Radium adsorption from acidic mine water onto different kinds of sandstone is characterized by high distribution ratios (3400 mL/g). When contacted with groundwater, the sorption is decreased more than 20-fold (60-180 mL/g). For claystone and lime marl the distribution ratios amount to 130 and 480 mL/g, respectively, and they are nearly constant in the mine flooding process. The main adsorption mechanisms on the leached sandstone and the clayey sediments were identified as coprecipitation and ion exchange, respectively. The long-term migration behaviour in the aquifers of the south-east Saxon Elbe basin was calculated on the basis of Hadermanns' equation, considering retardation, dispersion and radioactive decay.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:571-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Baraniak, L.]]></dc:creator>
<dc:creator><![CDATA[Thieme, M.]]></dc:creator>
<dc:creator><![CDATA[Funke, H.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Nindel, K.]]></dc:creator>
<dc:creator><![CDATA[Schreyer, J.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-571-1</dc:identifier>
<dc:title><![CDATA[Radium Sorption on Sandy and Clayey Sediments of the Upper Saxon Elbe River Valley]]></dc:title>
<dc:source><![CDATA[4 th International Conference on Nuclear and Radiochemistry, Saint Malo, France, Sept.8-13, 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The interaction of radium with characteristic sediments of the upper Saxon Elbe river valley was investigated with a two-fold aim: to provide key data for transport modelling within the framework of mining site restoration and to study the influence of barium-radium-sulfate coprecipitation on the radium adsorption behaviour. 
For this purpose sorption measurements were carried out on site-specific sediments (different kinds of sandstone, claystone and lime marl) using  (1) original low-mineralized groundwater of this area, (2) typical acidic mine water coming from sulfuric acid residues of a former in-situ leaching process (~3 g/L SO<SUB>4</SUB><SUP>2-</SUP>, pH _ 2.5) and  (3) groundwater which was contaminated by 2% mine water. The distribution ratios (R<SUB>d</SUB>) were determined by batch experiments using an 8 weeks' equilibration at aquifer temperature (14C).
<P>Radium sorption from pure and slightly contaminated groundwater onto limonite-rich turonian sandstone is characterized by relatively low distribution ratios (60-180 mL/g). When contacted with mine water, the sorption was enhanced by more than 20-fold compared to the pure and contaminated groundwaters. For the typical lime marl, the strongest sorption occured from the groundwater (390-520 mL/g) and a slightly reduced sorption took place from the acidic mine water. </P>
<P>In addition, the radium sorption was studied as a function of the Ba<SUP>2+</SUP> and SO<SUB>4</SUB><SUP>2-</SUP> concentration. The results were discussed in terms of the ion product and the solubility product. Conclusions were drawn regarding the predominant sorption mechanisms: coprecipitation, surface complexation and ion exchange.</P>
<P>The long-term migration behaviour in the aquifers of the south-east Saxon Elbe basin was calculated on the basis of Hadermanns' equation, considering convection, dispersion, retardation and radioactive decay. </P>]]></dc:description>
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<identifier>HZDR:PUBLDB:1556-1</identifier>
<datestamp>2025-02-05</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Schell, N.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Claußner, J.]]></dc:creator>
<dc:creator><![CDATA[Oehme, W.]]></dc:creator>
<dc:creator><![CDATA[Prokert, F.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Schlenk, R.]]></dc:creator>
<dc:creator><![CDATA[Pröhl, D.]]></dc:creator>
<dc:creator><![CDATA[Funke, H.]]></dc:creator>
<dc:creator><![CDATA[Eichhorn, F.]]></dc:creator>
<dc:creator><![CDATA[Betzl, M.]]></dc:creator>
<dc:creator><![CDATA[Dienel, S.]]></dc:creator>
<dc:creator><![CDATA[Brendler, V.]]></dc:creator>
<dc:creator><![CDATA[Denecke, M. A.]]></dc:creator>
<dc:creator><![CDATA[Krug, H.]]></dc:creator>
<dc:creator><![CDATA[Neumann, W.]]></dc:creator>
<dc:creator><![CDATA[Hüttig, G.]]></dc:creator>
<dc:creator><![CDATA[Reichel, P.]]></dc:creator>
<dc:creator><![CDATA[Strauch, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1556-1</dc:identifier>
<dc:title><![CDATA[ROBL - a CRG Beamline for Radiochemistry and Materials Research at the ESRF]]></dc:title>
<dc:source><![CDATA[Journal of Synchrotron Radiation, 6 (1999) 1076-1085]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The paper describes the Rossendorf Beamline (ROBL) built by the Forschungszentrum Rossendorf at the ESRF. ROBL comprises two different and independently operating experimental stations: a radiochemistry laboratory for X-ray absorption spectroscopy of non-sealed radioactive samples and a general purpose materials research station for X-ray diffraction and reflectometry mainly of thin films and interfaces modified by ion beam techniques. The radiochemistry set-up is worldwide an unique installation at a modern synchrotron radiation source.]]></dc:description>
<dc:subject><![CDATA[synchrotron radiation beamline]]></dc:subject>
<dc:subject><![CDATA[EXAFS]]></dc:subject>
<dc:subject><![CDATA[XANES]]></dc:subject>
<dc:subject><![CDATA[radiochemistry laboratory]]></dc:subject>
<dc:subject><![CDATA[radionuclides]]></dc:subject>
<dc:subject><![CDATA[X-ray diffraction and reflectometry]]></dc:subject>
<dc:subject><![CDATA[thin films]]></dc:subject>
<dc:subject><![CDATA[interfaces]]></dc:subject>
<dc:subject><![CDATA[melts]]></dc:subject>
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<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Schell, N.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Claußner, J.]]></dc:creator>
<dc:creator><![CDATA[Oehme, W.]]></dc:creator>
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<dc:creator><![CDATA[Dienel, S.]]></dc:creator>
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<dc:creator><![CDATA[Denecke, M. A.]]></dc:creator>
<dc:creator><![CDATA[Krug, H.]]></dc:creator>
<dc:creator><![CDATA[Neumann, W.]]></dc:creator>
<dc:creator><![CDATA[Hüttig, G.]]></dc:creator>
<dc:creator><![CDATA[Reichel, P.]]></dc:creator>
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<dc:title><![CDATA[ROBL - a CRG Beamline for Radiochemistry and Materials Research at the ESRF]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf, Wissenschaftlich-Technische Berichte; FZR-256 April 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The paper describes the Rossendorf Beamline (ROBL) built by the Forschungszentrum Rossendorf at the ESRF. ROBL comprises two different and independently operating experimental stations: a radiochemistry laboratory for X-ray absorption spectroscopy of non-sealed radioactive samples and a general purpose materials research station for X-ray diffraction and reflectometry mainly of thin films and interfaces modified by ion beam techniques. The radiochemistry set-up is worldwide an unique installation at a modern synchrotron radiation source.]]></dc:description>
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<dc:subject><![CDATA[EXAFS]]></dc:subject>
<dc:subject><![CDATA[XANES]]></dc:subject>
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<dc:subject><![CDATA[radionuclides]]></dc:subject>
<dc:subject><![CDATA[X-ray diffraction and reflectometry]]></dc:subject>
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<dc:subject><![CDATA[interfaces]]></dc:subject>
<dc:subject><![CDATA[melts]]></dc:subject>
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<dc:creator><![CDATA[Prokert, F.]]></dc:creator>
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<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Schell, N.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2449-1</dc:identifier>
<dc:title><![CDATA[Das ROBL-Strahlrohr an der ESRF: (Röntgenoptik und Strahlcharakteristika, der MRH-Meßplatz)]]></dc:title>
<dc:source><![CDATA[Workshop "Strukturanalyse von Kristalloberflächen und dünnen Schichten mit Synchrotronstrahlung", LMU München, Oct.  8 - 10, 1997]]></dc:source>
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<dc:creator><![CDATA[Neelmeijer, C.]]></dc:creator>
<dc:creator><![CDATA[Wagner, W.]]></dc:creator>
<dc:creator><![CDATA[Schramm, H.-P.]]></dc:creator>
<dc:creator><![CDATA[Thiel, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-242-1</dc:identifier>
<dc:title><![CDATA["De re metallica" (G. Agricola) - IBA on air]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 99 (1995) 390]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[On the occasion of Georgius Agricola's 500th birthday in 1994 attention has been focused on the paint material found in an exemplar of his famous scientific book “De re metallica”. The very thin color coatings on the highly sensitive paper substrate represent a challenge to the power and the guaranteed non-destructiveness of IBA. The combined implementation of PIXE and RBS on the external proton beam set-up allows one to determine the chemical elements of the pigments used and to identify the presence of organic layers. Results from selected colors are given to emphasize the complementary character of on-air PIXE-RBS analysis.]]></dc:description>
<dc:subject><![CDATA[ion beam analysis]]></dc:subject>
<dc:subject><![CDATA[non-destructive analysis]]></dc:subject>
<dc:subject><![CDATA[external proton beam]]></dc:subject>
<dc:subject><![CDATA[PIXE]]></dc:subject>
<dc:subject><![CDATA[RBS]]></dc:subject>
<dc:subject><![CDATA[book painting]]></dc:subject>
<dc:subject><![CDATA[thin layers]]></dc:subject>
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<dc:creator><![CDATA[Neelmeijer, C.]]></dc:creator>
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<dc:creator><![CDATA[Schramm, H.-P.]]></dc:creator>
<dc:creator><![CDATA[Thiel, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-242-2</dc:identifier>
<dc:title><![CDATA["De re metallica" (G. Agricola) - IBA on air]]></dc:title>
<dc:source><![CDATA[Denton-Conf. 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[On the occasion of Georgius Agricola's 500th birthday in 1994 attention has been focused on the paint material found in an exemplar of his famous scientific book “De re metallica”. The very thin color coatings on the highly sensitive paper substrate represent a challenge to the power and the guaranteed non-destructiveness of IBA. The combined implementation of PIXE and RBS on the external proton beam set-up allows one to determine the chemical elements of the pigments used and to identify the presence of organic layers. Results from selected colors are given to emphasize the complementary character of on-air PIXE-RBS analysis.]]></dc:description>
<dc:subject><![CDATA[ion beam analysis]]></dc:subject>
<dc:subject><![CDATA[non-destructive analysis]]></dc:subject>
<dc:subject><![CDATA[external proton beam]]></dc:subject>
<dc:subject><![CDATA[PIXE]]></dc:subject>
<dc:subject><![CDATA[RBS]]></dc:subject>
<dc:subject><![CDATA[book painting]]></dc:subject>
<dc:subject><![CDATA[thin layers]]></dc:subject>
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<dc:creator><![CDATA[Tichtchenko, V. G.]]></dc:creator>
<dc:creator><![CDATA[Wagner, W.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
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<dc:title><![CDATA[Decay Study of Hot Nuclei Below the Multifragmentation Threshold with the FOBOS Detector at Dubna]]></dc:title>
<dc:source><![CDATA[Int. Research Workshop, Poiana Brusov, Romania, Oct. 7 - 14, 1996]]></dc:source>
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<identifier>HZDR:PUBLDB:754-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Renz, G.]]></dc:creator>
<dc:creator><![CDATA[Schilling, K.-D.]]></dc:creator>
<dc:creator><![CDATA[Strekalovsky, O. V.]]></dc:creator>
<dc:creator><![CDATA[Tichtchenko, V. G.]]></dc:creator>
<dc:creator><![CDATA[Wagner, W.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
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<dc:identifier>https://www.hzdr.de/publications/Publ-754-1</dc:identifier>
<dc:title><![CDATA[Decay Study of Hot Nuclei Below the Multifragmentation Threshold with the FOBOS Detector at Dubna]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-159 Preprint]]></dc:source>
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<identifier>HZDR:PUBLDB:1801-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Stoemenos, J.]]></dc:creator>
<dc:creator><![CDATA[Pecz, B.]]></dc:creator>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1801-1</dc:identifier>
<dc:title><![CDATA[Epitaxial aluminum carbide formation in 6H-SiC by high dose Al<sup>+</sup> implantation]]></dc:title>
<dc:source><![CDATA[Applied Physics Letters 74 (1999) 2602]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Aluminum carbide precipitates are formed after Al ion implantation with dose 3x10<sup>17</sup> cm<sup>-2</sup> at 500°C into single crystalline 6H SiC. The aluminum carbide (Al<sub>4</sub>C<sub>3</sub>) precipitates are in epitaxial relation with 6H-SiC matrix, having the following orientation relation, [0001]6H-SiC//[11-20]Al<sub>4</sub>C<sub>3</sub> and [11-20]6H-SiC//[11-20]Al<sub>4</sub>C<sub>3</sub> , as transmission electron microscopy reveals. The aluminum carbide appears around the maximum of the Al depth distribution. Si precipitates were also detected in the same zone. ]]></dc:description>
<dc:subject><![CDATA[high dose implantation]]></dc:subject>
<dc:subject><![CDATA[silicon carbide]]></dc:subject>
<dc:subject><![CDATA[phase formation]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<identifier>HZDR:PUBLDB:1802-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1802-1</dc:identifier>
<dc:title><![CDATA[Experimentelle Realisierung einer freien Flüssigmetalloberfläche]]></dc:title>
<dc:source><![CDATA[Machbarkeitsstudie / Abschlußbericht für DARA GmbH, September 1995]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1803-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:description><![CDATA[The German 1000 roofs PV programme, in which more than 2000 roof-mounted grid connected PV systems are now operating, provides invaluable information on the operational performance of the installed PV systems, the PV users and their consumption behaviour. The Institut für Solarenergieforschung (ISFH) and the Forschungszentrum Rossendorf (FZR), responsible for the organization of the 1000 roofs programme in the Federal States of Lower Saxony and Saxony, have been analysing the monitored performance and consumption data of more than 300 PV systems operating since 1991. The purpose of this work is to examine the relationship between PV system yield and electricity consumption for the realized projects and to take advantage of the first-hand information on the PV users consumption behaviour for future PV applications.]]></dc:description>
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<dc:title><![CDATA[Tc(V) and Re(V) complexes of N-(MAG1)-Histamine]]></dc:title>
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<dc:description><![CDATA[The synthesis of N-(MAG1)-histamine and the preparation of its Tc and Re complexes are reported. As proven by spectroscopic methods, HPLC investigations and by X-ray structure analysis, N-(MAG1)-histamine forms stable, neutral and square pyramidal 1:1 coordination compounds with MO3*-cores of Tc and Re. The preparation of the isostructural 99mTcO(V)-N-(MAG1)-histamine complex has been achieved with 80-95% radiochemical yield.]]></dc:description>
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<dc:title><![CDATA[Tc(V) and Re(V) complexes of N-(MAG1)-Histamine]]></dc:title>
<dc:source><![CDATA[36. Intern. Jahrestagung DGN, Leipzig, 01.-04.04.1998]]></dc:source>
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<dc:description><![CDATA[The synthesis of N-(MAG1)-histamine and the preparation of its Tc and Re complexes are reported. As proven by spectroscopic methods, HPLC investigations and by X-ray structure analysis, N-(MAG1)-histamine forms stable, neutral and square pyramidal 1:1 coordination compounds with MO3*-cores of Tc and Re. The preparation of the isostructural 99mTcO(V)-N-(MAG1)-histamine complex has been achieved with 80-95% radiochemical yield.]]></dc:description>
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<dc:title><![CDATA[Tc(V) and Re(V) complexes of N-(MAG1)-Histamine]]></dc:title>
<dc:source><![CDATA[Nuklearmedizin 37 (1998) A53]]></dc:source>
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<dc:description><![CDATA[The synthesis of N-(MAG1)-histamine and the preparation of its Tc and Re complexes are reported. As proven by spectroscopic methods, HPLC investigations and by X-ray structure analysis, N-(MAG1)-histamine forms stable, neutral and square pyramidal 1:1 coordination compounds with MO3*-cores of Tc and Re. The preparation of the isostructural 99mTcO(V)-N-(MAG1)-histamine complex has been achieved with 80-95% radiochemical yield.]]></dc:description>
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<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
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<dc:title><![CDATA[Computer simulation of ion-beam-induced processes in solids: An overview of the activities at the FZ Rossendorf]]></dc:title>
<dc:source><![CDATA[Environmental Molecular Science Laboratory at Pacific Northwest National Laboratory, Richland, WA, USA, May 7,1999]]></dc:source>
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<dc:creator><![CDATA[Ferse, W.]]></dc:creator>
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<dc:title><![CDATA[The Application of the Expert System XUMA in the State of Saxony]]></dc:title>
<dc:source><![CDATA[Proceedings of 4th Workshop on Information Managem,ent in Nuclear Safety, Radiation Protection and Environmental Protection, GRS-105, Köln, January 1994]]></dc:source>
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<dc:description><![CDATA[In the last years contaminated sites have become a relevant problem in the Federal Republic of Germany because there exist a large number of these sites. That's why in Germany more intensive efforts are undertaken in order to start necessary remediations. Basic initial conditions for an effective execution of these works are on the one side a systematic registration of these sites and on the other side the creation of a uniform evaluation capability for the assessment of environmental hazards.

Regarding this background the Research Centre Rossendorf (FZR) together with Nuclear Engineering and Analytics, Inc. Rossendorf apply and modify the computer code system XUMA (German synonym for expert system on environmental hazards of contaminated sites) which is a joint project of the Institute for Applied Information Science of the Karlsruhe Nuclear Research Centre and the State Institute for Environmental Protection of Baden-Württemberg. XUMA is a knowledge based computer system, which shall support the staff of the responsible governmental offices in the uniform evaluation of the hazard potential, the preparation of analysis plans, and the assessment of contaminated sites and mines.

To enable the registration and evaluation of contaminated sites at engineering offices FZR developes an interface program which can be generated automatically from the knowledge base of the expert system XUMA. This interface program can be executed at each IBM-compatible PC without any additional runtime environment.]]></dc:description>
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<datestamp>2020-12-01</datestamp>
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<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Schuster, G.]]></dc:creator>
<dc:creator><![CDATA[Teske, K.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Henkel, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-34-1</dc:identifier>
<dc:title><![CDATA[Neutron and X-ray Investigations on the Oxigen Bonding in YBa2Cu30(7-x) combined with Physico-chemical Methods]]></dc:title>
<dc:source><![CDATA[Fresenius Zeitschrift für Analyt. Chemie 349 (1994) 1-3 pp. 231-233]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The occupancy of the oxygen lattice positions at different annealing conditions in Yba2Cu3O(7-x) were determined by Rietveld refinements using neutron and X-ray diffraction data. The occupation density for the oxygen positions O1 to O4 were ascertained. The values of the oxygen content of the samples from this method were compared with those measured by thermoanalysis. The O1 and O4 oxygen atoms are exchangeable by thermal treatment. The oxygen in the planes is fixed and cannot be removed by thermal treatment up to 935oC. The binding strength of O1 in the lattice is stronger than that of O4 atoms; this is demonstrated by a higher temperature of dissociation of the O1 atoms. The amount of the oxygen taken up is not exactly equal to the oxygen actually in the lattice positions. In the temperature region below 400oC adsorption and chemisorption processes become dominant.]]></dc:description>
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<identifier>HZDR:PUBLDB:34-2</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Schuster, G.]]></dc:creator>
<dc:creator><![CDATA[Teske, K.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Henkel, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-34-2</dc:identifier>
<dc:title><![CDATA[Neutron and X-ray Investigations on the Oxigen Bonding in YBa2Cu30(7-x) combined with Physico-chemical Methods]]></dc:title>
<dc:source><![CDATA[7. Tagung Festkörperanalytik, Chemnitz, 19. - 23. Juni 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The occupancy of the oxygen lattice positions at different annealing conditions in Yba2Cu3O(7-x) were determined by Rietveld refinements using neutron and X-ray diffraction data. The occupation density for the oxygen positions O1 to O4 were ascertained. The values of the oxygen content of the samples from this method were compared with those measured by thermoanalysis. The O1 and O4 oxygen atoms are exchangeable by thermal treatment. The oxygen in the planes is fixed and cannot be removed by thermal treatment up to 935oC. The binding strength of O1 in the lattice is stronger than that of O4 atoms; this is demonstrated by a higher temperature of dissociation of the O1 atoms. The amount of the oxygen taken up is not exactly equal to the oxygen actually in the lattice positions. In the temperature region below 400oC adsorption and chemisorption processes become dominant.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1827-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1827-1</dc:identifier>
<dc:title><![CDATA[Anwendung neuronaler Netze zur akustischen Leckortung an komplizierten Strukturen]]></dc:title>
<dc:source><![CDATA[Preprint VDI/GVC Düsseldorf - Fachtagung Prozeß- und Anlagensicherheit, November 1994, S. 135 - 146]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Eine Methode zur Erkennung und Ortung von Lecks an Druckanlagen komplizierter 3-dimensionaler Topologie ist entwickelt worden. Sie basiert auf der Merkmalsextraktion aus dem leckinduzierten Körper- und Luftschall und wendet neuronale Netze zur Mustererkennung an. Die zum Anlernen der neuronalen Netze notwendigen Schallmuster werden mit Hilfe von simulierten Lecks an einer Originalstruktur erzeugt. Als Merkmale zur Charakterisierung des Leckortes werden Kohärenzwerte zwischen hochfrequenten Mikrofonsignalen und RMS-Werte von Schallemissionssensoren angewendet. Die Methode ist sogar einsatzfähig, wenn die Leckortung auf der Basis von Laufzeit- oder Dämpfungsdifferenzen versagt. Die Methode wird prototypisch für einen russischen WWER-Druckwasserreaktor entwickelt. Die Anwendung neuronaler Netze ermöglicht eine Adaption der Leckortungsmethode an Druckanlagen unterschiedlicher Topologie.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1829-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Noack, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1829-1</dc:identifier>
<dc:title><![CDATA[Neutron-Physical Development of Reflectors for the Pulsed Reactor IBR-2]]></dc:title>
<dc:source><![CDATA[Kerntechnik 59 (1994) 6, S. 291 - 297, München: Hanser Verlag, 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The pulsed fast reactor IBR-2, Dubna, is at present the most powerful pulsed neutron source used for condensed matter research. The neutron pulses are generated periodically by reactivity modulation, which is accomplished by a rotating two-reflector system. The neutron physics which has been involved in the development of various reflectors is analysed with respect to the neutron pulse length. Two new reflectors are proposed.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:3392-1</identifier>
<datestamp>2025-12-08</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gabriel, F.]]></dc:creator>
<dc:creator><![CDATA[Gippner, P.]]></dc:creator>
<dc:creator><![CDATA[Grosse, E.]]></dc:creator>
<dc:creator><![CDATA[Janssen, D.]]></dc:creator>
<dc:creator><![CDATA[Michel, P.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Schamlott, A.]]></dc:creator>
<dc:creator><![CDATA[Seidel, W.]]></dc:creator>
<dc:creator><![CDATA[Wolf, A.]]></dc:creator>
<dc:creator><![CDATA[Wünsch, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3392-1</dc:identifier>
<dc:title><![CDATA[The Rossendorf radiation source ELBE and its FEL projects]]></dc:title>
<dc:source><![CDATA[Nucl. Instr. Meth. B 161(2000)1143-1147 PACS classification codes: 41.60.Cr; 41.85.Lc]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The Forschungszentrum Rossendorf (FZR) is constructing a superconducting Electron Linac [F. Gabriel, J. Voigtländer, et al.,
ELBE Design Report 1998, http://www.fz-rossendorf.de/FWQ/report_d.htm; Annual Report 1996, FZR-179 (1997) 3; Annual
Report 1997, FZR-215 (1998) 3] with high Brilliance and low Emittance (ELBE) which can deliver a 1 mA cw beam of 40
MeV. ELBE will be equipped with a free-electron laser (FEL) system for the production of infrared (IR) light in the range 5¯300 
um and will thus cover the range from the infrared to the THz regime. The electron beam can also be used to generate X-rays,
bremsstrahlung, positrons or fast neutrons.]]></dc:description>
<dc:subject><![CDATA[Free-electron laser]]></dc:subject>
<dc:subject><![CDATA[Undulator magnet]]></dc:subject>
<dc:subject><![CDATA[Infrared]]></dc:subject>
<dc:subject><![CDATA[Superconducting RF linac]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0168-583X(99)00909-X]]></dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:1472-1</identifier>
<datestamp>2019-03-04</datestamp>
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</header>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kotte, R.]]></dc:creator>
<dc:creator><![CDATA[Barz, H.-W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1472-1</dc:identifier>
<dc:title><![CDATA[On the sequence of proton and composite particle emission in central collisions of Ru(Zr)+Ru(Zr) at 400 AMeV]]></dc:title>
<dc:source><![CDATA[Proceedings of the International Workshop XXVII on Gross Properties of Nuclei and Nuclear Excitations, Hirschegg, Austria, January 17 - 23, 1999, p. 181]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1473-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barz, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Kotte, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1473-1</dc:identifier>
<dc:title><![CDATA[Excitation energies of clusters from light fragment correlations]]></dc:title>
<dc:source><![CDATA[Workshop on Multifragmentation, Hirschegg, 18.-22. Januar 1999, Austria]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:1473-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barz, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Kotte, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1473-2</dc:identifier>
<dc:title><![CDATA[Excitation energies of clusters from light fragment correlations]]></dc:title>
<dc:source><![CDATA[Proceedings of the International Workshop XXVII on Gross Properties of Nuclei and Nuclear Excitations, Hirschegg, Austria,  January 17-23, 1999, p. 189]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:1476-1</identifier>
<datestamp>2025-02-06</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grigull, S.]]></dc:creator>
<dc:creator><![CDATA[Behrisch, R.]]></dc:creator>
<dc:creator><![CDATA[Parascandola, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1476-1</dc:identifier>
<dc:title><![CDATA[Nitrogen implantation into carbon: retention, release and target-erosion processes]]></dc:title>
<dc:source><![CDATA[Journal of Nuclear Materials 275 (1999) 158-163]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0022-3115(99)00112-9]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1476-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1476-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grigull, S.]]></dc:creator>
<dc:creator><![CDATA[Behrisch, R.]]></dc:creator>
<dc:creator><![CDATA[Parascandola, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1476-2</dc:identifier>
<dc:title><![CDATA[Nitrogen implantation into carbon: retention, release and target-erosion processes]]></dc:title>
<dc:source><![CDATA[13th international conference on plasma surface interactions in controlled fusion devices, San Diego, USA, 18.-22. Mai, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1476-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1478-2</identifier>
<datestamp>2025-02-06</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grosse, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1478-2</dc:identifier>
<dc:title><![CDATA[In-Medium Properties of Kaons and Antikaons as Studied by Threshold Production in Nuclear Collisions]]></dc:title>
<dc:source><![CDATA[Nuclear Physics A654 (1999) 501c-504c]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[In a systematic experimental study of K$^{+}$ and K$^{-}$ production at energies close to and below the free nucleon-nucleon production threshold we have found several features indicating a change of kaon properties within the nuclear medium.]]></dc:description>
<dc:subject><![CDATA[meson production]]></dc:subject>
<dc:subject><![CDATA[kaon production]]></dc:subject>
<dc:subject><![CDATA[nuclear medium]]></dc:subject>
<dc:subject><![CDATA[medium effects]]></dc:subject>
<dc:subject><![CDATA[threshold production]]></dc:subject>
<dc:subject><![CDATA[heavy ion collision]]></dc:subject>
<dc:subject><![CDATA[nucleus nucleus collision]]></dc:subject>
<dc:subject><![CDATA[meson mass]]></dc:subject>
<dc:subject><![CDATA[kaon mass]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<header>
<identifier>HZDR:PUBLDB:1479-1</identifier>
<datestamp>2025-02-06</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Srinivas, P.]]></dc:creator>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Subramanian, A. R.]]></dc:creator>
<dc:creator><![CDATA[Raghavan, S. A. V.]]></dc:creator>
<dc:creator><![CDATA[Rangisetty, J. B.]]></dc:creator>
<dc:creator><![CDATA[Gupta, C. N. V. H. B.]]></dc:creator>
<dc:creator><![CDATA[Parimoo, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1479-1</dc:identifier>
<dc:title><![CDATA[Synthesis and preliminary binding affinities of 1(1,2-dihydro-2-acenaphthylenyl)piperazine - a new arylpiperazine]]></dc:title>
<dc:source><![CDATA[Pharmaceutica Acta Helvetiae 74 (1999) 73-73]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The first synthesis of  1-(1,2-dihydro-2-acenaphthylenyl)piperazine (5)  a new arylpiperazine is described. Preliminary binding studies on this new arylpiperazine reveal affinity for the 5-HT<SUB>1A</SUB> and 5-HT<SUB>2A</SUB> receptor subtypes. Incorporation of a dopamine pharmacophore onto this arylpiperazine provided compound (7) a potential antipsychotic with an atypical profile.]]></dc:description>
<dc:subject><![CDATA[Arylpiperazine]]></dc:subject>
<dc:subject><![CDATA[1-(1,2-dihydro-2-acenaphthylenyl)piperazine]]></dc:subject>
<dc:subject><![CDATA[5-HT]]></dc:subject>
<dc:subject><![CDATA[Dopamine]]></dc:subject>
<dc:subject><![CDATA[Atypical antipsychotic]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0031-6865(99)00019-9]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1479-1</dc:relation>
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<header>
<identifier>HZDR:PUBLDB:1480-1</identifier>
<datestamp>2025-02-06</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
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<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Pavlenko, O. P.]]></dc:creator>
<dc:creator><![CDATA[Gallmeister, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1480-1</dc:identifier>
<dc:title><![CDATA[Dileptons, Charm and Bottom in Relativistic Heavy-Ion Collisions]]></dc:title>
<dc:source><![CDATA[Progress in Particle and Nuclear Physics 42 (1999) 335-343]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
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<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0146-6410(99)00090-3]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1480-1</dc:relation>
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<header>
<identifier>HZDR:PUBLDB:1481-1</identifier>
<datestamp>2025-02-06</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Gallmeister, K.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Pavlenko, O. P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1481-1</dc:identifier>
<dc:title><![CDATA[Physical Information in the Thermal Continuum Dilepton Spectra]]></dc:title>
<dc:source><![CDATA[Progress in Particle and Nuclear Physics 42 (1999) 333-334]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1488-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Schmeide, K.]]></dc:creator>
<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:creator><![CDATA[Bubner, M.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1488-1</dc:identifier>
<dc:title><![CDATA[Effect of Humic Acid on the Uranium(VI) Sorption onto Phyllite and its Mineralogical Constituents]]></dc:title>
<dc:source><![CDATA[Migration´99 - Conference]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[
Organic materials, such as humic and fulvic acids, that are present in natural aquifers interact with dissolved inorganic contaminants and affect their sorption behavior on geological materials and thus, their migration in aquifers. Consequently, a quantification of the influence of humic material on radionuclide sorption is necessary.
Phyllite was used as site-specific rock material because it is quite common in the Western Erzgebirge' in Saxony, Germany, and is closely associated with uranium deposits of the uranium mining areas in East Germany. Site specific humic acid, isolated from the bog Kleiner Kranichsee' and a 14C-labelled synthetic humic acid were used for the experiments.
The effect of humic acid was studied on the sorption behavior of uranium(VI) onto phyllite and its mineralogical components muscovite, albite and quartz in air-equilibrated batch experiments as a function of pH. The uranium sorption is strongly affected by both the pH and the presence of organic material. The kinetics and reversibility of the uranium and humic acid sorption were studied using the 14C-labelled humic acid. Furthermore, the influence of competing sulfate ions on the uranyl and humic acid sorption onto phyllite was determined, because seepage waters of the uranium mining areas in Saxony contain, among other anions, relatively high concentrations of sulfate (3 10-2 M).


]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:1819-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1819-1</dc:identifier>
<dc:title><![CDATA[A novel method to investigate ion-beam-induced defect evolution in Si]]></dc:title>
<dc:source><![CDATA[5th International Symposium on Process Physics and Modeling in Semiconductor Device Manufacturing, 195th Meeting of the Electrochemical Society, Seattle, WA, USA, May 2-6, 1999 (invited lecture)]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1819-2</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1819-2</dc:identifier>
<dc:title><![CDATA[A novel method to investigate ion-beam-induced defect evolution in Si]]></dc:title>
<dc:source><![CDATA[pp. 58-74 in: Process Physics and Modeling in Semiconductor Technology (Edited by C. S. Murthy, G. R. Srinivasan, S. T. Dunham), Proceedings Volume 99-1, The Electrochemical Society, Pennington, NJ]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:1820-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Jankowsky, R.]]></dc:creator>
<dc:creator><![CDATA[Kirsch, S.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1820-1</dc:identifier>
<dc:title><![CDATA[Solution structure of technetium(V) and rhenium(V) peptide complexes as studied by EXAFS spectroscopy and capillary electrophoresis (CE)]]></dc:title>
<dc:source><![CDATA[Technetium, Rhenium and Other Metals in Chemistry and Nuclear Medicine
(Edited by Nicolini M., Mazzi, U.) SGE Editoriali Padova (1999) pp.229-235]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Structural investigations on rhenium and technetium peptide complexes have been carried out using X-ray absorption spectroscopy (EXAFS) and capillary electrophoresis. Small cysteine containing peptides with altered amino acid sequences were used as model systems to study the metal complexation behaviour. By means of capillary electrophoresis, complex species existing over the pH range could be identified as well as protonable groups in these complexes. EXAFS measurements in solution delivered information about the complex coordination spheres. The metal complexation modes and complex stoichiometries of directly labelled metal complexes of large biologically active peptides could be elucidated. ]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:14352-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Araki, K.]]></dc:creator>
<dc:creator><![CDATA[Mitsumoto, K.]]></dc:creator>
<dc:creator><![CDATA[Akatsu, M.]]></dc:creator>
<dc:creator><![CDATA[Nemoto, Y.]]></dc:creator>
<dc:creator><![CDATA[Suzuki, H. S.]]></dc:creator>
<dc:creator><![CDATA[Tanida, H.]]></dc:creator>
<dc:creator><![CDATA[Takagi, S.]]></dc:creator>
<dc:creator><![CDATA[Yasin, S.]]></dc:creator>
<dc:creator><![CDATA[Zherlitsyn, S.]]></dc:creator>
<dc:creator><![CDATA[Wosnitza, J.]]></dc:creator>
<dc:creator><![CDATA[Goto, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14352-1</dc:identifier>
<dc:title><![CDATA[Low-Temperature Elastic Properties of Non-Kramers Doublet Compound PrMg<sub>3</sub>]]></dc:title>
<dc:source><![CDATA[Strongly Correlated Electron Systems 2010 (SCES 2010), 27.06.-02.07.2010, Santa Fe, USA]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[We have investigated low-temperature elastic properties of PrMg<sub>3</sub> with a non-Kramers Gamma<sub>3</sub> doublet ground state using ultrasonic measurements. Although the Gamma<sub>3</sub> doublet possesses electric quadrupoles O<sub>u</sub> and O<sub>v</sub> with Gamma<sub>3</sub>-symmetry and magnetic octupole T<sub>xyz</sub> with Gamma<sub>2</sub>, PrMg<sub>3</sub> reveals no sign of symmetry breaking long-range ordering down to 20 mK. [1] The elastic constant of (C<sub>11</sub>-C<sub>12</sub>)/2 in PrMg<sub>3</sub> exhibits remarkable softening below 8 K, which is well described in terms of a Curie-type quadrupole susceptibility for the Gamma<sub>3</sub> doublet. An appreciable upturn in (C<sub>11</sub>-C<sub>12</sub>)/2 below 800 mK in PrMg<sub>3</sub> may indicate an transition into an exotic ground state due to the quadrupole Kondo state being screened by conduction electrons. Frequency dependence in (C<sub>11</sub>-C<sub>12</sub>)/2 and its attenuation coefficients at low temperature in PrMg<sub>3</sub> suggests quadrupole fluctuations possessing a characteristic relaxation time tau = tau<sub>0</sub>exp(E/kT) with tau<sub>0</sub> = 6x10<sup>-11</sup> sec and an activation energy E = 410 mK. The low-temperature behavior in (C<sub>11</sub>-C<sub>12</sub>)/2 of PrMg3 under magnetic fields is also presented.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:14509-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Anelli, M.]]></dc:creator>
<dc:creator><![CDATA[Bertolucci, S.]]></dc:creator>
<dc:creator><![CDATA[Bini, C.]]></dc:creator>
<dc:creator><![CDATA[Branchini, P.]]></dc:creator>
<dc:creator><![CDATA[Corradi, G.]]></dc:creator>
<dc:creator><![CDATA[Curceanu, C.]]></dc:creator>
<dc:creator><![CDATA[Dezorzi, G.]]></dc:creator>
<dc:creator><![CDATA[Di Domenico, A.]]></dc:creator>
<dc:creator><![CDATA[Di Micco, B.]]></dc:creator>
<dc:creator><![CDATA[Ferrari, A.]]></dc:creator>
<dc:creator><![CDATA[Fiore, S.]]></dc:creator>
<dc:creator><![CDATA[Gauzzi, P.]]></dc:creator>
<dc:creator><![CDATA[Giovannella, S.]]></dc:creator>
<dc:creator><![CDATA[Happacher, F.]]></dc:creator>
<dc:creator><![CDATA[Iliescu, M.]]></dc:creator>
<dc:creator><![CDATA[Luca', A.]]></dc:creator>
<dc:creator><![CDATA[Martini, M.]]></dc:creator>
<dc:creator><![CDATA[Miscetti, S.]]></dc:creator>
<dc:creator><![CDATA[Nguyen, F.]]></dc:creator>
<dc:creator><![CDATA[Passeri, A.]]></dc:creator>
<dc:creator><![CDATA[Prokoviev, A. V.]]></dc:creator>
<dc:creator><![CDATA[Sarra, I.]]></dc:creator>
<dc:creator><![CDATA[Sciascia, B.]]></dc:creator>
<dc:creator><![CDATA[Sirghi, F.]]></dc:creator>
<dc:creator><![CDATA[Tagnani, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14509-1</dc:identifier>
<dc:title><![CDATA[Measurement of the neutron detection efficiency of a 80% absorber - 20% scintillating fiber calorimeter]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research A 626-627(2011), 67-71]]></dc:source>
<dc:date>2011</dc:date>
<dc:description><![CDATA[The neutron detection efficiency of a sampling calorimeter made of 1 mm diameter scintillating fibers embedded in a lead/bismuth structure has been measured at the neutron beam of the Svedberg Laboratory at Uppsala. A significant enhancement of the detection efficiency with respect to a bulk organic scintillator detector with the same thickness is observed.]]></dc:description>
<dc:subject><![CDATA[Neutron detection]]></dc:subject>
<dc:subject><![CDATA[calorimetry]]></dc:subject>
<dc:subject><![CDATA[scintillating fibers]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/j.nima.2010.10.094]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14509-1</dc:relation>
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<header>
<identifier>HZDR:PUBLDB:14552-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kluge, T.]]></dc:creator>
<dc:creator><![CDATA[Enhardt, W.]]></dc:creator>
<dc:creator><![CDATA[Kraft, S. D.]]></dc:creator>
<dc:creator><![CDATA[Schramm, U.]]></dc:creator>
<dc:creator><![CDATA[Zeil, K.]]></dc:creator>
<dc:creator><![CDATA[Cowan, T. E.]]></dc:creator>
<dc:creator><![CDATA[Bussmann, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14552-1</dc:identifier>
<dc:title><![CDATA[Enhanced laser ion acceleration from mass-limited foils]]></dc:title>
<dc:source><![CDATA[Physics of Plasmas 17(2010)12, 123103-123109]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[This paper reports on simulations of solid mass-limited targets (MLT) via electrodynamic 2D3V particle-in-cell simulations. The interaction with long (300 fs) high intensity (10<sup>20</sup> W/cm²) laser pulses with targets of diameter down to 1 m is described in detail with respect to electron dynamics and proton and ion acceleration. Depending on the foil diameter, different effects consecutively arise. Electrons laterally recirculate within the target, smoothening the target rear accelerating sheath and increasing the hot electron density and temperature. Our results suggest that the most significant ion energy enhancement to should be expected for MLT with diameter below the laser focal spot size. The spread of energetic protons is decreased for medium sized foils while it is greatly increased for foils of size near the focal spot size.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:language>eng</dc:language>
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<header>
<identifier>HZDR:PUBLDB:15031-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barth, T.]]></dc:creator>
<dc:creator><![CDATA[Hampel, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-15031-1</dc:identifier>
<dc:title><![CDATA[Experiments on the transport, deposition and resuspension of nuclear aerosols]]></dc:title>
<dc:source><![CDATA[International Aerosol Conference – IAC 2010, 29.08.-03.09.2010, Helsinki, Finnland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Nuclear aerosol deposition and the assessment of its resuspension during a design basis accident in the primary circuit are a key issue in the development and certification of advanced pebble bed High Temperature Reactors (HTRs). Nuclear aerosols, in particular graphite dust in size of d = [0.1; 50] μm, are deposited during operation in the primary circuit (Moormann (2008)). It is of general interest how much of these aerosols escape from the primary circuit into the containment during a depressurization scenario. The knowledge about the amount of resuspended dust allows the detailed estimate of the dose escaping the primary circuit
Flow conditions in the primary circuit range from laminar flows in the recuperator till turbulent high Reynolds number flows in the pipes and ducts. Considering the particle size distribution published by Moormann (2008), particle Stokes numbers will range from very small Stk << 1 till moderately high Stk > 1. In order to investigate the fluid mechanic behavior between the flow and the aerosol within the set of characteristic numbers, we designed a small scale gas aerosol test facility (Figure 1).

We found a turbulent square duct flow most suitable because all the flow features such as streamwise and spanwise velocity gradients, as well as vortical structures are apparent. Furthermore, there will be a wide range of experimental and numerical data for comparison.
The test facility is a small scale wind tunnel in total length of 6 m with a 10 x 10 cm² square duct section. A 500 W radial fan at the outlet of the channel accelerates the flow field from 0 up to 7.5 m/s which is equivalent to a Reynolds number of about Re = 50 k.
The inlet is equipped with a HEPA filter to clean the incoming air. A nozzle contracts the flow into a square duct which is divided into a flow formation zone (15 x d) and a test section (5 x d). In the beginning of the flow formation zone the dust feeder or the aerosol generator injects the aerosol. The length of 15 x d for the flow formation zone ensures that the test section is streamed by a well developed turbulent channel flow with an evenly distributed aerosol. Both, test section and flow formation zone, are made of transparent acrylic glass to allow optical flow field measurements, such as PIV, high speed camera imaging for the analysis of the flow field and microscopic imaging techniques for the surface particle detection.
A diffusor stage decelerates the flow before it enters the electrostatic filter for air cleaning purposes. Finally, the 500 W radial fan produces the pressure drop for the desired flow speed.
Preliminary measurements of total pressure drop in the square duct section and time averaged mean center velocity profiles for different Reynolds number will be presented on the poster.]]></dc:description>
<dc:subject><![CDATA[Nuclear Aerosol Particles]]></dc:subject>
<dc:subject><![CDATA[Deposition]]></dc:subject>
<dc:subject><![CDATA[Resuspension]]></dc:subject>
<dc:subject><![CDATA[VHTR]]></dc:subject>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1831-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Hensel, F.]]></dc:creator>
<dc:creator><![CDATA[Schütz, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1831-2</dc:identifier>
<dc:title><![CDATA[Ultrasonic Two-Phase Flow Measurements Based on Pattern Recognition Techniques]]></dc:title>
<dc:source><![CDATA[XIII IMEKO World Congress, Torino September 5-9, 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The state-of art of ultrasonic two-phase flow measurements is characterised by a number of different approaches commonly based on the identification and characterisation of individual voids (bubbles, plugs etc.) applying the techniques of ultrasonic testing. The recorded individual events are integrated to extract parameters as void fraction or volume flow rates. The main limitation of these methods arises from the complicated structure of two-phase flow at higher void fractions which leads to multiple diffractions of the sound beam. The measurement is therefore limited to low void fractions or a simple flow structure.
The main idea of the present work was to overcome these limitations by means of pattern recognition. An ultrasonic beam crossing the two-phase flow is modulated by the changing structure of the voids passing by and therefore the through-transmission signal must contain information about the parameters of the two-phase flow even if  information about individual flow effects cannot be derived. Therefore it was supposed that a pattern recognition algorithm trained with signals obtained at known conditions is able to identify the set of the flow parameters (flow rates, void fraction etc.) in an unknown situation.
]]></dc:description>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1831-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Hensel, F.]]></dc:creator>
<dc:creator><![CDATA[Schütz, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1831-1</dc:identifier>
<dc:title><![CDATA[Ultrasonic Two-Phase Flow Measurements Based on Pattern Recognition Techniques]]></dc:title>
<dc:source><![CDATA[From Measurement to Innovation. Proceedings of the XIII IMEKO World Congress, Vol.2, p. 1112-111]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The state-of art of ultrasonic two-phase flow measurements is characterised by a number of different approaches commonly based on the identification and characterisation of individual voids (bubbles, plugs etc.) applying the techniques of ultrasonic testing. The recorded individual events are integrated to extract parameters as void fraction or volume flow rates. The main limitation of these methods arises from the complicated structure of two-phase flow at higher void fractions which leads to multiple diffractions of the sound beam. The measurement is therefore limited to low void fractions or a simple flow structure.
The main idea of the present work was to overcome these limitations by means of pattern recognition. An ultrasonic beam crossing the two-phase flow is modulated by the changing structure of the voids passing by and therefore the through-transmission signal must contain information about the parameters of the two-phase flow even if  information about individual flow effects cannot be derived. Therefore it was supposed that a pattern recognition algorithm trained with signals obtained at known conditions is able to identify the set of the flow parameters (flow rates, void fraction etc.) in an unknown situation.
]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1831-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:103-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Scheffler, M.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Liewers, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-103-1</dc:identifier>
<dc:title><![CDATA[Komponentenschwingungen an WWER-Reaktoren "Diagnose und Modellierung"]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Seit Anfang der 70er Jahre sind an WWER-440-Reaktoren mehrfach anomale Schwingungen von Einbauten des RDB beobachtet worden, die teilweise zu Komponentenschäden führten.
Daher wurden speziell für den WWER-Typ zugeschnittene Diagnoseverfahren entwickelt, die auf der Korrelationsanalyse von Schwankungsanteilen des Neutronenflusses (incore und excore) und von nichtnuklearen Signalen wie Körperschall, Druckfluktuation und Beschleunigungen beruhen.
Um eine wirklich sensitive Fehlerfrüherkennung zu erreichen, wird ein theoretisches Schwingungsmodell auf der Basis Finiter Elemente (FE) entwickelt. Dieses Modell gestattet die Interpretation von gemessenen Schwingungssignalen in dem Sinne, daß die gemessenen Resonanzpeaks den Eigenschwingungen des gekoppelten mechanischen Systems zugeordnet werden können.
Darüber hinaus werden Sensitivitätsstudien durchgeführt, die die Veränderungen des Schwingungsverhaltens bei mechanischen Komponentenschäden verdeutlichen.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-103-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:216-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Barz, H.-U.]]></dc:creator>
<dc:creator><![CDATA[Konheiser, J.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-216-1</dc:identifier>
<dc:title><![CDATA[Fluenzberechnungen für das Bestrahlungsprogramm Rheinsberg von Materialproben im Rheinsberger Reaktor im Zeitraum 1984-1988]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-51 August 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Im Zeitraum von 1984 - 1988 wurde am Rheinsberger Reaktor ein umfangreiches Bestrahlungsprogramm für Stahlproben aus verschiedenen Druckbehältermaterialien durchgeführt. Zielstellung des Vorhabens ist die Ermittlung der Veränderung der bruchmechanische Eigenschaften durch den Einfluß der Neutronenstrahlung.
Ein Teilaspekt für diese Zielstellung ist die Bestimmung der Parameter für die Neutronenbelastung. In diesem Bericht werden das methodische Vorgehen zur Gewinnung dieser Werte beschrieben, mögliche Fehlerquellen diskutiert sowie ein umfangreicher Überblick über die Ergebnisse gegeben.
Grundlage der transporttheoretischen Berechnungen bei gegebenen Spaltquellen war die Vielgruppen-Monte-Carlo-Methode mit speziellen Verfahren zur Minimierung der statistischen Fehler, so daß Ergebnisse mit kleinem statistischen Fehler für jede Einzelprobe, die im allgemeinen noch in vertikaler bzw. horizontaler Richtung unterteilt wurde, erzielt werden konnten.
Zur Berechnung der Spaltquelle wurde die für ein Zeitraster für jedes Kassettenelement gegebenen Abbranddaten zugrunde gelegt, auf deren Basis für jeder Reaktorbetriebsperiode die integralen Spaltquellverteilungen für verschiedene Spaltisotope berechnet wurden.
Dargestelt werden die für die Neutronenversprödung relevanten Ergebnisse, nämlich die kumulativen Neutronenflüsse im Energiebereich größer 0,5 und 1 MeV sowie eine dpa-Rate. Als allgemeines Resultat kann man die starke Abhängigkeit der Ergebnisse in radialer Richtung vom Reaktormittelpunkt anführen. Dagegen ergaben sich in azimulater und vertikaler Richtung nur relativ schwache Veränderungen.]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-216-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:259-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Carl, H.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Zschau, J.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-259-1</dc:identifier>
<dc:title><![CDATA[Schaffung eines Internationalen Zentrums für Information und Frühwarnung bei nuklearen Ereignissen in mittel- und osteuropäischen Kernkraftwerken]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-57]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Im Rahmen eines vom Sächsischen Staatsministeriums für Wissenschaft und Kunst geförderten Vorhabens wurden 1994 die Untersuchungen zu den Aufgaben, zu den zu erwartenden Kosten und zu den Realisierungschancen für ein internationales Zentrum für Information und Frühwarnung bei nuklearen Ereignissen in mittel- und osteuropäischen Kernkraftwerken planmäßig fortgesetzt und das laufende Projekt mit dem Abschlußbericht zum 31.12.1994 abgeschlossen.
Für die anstehenden Aufgaben, nämlich Abschätzung der Emissionen, Prognose der Radioaktivitätsausbreitung, Verfolgung der Lageentwicklung und Mitwirkung bei der Vorbereitung von Notfallschutzmaßnahmen sind im wesentlichen radiologische Meßwerte über die freigesetzten radioaktiven Stoffe und meteorologischen Kennwerte zur Beschreibung der Ausbreitungsbedingungen an das Zentrum zu übertragen. Betriebliche Informationen über den Anlagenzustand sind nur im Sinne von Hintergrundinformationen erforderlich, wozu 8 bis 10 ausgewählte sicherheitsrelevante Betriebsparameter ausreichend sind.

Obwohl der Sinn eines solchen Vorhabens außer Frage steht, sind die Realisierungschancen ohne eine umfassende Förderung durch die EG und andere internationale Organisationen - World Association of Nuclear Operators WANO, International Atomic Energy Agency IAEA - gering.]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-259-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:1849-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heinze, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1849-1</dc:identifier>
<dc:title><![CDATA[Konfiguration und Parametrierung eines Meßsystems zur Erfassung der Wärmeflüsse in einer Wohnsiedlung]]></dc:title>
<dc:source><![CDATA[Diplomarbeit Technische Universität Dresden, Institut für Energiemaschinen und Maschinenlabor, Dezember 1994 (Betreuer Dr. Naehring)]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Für die Wohnsiedlung Rossendorf wurde ein Meßsystem zur Erfassung der Wärmeflüsse für Heizung und Warmwaser entworfen, realisiert und erprobt. Zum Einsatz kam ein industrielles Meßsystem mit Prozeßrechner der Firma Johnson Controls. Durch Testmessungen wurde der Nachweis der Funktionsfähigkeit der Anlage erbracht. Als kritisch erwies sich die genaue Bestimmung der Wärme- bzw. Volumenströme.
]]></dc:description>
<dc:type>info:eu-repo/semantics/masterThesis</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1849-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1491-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Geipel, G.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Brendler, V.]]></dc:creator>
<dc:creator><![CDATA[Rutsch, M.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1491-1</dc:identifier>
<dc:title><![CDATA[Spectroscopic properties of Uranium(VI) minerals studied by time-resolved laser-induced fluorescence spectroscopy (TRLFS)]]></dc:title>
<dc:source><![CDATA[Migration´99, Conference Incline Village, CA]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[About 160 uranium minerals are known. Although many of these minerals show fluorescence properties, detailed fluorescence spectra are not published in the literature. We studied the fluorescence properties of 120 uranium minerals in order to provide a data base of potential solids that may form in the flooding process of defunct uranium mines.
]]></dc:description>
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<identifier>HZDR:PUBLDB:433-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Ortlepp, H.-G.]]></dc:creator>
<dc:creator><![CDATA[Wagner, W.]]></dc:creator>
<dc:creator><![CDATA[Dietterle, S.]]></dc:creator>
<dc:creator><![CDATA[Dshemuchadse, S.]]></dc:creator>
<dc:creator><![CDATA[Doronin, V. N.]]></dc:creator>
<dc:creator><![CDATA[Ivanovsky, S. I.]]></dc:creator>
<dc:creator><![CDATA[Kamanin, D. V.]]></dc:creator>
<dc:creator><![CDATA[Aleksandrov, A. A.]]></dc:creator>
<dc:creator><![CDATA[Aleksandrova, I. A.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-433-1</dc:identifier>
<dc:title><![CDATA[Spectroscopy of correlated fragments from the fission of hot nuclei performed at the FOBOS 4pi - array]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-102 Preprint]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1493-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kutschke, S.]]></dc:creator>
<dc:creator><![CDATA[Panak, P.]]></dc:creator>
<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1493-1</dc:identifier>
<dc:title><![CDATA[Charakterization of Thiobacillus isolates from a Uranium mining waste pile]]></dc:title>
<dc:source><![CDATA[BAGECO 6th Symposium, Florenz]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[In the natural bioleaching systems autochtonic microorganisms are involved in the solubilization of metals from solid minerals. The widest spreaded mesophilic group of bioleaching microorganisms are the chemolithoautotrophic bacteria Thiobacillus ferrooxidans, Thiobacillus thiooxidans, and Leptospirillum ferrooxidans. 
From soil samples drawn from two particular sites of a former uranium mine in Saxony, Germany, which were polluted in different extend with heavy metals, several Thiobacillus strains were cultured. Using ARDREA the strains were classified in two uranium-waste-site-specific 16S rDNA subgroups of the species Thiobacillus ferrooxidans. Moreover, RAPD and PFGE analyses have demonstrated that the natural T. ferrooxidans isolates possess also group-specific genomic organization. The strains from the more polluted sample were tolerant to higher concentrations of uranyl ions which were lethal for the isolates of the second group. In these strains the expression of at least three genes was influenced by the presence of uranyl ions. The uranium binding capability of the uranium mine isolates was strain-specific and higher than those of the reference T. ferrooxidans strains recovered from other environments.]]></dc:description>
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<identifier>HZDR:PUBLDB:1495-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Wober, J.]]></dc:creator>
<dc:creator><![CDATA[Flemming, K.]]></dc:creator>
<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1495-1</dc:identifier>
<dc:title><![CDATA[Classification of Desulfovibrio isolates recovered from a uranium mining waste pile]]></dc:title>
<dc:source><![CDATA[BAGECO 6th Symposium, Florenz]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[
A large variety of bacteria was demonstrated  to be present in soil and sediment samples of a uranium waste pile in Saxony, Germany. Anaerobic sulfate-reducing bacteria belonging to the genus Desulfovibrio were found among them. The study of these bacteria, which are also known to reduce U(VI), is of great importance for the development of bioremediation procedures for decontamination of the environments polluted with uranium. The indigenous for the waste Desulfovibrio isolates were classified by the use of Amplified Ribosomal DNA Restriction Endonucleases Analysis (ARDREA), Random Amplified Polymorphic DNA (RAPD), Repetitive Primer Amplified Polymorphic DNA (rep-APD), and 16S rDNA Sequence.
The 16S and IGS rDNA retrieval allowed us to affiliate the natural Desulfovibrio isolates to the subspecies Desulfovibrio vulgaris (oxamicus). Using RAPD and rep-APD analyses, the natural isolates were grouped in particular cluster which was not very closely related to the type strain D. vulgaris (oxamicus) 1925T. Results demonstrating the capability of the uranium waste isolates to reduce U(VI) to U(IV) will be presented.
]]></dc:description>
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<identifier>HZDR:PUBLDB:14530-2</identifier>
<datestamp>2025-06-05</datestamp>
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            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Lifante, C.]]></dc:creator>
<dc:creator><![CDATA[Frank, T.]]></dc:creator>
<dc:creator><![CDATA[Burns, A. D.]]></dc:creator>
<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14530-2</dc:identifier>
<dc:title><![CDATA[Prediction of polydisperse steam bubble condensation in sub-cooled water using the Inhomogeneous MUSIG model]]></dc:title>
<dc:source><![CDATA[CFD4NRS-3, Workshop on Experimental Validation and Application of CFD and CMFD Codes to Nuclear Reactor Safety Issues, 14.-16.09.2010, Washington D.C., USA]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The aim of this paper is to present the validation of a new methodology implemented in ANSYS CFX  (ANSYS, 2009), that extends the standard capabilities of the inhomogeneous MUltiple-SIze Group model (MUSIG) by additionally accounting for bubble size changes due to heat and mass transfer.  Bubble condensation plays an important role in sub-cooled boiling or steam injection into pools among many other applications of interest in the Nuclear Reactor Safety (NRS) area and other engineering areas. Since the mass transfer rate between phases is proportional to the interfacial area density, a polydisperse modelling approach considering different bubble sizes is of main importance, because an accurate prediction of the bubble diameter distribution is required. 
The standard MUSIG approach is an inhomogeneous one with respect to bubble velocities, which combines the size classes into different so-called velocity groups to precisely capture the different behaviour of the bubbles depending on their size. In the framework of collaboration between ANSYS and the Forschungszentrum Dresden-Rossendorf (FZD) an extension of the MUSIG model was developed, which allows to take into account the effect of mass transfer due to evaporation and condensation on the bubble size distribution changes in addition to breakup and coalescence effects. 
After the successful verification of the model, the next step was the validation of the new developed model against experimental data. For this purpose an experiment was chosen, which was investigated in detail at the TOPFLOW test facility at FZD. It consists of a steam bubble condensation case at 2MPa pressure in 3.9K sub-cooled water at a large diameter (DN200) vertical pipe. Sub-cooled water flows into the 195.3 mm wide and 8 m height pipe, were steam is injected at z=0.0 m and is recondensing. The experimental results are published in (Lucas, et al., 2007). Using a wire-mesh sensor technique the main characteristics of the two-phase flow were measured, i.e. radial steam volume fraction distribution and bubble diameter distribution at different heights and cross-sections. 
ANSYS CFX 12.0 was used for the numerical prediction. A 60 degrees pipe sector was modelled in order to save computational time, discretized into a mesh containing about 260.000 elements refined towards the pipe wall and towards the location of the steam injection nozzles. Interfacial forces due to drag, lift, turbulent dispersion and wall lubrication force were considered. The numerical results were compared to the experimental data. The agreement is highly satisfactory, proving the capability of the new MUSIG model extension to accurately predict such complex two-phase flow.]]></dc:description>
<dc:subject><![CDATA[polydisperse]]></dc:subject>
<dc:subject><![CDATA[bubble]]></dc:subject>
<dc:subject><![CDATA[condensation]]></dc:subject>
<dc:subject><![CDATA[phase transfer]]></dc:subject>
<dc:subject><![CDATA[CFD]]></dc:subject>
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<identifier>HZDR:PUBLDB:14530-1</identifier>
<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Lifante, C.]]></dc:creator>
<dc:creator><![CDATA[Frank, T.]]></dc:creator>
<dc:creator><![CDATA[Burns, A. D.]]></dc:creator>
<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14530-1</dc:identifier>
<dc:title><![CDATA[Prediction of polydisperse steam bubble condensation in sub-cooled water using the Inhomogeneous MUSIG model]]></dc:title>
<dc:source><![CDATA[CFD4NRS-3, Workshop on Experimental Validation and Application of CFD and CMFD Codes to Nuclear Reactor Safety Issues, paper 13.3, 14.-16.09.2010, Washington D.C., USA]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The aim of this paper is to present the validation of a new methodology implemented in ANSYS CFX  (ANSYS, 2009), that extends the standard capabilities of the inhomogeneous MUltiple-SIze Group model (MUSIG) by additionally accounting for bubble size changes due to heat and mass transfer.  Bubble condensation plays an important role in sub-cooled boiling or steam injection into pools among many other applications of interest in the Nuclear Reactor Safety (NRS) area and other engineering areas. Since the mass transfer rate between phases is proportional to the interfacial area density, a polydisperse modelling approach considering different bubble sizes is of main importance, because an accurate prediction of the bubble diameter distribution is required. 
The standard MUSIG approach is an inhomogeneous one with respect to bubble velocities, which combines the size classes into different so-called velocity groups to precisely capture the different behaviour of the bubbles depending on their size. In the framework of collaboration between ANSYS and the Forschungszentrum Dresden-Rossendorf (FZD) an extension of the MUSIG model was developed, which allows to take into account the effect of mass transfer due to evaporation and condensation on the bubble size distribution changes in addition to breakup and coalescence effects. 
After the successful verification of the model, the next step was the validation of the new developed model against experimental data. For this purpose an experiment was chosen, which was investigated in detail at the TOPFLOW test facility at FZD. It consists of a steam bubble condensation case at 2MPa pressure in 3.9K sub-cooled water at a large diameter (DN200) vertical pipe. Sub-cooled water flows into the 195.3 mm wide and 8 m height pipe, were steam is injected at z=0.0 m and is recondensing. The experimental results are published in (Lucas, et al., 2007). Using a wire-mesh sensor technique the main characteristics of the two-phase flow were measured, i.e. radial steam volume fraction distribution and bubble diameter distribution at different heights and cross-sections. 
ANSYS CFX 12.0 was used for the numerical prediction. A 60 degrees pipe sector was modelled in order to save computational time, discretized into a mesh containing about 260.000 elements refined towards the pipe wall and towards the location of the steam injection nozzles. Interfacial forces due to drag, lift, turbulent dispersion and wall lubrication force were considered. The numerical results were compared to the experimental data. The agreement is highly satisfactory, proving the capability of the new MUSIG model extension to accurately predict such complex two-phase flow.]]></dc:description>
<dc:subject><![CDATA[polydisperse]]></dc:subject>
<dc:subject><![CDATA[bubble]]></dc:subject>
<dc:subject><![CDATA[condensation]]></dc:subject>
<dc:subject><![CDATA[phase transfer]]></dc:subject>
<dc:subject><![CDATA[CFD]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:1497-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kutschke, S.]]></dc:creator>
<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1497-1</dc:identifier>
<dc:title><![CDATA[Molecular charakterization of Thiobacillus isolates recovered from a uranium mining waste pile]]></dc:title>
<dc:source><![CDATA[VAAM-Conference, Göttingen]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[
In natural bioleaching systems autochtonic microorganisms are involved in the solubilization of metals from solid minerals. The widest spreaded mesophilic group of bioleaching microorganisms are the chemolithoautotrophic bacteria Thiobacillus ferrooxidans, Thiobacillus thiooxidans and Leptospirillum ferrooxidans. 
From the soil samples of different sites and depths of a former uranium mine in Saxony, Germany, several Thiobacillus strains were cultured. They were classified by the use of the amplified ribosomal DNA restriction enzyme analysis (ARDREA). The genomic organization of the strains was investigated using random amplified polymorphic DNA (RAPD) and pulsed-field gel electrophoresis (PFGE). 
All strains were affiliated to the species T. ferrooxidans. Moreover, it was possible to distinguish members belonging to the two closely related phylogenetic groups of the species - one related to the reference strain T. ferrooxidans ATCC 33020 (recovered from a uranium mine) and a second one, related to the strain 21834 (recovered from a coal mine). 
By the use of the RAPD and PFGE fingerprinting methods it was demonstrated that the strains recovered from different depths differ in their genomic organization.]]></dc:description>
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<identifier>HZDR:PUBLDB:1498-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Wober, J.]]></dc:creator>
<dc:creator><![CDATA[Flemming, K.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, K.]]></dc:creator>
<dc:creator><![CDATA[Hard, B.]]></dc:creator>
<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1498-1</dc:identifier>
<dc:title><![CDATA[Classification of Desulfovibrio isolates recovered from a uranium mining weaste pile]]></dc:title>
<dc:source><![CDATA[VAAM-Conference, Göttingen]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[A large variety of bacteria was demonstrated  to be present in soil and sediment samples of a uranium waste pile in Saxony, Germany. Anaerobic sulfate-reducing bacteria belonging to the genus Desulfovibrio were found among them. The study of these bacteria, which are also known to reduce U(VI), is of great importance for the development of bioremediation procedures for decontamination of the environments polluted with uranium. The indigenous for the waste Desulfovibrio isolates were classified by the use of Amplified Ribosomal DNA Restriction Endonucleases Analysis (ARDREA), Random Amplified Polymorphic DNA (RAPD), Repetitive Primer Amplified Polymorphic DNA (rep-APD), 16S rDNA Sequencing, and as well as with classical microbiological methods.
Using 16S- and IGS-ARDREA the pile isolates were phylogenetically affiliated to Desulfovibrio vulgaris (oxamicus). The RAPD and rep-APD analyses have demonstrated a close genomic relationship between the pile isolates, but D. vulgaris (oxamicus) 1925T was not closely related to them. These results are in agreement to the taxonomic characterization of the strains by comparison of the fatty acid spectra. ]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:14508-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
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            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Beyer, M.]]></dc:creator>
<dc:creator><![CDATA[Szalinski, L.]]></dc:creator>
<dc:creator><![CDATA[Barthel, F.]]></dc:creator>
<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14508-1</dc:identifier>
<dc:title><![CDATA[Experimentelle Ergebnisse im Rahmen des TOPFLOW-II Projektes]]></dc:title>
<dc:source><![CDATA[CFD-Forschungsverbund, Entwicklung und Anwendung von Computational Fluid Dynamics (CFD) Programmen für Phänomene im Kühlkreislauf und Sicherheitseinschluss von Leichtwasserreaktoren, 23.09.2010, Grosshartpenning, Deutschland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Der Vortrag beschreibt die im TOPFLOW-II Projekt erzielten Ergebnisse und den Realisierungsstand der Arbeiten. Nach einer kurzen Einführung zu Ziel und Aufgabenstellung des Projektes, werden detailliert die Resultate der Kondensationsexperimente und erste Auswertungen der Messdaten erläutert. Hierbei wird auch zum Teil auf Einzeleffekte eingegangen und die Reproduzierbarkeit der Ergebnisse nachgewiesen. Eine Beschreibung der Druckentlastungsversuche und die Darstellung ausgewählter Messdaten sowie Vorschläge zur Datenauswertung schließen sich an. Nachfolgend wird der erreichte Stand bei den Messungen mit dem Schnellen Röntgentomographen an der Teststrecke Ti-Rohr DN50 für aufwärtsgerichtete Luft/Wasser-Strömungen vorgestellt. Eine Zusammenfassung und ein Überblick zur Projektrealisierung beenden den Vortrag.]]></dc:description>
<dc:subject><![CDATA[TOPFLOW]]></dc:subject>
<dc:subject><![CDATA[wire-mesh sensor]]></dc:subject>
<dc:subject><![CDATA[ROFEX]]></dc:subject>
<dc:subject><![CDATA[X-ray tomograph]]></dc:subject>
<dc:subject><![CDATA[CFD]]></dc:subject>
<dc:subject><![CDATA[two-phase flow]]></dc:subject>
<dc:subject><![CDATA[steam condensation]]></dc:subject>
<dc:subject><![CDATA[pressure release]]></dc:subject>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Nepijko, S. A.]]></dc:creator>
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<dc:creator><![CDATA[Freund, H.-J.]]></dc:creator>
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<dc:title><![CDATA[Local melting of the NiAl-substrate under deposited Pd-clusters during electron irradiation in a transmission electron microscope]]></dc:title>
<dc:source><![CDATA[Third International Conference 99 Sumy, Ukraine]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[We have shown that holes with diameters in the nanometer range may be created in the Al2O3/NiAl(110) substrate if metal clusters deposited on it are irradiated by the intense convergent electron beam in TEM. The localisation and size of holes can be controlled to some extend. The formation of holes can be interrupted by lowering the beam intensity below a critical value. It can be continued by increasing the intensity above the threshold value. We have also disclosed the necessity of clusters' presence on the surface for the start of holes' formation.]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Stefani, F.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1503-1</dc:identifier>
<dc:title><![CDATA[On the uniqueness of velocity reconstruction in conducting fluids from measurements of induced electromagnetic fields]]></dc:title>
<dc:source><![CDATA[Inverse Problems 16 (2000), pp. 1-9]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The problem of velocity reconstruction in conducting fluids from measurements of induced magnetic fields and electric potentials is discussed in spherical geometry.
Under the special case that the externally applied magnetic field is uniform and homogeneous throughout the fluid, the non-uniqueness problem is treated in detail. Assuming kinetic energy minimization for the moving fluid it is shown that the velocity field can be reconstructed completely. ]]></dc:description>
<dc:subject><![CDATA[Inverse Problems]]></dc:subject>
<dc:subject><![CDATA[Magnetohydrodynamics]]></dc:subject>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1504-1</dc:identifier>
<dc:title><![CDATA[Some Issues by Using the Master Curve Concept]]></dc:title>
<dc:source><![CDATA[Proc. of the 15th International Conference on Structural Mechanics in Reactor Technology (SmiRT-15), Seoul, Korea, August 1999, Vol. 5, p. 383-390]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The master curve concept allows to determine limit curves of fracture toughness for defined failure probabilities and a reference temperatures based on it. Thus fracture mechanical values can be supplied for the stress analysis. This paper presents the application of the master curve concept for the determination of the reference temperature over the thickness of a plate of RPV steel. It was shown that the master curve concept is applicable for the  fracture mechanical characterisation of material in different conditions using small test specimens. A special problem with the use small specimens is the definition of the test temperature, at which fracture toughness values can be determined within the validity limits. It became clear that the criteria for definition the test temperature and the minimum number of specimens indicated in the ASTM E1921-97 standard are applicable and sufficient respectively only for homogeneous materials.]]></dc:description>
<dc:subject><![CDATA[reactor pressure vessel steel]]></dc:subject>
<dc:subject><![CDATA[fracture mechanical assesment]]></dc:subject>
<dc:subject><![CDATA[trend curves]]></dc:subject>
<dc:subject><![CDATA[J-integral concept]]></dc:subject>
<dc:subject><![CDATA[fracture mechanical values]]></dc:subject>
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<identifier>HZDR:PUBLDB:1504-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1504-7</dc:identifier>
<dc:title><![CDATA[Some Issues by Using the Master Curve Concept]]></dc:title>
<dc:source><![CDATA[Proc. of the 15th International Conference on Structural Mechanics in Reactor Technology (SmiRT-15), Seoul, Korea, August 1999, Vol. 5, p. 383-390]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The master curve concept allows to determine limit curves of fracture toughness for defined failure probabilities and a reference temperatures based on it. Thus fracture mechanical values can be supplied for the stress analysis. This paper presents the application of the master curve concept for the determination of the reference temperature over the thickness of a plate of RPV steel. It was shown that the master curve concept is applicable for the  fracture mechanical characterisation of material in different conditions using small test specimens. A special problem with the use small specimens is the definition of the test temperature, at which fracture toughness values can be determined within the validity limits. It became clear that the criteria for definition the test temperature and the minimum number of specimens indicated in the ASTM E1921-97 standard are applicable and sufficient respectively only for homogeneous materials.]]></dc:description>
<dc:subject><![CDATA[reactor pressure vessel steel]]></dc:subject>
<dc:subject><![CDATA[fracture mechanical assesment]]></dc:subject>
<dc:subject><![CDATA[trend curves]]></dc:subject>
<dc:subject><![CDATA[J-integral concept]]></dc:subject>
<dc:subject><![CDATA[fracture mechanical values]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:1505-2</identifier>
<datestamp>2019-03-04</datestamp>
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</header>
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Ohlmeyer, H.]]></dc:creator>
<dc:creator><![CDATA[Otremba, F.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1505-2</dc:identifier>
<dc:title><![CDATA[Elastic plastic finite element analysis of a BWR feed water distributor exposed to an extreme pressure load]]></dc:title>
<dc:source><![CDATA[15-th International Conference on Structural Mechanics in Nuclear Technology (SMIRT-15), Seoul, Korea, August 15-20 1999, Proceedings Vol. VII pp. 177-184]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[During a hypothetical break of a BWR feed water line, the feed water distributor (FWD) inside the RPV is subjected to a high pressure load for a short time (10 ms). Because of the sudden coolant release from the inner volume of the FWD there is a  pressure difference between the inner and outer surface. It is conservatively assumed that the pressure difference nearly can reach the operating pressure for a few milliseconds. The distributor box and the ring line of the feed water distributor are modelled with shell and volume elements capable of being used for large strain analyses with elastic-plastic material behaviour. It is demonstrated by non-linear static calculations (without consideration of the inertia of the material) that a buckling instability occurs at about 60% and 80% of the maximum pressure load. The arc-length method is used for the numerical solution to overcome these points of instability. To evaluate the influence of the dynamics of the process a non-linear transient analysis is done showing that the maximum strain occurs with a time delay to the pressure peak. The maximum plastic strain differs only insignificantly between static and transient solution. Inspite of the large strains the mechanical integrity is maintained during the hypothetical event.]]></dc:description>
<dc:subject><![CDATA[BWR]]></dc:subject>
<dc:subject><![CDATA[Finite element analysis]]></dc:subject>
<dc:subject><![CDATA[Large strain]]></dc:subject>
<dc:subject><![CDATA[Plasticity]]></dc:subject>
<dc:subject><![CDATA[Transient analysis]]></dc:subject>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Ohlmeyer, H.]]></dc:creator>
<dc:creator><![CDATA[Otremba, F.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1505-7</dc:identifier>
<dc:title><![CDATA[Elastic plastic finite element analysis of a BWR feed water distributor exposed to an extreme pressure load]]></dc:title>
<dc:source><![CDATA[15-th International Conference on Structural Mechanics in Nuclear Technology (SMIRT-15), Seoul, Korea, August 15-20 1999, Proceedings Vol. VII pp. 177-184]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[During a hypothetical break of a BWR feed water line, the feed water distributor (FWD) inside the RPV is subjected to a high pressure load for a short time (10 ms). Because of the sudden coolant release from the inner volume of the FWD there is a  pressure difference between the inner and outer surface. It is conservatively assumed that the pressure difference nearly can reach the operating pressure for a few milliseconds. The distributor box and the ring line of the feed water distributor are modelled with shell and volume elements capable of being used for large strain analyses with elastic-plastic material behaviour. It is demonstrated by non-linear static calculations (without consideration of the inertia of the material) that a buckling instability occurs at about 60% and 80% of the maximum pressure load. The arc-length method is used for the numerical solution to overcome these points of instability. To evaluate the influence of the dynamics of the process a non-linear transient analysis is done showing that the maximum strain occurs with a time delay to the pressure peak. The maximum plastic strain differs only insignificantly between static and transient solution. Inspite of the large strains the mechanical integrity is maintained during the hypothetical event.]]></dc:description>
<dc:subject><![CDATA[BWR]]></dc:subject>
<dc:subject><![CDATA[Finite element analysis]]></dc:subject>
<dc:subject><![CDATA[Large strain]]></dc:subject>
<dc:subject><![CDATA[Plasticity]]></dc:subject>
<dc:subject><![CDATA[Transient analysis]]></dc:subject>
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<identifier>HZDR:PUBLDB:2665-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kachurin, G. A.]]></dc:creator>
<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Zhuravlev, K. S.]]></dc:creator>
<dc:creator><![CDATA[Pazdnikov, N. A.]]></dc:creator>
<dc:creator><![CDATA[Volodin, V. A.]]></dc:creator>
<dc:creator><![CDATA[Gutakovskii, A. G.]]></dc:creator>
<dc:creator><![CDATA[Leier, A. F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2665-1</dc:identifier>
<dc:title><![CDATA[Photo-luminescence from SiO<SUB>2</SUB> layers implanted with Si<SUP>+</SUP> and annealed in a pulse regime]]></dc:title>
<dc:source><![CDATA[Phys. Techn. Semicond. 31/No. 6 (1997) 730 (in Russian)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kachurin, G. A.]]></dc:creator>
<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Zhuravlev, K. S.]]></dc:creator>
<dc:creator><![CDATA[Pazdnikov, N. A.]]></dc:creator>
<dc:creator><![CDATA[Volodin, V. A.]]></dc:creator>
<dc:creator><![CDATA[Gutakovskii, A. G.]]></dc:creator>
<dc:creator><![CDATA[Leier, A. F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2665-2</dc:identifier>
<dc:title><![CDATA[Photo-luminescence from SiO<SUB>2</SUB> layers implanted with Si<SUP>+</SUP> and annealed in a pulse regime]]></dc:title>
<dc:source><![CDATA[Semicond. 31/No. 6 (1997) 626 ( English version)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1566-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Höhne, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1566-2</dc:identifier>
<dc:title><![CDATA[1:5 scaled Plexiglas Mixing Model of the PWR Konvoi]]></dc:title>
<dc:source><![CDATA[International Conference on Nuclear Engineering (ICONE-7), April 19-23,1999, Tokio, Japan]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The coolant mixing in the downcomer and lower plenum depends significantly on the construction of the reactor vessel and on the instantaneous flow conditions. Therefore the Institute for Safety Research of Forschungszentrum Rossendorf has constructed a 1:5 mixing test facility representing the geometry of the German Konvoi type pressurized water reactor. The mock-up of the test facility and the measuring systems are explained in the poster.]]></dc:description>
<dc:subject><![CDATA[PWR]]></dc:subject>
<dc:subject><![CDATA[Coolant Mixing]]></dc:subject>
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<identifier>HZDR:PUBLDB:1566-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Höhne, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1566-1</dc:identifier>
<dc:title><![CDATA[1:5 scaled Plexiglas Mixing Model of the PWR Konvoi]]></dc:title>
<dc:source><![CDATA[International Conference on Nuclear Engineering (ICONE-7), April 19-23 1999, Tokio, Japan]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The coolant mixing in the downcomer and lower plenum depends significantly on the construction of the reactor vessel and on the instantaneous flow conditions. Therefore the Institute for Safety Research of Forschungszentrum Rossendorf has constructed a 1:5 mixing test facility representing the geometry of the German Konvoi type pressurized water reactor. The mock-up of the test facility and the measuring systems are explained in the poster.]]></dc:description>
<dc:subject><![CDATA[PWR]]></dc:subject>
<dc:subject><![CDATA[Coolant Mixing]]></dc:subject>
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<identifier>HZDR:PUBLDB:2458-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2458-1</dc:identifier>
<dc:title><![CDATA[Nitrierung austenitischer Edelstähle mittels Plasma-Immersions-Ionenimplantation]]></dc:title>
<dc:source><![CDATA[OWT-97, Chemnitz, June 16-18, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<identifier>HZDR:PUBLDB:2459-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
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<dc:creator><![CDATA[Romano-Rodriguez, A.]]></dc:creator>
<dc:creator><![CDATA[Kögler, R.]]></dc:creator>
<dc:creator><![CDATA[Bachrouri, A.]]></dc:creator>
<dc:creator><![CDATA[Perez-Rodriguez, A.]]></dc:creator>
<dc:creator><![CDATA[Serre, C.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Calvo-Barrio, L.]]></dc:creator>
<dc:creator><![CDATA[Morante, J. R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2459-1</dc:identifier>
<dc:title><![CDATA[Influence of the substrate structure (SIMOX, bulk Si) on the SiC synthesis by high dose carbon implantation]]></dc:title>
<dc:source><![CDATA[7th Int. Conf. on Gettering and Defect Engineering in Semiconductor Technology, GADEST'97, Spa, Belgium, Oct. 5-10, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2460-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Markwitz, A.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Nitzsche, P.]]></dc:creator>
<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
<dc:creator><![CDATA[Seifarth, H.]]></dc:creator>
<dc:creator><![CDATA[Strobel, M.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2460-1</dc:identifier>
<dc:title><![CDATA[Dünnschichtsysteme für die Photo- und Elektrolumineszenz]]></dc:title>
<dc:source><![CDATA[Photonik-Symposium, Würzburg, Oct. 8 - 10, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:1766-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bergmann, U.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Bergner, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1766-1</dc:identifier>
<dc:title><![CDATA[Ultraschallverfahren zur Messung des duktilen Rißfortschritts bei quasistatischer Dreipunktbiegung]]></dc:title>
<dc:source><![CDATA[27. Vortragsveranstaltung des DVM-Arbeitskreises Bruchvorgänge, Köln, 14. - 15. Februar 1995, Proc. S. 177]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Es wird ein Ultraschall-Laufzeit-Bewegungsverfahren vorgestellt, mit dem der duktile Rißfortschritt in 3-Punkt-Biegeproben kleiner Abmessungen gemessen werden kann. Das Verfahren erfüllt die Genauigkeitsanforderungen nach DIN 54120 und arbeitet quasikontinuierlich. ]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:bookPart</dc:type>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1568-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Willschütz, H.-G.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1568-1</dc:identifier>
<dc:title><![CDATA[CFD-Calculations to a Core Catcher Benchmark]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-257 April 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[There are numerous experiments for the exploration of the corium spreading behaviour, but comparable data have not been available up to now in the field of the long term behaviour of a corium expanded in a core catcher. The difficulty consists in the experimental simulation of the decay heat that can be neglected for the short-run course of events like relocation and spreading, which must, however, be considered during investigation of the long time behaviour.
Therefore the German GRS, defined together with Battelle Ingenieurtechnik a benchmark problem in order to determine particular problems and differences of CFD codes simulating an expanded corium and from this, requirements for a reasonable measurement of experiments, that will be performed later.
First the finite-volume-codes Comet 1.023, CFX 4.2 and CFX-TASCflow were used. To be able to make comparisons to a finite-element-code, now calculations are performed at the Institute of Safety Research at the Forschungszentrum Rossendorf with the code ANSYS/FLOTRAN.For the benchmark calculations of stage 1 a pure and liquid melt with internal heat sources was assumed uniformly distributed over the area of the planned core catcher of a EPR plant.
Using the Standard-k-e-turbulence model and assuming an initial state of a motionless superheated melt several large convection rolls will establish within the melt pool. The temperatures at the surface do not sink to a solidification level due to the enhanced convection heat transfer. The temperature gradients at the surface are relatively flat
while there are steep gradients at the ground where the no slip condition is applied. But even at the ground no  solidification temperatures are observed.
Although the problem in the ANSYS-calculations is handled two-dimensional and not three-dimensional like in the finite-volume-codes, there are no fundamental deviations to the results of the other codes.]]></dc:description>
<dc:subject><![CDATA[corium pool]]></dc:subject>
<dc:subject><![CDATA[internal heat sources]]></dc:subject>
<dc:subject><![CDATA[CFD-Calculations with different codes]]></dc:subject>
<dc:subject><![CDATA[long term behaviour]]></dc:subject>
<dc:subject><![CDATA[core catcher]]></dc:subject>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1463-1</identifier>
<datestamp>2025-02-12</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Noetzel, J.]]></dc:creator>
<dc:creator><![CDATA[Geisler, H.]]></dc:creator>
<dc:creator><![CDATA[Brand, K.]]></dc:creator>
<dc:creator><![CDATA[Gorbunov, A.]]></dc:creator>
<dc:creator><![CDATA[Tselev, A.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1463-1</dc:identifier>
<dc:title><![CDATA[Structural investigations of laser-deposited Fe/Al multilayers]]></dc:title>
<dc:source><![CDATA[Applied Physics A Vol. 68, No. 5 (1999), pp. 497-503]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Fe/Al multilayers are prepared by crossed-beam pulsed laser deposition and investigated by Rutherford backscattering, conversion electron Mössbauer spectroscopy and transmission electron microscopy. The
results are compared with purely ballistic simulations of the deposition process using the TRIYDN4.0 code. It is found that the intermixing of adjacent layers must be decribed in terms of ballistic mixing followed
by chemical mixing. The phase build-up in the transition layer between adjacent layers follows the non-equilibrium behaviour of Fe/Al in analogy to investigations on mechanically alloyed and ion-beam mixed Fe/Al. In
Fe-rich areas a bcc-solid-solution is formed. In Al-rich environment an amorphous phase is observed.]]></dc:description>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1007/s003390050932]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1463-1</dc:relation>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1569-1</identifier>
<datestamp>2019-03-04</datestamp>
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            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:creator><![CDATA[Jäger, H.-U.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1569-1</dc:identifier>
<dc:title><![CDATA[Institute of Ion Beam Physics and Materials Research; Annual Report 1998]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-253 März 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1570-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Strobel, M.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1570-2</dc:identifier>
<dc:title><![CDATA[Can core/shell nanocrystals be formed by sequential ion implantation? Predictions from kinetic lattice Monte Carlo simulations]]></dc:title>
<dc:source><![CDATA[11th Int. Conf. on Ion Beam Modification of Materials, Amsterdam, The Netherlands,
Aug. 31 - Sept. 4, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:audience>Students</dc:audience>
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<identifier>HZDR:PUBLDB:1570-1</identifier>
<datestamp>2024-12-18</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Strobel, M.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1570-1</dc:identifier>
<dc:title><![CDATA[Can core/shell nanocrystals be formed by sequential ion implantation? Predictions from kinetic lattice Monte Carlo simulations]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 148 (1999) 104-109]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0168-583X(98)00784-8]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1570-1</dc:relation>
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<header>
<identifier>HZDR:PUBLDB:1575-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1575-2</dc:identifier>
<dc:title><![CDATA[Plasma based ion implantation]]></dc:title>
<dc:source><![CDATA[NATO ASI, "Advanced Technologies Based on Wave and Beam Generated Plasmas", 
Sozopol, Bulgaria, May 28 - 30, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1575-2</dc:relation>
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<header>
<identifier>HZDR:PUBLDB:1575-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1575-1</dc:identifier>
<dc:title><![CDATA[Plasma based ion implantation]]></dc:title>
<dc:source><![CDATA[H. Schlüter and A. Shivarova (eds.): Advanced Technologies Based on Wave and Beam Generated Plasmas, 191-244, 1999 Kluwer Academic Publishers]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1577-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1577-1</dc:identifier>
<dc:title><![CDATA[3D Nodal Expansion Method HEXNEM for Solution of the Neutron Diffusion Equation in Hexagonal Geometry]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik '99, 18. - 20. Mai, 1999, Karlsruhe, S. 15 - 18]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The nodal expansion method (NEM) used in the hexagonal version of the code DYN3D is based on the node averaged values of fluxes in the node volume and averaged values of fluxes and currents at the interfaces of the nodes [1]. The 3-dimensional neutron diffusion equation for two energy groups is split into a 2-dimensional equation in the hexagonal plane solved with the help of Bessel functions and a 1-dimensional equation in axial direction solved by polynomial expansion. The two equation systems are coupled by the transversal bucklings. The accuracy of this method is sufficient  for the VVER-440 where the assembly pitch is 14.7 cm. The assemblies of the VVER-1000 have a larger pitch of 24.1 cm. Comparing with mathematical benchmarks for the VVER-1000 the maximal deviation of powers is in the order of 5%. The new nodal expansion method HEXNEM presented here uses a different flux expansion in the nodes. In addition to the average values at the interfaces of the hexagon the values at the corner points are included, too. It is shown that the accuracy is improved for the VVER-1000 problems.]]></dc:description>
<dc:subject><![CDATA[neutron diffusion theory]]></dc:subject>
<dc:subject><![CDATA[nodal method]]></dc:subject>
<dc:subject><![CDATA[hexagonal geometry]]></dc:subject>
<dc:subject><![CDATA[two energy groups]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1577-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1577-7</dc:identifier>
<dc:title><![CDATA[3D Nodal Expansion Method HEXNEM for Solution of the Neutron Diffusion Equation in Hexagonal Geometry]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik '99, 18. - 20. Mai, 1999, Karlsruhe, S. 15 - 18]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The nodal expansion method (NEM) used in the hexagonal version of the code DYN3D is based on the node averaged values of fluxes in the node volume and averaged values of fluxes and currents at the interfaces of the nodes [1]. The 3-dimensional neutron diffusion equation for two energy groups is split into a 2-dimensional equation in the hexagonal plane solved with the help of Bessel functions and a 1-dimensional equation in axial direction solved by polynomial expansion. The two equation systems are coupled by the transversal bucklings. The accuracy of this method is sufficient  for the VVER-440 where the assembly pitch is 14.7 cm. The assemblies of the VVER-1000 have a larger pitch of 24.1 cm. Comparing with mathematical benchmarks for the VVER-1000 the maximal deviation of powers is in the order of 5%. The new nodal expansion method HEXNEM presented here uses a different flux expansion in the nodes. In addition to the average values at the interfaces of the hexagon the values at the corner points are included, too. It is shown that the accuracy is improved for the VVER-1000 problems.]]></dc:description>
<dc:subject><![CDATA[neutron diffusion theory]]></dc:subject>
<dc:subject><![CDATA[nodal method]]></dc:subject>
<dc:subject><![CDATA[hexagonal geometry]]></dc:subject>
<dc:subject><![CDATA[two energy groups]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<header>
<identifier>HZDR:PUBLDB:3099-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kögler, R.]]></dc:creator>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Kaschny, J. R.]]></dc:creator>
<dc:creator><![CDATA[Werner, P.]]></dc:creator>
<dc:creator><![CDATA[Danilin, A. B.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3099-1</dc:identifier>
<dc:title><![CDATA[Detection of metastable defective regions in ion-implanted Si by means of metal gettering]]></dc:title>
<dc:source><![CDATA[MRS Symp. Proc. 469 (1997) 224]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:3098-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ulbricht, A.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Nikolaev, Y.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3098-1</dc:identifier>
<dc:title><![CDATA[Nachweis und Analyse neutroneninduzierter Defektstrukturen in Eisenlegierungen]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik 2000, Bonn, 23.-25. Mai, Tagungsbericht S. 587]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Nach Bestrahlung unter WWER-Reaktor-typischen Bedingungen werden an Testlegierungen mikrostrukturelle Veränderungen mit Neutronenkleinwinkelstreuung untersucht und dabei gezielt der Einfluß, der als versprödungsfördernd geltende Elemente Cu, P und Ni, herausgearbeitet.]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:3098-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ulbricht, A.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Nikolaev, Y.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3098-7</dc:identifier>
<dc:title><![CDATA[Nachweis und Analyse neutroneninduzierter Defektstrukturen in Eisenlegierungen]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik 2000, Bonn, 23.-25. Mai, Tagungsbericht S. 587]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Nach Bestrahlung unter WWER-Reaktor-typischen Bedingungen werden an Testlegierungen mikrostrukturelle Veränderungen mit Neutronenkleinwinkelstreuung untersucht und dabei gezielt der Einfluß, der als versprödungsfördernd geltende Elemente Cu, P und Ni, herausgearbeitet.]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:1821-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Noll, B.]]></dc:creator>
<dc:creator><![CDATA[Noll, S.]]></dc:creator>
<dc:creator><![CDATA[Hilger, C. S.]]></dc:creator>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Syhre, R.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1821-1</dc:identifier>
<dc:title><![CDATA[Derivates of 6-methyl-8alpha-amino-ergoline: Sythesis and affinity to the dopamine D<SUB>2</SUB> receptor]]></dc:title>
<dc:source><![CDATA[Technetium, Rhenium and Other Metals in Chemistry and Nuclear Medicine
(Edited by Nicolini M., Mazzi U.) SGE Editoriali Padova (1999) pp. 237-240]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Organic derivatives  (2)  of 6-methyl-8alpha-amino-ergoline  1  and derived complexes of rhenium  (3,5)  and technetium  (4)  have been prepared and evaluated with regard to their affinity to the dopamine D<SUB>2</SUB> receptor. The molecular structure of the rhenium complex  3  was determined. The affinity of the benzoyl derivative  2b  is comparable with that of terguride (IC<SUB>50</SUB> values 2.7 for  2b  vs. 4.8 nMol), while the affinities of the related Tc and Re complexes are in the range from 54 to 165 nMol.]]></dc:description>
<dc:type>info:eu-repo/semantics/book</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:book</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1821-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:1822-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Noll, B.]]></dc:creator>
<dc:creator><![CDATA[Noll, S.]]></dc:creator>
<dc:creator><![CDATA[Leibnitz, P.]]></dc:creator>
<dc:creator><![CDATA[Jankowsky, R.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1822-1</dc:identifier>
<dc:title><![CDATA[Tc(V) and Re(V) complexes with Mercaptoacetylglysine (MAG<SUB>1</SUB>]]></dc:title>
<dc:source><![CDATA[Technetium, Rhenium and Other Metals in Chemistry and Nuclear Medicine
(Edited by Nicolini M., Mazzi U.) SGE Editoriali Padova (1999) pp. 241-244]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Mercaptoacetyl glycine (MAG<SUB>1</SUB>)  (1)  forms, in the presence of appropriate monodentate ligands, tridentate/monodentate (3+1) coordinated complexes with Tc(V) and Re(V). Exchange of the chlorine by monodentate ligands in [MO(MAG<SUB>1</SUB>)Cl]<SUP>-</SUP>  (2)  gives access to new mixed-ligand complexes [MO(MAG<SUB>1</SUB>)(XR)]  (3) . Some representatives have been prepared and characterized by elemental analysis, ir and uv spectroscopy and EXAFS. Thiobenzoate as monodentate ligand gives the complex  (4)  that, after debenzoylation, reacts with halogen containing compounds under displacement of the halogen by a [MO(SNO)S] moiety.]]></dc:description>
<dc:type>info:eu-repo/semantics/book</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:book</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1822-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1823-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Wüst, F.]]></dc:creator>
<dc:creator><![CDATA[Skaddan, M. B.]]></dc:creator>
<dc:creator><![CDATA[Carlson, K. E.]]></dc:creator>
<dc:creator><![CDATA[Leibnitz, P.]]></dc:creator>
<dc:creator><![CDATA[Katzenellenbogen, J. A.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1823-1</dc:identifier>
<dc:title><![CDATA[Synthesis and receptor binding of novel progestin-rhenium complexes]]></dc:title>
<dc:source><![CDATA[Technetium, Rhenium and Other Metals in Chemistry and Nuclear Medicine
(Edited by Nicolini M., Mazzi U.) SGE Editoriali Padova (1999) pp. 491-495]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[A series of rhenium "n+1" mixed-ligand, thioether-carbonyl and organometallic complexes of 21-substituted progesterone have been synthesized. The conjugates contain the rhenium metal at several oxidation states, being +5, +3 and +1. The complexes were used in a competitive receptor-binding assay (rat-uterus, 0°C) to determine their binding to the progesterone receptor. The best affinity of 9% (RU 5020=100%) was obtained with a "3+1" mixed-ligand complex, containing a NMe group as the central donor atom in the tridentate ligand part.  ]]></dc:description>
<dc:type>info:eu-repo/semantics/book</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:book</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1823-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1824-1</identifier>
<datestamp>2023-05-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kniess, T.]]></dc:creator>
<dc:creator><![CDATA[Noll, S.]]></dc:creator>
<dc:creator><![CDATA[Noll, B.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1824-1</dc:identifier>
<dc:title><![CDATA[Effective coupling of Re/Tc-MAG<SUB>3</SUB> complexes with amines and nucleobases in aprotic solvents.]]></dc:title>
<dc:source><![CDATA[Journal of Radioanalytical and Nuclear Chemistry, 240, No. 2 (1999), 657-660]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The coupling of Re- and <SUP>99m</SUP>Tc-MAG<SUB>3</SUB> complexes with amines and nucleobases was carried out with good yields using O-(benzotriazol-1-yl-)N,N,N',N'-tetramethyl-
uronium-tetrafluoroborate (TBTU), and base in polar aprotic solvents (NMP, DMF, DMSO). The one step reaction followed by simple gel chromatography makes the method well appropriate for preparations at the low no-carrier-added level of technetium-99m.]]></dc:description>
<dc:subject><![CDATA[Re/Tc-MAG3]]></dc:subject>
<dc:subject><![CDATA[nucleobases]]></dc:subject>
<dc:subject><![CDATA[coupling]]></dc:subject>
<dc:subject><![CDATA[TBTU]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1007/BF02349428]]></dc:relation>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1828-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Schäfer, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1828-1</dc:identifier>
<dc:title><![CDATA[Post-Test Calculations of the IAEA-SPE4]]></dc:title>
<dc:source><![CDATA[Proc. 2. SPE-4 Workshop, Budapest, May 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[In the Research Center Rossendorf post test calculations of the SPE4 were performed using the thermohydraulic code ATHLET. The SPE-4 experiment was a small break loss of coolant accident in the cold leg with unavailable high pressure injection system. For the prevention of core damage the secondary side bleed and feed was used. The experiment was performed at the Hungarian PMK-2 test facility, modelling the Paks VVER-440 reactor. In the calulations different nodalizations were tested for modelling the hydroaccumulators and the horizontal steam generator. Deviations between calculation and experiment were observed especially in the primary pressure decay and consequently in the behaviour of accumulator injection. It was found, that the prediction of observed core dry out depends on the correct calculation of the low pressure injection setpoint.]]></dc:description>
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<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1828-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Schäfer, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1828-7</dc:identifier>
<dc:title><![CDATA[Post-Test Calculations of the IAEA-SPE4]]></dc:title>
<dc:source><![CDATA[Proc. 2. SPE-4 Workshop, Budapest, May 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[In the Research Center Rossendorf post test calculations of the SPE4 were performed using the thermohydraulic code ATHLET. The SPE-4 experiment was a small break loss of coolant accident in the cold leg with unavailable high pressure injection system. For the prevention of core damage the secondary side bleed and feed was used. The experiment was performed at the Hungarian PMK-2 test facility, modelling the Paks VVER-440 reactor. In the calulations different nodalizations were tested for modelling the hydroaccumulators and the horizontal steam generator. Deviations between calculation and experiment were observed especially in the primary pressure decay and consequently in the behaviour of accumulator injection. It was found, that the prediction of observed core dry out depends on the correct calculation of the low pressure injection setpoint.]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:1579-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Grosse, E.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1579-1</dc:identifier>
<dc:title><![CDATA[Proceedings of the Miniworkshop "Electromagnetic Radiation off Colliding Hadron Systems: Dileptons and Bremsstrahlung"]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-258 April 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Since several years various groups of the Institute of Nuclear und Hadron Physics at Forschungszentrurn Rossendorf (FZR) are involved in medium energy physics projects where electromagnetic signals play a role:
(i) pp bremsstrahlung experiments at COSY-ToF have been proposed by a group from Dresden with FZR participation, and a large part of the ToF detector system has been
built in Rossendorf. 
(ii) The FZR is presently building one of the large wire chamber planes for the HADES detector at GSI and is also actively taking part in the HADES commissioning.
(iii) The theory group here at Rossendorf is working in the field of dilepton production and other electromagnetic processes. 
To discuss the research in these fields with colleagues from other places and to coordinate the efforts this mini-workshop was organized. The idea was to discuss the results of the experiments at different accelerators, the status of the calculations and the plans for future investigations. Besides bremsstrahlung special emphasis will be on dielectron production; other processes with electromagnetic signals (like vector-meson production) have also been discussed.]]></dc:description>
<dc:type>info:eu-repo/semantics/preprint</dc:type>
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<dc:type>doc-type:report</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:864-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Jahnke, U.]]></dc:creator>
<dc:creator><![CDATA[Bohne, W.]]></dc:creator>
<dc:creator><![CDATA[Eades, J.]]></dc:creator>
<dc:creator><![CDATA[Egidy, T.]]></dc:creator>
<dc:creator><![CDATA[Figuera, P.]]></dc:creator>
<dc:creator><![CDATA[Fuchs, H.]]></dc:creator>
<dc:creator><![CDATA[Galin, J.]]></dc:creator>
<dc:creator><![CDATA[Goldenbaum, F.]]></dc:creator>
<dc:creator><![CDATA[Gulda, K.]]></dc:creator>
<dc:creator><![CDATA[Golubeva, Y. S.]]></dc:creator>
<dc:creator><![CDATA[Hartmann, F. J.]]></dc:creator>
<dc:creator><![CDATA[Hilscher, D.]]></dc:creator>
<dc:creator><![CDATA[Iljinov, A. S.]]></dc:creator>
<dc:creator><![CDATA[Jastrzebski, J.]]></dc:creator>
<dc:creator><![CDATA[Kurcewicz, W.]]></dc:creator>
<dc:creator><![CDATA[Lott, B.]]></dc:creator>
<dc:creator><![CDATA[Morjean, M.]]></dc:creator>
<dc:creator><![CDATA[Pausch, G.]]></dc:creator>
<dc:creator><![CDATA[Péghaire, A.]]></dc:creator>
<dc:creator><![CDATA[Pienkowski, L.]]></dc:creator>
<dc:creator><![CDATA[Polster, D.]]></dc:creator>
<dc:creator><![CDATA[Proschitzki, S.]]></dc:creator>
<dc:creator><![CDATA[Quednau, B.]]></dc:creator>
<dc:creator><![CDATA[Rossner, H.]]></dc:creator>
<dc:creator><![CDATA[Schmid, S.]]></dc:creator>
<dc:creator><![CDATA[Schmid, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-864-1</dc:identifier>
<dc:title><![CDATA[Production and decay of hot nuclei following antiproton annihilation at rest and in flight]]></dc:title>
<dc:source><![CDATA[Jadernaja fizika 59 (1996) 9 pp, 1625-1634]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1834-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barz, H.-U.]]></dc:creator>
<dc:creator><![CDATA[Böhmer, B.]]></dc:creator>
<dc:creator><![CDATA[Konheiser, J.]]></dc:creator>
<dc:creator><![CDATA[Stephan, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1834-1</dc:identifier>
<dc:title><![CDATA[Aufgaben und Probleme bei der Bestimmung der Neutronenbelastung für den WWER-1000]]></dc:title>
<dc:source><![CDATA[5. Deutsch-Russisches WTZ-Seminar der Arbeitsgruppe Komponentensicherheit, Stuttgart, 03. - 05. Oktober 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Es werden Erfahrungen der auf diesem Gebiet tätigen Mitarbeiter in Rossendorf bei der Berechnung und Messung von Neutronenfluenzen sowie bei der Anwendung der Spektrumsjustierung dargelegt. An Hand dieser Erfahrungen wird auf noch offene Probleme eingegangen, die insbesondere bei neutronendosimetrischen Problemen zum Reaktor WWER-1000 auftreten. Es werden Möglichkeiten zur Bewältigung dieser Probleme diskutiert und auf eigene Vorstellungen eingegangen. Insbesondere wird betont, daß man mit Hilfe moderner Verfahren der Varianzreduktion die genaue 3-dimensionale Monte-Carlo Methode als Standardverfahren für die Transportrechnungen anwenden kann.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:language>ger</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1838-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1838-1</dc:identifier>
<dc:title><![CDATA[Contactless Control of Nonlinear Flow Phenomena in the Czochralski Crystal Growth of Silicon by Use of Magnetic Fields]]></dc:title>
<dc:source><![CDATA[Workshop Potential of Nonlinear Dynamics for Technological Applications, BMFT-VDI, Frankfurt/M., 24.11.1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Control of melt motions is important for most of the crystal growth technologies in order to improve the crystal quality and the yield. There were several attempts in the past to use steady magnetic fields for a damping of instabilities. Much more possibilities for flow control exist if unsteady magnetic fields are used, preferably in combination with steady fields. This new active melt control is attractive for industrial use. Principal mechanisms of this type of flow control are presented in this lecture, particularly adressed to the needs of the Si-Cz-technology. The research project is developed together with the institute of physics Riga and Wacker Chemitronics Ltd. Burghausen]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1841-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1841-1</dc:identifier>
<dc:title><![CDATA[Magnetohydrodynamic Flow Around a Circular Cylinder - Numerical Simulation up to Renolds numbers of 1000]]></dc:title>
<dc:source><![CDATA[DFG-Kolloquium, Bonn, 24.06.1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1841-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1035-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Friebe, M.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:creator><![CDATA[Mohammed, A.]]></dc:creator>
<dc:creator><![CDATA[Eisenhut, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1035-1</dc:identifier>
<dc:title><![CDATA[Präparation und In-Vivo-Testung von Melanom-affinen '3+1' (<SUP>99m</SUP>Tc)-Oxotechnetium(V)-Gemischt-Ligandkomplexen]]></dc:title>
<dc:source><![CDATA[DGN-Tagung, 36. Internationale Jahrestagung, Leipzig, 01.-04. April 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1035-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1035-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Friebe, M.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:creator><![CDATA[Mohammed, A.]]></dc:creator>
<dc:creator><![CDATA[Eisenhut, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1035-2</dc:identifier>
<dc:title><![CDATA[Präparation und In-Vivo-Testung von Melanom-affinen '3+1' (<SUP>99m</SUP>Tc)-Oxotechnetium(V)-Gemischt-Ligandkomplexen]]></dc:title>
<dc:source><![CDATA[Nuklearmedizin 37 (1998) A49]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1035-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<header>
<identifier>HZDR:PUBLDB:2399-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Strobel, M.]]></dc:creator>
<dc:creator><![CDATA[Palard, M.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:creator><![CDATA[Markwitz, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2399-1</dc:identifier>
<dc:title><![CDATA[Predictive simulations of high-dose ion implantation]]></dc:title>
<dc:source><![CDATA[Int. Workshop on Challenges in Predictive Process Simulation (ChiPPS '97), Wandlitz, Germany, Aug. 17 - 20, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1846-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, U.]]></dc:creator>
<dc:creator><![CDATA[Richter, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1846-1</dc:identifier>
<dc:title><![CDATA[Zusammenhang zwischen bruchmechanischen und mechanisch-technologischen Kennwerten für Reaktordruckbehälterstähle]]></dc:title>
<dc:source><![CDATA[Werkstoffprüfung '94, Bad Nauenheim, 01. - 02. Dezember 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Im Rahmen der wissenschaftlich-technischen Zusammenarbeit zwischen Deutschland und Rußland und einem Koordinierten Forschungsprogramm der IAEA wird das Bestrahlungsverhalten russischer und westlicher Reaktordruckbehälter(RDB)stähle untersucht. Im unbestrahlten Ausgangszustand weisen die Chargen des Grundwerkstoffes 15Ch2MFA des russischen Druckwassereaktors WWER-440 eine große Streuung in den im Charpy-V Test ermittelten Übergangstemperaturen und Hochlageenergien auf. Eine geringe Streuung in diesen Kennwerten haben die untersuchten Chargen des Grundwerkstoffes 15Ch2NMFA(A) des russischen Druckwasserreaktors WWER-1000. Die ermittelten Übergangstemperaturen liegen niedriger als bei den ASTM RDB-Stählen A533B Cl. 1 und ASTM A508 Cl. 3. Die J-Integralwerte für technische (J0,2)- und physikalische Rißinitiierung der untersuchten RDB-Stähle und der dazugehörigen Schweißgüter wurden mit den Hochlageenergien aus dem Charpy-V Test und den Streckgrenzen des Zugversuches korreliert.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
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<dc:language>ger</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1848-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Noll, S.]]></dc:creator>
<dc:creator><![CDATA[Noll, B.]]></dc:creator>
<dc:creator><![CDATA[Knieß, T.]]></dc:creator>
<dc:creator><![CDATA[Kampf, G.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1848-1</dc:identifier>
<dc:title><![CDATA[Rhenium and technetium complexes with nucleic acid components]]></dc:title>
<dc:source><![CDATA[Technetium, Rhenium and Other Metals in Chemistry and Nuclear Medicine
(Edited by Nicolini M., Mazzi U.) SGE Editoriali Padova (1999) pp. 553-556]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Re/Tc labelled nucleobases and nucleosides are developed and characterized in connection with cell uptake studies on cultured normal and tumour cells [1,2]. Stable Re and Tc complexes of nucleic acid components have been prepared where uracil derivatives are either involved in a mercaptoacetyl glycine (MAG) SN<SUB>3</SUB> coordination sphere or are part of "3+1" mixed-ligand complexes. Furthermore a prelabelling method has been successfully used for coupling the nucleic acid components to a performed Re/Tc complex.
Uptake of such complexes into proliferating cultured normal and tumour cells and their crude cytosolic and nuclear fractions, including postincubation effects and the influence of the metabolic state of the cells, has been observed.  
]]></dc:description>
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<dc:type>doc-type:book</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:14426-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:creator><![CDATA[Baier, S.]]></dc:creator>
<dc:creator><![CDATA[Duerigen, S.]]></dc:creator>
<dc:creator><![CDATA[Fridman, E.]]></dc:creator>
<dc:creator><![CDATA[Merk, B.]]></dc:creator>
<dc:creator><![CDATA[Weiss, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14426-1</dc:identifier>
<dc:title><![CDATA[Development of the coupled 3D neutron kinetics/thermal-hydraulics code DYN3D-HTR for the simulation of transients in block-type HTGR]]></dc:title>
<dc:source><![CDATA[5th Topical Meeting in High Temperature Reactor Technology, 18.-20.10.2010, Prague, Czech Republic]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[At the Forschungszentrum Dresden-Rossendorf (FZD), the Light Water Reactor (LWR) dynamics code DYN3D is extended and adopted for the application to block-type High temperature gas-cooled reactor (HTGR). DYN3D is a two-group diffusion code for 3D steady-state and transient core calculations based on nodal expansion methods. In addition to the neutron kinetics, it disposes of a thermal-hydraulics model for flow in parallel coolant channels. Macroscopic cross section data libraries precalculated with variation of burn-up, reactor poisons concentrations and thermal-hydraulic feedback parameters are linked to the code. Recently, a multi-group version of the code was developed.
In this paper, we give an overview of the latest developments of DYN3D concerning block-type HTGR.
The SP3 transport approximation is implemented into the multi-group DYN3D code to take anisotropy of the neutron flux and heterogeneity of the core more precisely into account. The SP3 method previously implemented into DYN3D for square fuel element geometry of LWR is being extended for hexagonal geometry of the graphite blocks, where the hexagons are subdivided into triangular nodes to be able to perform a systematic mesh refinement.
The main challenge in cross section generation for the HTGR core calculations is the treatment of the so-called double heterogeneity. The Reactivity equivalent Physical Transformation (RPT) approach is applied in order to eliminate the double-heterogeneity of HTGR fuel elements in HELIOS calculations. The full core analysis of the reference simplified HTGR core is performed with DYN3D using macroscopic nodal cross sections provided by HELIOS. The DYN3D results are verified against full core Monte Carlo simulations. 
A 3D heat conduction module coupled with a channel-type coolant flow model is implemented to take into account the temperature reactivity feedback to neutronics physically correctly. It is shown that there is significant redistribution of the produced heat by heat conduction between the graphite blocks.]]></dc:description>
<dc:subject><![CDATA[high temperature reactor]]></dc:subject>
<dc:subject><![CDATA[reactor dynamics]]></dc:subject>
<dc:subject><![CDATA[computer code]]></dc:subject>
<dc:subject><![CDATA[double heterogeneity]]></dc:subject>
<dc:subject><![CDATA[SP3 transport approximation]]></dc:subject>
<dc:subject><![CDATA[heat conduction]]></dc:subject>
<dc:subject><![CDATA[temperature reactivity feedback]]></dc:subject>
<dc:subject><![CDATA[computer code]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:14426-2</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:creator><![CDATA[Baier, S.]]></dc:creator>
<dc:creator><![CDATA[Duerigen, S.]]></dc:creator>
<dc:creator><![CDATA[Fridman, E.]]></dc:creator>
<dc:creator><![CDATA[Merk, B.]]></dc:creator>
<dc:creator><![CDATA[Weiss, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14426-2</dc:identifier>
<dc:title><![CDATA[Development of the coupled 3D neutron kinetics/thermal-hydraulics code DYN3D-HTR for the simulation of transients in block-type HTGR]]></dc:title>
<dc:source><![CDATA[5th Topical Meeting on High Temperature Reactor Technology, 18.-20.10.2010, Pargue, Czech Republic<br>Conference Website http://www.htr2010.eu/authors-area/upload/docs/htr2010_pdfonly.rar, Paper #036]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[At the Forschungszentrum Dresden-Rossendorf (FZD), the Light Water Reactor (LWR) dynamics code DYN3D is extended and adopted for the application to block-type High temperature gas-cooled reactor (HTGR). DYN3D is a two-group diffusion code for 3D steady-state and transient core calculations based on nodal expansion methods. In addition to the neutron kinetics, it disposes of a thermal-hydraulics model for flow in parallel coolant channels. Macroscopic cross section data libraries precalculated with variation of burn-up, reactor poisons concentrations and thermal-hydraulic feedback parameters are linked to the code. Recently, a multi-group version of the code was developed.
In this paper, we give an overview of the latest developments of DYN3D concerning block-type HTGR.
The SP3 transport approximation is implemented into the multi-group DYN3D code to take anisotropy of the neutron flux and heterogeneity of the core more precisely into account. The SP3 method previously implemented into DYN3D for square fuel element geometry of LWR is being extended for hexagonal geometry of the graphite blocks, where the hexagons are subdivided into triangular nodes to be able to perform a systematic mesh refinement.
The main challenge in cross section generation for the HTGR core calculations is the treatment of the so-called double heterogeneity. The Reactivity equivalent Physical Transformation (RPT) approach is applied in order to eliminate the double-heterogeneity of HTGR fuel elements in HELIOS calculations. The full core analysis of the reference simplified HTGR core is performed with DYN3D using macroscopic nodal cross sections provided by HELIOS. The DYN3D results are verified against full core Monte Carlo simulations. 
A 3D heat conduction module coupled with a channel-type coolant flow model is implemented to take into account the temperature reactivity feedback to neutronics physically correctly. It is shown that there is significant redistribution of the produced heat by heat conduction between the graphite blocks.]]></dc:description>
<dc:subject><![CDATA[high temperature reactor]]></dc:subject>
<dc:subject><![CDATA[reactor dynamics]]></dc:subject>
<dc:subject><![CDATA[computer code]]></dc:subject>
<dc:subject><![CDATA[double heterogeneity]]></dc:subject>
<dc:subject><![CDATA[SP3 transport approximation]]></dc:subject>
<dc:subject><![CDATA[heat conduction]]></dc:subject>
<dc:subject><![CDATA[temperature reactivity feedback]]></dc:subject>
<dc:subject><![CDATA[computer code]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14426-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1850-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kunze, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1850-1</dc:identifier>
<dc:title><![CDATA[Ultraschallverfahren zur Erfassung von Rißbildung und Rißfortschritt bei quasistatischer Belastung]]></dc:title>
<dc:source><![CDATA[Diplomarbeit Technische Universität Dresden, Fakultät Maschinenwesen, Juli 1994 (Betreuer: Dr. Böhmert)]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Es wurde ein Ultraschallverfahren zur Rißlängenmessung während des Dreipunktbiegeversuchs entwickelt, das auf der Beugung von Ultraschallwellen an der Rißspitze beruht. Die Information über Rißlänge und Rißfortschritt wird aus der Laufzeit der gebeugten Ultraschallwellen gewonnen. Das vorgestellte Verfahren ist das einzige der bisher bekannten Ultraschallverfahren, das an einer so kleinen Probenform erfolgreich angewendet wurde.]]></dc:description>
<dc:type>info:eu-repo/semantics/masterThesis</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1850-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:250-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Kalinenko, V.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-250-1</dc:identifier>
<dc:title><![CDATA[Analysis of transients for NPP with VVER-440 using the code SiTAP]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-54]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The report contains results of the analysis of the transients "Loop connection" and "SG tube rupture" for NPP with VVER-440 type reactors. To obtain detailled informations about NPP's dynamic characteristics, various variants of initial and boundary conditions are considered.
Calculation of these transients was performed with use of the code SiTAP developed at the Nuclear Safety Institute of Russian Research Centre "Kurchatov Institute". SiTAP is a multi-functional computer tool for fast analysis of transient and accidental processes of VVER type reactors for engineers working in the field of NPP dynamics.
SiTAP can be used for comparative analysis of several variants of accident scenarios to find out the conditions leading to the most severe consequences from safety point of view. For this cases, additional analyses using best-estimate codes should be carried out.
The results from SiTAP for faulty loop connection leading to a boron dilution accident are intended to be used as boundary conditions for a more detailled analysis by the help of the three-dimensional reactor core model DYN3D, developed in the Research Centre Rossendorf for the simulation of reactivity initiated accidents.]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-250-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2969-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2969-1</dc:identifier>
<dc:title><![CDATA[Verfahren und Schaltungsanordnung zur Maximum-Power-Point-Steuerung von Solargeneratoren]]></dc:title>
<dc:source><![CDATA[DE 199 04 561 A1]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[...wird nachgereicht.]]></dc:description>
<dc:type>info:eu-repo/semantics/patent</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:patent</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2969-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:2720-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2720-1</dc:identifier>
<dc:title><![CDATA[Melanoidine - Chemisch modifizierbare Funktionalitätsmodelle zur Untersuchung des Komplexbildungsverhaltens von Huminsäuren]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Karlsruhe, Institutsseminar INE, Karlsruhe, Germany, 17.09.1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2720-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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</metadata>
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<header>
<identifier>HZDR:PUBLDB:1582-1</identifier>
<datestamp>2024-12-18</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Jankowsky, R.]]></dc:creator>
<dc:creator><![CDATA[Noll, B.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1582-1</dc:identifier>
<dc:title><![CDATA[Capillary electrophoresis of <SUP>99m</SUP>technetium radiopharmaceuticals]]></dc:title>
<dc:source><![CDATA[Journal of Chromatography B, 724 (1999) 365-371]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Diagnostically used <SUP>99m</SUP>Tc kit radiopharmaceuticals were analyzed using capillary zone electrophoresis with radioactivity detection: <SUP>99m</SUP>Tc-bis(bis(2-ethyloxyethyl)phosphino)ethane (<SUP>99m</SUP>Tc-Myoview, <SUP>99m</SUP>Tc-Tetrofosmin), <SUP>99m</SUP>Tc-trans(1,2-bis(dehydro-2,2,5,5,-tetramethyl-3-furanone-4-methylene-amino)ethane)-tris(3-methoxy-1-propyl)phosphine) (<SUP>99m</SUP>Tc-Technescan Q12, <SUP>99m</SUP>Tc-Furifosmin), <SUP>99m</SUP>Tc-methoxyisobutylisonitrile (<SUP>99m</SUP>Tc-MIBI), <SUP>99m</SUP>Tc-<SUB>L,L</SUB>-ethylenecysteine diethylester dimer (<SUP>99m</SUP>Tc-ECD), <SUP>99m</SUP>Tc-d,l-hexamethylene propyleneamine oxime (<SUP>99m</SUP>Tc-HMPAO), <SUP>99m</SUP>Tc-diethylenetriaminepentaacetic acid (<SUP>99m</SUP>Tc-DTPA), <SUP>99m</SUP>Tc-ethylene hepatobiliary iminodiacetic acid (<SUP>99m</SUP>Tc-EHIDA), <SUP>99m</SUP>Tc-<SUB>L,L</SUB>-ethylenecysteine (<SUP>99m</SUP>Tc-EC), <SUP>99m</SUP>Tc-mercaptoacetylglycylglycylglycine (<SUP>99m</SUP>Tc-MAG<SUB>3</SUB>), <SUP>99m</SUP>Tc-dimercaptosuccinic acid (<SUP>99m</SUP>Tc-DMSA), <SUP>99m</SUP>Tc-methylene diphosphonate (<SUP>99m</SUP>Tc-MDP) and <SUP>99m</SUP>NaTcO<SUB>4</SUB>. A pressure-driven capillary zone electrophoresis was employed to detect small anions of high electrophoretic mobility and cations within one run. Effective <SUP>99m</SUP>Tc complex charges could be determined by a neutral internal standard. All complexes showed the expected electrophoretic behaviours in view of their charges. Pure products were obtained for the majority of the studied complexes. In the case of <SUP>99m</SUP>Tc-Q12, <SUP>99m</SUP>Tc-EHIDA and <SUP>99m</SUP>Tc-MDP, complex mixtures were detected. The high potential of CE for the analysis of <SUP>99m</SUP>Tc radiopharmaceuticals could be shown. ]]></dc:description>
<dc:subject><![CDATA[Radiopharmaceuticals]]></dc:subject>
<dc:subject><![CDATA[<SUP>99m</SUP>Technetium]]></dc:subject>
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<dc:language>eng</dc:language>
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<header>
<identifier>HZDR:PUBLDB:1853-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Friebe, M.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Berger, R.]]></dc:creator>
<dc:creator><![CDATA[Syhre, R.]]></dc:creator>
<dc:creator><![CDATA[Papadopoulos, M.]]></dc:creator>
<dc:creator><![CDATA[Chiotellis, E.]]></dc:creator>
<dc:creator><![CDATA[Suda, K.]]></dc:creator>
<dc:creator><![CDATA[Wunderli-Allenspach, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1853-1</dc:identifier>
<dc:title><![CDATA[Amine group bearing '3+1' oxotechnetium(V) and oxorhenium(V) complexes: Synthesis, characterization of lipophilicity and permeation through the blood-brain barrier]]></dc:title>
<dc:source><![CDATA[Technetium, Rhenium and Other Metals in Chemistry and Nuclear Medicine
(Edited by Nicolini M., Mazzi U.) SGE Editoriali Padova (1999) pp. 627-631]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[A set of technetium(V) mixed-ligand complexes was synthesized with different protonation constants pK<SUB>a</SUB>, brought about by substitution. They were characterized regarding their lipophilicity and compared to the corresponding rhenium(V) complexes. Partition coefficients P, determined by reversed phase HPLC and the octanol shake flask method, were higher for the technetium than for the analogous rhenium species. Investigations were performed to assess the influence of the physicochemical molecule parameters on the biological behaviour of these compounds. The state of ionisation of the molecules had a significant influence on brain uptake in vivo. Less uptake was found for compounds with pK<SUB>a</SUB> values around 9.5, which are fully protonated at physiological pH, than for those with pK<SUB>a</SUB> values around 7.5, which are ionised to only about 50% at pH 7.4. transport through cells was studied with an in vitro blood-brain barrier (BBB) model, based on the human umbilical cord cell line ECV304. The resulting in vitro permeation curves agree with the in vivo results obtained in mice and rats with short incubation times (up to 30 min).]]></dc:description>
<dc:type>info:eu-repo/semantics/book</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1854-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1854-1</dc:identifier>
<dc:title><![CDATA[Vibration Modelling - Investigation of Mechanical Accident Sequences at a VVER-440 Type Reactor]]></dc:title>
<dc:source><![CDATA[International Conference on Fault Diagnosis, Toulouse / France, 05 - 07 April, 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[During abnormal core barrel motion of a VVER-440 type reactor significant phase relations and coherences between incore and excore neutron noise signals were observed. For the explanation of the phenomena a numerical algorithm based on the non-linear equations of motion of a double pendulum was developed. In order to confirm the numerical results qualitatively additional experiments at a small set-up modelling the control elements were performed. The typical signal patterns observed at the VVER-440 could be shown to originate from mechanical impacts between the control elements and the neighbouring fuel cassettes.]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:1855-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barz, H.-U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1855-1</dc:identifier>
<dc:title><![CDATA[Adjustment and Application of Monte Carlo Neutron Calculation with Respect to Embrittlement Problems]]></dc:title>
<dc:source><![CDATA[Common Workshop of the EURATOM Working Group for Reactor Dosimentry  and the Working Group for Reactor Dosimetry of VVER-Reactors on Pressure Vessel Surveillance Programmes and Their Applications, ...]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[Problems of the calculation of neutron fluences for reactor pressure vessel embrittlement determination were discussed. For the example of the calculation of neutron fluences of irradiated specimens within the Rheinsberg reactor (time period 1984-1988) it was shown, for which parts of the problem Monte Carlo methods can be very well applicated.   
Some special measures were discussed, which are  used for the own Monte Carlo codes (system TRAMO), especially the improved "Weight Window Method" and a proper calculation of the needed weights. Further the preparation of all needed data to take into account the history for each irradiation period was described and the influence of different neutron group data and the different handling of anisotropy of elastic scattering was considered.]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:3252-1</identifier>
<datestamp>2025-12-09</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Plettner, C.]]></dc:creator>
<dc:creator><![CDATA[Schnare, H.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Kaeubler, L.]]></dc:creator>
<dc:creator><![CDATA[Doenau, F.]]></dc:creator>
<dc:creator><![CDATA[Ragnarsson, I.]]></dc:creator>
<dc:creator><![CDATA[Afanasjev, A.]]></dc:creator>
<dc:creator><![CDATA[Algora, A.]]></dc:creator>
<dc:creator><![CDATA[Deangelis, G.]]></dc:creator>
<dc:creator><![CDATA[Gadea, A.]]></dc:creator>
<dc:creator><![CDATA[Napoli, D.]]></dc:creator>
<dc:creator><![CDATA[Eberth, J.]]></dc:creator>
<dc:creator><![CDATA[Steinhardt, T.]]></dc:creator>
<dc:creator><![CDATA[Thelen, O.]]></dc:creator>
<dc:creator><![CDATA[Hausmann, M.]]></dc:creator>
<dc:creator><![CDATA[Mueller, A.]]></dc:creator>
<dc:creator><![CDATA[Jungclaus, A.]]></dc:creator>
<dc:creator><![CDATA[Lieb, K.-P.]]></dc:creator>
<dc:creator><![CDATA[Jenkins, D.]]></dc:creator>
<dc:creator><![CDATA[Wadsworth, R.]]></dc:creator>
<dc:creator><![CDATA[Wilson, A.]]></dc:creator>
<dc:creator><![CDATA[Frauendorf, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3252-1</dc:identifier>
<dc:title><![CDATA[Very high rotational frequencies and band termination in 73Br]]></dc:title>
<dc:source><![CDATA[Physical Review C, Vol. 62, 014313]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Rotational bands in 73Br have been investigated 
up to spins of 65/2 using the EUROBALL 
III spectrometer. One of the 
negative-parity bands displays the highest rotational 
frequency 1.85 MeV reported to date in nuclei heavier than 25.
At high frequencies, the experimental dynamic moment of inertia  for all bands decrease to very low values,  indicating
a lose of collectivity. The bands are described in the configuration-dependent cranked 
Nilsson-Strutinsky model. The calculations indicate that 
one of the negative-parity bands is observed up to its terminating single-particle state at spin 63/2. 
This result establishes the first band termination in the 
A =70 mass region.]]></dc:description>
<dc:subject><![CDATA[rotational bands]]></dc:subject>
<dc:subject><![CDATA[band termination]]></dc:subject>
<dc:subject><![CDATA[cranking calculations]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevC.62.014313]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-3252-1</dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:1851-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1851-1</dc:identifier>
<dc:title><![CDATA[Experimental and Numerical Investigation of Control Element Vibration During Abnormal Core Barrel Motion at a VVER-440 Type Reactor]]></dc:title>
<dc:source><![CDATA[International Simulators Conference (SIMULATORS X), Arlington / Viginia, 29th March - 1st April 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[In 1985 abnormal core barrel motion had occured at unit 2 of the Greifswald NPP indicated by extremly large neutron noise. Amplitudes of up to 4mm were estimated from the external neutron noise signals.
The coherence and phase relations between excore and incore neutron noise signals exhibited typical features from which it could be concluded that even the control elements were forced to vibrations by the moving core barrel.
To obtain principal understanding about these phenomena and to draw conclusions for the surveillance of the excore and incore neutron signals, experimental and numerical investigations were performed. An experimental set-up was constructed providing all necessary displacement signals via HALL probes. This physical model, being a double pendulum with an annular channel surrounding the lower pendulum, can be operated in a linear mode (small excitation amplitudes) as well as in a non-linear mode (larger amplitudes which cause impacts between channel and lower pendulum).
The numerical simulation algorithm is based on a mechanical system consisting of linear elements (inertia, dampers, springs) and non-linear elements (gaps). In this way impacts between control element and neighbouring fuel cassettes which are strongly non-linear events can be modeled. After simulating the time series, which is possible for any detector position at the control element or at the set-up respectively, transfer functions, coherences, phase relations etc. can be computed.
It could be shown that the typical linear phase shifts between excore and incore neutron noise signals are due to impacts between the control elements and the neighbouring fuel cassettes. The obtained results can be used to establish a sensitive detection procedure for control element vibrations induced by abnormal core barrel motion.]]></dc:description>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1852-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1852-1</dc:identifier>
<dc:title><![CDATA[Regelelementschwingungen bei anomaler Kernbehälterbewegung in einem Druckwasserreaktor vom Typ WWER-440]]></dc:title>
<dc:source><![CDATA[4. Tagung über Dynamische Probleme, Modellierung und Wirklichkeit, Universität Hannover, 07. - 08. Oktober 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[Während der anomalen Kernbehälterbewegung bei einem Reaktor vom Typ WWER-440 wurden signifikante Phasen- und Kohärenzbeziehungen zwischen dem Excore- und dem Incoreneutronenrauschen beobachtet. Für die Erklärung der Phänomene wurde ein numerischer Algorithmus entwickelt, der auf den nichtlinearen Bewegungsgleichungen eines Doppelpendels beruht. Zur qualitativen Verifizierung der numerischen Resultate wurden außerdem Experimente an einem kleinen physischen Modell der Regelelemente durchgeführt. Es konnte nachgewiesen werden, daß die am WWER-440 beobachteten typischen Signalmuster von mechanischen Anschlagvorgängen zwischen Regelelementen und benachbarten Brennstoffkassetten herrühren. 	]]></dc:description>
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<dc:type>doc-type:conferenceObject</dc:type>
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<dc:language>ger</dc:language>
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<header>
<identifier>HZDR:PUBLDB:1858-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Böhmer, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1858-1</dc:identifier>
<dc:title><![CDATA[Comments on Spectrum Adjustment for Reactor Pressure Vessel Dosimetry]]></dc:title>
<dc:source><![CDATA[Common Workshop of the EURATOM Working Group for Reactor Dosimetry and the Working Group for Reactor Dosimetry of VVER-Reactors on Pressure Vessel Surveillance Programmes and Their Applications, R ...]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[After a short review about the state of art of spectrum adjustment for reactor pressure vessel dosimetry and their realization in Rossendorf plans for future developments are described. The most important outstanding problem is the calculation of covariances of the theoretical input spectra. 
As example for an advanced spectrum adjustment some preliminary results of a reevaluation of 1984/85 irradiation experiments in Rheinsberg were presented.    
Suggestions are made for common projects in the frame of the WGRD, VVER and EWGRD, especially the development and maintenance of a common reactordosimetric database for VVER type reactors and the organization of benchmark exercises for calculations of detector cross sections and spectrum covariances.]]></dc:description>
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<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1507-1</identifier>
<datestamp>2025-01-13</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Witke, W.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1507-1</dc:identifier>
<dc:title><![CDATA[A new mechano-optical technique to measure local velocities in opaque fluids]]></dc:title>
<dc:source><![CDATA[Flow Measurement and Instrumentation, Vol. 11/2 (2000) 71-78]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[A novel technique has been developed to measure the local velocities in opaque liquid flows such as liquid metals. The measuring principle is based on the separation of a direct mechanical interaction between flow and sensor tip and the optical acquisition and processing of the signal. In principle, this fact allows the extension of the range of applicability to higher temperatures. Furthermore, the insensitivity of the system to electrical noise and external magnetic fields can be considered as an
important advantage. Until now, the sensor has been tested in metallic melts up to temperatures of about 350 °C. We present measurements of the local velocity obtained in an eutectic InGaSn melt driven by a rotating magnetic field.]]></dc:description>
<dc:subject><![CDATA[flow measurement technique]]></dc:subject>
<dc:subject><![CDATA[local sensor]]></dc:subject>
<dc:subject><![CDATA[velocity]]></dc:subject>
<dc:subject><![CDATA[opaque fluids]]></dc:subject>
<dc:subject><![CDATA[liquid metals]]></dc:subject>
<dc:subject><![CDATA[mechano-optical principle]]></dc:subject>
<dc:subject><![CDATA[rotating magnetic field]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0955-5986(00)00010-8]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1507-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1509-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1509-2</dc:identifier>
<dc:title><![CDATA[Electromagnetic control of flow around bodies]]></dc:title>
<dc:source><![CDATA[Einladungsvortrag am LEGI Grenoble (04.02.1999)]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The flow around bodies (cylinder, plate) can be controlled by applying
electromagnetic forces originating from electrodes and permanent magnets
suitably placed on the surface of the body. There is a large variety for
applying those forces with respect to the geometrical arrangement and the
electrical current feeding the electrodes. The goals of this approach are
flow stabilization, drag reduction or manoeuvrability of the body in an
electrically low-conducting fluid like seawater.

Experimental and numerical results of our research programme will be
presented. Experiments were performed using a copper sulfate electrolytic
solution, a sodium hydroxide loop and large saltwater channels available at
a shipbuilding research center in Hamburg. A strong flow control has been
confirmed. The energetic limitations of the approach will be discussed
]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1509-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1510-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Priede, J.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1510-1</dc:identifier>
<dc:title><![CDATA[Oscillatory instability of electromagnetically levitated solid bodies]]></dc:title>
<dc:source><![CDATA[Journal IEEE Transactions on Magnetics, USA, Vol. 36. No. 1, pp. 354-357, January 2000]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[This paper presents a linear-stability analysis of small-amplitude oscillations of a solid body suspended in an alternating magnetic field. An original theory is developed for an arbitrary configuration of the magnetic field. Stability of a solid sphere in an axisymmetric linear magnetic field is calculated analytically. Oscillations of the sphere are found to develop as the frequency of the field exceeds certain critical threshold relative to the characteristic diffusion time of the magnetic field in the sphere. The critical frequency for the onset of oscillations in linear magnetic field coincides with the critical frequency for the spin-up instability in uniform magnetic field. The growth rate of oscillations attains a maximum at some frequency above the threshold and tends to zero at high frequencies.

]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1510-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1512-1</identifier>
<datestamp>2025-01-13</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grants, I.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1512-1</dc:identifier>
<dc:title><![CDATA[Linearized solution of quasi-steady Stefan problem in vertical gradient freeze configuration]]></dc:title>
<dc:source><![CDATA[Journal of Crystal Growth Elsevier 207 (1999) 138-147]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The present paper deals with a shape of a sharp phase boundary under conductivity controlled quasisteady solidification in a long cylinder with a given surface temperature and growth velocity. An approximate analytical closed form solution is obtained linearizing the Stefan problem in a neighbourhood of the practically desirable planar interface. The relative error of the solution is evaluated numerically and shown below 15% for reasonable interface depths (1/2 of the crystal radius) and desreasing linearly (or more rapidly) as interface deformation decreases.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0022-0248(99)00346-2]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1512-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1515-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Avilov, V.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1515-1</dc:identifier>
<dc:title><![CDATA[Elektromagnetische Grenzschichtkontrolle - Theorie und Numerik]]></dc:title>
<dc:source><![CDATA[Statusseminar "Technische Anwendungen von Erkenntnissen der Nichtlinearen Dynamik", Frankfurt, 23./24.02.1999
Tagungsband. S. 201-204]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Im Rahmen des Verbundprojektes wurden theoretische Untersuchungen zur Modellierung der aus periodischen Anordnungen von alternierenden Magneten und Elektroden entstehenden wandnahen Lorentzkräfte bei Körperumströmungen in schwach-leitfähigen Fluiden durchgeführt. Hierbei konnte die Beschreibung der Lorentzkräfte für die klassische Konfiguration aus rechteckigen Magneten und Elektroden entschieden verbessert werden.  Diese Modellierung war notwendige Voraussetzung für die Durchführung numerischer Simulationen von Platten- und Tragflügelumströmungen, für welche im Rahmen des Verbundprojektes Umströmungsexperimente an der HSVA durchgeführt wurden. Existierende Codes zur Berechnung turbulenter Umströmungen enthalten stets aus der Turbulenztheorie abgeleitete Wandfunktionen für den wandnahen Bereich. Diese können hier nicht verwendet werden, da die elektromagnetische Kraft gerade im wandnahen Bereich ihre Wirkung entfaltet. Deshalb wurde bewußt eine direkte numerische Simulation der Umströmung gewählt, obwohl diese zunächst auf relativ niedrige Reynolds-Zahlen beschränkt ist. Hierbei fand ein moderner Code mit spektralen Elementen Anwendung. Die Simulationen belegen, daß mit Hilfe der Grenzschichtkontrolle durch wandparallele Lorentzkräfte die Strömungsablösung an der Saugseite eines angestellten Ruders wirksam verzögert bzw. unterdrückt werden kann und damit eine erhebliche Auftriebsverbesserung erreicht wird.


]]></dc:description>
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<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1515-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:1515-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Avilov, V.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1515-7</dc:identifier>
<dc:title><![CDATA[Elektromagnetische Grenzschichtkontrolle - Theorie und Numerik]]></dc:title>
<dc:source><![CDATA[Statusseminar "Technische Anwendungen von Erkenntnissen der Nichtlinearen Dynamik", Frankfurt, 23./24.02.1999
Tagungsband. S. 201-204]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Im Rahmen des Verbundprojektes wurden theoretische Untersuchungen zur Modellierung der aus periodischen Anordnungen von alternierenden Magneten und Elektroden entstehenden wandnahen Lorentzkräfte bei Körperumströmungen in schwach-leitfähigen Fluiden durchgeführt. Hierbei konnte die Beschreibung der Lorentzkräfte für die klassische Konfiguration aus rechteckigen Magneten und Elektroden entschieden verbessert werden.  Diese Modellierung war notwendige Voraussetzung für die Durchführung numerischer Simulationen von Platten- und Tragflügelumströmungen, für welche im Rahmen des Verbundprojektes Umströmungsexperimente an der HSVA durchgeführt wurden. Existierende Codes zur Berechnung turbulenter Umströmungen enthalten stets aus der Turbulenztheorie abgeleitete Wandfunktionen für den wandnahen Bereich. Diese können hier nicht verwendet werden, da die elektromagnetische Kraft gerade im wandnahen Bereich ihre Wirkung entfaltet. Deshalb wurde bewußt eine direkte numerische Simulation der Umströmung gewählt, obwohl diese zunächst auf relativ niedrige Reynolds-Zahlen beschränkt ist. Hierbei fand ein moderner Code mit spektralen Elementen Anwendung. Die Simulationen belegen, daß mit Hilfe der Grenzschichtkontrolle durch wandparallele Lorentzkräfte die Strömungsablösung an der Saugseite eines angestellten Ruders wirksam verzögert bzw. unterdrückt werden kann und damit eine erhebliche Auftriebsverbesserung erreicht wird.


]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
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<dc:audience>Researchers</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1583-1</identifier>
<datestamp>2024-12-18</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Huxel, N.]]></dc:creator>
<dc:creator><![CDATA[Brentano, P.]]></dc:creator>
<dc:creator><![CDATA[Eberth, J.]]></dc:creator>
<dc:creator><![CDATA[Enders, J.]]></dc:creator>
<dc:creator><![CDATA[Herzberg, R.-D.]]></dc:creator>
<dc:creator><![CDATA[Neumann-Cosel, P.]]></dc:creator>
<dc:creator><![CDATA[Nicolay, N.]]></dc:creator>
<dc:creator><![CDATA[Pietralla, N.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Rangacharyulu, C.]]></dc:creator>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:creator><![CDATA[Richter, A.]]></dc:creator>
<dc:creator><![CDATA[Schlegel, C.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Skoda, S.]]></dc:creator>
<dc:creator><![CDATA[Thomas, H. G.]]></dc:creator>
<dc:creator><![CDATA[Wiedenhöver, I.]]></dc:creator>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:creator><![CDATA[Zilges, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1583-1</dc:identifier>
<dc:title><![CDATA[Complete scissors mode strength in heavy deformed odd-mass nuclei: a case study of <SUP>165</SUP>Ho and <SUP>169</SUP>Tm]]></dc:title>
<dc:source><![CDATA[Nuclear Physics A 645 (1999) 239-261]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0375-9474(98)00610-1]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1583-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1584-1</identifier>
<datestamp>2024-12-18</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Paul, E. S.]]></dc:creator>
<dc:creator><![CDATA[Fossan, D. B.]]></dc:creator>
<dc:creator><![CDATA[Hauschild, K.]]></dc:creator>
<dc:creator><![CDATA[Hibbert, I. M.]]></dc:creator>
<dc:creator><![CDATA[Nolan, P. J.]]></dc:creator>
<dc:creator><![CDATA[Schnare, H.]]></dc:creator>
<dc:creator><![CDATA[Sears, J. M.]]></dc:creator>
<dc:creator><![CDATA[Thorslund, I.]]></dc:creator>
<dc:creator><![CDATA[Wadsworth, R.]]></dc:creator>
<dc:creator><![CDATA[Wilson, J. N.]]></dc:creator>
<dc:creator><![CDATA[Ragnarsson, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1584-1</dc:identifier>
<dc:title><![CDATA[High-fold Gamma-ray spectroscopy of <SUP>117</SUP>I: Coexistence of collective and noncollective structures]]></dc:title>
<dc:source><![CDATA[Physical Review C, Volume 59, Number 4, April 1999, 1984-1998]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevC.59.1984]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1584-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1585-1</identifier>
<datestamp>2024-12-18</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Lobach, Y. N.]]></dc:creator>
<dc:creator><![CDATA[Käubler, L.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Pasternak, A. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1585-1</dc:identifier>
<dc:title><![CDATA[Lifetimes and collectivity of low-lying states in <SUP>115</SUP>Sn]]></dc:title>
<dc:source><![CDATA[Physical Review C, Volume 59, Number 4, April 1999, 1975-1983]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevC.59.1975]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1585-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:535-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Futterschneider, H.]]></dc:creator>
<dc:creator><![CDATA[Hirsch, W.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-535-1</dc:identifier>
<dc:title><![CDATA[Elektroenergieerzeugung einer kombinierten Wind-Photovoltaik-Anlage in Ottendorf-Okrilla (Sachsen)]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-138 April 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Vom Zentrallager der Plus-Warenhandelsgesellschaft in Ottendorf-Okrilla (Sachsen) wird seit 1992 eine hybride Wind-Photovoltaik-Anlage zur Erzeugung von Elektroenergie betrieben. Die Anlage besteht aus einer 60-kW-Windkraftanlage des Typs TW 60 und einer Phtovoltaikanlage mit einer Spitzenleistung von 3,18 kW. Letztere zeichnet sich durch einige Besonderheiten (Orientierung des Generators, Master-Slave-Betieb der Wechselrichter) aus. Das Betriebsverhalten der Anlagen wurde über einen längeren Zeitraum untersucht.

Im Jahr 1995 erreichte die Photovoltaikanlage mit 689 Vollastbetriebsstunden etwa die Ergebnisse anderer Photovoltaikanlagen in Sachsen. Mögliche höhere Erträge werden durch die gewählte Orientierung des Generators verhindert. Die Master-Slave-Schaltung der Wechselrichter arbeitete ohne Probleme. Ihre Effektivität wurde durch die nicht optimale Abstimmung von Generator- und Wechselrichterleistung beeinträchtigt. ]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1586-1</identifier>
<datestamp>2024-12-18</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Aszódi, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1586-1</dc:identifier>
<dc:title><![CDATA[Numerical Simulation of the Emergency Condenser of the SWR1000]]></dc:title>
<dc:source><![CDATA[Nuclear Science and Engineering 135 (2000) No.3 267-279]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The SWR1000 is a new innovative boiling water reactor concept, which is developed by Siemens AG. This concept is characterized in particular by passive safety systems (e.g. four emergency condensers, four building condensers, eight passive pressure pulse transmitters, six gravity-driven core flooding lines). In the framework of BWR Physics and Thermohydraulic Complementary Action (BWR-CA) to the EU BWR R&D Cluster emergency condenser tests were performed by Forschungszentrum Jülich at the NOKO test facility. In this paper post test calculations with ATHLET are presented, which aim at the determination of the removable power of the emergency condenser and its operation mode. The 1D thermal-hydraulic code ATHLET was extended by the module KONWAR for the calculation of the heat transfer coefficient during condensation in horizontal tubes. In addition, results of CFD-calculations using the code CFX-4 are presented, which investigate the natural convection during the heat up process at the secondary side of the NOKO test facility. ]]></dc:description>
<dc:subject><![CDATA[BWR]]></dc:subject>
<dc:subject><![CDATA[emergency condenser]]></dc:subject>
<dc:subject><![CDATA[condensation in horizontal tubes]]></dc:subject>
<dc:subject><![CDATA[1D-modelling]]></dc:subject>
<dc:subject><![CDATA[heat transfer in large pools]]></dc:subject>
<dc:subject><![CDATA[computational fluid dynamics]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:1588-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:creator><![CDATA[Decker, B.]]></dc:creator>
<dc:creator><![CDATA[Grochowski, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1588-1</dc:identifier>
<dc:title><![CDATA[Revised Performance Data of Small Grid Connected PV Systems Based on in situ Measurements]]></dc:title>
<dc:source><![CDATA[Proceedings of the 14th European Union Photovoltaic Solar Energy Conference and Exhibition, Barcelona (Spain), 30. June - 04. July 1997, Volume II, p. 2652]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The mean annual yield (700 kWh/a*kWp) and performance ratio (65%) of small grid connected PV systems which were installed within the 1000-Roofs-Programme in Germany are lower than expected. By investigating the parameters determining the performance ratio it could be shown that for well designed PV systems the PR should range within 70 to 80 %. The real power of the PV arrays as the most critical parameter of the performance ratio was measured with a newly developed PV system analyzer. In most investigated systems the measured power was 10 to 20 % lower than the nominal power. The revised performance data based on the measurements agree with the above given values. Based on a typical irradiation of 1100 kWh/m2 in module plane a mean annual yield of more than 800 kWh/a*kWp can be expected.]]></dc:description>
<dc:subject><![CDATA[Small grid connected PV systems - 1:Performance - 2:PV Array - 3]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:1588-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:creator><![CDATA[Decker, B.]]></dc:creator>
<dc:creator><![CDATA[Grochowski, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1588-7</dc:identifier>
<dc:title><![CDATA[Revised Performance Data of Small Grid Connected PV Systems Based on in situ Measurements]]></dc:title>
<dc:source><![CDATA[Proceedings of the 14th European Union Photovoltaic Solar Energy Conference and Exhibition, Barcelona (Spain), 30. June - 04. July 1997, Volume II, p. 2652]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The mean annual yield (700 kWh/a*kWp) and performance ratio (65%) of small grid connected PV systems which were installed within the 1000-Roofs-Programme in Germany are lower than expected. By investigating the parameters determining the performance ratio it could be shown that for well designed PV systems the PR should range within 70 to 80 %. The real power of the PV arrays as the most critical parameter of the performance ratio was measured with a newly developed PV system analyzer. In most investigated systems the measured power was 10 to 20 % lower than the nominal power. The revised performance data based on the measurements agree with the above given values. Based on a typical irradiation of 1100 kWh/m2 in module plane a mean annual yield of more than 800 kWh/a*kWp can be expected.]]></dc:description>
<dc:subject><![CDATA[Small grid connected PV systems - 1:Performance - 2:PV Array - 3]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:1863-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ferse, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1863-1</dc:identifier>
<dc:title><![CDATA[Evaluation of Environmental Problems Using Decision-Analysis Methods and Knowledge-Based Systems]]></dc:title>
<dc:source><![CDATA[Workshop of the German PIN-Project Group (Processess of International Negotation), Rossendorf, March 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[A knowlegde-based strategy for the evaluation of risks produced by contaminated sites is presented, which also gives a ranking for the temporal sequence of remediation. This strategy supports the responsible government offices. It is based on the Saxonian evaluation method for contaminated sites and is implemented in the computer programs XUMA and GEFA.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1863-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1864-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ferse, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1864-1</dc:identifier>
<dc:title><![CDATA[Possibilities for Decision-Analysis in Planing Energy Distribution Systems]]></dc:title>
<dc:source><![CDATA[Workshop "Strategic Energy Planning", ESAG Dresden, October 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[A concept for the use of decision-analysis in planning local energy distribution systems is introduced. The concept is based on the coupling of multiple independent modules, what enables the finding of a solution optimum in cost and environmental compatibility by variation of boundary conditions and input parameters. The first modul is  presented.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1864-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1875-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Noack, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1875-1</dc:identifier>
<dc:title><![CDATA[Eine Plasmaneutronenquelle für die Fusionsmaterialforschung]]></dc:title>
<dc:source><![CDATA[Institut für Strahlenschutzphysik, TU Dresden, Dresden, 27.05.1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The contents is largely covered by a the extended contribution to this annual report.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1875-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1878-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, U.]]></dc:creator>
<dc:creator><![CDATA[Richter, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1878-1</dc:identifier>
<dc:title><![CDATA[Material Investigation at Research Center Rossendorf Related to the Coordinated Research Programme Optimizing of Reactor Pressure Vessel Surveillance Programmes and Their Analysis Phase 3"]]></dc:title>
<dc:source><![CDATA[Sixth Meeting of Participants in the Coordinated Research Programme "Optimizing of Reactor Pressure Vessel Surveillance Programmes and Their Analysis - Phase 3", Vienna, November 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The paper gives results of the contribution of Research Center Rossendorf to the IAEA Coordinated Research Programme "Optimizing of Reactor Pressure Vessel Surveillance Programmes and Their Analysis - Phase 3". The report includes information about material and specimen fabrication, the irradiation conditions, and the test methods. For the unirradiated state impact energy-temperature curves, dynamic J integrals for cleavage fracture, quasistatic crack resistance curves, and crack initiation J integral values are given.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1878-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:1886-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Maletti, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1886-1</dc:identifier>
<dc:title><![CDATA[Remarks About the Thermal Use of Solar Energy in Saxonia]]></dc:title>
<dc:source><![CDATA[Energieanwendung/Energie- und Umwelttechnik 42 (1993), S. 578]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[By the installation of more than 400 modern solar thermal collector plants with a summarized collector area of about 3000 m2 a remarkable entry in the thermal use of solar energy was reached in Saxonia in 1992. Simultaneously a network of little enterprises came into existence, which now work actively in the field of energy and environmental techniques. This development was essentially supported by the Saxonian promotion programme of rational use and application of renewable sources of energy.
 	]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1886-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1894-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Weier, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1894-1</dc:identifier>
<dc:title><![CDATA[Untersuchungen zum Zylindernachlauf im MHD-Fall]]></dc:title>
<dc:source><![CDATA[Diplomarbeit Universität Halle-Wittenberg, November 1993 (Betreuer: G. Gerbeth)]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[In der Arbeit wird experimentell und theoretisch die Frage behandelt, wie ein externes longitudinales Magnetfeld die Stabilität des Zylinder-Nachlaufs (Karmansche Wirbelstraße) beeinflußt. Die Messungen wurden am Quecksilber-Versuchsstand des IMG Grenoble durchgeführt. Die Unterdrückung der Wirbel-straße wurde vom theoretischen Modell vorhergesagt und im Experiment verifiziert. Überraschend wurde sowohl vom Modell als auch im Experiment die Tendenz zu langwelligen Störungen gefunden, die bei wachsendem Magnetfeld immer ausgeprägter werden.]]></dc:description>
<dc:type>info:eu-repo/semantics/masterThesis</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1894-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:1897-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barz, U.]]></dc:creator>
<dc:creator><![CDATA[Bertram, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1897-1</dc:identifier>
<dc:title><![CDATA[Calculation of Neutron Fluence in the Region of the Pressure Vessel for the History of Different Reactors by Using the Monte-Carlo-Method]]></dc:title>
<dc:source><![CDATA[Nuclear Engineering and Design 137 (1992), 71]]></dc:source>
<dc:date>1992</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1898-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Block, F. R.]]></dc:creator>
<dc:creator><![CDATA[Dittmer, R.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1898-1</dc:identifier>
<dc:title><![CDATA[Bubble Detection in Liquid Metals]]></dc:title>
<dc:source><![CDATA[Proc. International Conference on "MHD Processes to Protection of Environment", Kiev / Ukraine, June 1992]]></dc:source>
<dc:date>1992</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1901-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Dietze, K.]]></dc:creator>
<dc:creator><![CDATA[Hüttel, G.]]></dc:creator>
<dc:creator><![CDATA[Lehmann, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1901-1</dc:identifier>
<dc:title><![CDATA[Neutron Data Check by Sample Reactivity Measurements in Reactor Configurations with Specially Designed Neutronic Properties]]></dc:title>
<dc:source><![CDATA[Progress Report on Nuclear Data Research in the F.R. of Germany, NEANDC-Report, 1992]]></dc:source>
<dc:date>1992</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1902-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Dietze, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1902-1</dc:identifier>
<dc:title><![CDATA[Integral Test of FPND by Reactivity Measurements in Reactor Configurations with Specially Designed Adjoint Spectra]]></dc:title>
<dc:source><![CDATA[Proc. Specialists Meeting on FPND, in Report JAERI, Tokai-Mura / Japan, May 1992]]></dc:source>
<dc:date>1992</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<identifier>HZDR:PUBLDB:1903-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Häusler, R.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Erbacher, F. J.]]></dc:creator>
<dc:creator><![CDATA[Lübke, L.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, H.]]></dc:creator>
<dc:creator><![CDATA[Wetzel, L.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1903-1</dc:identifier>
<dc:title><![CDATA[Temperaturtransiente Kriech-Berst-Versuche an ZrNb1-Hüllrohren - Vergleich zu Zircaloy-4-Hüllrohren]]></dc:title>
<dc:source><![CDATA[Proc. Jahrestagung Kerntechnik 1992, Karlsruhe, Mai 1992]]></dc:source>
<dc:date>1992</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:1905-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Lenkey, G. B.]]></dc:creator>
<dc:creator><![CDATA[Major, Z.]]></dc:creator>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1905-1</dc:identifier>
<dc:title><![CDATA[The Dynamic Calibration Problems in Instrumented Impact Testing]]></dc:title>
<dc:source><![CDATA[Proc. 9th Biennial European Conference on Fracture (EFC 9), Varna / Bulgaria, September 1992]]></dc:source>
<dc:date>1992</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
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<dc:audience>Researchers</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1906-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Liewers, P.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1906-1</dc:identifier>
<dc:title><![CDATA[Systematic Analysis of Noisy Signals in the Nuclear Reactor Noise Diagnosis of Abnormal Core Barrel Motion]]></dc:title>
<dc:source><![CDATA[Proc. of the 5th Symposium IMECO TC-10, Dresden, September 1992]]></dc:source>
<dc:date>1992</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:1906-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Liewers, P.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1906-7</dc:identifier>
<dc:title><![CDATA[Systematic Analysis of Noisy Signals in the Nuclear Reactor Noise Diagnosis of Abnormal Core Barrel Motion]]></dc:title>
<dc:source><![CDATA[Proc. of the 5th Symposium IMECO TC-10, Dresden, September 1992]]></dc:source>
<dc:date>1992</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
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<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1906-7</dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:1861-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1861-1</dc:identifier>
<dc:title><![CDATA[Results of Material Investigations Based on the Rheinsberg - Irradiation Programme]]></dc:title>
<dc:source><![CDATA[Multilateral Symposium on Safety Research for VVER-Reactors, Cologne, September 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[Neutron embrittlement of reactor pressure vessel is a critical safety-related problem for VVER type reactors. For a better knowledge of this problem an irradiation programme was carried out in the VVER-2 reactor in Rheinsberg from 1984 - 89. With the programme the procedure and methods for the calculation of the transition temperature shift should be examined, the irradiation-induced change of fracture toughness should be determined and the influence of postirradiation annealing had to be investigated. 33 heats of both basic and weld material from low alloyed Cr-Mo-V and Cr-Mo-Ni steels were tested. The neutron fluence amounted to (1.5-79) x 1018 n/cm² (E>1MeV). In the unirradiated state the VVER material shows satisfying properties of strength and toughness and is comparable with the performance of ASTM type steels. The shift of the transition temperature is not always correctly predicted by means of the normally applied trend curves.]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:7-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Eckert, W.]]></dc:creator>
<dc:creator><![CDATA[Knopf, U.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-7-1</dc:identifier>
<dc:title><![CDATA[1000-Dächer-Programm in Sachsen und Thüringen: Programmablauf, Anlagentechnik und Ergebnisse]]></dc:title>
<dc:source><![CDATA[8. Nationales Symposium "Photovoltaische Solarenergie", Staffelstein, 17.-19. März 1993, Tagungsband S. 125]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The paper dealt with the first results of the 1000-Roof-Photovoltaic Programme in the German Federal States of Saxony and Thuringia. Experiences in designing and mounting the pv-plants are discussed. Up to the end of 1992 totally 70 small pv-plants were coupled to the grid in both states. From the first results a mean energy production of about 700 kWh per installed power of 1 kWp can be extrapolated. The most technical difficulties resulted from the used DC-AC-inverters. Additional problems were caused by the grid itself, which was still integrated in the East European Network.
]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:7-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Eckert, W.]]></dc:creator>
<dc:creator><![CDATA[Knopf, U.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-7-7</dc:identifier>
<dc:title><![CDATA[1000-Dächer-Programm in Sachsen und Thüringen: Programmablauf, Anlagentechnik und Ergebnisse]]></dc:title>
<dc:source><![CDATA[8. Nationales Symposium "Photovoltaische Solarenergie", Staffelstein, 17.-19. März 1993, Tagungsband S. 125]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The paper dealt with the first results of the 1000-Roof-Photovoltaic Programme in the German Federal States of Saxony and Thuringia. Experiences in designing and mounting the pv-plants are discussed. Up to the end of 1992 totally 70 small pv-plants were coupled to the grid in both states. From the first results a mean energy production of about 700 kWh per installed power of 1 kWp can be extrapolated. The most technical difficulties resulted from the used DC-AC-inverters. Additional problems were caused by the grid itself, which was still integrated in the East European Network.
]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
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<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-7-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1865-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ferse, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1865-1</dc:identifier>
<dc:title><![CDATA[The Application of the Expert System XUMA in Saxony]]></dc:title>
<dc:source><![CDATA[WINRE'93, 4th Workshop of Information Management in Nuclear Safety, Radiation Protection and Environmental Protection, Köln, November 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[A computer system is presented which will be an effective support for the Saxonian government offices responsible for the evaluation of contaminated sites and the decision concernig the kind of remediation. This system  XUMA (German synonym for expert system on environmental hazards of contaminated sites) includes a knowledge base with the principal methods for handling contaminated sites. The main features of XUMA are:
              Evaluation of contaminated sites,
 	Creation of  analysis plans,
 	Assessment of contaminated sites,
 	Knowledge acquisition tool and
 	Explanation capability.
Furthermore XUMA's embedding into environmental IT-systems in Saxony is described.]]></dc:description>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1865-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1866-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ferse, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1866-1</dc:identifier>
<dc:title><![CDATA[The Possibilities of the Evaluation of Radioactive Contaminated Sites Using the Knowledge-Based System XUMA]]></dc:title>
<dc:source><![CDATA[Karlshors´ter Workshop, Bundesamt für Strahlenschutz, Berlin, November 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The possibilities to evaluate radioactive contaminated sites with knowledge-based methods are discussed on the basis of a knowledge-based evaluation system for non-radioactive sites. The discussion treats methodical and programming aspects.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1867-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Langenbrunner, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1867-1</dc:identifier>
<dc:title><![CDATA[Dispersion of Gas Bubbles in a Two-Dimensional MHD Turbulence]]></dc:title>
<dc:source><![CDATA[7th Beer-Sheva International Seminar on MHD Flows and Turbulence, Jerusalem, 14. - 18. February 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The dispersion of small gas bubbles in a vertical upwards liquid metal two phase flow is investigated theoretically as well as experimentally. Local void fraction measurements are presented for a vertical sodium-argon flow with and without external magnetic field. The dispersion of an initially narrow void distribution shows this behaviour clearly: There is an overall focussing effect of the magnetic field on the void distribution, but the dispersion of gas bubbles is much more suppressed parallel to the field than perpendicular to it.
The bubble transport is modelled by a simple diffusion equation. The model takes into account that bubbles represent no passive tracer of the flow field but have an own dynamics due to their relative velocity to the liquid phase. The experimental results will be analyzed in terms of the corresponding diffusion coefficients.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:3210-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Bagryansky, P. A.]]></dc:creator>
<dc:creator><![CDATA[Anikeev, A. V.]]></dc:creator>
<dc:creator><![CDATA[Collatz, S.]]></dc:creator>
<dc:creator><![CDATA[Deichuli, P. P.]]></dc:creator>
<dc:creator><![CDATA[Ivanov, A. A.]]></dc:creator>
<dc:creator><![CDATA[Karpushov, A. N.]]></dc:creator>
<dc:creator><![CDATA[Korepanov, S. A.]]></dc:creator>
<dc:creator><![CDATA[Lizunov, A. A.]]></dc:creator>
<dc:creator><![CDATA[Maximov, V. V.]]></dc:creator>
<dc:creator><![CDATA[Murakhtin, S. V.]]></dc:creator>
<dc:creator><![CDATA[Noack, K.]]></dc:creator>
<dc:creator><![CDATA[Otto, G.]]></dc:creator>
<dc:creator><![CDATA[Saunichev, K. N.]]></dc:creator>
<dc:creator><![CDATA[Shichovtsev, I. V.]]></dc:creator>
<dc:creator><![CDATA[Shukaev, A. N.]]></dc:creator>
<dc:creator><![CDATA[Stupishin, N. V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3210-1</dc:identifier>
<dc:title><![CDATA[Recent Results of Experiments on the Gas Dynamic Trap]]></dc:title>
<dc:source><![CDATA[International Conference "Open Systems '98", July 27-31, 1998, Novosibirsk, Russia, Transactions of Fusion Technology, 35 (1999) 79]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[This report summarizes the results of experimental investigations obtained during the last five years at the Gas Dynamic Trap experimental facility of the Budker Institute Novosibirsk. Due to an essential upgrade of the main components performed in this period, the following plasma parameters have been achieved: electron temperature - 90-110 eV, fast ion density - up to 0.8*10^13 cm^-3, mean energy of fast ions - 5-8 keV, plasma-ß - 15-20%. The paper describes the following investigations: effect of wall conditioning  on neutral gas dynamics, longitudinal electron heat flux, confinement of the high-ß two-component plasma, fast ion parameters under high-ß conditions, fueling of the target plasma by gas puffing. It presents results of measurements and of calculations.]]></dc:description>
<dc:subject><![CDATA[gas dynamic trap]]></dc:subject>
<dc:subject><![CDATA[plasma parameters]]></dc:subject>
<dc:subject><![CDATA[wall conditioning]]></dc:subject>
<dc:subject><![CDATA[neutral gas]]></dc:subject>
<dc:subject><![CDATA[electron heat flux]]></dc:subject>
<dc:subject><![CDATA[high-ß plasma]]></dc:subject>
<dc:subject><![CDATA[gas puffing]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-3210-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:3210-7</identifier>
<datestamp>2019-03-04</datestamp>
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</header>
<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Bagryansky, P. A.]]></dc:creator>
<dc:creator><![CDATA[Anikeev, A. V.]]></dc:creator>
<dc:creator><![CDATA[Collatz, S.]]></dc:creator>
<dc:creator><![CDATA[Deichuli, P. P.]]></dc:creator>
<dc:creator><![CDATA[Ivanov, A. A.]]></dc:creator>
<dc:creator><![CDATA[Karpushov, A. N.]]></dc:creator>
<dc:creator><![CDATA[Korepanov, S. A.]]></dc:creator>
<dc:creator><![CDATA[Lizunov, A. A.]]></dc:creator>
<dc:creator><![CDATA[Maximov, V. V.]]></dc:creator>
<dc:creator><![CDATA[Murakhtin, S. V.]]></dc:creator>
<dc:creator><![CDATA[Noack, K.]]></dc:creator>
<dc:creator><![CDATA[Otto, G.]]></dc:creator>
<dc:creator><![CDATA[Saunichev, K. N.]]></dc:creator>
<dc:creator><![CDATA[Shichovtsev, I. V.]]></dc:creator>
<dc:creator><![CDATA[Shukaev, A. N.]]></dc:creator>
<dc:creator><![CDATA[Stupishin, N. V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3210-7</dc:identifier>
<dc:title><![CDATA[Recent Results of Experiments on the Gas Dynamic Trap]]></dc:title>
<dc:source><![CDATA[International Conference "Open Systems '98", July 27-31, 1998, Novosibirsk, Russia, Transactions of Fusion Technology, 35 (1999) 79]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[This report summarizes the results of experimental investigations obtained during the last five years at the Gas Dynamic Trap experimental facility of the Budker Institute Novosibirsk. Due to an essential upgrade of the main components performed in this period, the following plasma parameters have been achieved: electron temperature - 90-110 eV, fast ion density - up to 0.8*10^13 cm^-3, mean energy of fast ions - 5-8 keV, plasma-ß - 15-20%. The paper describes the following investigations: effect of wall conditioning  on neutral gas dynamics, longitudinal electron heat flux, confinement of the high-ß two-component plasma, fast ion parameters under high-ß conditions, fueling of the target plasma by gas puffing. It presents results of measurements and of calculations.]]></dc:description>
<dc:subject><![CDATA[gas dynamic trap]]></dc:subject>
<dc:subject><![CDATA[plasma parameters]]></dc:subject>
<dc:subject><![CDATA[wall conditioning]]></dc:subject>
<dc:subject><![CDATA[neutral gas]]></dc:subject>
<dc:subject><![CDATA[electron heat flux]]></dc:subject>
<dc:subject><![CDATA[high-ß plasma]]></dc:subject>
<dc:subject><![CDATA[gas puffing]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-3210-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1518-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Dönau, F.]]></dc:creator>
<dc:creator><![CDATA[Almehed, D.]]></dc:creator>
<dc:creator><![CDATA[Nazmitdinov, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1518-1</dc:identifier>
<dc:title><![CDATA[Integral representation of the RPA correlation energy]]></dc:title>
<dc:source><![CDATA[Physics Review Letters 83, 1999, 280-3]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Using the spectral function F'(z)/F(z) the RPA correlation energy and other properties of a finite system can be written as a contour integral in a compact way. This yields a transparent expression and reduces drastically the numerical efforts for obtaining reliable values. The method applied to pairing vibrations in rotating nuclei as an illustrative example.]]></dc:description>
<dc:subject><![CDATA[Random Phase Approximation]]></dc:subject>
<dc:subject><![CDATA[Hatree-Fock]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1589-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Scheunemann, M.]]></dc:creator>
<dc:creator><![CDATA[Mäding, P.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Iterbeke, K.]]></dc:creator>
<dc:creator><![CDATA[Tourwe, D.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1589-1</dc:identifier>
<dc:title><![CDATA[Die Synthese von <SUP>18</SUP>F-markierten Derivaten des Neurotensins für die Entwicklung neuartiger Radiotracer zur Diagnose von Tumoren]]></dc:title>
<dc:source><![CDATA[4. Deutsches Peptidsymposium 21. - 24. März 1999 / Programm und Abstracts S. 134.]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Neurotensin (NT) ist ein regulatorisches Tridekapeptid (Pyr-Leu-Tyr-Glu-Asn-Lys-Pro-Arg-Arg-Pro-Tyr-Ile-Leu), das bei Säugetieren sowohl im Zentralen Nervensystem als auch im Intestinaltrakt gebildet wird. Membranrezeptoren für dieses Peptid finden sich in verschiedenen Geweben. Insbesondere in manchen Tumoren, u.a. dem kleinzelligen Lungenkarzinom und dem Karzinom der Bauchspeicheldrüse werden Neurotensinrezeptoren verstärkt exprimiert. Das Ziel unserer Untersuchungen bestand darin, das biologisch aktive Hexapeptid NT(8-13) mit dem Isotop <SUP>18</SUP>F in möglichst hoher Chemo- und Regioselektivität für die Anwendung in der Positronen Emissions Tomographie zu markieren. Die Umsetzung von NT(8-13) mit [<SUP>18</SUP>F]SFB gelang  in wässrigem Puffer bei pH 7.2 - 8.3. Das Reaktionsprodukt 4-[<SUP>18</SUP>F]FB-NT(8-13) wurde über eine semipräparative HPLC an RP-18 gereinigt und fällt mit einer radiochemischen Reinheit von >99.5% und einer radiochemischen Ausbeute von 43% (zerfallskorrigiert) an. Die Substanz entspricht in ihrer chromatographischen Charakteristik der Referenzsubstanz, die durch Umsetzung von NT(8-13) mit nichtradioaktivem SFB gewonnen wurde. Durch Einbeziehen von Pseudopeptiden wie [Arg<SUP>8</SUP>Psi(CH<SUB>2</SUB>NH)Arg<SUP>9</SUP>]NT(8-13) möchten wir dem Problem der metabolischen Instabilität natürlicher Peptide in vivo begegnen.]]></dc:description>
<dc:subject><![CDATA[Neurotensin (8-13)]]></dc:subject>
<dc:subject><![CDATA[Neurotensinrezeptor]]></dc:subject>
<dc:subject><![CDATA[Positronen Emissions Tomographie]]></dc:subject>
<dc:subject><![CDATA[[<SUP>18</SUP>F]SFB]]></dc:subject>
<dc:subject><![CDATA[Pseudopeptid]]></dc:subject>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:14476-2</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Willschütz, H.-G.]]></dc:creator>
<dc:creator><![CDATA[Diercks, F.]]></dc:creator>
<dc:creator><![CDATA[Leyer, S.]]></dc:creator>
<dc:creator><![CDATA[Krüssenberg, A.-K.]]></dc:creator>
<dc:creator><![CDATA[Schäfer, F.]]></dc:creator>
<dc:creator><![CDATA[Hristov, H. V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14476-2</dc:identifier>
<dc:title><![CDATA[Experimentelle und analytische Untersuchungen zu passiven Komponenten des KERENA TM Konzeptes im Versuchsstand INKA]]></dc:title>
<dc:source><![CDATA[42. Kraftwerkstechnisches Kolloquium 2010, 12.-13.10.2010, Congress Center Dresden, Deutschland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Das KERENA TM  - Konzept ist eine kontinuierliche  Weiterentwicklung der seit Jahren bewährten (deutschen) Siedewassertechnologie der "Baulinie 72". Die Kombination von betriebserprobten aktiven Sicherheitssystemen mit neu hinzugekommenen passiven Sicherheitssystemen setzt die Forderungen der "Defense in Depth"-Philsophie konsequent um. Insbesondere für die neu eingeführten passiven Sicherheitssysteme muss das Betriebsverhalten durch experimentelle Untersuchungen validiert und die thermohydraulischen Berechnungsprogramme müssen qualifiziert werden, so dass sie die auftretenden Naturumlaufphänomene korrekt berechnen können. Mit den vorliegenden Arbeiten wird die Eignung des Thermohydraulikprogrammsystems ATHLET der Gesellschaft für Anlagen- und Reaktorsicherheit (GRS) mbH als ein Programm, das im Genehmigungs- und Aufsichtsverfahren in verschiedenen Ländern eingesetzt wird, zur Berechnung des Betriebsverhalten der passiven Komponenten untersucht. Dazu wurde ein Modell für die Versuchsanlage INKA (INtegral test facility in KArlstein) entwickelt, mit dem sowohl Vorausrechnungen des Kennfelds der passiven Komponenten Notkondensator und Gebäudekondensator als auch Nachrechnungen zu Experimenten durchgeführt wurden.]]></dc:description>
<dc:subject><![CDATA[KERENA]]></dc:subject>
<dc:subject><![CDATA[ATHLET]]></dc:subject>
<dc:subject><![CDATA[Boiling Water Reactor]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
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<dc:audience>Students</dc:audience>
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<identifier>HZDR:PUBLDB:14476-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Willschütz, H.-G.]]></dc:creator>
<dc:creator><![CDATA[Diercks, F.]]></dc:creator>
<dc:creator><![CDATA[Leyer, S.]]></dc:creator>
<dc:creator><![CDATA[Krüssenberg, A.-K.]]></dc:creator>
<dc:creator><![CDATA[Schäfer, F.]]></dc:creator>
<dc:creator><![CDATA[Hristov, H. V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14476-1</dc:identifier>
<dc:title><![CDATA[Experimentelle und analytische Untersuchungen zu passiven Komponenten des KERENA TM Konzeptes im Versuchsstand INKA]]></dc:title>
<dc:source><![CDATA[42. Kraftwerkstechnisches Kolloquium 2010, 12.-13.10.2010, Congress Center Dresden, Deutschland<br>Experimentelle und analytische Untersuchungen zu passiven Komponenten des KERENA TM Konzeptes im Versuchsstand INKA]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Das KERENA TM  - Konzept ist eine kontinuierliche  Weiterentwicklung der seit Jahren bewährten (deutschen) Siedewassertechnologie der "Baulinie 72". Die Kombination von betriebserprobten aktiven Sicherheitssystemen mit neu hinzugekommenen passiven Sicherheitssystemen setzt die Forderungen der "Defense in Depth"-Philsophie konsequent um. Insbesondere für die neu eingeführten passiven Sicherheitssysteme muss das Betriebsverhalten durch experimentelle Untersuchungen validiert und die thermohydraulischen Berechnungsprogramme müssen qualifiziert werden, so dass sie die auftretenden Naturumlaufphänomene korrekt berechnen können. Mit den vorliegenden Arbeiten wird die Eignung des Thermohydraulikprogrammsystems ATHLET der Gesellschaft für Anlagen- und Reaktorsicherheit (GRS) mbH als ein Programm, das im Genehmigungs- und Aufsichtsverfahren in verschiedenen Ländern eingesetzt wird, zur Berechnung des Betriebsverhalten der passiven Komponenten untersucht. Dazu wurde ein Modell für die Versuchsanlage INKA (INtegral test facility in KArlstein) entwickelt, mit dem sowohl Vorausrechnungen des Kennfelds der passiven Komponenten Notkondensator und Gebäudekondensator als auch Nachrechnungen zu Experimenten durchgeführt wurden.]]></dc:description>
<dc:subject><![CDATA[KERENA]]></dc:subject>
<dc:subject><![CDATA[ATHLET]]></dc:subject>
<dc:subject><![CDATA[Boiling Water Reactor]]></dc:subject>
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<identifier>HZDR:PUBLDB:1576-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1576-1</dc:identifier>
<dc:title><![CDATA[Analysis of the Exercise 2 of the OECD - MSLB Benchmark with the Code DYN3D/R]]></dc:title>
<dc:source><![CDATA[M&C'99 - Madrid International Conference on Mathematics and Computation, Reactor Physics and Enviromental Analysis in Nuclear Applications, pp. 1794-1803, Madrid, 27-30 September 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The Cartesian version of the 3D core model DYN3D coupled with the thermohydraulic plant
model ATHLET will be used for the analysis of the OECD Main Steam Line Break (MSLB)
Benchmark which is based on real plant design and operational data of the TMI-1 PWR.  The
three exercises of the benchmark are a point kinetics plant simulation (exercise 1), a
coupled 3D neutronics/core thermal-hydraulics evaluation of the core response (exercise 2)
and a best estimate coupled core-plant transient analysis (exercise 3).  The presented
calculations of the exercise 2 are performed with the DYN3D code alone.  The core boundary
conditions provided by calculations of the Penn State University with the TRAC-PF1/NEM code
system are used as input for the two scenarios of this exercise.  Considering the best
estimate case (scenario 1) the reactor does not become critical during the transient.
Defining a more serious test for the codes, the efficiency of the control rods was
decreased to obtain a return to power in the transient (scenar io 2).  The influence of
different thermohydraulic modelling on the results is investigated with the help of the
DYN3D calculations for scenario 2.  The core averaged values as the total nuclear power or
the reactivity show a low sensitivity against the variation of the thermohydraulic model.
Considering local values as the maximum nodal Doppler temperature an impact of the
thermohydraulic model is observed.]]></dc:description>
<dc:subject><![CDATA[main steam line break]]></dc:subject>
<dc:subject><![CDATA[benchmark]]></dc:subject>
<dc:subject><![CDATA[pressurized water reactor]]></dc:subject>
<dc:subject><![CDATA[coupled neutronic thermohydraulic codes]]></dc:subject>
<dc:subject><![CDATA[DYN3D]]></dc:subject>
<dc:subject><![CDATA[ATHLET]]></dc:subject>
<dc:subject><![CDATA[3-dimensional]]></dc:subject>
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<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1576-7</dc:identifier>
<dc:title><![CDATA[Analysis of the Exercise 2 of the OECD - MSLB Benchmark with the Code DYN3D/R]]></dc:title>
<dc:source><![CDATA[M&C'99 - Madrid International Conference on Mathematics and Computation, Reactor Physics and Enviromental Analysis in Nuclear Applications, pp. 1794-1803, Madrid, 27-30 September 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The Cartesian version of the 3D core model DYN3D coupled with the thermohydraulic plant
model ATHLET will be used for the analysis of the OECD Main Steam Line Break (MSLB)
Benchmark which is based on real plant design and operational data of the TMI-1 PWR.  The
three exercises of the benchmark are a point kinetics plant simulation (exercise 1), a
coupled 3D neutronics/core thermal-hydraulics evaluation of the core response (exercise 2)
and a best estimate coupled core-plant transient analysis (exercise 3).  The presented
calculations of the exercise 2 are performed with the DYN3D code alone.  The core boundary
conditions provided by calculations of the Penn State University with the TRAC-PF1/NEM code
system are used as input for the two scenarios of this exercise.  Considering the best
estimate case (scenario 1) the reactor does not become critical during the transient.
Defining a more serious test for the codes, the efficiency of the control rods was
decreased to obtain a return to power in the transient (scenar io 2).  The influence of
different thermohydraulic modelling on the results is investigated with the help of the
DYN3D calculations for scenario 2.  The core averaged values as the total nuclear power or
the reactivity show a low sensitivity against the variation of the thermohydraulic model.
Considering local values as the maximum nodal Doppler temperature an impact of the
thermohydraulic model is observed.]]></dc:description>
<dc:subject><![CDATA[main steam line break]]></dc:subject>
<dc:subject><![CDATA[benchmark]]></dc:subject>
<dc:subject><![CDATA[pressurized water reactor]]></dc:subject>
<dc:subject><![CDATA[coupled neutronic thermohydraulic codes]]></dc:subject>
<dc:subject><![CDATA[DYN3D]]></dc:subject>
<dc:subject><![CDATA[ATHLET]]></dc:subject>
<dc:subject><![CDATA[3-dimensional]]></dc:subject>
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Scheffler, M.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Runkel, J.]]></dc:creator>
<dc:creator><![CDATA[Südmersen, U.]]></dc:creator>
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<dc:title><![CDATA[Numerische und experimentelle Untersuchungen zum Schwingungsverhalten eines Siedewasserreaktors]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik '97, Aachen, 13. - 15. Mai 1997, Tagungsbericht S.437]]></dc:source>
<dc:date>1997</dc:date>
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<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
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<dc:title><![CDATA[Technische Überprüfung von Photovoltaik-Systemen]]></dc:title>
<dc:source><![CDATA[12. Symposium Photovoltaische Solarenergie, Staffelstein, 26. - 28. 2. 1997, Tagungsband S. 140]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Die Erfahrungen der Vermessung und von durchgeführten Vorort-Inspektionen an mehr als 100 PV-Anlagen zeigen die derzeit noch bestehende Notwendigkeit der Durchführung solcher Inspektionen. Das Ziel besteht in der Gewährleistung der Funktion und der Qualität des Gesamtsystems. Auf einzelne häufiger anzutreffende Fehlerquellen wird detailliert eingegangen.]]></dc:description>
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<dc:title><![CDATA[Technische Überprüfung von Photovoltaik-Systemen]]></dc:title>
<dc:source><![CDATA[12. Symposium Photovoltaische Solarenergie, Staffelstein, 26. - 28. 2. 1997, Tagungsband S. 140]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Die Erfahrungen der Vermessung und von durchgeführten Vorort-Inspektionen an mehr als 100 PV-Anlagen zeigen die derzeit noch bestehende Notwendigkeit der Durchführung solcher Inspektionen. Das Ziel besteht in der Gewährleistung der Funktion und der Qualität des Gesamtsystems. Auf einzelne häufiger anzutreffende Fehlerquellen wird detailliert eingegangen.]]></dc:description>
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<dc:creator><![CDATA[Thess, A.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1907-1</dc:identifier>
<dc:title><![CDATA[Linear Stability of Marangoni-Hartmann Convection]]></dc:title>
<dc:source><![CDATA[Ed. H. J. Rath: Microgravity Fluid Dynamics, Berlin, Heidelberg, New York, Springer 1992, p. 285 - 296]]></dc:source>
<dc:date>1992</dc:date>
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<dc:title><![CDATA[Modelling of Fuel Rod Behavior and Heat Transfer in the Code FLOCAL for Reactivity Accident Analysis of Reactor Cores]]></dc:title>
<dc:source><![CDATA[Proceedings of the First Baltic Heat Transfer Conference (Gothenburg, Sweden, August 1991)]]></dc:source>
<dc:date>1991</dc:date>
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<dc:title><![CDATA[Modelling of Fuel Rod Behavior and Heat Transfer in the Code FLOCAL for Reactivity Accident Analysis of Reactor Cores]]></dc:title>
<dc:source><![CDATA[Transport Processes in Engineering 2: Recent Advances in Heat Transfer, Elsevier Publ., Amsterdam, 1992, p. 1214 - 1228]]></dc:source>
<dc:date>1992</dc:date>
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<dc:creator><![CDATA[Schuster, G.]]></dc:creator>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
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<dc:title><![CDATA[Neutronographische Untersuchungen zur Temperaturabhängigkeit der Besetzung der Sauerstoffpositionen in der YBa2 Cu30 O(x-7) - Elemtarzelle]]></dc:title>
<dc:source><![CDATA[Proc. Jahrestagung der Deutschen Gesellschaft für Kristallwachstum und Kristallzüchtung, Dresden, March 1992]]></dc:source>
<dc:date>1992</dc:date>
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<dc:creator><![CDATA[Schuster, G.]]></dc:creator>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Teske, K.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
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<dc:title><![CDATA[Unexpected polymeric string formation between Ag(I) and a homoleptic cage: Synthesis and crystal structure of [R,R'-S6tricosane] and {[Ag(R,R'-S6hexacosane)(tos)]}]]></dc:title>
<dc:source><![CDATA[Communication in J. Chem. Soc. Chem. Communications]]></dc:source>
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<dc:description><![CDATA[The large cavity homoleptic thioether cages [R,R'-S6tricosane] (1-hydroxymethyl-9-methyl-3,7,11,15,18,22-hexathiabicyclo[7.7.7]tricosane) (1) and [R,R'S6hexacosane] (1-hydroxymethyl-10-methyl-3,8,12,17,20,25-hexathiabicyclo[8.8.8]hexacosane) (2) have been synthesized and the structure of 1 and the complex [Ag(2)](tos)¥ been elucitated, the latter one showing a polymeric string with Ag+ coordinating by three different cages.


]]></dc:description>
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<dc:source><![CDATA[Nuclear Physics A 607 (1996) pp. 457-486]]></dc:source>
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<dc:creator><![CDATA[Müller, R.]]></dc:creator>
<dc:creator><![CDATA[Gleisberg, O.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-975-1</dc:identifier>
<dc:title><![CDATA[Untersuchung der Wechselwirkungen zwischen ZrNb1 und austenitischem Stahl bei hohen Temperaturen]]></dc:title>
<dc:source><![CDATA[29. Kolloquium des Arbeitskreises für Elektronenmikroskopische Direktabbildung und Analyse von Oberflächen (EDO) 8.-11. Oktober 1996 in Münster]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:975-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Müller, R.]]></dc:creator>
<dc:creator><![CDATA[Gleisberg, O.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-975-2</dc:identifier>
<dc:title><![CDATA[Untersuchung der Wechselwirkungen zwischen ZrNb1 und austenitischem Stahl bei hohen Temperaturen]]></dc:title>
<dc:source><![CDATA[Elektronenmikroskop. Direktabb. und Analyse v. Oberfl., 29 (1996)]]></dc:source>
<dc:date>1996</dc:date>
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<header>
<identifier>HZDR:PUBLDB:2230-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Jankuhn, S.]]></dc:creator>
<dc:creator><![CDATA[Butz, T.]]></dc:creator>
<dc:creator><![CDATA[Flagmeyer, R.-H.]]></dc:creator>
<dc:creator><![CDATA[Reinert, T.]]></dc:creator>
<dc:creator><![CDATA[Vogt, J.]]></dc:creator>
<dc:creator><![CDATA[Barckhausen, B.]]></dc:creator>
<dc:creator><![CDATA[Hammerl, J.]]></dc:creator>
<dc:creator><![CDATA[Protsch Von Zieten, R.]]></dc:creator>
<dc:creator><![CDATA[Grambole, D.]]></dc:creator>
<dc:creator><![CDATA[Herrmann, F.]]></dc:creator>
<dc:creator><![CDATA[Bethge, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2230-1</dc:identifier>
<dc:title><![CDATA[Untersuchung historischer menschlicher Knochen mit Ionen-Mikrosonde]]></dc:title>
<dc:source><![CDATA[Frühjahrstagung der Fachverbände Chemische Physik, Kurzzeitphysik, Plasmaphysik,  Polymerphysik, Bayreuth, March 9 - 13, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:1937-1</identifier>
<datestamp>2023-05-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Alberto, R.]]></dc:creator>
<dc:creator><![CDATA[Dilworth, J. R.]]></dc:creator>
<dc:creator><![CDATA[Zheng, Y.]]></dc:creator>
<dc:creator><![CDATA[Ortner, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1937-1</dc:identifier>
<dc:title><![CDATA[Rhenium and Technetium Complexes with Diphenyl(2-pyridyl)phosphine]]></dc:title>
<dc:source><![CDATA[Polyhedron 18 (1999) 2995-3005]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The potentially bidentate ligand diphenyl(2-pyridyl)phosphine (PPh2py) reacted with (NEt4)2[MI(CO)3X3] complexes (M = Re, Tc) to give (NEt4)[MI(CO)3X2(PPh2py-P)] or [MI(CO)3X(PPh2py-P)2] depending on the amount of the ligand used. The reaction with (NBu4)[TcVINCl4] yielded [TcVNCl2(PPh2py-P)2] whereas from the reaction with (NBu4)[ReOCl4] the complexes [ReVOCl3(PPh2py-P,N)], [ReVOCl3(OPPh2py-O,N)], [ReIVCl4(OPPh2py-O,N) and [ReIVCl3(OH)(OPPh2py-O,N)] have been isolated. Reduction of the metal center occurs using an excess of PPh2py and heating of the reaction mixtures under reflux. 
The products have been characterised spectroscopically and by X-ray structure analysis. Monodentate co-ordination via phosphorus has been found for the rhenium(I) carbonyl complexes and [TcVNCl2(PPh2py-P)2]. In the latter compound a trigonal-bipyramidal coordination sphere is formed with the phosphines as axial ligands (bond angle P-Re-P: 161.69(3)°).  The chelated complexes show small N-Re-P and N-Re-O bite angles of  63.6°  and 77.7 - 82.2° due to the 4-membered or 5-membered chelate rings. The pyridine nitrogen occupies the axial position (trans to "O2-")  in [ReOCl3(PPh2py-P,N)] whereas equatorial co-ordination is found in [ReOCl3(OPPh2py-O,N)].]]></dc:description>
<dc:subject><![CDATA[Rhenium]]></dc:subject>
<dc:subject><![CDATA[Technetium]]></dc:subject>
<dc:subject><![CDATA[Diphenylpyridylphosphine]]></dc:subject>
<dc:subject><![CDATA[Diphenylpyridylphosphine oxide]]></dc:subject>
<dc:subject><![CDATA[X-ray structures]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:202-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Liewers, P.]]></dc:creator>
<dc:creator><![CDATA[Scheffler, M.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-202-2</dc:identifier>
<dc:title><![CDATA[Component Vibration of VVER-reactors -Diagnostics and modelling-]]></dc:title>
<dc:source><![CDATA[IMORN-25, 13.-15. Juni 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Flow induced vibrations of reactor pressure vessel (RPV) internals (control element and core barrel motions) at VVER-440 reactors have lead to the development of dedicated methods for on-line monitoring. These methods need a certain developed stage of the faults to be detected. To achieve a real sensitive early detection of mechanical faults of RPV internals, a theoretical vibration model was developed based on finite elements. The model comprises the whole primary circuit including the steam generators (SG). By means of that model all eigenfrequencies up to 30 Hz and the corresponding mode shapes were calculated for the normal vibration behaviour. Moreover the shift of eigenfrequencies and of amplitudes due to the degradation or to the failure of internal clamping and spring elements could be investigated, showing that a recognition of such degradations even inside the RPV is possible by pure excore vibration measurements. A true diagnostics, that is the identification of the failed component, might become possible because different faults influence different and well separated eigenfrequencies.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:202-1</identifier>
<datestamp>2020-12-07</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Liewers, P.]]></dc:creator>
<dc:creator><![CDATA[Scheffler, M.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-202-1</dc:identifier>
<dc:title><![CDATA[Component Vibration of VVER-reactors -Diagnostics and modelling-]]></dc:title>
<dc:source><![CDATA[Progress in Nuclear Energy, Vol. 29, Number 3/4, pp. 129 - 138]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Flow induced vibrations of reactor pressure vessel (RPV) internals (control element and core barrel motions) at VVER-440 reactors have lead to the development of dedicated methods for on-line monitoring. These methods need a certain developed stage of the faults to be detected. To achieve a real sensitive early detection of mechanical faults of RPV internals, a theoretical vibration model was developed based on finite elements. The model comprises the whole primary circuit including the steam generators (SG). By means of that model all eigenfrequencies up to 30 Hz and the corresponding mode shapes were calculated for the normal vibration behaviour. Moreover the shift of eigenfrequencies and of amplitudes due to the degradation or to the failure of internal clamping and spring elements could be investigated, showing that a recognition of such degradations even inside the RPV is possible by pure excore vibration measurements. A true diagnostics, that is the identification of the failed component, might become possible because different faults influence different and well separated eigenfrequencies.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/0149-1970(95)00002-2]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:1835-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barz, H.-U.]]></dc:creator>
<dc:creator><![CDATA[Böhmer, B.]]></dc:creator>
<dc:creator><![CDATA[Konheiser, J.]]></dc:creator>
<dc:creator><![CDATA[Stephan, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1835-1</dc:identifier>
<dc:title><![CDATA[High Precision Neutron Fluence Calculations, Activation Measurements and Spectrum Adjustment for the Rheinsberg Pressure Vessel Steel Irradiation Program]]></dc:title>
<dc:source><![CDATA[Presentation to the EWGRD, WGRD-VVER Meeting, Rez, Tschechien, April 18 - 22, 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The overall approach comprises the pure calculation part, the gamma spectrometric analyses of fluence monitors and the comparison of theoretical and experimental results using the spectrum adjustment procedure. Monte Carlo methods were used to perform the transport calculations. By application of special measures of variance reduction the statistical errors could be reduced so much that accurate 3-dimensional Monte Carlo methods could be generally used in reasonable calculation time. The uncertainties of the results due to the use of different group values of neutron cross sections were assessed by testing different group sets. In that way it could be shown that the kind of group data is of minor influence.]]></dc:description>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1809-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1809-1</dc:identifier>
<dc:title><![CDATA[Irradiation Programme in the Rheinsberg VVER-2 Reactor to Evaluate the Susceptibility of Russian Reactor Pressure Vessel Steels against Neutron Embrittlement]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik, Stuttgart, 17. - 19. Mai 1994, Proc. pp. 388 - 391]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[An extensive irradiation programme was performed in the Rheinsberg VVER-2 reactor from 1984 to 1988. The programm comprised 25 different heats from  base or weld metal of VVER-440- and 1000-type reactor pressure vessel steels using specimens of variant geometry (CT, COD, tension, Charpy-V). Mainly, it focused on validating of the safety assessment procedure and on determining of fracture mechanics parameters in their dependence of fluence and thermal annealing.
At present the investigation of the irradiated specimen is still outstanding. In the unirradiated state all VVER-type steels investigated show good toughness and strength properties and are comparable with A 533 class 1 and A 508 class 3 steels. The scattering between the different heats of same materials is partly large and does not correlate with the chemical composition or the heat treatment. The results of irradiated specimens up to now do not always confirm the values which are obtained on the base of the valid safety assessment procedure in a conserva- tive wise. That supports the urgency to extend the data base for irradiated VVER-type pressure vessel steels.]]></dc:description>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1809-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1836-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Eichhorn, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1836-1</dc:identifier>
<dc:title><![CDATA[Characterisation of Irradiation-Induced Precipitates in VVER-Type RPV Steel 15Kh2MFA by Anomalous Small Angle Ray Scattering]]></dc:title>
<dc:source><![CDATA[5th Meeting of the International Group on Radiation Damage Mechanisms, Santa Barbara, May 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Irradiation-induced precipitates are the cause for neutron embrittlement of reactor pressure vessel steels. It can be shown that for the VVER-type steel 15Kh2MFA the shift in the ductile-brittle transition temperature depends nearly linearly on the volume fraction of these precipitates.
The nature of the irradiation-induced precipitates has been investigated at the steel 15Kh2MFA. This steel differes from ASTM-type A503 and 533 steels mainly in its content of the carbide forming elements chromium, molybdenum and vanadium.
Small angle neutron scattering (SANS) experiments using the SANS-2 facility at the FRG-1 reactor in Geesthacht (Germany) were employed in the past. SANS gives information about size and volume fraction of the precipitates, but hardly about the chemical composition.
In order to prove and to characterize the nature of the irradiation-induced precipi- tates anomalous small angle X-ray scattering (ASAXS) has been carried out at the JUSIFA facility of Hamburg synchrotron laboratory HASYLAB (Germany) at present. By the method of contrast variation, it is also possible to get information on the chemical composition.
ASAXS experiments with contrast variation at energies near the vanadium-K -absorption-edge reveal the content of vanadium within the irradiation-induced precipitates. The scattering density of the precipitates is lower than the scattering density of the iron matrix. The chemical shift of the vanadium K -absorption-edge shows that vanadium does not precipitate in an elementary state. Assuming, the precipitates are vanadium carbide these results can be explained. The results are in accordance with those of SANS experiments and former positron annihilation spectroscopy experiments.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:229-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Bojarevics, A.]]></dc:creator>
<dc:creator><![CDATA[Gelfgat, Y. M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-229-1</dc:identifier>
<dc:title><![CDATA[Thermocapillary convection in a liquid metal under influence of the magnetic field - experimental techniques and results of the tests]]></dc:title>
<dc:source><![CDATA[Konferenz "Energy Transfer in MHO Flows", Aussois / France, Sept.1994, pp. 117 - 126]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Thermocapillary convection in low-Prandtl-number fluids up to now remains insufficiently studied experimentally due to difficulties to realize free surface conditions on liquid metals. A novel technique has been developed to produce small sized easily transportable deep vacuum container filled with a thin layer of gallium under a transparent glass window. The first tests showed that the free surface of the liquid gallium did not deteriorate during a period of up to 45 days. The flow pattern on the free surface, while point heating the bottom of the container, has been demonstrated. The temperature gradient on the free surface of the liquid gallium caused surface relief deformations of an order up to 10 - 100 microns. Video recordings of the tracer particle motion on the free surface of liquid gallium due to thermal convection and surface relief deformations due to changes in heating conditions has been made. The presence of the thermocapillary convection has been demonstrated.]]></dc:description>
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<identifier>HZDR:PUBLDB:229-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Bojarevics, A.]]></dc:creator>
<dc:creator><![CDATA[Gelfgat, Y. M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-229-7</dc:identifier>
<dc:title><![CDATA[Thermocapillary convection in a liquid metal under influence of the magnetic field - experimental techniques and results of the tests]]></dc:title>
<dc:source><![CDATA[Konferenz "Energy Transfer in MHO Flows", Aussois / France, Sept.1994, pp. 117 - 126]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Thermocapillary convection in low-Prandtl-number fluids up to now remains insufficiently studied experimentally due to difficulties to realize free surface conditions on liquid metals. A novel technique has been developed to produce small sized easily transportable deep vacuum container filled with a thin layer of gallium under a transparent glass window. The first tests showed that the free surface of the liquid gallium did not deteriorate during a period of up to 45 days. The flow pattern on the free surface, while point heating the bottom of the container, has been demonstrated. The temperature gradient on the free surface of the liquid gallium caused surface relief deformations of an order up to 10 - 100 microns. Video recordings of the tracer particle motion on the free surface of liquid gallium due to thermal convection and surface relief deformations due to changes in heating conditions has been made. The presence of the thermocapillary convection has been demonstrated.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:3424-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3424-1</dc:identifier>
<dc:title><![CDATA[Ion Implantation Induced Defects in 6H-SiC and Their Annealing Behaviour]]></dc:title>
<dc:source><![CDATA[Materials Science Forum 363-365 (2001) 442]]></dc:source>
<dc:date>2001</dc:date>
<dc:description><![CDATA[Fourfold Al+ implantations into 6H-SiC have been carried out in order to create a laterally structured p-doped layer. This way, a 400 nm thick box-shaped Al profile with a concentration plateau of 5x1019 cm-3 buried 200 nm below the SiC surface could be realized. The defects caused by the ion implantation should be minimized by implantation at higher substrate temperatures and post implantation annealing. In addition to the traditional furnace annealing a flash lamp annealing has been used. The defect structure after implantation and annealing has been investigated by Slow Positron Implantation Spectroscopy (SPIS). It could be shown that vacancies and vacancy agglomerates can be removed using furnace annealing at 1650 0C. However, dislocation loops in the implantation region remain stable at this temperature. Using flash lamp annealing a further defect removal could be observed. ]]></dc:description>
<dc:subject><![CDATA[6H-SiC]]></dc:subject>
<dc:subject><![CDATA[ion implantation]]></dc:subject>
<dc:subject><![CDATA[radiation damage]]></dc:subject>
<dc:subject><![CDATA[post implantation heat treatment]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:3424-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3424-2</dc:identifier>
<dc:title><![CDATA[Ion Implantation Induced Defects in 6H-SiC and Their Annealing Behaviour]]></dc:title>
<dc:source><![CDATA[12th International Conference on Positron Annihilation, München, Germany, August 6-12, 2000]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Fourfold Al+ implantations into 6H-SiC have been carried out in order to create a laterally structured p-doped layer. This way, a 400 nm thick box-shaped Al profile with a concentration plateau of 5x1019 cm-3 buried 200 nm below the SiC surface could be realized. The defects caused by the ion implantation should be minimized by implantation at higher substrate temperatures and post implantation annealing. In addition to the traditional furnace annealing a flash lamp annealing has been used. The defect structure after implantation and annealing has been investigated by Slow Positron Implantation Spectroscopy (SPIS). It could be shown that vacancies and vacancy agglomerates can be removed using furnace annealing at 1650 0C. However, dislocation loops in the implantation region remain stable at this temperature. Using flash lamp annealing a further defect removal could be observed. ]]></dc:description>
<dc:subject><![CDATA[6H-SiC]]></dc:subject>
<dc:subject><![CDATA[ion implantation]]></dc:subject>
<dc:subject><![CDATA[radiation damage]]></dc:subject>
<dc:subject><![CDATA[post implantation heat treatment]]></dc:subject>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<record>
<header>
<identifier>HZDR:PUBLDB:3148-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3148-1</dc:identifier>
<dc:title><![CDATA[Theoretische Beschreibung von Implantationsprozessen. Grundlagen, Methoden, Anwendungen]]></dc:title>
<dc:source><![CDATA[Sommerschule "Nukleare Sonden und Ionen", Bad Blankenburg, Germany, Sept. 21-25, 1998 (invited lecture)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-3148-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:3151-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3151-1</dc:identifier>
<dc:title><![CDATA[Determination of the as-implanted defect structure in silicon by a combined simulation method]]></dc:title>
<dc:source><![CDATA[MRS-ICAM99 Conference, Symposium JJ: Multiscale Materials Modeling, Beijing, China, June 13-18, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1871-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1871-1</dc:identifier>
<dc:title><![CDATA[A Method for Acoustic Leak Detection at Complicated Geometrical Structures]]></dc:title>
<dc:source><![CDATA[IMORN-24 (Informal Meeting on Reactor Noise), Oybin / Germany, 23 - 25 June 1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[A method for detecting and localizing leaks at complicated three-dimensional topologies by measuring the leak induced structure-borne and airborne sound and by applying pattern recognition procedures is being developed. The sound patterns necessary to train fuzzy logic classifiers and neural networks are generated with simulated leaks at the original structure. As features for characterizing the occurrence and the location of a leak, coherence values between high-frequency microphone signals and RMS-values of acoustic emission sensors are used. The method is even applicable when localization based on propagation time differences or sound attenuation differences fail.]]></dc:description>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<record>
<header>
<identifier>HZDR:PUBLDB:48-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kereszturi, A.]]></dc:creator>
<dc:creator><![CDATA[Telbisz, M.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Krell, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-48-1</dc:identifier>
<dc:title><![CDATA[Results of a three-dimensional hexagonal kinetic benchmark problem]]></dc:title>
<dc:source><![CDATA[ENS Regional Meeting in Portoroz 1993 "Nuclear Energy in Central Europe: Present and Perspectives"]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The recent safety analysis investigations of the VVER type reactors require the use of three-dimensional hexagonal kinetic codes. For this purpose the codes KIKO3D and DYN3D were developed in the Atomic Research Institute Budapest and in the Research Center Rossendorf, respectively. The kinetic codes have to be validated before being used for safety assessments. A benchmark problem is defined, as the first step of the validation procedure of hexagonal kinetic programs.
The problem describes a rod ejection transient in a VVER-type geometry, where the worth of the ejected rod is just below the prompt critical value. The initial power is near to zero and the power rise is not too large. Therefore, the transient can be treated without feedback based on given the time-dependence of the cross sections and geometry.
KIKO3D results are presented, i.e the solution of time dependent nodal equations by the Improved Quasistatic (IQS) Method. The time dependence of the integrated power and the reactivity are compared with the adiabatic results. These results are also compared with the results of two different DYN3D calculations carried out in Rossendorf and in Berlin. ]]></dc:description>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-48-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1872-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1872-1</dc:identifier>
<dc:title><![CDATA[ISP-33 Pre- and Posttest Calculations in the FZR Rossendorf]]></dc:title>
<dc:source><![CDATA[2nd Workshop ISP-33, Lappeeranta / Finland, 17 - 19 May 1993, ISP-33 Compasion Report, OECD/NEA in preparation]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[Calculations relating to the OECD/NEA/CSNI International Standard Problem No. 33 were carried out with the GRS code ATHLET.This problem was a natural circulation experiment with primary coolant inventory reduced stepwise. The experiment was conducted in the PACTEL facility in Lappeenranta (Finland), which is a 1/305 volumetrically  scaled,  full  height  three  loop  simulator of the Russian VVER-440 type reactor. The main events of the experiment could be shown and explained by the ATHLET calculations:
-	After the second draining the mass flow in the loops stagnates. Simultaneously, the primary pressure increases and the pressurizer is partly refilled.
-	In the periods after the third drain step the mass flow through the three loops is nonequally distributed, which could be reproduced by the ATHLET calculations at least qualitatively.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1872-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:14498-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Duerigen, S.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Mittag, S.]]></dc:creator>
<dc:creator><![CDATA[Merk, B.]]></dc:creator>
<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14498-1</dc:identifier>
<dc:title><![CDATA[A nodal SP3 approach for reactors with hexagonal fuel assemblies]]></dc:title>
<dc:source><![CDATA[20th Symposium of AER on VVER Reactor Physics and Reactor Safety, 20.-24.09.2010, Hanasaari, Espoo, Finland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The neutronics model of the nodal reactor dynamics code DYN3D developed for 3-D analyses of steady states and transients in light-water reactors has been extended by a simplified P3 (SP3) neutron transport option to overcome the limitations of the diffusion approach. To provide a method being applicable to reactors with hexagonal fuel assemblies and furthermore allowing flexible mesh refinement, the nodal SP3 method has been
developed on the basis of a flux expansion in trigonal-z geometry. Dividing a hexagonal fuel assembly into six triangular nodes, steady-state test calculations for one assembly as well as for a 'minicore' consisting of seven fuel assemblies have been performed, in which both a symmetric and an asymmetric material composition are chosen to be compared with more accurate HELIOS transport calculations in each case.]]></dc:description>
<dc:subject><![CDATA[nodal]]></dc:subject>
<dc:subject><![CDATA[simplified P3]]></dc:subject>
<dc:subject><![CDATA[SP3]]></dc:subject>
<dc:subject><![CDATA[DYN3D]]></dc:subject>
<dc:subject><![CDATA[trigonal]]></dc:subject>
<dc:subject><![CDATA[hexagonal]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<header>
<identifier>HZDR:PUBLDB:14498-2</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Duerigen, S.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Mittag, S.]]></dc:creator>
<dc:creator><![CDATA[Merk, B.]]></dc:creator>
<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14498-2</dc:identifier>
<dc:title><![CDATA[A nodal SP3 approach for reactors with hexagonal fuel assemblies]]></dc:title>
<dc:source><![CDATA[20th Symposium of AER on VVER Reactor Physics and Reactor Safety, 20.-24.09.2010, Hanasaari, Espoo, Finland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The neutronics model of the nodal reactor dynamics code DYN3D developed for 3-D analyses of steady states and transients in light-water reactors has been extended by a simplified P3 (SP3) neutron transport option to overcome the limitations of the diffusion approach. To provide a method being applicable to reactors with hexagonal fuel assemblies and furthermore allowing flexible mesh refinement, the nodal SP3 method has been
developed on the basis of a flux expansion in trigonal-z geometry. Dividing a hexagonal fuel assembly into six triangular nodes, steady-state test calculations for one assembly as well as for a 'minicore' consisting of seven fuel assemblies have been performed, in which both a symmetric and an asymmetric material composition are chosen to be compared with more accurate HELIOS transport calculations in each case.]]></dc:description>
<dc:subject><![CDATA[nodal]]></dc:subject>
<dc:subject><![CDATA[simplified P3]]></dc:subject>
<dc:subject><![CDATA[SP3]]></dc:subject>
<dc:subject><![CDATA[DYN3D]]></dc:subject>
<dc:subject><![CDATA[trigonal]]></dc:subject>
<dc:subject><![CDATA[hexagonal]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1519-2</identifier>
<datestamp>2025-01-15</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Hobert, H.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Hausmann, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1519-2</dc:identifier>
<dc:title><![CDATA[Raman investigation of lattice defects in the CoSi<SUB>2</SUB> synthesis using focused ion beam implantation]]></dc:title>
<dc:source><![CDATA[Microelectronic Engineering 50 (2000) 187-192]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[CoSi2 layers were produced by 70 keV Co focused ion implantation into (111)Si. Within a comparative study the CoSi2 layer quality and implantation damage were investigated as a function of pixel dwell-time and substrate temperature. Irradiation damage measurements were done by micro-Raman analysis. The results suggest that the dwell-time dependence of the CoSi2 layer formation - continuous layers for short and disrupted for long dwell-time - is caused by an adequate change from crystalline to amorphous silicon.  ]]></dc:description>
<dc:subject><![CDATA[Focused ion beam]]></dc:subject>
<dc:subject><![CDATA[Raman scattering]]></dc:subject>
<dc:subject><![CDATA[Ion implantation]]></dc:subject>
<dc:subject><![CDATA[Damage]]></dc:subject>
<dc:subject><![CDATA[CoSi2]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0167-9317(99)00281-6]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1519-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1519-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Hobert, H.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Hausmann, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1519-1</dc:identifier>
<dc:title><![CDATA[Raman investigation of lattice defects in the CoSi<SUB>2</SUB> synthesis using focused ion beam implantation]]></dc:title>
<dc:source><![CDATA[European Workshop Materials for Advanced Metallization, 8.-10. März, Ostende, Belgien]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[CoSi2 layers were produced by 70 keV Co focused ion implantation into (111)Si. Within a comparative study the CoSi2 layer quality and implantation damage were investigated as a function of pixel dwell-time and substrate temperature. Irradiation damage measurements were done by micro-Raman analysis. The results suggest that the dwell-time dependence of the CoSi2 layer formation - continuous layers for short and disrupted for long dwell-time - is caused by an adequate change from crystalline to amorphous silicon.  ]]></dc:description>
<dc:subject><![CDATA[Focused ion beam]]></dc:subject>
<dc:subject><![CDATA[Raman scattering]]></dc:subject>
<dc:subject><![CDATA[Ion implantation]]></dc:subject>
<dc:subject><![CDATA[Damage]]></dc:subject>
<dc:subject><![CDATA[CoSi2]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1519-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1520-1</identifier>
<datestamp>2025-01-15</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bonfada, E.]]></dc:creator>
<dc:creator><![CDATA[Maichle-Mößmer, C.]]></dc:creator>
<dc:creator><![CDATA[Strähle, J.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1520-1</dc:identifier>
<dc:title><![CDATA[Synthese, Charakterisierung und Struktur von Carbonyl- und Hydrido-Isocyanatokomplexen des Rutheniums]]></dc:title>
<dc:source><![CDATA[Zeitschrift für anorganische und allgemeine Chemie 1999, 625, 1327-1330]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[
Synthesis, Characterization and Structure of Carbonyl and Hydrido Isocyanato Complexes of Ruthenium 

Abstract. [Ru(CO)H(NCO)(PPh2Me)3] is formed during the reaction between [RuCl3(PPh2Me)3] and NaOCN in EtOH. The compound crystallizes in the monoclinic space group P21/n  (a=1256.4(4), b=1487.2(2), c=1993.5(5) pm, b=97.28(1)°, Z=4).  The distorted octahedral coordination sphere of RuII contains the phosphine ligands in meridional arrangement, their P atoms forming a plane together with the hydride ligand.
The reaction of [RuCl3(PPh3)2] with NaOCN in EtOH yields [Ru(NCO)-(CO)(CH3COO)-(PPh3)2] with trans coordinated Ph3P ligands. 
The formation of hydrido, carbonyl and acetato ligands are due to the reaction of the transition metal with the solvent ethanol.





]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1002/(SICI)1521-3749(199908)625:8<1327::AID-ZAAC1327>3.0.CO;2-Y]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1520-1</dc:relation>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1521-1</identifier>
<datestamp>2025-01-15</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Alberto, R.]]></dc:creator>
<dc:creator><![CDATA[Schibli, R.]]></dc:creator>
<dc:creator><![CDATA[Waibl, R.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Schubiger, P. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1521-1</dc:identifier>
<dc:title><![CDATA[Basic aqueous chemistry of [M(OH<sub>2</sub>)<SUB>3</SUB>(CO)<SUB>3</SUB>]<sup>+</sup>(M=Re,Tc) directed towards radiopharmaceutical application]]></dc:title>
<dc:source><![CDATA[Coord. Chem. Rev. 190-192 (1999) 901-919]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[
Abstract
	A review on the synthesis and properties of the organometallic aqua-ion [M(OH2)3(CO)3]+ (M = Re, 99Tc, 99mTc), as relevant for radiopharmaceutical application, is presented. These important starting compounds can be prepared quantitatively a) on the no carrier added level (99mTc) in water or b) in organic solvents (Re, 99Tc) at atmospheric pressure in a short time and from [MO4]-. The main characteristics of these carbonyl complexes are the high substitution stability of the three CO ligands and the substitution lability of the coordinated water molecules. [M(OH2)3(CO)3]+ can be considered as a "semi aquo-ion". On the macroscopic level, upon titration with OH-, hydroxo-bridged oligomers have been isolated  and characterized. The formation of hydroxo-bridged complexes is a consequence of the considerable Broenstedt acidity of [M(OH2)3(CO)3]+, whereas on the no carrier added level (n.c.a.) no such behavior was observed. Conditions and products of the water exchange by imidazole (im) and derivatives thereof (histamine, histidine) will be presented. The different mononuclear complexes with these ligands are of extraordinary inertness, which is the base for a potential application in biology and nuclear medicine. Finally, as a base for bioorganometallic chemistry, the adoption of the results from basic coordination chemistry to the labeling of biomolecules with an organometallic moiety will be exemplified with a selected penta-peptide and a recombinant single chain fragment. 
Keywords: Tc-carbonyls, Tc-peptide complexes, scFv, cancer diagnosis, radiopharmacy
]]></dc:description>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0010-8545(99)00128-9]]></dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:14433-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Giesecke, A.]]></dc:creator>
<dc:creator><![CDATA[Stefani, F.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14433-1</dc:identifier>
<dc:title><![CDATA[Electromagnetic induction in non-uniform domains]]></dc:title>
<dc:source><![CDATA[Workshop on Numerical Simulations of MHD flows, 18.-20.10.2010, Karlsruhe, Deutschland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Numerical simulations of the electromagnetic induction equation are carried out applying a grid based finite volume method where insulating boundaries are treated by the boundary element method. A prescribed flow of liquid sodium provides the energy source for self-generation of a magnetic field and the influences of non-uniform material properties on the induction process are examined by means of internal assemblies and outer container walls with high conductivity or high permeability.

High permeability material even if localized in a small volume like the flow driving impellers in the French VKS dynamo experiment, essentially determines the field generation process (decrease of the effective critical magnetic Reynolds number and enforcing of internal boundary conditions on material interfaces). Permeability caused facilitation of dynamo action might be important as well for the helical flow in cooling circuits of fast breeders. Preliminary simulations for a model flow in and around soft-iron sub-assemblies (that comprise the nuclear fuel pins) show a reduction of the critical magnetic Reynolds number for the onset of dynamo action by a factor of 2.

The third examined configuration is motivated by an application of the contactless inductive flow tomography (CIFT) in a continuous casting model experiment. Consideration of the finite conductivity of the copper container walls results in a quantitative modification of the current distribution within the solid material. An enhanced current yields an amplified induced magnetic field outside of the container which must be considered in the reconstruction of the fluid velocity field.]]></dc:description>
<dc:subject><![CDATA[Dynamo]]></dc:subject>
<dc:subject><![CDATA[Conductivity]]></dc:subject>
<dc:subject><![CDATA[Permeability]]></dc:subject>
<dc:subject><![CDATA[Induction]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:14493-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schulze, R.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14493-1</dc:identifier>
<dc:title><![CDATA[Progress Report: Cold quarks stars from hot lattice QCD]]></dc:title>
<dc:source><![CDATA[74. Jahrestagung der DPG und DPG Frühjahrstagung der Fachverbände, 15.-19.03.2010, Bonn, Germany]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Based on a quasiparticle model for �� stable and electrically neutral deconfined matter we address the mass-radius relation of pure quark stars. The model is adjusted to recent hot lattice QCD results for 2+1 flavors with almost physical quark masses [1].We find rather small radii and masses of equilibrium configurations composed of cold deconfined matter, well distinguished from neutron or hybrid stars.
[1] Bazavov et al., Phys. Rev. D 80 (2009) 014504.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:3185-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Borodkin, G.]]></dc:creator>
<dc:creator><![CDATA[Böhmer, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3185-1</dc:identifier>
<dc:title><![CDATA[Validation of 3D Synthesis RPV Neutron Fluence Calculations using VVER-1000 Ex-Vessel Reference Dosimetry Results (Invited Paper)]]></dc:title>
<dc:source><![CDATA[2000 ANS Annual Meeting, San Diego, California, June 4-8 2000, Trans. Am. Nucl. Soc., Vol.82,p.223-225 (2000)]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[3D synthesis based on detailed and improved calculations by SN-codes DORT, ANISN and the BUGLE-96 library has been validated using reference activation data from the Balakovo-3  ex-vessel dosimetry benchmark. The 3D spatial neutron source distribution including pin-to-pin power variations and the complex baffle construction were modeled in detail. All particulars of reactor operation such as coolant temperature changes, assembly power asymmetry and fuel burnup influence on space-energy neutron source distributions were taken into account. 
The discrepancies found do not exceed 10%. The average relation between calculated and measured valuse is 0,99. The calculated results show a systematic underestimation for 237Np(n,f) ( -6% on the average), 93Nb(n,n') ( -8%) and systematic overestimation for 58Ni(n,p) and 54Fe(n,p) ( +7%). Generally, the agreement between experiment and calculation is  even closer as expected from uncertainty considerations.
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:3185-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Borodkin, G.]]></dc:creator>
<dc:creator><![CDATA[Böhmer, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3185-7</dc:identifier>
<dc:title><![CDATA[Validation of 3D Synthesis RPV Neutron Fluence Calculations using VVER-1000 Ex-Vessel Reference Dosimetry Results (Invited Paper)]]></dc:title>
<dc:source><![CDATA[2000 ANS Annual Meeting, San Diego, California, June 4-8 2000, Trans. Am. Nucl. Soc., Vol.82,p.223-225 (2000)]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[3D synthesis based on detailed and improved calculations by SN-codes DORT, ANISN and the BUGLE-96 library has been validated using reference activation data from the Balakovo-3  ex-vessel dosimetry benchmark. The 3D spatial neutron source distribution including pin-to-pin power variations and the complex baffle construction were modeled in detail. All particulars of reactor operation such as coolant temperature changes, assembly power asymmetry and fuel burnup influence on space-energy neutron source distributions were taken into account. 
The discrepancies found do not exceed 10%. The average relation between calculated and measured valuse is 0,99. The calculated results show a systematic underestimation for 237Np(n,f) ( -6% on the average), 93Nb(n,n') ( -8%) and systematic overestimation for 58Ni(n,p) and 54Fe(n,p) ( +7%). Generally, the agreement between experiment and calculation is  even closer as expected from uncertainty considerations.
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1523-1</identifier>
<datestamp>2025-01-15</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Preusche, S.]]></dc:creator>
<dc:creator><![CDATA[Füchtner, F.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Zessin, J.]]></dc:creator>
<dc:creator><![CDATA[Krug, H.]]></dc:creator>
<dc:creator><![CDATA[Neumann, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1523-1</dc:identifier>
<dc:title><![CDATA[Long-distance transport of radionuclides between PET cyclotron and PET radiochemistry]]></dc:title>
<dc:source><![CDATA[Appl. Rad. Isot. 51 (1999) 625-630]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The Rossendorf PET Center has a special feature: its PET cyclotron and the radiochemical laboratories are 500 metres away from each other. The distance is bridged by our radionuclide transport system (RATS).
Details of RATS such as layout, technical parameters, control system, radiation protection and our experience in long-distance transport of radionuclides, are indicated below.
]]></dc:description>
<dc:subject><![CDATA[RATS]]></dc:subject>
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<dc:creator><![CDATA[Lopez Jimenez, J.]]></dc:creator>
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<dc:title><![CDATA[BWR Physics and Thermohydraulics Complementary Actions to the BWR R & D Cluster]]></dc:title>
<dc:source><![CDATA[Proceedings of the FISA-97 Symposium on EU Research on Severe Accidents Luxembourg, 17 to 19 November, 1997]]></dc:source>
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<dc:description><![CDATA[An overview is given on the EU-IPSS-BWR R&D Cluster project "BWR-Physics and Thermohydraulics Complementary Actions". Six institutes/companies from 5 countries are working on three main topics:
- Design of innovative components (thermal valves, emergency condensers, isolation condensers and building condensers)
- Enlarged assesment of the performances of the innovative components
- Understanding of the physical phenomena which determine the dynamical behaviour of BWRs.
Selected results of the different topics are presented.

]]></dc:description>
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<dc:title><![CDATA[BWR Physics and Thermohydraulics Complementary Actions to the BWR R & D Cluster]]></dc:title>
<dc:source><![CDATA[Proceedings of the FISA-97 Symposium on EU Research on Severe Accidents Luxembourg, 17 to 19 November, 1997]]></dc:source>
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<dc:description><![CDATA[An overview is given on the EU-IPSS-BWR R&D Cluster project "BWR-Physics and Thermohydraulics Complementary Actions". Six institutes/companies from 5 countries are working on three main topics:
- Design of innovative components (thermal valves, emergency condensers, isolation condensers and building condensers)
- Enlarged assesment of the performances of the innovative components
- Understanding of the physical phenomena which determine the dynamical behaviour of BWRs.
Selected results of the different topics are presented.

]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Dudlik, A.]]></dc:creator>
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<dc:title><![CDATA[Transiente Strömungsvorgänge in Rohrleitungen, Visualisierung und Berechnung von Kavitationen in Rohrleitungssystemen hinter schnellschließenden Regelklappen]]></dc:title>
<dc:source><![CDATA[Workshop "Meßtechnik für stationäre und transiente Mehrphasenströmungen", Rossendorf 6.-7. November 1997]]></dc:source>
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<dc:creator><![CDATA[Dudlik, A.]]></dc:creator>
<dc:creator><![CDATA[Schlüter, S.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1613-1</dc:identifier>
<dc:title><![CDATA[Transiente Strömungsvorgänge in Rohrleitungen, Visualisierung und Berechnung von Kavitationen in Rohrleitungssystemen hinter schnellschließenden Regelklappen]]></dc:title>
<dc:source><![CDATA[Workshop "Meßtechnik für stationäre und transiente Mehrphasenströmungen", Rossendorf, 06.-07. November 1997, Forschungszentrum Rossendorf; FZR-204, S. 39 - 50]]></dc:source>
<dc:date>1997</dc:date>
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<identifier>HZDR:PUBLDB:1614-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Gehrke, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1614-1</dc:identifier>
<dc:title><![CDATA[ASAXS-Investigations of the Influence of the Irradiation Temperature on the Formation of Defects in Nuclear Pressure Vessel Steel A-533-B1]]></dc:title>
<dc:source><![CDATA[Hamburger Synchrotronstrahlunslabor HASYLAB, Jahresbericht 1996, Hamburg, 1997, S. 255]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1615-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Hadek, J.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1615-1</dc:identifier>
<dc:title><![CDATA[Neutron Flux Reconstruction ina Hexagonal Cassete - Theory and Implementation into the Code DYN3D/H1.1]]></dc:title>
<dc:source><![CDATA[Nucleon No. 3, (1997), pp. 8 - 14]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The reconstruction of neutron flux density and thermal power density inside the hexagonal cassette of VVER type is described. The method of successive smooting combined with following analytical solution was used for the detailed pointwise evaluation of neutron fluxes and thermal power densities distributions in the cassette interior. The program module RECON based on the above mentioned method is presented. Results generated by the 3-dimensional reactor dynamic code DYN3D are used as input data for this subprogram. RECON can be used for methodical off-line investigation or to be implemented into the code DYN3D. This implementation is demonstrated.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<identifier>HZDR:PUBLDB:1621-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kolevzon, V.]]></dc:creator>
<dc:creator><![CDATA[Pozniakov, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1621-1</dc:identifier>
<dc:title><![CDATA[Temperature.dependent behaviour of capillary waves at Hg-vapour and Hg-HgO interfaces]]></dc:title>
<dc:source><![CDATA[Journal of Physics: Condensed Matter, Vol. 9, 1997, pp. 6815 - 6826]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<identifier>HZDR:PUBLDB:1622-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kolevzon, V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1622-1</dc:identifier>
<dc:title><![CDATA[Relaxations of temperature and charges at a liquid metal surface]]></dc:title>
<dc:source><![CDATA[Physics Letters A 230, 1997, pp. 358 - 362]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<identifier>HZDR:PUBLDB:1627-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Priede, J.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1627-1</dc:identifier>
<dc:title><![CDATA[Hydrothermal wave instability of the thermocapillary driven convection in a coplanar magnetic field]]></dc:title>
<dc:source><![CDATA[Journal of Fluid Mechanics, Vol. 347, 1997, pp.141 - 169]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/contributionToPeriodical</dc:type>
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<identifier>HZDR:PUBLDB:14513-2</identifier>
<datestamp>2025-06-05</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14513-2</dc:identifier>
<dc:title><![CDATA[The Master Curve approach an approved fracture mechanics test method for more than one decade]]></dc:title>
<dc:source><![CDATA[COMAT 2010 RECENT TRENDS IN STRUCTURAL MATERIALS, 25.-26.11.2010, Plzen, Czech Republic<br>Proceedings of COMAT 2010 Recent Trends in Structural Materials, Plzen: COMTES FHT a.s.]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The paper gives an overview about the development of the Master Curve approach since the first version of the appropriate test standard ASTM E1921 was issued. The main focus is on the application of ASTM E1921 for the determination of fracture toughness values applied in the nuclear reactor pressure vessel integrity assessment. Test parameters influencing the reference temperature were assessed.]]></dc:description>
<dc:subject><![CDATA[fracture toughness]]></dc:subject>
<dc:subject><![CDATA[ductile-to-brittle transition]]></dc:subject>
<dc:subject><![CDATA[reactor pressure vessel steel]]></dc:subject>
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<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14513-1</dc:identifier>
<dc:title><![CDATA[The Master Curve approach an approved fracture mechanics test method for more than one decade]]></dc:title>
<dc:source><![CDATA[COMAT 2010 RECENT TRENDS IN STRUCTURAL MATERIALS, 25.-26.11.2010, Plzen, Czech Republic]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The paper gives an overview about the development of the Master Curve approach since the first version of the appropriate test standard ASTM E1921 was issued. The main focus is on the application of ASTM E1921 for the determination of fracture toughness values applied in the nuclear reactor pressure vessel integrity assessment. Test parameters influencing the reference temperature were assessed.]]></dc:description>
<dc:subject><![CDATA[fracture toughness]]></dc:subject>
<dc:subject><![CDATA[ductile-to-brittle transition]]></dc:subject>
<dc:subject><![CDATA[reactor pressure vessel steel]]></dc:subject>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
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<dc:language>eng</dc:language>
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<header>
<identifier>HZDR:PUBLDB:14517-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Plevachuk, Y.]]></dc:creator>
<dc:creator><![CDATA[Sklyarchuk, V.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Novakovic, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14517-1</dc:identifier>
<dc:title><![CDATA[Surface tension and density of liquid Bi-Pb, Bi-Sn and Bi-Pb-Sn eutectic alloys]]></dc:title>
<dc:source><![CDATA[Surface Science 605(2011), 1034-1042]]></dc:source>
<dc:date>2011</dc:date>
<dc:description><![CDATA[Surface tension and density measurements of liquid Bi-Pb, Bi-Sn and Bi-Pb-Sn eutectic alloys were carried out by the large drop method in the temperature range 350 - 750 K. The regular solution model is used in conjunction with Butler's equation to calculate the surface tension of binary and ternary alloys of the Bi-Pb-Sn system, while the surface tension of ternary alloys is also predicted by geometric models. The new experimental results were compared with the calculated values of the surface tension as well as with the data available in literature.]]></dc:description>
<dc:subject><![CDATA[surface tension]]></dc:subject>
<dc:subject><![CDATA[density eutectic alloys]]></dc:subject>
<dc:subject><![CDATA[large drop method]]></dc:subject>
<dc:subject><![CDATA[bismuth]]></dc:subject>
<dc:subject><![CDATA[lead]]></dc:subject>
<dc:subject><![CDATA[tin]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:21-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Maroti, L.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Windberg, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-21-1</dc:identifier>
<dc:title><![CDATA[Investigation of two-phase flow phenomena at integral test facilities using needle conductivity probes]]></dc:title>
<dc:source><![CDATA[8th International Conference on Thermal Engineering and Thermogrammetry, Budapest, 2.-4.6.1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The paper deals with the utilization of needle shaped conductivity probes developed in Rossendorf during a small break LOCA experiment at the Budapest PMK test facility. A 1-%-break at the down-comer inlet was simulated, the ECC tanks were switched off. The probes worked properly under primary circuit conditions (12.3 MPa, 300 °C), the data acquision system provided clearly readable data in spite of the high electrical disturbance level caused by the directly heated fuel rod simulators of PMK. The paper presents plots of the signals of the probes. The level drop in the upper plenum of the reactor, the hot leg loop-seal clearing and the emptying of the steam generator cold collector were indicated. Closely after the loop-seal clearing void fraction oscillations with a period of about 22-24 sec were observed at the reactor outlet and the steam generator inlet.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:21-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Maroti, L.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Windberg, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-21-2</dc:identifier>
<dc:title><![CDATA[Investigation of two-phase flow phenomena at integral test facilities using needle conductivity probes]]></dc:title>
<dc:source><![CDATA[8th International Conference on Thermal Engineering and Thermogrammetry, Budapest, 2.-4.6.1993, p. 275 - 280]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The paper deals with the utilization of needle shaped conductivity probes developed in Rossendorf during a small break LOCA experiment at the Budapest PMK test facility. A 1-%-break at the down-comer inlet was simulated, the ECC tanks were switched off. The probes worked properly under primary circuit conditions (12.3 MPa, 300 °C), the data acquision system provided clearly readable data in spite of the high electrical disturbance level caused by the directly heated fuel rod simulators of PMK. The paper presents plots of the signals of the probes. The level drop in the upper plenum of the reactor, the hot leg loop-seal clearing and the emptying of the steam generator cold collector were indicated. Closely after the loop-seal clearing void fraction oscillations with a period of about 22-24 sec were observed at the reactor outlet and the steam generator inlet.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-21-2</dc:relation>
<dc:audience>Researchers</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:9-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-9-1</dc:identifier>
<dc:title><![CDATA[Projektvorbereitung und -abwicklung des Bund-Länder-1000-Dächer-Photovoltaik-Programms]]></dc:title>
<dc:source><![CDATA[BMFT-Statusbericht Photovoltaik / BMFT-Statusseminar 27.-29.4.1993 in Bad Breisig, Tagungsband S.66]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The report summarizes the present state of the 1000-Roof-Photovoltaic-Programme (sponsered by the BMFT and the Federal States) in the five new German Federal states. After some starting problems the programme is well accepted also in East Germany now, especially in Brandenburg, Saxony and Thuringia. Statistical data are given on the siutation in the single states. 
Some operation results are discussed in more detail. A final yield of 2 kWh/kWp.a seems to be possible, at least in the region of Saxony. The share of the direct used solar energy by the plant owner strongly depends on the individual energy consumption and on the season. During the winter only a share of 10 % is realistic, but in summer the value can reach 50 % or more. The average performance ratio of several systems is estimated to 68 %.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-9-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:9-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-9-7</dc:identifier>
<dc:title><![CDATA[Projektvorbereitung und -abwicklung des Bund-Länder-1000-Dächer-Photovoltaik-Programms]]></dc:title>
<dc:source><![CDATA[BMFT-Statusbericht Photovoltaik / BMFT-Statusseminar 27.-29.4.1993 in Bad Breisig, Tagungsband S.66]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The report summarizes the present state of the 1000-Roof-Photovoltaic-Programme (sponsered by the BMFT and the Federal States) in the five new German Federal states. After some starting problems the programme is well accepted also in East Germany now, especially in Brandenburg, Saxony and Thuringia. Statistical data are given on the siutation in the single states. 
Some operation results are discussed in more detail. A final yield of 2 kWh/kWp.a seems to be possible, at least in the region of Saxony. The share of the direct used solar energy by the plant owner strongly depends on the individual energy consumption and on the season. During the winter only a share of 10 % is realistic, but in summer the value can reach 50 % or more. The average performance ratio of several systems is estimated to 68 %.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-9-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1877-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1877-1</dc:identifier>
<dc:title><![CDATA[Nachbestrahlungsuntersuchungen zum Bestrahlungsprogramm Rheinsberg]]></dc:title>
<dc:source><![CDATA[4. Seminar zur wissenschaftlich-technischen Zusammenarbeit zwischen der Russischen Föderation und der Bundesrepublik Deutschland zum Thema: "Komponentensicherheit und Qualitässicherung (WWER)", St ...]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The irradiation programme Rheinsberg serves to investigate the neutron embrittlement of VVER type reactor pressure vessel steel. Within this programme Charpy-V (partly with fatigue crack and side grooved), CT- and tensile specimes of 24 different heats from VVER 440 type and VVER 1000 type reactor pressure vessel steel (basic or weld material) were irradiated in the high flux channels of the  VVER-2 Rheinsberg from 1984 - 88.  The testing and evaluation of the irradiated specimen will be done within the framework of bilateral scientific-technical cooperation between Russia and Germany. The report gives a systematic review of all material data existing for the unirradiated initial state. Results of Charpy- V-impact tests and quasistatic 3-point-bending tests are discussed in detail.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1877-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1880-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Enkelmann, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1880-1</dc:identifier>
<dc:title><![CDATA[Promotion of Renewing of District Heating Systems in Saxonia]]></dc:title>
<dc:source><![CDATA[Energieanwendung und Energietechnik 42 (1993) 5, S. 276]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[In 1992 in the new Federal States of Germany the renewing of district heating plants was supported by the gouvernment. Plants for heat generation, and heat transport and distribution and customer installations were included in the renewing. In Saxonia an amount of approximately 80 million DM could be devided among the applicants. With regard to the enormous uncovered demand the gouvernment decided to continue the program from 1993 up to 1995. Based on the experiences with the 1992 promotion program some hints can be given to the user of the new program.]]></dc:description>
<dc:type>info:eu-repo/semantics/contributionToPeriodical</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:contributionToPeriodical</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1880-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1631-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1631-1</dc:identifier>
<dc:title><![CDATA[Zur Physik und Sicherheit von WWER-Reaktoren]]></dc:title>
<dc:source><![CDATA[Atomwirtschaft-Atomtechnik 42 (1997) 792]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[A brief information about the 7th Symposium of Atomic Energy Research held in
Hoernitz near Zittau (Germany) in September 23-26, 1997, is given. Atomic 
Energy Research (AER) is an internatiol association of 23 nuclear power plants,
organisations for scientific-technical support of nuclear authorities and
research institutions from 8 countries on the physics and nuclear safety of
Russian VVER type reactors. At the symposium, about 70 papers were contributed
in sessions on neutron transport methods, core design and reactor operation,
core monitoring, reactor dynamics and reactor safety, waste management and
criticality safety, thermo- and fluid-dynamics.]]></dc:description>
<dc:type>info:eu-repo/semantics/contributionToPeriodical</dc:type>
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<dc:language>ger</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1634-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schurig, C.]]></dc:creator>
<dc:creator><![CDATA[Fiedler, U.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1634-1</dc:identifier>
<dc:title><![CDATA[Nondestructive Characterization of Rector Pressure Vessel Materials Using Neural Networks]]></dc:title>
<dc:source><![CDATA[Proc. of EUROMAT '97, Maastricht, April 1997, p. 347]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1634-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1634-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schurig, C.]]></dc:creator>
<dc:creator><![CDATA[Fiedler, U.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1634-7</dc:identifier>
<dc:title><![CDATA[Nondestructive Characterization of Rector Pressure Vessel Materials Using Neural Networks]]></dc:title>
<dc:source><![CDATA[Proc. of EUROMAT '97, Maastricht, April 1997, p. 347]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:bookPart</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:creator><![CDATA[Markwitz, M.]]></dc:creator>
<dc:creator><![CDATA[Strobel, M.]]></dc:creator>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
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<dc:title><![CDATA[Formation of d-layers of Ge nanocrystals in SiO2]]></dc:title>
<dc:source><![CDATA[E-MRS Spring Meeting, Symposium 1 - Microcrystalline and Nanocrystalline Semiconductors, Strasbourg, France, June 1-4, 1999]]></dc:source>
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<dc:creator><![CDATA[Ferse, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1654-1</dc:identifier>
<dc:title><![CDATA[Erweiterung des GEFA-Wissenserwerbes für Rüstungsaltlasten]]></dc:title>
<dc:source><![CDATA[Seminar der Rüstungsaltlastenvertreter der neuen Bundesländer, Umweltbundesamt Berlin, Januar 1997]]></dc:source>
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<dc:title><![CDATA[Die Anwendung wissensbasierter Methoden bei der Bewertung von Altlasten XPS'97]]></dc:title>
<dc:source><![CDATA[4. Deutsche Jahrestagung Wissensbasierter Systeme, Bad Honnef, März 1997]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Ferse, W.]]></dc:creator>
<dc:creator><![CDATA[Geiger, W.]]></dc:creator>
<dc:creator><![CDATA[Reißfelder, M.]]></dc:creator>
<dc:creator><![CDATA[Reitz, T.]]></dc:creator>
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<dc:creator><![CDATA[Weidemann, R.]]></dc:creator>
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<dc:title><![CDATA[Das wissensbasierte System XUMA-GEFA für Altlasten: Vom Prototyp zum Produktionssystem]]></dc:title>
<dc:source><![CDATA[11. Internationales Symposium der Gesellschaft für Informatik, Straßburg, 10. - 12. September 1997]]></dc:source>
<dc:date>1997</dc:date>
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<identifier>HZDR:PUBLDB:3097-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Grahn, A.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
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<dc:title><![CDATA[Dissipative Strukturbildung bei exothermen Grenzflächenreaktionen]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-307 Dezember 2000]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Der Bericht beschäftigt sich mit spontaner Grenzflächenkonvektion und -turbulenz beim Stoff- und Wärmeübergang an fluiden Phasengrenzen zwischen zwei nicht mischbaren Phasen. Solche Effekte sind von großer industrieller Bedeutung, da die erzielten Stoffübergangsraten um ein Vielfaches über den bei gewöhnlicher Diffusion auftretenden liegen. Zwei unterschiedliche Mechanismen sind der Motor für die Instabilitäten: Marangoni-Instabilität: Die Grenzflächenspannung ist eine Funktion der Temperatur und der Grenzflächenkonzentration des ausgetauschten Stoffes. Schwankungen der Temperatur und der Konzentration entlang der Phasengrenze führen folglich zu Grenzflächenspannungsgradienten. Grenzflächenspannungsgetriebene Instabilitäten äußern sich durch rollenförmige oder polygonale Konvektionszellen, Eruptionen oder Turbulenz an der Phasengrenze. Schwerkraftgetriebene Instabilität: Die Dichte ist ebenfalls eine Funktion der Temperatur und der Konzentration des gelösten Stoffes. Der Transport eines Stoffes über eine fluide Phasengrenze verändert die Zusammensetzung und die Dichte der angrenzenden Flüssigkeitsschichten, sodass instabile Dichteschichtungen auftreten können. Temperaturgradienten entstehen dabei durch Freisetzung von Reaktions- und/oder Lösungsenthalpie. Auftriebsbewegungen haben die Form von Thermiken (engl. plumes, thermals). Die Phänomene der Grenzflächenkonvektion werden in einer vertikalen Kapillarspaltgeometrie untersucht. Neben Stoffsystemen mit reaktivem Stoffübergang (Neutralisation von Karbonsäuren, Hydrolyse und Veresterung von Alkanoylhloriden) kamen auch solche mit reaktionsfreiem Stoffübergang (Karbonsäuren, Tensid) zur Anwendung. Die instabile Dichteschichtung, die durch den Konzentrationsgradienten infolge der Stoffdiffusion erzeugt wird, führt zu Auftriebskonvektion in Form von Thermiken. Die Anwesenheit einer exothermen Reaktion bewirkt eine Vergrößerung des Längenwachstums der Thermiken in der oberen Phase durch Aufprägung eines zusätzlich destabilisierenden Temperaturgradienten. In der unteren Phase kommt es dagegen zum Entstehen des doppeldiffusiven Fingerregimes bei Überlagerung des destabilisierenden Konzentrationsgradienten durch den stabilisierenden Temperaturgradienten. Beim Übergang eines Tensids konnten die für diese Stoffklasse charakteristischen Rollzellen, die durch Grenzflächenspannungsgradienten angetrieben werden, beobachtet werden. Diese Konvektionsstrukturen bleiben auf einen schmalen Bereich ober- und unterhalb der Phasengrenze beschränkt. 
Die Transportgleichungen für Impuls, Stoff und Wärme wurden in ihrer 2-dimensionalen Form in einen Rechenkode umgesetzt und der Übergang einer einzelnen Komponente simuliert. Die hydrodynamischen Bedingungen an der Phasengrenze wurden so formuliert, dass lokale Änderungen der Zusammensetzung und der Temperatur zu Grenzflächenspannungsgradienten führen und die Phasengrenze damit dem Marangonieffekt unterliegt. Die Stoffeigenschaften wurden mit Ausnahme der Dichte im Volumenkraftterm der Impulsgleichung als konstant angenommen, sodass dichtegetriebene Konvektionen simuliert werden können. Die verschiedenen Konvektionsformen werden durch die Simulation qualitativ gut wiedergegeben. Bei Marangonikonvektion kommt es zu einer Verschiebung des steilen Konzentrationsgradienten von der Phasengrenze in die Kerne der Phasen, was zum schnellen Absterben der Marangonikonvektion führt. Die Wiedergabe des Längenwachstums der Thermiken durch Simulation eines realen Stoffsystems ist zufriedenstellend. Ebenso gibt die Simulation eine realistische Abschätzung zu erwartender Stoffströme bei Anwesenheit hydrodynamischer Instabilitäten. Größere Abweichungen zwischen Simulation und Experiment sind jedoch bei der horizontalen Größenskala der Fingerstruktur festzustellen, die wahrscheinlich auf die Boussinesq-Approximation zurückzuführen sind.
]]></dc:description>
<dc:subject><![CDATA[Marangoni instability]]></dc:subject>
<dc:subject><![CDATA[Rayleigh-Bénard convection]]></dc:subject>
<dc:subject><![CDATA[mass transfer]]></dc:subject>
<dc:subject><![CDATA[fluid-fluid interface]]></dc:subject>
<dc:subject><![CDATA[numerical simulation]]></dc:subject>
<dc:subject><![CDATA[capillary gap experiments]]></dc:subject>
<dc:subject><![CDATA[chemical reaction]]></dc:subject>
<dc:subject><![CDATA[interfacial chemical reaction]]></dc:subject>
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<identifier>HZDR:PUBLDB:161-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
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<dc:creator><![CDATA[Thibault, J.-P.]]></dc:creator>
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<dc:title><![CDATA[Influence of external magnetic fields on slip ratio in LMMHD two-phase flow]]></dc:title>
<dc:source><![CDATA["Energy Transfer in MHD Flows", Sept. 1994, Aussois, Frankreich, pp. 607 - 616]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[LMMHD two-phase flow modelling strongly depends on the accuracy of the constitutive equations and the corresponding closure laws. Several questions rise from various attempts to model these flows. They are mainly connected with the modification of two-phase flow (interfacial dragging, wall friction, apparent elec- trical conductivity, etc.) due to the electromagnetic forces.
The present paper presents a comprehensive survey of the LMMHD two-phase investigations performed in our two laboratories using different liquid systems, mercury-air (LEGI-IMG) and sodium-argon (FZR), with quite different properties. The remarkable difference in the material properties allow us to reach a wide range of nondimensional parameters.
For theoretical predictions a two fluid model (LEGI-IMG) and a bubbly flow model (FZR) have been developed in order to meet the requirements of the corresponding facilities.
The experiments have been realized in rectangular vertical test sections immersed into a transverse magnetic field. The gas is injected in the entrance region of the magnetic field. The distribution of the local void fraction across the channel cross section was measured by means of single wire resistivity probes. The electrical boundary conditions of the test sections are rather different. While the FZR test section consists of a simple stainless steel channel (thickness of the walls: 5 mm), the LEGI-IMG configuration, which includes segmented copper electrodes and an external load resistance, is more similar to a MHD generator. In the FZR experiment a volumetric quality in the range of 0.06 - 0.09 leads to a pure bubbly flow regime. In contrast to this the LEGI-IMG facility usually work with considerable higher gas flow rates.
We present experimental results showing the dependence of the mean values of the void fraction, the slip ratio and the gas velocity on the magnetic field strength as well as on the mean sodium velocity. These results will be compared with the theoreti ...]]></dc:description>
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<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Mihalache, G.]]></dc:creator>
<dc:creator><![CDATA[Thibault, J.-P.]]></dc:creator>
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<dc:title><![CDATA[Influence of external magnetic fields on slip ratio in LMMHD two-phase flow]]></dc:title>
<dc:source><![CDATA["Energy Transfer in MHD Flows", Sept. 1994, Aussois, Frankreich, pp. 607 - 616]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[LMMHD two-phase flow modelling strongly depends on the accuracy of the constitutive equations and the corresponding closure laws. Several questions rise from various attempts to model these flows. They are mainly connected with the modification of two-phase flow (interfacial dragging, wall friction, apparent elec- trical conductivity, etc.) due to the electromagnetic forces.
The present paper presents a comprehensive survey of the LMMHD two-phase investigations performed in our two laboratories using different liquid systems, mercury-air (LEGI-IMG) and sodium-argon (FZR), with quite different properties. The remarkable difference in the material properties allow us to reach a wide range of nondimensional parameters.
For theoretical predictions a two fluid model (LEGI-IMG) and a bubbly flow model (FZR) have been developed in order to meet the requirements of the corresponding facilities.
The experiments have been realized in rectangular vertical test sections immersed into a transverse magnetic field. The gas is injected in the entrance region of the magnetic field. The distribution of the local void fraction across the channel cross section was measured by means of single wire resistivity probes. The electrical boundary conditions of the test sections are rather different. While the FZR test section consists of a simple stainless steel channel (thickness of the walls: 5 mm), the LEGI-IMG configuration, which includes segmented copper electrodes and an external load resistance, is more similar to a MHD generator. In the FZR experiment a volumetric quality in the range of 0.06 - 0.09 leads to a pure bubbly flow regime. In contrast to this the LEGI-IMG facility usually work with considerable higher gas flow rates.
We present experimental results showing the dependence of the mean values of the void fraction, the slip ratio and the gas velocity on the magnetic field strength as well as on the mean sodium velocity. These results will be compared with the theoreti ...]]></dc:description>
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<identifier>HZDR:PUBLDB:179-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Futterschneider, H.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Morgenstern, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-179-1</dc:identifier>
<dc:title><![CDATA[Solar betriebene netzunabhängige Meßstation - Energiebilanzen eines einjährigen Betriebes]]></dc:title>
<dc:source><![CDATA[9. Internationales Sonnenforum, Stuttgart, 28.6.-1.7.1994, Tagungsbaricht S. 1243 - 1250]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Für die dosimetrische Umgebungsüberwachung des Forschungsstandortes Rossendorf wurden zwei solar betriebene netzunabhängige Meßsysteme konzipiert und in einem einjährigen Meßzyklus erprobt. Eine wesentliche Forderung bestand in der Gewährleistung einer 100%igen Versorgungssicherheit der Meßsonden.
Die energetisch relevanten Ergebnisse dieser Langzeiterprobung werden diskutiert. Zur Analyse der Energiebilanzen wurden die 10-Minuten-Mittelwerte von Mudolstrom ,und -spannung, Batteriestrom und -spannung, der jeweilige Laststrom und die solare Einstrahlung gemessen. Beide Systeme liefen auch im sehr einstrah- lungsarmen Winter 1993/94 ohne Ausfall. Die vollständige Jahresbilanz des Systems 1 ergab einen reinen Solarbetrieb während 3022 h, einen Batteriebetrieb während 4686 h und in der restlichen Zeit einen Mischbetrieb.
Die gewählte Dimensionierung der beiden photovoltaischen Energieversorgungssysteme erwies sich als ausreichend für einen sicheren Betrieb, die der Auslegung zugrunde liegenden Parameter (spezifische Modulgröße 33 - 41 Wp/W, spezifische Batteriegröße 33 d) können für Systeme mit beliebig großen Lasten verallgemeinert werden.]]></dc:description>
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<dc:creator><![CDATA[Futterschneider, H.]]></dc:creator>
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<dc:creator><![CDATA[Morgenstern, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-179-7</dc:identifier>
<dc:title><![CDATA[Solar betriebene netzunabhängige Meßstation - Energiebilanzen eines einjährigen Betriebes]]></dc:title>
<dc:source><![CDATA[9. Internationales Sonnenforum, Stuttgart, 28.6.-1.7.1994, Tagungsbaricht S. 1243 - 1250]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Für die dosimetrische Umgebungsüberwachung des Forschungsstandortes Rossendorf wurden zwei solar betriebene netzunabhängige Meßsysteme konzipiert und in einem einjährigen Meßzyklus erprobt. Eine wesentliche Forderung bestand in der Gewährleistung einer 100%igen Versorgungssicherheit der Meßsonden.
Die energetisch relevanten Ergebnisse dieser Langzeiterprobung werden diskutiert. Zur Analyse der Energiebilanzen wurden die 10-Minuten-Mittelwerte von Mudolstrom ,und -spannung, Batteriestrom und -spannung, der jeweilige Laststrom und die solare Einstrahlung gemessen. Beide Systeme liefen auch im sehr einstrah- lungsarmen Winter 1993/94 ohne Ausfall. Die vollständige Jahresbilanz des Systems 1 ergab einen reinen Solarbetrieb während 3022 h, einen Batteriebetrieb während 4686 h und in der restlichen Zeit einen Mischbetrieb.
Die gewählte Dimensionierung der beiden photovoltaischen Energieversorgungssysteme erwies sich als ausreichend für einen sicheren Betrieb, die der Auslegung zugrunde liegenden Parameter (spezifische Modulgröße 33 - 41 Wp/W, spezifische Batteriegröße 33 d) können für Systeme mit beliebig großen Lasten verallgemeinert werden.]]></dc:description>
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<dc:creator><![CDATA[Galindo, V.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
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<dc:creator><![CDATA[Treuner, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-159-2</dc:identifier>
<dc:title><![CDATA[Unsteady Thermocapillary Drop Migration in a Uniform Temperature Gradient]]></dc:title>
<dc:source><![CDATA[Proc. "Drop Tower Days 94", Bremen, Juli 1994, pp. 90 - 94]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[A theoretical analysis of liquid drop unsteady migration under microgravity conditions is presented, if an interfracial tension gradient is generated on the drop surface by a uniform temperature gradient in the surrounding liquid. The effect of buoyancy due to a residual gravity vector aligned parallel to the temperature gradient is included. The relevant equations are solved in the creeping flow limit where in the convective transport of momentum as well as that of the energy is neglected, i.e. at low Reynolds and Marangoni numbers. The flow and the temperature field within and around the drop are obtained after transforming the results from the Laplace transform domain, in which they are derived, to the time domain. The time transient behaviour of the Migration speed depends strongly on the choice of the initial flow and temperature fields. The comparison with other initial conditions from the literature is performed.]]></dc:description>
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<dc:title><![CDATA[Unsteady Thermocapillary Drop Migration in a Uniform Temperature Gradient]]></dc:title>
<dc:source><![CDATA["Drop Tower Days 94", Bremen, Juli 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[A theoretical analysis of liquid drop unsteady migration under microgravity conditions is presented, if an interfracial tension gradient is generated on the drop surface by a uniform temperature gradient in the surrounding liquid. The effect of buoyancy due to a residual gravity vector aligned parallel to the temperature gradient is included. The relevant equations are solved in the creeping flow limit where in the convective transport of momentum as well as that of the energy is neglected, i.e. at low Reynolds and Marangoni numbers. The flow and the temperature field within and around the drop are obtained after transforming the results from the Laplace transform domain, in which they are derived, to the time domain. The time transient behaviour of the Migration speed depends strongly on the choice of the initial flow and temperature fields. The comparison with other initial conditions from the literature is performed.]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:identifier>https://www.hzdr.de/publications/Publ-1839-1</dc:identifier>
<dc:title><![CDATA[LMMHD Activities at Reearch Center Rossendorf]]></dc:title>
<dc:source><![CDATA[Kawasaki, Japan: Nippon Steel Corp., 31. 10. 1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[A review on R&D activities of the FZR group in the field of Liquid Metal MHD is given in this lecture. Particular emphasis is put on the measurements and theoretical results with respect to heat&mass transfer in anisotropic MHD turbelence. Corresponding models, experimental set-ups, and measuring techniques are described. Two-phase flow measurements are presented obtained at the FZR sodium facility. The prospects of cylindrical turbulence  promoters are discussed.]]></dc:description>
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<identifier>HZDR:PUBLDB:1839-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1839-2</dc:identifier>
<dc:title><![CDATA[LMMHD Activities at Reearch Center Rossendorf]]></dc:title>
<dc:source><![CDATA[Tokyo, Japan: Tokyo Institute of Technology, 31. 10.1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[A review on R&D activities of the FZR group in the field of Liquid Metal MHD is given in this lecture. Particular emphasis is put on the measurements and theoretical results with respect to heat&mass transfer in anisotropic MHD turbelence. Corresponding models, experimental set-ups, and measuring techniques are described. Two-phase flow measurements are presented obtained at the FZR sodium facility. The prospects of cylindrical turbulence  promoters are discussed.]]></dc:description>
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<identifier>HZDR:PUBLDB:1840-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1840-1</dc:identifier>
<dc:title><![CDATA[MHD Research at Research Center Rossenorf - Relations to LMFBR]]></dc:title>
<dc:source><![CDATA[O-arai, Japan: O-arai Engineering Center, PNC, 02.11.1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[A review on R&D activities of the FZR group in the field of Liquid Metal MHD is given in this lecture. Special attention is paid to sodium related experiences (facility, experimental programme, measuring techniques) being of interest for the Breeder development. In particular, first tests of a contactless gas phase detection system are presented. This system was developed by RWTH Aachen and FZR, and tested for the first time at FZR. It allows a detection of small, even single gas bubbles independent of their acoustic activity.]]></dc:description>
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<identifier>HZDR:PUBLDB:245-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Galindo, V.]]></dc:creator>
<dc:creator><![CDATA[Treuner, M.]]></dc:creator>
<dc:creator><![CDATA[Langbein, D.]]></dc:creator>
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<dc:title><![CDATA[Thermocapillary Bubble Migration at Higher Marangoni numbers - Theory and Experiment]]></dc:title>
<dc:source><![CDATA[Bulltin of the American Physical Society, Series II, 39 (1994), 9, p. 1841]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Single bubble motion driven purely by thermocapillarity (i.e. a linear temperature gradient in the surrounding liquid) is analyzed theoretically with the following steps: A full numerical simulation up to Re of several hundreds depending on the Prandtl-number of the liquid, and a simple analytical treatment describing the asymptotic migration at high Re. Results of short-term microgravity experiments performed at drop Tower Bremen will be reported for 20 < Re < 160. The theoretical migration velocities are slightly higher than the experimental values which might be due to the short-time nature of the experiments. An unsteady theoretical analysis will be given explaining, at least in part, the remaining discrep-ancy between theory and experiment.
]]></dc:description>
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<identifier>HZDR:PUBLDB:245-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Galindo, V.]]></dc:creator>
<dc:creator><![CDATA[Treuner, M.]]></dc:creator>
<dc:creator><![CDATA[Langbein, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-245-1</dc:identifier>
<dc:title><![CDATA[Thermocapillary Bubble Migration at Higher Marangoni numbers - Theory and Experiment]]></dc:title>
<dc:source><![CDATA[1994 Meeting APS/DFD, Atlanta, 20-22 November]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Single bubble motion driven purely by thermocapillarity (i.e. a linear temperature gradient in the surrounding liquid) is analyzed theoretically with the following steps: A full numerical simulation up to Re of several hundreds depending on the Prandtl-number of the liquid, and a simple analytical treatment describing the asymptotic migration at high Re. Results of short-term microgravity experiments performed at drop Tower Bremen will be reported for 20 < Re < 160. The theoretical migration velocities are slightly higher than the experimental values which might be due to the short-time nature of the experiments. An unsteady theoretical analysis will be given explaining, at least in part, the remaining discrep-ancy between theory and experiment.
]]></dc:description>
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<identifier>HZDR:PUBLDB:797-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Weier, T.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Platacis, E.]]></dc:creator>
<dc:creator><![CDATA[Lielausis, O.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-797-1</dc:identifier>
<dc:title><![CDATA[Experiments on cylinder wake stabilization in an electrolyte solution by means of electromagnetic forces localized on the cylinder surface]]></dc:title>
<dc:source><![CDATA[Flow Control - Workshop, Cargese, July 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Electromagnetic body forces, i.e. Lorentz forces, have been used to modify the boundary layer around a circular cylinder in cross flow. Depending on the polarity of the applied electric field different effects on the flow can be obtained. Lorentz forces directed with the mean flow are able to prevent the boundary layer from separation. Therefore flow separation as well as the von Karman vortex trail can be suppressed. When the momentum gain produced by the Lorentz forces in the boundary layer is high enough, thrust is produced, what results in a jet flow originated from the cylinders back side. If the Lorentz forces are directed opposite to the mean flow, the separation points are shifted towards the front stagnation point, the recirculation region broadens and the von Karman vortex trail is modified. The described technique gives a variety of opportunities to control the flow around the cylinder and the flow structure of the cylinder wake. Results from flow visualizations and numerical calculations are presented.]]></dc:description>
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<identifier>HZDR:PUBLDB:797-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Weier, T.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Platacis, E.]]></dc:creator>
<dc:creator><![CDATA[Lielausis, O.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-797-2</dc:identifier>
<dc:title><![CDATA[Experiments on cylinder wake stabilization in an electrolyte solution by means of electromagnetic forces localized on the cylinder surface]]></dc:title>
<dc:source><![CDATA[Experimental Thermal and Fluid Science, Vol.16, 1998, pp.84-91, Elsevier Science]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Electromagnetic body forces, i.e. Lorentz forces, have been used to modify the boundary layer around a circular cylinder in cross flow. Depending on the polarity of the applied electric field different effects on the flow can be obtained. Lorentz forces directed with the mean flow are able to prevent the boundary layer from separation. Therefore flow separation as well as the von Karman vortex trail can be suppressed. When the momentum gain produced by the Lorentz forces in the boundary layer is high enough, thrust is produced, what results in a jet flow originated from the cylinders back side. If the Lorentz forces are directed opposite to the mean flow, the separation points are shifted towards the front stagnation point, the recirculation region broadens and the von Karman vortex trail is modified. The described technique gives a variety of opportunities to control the flow around the cylinder and the flow structure of the cylinder wake. Results from flow visualizations and numerical calculations are presented.]]></dc:description>
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<identifier>HZDR:PUBLDB:817-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Wagner, W.]]></dc:creator>
<dc:creator><![CDATA[Herbach, C.-M.]]></dc:creator>
<dc:creator><![CDATA[Ortlepp, H.-G.]]></dc:creator>
<dc:creator><![CDATA[Aleksandrov, A. A.]]></dc:creator>
<dc:creator><![CDATA[Aleksandrova, I. A.]]></dc:creator>
<dc:creator><![CDATA[Dietterle, L.]]></dc:creator>
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<dc:creator><![CDATA[Kamanin, D. V.]]></dc:creator>
<dc:creator><![CDATA[Matthies, A.]]></dc:creator>
<dc:creator><![CDATA[Pausch, G.]]></dc:creator>
<dc:creator><![CDATA[Penionzhkevich, Y. E.]]></dc:creator>
<dc:creator><![CDATA[Renz, G.]]></dc:creator>
<dc:creator><![CDATA[Schilling, K.-D.]]></dc:creator>
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<dc:creator><![CDATA[Tsurin, I. P.]]></dc:creator>
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<dc:creator><![CDATA[Vasko, V. M.]]></dc:creator>
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<dc:title><![CDATA[The Binary and Ternary Decay of Hot Heavy Nuclei Produced in the Reaction 14N (34 AMeV) + 197Au]]></dc:title>
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<dc:creator><![CDATA[Wagner, W.]]></dc:creator>
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<dc:title><![CDATA[The binary decay of hot heavy nuclei: fission, evaporation, and also flow?]]></dc:title>
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<dc:creator><![CDATA[Ortlepp, H.-G.]]></dc:creator>
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<dc:creator><![CDATA[Gippner, P.]]></dc:creator>
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<dc:creator><![CDATA[Aleksandrov, A. A.]]></dc:creator>
<dc:creator><![CDATA[Aleksandrova, I. A.]]></dc:creator>
<dc:creator><![CDATA[Doronin, V. N.]]></dc:creator>
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<dc:title><![CDATA[The COMBAS fragment separator of radioactive nuclei and the FOBOS 4pi - detector for charged particles]]></dc:title>
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<identifier>HZDR:PUBLDB:1965-1</identifier>
<datestamp>2023-05-05</datestamp>
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<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Shatrov, V.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1965-1</dc:identifier>
<dc:title><![CDATA[Cylinder wake control by magnetics fields in liquid metal flows]]></dc:title>
<dc:source><![CDATA[Experimental Thermal and Fluid Science 16 (1998) 92-99]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[In the present paper we are concerned with the control of wake instabilities in the flow of an electrically conducting fluid around a circular cylinder by means of external magnetic fields. Besides the Reynolds number (Re) a second parameter N appears describing the strength of the magnetic body force. This offers, depending on the direction of the magnetic field, a large variety of flow configurations and therefore different transition regimes. We perform a numerical simulation of the unsteady two-dimensional flow and characterize the different flow regimes. Strong magnetic fields are capable to stabilize the 2-D flow and to suppress the shedding of vortices. We present curves of neutral 2-D stability in the (Re,N)-parameter plane separating steady and periodic flow regimes. We further perform a linear 3-D stability analysis of the 2-D flow being either steady or periodic and show how the magnetic field influences the 3-D instabilities. We pay special attention to the case when the magnetic field is aligned with the oncoming flow. Here we find 3-D instability in parameter regions above the 2-D stability curve in the (Re, N)-plane where the flow is 2-D stable (steady). This firstly confirms a general result of Hunt (J.C.R. Hunt, Proc. Roy. Soc. A 293 (1966) 342) obtained from a stability analysis of parallel flows and shows that the magnetic field influences 2-D and 3-D instabilities in a different way.]]></dc:description>
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<identifier>HZDR:PUBLDB:392-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Käubler, L.]]></dc:creator>
<dc:creator><![CDATA[Döring, J.]]></dc:creator>
<dc:creator><![CDATA[Funke, L.]]></dc:creator>
<dc:creator><![CDATA[Kleinwächter, P.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
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<dc:identifier>https://www.hzdr.de/publications/Publ-392-1</dc:identifier>
<dc:title><![CDATA[In-Beam Investigation and the Structur of States in 113Sn]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-95 Preprint]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2346-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Aroun, J.]]></dc:creator>
<dc:creator><![CDATA[Eichhorn, F.]]></dc:creator>
<dc:creator><![CDATA[Hempel, A.]]></dc:creator>
<dc:creator><![CDATA[Lukas, P.]]></dc:creator>
<dc:creator><![CDATA[Kolman, B.]]></dc:creator>
<dc:creator><![CDATA[Neufuss, K.]]></dc:creator>
<dc:creator><![CDATA[Mikula, P.]]></dc:creator>
<dc:creator><![CDATA[Strunz, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2346-1</dc:identifier>
<dc:title><![CDATA[SANS investigation of plasma-sprayed materials using double-crystal diffractometer]]></dc:title>
<dc:source><![CDATA[Physica B234-236 (1997) 1011]]></dc:source>
<dc:date>1997</dc:date>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Simoen, E.]]></dc:creator>
<dc:creator><![CDATA[Vanhellemont, J.]]></dc:creator>
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<dc:creator><![CDATA[Claeys, C.]]></dc:creator>
<dc:creator><![CDATA[Gaubas, E.]]></dc:creator>
<dc:creator><![CDATA[Kaniava, A.]]></dc:creator>
<dc:creator><![CDATA[Ohyama, H.]]></dc:creator>
<dc:creator><![CDATA[Sunaga, H.]]></dc:creator>
<dc:creator><![CDATA[Nashiyama, I.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2349-1</dc:identifier>
<dc:title><![CDATA[Proton irradiation effects in silicon junction diodes and charge-coupled devices]]></dc:title>
<dc:source><![CDATA[Radiation Phys.Chem. 50 (1997) 417]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Spaeth, M.]]></dc:creator>
<dc:creator><![CDATA[Kühn, M.]]></dc:creator>
<dc:creator><![CDATA[Kreißig, U.]]></dc:creator>
<dc:creator><![CDATA[Richter, F.]]></dc:creator>
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<dc:title><![CDATA[Preparation of CNx films by ion beam assisted filtered cathodic arc deposition]]></dc:title>
<dc:source><![CDATA[Diamond and Rel. Mat. 6 (1997) 626]]></dc:source>
<dc:date>1997</dc:date>
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<dc:creator><![CDATA[Spieß, L.]]></dc:creator>
<dc:creator><![CDATA[Nennewitz, O.]]></dc:creator>
<dc:creator><![CDATA[Weishart, H.]]></dc:creator>
<dc:creator><![CDATA[Lindner, J.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Romanus, H.]]></dc:creator>
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<dc:creator><![CDATA[Petzoldt, J.]]></dc:creator>
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<dc:title><![CDATA[Aluminium implantation of p-SiC for ohmic contacts]]></dc:title>
<dc:source><![CDATA[Diamond and Rel. Mat. 6 (1997) 1414]]></dc:source>
<dc:date>1997</dc:date>
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<dc:creator><![CDATA[Verbitskaya, E. M.]]></dc:creator>
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<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2354-1</dc:identifier>
<dc:title><![CDATA[Formation of radiation defects in high-resistivity silicon as a result of cyclic irradiation and annealing]]></dc:title>
<dc:source><![CDATA[Semiconductors 31 (1997) 189]]></dc:source>
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<dc:creator><![CDATA[Weise, G.]]></dc:creator>
<dc:creator><![CDATA[Mattern, N.]]></dc:creator>
<dc:creator><![CDATA[Hermann, H.]]></dc:creator>
<dc:creator><![CDATA[Teresiak, A.]]></dc:creator>
<dc:creator><![CDATA[Bächer, I.]]></dc:creator>
<dc:creator><![CDATA[Brückner, W.]]></dc:creator>
<dc:creator><![CDATA[Bauer, H.-D.]]></dc:creator>
<dc:creator><![CDATA[Vinzelberg, H.]]></dc:creator>
<dc:creator><![CDATA[Reiss, G.]]></dc:creator>
<dc:creator><![CDATA[Kreißig, U.]]></dc:creator>
<dc:creator><![CDATA[Mäder, M.]]></dc:creator>
<dc:creator><![CDATA[Markschläger, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2356-1</dc:identifier>
<dc:title><![CDATA[Preparation, structure and properties of MoS<SUB>x</SUB> films]]></dc:title>
<dc:source><![CDATA[Thin Solid Films 298 (1997) 98]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:583-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-583-1</dc:identifier>
<dc:title><![CDATA[Pulsationen bei der Druckentlastung von Reaktoren]]></dc:title>
<dc:source><![CDATA[ACHEMA '97, Frankfurt/M., 9.-14.6.1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[During two-phase blowdown from pressure vessels considerable pulsations of the discharged mass flow rate were found. Regions of instability were predicted by a linear stability analysis. The oscillations are caused by the following feedback circuit: boil up - level movement - void fraction of the discharging mixture - critical discharge rate - velocity of pressure decrease - boil up.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-583-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1624-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Shatrov, V.]]></dc:creator>
<dc:creator><![CDATA[Tomboulides, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1624-1</dc:identifier>
<dc:title><![CDATA[Two and three-dimensional Instabilities of the Cylinder Wake in an Aligned Magnetic Field]]></dc:title>
<dc:source><![CDATA[Physics of Fluids, Vol. 9, 1997, pp. 3114 - 3116]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[2-D and 3-D instabilities in the wake of a circular cylinder placed in an electrically
conducting fluid and subjected to a constant magnetic field aligned with the freestream are investigated numerically. Increasing magnetic fields suppress 2-D instability
(vortex shedding), whereas 3-D instabilities are influenced in a more complex way. In the presence of a magnetic field, 3-D instability has been detected below the 2-D stability threshold. This can lead to a reversal of the order of instabilities, i.e. 3-D instability appears at lower Re than 2-D instability.
]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:493-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Schäfer, F.]]></dc:creator>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Ézsöl, G.]]></dc:creator>
<dc:creator><![CDATA[Guba, A.]]></dc:creator>
<dc:creator><![CDATA[Perneczky, L.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-493-1</dc:identifier>
<dc:title><![CDATA[Simulation of a Small Cold Leg Break Experiment on PMK-2 Test Facility using the codes RELAP5 and ATHLET]]></dc:title>
<dc:source><![CDATA[Nuclear Technology Vol. 118, May 1997, pp. 162-174]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Results of a small break loss of coolant accident experiment, conducted on the PMK-2 integral type test facility are presented. The experiment simulated a 1% break in the cold leg of a VVER-440-type reactor. The main phenomena of the experiment are discussed and in case of selected events a more detailed interpretation with the help of measured void fraction, obtained by a special measurement device is given. Two thermohydraulic computer codes, RELAP5 and ATHLET, are used for post test calculations. The aim of the presented calculations is to investigate the code capability for modeling natural circulation phenomena in VVER-440-type reactors. Therefore the results of the experiment and both calculations are compared. Both codes predict most of the transient events well, with the exception that RELAP5 fails to predict the dry-out-period in the core. In the experiment the hot and cold leg loop seal clearing is accompanied by natural circulation instabilities, which can be explained by means of the ATHLET calculation.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-493-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:581-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Aszodi, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-581-1</dc:identifier>
<dc:title><![CDATA[Verhalten von Lagertanks bei externem Feuer]]></dc:title>
<dc:source><![CDATA[ACHEMA '97, Frankfurt/M., 9.-14.6.1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Wenn ein zylindrischer Lagertank durch ein externes Feuer von der Seite intensiver Wärmeeinwirkung ausgesetzt ist, so setzt der Massenverlust infolge von Dampffreisetzung viel eher ein, als im Fall einer Wärmezuführung vom Behälterboden. Mittels eines vereinfachten Modells konnten die Details des Erwärmungsprozesses und die Ursachen für das unterschiedliche Verhalten in Abhängigkeit von der Art und Weise der Wärmezufuhr erklärt werden. Die ZUfuhr vom Boden führt zu einer irregulären thermischen Konvektion und damit einer guten Durchmischung des Fluids, so daß die Sättigungstemperatur an allen Punkten im Behälter nahezu gleichzeitig erreicht wird. Die maximale Enthalpie im Behälter verbleibt während der gesamten Zeit nahe dem Mittelwert. Wird der Behälter von der Seite beheizt, so bildet sich eine stabile horizontale Temperaturschichtung heraus. Die Bildung von Dampf erfolgt bereits lange bevor die mittlere Temperatur den Siedepunkt erreicht hat. Passive konstruktive Maßnahmen, wie der Einbau von Prallplatten, können die Schichtung stören, das verstärkte Aufheizen an der Oberfläche vermeiden und die Freisetzung von Dampf verzögern. Eine durchgreifende Vermischung des flüssigen Inhalts konnte jedoch nicht erreicht werden. Die genaue Gestalt und die Wirkung dieser Prallplatten hängt von der konkreten Behältergeometrie ab und läßt sich weiter optimieren.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:763-3</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-763-3</dc:identifier>
<dc:title><![CDATA[Natural circulation experiments at the ISB-VVER integral test facility and calculations using the code athlet]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik Aachen 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[In 1995 at the integral test facility ISB-VVER in Elektrogorsk near Moscow natural circulation experiments were performed, which were scientifically accompanied by the Forschungszentrum Rossendorf. These experiments were the first of this kind at a test facility, which models VVER-1000 thermalhydraulics. Using the code ATHLET which is being developed by "Gesellschaft für Anlagen- und Reaktorsicherheit", pre- and posttest calculations were done to determine the thermalhydraulic events to be expected and to define and tune the boundary conditions of the test. The conditions found for natural circulation instabilities and cold leg loop seal clearing could be confirmed by the tests. Besides the thermalhydraulic standard measuring system, the facility was equipped with needle shaped conductivity probes for measuring the local void fractions.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-763-3</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:763-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-763-7</dc:identifier>
<dc:title><![CDATA[Natural circulation experiments at the ISB-VVER integral test facility and calculations using the code athlet]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik Aachen 1997, Proceedings pp. 85-88]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[In 1995 at the integral test facility ISB-VVER in Elektrogorsk near Moscow natural circulation experiments were performed, which were scientifically accompanied by the Forschungszentrum Rossendorf. These experiments were the first of this kind at a test facility, which models VVER-1000 thermalhydraulics. Using the code ATHLET which is being developed by "Gesellschaft für Anlagen- und Reaktorsicherheit", pre- and posttest calculations were done to determine the thermalhydraulic events to be expected and to define and tune the boundary conditions of the test. The conditions found for natural circulation instabilities and cold leg loop seal clearing could be confirmed by the tests. Besides the thermalhydraulic standard measuring system, the facility was equipped with needle shaped conductivity probes for measuring the local void fractions.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-763-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2066-1</identifier>
<datestamp>2025-12-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Feudel, T.]]></dc:creator>
<dc:creator><![CDATA[Strecker, N.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2066-1</dc:identifier>
<dc:title><![CDATA[Atomistic simulation of ion implantation and its application in Si technology]]></dc:title>
<dc:source><![CDATA[Materials Science and Engineering B71 (2000) 128-136]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Atomistic computer simulations based on the binary collision approximation (BCA) are very well suited to predict the dependence of as-implanted dopant profiles on implant parameters like energy, dose and direction of incidence as well as on the arrangement of oxide, poly-Si and other materials on the single-crystalline Si substrate. In particular channeling effects, the enhanced dechanneling due to accumulation of radiation defects during ion bombardment and due to preexisting ion-beam-induced defects can be simulated in a reasonable manner. The BCA code Crystal-TRIM was successfully integrated into 1D and 2D process simulators for the Si technology. The application of the trajectory splitting algorithm and the lateral duplicatioin method ensures a high computational efficiency.]]></dc:description>
<dc:subject><![CDATA[Ion Implantation]]></dc:subject>
<dc:subject><![CDATA[Computer Simulation]]></dc:subject>
<dc:subject><![CDATA[Defects]]></dc:subject>
<dc:subject><![CDATA[Channeling]]></dc:subject>
<dc:subject><![CDATA[Silicon Technology]]></dc:subject>
<dc:subject><![CDATA[Process Simulation]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0921-5107(99)00362-1]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2066-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2066-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Feudel, T.]]></dc:creator>
<dc:creator><![CDATA[Strecker, N.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2066-2</dc:identifier>
<dc:title><![CDATA[Atomistic simulation of ion implantation and its application in Si technology]]></dc:title>
<dc:source><![CDATA[E-MRS 1999 Spring Meeting, Symposium F: Process Induced Defects in Semiconductors, Strasbourg, France, June 1-4, 1999 (invited lecture)]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Atomistic computer simulations based on the binary collision approximation (BCA) are very well suited to predict the dependence of as-implanted dopant profiles on implant parameters like energy, dose and direction of incidence as well as on the arrangement of oxide, poly-Si and other materials on the single-crystalline Si substrate. In particular channeling effects, the enhanced dechanneling due to accumulation of radiation defects during ion bombardment and due to preexisting ion-beam-induced defects can be simulated in a reasonable manner. The BCA code Crystal-TRIM was successfully integrated into 1D and 2D process simulators for the Si technology. The application of the trajectory splitting algorithm and the lateral duplicatioin method ensures a high computational efficiency.]]></dc:description>
<dc:subject><![CDATA[Ion Implantation]]></dc:subject>
<dc:subject><![CDATA[Computer Simulation]]></dc:subject>
<dc:subject><![CDATA[Defects]]></dc:subject>
<dc:subject><![CDATA[Channeling]]></dc:subject>
<dc:subject><![CDATA[Silicon Technology]]></dc:subject>
<dc:subject><![CDATA[Process Simulation]]></dc:subject>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2066-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2068-1</identifier>
<datestamp>2025-12-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Stoemenos, J.]]></dc:creator>
<dc:creator><![CDATA[Pecz, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2068-1</dc:identifier>
<dc:title><![CDATA[Phase formation after high dose aluminium implantation into silicon carbide]]></dc:title>
<dc:source><![CDATA[Journal of Applied Physics 87 (2000) 78-85]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[High doses of 350 keV Al+ ions were implanted into 6H-SiC single crystals at 500oC. The phase formation was studied by TEM, SIMS and AES. A critical Al concentration of about 10 at% was found below that the 6H-SiC structure remains stable. The Al atoms
occupy preferentially Si sites in the SiC lattice. The replaced Si atoms seem to be mobile under the given implantation conditions and diffuse out. At higher Al concentrations the SiC matrix is decomposed and precipitates of Si and Al4C3 are formed.
It was found that the Al4C3 precipitates have a perfect epitaxial orientation to the SiC matrix. The phase transformation is accompanied by atomic redistribution and strong volume swelling. The resulting changes in the atomic profiles can be accounted
for by a simple chemical reaction model.]]></dc:description>
<dc:subject><![CDATA[Silicon Carbide]]></dc:subject>
<dc:subject><![CDATA[Aluminum Implantation]]></dc:subject>
<dc:subject><![CDATA[Phase Formation]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<identifier>HZDR:PUBLDB:2065-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Ortner, K.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Hilditch, L.]]></dc:creator>
<dc:creator><![CDATA[Zheng, Y.]]></dc:creator>
<dc:creator><![CDATA[Dilworth, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2065-1</dc:identifier>
<dc:title><![CDATA[Gold Complexes with Thiosemicarbazones and Phosohine Thiolates]]></dc:title>
<dc:source><![CDATA[37. IUPAC-Kongress, Berlin, August 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Square-planar AuIII complexes are isoelectronic to PtII compounds which are frequently used for cancer therapy. Recently, cancerostatic properties have also been reported for dichloro[2-(dimethylamino-methyl)phenyl-C1,N]gold(III), [Au(damp-C1,N)Cl2] (I) [1], although the mechanism of cytotoxic action may well be different. This encourages us to study the ligand exchange chemistry of this type of compound more in detail.
We have synthesized and structurally characterized a series of AuIII complexes with bi- and tridentate thiosemicarbazones as well as with chelating phosphine thiol ligands which surprisingly stabilize gold in its formal oxidation state "+3".
Reactions of (I) with thiosemicarbazones result in a cleavage of the Au-N bond and protonation of the liberated dimethylamino group. Airstable, zwitterionic compounds are formed. The thiosemicarbazones co-ordinate as deprotonated chelate ligands substituting Cl-. Fig. 1 illustrates an example with the bidentate vanillinethiosemicarbazone. Remaining Cl- ligands can be replaced by further ligand exchange reactions, e.g. with thiolates.]]></dc:description>
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<identifier>HZDR:PUBLDB:539-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Hirsch, W.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Tetzlaff, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-539-1</dc:identifier>
<dc:title><![CDATA[Saxon Wind Energy Ressources: Comparison of WASP and KAMM Results]]></dc:title>
<dc:source><![CDATA[Proceedings of the 1996 European Union Wind Energy Conference and Exhibition, Göteborg (Sweden), 20.-24.5.1996, pp. 604-607]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The wind energy  ressources of a selected saxon area ( 64 km x 48 km ) has been investigated in detail. The region can be characterized by a mean height of  200 m a.s.l. with  complex surface profil. Based on measuring data of three stations WASP calculations with a grid step of 0.25 km has been performed for the whole region. The data are compared with calculation results of the mesoscale KAMM model. These calculations based on the geostrophic wind data of the Czech station Prague and used a 1.0 km and a 2.5 km grid ( coresponding 60 and 120 wind clusters ). The ressource maps ( mean wind velocity and power density ) calculated by both methods show corresponding high wind potential in the investigated area. Differences in the absolute values are explained by the features of the used programmes.]]></dc:description>
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<identifier>HZDR:PUBLDB:537-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Brünig, D.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-537-1</dc:identifier>
<dc:title><![CDATA[Solare Warmwasserbereitung und Fernwärmeeinspeisung -Waldblickschule Freital-]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-137, April 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[In ein mit Erdgas betriebenes konventionelles Fernwärmesystem (Anschlußleistung 2,1 MW) wurde eine Solarkollektoranlage mit einer Bruttofläche von 100 m² integriert. Die Kollektoranlage diente vorrangig der Erzeugung von Brauchwarmwasser für eine Schule, solare Überschüsse wurden in den Rücklauf des Fernwärmesystems eingespeist. Ein umfangreiches Meßprogramm ermöglichte Effizienzuntersuchungen des Systems.
Der jährliche Nettoertrag des Solarsystems lag bei 280 kWh/m² bei einem Systemnutzungsgrad von 26%. Beide Kennziffern wurden durch hohe Rücklauftemperaturen (58°C) im Nahwärmenetz negativ beeinflußt. Weitere Untersuchungen galten dem Betrieb der eingesetzten Schichtspeicher (Reihenschaltung). Bei Ausschöpfung der in dem Vorhaben deutlich gewordenen Optimierungspotentiale können in künftigen Anlagen Nettoerträge von 350 kWh/m² und solare Wärmegestehungskosten unter 30 Pf./kWh erreicht werden.
]]></dc:description>
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<identifier>HZDR:PUBLDB:499-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Ihle, T.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-499-1</dc:identifier>
<dc:title><![CDATA[Betriebsverhalten von netzgekoppelten Photovoltaikanlagen aus dem 1000-Dächer-Programm]]></dc:title>
<dc:source><![CDATA[11. Symposium Photovolterische Solarenergie, 13.-15.3.1996, Staffelstein, Tagungsband S. 294-298]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Durch das FZR werden an 50 PV-Anlagen in Sachsen mehrjährige Untersuchungen zum Betriebsverhalten durchgeführt. Das Untersuchungsprogramm umfaßt die technische Überprüfung des Anlagenzustandes und die Messung der Kennlinien des PV-Generators und der eingesetzten Wechselrichter. Ferner erfolgt eine monatliche Analyse der erreichten Energieerträge. Die ersten Ergebnisse dieser Untersuchungen sind im Beitrag zusammengefaßt.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:499-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Ihle, T.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-499-7</dc:identifier>
<dc:title><![CDATA[Betriebsverhalten von netzgekoppelten Photovoltaikanlagen aus dem 1000-Dächer-Programm]]></dc:title>
<dc:source><![CDATA[11. Symposium Photovolterische Solarenergie, 13.-15.3.1996, Staffelstein, Tagungsband S. 294-298]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Durch das FZR werden an 50 PV-Anlagen in Sachsen mehrjährige Untersuchungen zum Betriebsverhalten durchgeführt. Das Untersuchungsprogramm umfaßt die technische Überprüfung des Anlagenzustandes und die Messung der Kennlinien des PV-Generators und der eingesetzten Wechselrichter. Ferner erfolgt eine monatliche Analyse der erreichten Energieerträge. Die ersten Ergebnisse dieser Untersuchungen sind im Beitrag zusammengefaßt.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:655-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:creator><![CDATA[Schubart, R.]]></dc:creator>
<dc:creator><![CDATA[Grawe, H.]]></dc:creator>
<dc:creator><![CDATA[Górska, M.]]></dc:creator>
<dc:creator><![CDATA[Fitzgerald, J. B.]]></dc:creator>
<dc:creator><![CDATA[Heese, J.]]></dc:creator>
<dc:creator><![CDATA[Kluge, H.]]></dc:creator>
<dc:creator><![CDATA[Maier, K. H.]]></dc:creator>
<dc:creator><![CDATA[Rejmund, M.]]></dc:creator>
<dc:creator><![CDATA[Schramm, M.]]></dc:creator>
<dc:creator><![CDATA[Severyniak, D.]]></dc:creator>
<dc:creator><![CDATA[Spohr, K.]]></dc:creator>
<dc:creator><![CDATA[Käubler, L.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-655-1</dc:identifier>
<dc:title><![CDATA[In-beam spectroscopy and shell model structure of the neutron deficient 103In and 100, 102Cd]]></dc:title>
<dc:source><![CDATA[Physica Scripta T56 (1995) pp. 311]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1964-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Mößner, R.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1964-1</dc:identifier>
<dc:title><![CDATA[Bouyant Melt Flows Under the Influcence of Steady and Rotating Magnetic Fields]]></dc:title>
<dc:source><![CDATA[Journal of Crystal Growth, Vol.197, pp.341-354, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Rotating magnetic fields are of growing interest for crystal growth technologies from the melt. For a few millitesla they provide a controlled motion within the melt, thus controlling the heat and mass transfer and the temperature fluctuations. This paper gives numerical results for the stability thresholds of rotating magnetic field and buoyancy driven melt convections, also by additionally superimposing a steady magnetic field. Some numerical results are given for a possible explanation of the surprising stabilizing action of the rotating magnetic field on a pre-given buoyant flow.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:14247-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:creator><![CDATA[Vieluf, M.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-14247-1</dc:identifier>
<dc:title><![CDATA[Hochauflösende Rutherford-Streuspektrometrie zur Untersuchung von ZrO2-Schichtwachstum im Anfangsstadium]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Helmholtz-Zentrum Dresden-Rossendorf; FZD-537 2010<br>ISSN: 1437-322X]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Die vorliegende Arbeit entstand im Rahmen einer Kooperation des Forschungszentrums Dresden-Rossendorf mit Qimonda Dresden GmbH & Co. OHG. Mithilfe der hochauflösenden Rutherford-Streuspektrometrie (HR-RBS) wurden das Diffusionsverhalten und Schichtwachstum von ZrO2 auf SiO2 und TiN im Anfangsstadium untersucht. Auf Grund der exzellenten Tiefenauflösung von 0,3 nm an der Oberfläche stand die Analyse von Konzentrationsprofilen in ultradünnen Schichten, respektive an deren Grenzflächen im Vordergrund.
Zur qualitativen Verbesserung der Messergebnisse wurde erstmals ein zweidimensionaler positionsempfindlicher Halbleiterdetektor in den Aufbau der HR-RBS implementiert und charakterisiert. Außerdem wurde ein Messverfahren in Betrieb genommen, das mögliche Schädigungen durch den Ioneneintrag in die Messprobe minimiert. Durch die Optimierung der experimentellen Bedingungen und die Entwicklung eines Programmpaketes zur Unterstützung des Analysten konnte ein effizienter Routine-Messablauf erstellt werden.
Im Moment einer binären Kollision zwischen einfallendem Ion und Targetelement kommt es bei kleinem Stoßparameter zu Veränderungen des Ladungszustands der gestreuten Ionen, insbesondere durch die abrupte Geschwindigkeitsänderung des Projektils und der Überlappung der Elektronenwolken. Bei der HR-RBS mit Energie separierendem Dipolmagneten muss zur Interpretation von Streuspektren die Ladungszustandsverteilung der gestreuten Projektile bekannt sein. Erstmalig konnte eine signifikante Abhängigkeit der Ladungszustandsverteilung gestreuter C-Ionen sowohl von der Schichtdicke als auch der Ordnungszahl des detektierten Targetelements, hier der vierten Nebengruppe, nachgewiesen werden.
Diese gewonnen Erkenntnisse ermöglichten systematische Untersuchungen zum ZrO2-Schichtwachstum im Anfangsstadium. Zur Herstellung der ZrO2-Schichten wurde die Atomlagenabscheidung (ALD) verwendet. Anhand der nachgewiesenen Agglomeration von ZrO2 auf nativen SiO2 wurde mithilfe der Rasterkraftmikroskopie (AFM) zur Bestimmung von Oberflächenrauigkeiten eine Methode konzipiert, welche die Auswirkung lokaler Schichtdickeninhomogenitäten auf die niederenergetische Flanke eines Streuspektrums berücksichtigt. Auf dieser Grundlage durchgeführte Simulationsrechnungen ergeben, dass keine Diffusion von Zr in die darunter liegende Schicht stattfand, jedoch eine ZrSiO4-Grenzflächenschicht existiert. Für das Wachstum von ZrO2 auf TiN wird aus den hoch aufgelösten Streuspektren ein völlig anderes Verhalten abgeleitet. Messungen zu Oberflächentopografien der TiN-Schicht liefern nicht zu vernachlässigende Werte für die Rauigkeit. Um den Einfluss der Oberflächenrauigkeit auf die Form des hoch aufgelösten Spektrums erfassen zu können, wurde eine Software entwickelt. Auf Basis von AFM-Messungen ermöglicht dieses Programm das Extrahieren einer Energieverteilung aus den Weglängen von ausschließlich an der Oberfläche gestreuten Ionen. Unter Berücksichtigung des Effekts der Oberflächenrauigkeit auf die HR-RBS Spektrenform konnte die Diffusion von Zr in das polykristalline TiN erstmals verifiziert werden. Die Beobachtungen weisen daraufhin, dass bereits nach dem ersten ALD-Zyklus ein geringer Anteil der deponierten Zr-Atome bis in eine Tiefe von etwa 3 nm in das TiN diffundiert. Die vorläufigen Ergebnisse legen Korngrenzendiffusion nahe.]]></dc:description>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Galindo, V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1982-1</dc:identifier>
<dc:title><![CDATA[Einsatz von Magnetfeldern bei der Silizium-Czochalski-Kristallzüchtung]]></dc:title>
<dc:source><![CDATA[Berg und Hüttenmännischer Tag, TU Bergakademie Freiberg, 18.06.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Eine kontaktlose Beeinflussung der konvektiven Strömung in der Schmelze ist in vielen Kristallzüchtungstechnologien von großer Bedeutung. Gewöhnlich werden stationäre magnetische Felder benutzt, um solche Strömungen zu dämpfen. Überraschenderweise können auch aktive Strömungsantriebskräfte, die von instationären magnetischen Feldern erzeugt werden, von stabilisierendem Charakter sein. Wir stellen Resultate der numerischen Simulation der kombinierten Wirkung von homogenen und linearen stationären Magnetfeldern für die Silizium-Czochalski-Kristallzüchtung und von homogenen und rotierenden Magnetfeldern für die Bridgman-Anordnung vor. Es werden bei der Czochalski-Geometrie nicht nur die thermische Konvektion und die Rotation des Kristalls und des Tiegels in Betracht gezogen, sondern auch der Einfluß der antreibenden und/oder dämpfenden elektromagnetischen Kräfte sowie der Einfluß des induzierten elektrischen Stromes und der thermokapillar angetriebenen Strömungen an der freien deformierbaren Schmelzoberfläche. Aufgrund der hohen Reynolds-Zahl der Strömung ist die numerische Simulation laminar nicht mehr möglich. Es werden vergleichende Rechnungen mit einem Null-Gleichungs-Turbulenzmodell, das auf der Prandtl´schen Mischungsweg-Hypothese basiert, und einem anisotropen k-epsilon Turbulenzmodell durchgeführt.]]></dc:description>
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<identifier>HZDR:PUBLDB:2112-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Bagryansky, P. A.]]></dc:creator>
<dc:creator><![CDATA[Et Al.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2112-1</dc:identifier>
<dc:title><![CDATA[Neutral Particle Balance in GDT with Fast Titanium Coating of the First Wall]]></dc:title>
<dc:source><![CDATA[IEEE International Conference on Plasma Science, 1995, Madison, Wisconsin, USA, p. 200]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2114-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Anikeev, A. V.]]></dc:creator>
<dc:creator><![CDATA[Bagryansky, P. A.]]></dc:creator>
<dc:creator><![CDATA[Deichuli, P. P.]]></dc:creator>
<dc:creator><![CDATA[Ivanov, A. A.]]></dc:creator>
<dc:creator><![CDATA[Karpushov, A. N.]]></dc:creator>
<dc:creator><![CDATA[Kuznetsov, G. I.]]></dc:creator>
<dc:creator><![CDATA[Lizunov, A. A.]]></dc:creator>
<dc:creator><![CDATA[Maximiov, V. V.]]></dc:creator>
<dc:creator><![CDATA[Murakhtin, S. V.]]></dc:creator>
<dc:creator><![CDATA[Saunichev, K. N.]]></dc:creator>
<dc:creator><![CDATA[Stupishin, N. V.]]></dc:creator>
<dc:creator><![CDATA[Noack, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2114-1</dc:identifier>
<dc:title><![CDATA[Studies of Plasma Axial Confinement and Transverse Transport in the GDT Experiment]]></dc:title>
<dc:source><![CDATA[23rd EPS Conference on Controlled Fusion and Plasma Physics, Kiev, Ukraine, 1996, Proceedings Vol. 20C, part II, p. 688-691]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2114-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Anikeev, A. V.]]></dc:creator>
<dc:creator><![CDATA[Bagryansky, P. A.]]></dc:creator>
<dc:creator><![CDATA[Deichuli, P. P.]]></dc:creator>
<dc:creator><![CDATA[Ivanov, A. A.]]></dc:creator>
<dc:creator><![CDATA[Karpushov, A. N.]]></dc:creator>
<dc:creator><![CDATA[Kuznetsov, G. I.]]></dc:creator>
<dc:creator><![CDATA[Lizunov, A. A.]]></dc:creator>
<dc:creator><![CDATA[Maximiov, V. V.]]></dc:creator>
<dc:creator><![CDATA[Murakhtin, S. V.]]></dc:creator>
<dc:creator><![CDATA[Saunichev, K. N.]]></dc:creator>
<dc:creator><![CDATA[Stupishin, N. V.]]></dc:creator>
<dc:creator><![CDATA[Noack, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2114-7</dc:identifier>
<dc:title><![CDATA[Studies of Plasma Axial Confinement and Transverse Transport in the GDT Experiment]]></dc:title>
<dc:source><![CDATA[23rd EPS Conference on Controlled Fusion and Plasma Physics, Kiev, Ukraine, 1996, Proceedings Vol. 20C, part II, p. 688-691]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:2115-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ivanov, A. A.]]></dc:creator>
<dc:creator><![CDATA[Kumpf, H.]]></dc:creator>
<dc:creator><![CDATA[Noack, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2115-1</dc:identifier>
<dc:title><![CDATA[Improved Version of a Mirror Based 14 MeV Neutron Source]]></dc:title>
<dc:source><![CDATA[16th IAEA Fusion Energy Conference, Montreal, Canada, October 7-11, 1996, Proceedings Vol. III, pp. 667-675, IAEA-CN-64/GP-24]]></dc:source>
<dc:date>1996</dc:date>
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<header>
<identifier>HZDR:PUBLDB:2115-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ivanov, A. A.]]></dc:creator>
<dc:creator><![CDATA[Kumpf, H.]]></dc:creator>
<dc:creator><![CDATA[Noack, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2115-7</dc:identifier>
<dc:title><![CDATA[Improved Version of a Mirror Based 14 MeV Neutron Source]]></dc:title>
<dc:source><![CDATA[16th IAEA Fusion Energy Conference, Montreal, Canada, October 7-11, 1996, Proceedings Vol. III, pp. 667-675, IAEA-CN-64/GP-24]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:2117-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bagryansky, P. A.]]></dc:creator>
<dc:creator><![CDATA[Et Al.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2117-1</dc:identifier>
<dc:title><![CDATA[Recent Results of Experiments on the Gas Dynamic Trap]]></dc:title>
<dc:source><![CDATA[International Conference "Open Systems '98", July 27 - 31, 1998, Novosibirsk, Russia, Transactions of Fusion Technology, 35 (1999) 79]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:2118-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Karpushov, A. N. E. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2118-1</dc:identifier>
<dc:title><![CDATA[Energy Confinement of the High ß Two-Component Plasma in the Gas Dynamic Trap]]></dc:title>
<dc:source><![CDATA[International Conference "Open Systems '98", July 27 - 31, 1998, Novosibirsk, Russia, Transactions of Fusion Technology, 35 (1999) 190]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:audience>Researchers</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2120-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Murachtin, S. V. E. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2120-1</dc:identifier>
<dc:title><![CDATA[Wall Conditioning and Neutral Gas Transport at the GDT Facility]]></dc:title>
<dc:source><![CDATA[International Conference "Open Systems '98", July 27 - 31, 1998,
Novosibirsk, Russia, Transactions of Fusion Technology, 35 (1999) 370]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2120-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2121-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Collatz, S.]]></dc:creator>
<dc:creator><![CDATA[Noack, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2121-1</dc:identifier>
<dc:title><![CDATA[NEUSI - A Code for the Calculation of Neutral Particle Densities Inside the Plasma Region of the GDT]]></dc:title>
<dc:source><![CDATA[International Conference "Open Systems '98", July 27 - 31, 1998, Novosibirsk, Russia, Transactions of Fusion Technology, 35 (1999) 375]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Based on the Integral Transport Method the code NEUSI calculates the radial-, axial- and time-dependent distributions of fast and slow hydrogen atoms and hydrogen molecules in the plasma region of the GDT facility of the Budker Institute Novosibirsk. The present paper briefly describes the basic features and approximations of the code and gives some calculation results.]]></dc:description>
<dc:subject><![CDATA[mirror plasma]]></dc:subject>
<dc:subject><![CDATA[gas dynamic trap]]></dc:subject>
<dc:subject><![CDATA[neutral gas]]></dc:subject>
<dc:subject><![CDATA[transport calculation]]></dc:subject>
<dc:subject><![CDATA[integral transport method]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:2121-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Collatz, S.]]></dc:creator>
<dc:creator><![CDATA[Noack, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2121-7</dc:identifier>
<dc:title><![CDATA[NEUSI - A Code for the Calculation of Neutral Particle Densities Inside the Plasma Region of the GDT]]></dc:title>
<dc:source><![CDATA[International Conference "Open Systems '98", July 27 - 31, 1998, Novosibirsk, Russia, Transactions of Fusion Technology, 35 (1999) 375]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Based on the Integral Transport Method the code NEUSI calculates the radial-, axial- and time-dependent distributions of fast and slow hydrogen atoms and hydrogen molecules in the plasma region of the GDT facility of the Budker Institute Novosibirsk. The present paper briefly describes the basic features and approximations of the code and gives some calculation results.]]></dc:description>
<dc:subject><![CDATA[mirror plasma]]></dc:subject>
<dc:subject><![CDATA[gas dynamic trap]]></dc:subject>
<dc:subject><![CDATA[neutral gas]]></dc:subject>
<dc:subject><![CDATA[transport calculation]]></dc:subject>
<dc:subject><![CDATA[integral transport method]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2124-1</identifier>
<datestamp>2025-12-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Parascandola, S.]]></dc:creator>
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<dc:title><![CDATA[The interplay of sputtering and oxidation during plasma diffusion treatment]]></dc:title>
<dc:source><![CDATA[Applied Physics Letters 75 (1999) No. 13, 1851-1853]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Metals that form dense native surface oxide layers challenge plasma diffusion treatment techniques. Experimental results obtained during nitriding of stainless steel from real-time depth-resolved compositional analysis by elastic recoil detection give insight into the transport kinetics. In agreement with semi-quantitative considerations on the oxide removal and the oxide growth, the interplay of sputtering and oxidation emerges as a key parameter. On this background, suggestions for practical applications and optimization of the modification processes are given for different plasma diffusion treatment techniques.]]></dc:description>
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<dc:title><![CDATA[BWR Physics and Thermohydraulics Complementary Actions to the IPSS-BWR R&D Cluster]]></dc:title>
<dc:source><![CDATA[Final Report, CEA Cadarache: RT DER/SIS/LSS 98/32-1, February 1998]]></dc:source>
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<dc:description><![CDATA[As a complement of the EU-IPSS-BWR R&D Cluster project the "BWR-Physics and Thermohydraulics Complementary Actions" contributed to answer issues which are identified for the future BWR plants: The design of innovative components, an enlarged assesment of the performances and a better understanding of the underlying physical phenomena both thermohydraulics and neutronics and the interaction of the two.
Partners from 5 EU countries were involved in the project.
The report summarizes the main results (concerning thermal valves, isolation condensers, emergency condensor, building condenser and dynamical properties of BWR) of the project.
]]></dc:description>
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<dc:title><![CDATA[In-situ TEM study of the evolution of CoSi<SUB>2</SUB> precipitates during annealing and ion irradiation]]></dc:title>
<dc:source><![CDATA[10th International Conference on Microscopy of Semiconducting Materials, Oxford, UK, April 7 - 10, 1997]]></dc:source>
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<dc:title><![CDATA[In-situ TEM study of the evolution of CoSi<SUB>2</SUB> precipitates during annealing and ion irradiation]]></dc:title>
<dc:source><![CDATA[Proc. of the Royal Microscopical Society Conf. "Microscopy of Semiconducting Materials 1997"; Inst. Phys. Conf. Ser. 157 (1997) 501]]></dc:source>
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<dc:title><![CDATA[Maskenlose schreibende Ionenimplantation mit massensepatiertem FIB]]></dc:title>
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<dc:title><![CDATA[Mikro- und Nanostrukturierung mit Ionenfeinstrahlen]]></dc:title>
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<dc:title><![CDATA[Mikro- und Nanostrukturierung mit Ionenfeinstrahlen]]></dc:title>
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<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
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<dc:title><![CDATA[Photo-and electroluminescence from Ge implanted SiO<SUB>2</SUB> films]]></dc:title>
<dc:source><![CDATA[Gordon Conference, New Hampshire, USA, August 1997]]></dc:source>
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<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
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<dc:title><![CDATA[Institute of Safety Research; Annual Report 1996]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-190 August 1997]]></dc:source>
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<dc:description><![CDATA[The report gives an overview on the scientific work of the Institute of Safety Research in 1996. ]]></dc:description>
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<dc:creator><![CDATA[Prokert, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3208-1</dc:identifier>
<dc:title><![CDATA[Röntgenreflektometrie an Dünnschichtsystemen]]></dc:title>
<dc:source><![CDATA[Vortrag im Graduiertenkolleg der TU Chemnitz:
"Dünne Schichten und nichtkristalline Materialien"
Chemnitz , 8. Juni 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Übersicht über die Methoden und Einsatzmöglichkeiten der Röntgenreflektometrie (XRR). Diskussion der Anwendungen der XRR bei Herstellung und Charakterisierung dünner Schichten und von  Vielschichtsystemen. Als Beispiele wurden u.a. Ergebnisse eigener Messungen an der Rossendorfer Beamline (ROBL/ESRF)in Grenoble herangezogen. ]]></dc:description>
<dc:subject><![CDATA[Röntgenreflektometrie]]></dc:subject>
<dc:subject><![CDATA[Oberflächenrauhigkeit]]></dc:subject>
<dc:subject><![CDATA[Dünnschichtsysteme]]></dc:subject>
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<dc:creator><![CDATA[Anikeev, A. V.]]></dc:creator>
<dc:creator><![CDATA[Bagryansky, P. A.]]></dc:creator>
<dc:creator><![CDATA[Deichuli, P. P.]]></dc:creator>
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<dc:creator><![CDATA[Otto, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2113-1</dc:identifier>
<dc:title><![CDATA[The Plasma Neutron Source Simulations in the GDT Experiment]]></dc:title>
<dc:source><![CDATA[23rd EPS Conference on Controlled Fusion and Plasma Physics, Kiev, Ukraine, 1996, Proceedings Vol. 20C, part II, pp. 684-687]]></dc:source>
<dc:date>1996</dc:date>
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<dc:creator><![CDATA[Otto, G.]]></dc:creator>
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<dc:title><![CDATA[The Plasma Neutron Source Simulations in the GDT Experiment]]></dc:title>
<dc:source><![CDATA[23rd EPS Conference on Controlled Fusion and Plasma Physics, Kiev, Ukraine, 1996, Proceedings Vol. 20C, part II, pp. 684-687]]></dc:source>
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<dc:title><![CDATA[Plasma confinement and stability studies in the gas-dynamic trap experiment]]></dc:title>
<dc:source><![CDATA[16th IAEA fusion energy conferency, Montreal, Canada, October 7 - 11, 1996, Proceedings Vol. II, pp. 283-291, IAEA-CN-64/CP-22]]></dc:source>
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<dc:title><![CDATA[Plasma confinement and stability studies in the gas-dynamic trap experiment]]></dc:title>
<dc:source><![CDATA[16th IAEA fusion energy conferency, Montreal, Canada, October 7 - 11, 1996, Proceedings Vol. II, pp. 283-291, IAEA-CN-64/CP-22]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
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<dc:title><![CDATA[Finite-element based vibration analyses of WWER-440 type reactors]]></dc:title>
<dc:source><![CDATA[Annals of Nuclear Energy, Vol 26 (12), 1999, pp. 1037-1052]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[A finite-element-model describing the mechanical vibrations of the whole WWER-440 primary circuit was established to support the early detection of mechanical component faults. A special fluid-structure module was developed to consider the reaction forces of the fluid in the downcomer upon the moving core barrel and the rector pressure vessel. This fluid-structure interaction module is based on an approximated analytical 2D-solution of the coupled system of 3D fluid equations and the structural equations of motions. By means of the vibration model all igenfrequencies up to 30 Hz and the corresponding mode shapes were calculated. It is shown that the fluid-structure interaction strongly influences those modes that lead to a relative displacement between reactor pressure vessel and core barrel. Moreover, by means of the model the shift of eigenfrequencies due to the degradation or to the failure of internal clamping and spring elements was investigated. Comparing the frequency spectra of the normal and the faulty structure, it could be proved that a recognition of such degradations and failures even inside the reactor pressure vessel is possible by pure excore vibration measurements.]]></dc:description>
<dc:subject><![CDATA[finite-element-modelling]]></dc:subject>
<dc:subject><![CDATA[fluid-structure interactions]]></dc:subject>
<dc:subject><![CDATA[vibration monitoring]]></dc:subject>
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<identifier>HZDR:PUBLDB:2376-1</identifier>
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2376-1</dc:identifier>
<dc:title><![CDATA[Schwingungsmodellierung zur Unterstützung der Diagnostik an Druckwasserreaktoren]]></dc:title>
<dc:source><![CDATA[Sächsisches Kolloquium Technische Diagnostik, TU Dresden, 29.01.1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Überblicksvortrag zu den Arbeiten zur Schwingungsmodellierung und Diagnostik an Reaktoren des Typs WWER-440]]></dc:description>
<dc:subject><![CDATA[Finite-Elemente-Analyse]]></dc:subject>
<dc:subject><![CDATA[Schwingungsüberwachung]]></dc:subject>
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<identifier>HZDR:PUBLDB:1111-3</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
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<dc:title><![CDATA[Post Test Calculations for a Small Break LOCA Experiment at the Integral Test Facility ISB-VVER Using the Thermalhydraulic Code ATHLET]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik Mannheim 1996, Proceedings pp. 122-125]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The ISB-VVER facility of the Elektrogorsk Research and Engineering Center is currently the only operating integral test facility for the thermal hydraulic behaviour of the Russian pressurized water reactor VVER-1000. In 1993 it was decided, to perform a test for a small break at the upper plenum with locked rotor of all circulating pumps as the 1st Russian Standard Problem. The experimental results were made available to the Research Center Rossendorf, where post test calculations were carried out using the GRS-code ATHLET. The main results of these calculations are presented in this paper.]]></dc:description>
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
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<dc:title><![CDATA[Post Test Calculations for a Small Break LOCA Experiment at the Integral Test Facility ISB-VVER Using the Thermalhydraulic Code ATHLET]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik Mannheim 1996, Proceedings pp. 122-125]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The ISB-VVER facility of the Elektrogorsk Research and Engineering Center is currently the only operating integral test facility for the thermal hydraulic behaviour of the Russian pressurized water reactor VVER-1000. In 1993 it was decided, to perform a test for a small break at the upper plenum with locked rotor of all circulating pumps as the 1st Russian Standard Problem. The experimental results were made available to the Research Center Rossendorf, where post test calculations were carried out using the GRS-code ATHLET. The main results of these calculations are presented in this paper.]]></dc:description>
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<identifier>HZDR:PUBLDB:1112-1</identifier>
<datestamp>2023-05-02</datestamp>
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1112-1</dc:identifier>
<dc:title><![CDATA[Post Test Calculations to 11% Break LOCA Experiments at the Integral Test Facility ISB-VVER Using the Thermohydraulic Code ATHLET]]></dc:title>
<dc:source><![CDATA[Nuclear Engineering and Design 170 (1997) pp. 3-7]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The considered test was a break on the upper plenum with different modes of emergency core cooling. The reference case was the non-availability of emergency cooling. Injecting the emergency coolant into the cold leg, no increasing of rod cladding temperatures was observed, but natural circulation instabilities occurred. Injecting the cooling into the hot leg, the cooling situation was getting worse. Due to the injected cold emergency coolant, the fluid density in the discharge volume was enhanced and the break mass flow increased. The observed events in the test were reproduced by the code with good agreement

]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2024-3</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Willschütz, H.-G.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2024-3</dc:identifier>
<dc:title><![CDATA[Calculation of a Mixed Convection Flow Benchmark Using Different CFD Codes]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik '99, Tagungsbericht S. 135-138, Karlsruhe 18.-20. Mai 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[New reactor designs comprise passive elements for decay heat removal. Computational-Fluid-Dynamics codes are an appropriate tool for the assessment of the efficiency of those components. Most of these codes are based either on the Finite-Volume or the Finite-Element method. Because of the importance for reactor safety these numerical tools have to be thoroughly validated using results from experimental setups.
The governing mechanism in passive components for decay heat removal is natural convection and heat transfer with internal heating. To assess the capability describing mixed convection flow, post test calculations of an IAHR benchmark exercise were performed (Kamide et. al, 1991). The commercial codes CFX-4® and ANSYS/FLOTRAN® were used, representing the Finite-Volume Method and the Finite-Element Method respectively.
This paper presents a discussion of the problems and capabilities of each code to calculate complex flow regimes and temperature fields.
]]></dc:description>
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
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<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2024-7</dc:identifier>
<dc:title><![CDATA[Calculation of a Mixed Convection Flow Benchmark Using Different CFD Codes]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik '99, Tagungsbericht S. 135-138, Karlsruhe 18.-20. Mai 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[New reactor designs comprise passive elements for decay heat removal. Computational-Fluid-Dynamics codes are an appropriate tool for the assessment of the efficiency of those components. Most of these codes are based either on the Finite-Volume or the Finite-Element method. Because of the importance for reactor safety these numerical tools have to be thoroughly validated using results from experimental setups.
The governing mechanism in passive components for decay heat removal is natural convection and heat transfer with internal heating. To assess the capability describing mixed convection flow, post test calculations of an IAHR benchmark exercise were performed (Kamide et. al, 1991). The commercial codes CFX-4® and ANSYS/FLOTRAN® were used, representing the Finite-Volume Method and the Finite-Element Method respectively.
This paper presents a discussion of the problems and capabilities of each code to calculate complex flow regimes and temperature fields.
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:270-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ézsöl, G.]]></dc:creator>
<dc:creator><![CDATA[Guba, A.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Schäfer, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-270-2</dc:identifier>
<dc:title><![CDATA[Small cold leg break experiment on PMK-2]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik, Nürnberg, 16. -18. Mai 1995, p. 119]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[In the framework of the computer code assessment programme for the VVER-440 type Paks Nuclear Power Plant a 1% cold leg break experiment has been executed on the PMK-2 integral type test facility. For the test it was considered that only high pressure injection system (HPIS) is available and there is no injection from the safety injection tanks (SIT). The experiment was the repetition of the test measured in 1990, with improved data aquisition system. In the report the results of the experiment were discussed and a description of the phenomena was given.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<record>
<header>
<identifier>HZDR:PUBLDB:270-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ézsöl, G.]]></dc:creator>
<dc:creator><![CDATA[Guba, A.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Schäfer, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-270-1</dc:identifier>
<dc:title><![CDATA[Small cold leg break experiment on PMK-2]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik 1995]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[In the framework of the computer code assessment programme for the VVER-440 type Paks Nuclear Power Plant a 1% cold leg break experiment has been executed on the PMK-2 integral type test facility. For the test it was considered that only high pressure injection system (HPIS) is available and there is no injection from the safety injection tanks (SIT). The experiment was the repetition of the test measured in 1990, with improved data aquisition system. In the report the results of the experiment were discussed and a description of the phenomena was given.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-270-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1986-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Hollstein, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1986-1</dc:identifier>
<dc:title><![CDATA[HEXNEM2 - a New Nodal Method for Hexagonal Geometry]]></dc:title>
<dc:source><![CDATA[presented at the AER Working Group D Meeting, Rez (Czech Republic), May 18-20, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[A new nodal method HEXNEM2 for hexagonal geometry is described. The method is based on a two-dimensional expansion of
the intranodal fluxes. Polynomials up to the second order and exponential functions are used in each group. By this method the singular
terms occurring in the transverse integration methods are avoided. Side averaged and corner point values of fluxes and currents are used
for the coupling of nodes. A calculation scheme for the outgoing partial currents at the sides and similar expressions for the corners from
given incoming values are used in the inner iteration which gives a fast running scheme. The method is tested against 2-dimensional
hexagonal benchmark problems for the VVER-type reactors. The results show that the multiplication factor and nodal powers are predicted
accurately. A considerable improvement can be shown of the results for the VVER-1000 benchmarks compared with the method developed
previously for the code DYN3D and the simpler method HEXNEM1. ]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1986-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2027-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schumacher, G.]]></dc:creator>
<dc:creator><![CDATA[Dettenwanger, F.]]></dc:creator>
<dc:creator><![CDATA[Schütze, M.]]></dc:creator>
<dc:creator><![CDATA[Hornauer, U.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2027-1</dc:identifier>
<dc:title><![CDATA[Microalloying effects in the oxidation of TiAl materials]]></dc:title>
<dc:source><![CDATA[Intermetallics Vol. 7 10 (1999) 1113-1120]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The influence of microalloying on the oxidation behavior of gamma-TiAl based alloys was studied. The microalloying elements were added by ion implantation. Oxidation tests at 1173 K in air showed that the addition of chlorine into TiAl improves the oxidation resistance resulting in a decrease of the oxidation rate by about 2 orders of magnitude compared to unalloyed TiAl. Microstructural investigations revealed that the formation of an protective alumina layer on top of Cl-implanted TiAl is the cause for the decrease in the oxidation rate. AES measurements in the initial stage of oxidation showed that chlorine is located under the alumina layer in the metal phase. Thermodynamic calculations, investigations on the temperature dependence of the chlorine effect and the oxidation kinetics of preoxidized Cl-implanted samples support the model of a selective Al-transport via AlCl. Furthermore, the influence of small additions (in the ppm range) of P, B, C and Br on the oxidation kinetics of g-TiAl-based alloys has been investigated. P, B and C implanted TiAl showed a different oxidation behaviour and oxide scale microstructure compared to Cl and Br microalloyed TiAl. Especially the P implanted sample revealed an extensive nitride formation connected with a breakaway oxidation after 100 h.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2027-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:8636-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Stephan, H.]]></dc:creator>
<dc:creator><![CDATA[Juran, S.]]></dc:creator>
<dc:creator><![CDATA[Walther, M.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Born, K.]]></dc:creator>
<dc:creator><![CDATA[Comba, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-8636-1</dc:identifier>
<dc:title><![CDATA[Synthesis, characterization and evaluation of novel chelating agents for copper radionuclides]]></dc:title>
<dc:source><![CDATA[7th International Symposium on Technetium in Chemistry and Nuclear Medicine, 06.-09.09.2006, Bressanone, Italy]]></dc:source>
<dc:date>2006</dc:date>
<dc:description><![CDATA[Three different hexadentate bispidine ligands L4  L6 have been prepared. Studies which have been performed to label these ligands with <SUP>67</SUP>Cu indicate a rapid formation of stable complexes under mild conditions (room temperature, aqueous solution). Challenge experiments of these complexes in the presence of a high excess of competing ligands such as glutathione, histidine and cyclam gave no evidence of radiocopper exchange. The <SUP>67</SUP>Cu complexes of the bispidine ligands investigated are also stable in rat plasma at least for 24 h.]]></dc:description>
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<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-8636-1</dc:relation>
<dc:audience>Researchers</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:8636-2</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Stephan, H.]]></dc:creator>
<dc:creator><![CDATA[Juran, S.]]></dc:creator>
<dc:creator><![CDATA[Walther, M.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Born, K.]]></dc:creator>
<dc:creator><![CDATA[Comba, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-8636-2</dc:identifier>
<dc:title><![CDATA[Synthesis, characterization and evaluation of novel chelating agents for copper radionuclides]]></dc:title>
<dc:source><![CDATA[U. Mazzi: Technetium, Rhenium and Other Metals in Chemistry and Nuclear Medicine, Padova: SGEditoriali, 2006, 88-89884-04-5, 219-222]]></dc:source>
<dc:date>2006</dc:date>
<dc:description><![CDATA[Three different hexadentate bispidine ligands L4  L6 have been prepared. Studies which have been performed to label these ligands with <SUP>67</SUP>Cu indicate a rapid formation of stable complexes under mild conditions (room temperature, aqueous solution). Challenge experiments of these complexes in the presence of a high excess of competing ligands such as glutathione, histidine and cyclam gave no evidence of radiocopper exchange. The <SUP>67</SUP>Cu complexes of the bispidine ligands investigated are also stable in rat plasma at least for 24 h.]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:bookPart</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-8636-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2125-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Teterin, Y. A.]]></dc:creator>
<dc:creator><![CDATA[Nefedov, V. I.]]></dc:creator>
<dc:creator><![CDATA[Lebedev, A. M.]]></dc:creator>
<dc:creator><![CDATA[Dementjev, A. P.]]></dc:creator>
<dc:creator><![CDATA[Utkin, I. O.]]></dc:creator>
<dc:creator><![CDATA[Teterin, A. Y.]]></dc:creator>
<dc:creator><![CDATA[Bubner, M.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2125-1</dc:identifier>
<dc:title><![CDATA[X-ray photoelectron spectroscopy investigation of the interaction of U(VI) and Fe(III) with natural humic acid in aqueous solutions]]></dc:title>
<dc:source><![CDATA[Journal für Praktische Chemie Vol. 341, Issue 8 (1999), pp. 773-777]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[X-ray photoelectron spectroscopy investigation of the interaction of U(VI) and Fe(III) with natural humic acid in aqueous solutions.
Dedicated to Prof. Dr. Egon Uhlig on the occasion of his 70th birthday.
Abstract
Complexes of U(VI) and Fe(III) with natural humic acid (NHA) were studied by X-ray photoelectron spectroscopy (XPS). It follows from the analysis of the uranium and iron concentrations at the surface and in the bulk of the humates that the reaction in solution is heterogeneous. The NHA reacts as a particle. In solutions containing either U(VI) or Fe(III), NHA reacts similar with Fe(III) and U(VI). However, in a mixed solution of Fe(III) and U(VI), NHA reacts predominantly with iron. In comparison to Fe(III) complexes, the complexes with U(VI) are formed mostly in the inner of the NHA particle. Therefore, the concentration ratio U/Fe as measured by XPS increases by powdering of the particles. Salts of Fe(III) can be used to inhibit the uranium migration in form of its soluble humates.



]]></dc:description>
<dc:subject><![CDATA[Keywords: Humic acid complexes]]></dc:subject>
<dc:subject><![CDATA[Uranyl complexes]]></dc:subject>
<dc:subject><![CDATA[Iron complexes]]></dc:subject>
<dc:subject><![CDATA[XPS of humates]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2125-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2126-1</identifier>
<datestamp>2025-04-17</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gallmeister, K.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Pavlenko, O.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2126-1</dc:identifier>
<dc:title><![CDATA[Is there a unique thermal source of dileptons in Pb(158 A · GeV) + Au, Pb reactions?]]></dc:title>
<dc:source><![CDATA[Physics Letters B 473 (2000) 20-24]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[An analysis of the dilepton measurements in the reactions Pb(158 A · GeV) + Au, Pb  points to a unique
thermal source contributing to the invariant mass and transverse momentum spectra. Effects of the flow pattern are discussed.]]></dc:description>
<dc:subject><![CDATA[dileptons]]></dc:subject>
<dc:subject><![CDATA[heavy-ion collisions]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0370-2693(99)01439-2]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2126-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:3538-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Stefani, F.]]></dc:creator>
<dc:creator><![CDATA[Gailitis, A.]]></dc:creator>
<dc:creator><![CDATA[Lielausis, O.]]></dc:creator>
<dc:creator><![CDATA[Platacis, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3538-1</dc:identifier>
<dc:title><![CDATA[Magnetic field self-excitation in the Riga dynamo experiment]]></dc:title>
<dc:source><![CDATA[ICTAM 2000, 20th Int. Congress of Theoretical and Applied Mechanics, Chicago, USA, 27.8.-2.9.2000]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The theory of magnetic field generation in cosmic bodies due to the homogeneous dynamo effect has been widely elaborated during the last decades. However, an experimental verification of this effect was still missing until recently. At the Riga dynamo facility, self-excitation of a magnetic field in a liquid metal flow has been observed for the first time in November 1999. For increasing rotation rate of the driving propeller, the amplification of an applied magnetic field has been measured. At the highest rotation rate of 2150 rpm, an exponentially increasing 1.3 Hz signal has been detected on the background of the amplified 1 Hz signal. Additionally, after switching off the excitation current at a slightly lower rotation rate, a slowly decreasing eigenmode was observed. The results are shown to correspond convincingly with numerical predictions.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-3538-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:3127-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Richter, H.]]></dc:creator>
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<dc:title><![CDATA[Untersuchungen zum Rißeinleitungsverhalten von Stahl unter schlagartiger Belastung mittels Schallemission]]></dc:title>
<dc:source><![CDATA[Deutsche Gesellschaft für Zerstötungsfreie Prüfung e. V., Statusberichte zur Entwicklung und Anwendung der Schallemissionsanalyse, 11. Kolloquium Schallemission, Jena, 6. - 7. 3. 1997, Berichtsband 58, S. 77]]></dc:source>
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<dc:description><![CDATA[Das kritische J-Integral J<sub>i</sub> ist als Zähigkeitsparameter zur Beschreibung der Einleitung des stabilen Rißwachstums (Initiierung) geeignet. Bei erhöhter Belastungsgeschwindigkeit erweist es sich jedoch als schwierig, die Initiierung zu detektieren und einem Punkt auf der Kraft-Durchbiegungs-Kurve zuzuordnen. In dieser Arbeit wird dieser Punkt mittels Schallemission (SE) bestimmt. Die Versuchstechnik zur Ermittlung von J<sub>i</sub> umfaßt ein Pendelschlagwerk mit hammerfinnenintegrierter Sonde zur schlagartigen und eine servohydraulische Prüfmaschine mit zusätzlicher Probeninstrumentierung zur dynamischen Belastung von ermüdungsangerissenen Kleinproben in ISO-V-Geometrie.
Es können verschiedene Arten von SE-Signalen beobachtet werden. Ein Signal korrespondiert mit der Rißinitiierung. Der Nachweis für die Initiierung bei Auftreten dieses Signals wird mit unterschiedlichen Mehrprobentechniken geführt.]]></dc:description>
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<dc:title><![CDATA[Untersuchungen zum Rißeinleitungsverhalten von Stahl unter schlagartiger Belastung mittels Schallemission]]></dc:title>
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Es können verschiedene Arten von SE-Signalen beobachtet werden. Ein Signal korrespondiert mit der Rißinitiierung. Der Nachweis für die Initiierung bei Auftreten dieses Signals wird mit unterschiedlichen Mehrprobentechniken geführt.]]></dc:description>
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<dc:creator><![CDATA[Schumacher, G.]]></dc:creator>
<dc:creator><![CDATA[Lang, C.]]></dc:creator>
<dc:creator><![CDATA[Schütze, M.]]></dc:creator>
<dc:creator><![CDATA[Hornauer, U.]]></dc:creator>
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<dc:title><![CDATA[Improvement of the Oxidation Resistance of gamma Titanium Aluminides by Microalloying with Chlorine using Ion Implantation]]></dc:title>
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<dc:description><![CDATA[High oxidation resistance of gamma titanium aluminides can be achieved by the formation of a continuous scale of slowly growing Al2O3. The formation of such a scale was stimulated by the addition of small amounts of chlorine. The additions were incorporated by ion implantation into the sample. The g-TiAl samples were oxidized at 1173 K in air for 100 h. Even if chlorine is present in very small quantities, it has a highly beneficial effect on the oxidation resistance (microalloying effect). The kinetics are changed from mixed TiO2/Al2O3- kinetics for unimplanted specimens to pure Al2O3- kinetics for chlorine implanted specimens.]]></dc:description>
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<dc:title><![CDATA[Cross-sectional micro-Raman Spectroscopy: a tool for structural investigations of thin polytypic SiC layers]]></dc:title>
<dc:source><![CDATA[Int. Conf. on Silicon Carbide, III-Nitrides and Related Materials, Stockholm, Sweden,
Aug. 31 - Sept. 5, 1997]]></dc:source>
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<dc:title><![CDATA[Cross-sectional micro-Raman Spectroscopy: a tool for structural investigations of thin polytypic SiC layers]]></dc:title>
<dc:source><![CDATA[Mat. Sci. Forum 264-268 (1998) 661]]></dc:source>
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<dc:creator><![CDATA[Wirth, H.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
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<dc:creator><![CDATA[Coleman, P. G.]]></dc:creator>
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<dc:title><![CDATA[Investigation of ion-implantation induced damage in 6H-SiC by RBS/C and PAS]]></dc:title>
<dc:source><![CDATA[Mat. Sci. Forum  264-268 (1998) 729]]></dc:source>
<dc:date>1998</dc:date>
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<dc:creator><![CDATA[Bonhaus, J.]]></dc:creator>
<dc:creator><![CDATA[Harlander, T.]]></dc:creator>
<dc:creator><![CDATA[Borchert, D.]]></dc:creator>
<dc:creator><![CDATA[Ecke, G.]]></dc:creator>
<dc:creator><![CDATA[Fontaine, F.]]></dc:creator>
<dc:creator><![CDATA[Fahrner, W. R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2195-2</dc:identifier>
<dc:title><![CDATA[High Sensitive Thermal Sensors in Heat Spreading Diamond for Industrial Application]]></dc:title>
<dc:source><![CDATA[IEEE International Symposium on Industrial Electronics, proceedings  vol. 1, 2 (1998) p. 157]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Bonhaus, J.]]></dc:creator>
<dc:creator><![CDATA[Harlander, T.]]></dc:creator>
<dc:creator><![CDATA[Borchert, D.]]></dc:creator>
<dc:creator><![CDATA[Ecke, G.]]></dc:creator>
<dc:creator><![CDATA[Fontaine, F.]]></dc:creator>
<dc:creator><![CDATA[Fahrner, W. R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2195-1</dc:identifier>
<dc:title><![CDATA[High Sensitive Thermal Sensors in Heat Spreading Diamond for Industrial Application]]></dc:title>
<dc:source><![CDATA[IEEE Int. Symp. on Industrial Electronics (ISIE `98) , Pretoria, South Africa, July 7 - 10, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2200-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Deshkovskaya, A. A.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2200-1</dc:identifier>
<dc:title><![CDATA[Einfluß der Ionenimplantation auf die Festigkeit von Quarzglas]]></dc:title>
<dc:source><![CDATA[28. Int. Konf. Physik der Wechselwirkung geladener Teilchen mit kristallinen Materialien, Moskau, May 25 - 27, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1792-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Ivanov, K.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Mittag, S.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1792-1</dc:identifier>
<dc:title><![CDATA[Comparative Study of a Boron Dilution Scenario in VVER Reactors]]></dc:title>
<dc:source><![CDATA[Specialist Meeting on Boron Dilution Reactivity Transients, State College, PA, USA, 18 - 20 October, 1995]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Subsequent studies have identified many scenarios which can lead to reactivity excursions due to boron dilution. The comparative study, presented in this paper, deals with the so-called "restart of the first reactor coolant pump" scenario and its reactor-dynamic consequences for the both VVER reactor types - VVER-440 and VVER-1000.
The transient simulations have been performed using the three-dimensional core dynamics code DYN3D. The DYN3D modeling features, including recent developments, as well as the cross-section generation methodology, involved in these calculations, are described. The analyzed accident scenario is outlined together with the assumptions made. The results of core response in this boron dilution accident for both VVER reactors have been compared within ranges, determined by the two reactivity values of interest: the criticaly limit and the reactivity initiated accident (RIA) limit.]]></dc:description>
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<identifier>HZDR:PUBLDB:2033-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Höhne, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2033-1</dc:identifier>
<dc:title><![CDATA[Coolant Mixing in Pressurized Water Reactors]]></dc:title>
<dc:source><![CDATA[AEA Technolgy, CFD, User Conference, Unterhaching, 19.-20.5. 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The three-dimensional flow distribution in the downcomer and the lower plenum of  PWR's was calculated with a computational fluid dynamics (CFD) code (CFX-4) and the results were presented at the conference]]></dc:description>
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<identifier>HZDR:PUBLDB:2033-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Höhne, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2033-7</dc:identifier>
<dc:title><![CDATA[Coolant Mixing in Pressurized Water Reactors]]></dc:title>
<dc:source><![CDATA[AEA Technolgy, CFD, User Conference, Unterhaching, 19.-20.5. 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The three-dimensional flow distribution in the downcomer and the lower plenum of  PWR's was calculated with a computational fluid dynamics (CFD) code (CFX-4) and the results were presented at the conference]]></dc:description>
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<identifier>HZDR:PUBLDB:14506-2</identifier>
<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Ferrari, A.]]></dc:creator>
<dc:creator><![CDATA[Cowan, T.]]></dc:creator>
<dc:creator><![CDATA[Margarone, D.]]></dc:creator>
<dc:creator><![CDATA[Prokupek, J.]]></dc:creator>
<dc:creator><![CDATA[Rus, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14506-2</dc:identifier>
<dc:title><![CDATA[Shielding assessment for the ELI high intensity laser beamline facility in Czech Republic]]></dc:title>
<dc:source><![CDATA[10th Conference of the Task Force on Shielding Aspects of Accelerators, Targets and Irradiation Facilities, SATIF-10, 02.-04.06.2010, Geneva, Switzerland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The production of laser-accelerated, high energy and high current particle beams requires a proper shielding assessment, especially when high intensity laser systems operate in repetition rate. The ELI (Extreme Light Infrastructure) future european facility in Czech Republic, where different optional laser beamlines are foreseen, will offer versatile electron and proton/ion sources, emitting in an unprecedented energy range (up to about 40 GeV for the electron case). For this facility a first extensive study that includes shielding and activation calculations for the 300 J laser beamline, which is the most critical for electron acceleration experiments, has been performed. Starting from analytical calculations, as well as from dedicated simulations, the main radiation fields produced in the laser-matter interaction have been defined. These fields have been then characterized as "source terms" in a full simulation with the Monte Carlo code FLUKA, where the produced secondary radiation has been studied to assess a proper shielding. The first results for the ELI shielding for the electron case, together with the activation calculations that drove several material solutions, are here presented and discussed.]]></dc:description>
<dc:subject><![CDATA[laser-accelerated electron and proton beams]]></dc:subject>
<dc:subject><![CDATA[shielding assessment]]></dc:subject>
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<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Ferrari, A.]]></dc:creator>
<dc:creator><![CDATA[Cowan, T.]]></dc:creator>
<dc:creator><![CDATA[Margarone, D.]]></dc:creator>
<dc:creator><![CDATA[Prokupek, J.]]></dc:creator>
<dc:creator><![CDATA[Rus, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14506-1</dc:identifier>
<dc:title><![CDATA[Shielding assessment for the ELI high intensity laser beamline facility in Czech Republic]]></dc:title>
<dc:source><![CDATA[10th Conference of the Task Force on Shielding Aspects of Accelerators, Targets and Irradiation Facilities, SATIF-10, 02.-04.10.2010, Geneva, Switzerland<br>Shielding Aspects of Accelerators, Targets and Irradiation Facilities - SATIF 10, Paris: OECD Nuclear Energy Agency Publications, 9789264096509 (PDF) ; 9789264034679 (print), 87-96]]></dc:source>
<dc:date>2011</dc:date>
<dc:description><![CDATA[The production of laser-accelerated, high energy and high current particle beams requires a proper shielding assessment, especially when high intensity laser systems operate in repetition rate. The ELI (Extreme Light Infrastructure) future european facility in Czech Republic, where different optional laser beamlines are foreseen, will offer versatile electron and proton/ion sources, emitting in an unprecedented energy range (up to about 40 GeV for the electron case). For this facility a first extensive study that includes shielding and activation calculations for the 300 J laser beamline, which is the most critical for electron acceleration experiments, has been performed. Starting from analytical calculations, as well as from dedicated simulations, the main radiation fields produced in the laser-matter interaction have been defined. These fields have been then characterized as "source terms" in a full simulation with the Monte Carlo code FLUKA, where the produced secondary radiation has been studied to assess a proper shielding. The first results for the ELI shielding for the electron case, together with the activation calculations that drove several material solutions, are here presented and discussed.]]></dc:description>
<dc:subject><![CDATA[laser-accelerated electron and proton beams]]></dc:subject>
<dc:subject><![CDATA[shielding assessment]]></dc:subject>
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<identifier>HZDR:PUBLDB:14510-1</identifier>
<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Beyer, M.]]></dc:creator>
<dc:creator><![CDATA[Schleicher, E.]]></dc:creator>
<dc:creator><![CDATA[Pietruske, H.]]></dc:creator>
<dc:creator><![CDATA[Seidel, T.]]></dc:creator>
<dc:creator><![CDATA[Szalinski, L.]]></dc:creator>
<dc:creator><![CDATA[Hampel, U.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14510-1</dc:identifier>
<dc:title><![CDATA[Status of the PTS Experiment at TOPFLOW]]></dc:title>
<dc:source><![CDATA[Steering Committee Meeting on R&D Cooperation between Forschungszentrum Dresden-Rossendorf and AREVA NP GmbH, 20.09.2010, Dresden, Deutschland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[After a short description of the aim and tasks of the project the experimental setup and the measurement technique were explained. Futhermore, the two executed air/water measurement series were specified. On the one hand, the behaviour of the flow through an Emergency Core Cooling (ECC) line into a Cold Leg of a Pressurized Water Reactor was investigated in dependence on some thermo hydraulic parameters. On the other hand, the occureance of thermal stratification inside the Cold Leg during ECC injection with different mass flows was analysed. An explanation of the next steps for the steam/water tests and an outlook completed the presentation.]]></dc:description>
<dc:subject><![CDATA[Pressurized Thermal Shock]]></dc:subject>
<dc:subject><![CDATA[Emergency Core Cooling]]></dc:subject>
<dc:subject><![CDATA[Pressurized Water Reactor]]></dc:subject>
<dc:subject><![CDATA[thermal stratification]]></dc:subject>
<dc:subject><![CDATA[mixing phenomena]]></dc:subject>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<identifier>HZDR:PUBLDB:176-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Brünig, D.]]></dc:creator>
<dc:creator><![CDATA[Naehring, F.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-176-1</dc:identifier>
<dc:title><![CDATA[Solare Brauchwasserbereitung und Einspeisung solarer Überschüsse in den Fernwärmerücklauf]]></dc:title>
<dc:source><![CDATA[Viertes Symposium Thermische Solarenergie, Staffelstein, 9.-10.6.1994, Tagungsband S. 241]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[In der Stadt Freital wird ein Modellvorhaben zur Integration solarer Warmwasserbereitung in ein neu geschaffenes Fernwärmesystem auf Erdgasbasis realisiert. Das Projekt beinhaltet den Bau einer solarthermischen Anlage mit einer Kollektorfläche von 100 m² auf einer Schule  und deren Einbindung in die im Keller der Schule errichtete Heizzentrale für das umliegende Wohngebiet. Mittels eines umfangreichen Meßprogramms werden die Ergebnisse erfaßt und analysiert.]]></dc:description>
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<identifier>HZDR:PUBLDB:176-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Brünig, D.]]></dc:creator>
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<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-176-7</dc:identifier>
<dc:title><![CDATA[Solare Brauchwasserbereitung und Einspeisung solarer Überschüsse in den Fernwärmerücklauf]]></dc:title>
<dc:source><![CDATA[Viertes Symposium Thermische Solarenergie, Staffelstein, 9.-10.6.1994, Tagungsband S. 241]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[In der Stadt Freital wird ein Modellvorhaben zur Integration solarer Warmwasserbereitung in ein neu geschaffenes Fernwärmesystem auf Erdgasbasis realisiert. Das Projekt beinhaltet den Bau einer solarthermischen Anlage mit einer Kollektorfläche von 100 m² auf einer Schule  und deren Einbindung in die im Keller der Schule errichtete Heizzentrale für das umliegende Wohngebiet. Mittels eines umfangreichen Meßprogramms werden die Ergebnisse erfaßt und analysiert.]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kögler, R.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:creator><![CDATA[Danilin, A. B.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3128-1</dc:identifier>
<dc:title><![CDATA[Defects remaining in MeV-ion-implanted and armealed Si away from the peak of the nuclear energy deposition profile]]></dc:title>
<dc:source><![CDATA[Nucl. Instr. Meth. B147 (1999) 96]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:creator><![CDATA[Zuhr, R. A.]]></dc:creator>
<dc:creator><![CDATA[Budai, J. D.]]></dc:creator>
<dc:creator><![CDATA[Datskos, P. G.]]></dc:creator>
<dc:creator><![CDATA[Meldrum, A.]]></dc:creator>
<dc:creator><![CDATA[Thomas, K. A.]]></dc:creator>
<dc:creator><![CDATA[Warmack, R. J.]]></dc:creator>
<dc:creator><![CDATA[White, C. W.]]></dc:creator>
<dc:creator><![CDATA[Feldman, L. C.]]></dc:creator>
<dc:creator><![CDATA[Strobel, M.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3130-1</dc:identifier>
<dc:title><![CDATA[Nanostructured arrays formed by finely focused ion beams]]></dc:title>
<dc:source><![CDATA[Mat. Res. Soc. Symp. Proc. 536 (1999) 251]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Antons, A.]]></dc:creator>
<dc:creator><![CDATA[Klinkhammer, F.]]></dc:creator>
<dc:creator><![CDATA[Kappius, L.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Trinkaus, H.]]></dc:creator>
<dc:creator><![CDATA[Mantl, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3131-1</dc:identifier>
<dc:title><![CDATA[Strukturierung von epitaktischen CoSi2/Si-Heterostrukturen durch lokale Oxidation]]></dc:title>
<dc:source><![CDATA[DPG-Frühjahrstagung des AK Festkörperphysik, Münster, March 22-26,1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1739-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Shatrov, V.]]></dc:creator>
<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1739-1</dc:identifier>
<dc:title><![CDATA[A numerical 3d stability analysis of the MHD cylinder wake flow]]></dc:title>
<dc:source><![CDATA[8th Beer-Sheva International Seminar on MHD flows and turbulence, Jerusalem, February 25 - 29, 1996, to appear in: Progress in Astronautics and Aeronautics, Ed.: Branover, H; Unger, Y; Washington]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[In the present paper the stability of the time-dependent, three-dimensional, incompressible flow around a circular cylinder exposed to an external magnetic field is investigated numerically. We perform a linear 3d stability analysis of the 2d flow being either steady or quasiperiodic as known from previous work. By monitoring the time evolution of the integral energy of the 3d disturbances in the computational domain we decide whether the flow is globally unstable or stable. The results are compared and validated with recent results for the purely hydrodynamic problem. We restrict the analysis to a magnetic field being aligned with the oncoming flow. For this case we numerically confirm the general result of Hunt that in the (Re, N)-plane parameter regions above the 2d-neutral stability curve exist where the flow is 3d-unstable but 2d stable (steady) because the magnetic field acts in a different way on 2d and 3d instabilities.]]></dc:description>
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<identifier>HZDR:PUBLDB:2133-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-2133-1</dc:identifier>
<dc:title><![CDATA[Institute of Radiochemistry, Report January 1998 - June 1999]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-272 September 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
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<identifier>HZDR:PUBLDB:2270-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prokert, F.]]></dc:creator>
<dc:creator><![CDATA[Betzl, M.]]></dc:creator>
<dc:creator><![CDATA[Eichhorn, F.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Schell, N.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2270-1</dc:identifier>
<dc:title><![CDATA[The Installations for Materials Research on ROBL at the ESRF]]></dc:title>
<dc:source><![CDATA[Jahrestagung DGK, Karlsruhe, März 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2141-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schmeide, K.]]></dc:creator>
<dc:creator><![CDATA[Zänker, H.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2141-1</dc:identifier>
<dc:title><![CDATA[Isolation and Characterization of Aquatic Humic Substances from the Bog 'Kleiner Kranichsee']]></dc:title>
<dc:source><![CDATA[FZKA 6124, Wissenschaftliche Berichte Forschungszentrum Karlsruhe, (G. Buckau, ed.). Karlsruhe 1998, p. 161.]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Surface water has been studied from the mountain bog 'Kleiner Kranichsee'. This bog is situated in the Johanngeorgenstadt area (Saxony/Germany) close to an abandoned uranium mine and mine tailing piles. The bog water contains about 130 mg/L of organics (primarily humic and fulvic acid). 
First, bog water colloids were determined for their particle size and size distribution using photon correlation spectroscopy (PCS) and scanning electron microscopy (SEM) in combination with size fractionation by filtration. Second, about 400 L of the bog water were processed in order to isolate aquatic humic substances. SupeliteTM DAX-8 (Supelco) was used as adsorption resin. The humic material was separated into humic and fulvic acids. A total of 14 g of humic acid and 10 g of fulvic acid were isolated. The humic substances were characterized in terms of their elemental composition, functional properties including proton exchange capacity, charge/size ratios and spectroscopic characteristics. The results were compared with data of a commercial humic acid from Aldrich.]]></dc:description>
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<identifier>HZDR:PUBLDB:1088-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1088-1</dc:identifier>
<dc:title><![CDATA[BRICK - ein Simulationstool für Mehrphasenströmungen in Behältern auf der Basis einer Partikelmethode]]></dc:title>
<dc:source><![CDATA[GVC-Jahrestagung '98, 30.9.-2.10.1998, Freiburg]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Im Rahmen der Entwicklung eines Gesamtmodells für die dynamische Simulation komplexer Druckentlastungssysteme bestehend aus Reaktor, Abblaseleitung, 
Entlastungsarmatur und Auffangeinrichtungen wurde ein 1-D-Behältermodell 
aufgestellt. Die Transportvorgänge im Behälter werden auf der Grundlage einer 
neu entwickelten Partikelmethode gelöst. Dadurch wird numerische Diffusion 
vermieden, was insbesondere bei der Berücksichtigung von Diskontinuitäten, wie 
z.B. dem Gemischspiegel, von Vorteil ist. Die implizite Wiedergabe der aktuellen Position des Gemischspiegels sowie ein spezielles Interface ermöglichen die 
Beachtung der Entwicklung einer Schaumkrone am Übergang zwischen dem 
Zweiphasengemisch und dem Gasraum. Die weitgehende Entkopplung der einzelnen 
Phänomene erlaubt eine modulare Codestruktur, bei der Modelle für 
Einzelphänomene leicht ausgetauscht werden können.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1088-2</identifier>
<datestamp>2023-05-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1088-2</dc:identifier>
<dc:title><![CDATA[BRICK - ein Simulationstool für Mehrphasenströmungen in Behältern auf der Basis einer Partikelmethode]]></dc:title>
<dc:source><![CDATA[Chemie-Ingenieur-Technik (70) 9198 pp. 1139]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Im Rahmen der Entwicklung eines Gesamtmodells für die dynamische Simulation komplexer Druckentlastungssysteme bestehend aus Reaktor, Abblaseleitung, 
Entlastungsarmatur und Auffangeinrichtungen wurde ein 1-D-Behältermodell 
aufgestellt. Die Transportvorgänge im Behälter werden auf der Grundlage einer 
neu entwickelten Partikelmethode gelöst. Dadurch wird numerische Diffusion 
vermieden, was insbesondere bei der Berücksichtigung von Diskontinuitäten, wie 
z.B. dem Gemischspiegel, von Vorteil ist. Die implizite Wiedergabe der aktuellen Position des Gemischspiegels sowie ein spezielles Interface ermöglichen die 
Beachtung der Entwicklung einer Schaumkrone am Übergang zwischen dem 
Zweiphasengemisch und dem Gasraum. Die weitgehende Entkopplung der einzelnen 
Phänomene erlaubt eine modulare Codestruktur, bei der Modelle für 
Einzelphänomene leicht ausgetauscht werden können.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1002/cite.3307009104]]></dc:relation>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:3147-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Bauer, R.]]></dc:creator>
<dc:creator><![CDATA[Walter, B.]]></dc:creator>
<dc:creator><![CDATA[Vorwieger, G.]]></dc:creator>
<dc:creator><![CDATA[Füchtner, F.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Will, E.]]></dc:creator>
<dc:creator><![CDATA[Linemann, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3147-1</dc:identifier>
<dc:title><![CDATA[The dopaminergic system is altered under neonatal asphyxia-studies with[<SUP>18</SUP>F]FDOPA.]]></dc:title>
<dc:source><![CDATA[Eur. J. Nucl. Med. 24 (1997) 1043.]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[There is evidence that the dopaminergic system is sensitive to asphyxia. However, the respective enzyme activities have not been measured in the living neonatal brain yet. In this study, FDOPA was used to estimate the activity of the aromatic amino acid decarboxylase (AADC) and the relative changes of monoamine oxidase (MAO) and catechol-o-methyl-transferase (COMT) in the neonatal pig brain. 
Two PET studies were performed under control conditions and under 2-hour asphyxia in each of 6 piglets and combined with measurements of cerebral blood flow (CBF) and volume (CBV). Plasma metabolites of FDOPA were also determined by HPLC.
As expected asphyxia elicited a 3-fold elevation  of the CBF and increased the CBV by 40%. The blood-brain transfer  of FDOPA, K<SUB>1</SUB>, and the clearance rate  constant from brain, k<SUB>2</SUB>, were unchanged. However, the rate of [F-18]fluoro-dopamine synthesis, k<SUB>3</SUB>, was increased in striatum from 0.038±0.016 min<SUP>-1</SUP> to 0.056±0.028 min<SUP>-1</SUP>. Also, the rate of conversion of FDOPA to 3-O-methyl-FDOPA (OMFD) by COMT in plasma decreased during asphyxia from 0.0080±0.0015 min<SUP>-1</SUP> to 0.0046±0.0010 min<SUP>-1</SUP>. Measurement of metabolites in tissue indicates that similar changes occurred also in the brain. Furthermore, the amount of FDOPAC as product of brain MAO activity was significantly decreased under asphyxia.
Increase of the extracellular level of dopamine is expected to be involved in severe disturbances of neuronal metabolism during asphyxia, e.g. by generating free radicals and quinones. In this study, evidence for an increase of the AADC activity and a decrease of MAO activity during asphyxia was obtained which may contribute to the  increase of extracellular dopamine. 
]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Bauer, R.]]></dc:creator>
<dc:creator><![CDATA[Walter, B.]]></dc:creator>
<dc:creator><![CDATA[Vorwieger, G.]]></dc:creator>
<dc:creator><![CDATA[Füchtner, F.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Will, E.]]></dc:creator>
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<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
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<dc:title><![CDATA[The dopaminergic system is altered under neonatal asphyxia-studies with[<SUP>18</SUP>F]FDOPA.]]></dc:title>
<dc:source><![CDATA[Congress of the European Association of Nuclear Medicine, Glasgow, Scottland, 23.-27.8.1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[There is evidence that the dopaminergic system is sensitive to asphyxia. However, the respective enzyme activities have not been measured in the living neonatal brain yet. In this study, FDOPA was used to estimate the activity of the aromatic amino acid decarboxylase (AADC) and the relative changes of monoamine oxidase (MAO) and catechol-o-methyl-transferase (COMT) in the neonatal pig brain. 
Two PET studies were performed under control conditions and under 2-hour asphyxia in each of 6 piglets and combined with measurements of cerebral blood flow (CBF) and volume (CBV). Plasma metabolites of FDOPA were also determined by HPLC.
As expected asphyxia elicited a 3-fold elevation  of the CBF and increased the CBV by 40%. The blood-brain transfer  of FDOPA, K<SUB>1</SUB>, and the clearance rate  constant from brain, k<SUB>2</SUB>, were unchanged. However, the rate of [F-18]fluoro-dopamine synthesis, k<SUB>3</SUB>, was increased in striatum from 0.038±0.016 min<SUP>-1</SUP> to 0.056±0.028 min<SUP>-1</SUP>. Also, the rate of conversion of FDOPA to 3-O-methyl-FDOPA (OMFD) by COMT in plasma decreased during asphyxia from 0.0080±0.0015 min<SUP>-1</SUP> to 0.0046±0.0010 min<SUP>-1</SUP>. Measurement of metabolites in tissue indicates that similar changes occurred also in the brain. Furthermore, the amount of FDOPAC as product of brain MAO activity was significantly decreased under asphyxia.
Increase of the extracellular level of dopamine is expected to be involved in severe disturbances of neuronal metabolism during asphyxia, e.g. by generating free radicals and quinones. In this study, evidence for an increase of the AADC activity and a decrease of MAO activity during asphyxia was obtained which may contribute to the  increase of extracellular dopamine. 
]]></dc:description>
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<dc:identifier>https://www.hzdr.de/publications/Publ-14298-1</dc:identifier>
<dc:title><![CDATA[Cyclin-Dependent Kinase 4/6 (Cdk4/6) Inhibitors: Perspectives in Cancer Therapy and Imaging]]></dc:title>
<dc:source><![CDATA[Mini-Reviews in Medicinal Chemistry 10(2010), 527-539]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Cyclin-dependent kinases 4 and 6 (Cdk4/6) are important components of cell cycle activation and control in early G<SUB>1</SUB> phase. Both enzymes and their regulators, e.g., cyclins, play critical roles in embryogenesis, homeostasis, and cancerogenesis. Cdk4/6 are attractive targets for cancer treatment. Recently, numerous selective small molecule inhibitors of Cdk4/6 have been developed. The potential of Cdk4/6 inhibitors, particularly, pyrido[2,3-d]pyrimidine derivatives, as both anti-cancer drugs and <SUP>124</SUP>I- and <SUP>18</SUP>F-radiolabeled tracers for cancer imaging using positron emission tomography is discussed.]]></dc:description>
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<dc:creator><![CDATA[Fridman, E.]]></dc:creator>
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<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14335-2</dc:identifier>
<dc:title><![CDATA[Preliminary analysis of HTGR core with DYN3D nodal diffusion code]]></dc:title>
<dc:source><![CDATA[5th International Topical Meeting on High Temperature Reactor Technology, 18.-20.10.2010, Czech Republic, Prague]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[DYN3D is an advanced nodal code for the three-dimensional steady-state and transient analysis of LWR cores with quadratic and hexagonal fuel assemblies. Although a new version of DYN3D for the simulation of block type High Temperature Gas cooled Reactors (HTGR) is currently under development, the main objective of this work is to demonstrate the applicability of the standard DYN3D version for the steady-state analysis of HTGR core. A preliminary reactor physic analysis procedure in which few group cross section sets are generated using HELIOS 1.9 transport lattice code and full core calculations are performed by DYN3D will be established. The Reactivity equivalent Physical Transformation (RPT) approach will be applied in order to eliminate the double-heterogeneity of HTGR fuel elements in HELIOS calculations. The full core analysis of the reference simplified HTGR core will be performed with DYN3D using macroscopic nodal cross sections provided by HELIOS. At this stage thermo-hydraulic feedback is not considered. The results of DYN3D calculations such as neutron multiplication factor, radial and axial power distribution, will be compared with those obtained from reference full core MCNP simulation.]]></dc:description>
<dc:subject><![CDATA[HTGR full core analysis]]></dc:subject>
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<dc:creator><![CDATA[Fridman, E.]]></dc:creator>
<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14335-1</dc:identifier>
<dc:title><![CDATA[Preliminary analysis of HTGR core with DYN3D nodal diffusion code]]></dc:title>
<dc:source><![CDATA[5th International Topical Meeting on High Temperature Reactor Technology, 18.-20.10.2010, Prague, Czech Republic<br>Preliminary analysis of HTGR core with DYN3D nodal diffusion code]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[DYN3D is an advanced nodal code for the three-dimensional steady-state and transient analysis of LWR cores with quadratic and hexagonal fuel assemblies. Although a new version of DYN3D for the simulation of block type High Temperature Gas cooled Reactors (HTGR) is currently under development, the main objective of this work is to demonstrate the applicability of the standard DYN3D version for the steady-state analysis of HTGR core. A preliminary reactor physic analysis procedure in which few group cross section sets are generated using HELIOS 1.9 transport lattice code and full core calculations are performed by DYN3D will be established. The Reactivity equivalent Physical Transformation (RPT) approach will be applied in order to eliminate the double-heterogeneity of HTGR fuel elements in HELIOS calculations. The full core analysis of the reference simplified HTGR core will be performed with DYN3D using macroscopic nodal cross sections provided by HELIOS. At this stage thermo-hydraulic feedback is not considered. The results of DYN3D calculations such as neutron multiplication factor, radial and axial power distribution, will be compared with those obtained from reference full core MCNP simulation.]]></dc:description>
<dc:subject><![CDATA[HTGR full core analysis]]></dc:subject>
<dc:subject><![CDATA[DYN3D]]></dc:subject>
<dc:subject><![CDATA[MCNP]]></dc:subject>
<dc:subject><![CDATA[HELIOS]]></dc:subject>
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<dc:title><![CDATA[High-frequency and high-field ESR in quantum spin systems]]></dc:title>
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<dc:title><![CDATA[ROBL - ein Strahlrohr für Radiochemie und Materialforschung an der ESRF]]></dc:title>
<dc:source><![CDATA[Gemeinsames Statusseminar im Kloster Seeon, Sept. 14 - 17, 1997]]></dc:source>
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<dc:creator><![CDATA[Mazur, K.]]></dc:creator>
<dc:creator><![CDATA[Sass, J.]]></dc:creator>
<dc:creator><![CDATA[Eichhorn, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2426-1</dc:identifier>
<dc:title><![CDATA[X-ray high resolution diffraction and reflectivity studies of the mechanical treatment related defects in opi-ready wafers]]></dc:title>
<dc:source><![CDATA[3th Autumn School on "X-ray scattering from surfaces and thin layers", Smolenice, Slovakia, Oct. 1 - 4, 1997]]></dc:source>
<dc:date>1997</dc:date>
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<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2427-2</dc:identifier>
<dc:title><![CDATA[Physik und Anwendungen der Plasma-Immersions-Ionenimplantation]]></dc:title>
<dc:source><![CDATA[Elektrotechnisches Kolloquium der Univ. Stuttgart, Jan. 23, 1997]]></dc:source>
<dc:date>1997</dc:date>
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<dc:creator><![CDATA[Möller, W.]]></dc:creator>
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<dc:title><![CDATA[Physik und Anwendungen der Plasma-Immersions-Ionenimplantation]]></dc:title>
<dc:source><![CDATA[VDE/ITG-Seminar "Teilchenstrahl- und Plasmatechnik", Helmsdorf b. Dresden, March 7, 1997 (invited lecture)]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2428-1</dc:identifier>
<dc:title><![CDATA[Basic aspects and applications of plasma immersion ion implantation]]></dc:title>
<dc:source><![CDATA[German-Japanese Seminar "Physics and Application of Low-Pressure Plasmas", Bad Honnef, June 18, 1997 (invited lecture)]]></dc:source>
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<identifier>HZDR:PUBLDB:2429-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2429-1</dc:identifier>
<dc:title><![CDATA[Ionenstrahlen zur Modifizierung und Analyse von Oberflächen]]></dc:title>
<dc:source><![CDATA[GDCh-Tagung "Oberflächenanalytik", Chemnitz, June 25, 1997 (invited lecture)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2397-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Reiss, S.]]></dc:creator>
<dc:creator><![CDATA[Strobel, M.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2397-1</dc:identifier>
<dc:title><![CDATA[Ionenstrahlsynthese von Nanoclustern und Schichten: Kinetik von Keimbildung, Wachstum und Ostwald-Reifen]]></dc:title>
<dc:source><![CDATA[Frühjahrstagung der DPG, Münster, Germany, March 17-21, 1997  (invited lecture)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:714-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Büscher, M.]]></dc:creator>
<dc:creator><![CDATA[Eßer, R.]]></dc:creator>
<dc:creator><![CDATA[Franzen, A.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:creator><![CDATA[Müller, H.]]></dc:creator>
<dc:creator><![CDATA[Prietzschtk, B.]]></dc:creator>
<dc:creator><![CDATA[Rimarzig, B.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:creator><![CDATA[Akindinov, A.]]></dc:creator>
<dc:creator><![CDATA[Chumakov, M.]]></dc:creator>
<dc:creator><![CDATA[Demechin, V.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:creator><![CDATA[Sibirtsev, A.]]></dc:creator>
<dc:creator><![CDATA[Kruglov, V.]]></dc:creator>
<dc:creator><![CDATA[Petrus, A.]]></dc:creator>
<dc:creator><![CDATA[Koptev, V.]]></dc:creator>
<dc:creator><![CDATA[Mikirtychyants, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-714-1</dc:identifier>
<dc:title><![CDATA[K<SUP>+</SUP> -meson production in <i>p</i>Be interactions at T<SUB>p</SUB> = 2.9 GeV]]></dc:title>
<dc:source><![CDATA[Zeitschrift für Physik A 355 (1996) pp. 93-100]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The production of K<SUP>+</SUP> and π<SUP>+</SUP> mesons and protons in <i>p</i>Be collisions at T<sub><i>p</i></sub>=2.9 GeV has been studied at the ITEP proton synchrotron. Ejectiles with a momentum of <i>p</i>=545 MeV/c were observed under an emission angle theta=17°. The detectors which have been developed for the identification of kaons out of a six orders of magnitude more intense background of pions and protons are described. A cross-section ration d<sup>2</sup>σ<sub>K<sup>+</sup></sub>/dωd<i>p</i>: d<sup>2</sup>σ<sub>π<sup>+</sup></sub>/dωd<i>p</i>: d<sup>2</sup>σ<sub><i>p</i><sup>+</sup></sub>/dωd<i>p</i> of (1±0.34):(85±1):(31±1) has been measured. Normalization with existing pion data yields an invariant differential cross section <i>E</i>∙d<sup>3</sup>σ<sub>K<sup>+</sup></sub>/d<sup>3</sup><i>p</i>=(3.1±1.2) mb GeV<sup>-2</sup>c<sup>3</sup>sr<sup>-1</sup> and a total cross section of σ<sub>tot</sub>(<i>p</i>Be) =(3.7±1.5) mb. These cross sections are compared with existing data and theoretical predictions. The A dependence of K<sup>+</sup> production in the few-GeV range is analyzed.]]></dc:description>
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<identifier>HZDR:PUBLDB:3119-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3119-1</dc:identifier>
<dc:title><![CDATA[Ion beam synthesis of semiconductor nanoclusters for opto- and microelectronics applications]]></dc:title>
<dc:source><![CDATA[in: Advances in Solid State Physics 39, pp. 171-181, ed. by B. Kramer, Vieweg-Verlag Braunschweig/Wiesbaden 1999]]></dc:source>
<dc:date>1999</dc:date>
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<header>
<identifier>HZDR:PUBLDB:3120-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3120-1</dc:identifier>
<dc:title><![CDATA[Measurements and CFX-simulations of a bubbly flow in a vertical pipe]]></dc:title>
<dc:source><![CDATA[3rd Int. Conf. on Advances in Fluid Mechanics, Montreal May 2000; in: M. Rahman, C.A. Brebbia (Ed.): Advances in Fluid Mechanics III, pp. 23-31, WITPress Southampton, Boston 2000, ISBN 1-85312-813-9]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[In the Forschungszentrum Rossendorf a measurements techniques test loop was constructed. Air water flow in a vertical tube was investigated using different two phase flow measuring techniques. Air was injected into an upward water flow at normally conditions applying different injection modes. Different tests with different relations of air and water superficial velocity were performed. For each test stationary conditions were settled. The paper describes the measuring techniques used and some experiments performed. Applying a wire mesh sensor, developed in FZR, the cross section of the void fraction could be determined. The time resolution achieved by the signal processing unit is 1024 frames per second. The spatial resolution equals 3 mm. At the investigated flow velocities, the bubble diameter distributions could be determined. Using the code CFX-4.2, void profiles over the tube cross section were calculated. The development of the void profiles is mainly influenced by bubble forces, which act perpendicular to the flow direction. Therefore the comparison of the calculated with the measured results for bubble flow regimes is a good validity test for the implemented two phase flow models. The two phase models of the code version CFX-4.2 are able to describe void profiles with a near wall void maximum, which will be found for bubbly flow showing a monodisperse bubble size distribution. To model flow regimes showing a bubble size distribution and the occurrence of bubble coalescence and diffraction, model extensions would be necessary. The consideration of larger bubbles, which may be deformed, requires the development of improved bubble force models.]]></dc:description>
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<identifier>HZDR:PUBLDB:3120-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3120-7</dc:identifier>
<dc:title><![CDATA[Measurements and CFX-simulations of a bubbly flow in a vertical pipe]]></dc:title>
<dc:source><![CDATA[3rd Int. Conf. on Advances in Fluid Mechanics, Montreal May 2000; in: M. Rahman, C.A. Brebbia (Ed.): Advances in Fluid Mechanics III, pp. 23-31, WITPress Southampton, Boston 2000, ISBN 1-85312-813-9]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[In the Forschungszentrum Rossendorf a measurements techniques test loop was constructed. Air water flow in a vertical tube was investigated using different two phase flow measuring techniques. Air was injected into an upward water flow at normally conditions applying different injection modes. Different tests with different relations of air and water superficial velocity were performed. For each test stationary conditions were settled. The paper describes the measuring techniques used and some experiments performed. Applying a wire mesh sensor, developed in FZR, the cross section of the void fraction could be determined. The time resolution achieved by the signal processing unit is 1024 frames per second. The spatial resolution equals 3 mm. At the investigated flow velocities, the bubble diameter distributions could be determined. Using the code CFX-4.2, void profiles over the tube cross section were calculated. The development of the void profiles is mainly influenced by bubble forces, which act perpendicular to the flow direction. Therefore the comparison of the calculated with the measured results for bubble flow regimes is a good validity test for the implemented two phase flow models. The two phase models of the code version CFX-4.2 are able to describe void profiles with a near wall void maximum, which will be found for bubbly flow showing a monodisperse bubble size distribution. To model flow regimes showing a bubble size distribution and the occurrence of bubble coalescence and diffraction, model extensions would be necessary. The consideration of larger bubbles, which may be deformed, requires the development of improved bubble force models.]]></dc:description>
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<identifier>HZDR:PUBLDB:1191-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Nebelung, C.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:creator><![CDATA[Henniger, J.]]></dc:creator>
<dc:creator><![CDATA[Mann, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1191-1</dc:identifier>
<dc:title><![CDATA[Vergleich von berechneten und gemessenen Alpha-Spektren von extrem dünnen Betonmeßpräparaten zur Freigabeentscheidung]]></dc:title>
<dc:source><![CDATA[Vortragstagung der GDCh-Fachgruppe Nuklearchemie 7.-9.9.1998, Dresden, Germany]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2037-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2037-1</dc:identifier>
<dc:title><![CDATA[Coupling of the Thermohydraulic Code ATHLET with the Neutron Kinetic Core Model DYN3D]]></dc:title>
<dc:source><![CDATA[International Conference "Thermophysical Aspects of WWER-Type
Reactor Safety", Obninsk, Russia, 21. - 24. November 1995]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2037-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2037-2</dc:identifier>
<dc:title><![CDATA[Coupling of the Thermohydraulic Code ATHLET with the Neutron Kinetic Core Model DYN3D]]></dc:title>
<dc:source><![CDATA[International Conference "Thermophysical Aspects of WWER-Type Reactor Safety", Obninsk, Russia, 21. - 24. November 1995, Proc. Vol. 2, pp. 155 - 164]]></dc:source>
<dc:date>1995</dc:date>
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<identifier>HZDR:PUBLDB:2020-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2020-1</dc:identifier>
<dc:title><![CDATA[Erste Nachrechnungen von Druckentlastungsexperimenten bei durchgehender Reaktion mit dem Programm BRICK]]></dc:title>
<dc:source><![CDATA[47. Sitzung des DECHEMA/GVC-Arbeitsausschuß "Sicherheitsgerechtes Auslegen von Chemieapparaten", Frankfurt am Main, 9./10. März 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Die Nachrechnungen von Druckentlastungsexperimenten bei durchgehender Reaktion dienen Validierung des Computerprogramms BRICK. Dafür stehen experimentelle Daten der Inburex GmbH Hamm (Kalorimeterversuche), des Wilhelm-Jost-Instituts Hamm (Entlastung eines 280 l Reaktors) sowie eigene kleinmaßstäbliche Experimente (Entlastung eines 1,95 l Reaktors) zur Verfügung. Als Reaktionssysteme wurden die Methanol/Essigsäureanhydridveresterung (verdampfendes System), die Ammoniumperoxodisulfatzersetzung (gasbildendes System) und Wasserstoffperoxidzersetzung (sowohl gasbildend als auch verdampfend) genutzt. Die Übereinstimmung zwischen den Rechnungen und den experimentellen Daten ist gut. Einen wesentlichen Unsicherheitsfaktor stellen die Wärmeströme über die Behälterwand vor. Daher sollten insbesondere die Korrelationen für die Wärmeübergänge sowohl für die Behälterinnenwand als auch an der Außenwand erweitert und ergänzt werden. ]]></dc:description>
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<identifier>HZDR:PUBLDB:1735-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Mittag, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1735-1</dc:identifier>
<dc:title><![CDATA[Burnup and Rod Worth Calculations for Paks-2 Using the Code DYN3D with two Different Group Data Libraries]]></dc:title>
<dc:source><![CDATA[Proc. of the 6th Symposium of AER, Kirkkonummi (Finland), 23 - 26 September 1996, p. 499]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The AER benchmark problem defined by L. Korpas et al. for the calculation of VVER­440 control rod worth was solved by using the code DYN3D in 1994. The KAB MAGRU library, generated by the NESSEL code was used then as a source of macroscopic group data. Now DYN3D calculations have been repeated with a new group data library created in EGP Prague by the KASSETA code.  Burnup calculations have been carried out for the cycles 4 to 7 of Paks­2 NPP. The critical boron concentrations as a function of time, calculated with both data libraries, were compared to the values measured in the progress of the cycles. The results are in good agreement.   The comparison of the fuel­element averaged burnup values after calculating 4 full cycles shows a maximum deviation of about 2 percent between the two data libraries. Concerning the control rod efficiencies the relative deviation is  higher. This is due to relatively great differences in the macroscopic group data produced for the control rod!
s by NESSEL and KASSETA.  The deviations between results calculated by the same code with different group data indicate that using different data libraries by the AER benchmark participants may be a main reason for the high differences between their results.

]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Alberto, R.]]></dc:creator>
<dc:creator><![CDATA[Schibli, R.]]></dc:creator>
<dc:creator><![CDATA[Schubiger, P. A.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2073-1</dc:identifier>
<dc:title><![CDATA[First Application of <I>f</I><I>ac</I>-[<SUP>99m</SUP>Tc(OH<SUB>2</SUB>)<SUB>3</SUB>(CO)<SUB>3</SUB>]<SUP>+</SUP> in Bioorganometallic Chemistry: Design, Structure, and in Vitro Affinity of a 5-HT<SUB>1A</SUB> Receptor Ligand Labeled with <SUP>99m</SUP>Tc]]></dc:title>
<dc:source><![CDATA[J. Am. Chem. Soc. 121, 25, 1999, 6076-6077]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Bioorganometallic chemistry comprises the combination of an organometallic transition metal complex and a targeting biomolecule. If ever such a combination should be applied, the synthesis has to be convenient, fast and requires one or two steps only. [<SUP>99m</SUP>Tc(OH<SUB>2</SUB>)<SUB>3</SUB>(CO)<SUB>3</SUB>]<SUP>+</SUP> 1 can be prepared in one step from [<SUP>99m</SUP>TcO<SUB>4</SUB>]<SUP>-</SUP> in saline and bidentate aromatic amines are very efficient chelators for this organometallic precursor. Consequently, we have derivatized a 5-HT<SUB>1A</SUB> (serotonergic) receptor ligand with high affinity and high selectivity for this subclass from the group of the arylpiperazines with a Schiff Base type chelator. In water, 1 radiolabels the receptor ligand in high yield and specific activity.]]></dc:description>
<dc:subject><![CDATA[Technetium]]></dc:subject>
<dc:subject><![CDATA[serotonin receptor]]></dc:subject>
<dc:subject><![CDATA[5-HT<SUB>1A</SUB>]]></dc:subject>
<dc:subject><![CDATA[Tc carbonyl complexes]]></dc:subject>
<dc:subject><![CDATA[bioorganometallic chemistry]]></dc:subject>
<dc:subject><![CDATA[schiff base]]></dc:subject>
<dc:subject><![CDATA[radio labelling]]></dc:subject>
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<identifier>HZDR:PUBLDB:1248-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Neumann, J.]]></dc:creator>
<dc:creator><![CDATA[Schlüter, S.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Tefera, N.]]></dc:creator>
<dc:creator><![CDATA[Vorst, K.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1248-1</dc:identifier>
<dc:title><![CDATA[Identifying Dangerous States in Chemical Plants Using Neural Networks]]></dc:title>
<dc:source><![CDATA[Proc. of the 6th European Congress on Intelligent Techniques and Soft Computing EUFIT '98 Aachen, Sept. 7-10, 1998, pp. 1237-1242]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[This paper describes the application of three-layer perceptron networks to the identification and diagnosis of dangerous states in strongly exothermic semibatch reactions. To assess the potential danger of different faults, separate perceptron networks were used for danger assessment and for fault isolation. Results are presented to illustrate the performance of the neural-network approach on real process data obtained from typical faults of a catalytic esterification process which were simulated in a laboratory reactor.]]></dc:description>
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<identifier>HZDR:PUBLDB:1248-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Neumann, J.]]></dc:creator>
<dc:creator><![CDATA[Schlüter, S.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Tefera, N.]]></dc:creator>
<dc:creator><![CDATA[Vorst, K.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1248-7</dc:identifier>
<dc:title><![CDATA[Identifying Dangerous States in Chemical Plants Using Neural Networks]]></dc:title>
<dc:source><![CDATA[Proc. of the 6th European Congress on Intelligent Techniques and Soft Computing EUFIT '98 Aachen, Sept. 7-10, 1998, pp. 1237-1242]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[This paper describes the application of three-layer perceptron networks to the identification and diagnosis of dangerous states in strongly exothermic semibatch reactions. To assess the potential danger of different faults, separate perceptron networks were used for danger assessment and for fault isolation. Results are presented to illustrate the performance of the neural-network approach on real process data obtained from typical faults of a catalytic esterification process which were simulated in a laboratory reactor.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2343-2</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Romano-Rodriguez, A.]]></dc:creator>
<dc:creator><![CDATA[Perez-Rodriguez, A.]]></dc:creator>
<dc:creator><![CDATA[Serre, C.]]></dc:creator>
<dc:creator><![CDATA[Calvo-Barrio, L.]]></dc:creator>
<dc:creator><![CDATA[Bachrouri, A.]]></dc:creator>
<dc:creator><![CDATA[Gonzalez-Varona, O.]]></dc:creator>
<dc:creator><![CDATA[Morante, J. R.]]></dc:creator>
<dc:creator><![CDATA[Kögler, R.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2343-2</dc:identifier>
<dc:title><![CDATA[TEM characterization of carbon ion implantation into epitaxial Si<SUB>1-x</SUB>Ge<SUB>x</SUB>]]></dc:title>
<dc:source><![CDATA[Int. Conf. on Microscopy of Semiconducting Materials, Oxford, England, April 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2343-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Romano-Rodriguez, A.]]></dc:creator>
<dc:creator><![CDATA[Perez-Rodriguez, A.]]></dc:creator>
<dc:creator><![CDATA[Serre, C.]]></dc:creator>
<dc:creator><![CDATA[Calvo-Barrio, L.]]></dc:creator>
<dc:creator><![CDATA[Bachrouri, A.]]></dc:creator>
<dc:creator><![CDATA[Gonzalez-Varona, O.]]></dc:creator>
<dc:creator><![CDATA[Morante, J. R.]]></dc:creator>
<dc:creator><![CDATA[Kögler, R.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2343-1</dc:identifier>
<dc:title><![CDATA[TEM characterization of carbon ion implantation into epitaxial Si<SUB>1-x</SUB>Ge<SUB>x</SUB>]]></dc:title>
<dc:source><![CDATA[Inst. Phys. Conf. Ser. 157 (1997) 419]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2208-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Fichtner, P.]]></dc:creator>
<dc:creator><![CDATA[Kaschny, J. R.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2208-1</dc:identifier>
<dc:title><![CDATA[Temperature effect on the morphology of helium bubble clusters in silicon]]></dc:title>
<dc:source><![CDATA[14th Int. Conf. On Electron Microscopy, Cancum, Mexico, Aug. 31-Sept.5, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2075-1</identifier>
<datestamp>2025-12-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Hausmann, S.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Hobert, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2075-1</dc:identifier>
<dc:title><![CDATA[Micro-Raman and Ion Channeling Study of Crystal Damage in Si Induced by Focused Ion Beam Co Implantation]]></dc:title>
<dc:source><![CDATA[Applied Physics A 71 (2000) 175-180]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The lattice damage of silicon produced by ion implantation at extremely high  current  density of 0.8 A/cm<SUP>2</SUP> (2.5 x 10<SUP>18</SUP> cm<SUP>-2</SUP> s<SUP>-1</SUP>) was investigated.  In a focused ion beam system, implantation  was carried out with  70 keV Co ions, fluences of 1.2 x 10<SUP>16</SUP> cm<SUP>-2</SUP> and 6.7 x 10<SUP>15</SUP> cm<SUP>-2</SUP> into Si (111) at room temperature and elevated temperatures between 355 °C and 400 °C. Radiation damage measurements were performed by Rutherford backscattering/channeling spectroscopy and micro-Raman analysis. The radiation damage was studied as a function of pixel dwell-time and implantation temperature. The critical temperature for amorphization  increases with current density. Although the fluence of the focused ion implantation was constant, crystalline layers were obtained for short and amorphous layers for long pixel dwell-times. The critical dwell-time of crystalline/amorphous transition increases with implantation temperature. From the results a typical time for defect annealing of 10<SUP>-5</SUP> s at 400 °C and an activation energy of (2.5±0.6) eV were deduced.]]></dc:description>
<dc:subject><![CDATA[focused ion beam]]></dc:subject>
<dc:subject><![CDATA[ion implantation]]></dc:subject>
<dc:subject><![CDATA[radiation damage]]></dc:subject>
<dc:subject><![CDATA[micro-Raman spectroscopy]]></dc:subject>
<dc:subject><![CDATA[ion channeling analysis]]></dc:subject>
<dc:subject><![CDATA[cobalt implantation]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1007/PL00021115]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:2076-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Hensel, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2076-1</dc:identifier>
<dc:title><![CDATA[Investigation of a Density Measurement Technique using Positron Radiation]]></dc:title>
<dc:source><![CDATA[4th Topical Meeting on Industrial Radiation and Radioisotope Measurements and Applications, October 3-7 1999, Raleigh (USA). ISBN 0-89448-646-2, 9]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The paper describes a density measurement technique using positron radiation. The method is appropriate for the determination of densities ranging from 10 kg/m3 to 100 kg/m3, e.g. for determining the density of foams or the humidity of pressurized gases. The focus of this paper is on the results obtained with an optimized low cost detector geometry. The technique makes use of the positron ranges in the measured matter, which is depending on its density. ]]></dc:description>
<dc:subject><![CDATA[density measurement]]></dc:subject>
<dc:subject><![CDATA[positron]]></dc:subject>
<dc:subject><![CDATA[positron annihilation]]></dc:subject>
<dc:subject><![CDATA[BGO]]></dc:subject>
<dc:subject><![CDATA[coincidence measurement]]></dc:subject>
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<identifier>HZDR:PUBLDB:2076-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Hensel, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2076-2</dc:identifier>
<dc:title><![CDATA[Investigation of a Density Measurement Technique using Positron Radiation]]></dc:title>
<dc:source><![CDATA[Applied Radiation and Isotopes 53 (2000) 617-624]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The paper describes a density measurement technique using positron radiation. The method is appropriate for the determination of densities ranging from 10 kg/m3 to 100 kg/m3, e.g. for determining the density of foams or the humidity of pressurized gases. The focus of this paper is on the results obtained with an optimized low cost detector geometry. The technique makes use of the positron ranges in the measured matter, which is depending on its density. ]]></dc:description>
<dc:subject><![CDATA[density measurement]]></dc:subject>
<dc:subject><![CDATA[positron]]></dc:subject>
<dc:subject><![CDATA[positron annihilation]]></dc:subject>
<dc:subject><![CDATA[BGO]]></dc:subject>
<dc:subject><![CDATA[coincidence measurement]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<identifier>HZDR:PUBLDB:2143-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-2143-1</dc:identifier>
<dc:title><![CDATA[Institute of Safety Research; Annual Report 1998]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-268 Juli 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The report gives an overview on the scientific work of the Institute of Safety Research in 1998.]]></dc:description>
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<identifier>HZDR:PUBLDB:2145-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Assmann, W.]]></dc:creator>
<dc:creator><![CDATA[Dobler, M.]]></dc:creator>
<dc:creator><![CDATA[Avasthi, D. K.]]></dc:creator>
<dc:creator><![CDATA[Kruijer, S.]]></dc:creator>
<dc:creator><![CDATA[Mieskes, H. D.]]></dc:creator>
<dc:creator><![CDATA[Nolte, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2145-1</dc:identifier>
<dc:title><![CDATA[Swift heavy ion induced formation of aplha-FeSi<SUB>2</SUB>]]></dc:title>
<dc:source><![CDATA[Nucl. Instr. Meth. B 146 (1998) 271]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2146-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Barth, K. L.]]></dc:creator>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Maucher, H. P.]]></dc:creator>
<dc:creator><![CDATA[Plass, M. F.]]></dc:creator>
<dc:creator><![CDATA[Lunk, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2146-1</dc:identifier>
<dc:title><![CDATA[In situ characterization of cubic boron nitride film growth in the IR spectral region]]></dc:title>
<dc:source><![CDATA[Thin Solid Films 313-314 (1998) 697]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2147-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Behrisch, R.]]></dc:creator>
<dc:creator><![CDATA[Grigull, S.]]></dc:creator>
<dc:creator><![CDATA[Kreißig, U.]]></dc:creator>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2147-1</dc:identifier>
<dc:title><![CDATA[Influence of surface roughness on measuring depth profiles and the total amount of implanted ions by RBS and ERDA]]></dc:title>
<dc:source><![CDATA[Nucl. Instr.  Meth. B 136-138 (1998) 628]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2149-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Coleman, P.]]></dc:creator>
<dc:creator><![CDATA[Störmer, J.]]></dc:creator>
<dc:creator><![CDATA[Plazaola, F.]]></dc:creator>
<dc:creator><![CDATA[Campillo, J. M.]]></dc:creator>
<dc:creator><![CDATA[Pacaud, Y.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2149-1</dc:identifier>
<dc:title><![CDATA[Post-implantation annealing of SiC studied by slow positron spectroscopies]]></dc:title>
<dc:source><![CDATA[J. Phys.: Condens. Matter 10 (1998) 1147]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2150-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Dvurechenskii, A. V.]]></dc:creator>
<dc:creator><![CDATA[Karanovich, A. A.]]></dc:creator>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:creator><![CDATA[Herrmann, F.]]></dc:creator>
<dc:creator><![CDATA[Kögler, R.]]></dc:creator>
<dc:creator><![CDATA[Rybin, A. V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2150-1</dc:identifier>
<dc:title><![CDATA[Depth distribution of point defects in Si bombarded by high-energy N<SUP>5+</SUP> and Si<SUP>5+</SUP> ions]]></dc:title>
<dc:source><![CDATA[Phys. Solid State  40 (1998) 195]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<identifier>HZDR:PUBLDB:2151-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Fichtner, P.]]></dc:creator>
<dc:creator><![CDATA[Kaschny, J. R.]]></dc:creator>
<dc:creator><![CDATA[Kling, A.]]></dc:creator>
<dc:creator><![CDATA[Trinkaus, H.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Zawislak, F. C.]]></dc:creator>
<dc:creator><![CDATA[Amaral, L.]]></dc:creator>
<dc:creator><![CDATA[Da Silva, M. F.]]></dc:creator>
<dc:creator><![CDATA[Soares, J. C.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2151-1</dc:identifier>
<dc:title><![CDATA[Nucleation and growth of platelet bubble structures in helium implanted silicon]]></dc:title>
<dc:source><![CDATA[Nucl. Instr. Meth. B 136 - 138 (1998) 460]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1159-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Schmeide, K.]]></dc:creator>
<dc:creator><![CDATA[Zänker, H.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1159-1</dc:identifier>
<dc:title><![CDATA[Characterization of Aquatic Humic Substances from Bog Water and their Complexation Behavior Toward Uranyl Ions]]></dc:title>
<dc:source><![CDATA[13th Radiochemical Conference Marianske Lazne 19.-24.4.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The investigation of the effects of humic substances (humic and fulvic acids) on the migration of radionuclides is important to assess their impact on the long-term safety of both radioactive waste  repository sites (e.g. Gorleben, Germany) and  abandoned uranium mines (Saxony and Thuringia, Germany).
We  extracted humic substances from bog water of the  'Hochmoor Kleiner  Kranichsee' which is in the vicinity  of  the  uranium mining   sites  at  Johanngeorgenstadt  (Saxony).   The   humic material was separated into humic and fulvic acid fractions and characterized   for   its  elemental  composition,   functional properties  including  proton  exchange  capacity,  charge/size distribution  ratios  and spectroscopic  characteristics.   The size  and  size distribution of humic colloids were studied  by photon correlation spectroscopy.  Furthermore, the complexation of site specific humic substances with uranyl ions was studied. The  results were compared with data of a commercial humic acid from Aldrich.]]></dc:description>
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<identifier>HZDR:PUBLDB:2155-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Wünsch, R.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-2155-1</dc:identifier>
<dc:title><![CDATA[Freie Elektronen Laser an der Strahlungsquelle ELBE: Theoretische Vorhersagen und eindimensionale Modellrechnungen]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-276 September 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Für die im Forschungszentrum Rossendorf im Bau befindliche Strahlungsquelle ELBE werden die Möglichkeiten zur Erzeugung kohärenter Strahlung mit Hilfe eines Freie Elektronen Lasers im Bereich des mittleren und fernen Infrarot vorgestellt. Mit Hilfe einfacher Modelle werden die Vorgänge bei der Erzeugung und Verstärkung kohärenter Strahlung erläutert und ihre Eigenschaften in Abhängigkeit von den Parametern des Elektronenstrahls und des verwendeten Undulators berechnet. Insgesamt werden 4 mögliche Varianten eines Undulators diskutiert. Anwendbarkeit und Genauigkeit der verwendeten Näherungsformeln werden mit Hilfe eindimensionaler Simulationsrechnungen getestet. ]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:14218-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schramm, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14218-1</dc:identifier>
<dc:title><![CDATA[Status of the FZD lab combining 150 TW laser pulses with the sc electron linac ELBE]]></dc:title>
<dc:source><![CDATA[14th Advanced Accelerator Concepts Workshop, 13.-19.06.2010, Annapolis, MD, USA, USA]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Talk on the status and prospects of the facility.]]></dc:description>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:14244-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hilger, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14244-1</dc:identifier>
<dc:title><![CDATA[Chiral condensate and medium modifications of open charm mesons]]></dc:title>
<dc:source><![CDATA[74. Jahrestagung der DPG und DPG Frühjahrstagung der Fachverbände, 15.-19.03.2010, Bonn, Deutschland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Mit Hilfe von QCD-Summenregeln untersuchen wir die Sensitivität von pseudoskalaren Mesonen bestehend aus einem leichten und einem schweren Quark (D, D_s und B) auf das chirale Kondensat und betrachten mögliche Verschiebungen oder Aufspaltungen der Massen (d.h. Änderungen der Spektralfunktionen) von Teilchen und Antiteilchen unter Annahme einer linearen Dichteabhängigkeit der Kondensate.
Um Systeme mit direkterer Abhängigkeit vom chiralen Kondensat zu untersuchen, betrachten wir Weinberg-Kapusta-Shuryak Summenregeln bei endlichen Dichten im schwer-leicht Sektor.
Die besondere Rolle der Gluonenkondensate in Systemen aus zwei schweren Quarks (z.B. J/psi) und deren Beziehung zur QCD Spur Anomalie ermöglicht eine Erweiterung der Methode der QCD Summenregeln auf Temperaturen nahe T_c. Unter Verwendung des Rossendorfer Quasi-Teilchen-Modells bestimmen wir die Temperaturabhängigkeit des Digluonen-Kondensats bei endlichen Baryondichten nahe T_c und diskutieren deren Auswirkung auf das J/psi.]]></dc:description>
<dc:subject><![CDATA[QCD sum rules]]></dc:subject>
<dc:subject><![CDATA[D mesons]]></dc:subject>
<dc:subject><![CDATA[open charm]]></dc:subject>
<dc:subject><![CDATA[J/Psi]]></dc:subject>
<dc:subject><![CDATA[chiral partner]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14244-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:2158-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kleinsorge, B.]]></dc:creator>
<dc:creator><![CDATA[Ilie, A.]]></dc:creator>
<dc:creator><![CDATA[Chowalla, M.]]></dc:creator>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Milne, W. I.]]></dc:creator>
<dc:creator><![CDATA[Robertson, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2158-1</dc:identifier>
<dc:title><![CDATA[Electrical and optical properties of boronated tetrahedrally bonded amorphous carbon (ta-C:B)]]></dc:title>
<dc:source><![CDATA[Diamond and Related Mat. 7 (1998) 472]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2159-1</identifier>
<datestamp>2025-04-17</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Stephan, H.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:creator><![CDATA[Klein, L.]]></dc:creator>
<dc:creator><![CDATA[Vögtle, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2159-1</dc:identifier>
<dc:title><![CDATA[Lipophilic urea-functionalized dendrimers as efficient carriers for oxyanions]]></dc:title>
<dc:source><![CDATA[Chem. Commun., 1999, 1875-1876]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Urea-functionalized dendrimers are prepared, which show very efficient phase transfer in particular of the diagnostically relevant anions pertechnetate, perrhenate and ATP. The extractability rates are evaluated quantitavely by tracer methods. Their pH dependancy allows to steer the release of guest molecules from the dendrimer host.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1039/A905862A]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2159-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:2041-1</identifier>
<datestamp>2025-12-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:creator><![CDATA[Klimenkov, M.]]></dc:creator>
<dc:creator><![CDATA[Strobel, M.]]></dc:creator>
<dc:creator><![CDATA[Stegemann, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Thees, H.-J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2041-1</dc:identifier>
<dc:title><![CDATA[Ion beam synthesis of narrow Ge nanocluster bands in thin SiO<SUB>2</SUB> films]]></dc:title>
<dc:source><![CDATA[Microelectronic Engineering 48 (1999) 231-234]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[This paper reports on self-organization of narrow bands of Ge nanoclusters in thin thermally grown SiO<SUB>2</SUB> layers by means of ion beam synthesis. Although the implanted Ge profile is distributed over almost the whole SiO2, a delta-like nanocluster band very close to, but well separated from the Si/SiO<SUB>2</SUB> interface is formed under specific implantation and annealing conditions. The evolution of this band can be explained by a model taking into account collisional ion beam mixing and reactions near the Si/SiO<SUB>2</SUB> interface, which describes in good agreement the experimental results. The reliable fabrication of such cluster bands are the basis for new memory applications.]]></dc:description>
<dc:subject><![CDATA[ion beam synthesis]]></dc:subject>
<dc:subject><![CDATA[thin SiO<SUB>2</SUB> films]]></dc:subject>
<dc:subject><![CDATA[nanocluster]]></dc:subject>
<dc:subject><![CDATA[self-organisation]]></dc:subject>
<dc:subject><![CDATA[non-volatile memories]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0167-9317(99)00377-9]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2041-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:2041-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:creator><![CDATA[Klimenkov, M.]]></dc:creator>
<dc:creator><![CDATA[Strobel, M.]]></dc:creator>
<dc:creator><![CDATA[Stegemann, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Thees, H.-J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2041-2</dc:identifier>
<dc:title><![CDATA[Ion beam synthesis of narrow Ge nanocluster bands in thin SiO<SUB>2</SUB> films]]></dc:title>
<dc:source><![CDATA[Insulating Films on Semiconductors,INFOS'99, Kloster Ban7, Germany, June 16-19,1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[This paper reports on self-organization of narrow bands of Ge nanoclusters in thin thermally grown SiO<SUB>2</SUB> layers by means of ion beam synthesis. Although the implanted Ge profile is distributed over almost the whole SiO2, a delta-like nanocluster band very close to, but well separated from the Si/SiO<SUB>2</SUB> interface is formed under specific implantation and annealing conditions. The evolution of this band can be explained by a model taking into account collisional ion beam mixing and reactions near the Si/SiO<SUB>2</SUB> interface, which describes in good agreement the experimental results. The reliable fabrication of such cluster bands are the basis for new memory applications.]]></dc:description>
<dc:subject><![CDATA[ion beam synthesis]]></dc:subject>
<dc:subject><![CDATA[thin SiO<SUB>2</SUB> films]]></dc:subject>
<dc:subject><![CDATA[nanocluster]]></dc:subject>
<dc:subject><![CDATA[self-organisation]]></dc:subject>
<dc:subject><![CDATA[non-volatile memories]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2041-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:2044-1</identifier>
<datestamp>2025-12-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ivanov, K. N.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Mittag, S.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2044-1</dc:identifier>
<dc:title><![CDATA[Comparative Study of a Boron Dilution Scenario in VVER Reactors]]></dc:title>
<dc:source><![CDATA[Annals of Nuclear Energy 26 (1999) 1331-1339]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Subsequent studies have identified many scenarios which can lead to reactivity excursions due to boron dilution. The comparative study, presented in this paper, deals with the so-called "restart of the first reactor coolant pump" scenario and its reactor-dynamic consequences for the both VVER reactor types - VVER-440 and VVER-1000. The transient simulations were performed using the three-dimensional core dynamics code DYN3D. The DYN3D modeling features, including recent developments, as well as the cross-section generation methodology, involved in these calculations, are described. The analyzed accident scenario is outlined together with the assumptions made. The results of core response in this boron dilution accident for both VVER reactors have been compared within ranges, determined by the two reactivity values of interest: the criticaly limit and the reactivity initiated accident (RIA) limit.]]></dc:description>
<dc:subject><![CDATA[VVER-reactors]]></dc:subject>
<dc:subject><![CDATA[boron dilution transient]]></dc:subject>
<dc:subject><![CDATA[three-dimensional core dynamics]]></dc:subject>
<dc:subject><![CDATA[reactivity initiated accidents]]></dc:subject>
<dc:subject><![CDATA[computer code DYN3D]]></dc:subject>
<dc:subject><![CDATA[group constants]]></dc:subject>
<dc:subject><![CDATA[cross section library]]></dc:subject>
<dc:subject><![CDATA[comparisons]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0306-4549(99)00018-3]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2044-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:2045-1</identifier>
<datestamp>2025-12-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bolano, S.]]></dc:creator>
<dc:creator><![CDATA[Bravo, J.]]></dc:creator>
<dc:creator><![CDATA[Carballo, R.]]></dc:creator>
<dc:creator><![CDATA[Garcia-Fontan, S.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Vazquez-Lopez, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2045-1</dc:identifier>
<dc:title><![CDATA[Synthesis and characterization of the bromide and hydride derivatives of rhenium(I) 1,2-bis(diphenylphosphinite)ethane complexes]]></dc:title>
<dc:source><![CDATA[Polyhedron 18 (1999) 1431-1436]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0277-5387(99)00002-9]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2045-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1715-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Beyer, M.]]></dc:creator>
<dc:creator><![CDATA[Carl, H.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Seidel, A.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Zschau, J.]]></dc:creator>
<dc:creator><![CDATA[Nowak, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1715-1</dc:identifier>
<dc:title><![CDATA[A technical system to improve the operational monitoring of the Zaporosh'ye nuclear power plant (remote monitoring system in Ukraine - first level of realization)]]></dc:title>
<dc:source><![CDATA[Proc. of the FOURTH INTERNATIONAL WOKRSHOP on real-time computing of the environmental consequence of an accident release from a nuclear installation, Aronsborg, Sweden, Oct. 7 - 11, 1996, Paper-N ...]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[A technical system to improve the operational monitoring of the Zaporozh'ye NPP as a tool for the supervisory authority is presented. The system is mainly directed to monitoring the operational data for early detection of, and information about, anomalous events and gives input data for source term estimation. Additionally, radiological data from the site and the environment as well as meteorological data are integrated in the system for pollution transport calculations. Thus the system's information is well suited to becoming a data source for RODOS system.
]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:bookPart</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1715-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:1716-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Beyer, M.]]></dc:creator>
<dc:creator><![CDATA[Carl, H.]]></dc:creator>
<dc:creator><![CDATA[Nowak, K.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Seidel, A.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Zschau, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1716-1</dc:identifier>
<dc:title><![CDATA[A technical system to improve the operational monitoring of the ukrainian nuclear power plant Zaporosh'ye (Unit 5)]]></dc:title>
<dc:source><![CDATA[Proc. of the OECD/NEANSC Specialists' meeting on in-core instrumentation and reactor core assessment, Mito-shi, Japan, Oct. 14 - 17, 1996, Paper-No. 88]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[In order to improve the operational surveillance of a VVER-1000 unit of the Ukrainian nuclear power plant Zaporosh'ye a technical monitoring system has been specified and installed during the last three years.
The technical system enables the operator and supervisory body to monitor the core and the unit continuously during normal and off-normal conditions, to assess the safety status of core and unit, and to impose appropriate measures. The system provides an early indication of any operational incident and of emissions of radioactive materials. Based on the system an immediate warning in emergency situations is possible as well as an effective emergency management. For this purpose 49 different safety related operational parameters of the core and unit - e.g.: neutron flux, pressure - primary and secondary circuit, fuel rod outlet water temperature, boron concentration - primary circuit and so on -, 18 radiological parameters of the unit and the plant side and 6 meteorological parameters are automatically monitored and evaluated.
The system was put into operation at the end of 1995. It is now working under test conditions.
The paper presents the technical solution of the system and the evaluation principles. Additionally the paper gives a short overview about the results obtained during the test operation of the system.
]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1994-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Stefani, F.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Gailitis, A.]]></dc:creator>
<dc:creator><![CDATA[Lielausis, O.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1994-1</dc:identifier>
<dc:title><![CDATA[Laboratory Experiments on Dynamo Action]]></dc:title>
<dc:source><![CDATA[SIAM Annual Meeting, University of Toronto (Canada), 13.-17. July 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Despite the great success of dynamo theory during the last decades an experimental verification of magnetic field self-excitation in conducting fluids is still missing. We summarize the outcomes of a workshop held in Riga in June 1998 on various experimental approaches to this topic. The Riga dynamo
experiment is presented in more detail.

]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1045-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Laggiard, E.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Runkel, J.]]></dc:creator>
<dc:creator><![CDATA[Stegemann, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1045-1</dc:identifier>
<dc:title><![CDATA[Noise Analysis Measurements and Numerical Evaluations of the Moderator Temperature Coefficient in PWRs]]></dc:title>
<dc:source><![CDATA[27th Informal Meeting on Reactor Noise (IMORN 27), Valencia, November 18 - 20, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The moderator temperature coefficient (MTC) of a 1400 MW pressurized water reactor (PWR) has been measured from neutron and temperature fluctuations in different reactor positions. In order to explain the deviations observed between the estimations, numerical evaluations of the MTC were performed using the 3D two energy groups DYN3D code for a prototype PWR. The differences between the experimental MTC estimations can be partially explained considering that the numerical MTC evaluations show a definite devitation of the neutronics from point kinetics.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1045-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Laggiard, E.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Runkel, J.]]></dc:creator>
<dc:creator><![CDATA[Stegemann, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1045-2</dc:identifier>
<dc:title><![CDATA[Noise Analysis Measurements and Numerical Evaluations of the Moderator Temperature Coefficient in PWRs]]></dc:title>
<dc:source><![CDATA[27th Informal Meeting on Reactor Noise (IMORN 27), Valencia,
November 18 - 20, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The moderator temperature coefficient (MTC) of a 1400 MW pressurized water reactor (PWR) has been measured from neutron and temperature fluctuations in different reactor positions. In order to explain the deviations observed between the estimations, numerical evaluations of the MTC were performed using the 3D two energy groups DYN3D code for a prototype PWR. The differences between the experimental MTC estimations can be partially explained considering that the numerical MTC evaluations show a definite devitation of the neutronics from point kinetics.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:14316-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:creator><![CDATA[Herrmannsdörfer, T.]]></dc:creator>
<dc:creator><![CDATA[Skrotzki, R.]]></dc:creator>
<dc:creator><![CDATA[Ignatchik, O.]]></dc:creator>
<dc:creator><![CDATA[Uhlarz, M.]]></dc:creator>
<dc:creator><![CDATA[Fiedler, J.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:creator><![CDATA[Wündisch, C.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Wosnitza, J.]]></dc:creator>
<dc:creator><![CDATA[Helm, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14316-1</dc:identifier>
<dc:title><![CDATA[Superconductivity in Ga-doped Germanium above 1 K]]></dc:title>
<dc:source><![CDATA[30th International Conference on the Physics of Semiconductors (ICPS), 25.-30.07.2010, Seoul, Korea]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The discovery of superconductivity in heavily boron-doped diamond [1] has demonstrated that group-IV semiconductors can become superconducting upon carrier doping even at ambient conditions. Meanwhile superconductivity has been found in further heavily doped group-IV semiconductors such as Si and SiC [2]. Compared to these semiconductors, Ge seems to be less promising for realizing superconductivity as was based upon estimates of the electron-phonon coupling strength [3]. The challenge is to achieve extremely high hole concentrations which are commonly limited by the equilibrium solid solubility of the acceptor. Nevertheless, we succeeded in making Ge superconducting as recently reported [4]. A nonequilibrium doping process consisting of 100 keV Ga+-ion implantation with a fluence of 21016cm-2 and subsequent 3 ms flash-lamp annealing (FLA) enabled hole concentrations as high as 1.41021 cm-2. The superconducting state was observed in a thin (~60 nm) Ge layer with a maximum Ga content of about 8 at.% at critical temperatures below 0.5 K. From the measured critical parameters it follows that Ga-doped Ge is a type-II superconductor with a large Ginzburg-Landau parameter (>103).
The structure as well as the superconducting properties of the Ga-doped Ge layers depend sensitively on the preparation conditions as shown in Fig. 1. In search for higher transition temperatures, implantation and annealing conditions were varied in a more comprehensive study. Critical temperatures above 1 K were obtained for samples either implanted with 41016 cm-2 and flash-lamp annealed at 52 Jcm-2 or implanted with 21016 cm-2 and subjected to rapid thermal annealing (RTA) at 910°C for 60 s (Fig. 2). Critical magnetic fields perpendicular and parallel to the Ge:Ga plane up to about 0.3 and 1 T, respectively, were observed. Thus superconductivity in thin Ge:Ge layers is a robust effect and could be utilized in superconducting quantum devices.

[1] E. A. Ekimov, V. A. Sidorov, E. D. Bauer, et al., Nature 428, 542 (2004)
[2] K. Iakoubovskii, Physica C 469, 675 (2009)
[3] L. Boeri, J. Kortus, O. K. Anderson, J. Phys. Chem. Solids 67, 552 (2006)
[4] T. Herrmannsdörfer, V. Heera, O. Ignatchik, et al., Phys. Rev. Lett. 102, 217003 (2009)]]></dc:description>
<dc:subject><![CDATA[superconductivity]]></dc:subject>
<dc:subject><![CDATA[germanium]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:2077-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hensel, F.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2077-1</dc:identifier>
<dc:title><![CDATA[SchaumPET – A Setup for Positron Emission Tomography (PET) Investigation of Foam in a Bubble Column]]></dc:title>
<dc:source><![CDATA[Abstract in "4th Topical Meeting on Industrial Radiation and Radioisotope Measurements and Applications · IRRMA99" Conference Program and Abstracts. October 3-7 1999, Raleigh (USA). ISBN 0-89448-646-2, 32]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The paper describes a Positron Emission Tomograph dedicated to the investigation of the behavior of foam in a bubble column as well as the current planning of experiments using this device. In these experiments, foam generation, foam stability and transport phenomena in the liquid phase are the main topics of interest. ]]></dc:description>
<dc:subject><![CDATA[positron emission tomography]]></dc:subject>
<dc:subject><![CDATA[nonmedical applications]]></dc:subject>
<dc:subject><![CDATA[BGO]]></dc:subject>
<dc:subject><![CDATA[coincidence logic]]></dc:subject>
<dc:subject><![CDATA[bubble column]]></dc:subject>
<dc:subject><![CDATA[foam]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
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<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2077-1</dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:2077-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hensel, F.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2077-7</dc:identifier>
<dc:title><![CDATA[SchaumPET – A Setup for Positron Emission Tomography (PET) Investigation of Foam in a Bubble Column]]></dc:title>
<dc:source><![CDATA[Abstract in "4th Topical Meeting on Industrial Radiation and Radioisotope Measurements and Applications · IRRMA99" Conference Program and Abstracts. October 3-7 1999, Raleigh (USA). ISBN 0-89448-646-2, 32]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The paper describes a Positron Emission Tomograph dedicated to the investigation of the behavior of foam in a bubble column as well as the current planning of experiments using this device. In these experiments, foam generation, foam stability and transport phenomena in the liquid phase are the main topics of interest. ]]></dc:description>
<dc:subject><![CDATA[positron emission tomography]]></dc:subject>
<dc:subject><![CDATA[nonmedical applications]]></dc:subject>
<dc:subject><![CDATA[BGO]]></dc:subject>
<dc:subject><![CDATA[coincidence logic]]></dc:subject>
<dc:subject><![CDATA[bubble column]]></dc:subject>
<dc:subject><![CDATA[foam]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2077-7</dc:relation>
<dc:audience>Researchers</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2951-1</identifier>
<datestamp>2025-12-03</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hausmann, S.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2951-1</dc:identifier>
<dc:title><![CDATA[Dwell-time related effects in focused ion beam synthesis of cobalt disilicide]]></dc:title>
<dc:source><![CDATA[Journal of Applied Physics (01/01/2000) Vol 87, No. 1, 57-62]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The influence of the high current density of a focused ion beam on the ion beam synthesis of CoSi2 layers has been investigated. After 35 keV Co+ or 70 keV Co2+ implantation into a heated Si(111) substrate and subsequent annealing, the layers have been investigated by scanning electron microscopy and Rutherford backscattering spectroscopy. It is shown that the mode of beam scanning influences the CoSi2 layer formation significantly. At a given substrate temperature, a sufficient low dwell-time is required to obtain a continuous layer rather than a laterally disrupted structure. With increasing target temperature, the dwell-time window becomes less restricted. The results are discussed in terms of  damaging and dynamic annealing of the silicon crystal. RBS/channeling investigations demonstrate that continuous or disrupted CoSi2 layers are formed when the substrate remains crystalline or becomes amorphous, respectively.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1063/1.371826]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2951-1</dc:relation>
<dc:audience>Researchers</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2083-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schibli, R.]]></dc:creator>
<dc:creator><![CDATA[Alberto, R.]]></dc:creator>
<dc:creator><![CDATA[Schaffland, A. O.]]></dc:creator>
<dc:creator><![CDATA[Schubiger, P. A.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2083-1</dc:identifier>
<dc:title><![CDATA[Derivatization strategies of small biomolecules for the labeling with the organometallic "<SUP>99m</SUP>Tc(CO)<SUB>3</SUB>"-core]]></dc:title>
<dc:source><![CDATA[13th International symposium on Radiopharmaceutical Chemistry, St. Louis,USA, 27.6.-1.7.1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Small, radiolabeled biomolecules, such as steroids, tracers for the central nervous system and biotin obtained considerable attention in diagnostic nuclear medicine. Nowadays, there are numerous short living isotopes available for SPECT (e.g. <SUP>131</SUP>I) and PET (e.g. <SUP>18</SUP>F, <SUP>11</SUP>C) imaging to label such biological vectors. Despite this fact. Tc-99m is still the isotope of choice for diagnostic purpose because of its ideal decay properties. However, unlike iodinated of fluorinated radiopharmaceuticals, Tc-99m requires a highly sophisticated functionalization and coordination chemistry. Attempts to substitute direct covalent bound isotopes by Tc-99m chelates were, apart from peptides, only partially successful. (1,2) The reason is mainly the size of the introduced chelates (interference with active site of the biomolecule) and the redox sensitivity of <SUP>99m</SUP>Tc in the oxidation state +3 and +5. Therefore, alternative approaches are required to overcome these problems by introduction of small, redox inert <SUP>99m</SUP>Tc-cores in combination with simple ligand systems.
Although the idea of labeling e.g. steroids with organometallic Re or Tc-compounds was published by Top et al. In 1995 the attempt failed due to synthetic problems of the precursor on the no-carrier added level.(3) Our group recently pioneered the synthesis of the organometallic Tc(I) complex fac-[M(OH<SUB>2</SUB>)<SUB>3</SUB>(CO)<SUB>3</SUB>]<SUP>+</SUP> (M=<SUP>99m</SUP>Tc  1a, <SUP>99</SUP>Tc  1b, Re  1c) under safe and pressureless conditions in aqueous media in high yields (<95%).(4,5) The compound is characterized by its water solubility, pronounced kinetic inertness (low spin d<SUP>6</SUP> system) and the substitution lability of the three coordinated water molecules enabling effective labeling under mild conditions. The small size of the organometallic center will minimize the interference with the binding side of a biomolecule. Therefore, this new label optimi ...]]></dc:description>
<dc:subject><![CDATA[Tc-99m]]></dc:subject>
<dc:subject><![CDATA[organometallic]]></dc:subject>
<dc:subject><![CDATA[Biotin]]></dc:subject>
<dc:subject><![CDATA[WAY]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:2083-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schibli, R.]]></dc:creator>
<dc:creator><![CDATA[Alberto, R.]]></dc:creator>
<dc:creator><![CDATA[Schaffland, A. O.]]></dc:creator>
<dc:creator><![CDATA[Schubiger, P. A.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2083-2</dc:identifier>
<dc:title><![CDATA[Derivatization strategies of small biomolecules for the labeling with the organometallic "<SUP>99m</SUP>Tc(CO)<SUB>3</SUB>"-core]]></dc:title>
<dc:source><![CDATA[J. Labelled Compd. Radiopharm. 42 (1999) S147-S149]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Small, radiolabeled biomolecules, such as steroids, tracers for the central nervous system and biotin obtained considerable attention in diagnostic nuclear medicine. Nowadays, there are numerous short living isotopes available for SPECT (e.g. <SUP>131</SUP>I) and PET (e.g. <SUP>18</SUP>F, <SUP>11</SUP>C) imaging to label such biological vectors. Despite this fact. Tc-99m is still the isotope of choice for diagnostic purpose because of its ideal decay properties. However, unlike iodinated of fluorinated radiopharmaceuticals, Tc-99m requires a highly sophisticated functionalization and coordination chemistry. Attempts to substitute direct covalent bound isotopes by Tc-99m chelates were, apart from peptides, only partially successful. (1,2) The reason is mainly the size of the introduced chelates (interference with active site of the biomolecule) and the redox sensitivity of <SUP>99m</SUP>Tc in the oxidation state +3 and +5. Therefore, alternative approaches are required to overcome these problems by introduction of small, redox inert <SUP>99m</SUP>Tc-cores in combination with simple ligand systems.
Although the idea of labeling e.g. steroids with organometallic Re or Tc-compounds was published by Top et al. In 1995 the attempt failed due to synthetic problems of the precursor on the no-carrier added level.(3) Our group recently pioneered the synthesis of the organometallic Tc(I) complex fac-[M(OH<SUB>2</SUB>)<SUB>3</SUB>(CO)<SUB>3</SUB>]<SUP>+</SUP> (M=<SUP>99m</SUP>Tc  1a, <SUP>99</SUP>Tc  1b, Re  1c) under safe and pressureless conditions in aqueous media in high yields (<95%).(4,5) The compound is characterized by its water solubility, pronounced kinetic inertness (low spin d<SUP>6</SUP> system) and the substitution lability of the three coordinated water molecules enabling effective labeling under mild conditions. The small size of the organometallic center will minimize the interference with the binding side of a biomolecule. Therefore, this new label optimi ...]]></dc:description>
<dc:subject><![CDATA[Tc-99m]]></dc:subject>
<dc:subject><![CDATA[organometallic]]></dc:subject>
<dc:subject><![CDATA[Biotin]]></dc:subject>
<dc:subject><![CDATA[WAY]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:760-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barz, H.-U.]]></dc:creator>
<dc:creator><![CDATA[Böhmer, B.]]></dc:creator>
<dc:creator><![CDATA[Konheiser, J.]]></dc:creator>
<dc:creator><![CDATA[Stephan, I.]]></dc:creator>
<dc:creator><![CDATA[Borodkin, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-760-2</dc:identifier>
<dc:title><![CDATA[Determination of Pressure Vessel Neutron Fluence Spectra for a Low Leakage Rovno-3 Reactor Core Using Three Dimensional Monte Carlo Neutron Transport Calculations and Ex-vessel Neutron Activation Data]]></dc:title>
<dc:source><![CDATA[in H.A. Abderrahim, P. D'hondt and B. Osmera (Ed.), Proceedings of the 9th International Symposium on Reactor Dosimetry, Prag (pp.58-66)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Three dimensional Monte Carlo calculations considering all known geometrical and composition details were used for the determination not only of fluence integrals but also of fluence spectra with good statistical accuracy. This was possible by the application of own specially developed codes (TRAMO) and successfully modifying variance reduction on the basis of the weight window method (TRAWEI). Modern multigroup data sets were applied. For the real representation of fission sources the burn up and power history also for the fuel rods within the fuel assemblies was considered. 
The investigation was accomplished for the irradiation period seven with a special low leakage loading of the reactor. During this period Russian and German detectors were irradiated in the ex-vessel cavity and analysed by advanced gamma spectrometric methods.
The reaction rates obtained with the calculated fluence spectra were compared with activation reaction rates measured in the ex-vessel cavity. Furthermore the calculated spectra were adjusted to the experimental reaction rates taking into account the variances and correlations of  calculated input spectra, detector sensitivities and measurements. Using the adjustment code COSA2 based on the  maximum likelihood method best estimate fluence spectra and fluence integrals could be provided.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:760-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barz, H.-U.]]></dc:creator>
<dc:creator><![CDATA[Böhmer, B.]]></dc:creator>
<dc:creator><![CDATA[Konheiser, J.]]></dc:creator>
<dc:creator><![CDATA[Stephan, I.]]></dc:creator>
<dc:creator><![CDATA[Borodkin, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-760-1</dc:identifier>
<dc:title><![CDATA[Determination of Pressure Vessel Neutron Fluence Spectra for a Low Leakage Rovno-3 Reactor Core Using Three Dimensional Monte Carlo Neutron Transport Calculations and Ex-vessel Neutron Activation Data]]></dc:title>
<dc:source><![CDATA[9th International Symposium on Reactor Dosimetry, Sept. 2-6, 1996, Prague]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Three dimensional Monte Carlo calculations considering all known geometrical and composition details were used for the determination not only of fluence integrals but also of fluence spectra with good statistical accuracy. This was possible by the application of own specially developed codes (TRAMO) and successfully modifying variance reduction on the basis of the weight window method (TRAWEI). Modern multigroup data sets were applied. For the real representation of fission sources the burn up and power history also for the fuel rods within the fuel assemblies was considered. 
The investigation was accomplished for the irradiation period seven with a special low leakage loading of the reactor. During this period Russian and German detectors were irradiated in the ex-vessel cavity and analysed by advanced gamma spectrometric methods.
The reaction rates obtained with the calculated fluence spectra were compared with activation reaction rates measured in the ex-vessel cavity. Furthermore the calculated spectra were adjusted to the experimental reaction rates taking into account the variances and correlations of  calculated input spectra, detector sensitivities and measurements. Using the adjustment code COSA2 based on the  maximum likelihood method best estimate fluence spectra and fluence integrals could be provided.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-760-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2862-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Zimmermann, T.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2862-1</dc:identifier>
<dc:title><![CDATA[Ring Transformations of Heterocyclic Compounds. XIX Spiro[dihydropyridine-indolines] - Novel Heterocycles with Two Spiro-Condensed N-Containing Subunits Easy Accessible by 1,3-Oxazinium Ring Transformation]]></dc:title>
<dc:source><![CDATA[J. Heterocyclic Chem. 35, 787 (1998)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The synthesis of hitherto unknown 1-benzoyl-1´,3´,3´-trimethyl-4,6-diphenylspiro[1,2-dihydropyridine-2,2´-indolines] 5 from 2,4,6-triphenyl-1,3-oxazinium tetrafluoroborate (1b) and 1,3,3-trimethyl-2-methylene-indolines 2 (used as such or generated in situ from the corresponding 3H-indolium salts 4) in the presence of triethylamine in anhydrous acetonitrile by a 3,6-[C3N+C2] 1,3-oxazinium ring transformation is reported. Structure elucidation is performed by an X-ray structure determination of the spiro[dihydropyridine-indoline] 5a. Spectroscopic data of the transformation products and their mode of formation are discussed.
]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2862-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2138-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schmeide, K.]]></dc:creator>
<dc:creator><![CDATA[Zänker, H.]]></dc:creator>
<dc:creator><![CDATA[Hüttig, G.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2138-1</dc:identifier>
<dc:title><![CDATA[Complexation of Aquatic Humic Substances from the Bog "Kleiner Kranichsee" with Uranium(VI)]]></dc:title>
<dc:source><![CDATA[FZKA 6324, Wissenschaftliche Berichte Forschungszentrum Karlsruhe, (G. Buckau, ed.). Karlsruhe 1999, p. 177.]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[As a contribution to Task 1 (Sampling and Characterization), we have characterized Derwent Reservoir fulvic acid by means of FTIR spectroscopy and capillary zone electrophoresis and compared to Kranichsee humic and fulvic acid and Aldrich humic acid.
Our contribution to Task 2 (Complexation) consists of two parts. First, we studied the complexation of Kranichsee humic acid (HA) and fulvic acid (FA) with uranyl(VI) ions by laser-induced fluorescence spectroscopy at pH 4 and an ionic strength of 0.1 M (NaClO4). The loading capacities were determined to be 14 ± 1 % and 13 ± 1 % for humic acid and fulvic acid, respectively. The complexation constants for Kranichsee humic acid and fulvic acid were found to be log ß = 6.35 ± 0.22 and log ß = 6.21 ± 0.20, respectively. These results were compared to the uranyl complexation behavior of other natural humic acids such as Aldrich HA and GoHy-573 HA. Second, we investigated original bog water of the mountain bog 'Kleiner Kranichsee' by ultrafiltration to determine the hydrodynamic particle size distribution, i.e., the 'apparent molecular weight' distribution of the organic substances in the bog water. Furthermore, the influence of uranyl complexation on this particle size distribution of humic colloids was investigated. No significant influence of the uranyl ions on the molecular weight distribution of the humic substances was found.]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
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<dc:type>doc-type:bookPart</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2138-1</dc:relation>
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<dc:audience>Students</dc:audience>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2930-1</identifier>
<datestamp>2025-12-03</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Gupta, A.]]></dc:creator>
<dc:creator><![CDATA[Reisgys, M.]]></dc:creator>
<dc:creator><![CDATA[Drews, A.]]></dc:creator>
<dc:creator><![CDATA[Seifert, S.]]></dc:creator>
<dc:creator><![CDATA[Syhre, R.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Alberto, R.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Schubiger, P. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2930-1</dc:identifier>
<dc:title><![CDATA[Chemical and biological characterization of technetium(I) and rhenium(I) tricarbonyl complexes with dithioether ligands serving as linkers for coupling the Tc(CO)<SUB>3</SUB> and Re(CO)<SUB>3</SUB> moieties to biologically active molecules]]></dc:title>
<dc:source><![CDATA[Bioconjugate Chem. 11 (2000) 414-424]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The organometallic precursor (NEt<SUB>4</SUB>)<SUB>2</SUB>[ReBr<SUB>3</SUB>(CO)<SUB>3</SUB>] was reacted with bidendate dithioethers (L) of the general formula H<SUB>3</SUB>C-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-S-R (R = -CH<SUB>2</SUB>CH<SUB>2</SUB>COOH, CH<SUB>2</SUB>-C=CH) and R'-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-S-R' (R' = CH<SUB>3</SUB>CH<SUB>2</SUB>-, CH<SUB>3</SUB>CH<SUB>2</SUB>-OH, CH<SUB>2</SUB>COOH) in methanol to form stable rhenium(I) tricarbonyl complexes of the general composition [ReBr(CO)<SUB>3</SUB>L]. Under these conditions the functional groups do not participate in the coordination. As a prototypic representative of this type of Re compounds the propargylic-group-bearing complex [ReBr(CO<SUB>3</SUB>)(H<SUB>3</SUB>C-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>C=CH)] Re<SUB>2</SUB> was studied by X-ray diffraction analysis. Its molecular structure exhibits a slightly distorted octahedron with facial coordination of the carbonyl ligands. 
The potentially tetradentate ligand HO-CH<SUB>2</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-OH was reacted with the trinitrato precursor [Re(NO<SUB>3</SUB>)<SUB>3</SUB>(CO)<SUB>3</SUB>]<SUP>2-</SUP> to yield a cationic complex [Re(CO)<SUB>3</SUB>(HO-CH<SUB>2</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-OH)]NO<SUB>3</SUB>  Re8 which shows the coordination of one hydroxy group. Re8 has been characterized by correct elemental analysis, infrared spectroscopy, capillary electrophoresis and X-ray diffraction analysis.
Ligand exchange reaction of the carboxylic group bearing ligands H<SUB>3</SUB>C-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-COOH and HOOC-CH<SUB>2</SUB>-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>-COOH with (NEt<SUB>4</SUB>)<SUB>2</SUB>[ReBr<SUB>3</SUB>(CO)<SUB>3</SUB>] in water and with equimolar amounts of NaOH led to complexes in which the bromide is replaced by the carboxylic group. The X-ray structure analysis of the complex [Re(CO)<SUB>3</SUB>(OOC-CH<SUB>2</SUB>-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>-COOH)] Re6 shows the second carboxylic group non-coordinated offering an ideal site for functionalization or coupling a biomolecule.
The no-carrier-added preparation of the analogue <SUP>99m</SUP>Tc(I) carbonyl thioether complexes could be performed using the precursor fac-[99mTc(H<SUB>2</SUB>O)<SUB>3</SUB>(CO)<SUB>3</SUB>]<SUP>+</SUP> 
with yields up to 90 %. The behaviour of the chlorine containing <SUP>99m</SUP>Tc complex <SUP>[99m</SUP>TcCl(CO)<SUB>3</SUB>(CH<SUB>3</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>CH<SUB>3</SUB>)] Tc1 in aqueous solution at physiological pH value was investigated. In saline, the chromatographically separated compound was stable for at least 120 min. However, in chloride free aqueous solution a water-coordinated cationic species Tc1a of the proposed composition [<SUP>99m</SUP>Tc(H<SUB>2</SUB>O)(CO)<SUB>3</SUB>(CH<SUB>3</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>CH<SUB>3</SUB>)]<SUP>+</SUP> occured. The cationic charge of the conversion product was confirmed by capillary electrophoresis. By the introduction of a carboxylic group into the thioether ligand as a third donor group the conversion could be suppressed and thus the neutrality of the complex preserved. 
Biodistribution studies in the rat demonstrated for the neutral complexes [<SUP>99m</SUP>TcCl(CO)<SUB>3</SUB>(CH<SUB>3</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>CH<SUB>3</SUB>)] Tc1 and [<SUP>99m</SUP>TcCl(CO)<SUB>3</SUB>(CH<SUB>2</SUB>-S-CH<SUB>2</SUB>CH<SUB>2</SUB>-S-CH<SUB>2</SUB>-C=CH)] Tc2 a significant initial brain uptake (1,03 ± 0.25 % and 0.78 ± 0.08 % ID/organ at 5 min. p.i.). Challenge experiments with glutathione clearly indicated that no transchelation reaction occurs in vivo.

]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1021/bc990162o]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:2154-1</identifier>
<datestamp>2025-11-26</datestamp>
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<dc:creator><![CDATA[Dohrmann, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2154-1</dc:identifier>
<dc:title><![CDATA[Medium Effects in K<SUP>+</SUP> and K<SUP>-</SUP> Poduction in Nuclear Collisions at Subthreshold Beam Energies]]></dc:title>
<dc:source><![CDATA[Nucl.Phys. A 663 (2000) 521-524]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[We have conducted systematic experimental studies of  K<sup>+</sup> and K<sup>-</sup> production and propagation in nucleus-nucleus collisions at beam energies close to and below the production threshold for free nucleon-nucleon (NN) collisions. In noncentral Au+Au collision, the  K<sup>+</sup> mesons are preferentially emitted perpendicular to the reaction plane and the excitation functions for K<sup>+</sup> and K<sup>-</sup> mesons nearly coincide when correcting for the threshold energy. In contrast, for NN collisions the K<sup>+</sup> yield exceeds the K<sup>-</sup> yield by two orders of magnitude near the respective NN threshold. Both effects are considered to be experimental signatures of a modification of kaon properties in the nuclear medium.]]></dc:description>
<dc:subject><![CDATA[In-medium modifications of K mesons]]></dc:subject>
<dc:subject><![CDATA[Particle and Resonance Production]]></dc:subject>
<dc:subject><![CDATA[Meson Production]]></dc:subject>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1951-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Werner, M.]]></dc:creator>
<dc:creator><![CDATA[Willschütz, H.-G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1951-1</dc:identifier>
<dc:title><![CDATA[Stress Analysis of BWR Components Under Accident Loads Using Finite Elements]]></dc:title>
<dc:source><![CDATA[Proceedings of TOPSAFE´98, Valencia (Spain), April 15-17, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[During a hypothetical accident the reactor pressure vessel internals of boiling water 
reactors can be exposed to considerable loads resulting from temperature gradients and pressure waves. The finite element (FE) analysis is an efficient tool to evaluate the  consequences of those loads by computing the maximum mechanical stresses in the  components.  3 dimensional FE models were developed for the core shroud, the upper and the lower core supporting structure, the steam separator pipes and the feed water distributor. The models of core shroud, upper core support structure and lower core support structure were coupled by means of the substructure technique. All FE models can be used for thermal and for structural mechanical analyses. As an example the FE analysis for the case of a station black-out scenario (loss of power supply for the main circulating pumps) with subsequent emergency core cooling is demonstrated. The transient temperature distributions within the core shroud and within the steam separator pipes as well were calculated based on the fluid temperatures and the heat transfer coefficients provided by thermo-hydraulic codes. At the maximum temperature gradients in the core shroud, the mechanical stress
distribution was computed in a static analysis with the actual temperature field being
the load. It could be shown that the maximum resulting material stresses do not exceed the permissible thresholds fixed in the appropriate regulations. Another scenario which was investigated is the break of a feed water line leading to a non-symmetric subpressure wave within the reactor pressure vessel. The dynamic structural response of the core shroud was assessed in a tranisient analysis. Even for this load case the maximum resulting stresses remain within the allowed limits at any time.]]></dc:description>
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<identifier>HZDR:PUBLDB:1951-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Werner, M.]]></dc:creator>
<dc:creator><![CDATA[Willschütz, H.-G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1951-7</dc:identifier>
<dc:title><![CDATA[Stress Analysis of BWR Components Under Accident Loads Using Finite Elements]]></dc:title>
<dc:source><![CDATA[Proceedings of TOPSAFE´98, Valencia (Spain), April 15-17, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[During a hypothetical accident the reactor pressure vessel internals of boiling water 
reactors can be exposed to considerable loads resulting from temperature gradients and pressure waves. The finite element (FE) analysis is an efficient tool to evaluate the  consequences of those loads by computing the maximum mechanical stresses in the  components.  3 dimensional FE models were developed for the core shroud, the upper and the lower core supporting structure, the steam separator pipes and the feed water distributor. The models of core shroud, upper core support structure and lower core support structure were coupled by means of the substructure technique. All FE models can be used for thermal and for structural mechanical analyses. As an example the FE analysis for the case of a station black-out scenario (loss of power supply for the main circulating pumps) with subsequent emergency core cooling is demonstrated. The transient temperature distributions within the core shroud and within the steam separator pipes as well were calculated based on the fluid temperatures and the heat transfer coefficients provided by thermo-hydraulic codes. At the maximum temperature gradients in the core shroud, the mechanical stress
distribution was computed in a static analysis with the actual temperature field being
the load. It could be shown that the maximum resulting material stresses do not exceed the permissible thresholds fixed in the appropriate regulations. Another scenario which was investigated is the break of a feed water line leading to a non-symmetric subpressure wave within the reactor pressure vessel. The dynamic structural response of the core shroud was assessed in a tranisient analysis. Even for this load case the maximum resulting stresses remain within the allowed limits at any time.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1953-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Bergner, F.]]></dc:creator>
<dc:creator><![CDATA[Schaper, M.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1953-1</dc:identifier>
<dc:title><![CDATA[Analyse von Rißschließvorgängen mit Ultraschallverfahren]]></dc:title>
<dc:source><![CDATA[30. Tagung des DVM-Arbeitskreises Bruchvorgänge, DVM-Bericht 230, S. 151-160, Dresden, 17.-18.02.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1953-7</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Bergner, F.]]></dc:creator>
<dc:creator><![CDATA[Schaper, M.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1953-7</dc:identifier>
<dc:title><![CDATA[Analyse von Rißschließvorgängen mit Ultraschallverfahren]]></dc:title>
<dc:source><![CDATA[30. Tagung des DVM-Arbeitskreises Bruchvorgänge, DVM-Bericht 230, S. 151-160, Dresden, 17.-18.02.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1954-1</identifier>
<datestamp>2023-05-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Stoemenos, J.]]></dc:creator>
<dc:creator><![CDATA[Pécz, B.]]></dc:creator>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1954-1</dc:identifier>
<dc:title><![CDATA[Epitaxial aluminum carbide formation in 6H-SiC by high-dose Al<sup>+</sup> implantation]]></dc:title>
<dc:source><![CDATA[Appl.Phys.Lett. 74 (1999) 2602]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Aluminum precipitates are formed after Al implantation with dose 3x10<sup>17</sup> cm<sup>-2</sup> at 500°C into single crystalline 6H-SiC. The aluminum carbide (Al<sub>4</sub>C<sub>3</sub>)precipitates are in epitaxial relation with 6H-SiC matrix, having the following orientation relation, [0001]6H-SiC//[0001]Al<sub>4</sub>C<sub>3</sub> and  [11-20]6H-SiC//[11-20]Al<sub>4</sub>C<sub>3</sub>, as transmission electron microscopy reveals. The aluminum carbide appears around the maximum of the Al depth distribution. Silicon precipitates were also detected in the same zone.]]></dc:description>
<dc:subject><![CDATA[High dose implantation]]></dc:subject>
<dc:subject><![CDATA[6H-SiC]]></dc:subject>
<dc:subject><![CDATA[Al₄C₃]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1063/1.123910]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:1959-1</identifier>
<datestamp>2023-04-27</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Gilles, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1959-1</dc:identifier>
<dc:title><![CDATA[Small Angle Neutron Scattering Investigations of the Microstructure of VVER 440-type Reactor Pressure Vessel Steel after Irradiation at 60 °C]]></dc:title>
<dc:source><![CDATA[Journal of Nuclear Materials, Vol. 254 (1998) 143-150]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The formation of point defects and precipitates after neutron irradiation of VVER-440-type reactor pressure vessel steel was investigated by small angle neutron scattering experiments. Irradiation at 60 °C increased the number of point defects, decreased the precipitates, which already exist in the unirradiated state, and formed a new typ of fine-scaled precipitates. Post-irradiation annealing near the operational temperature of the nuclear power plants (270 °C) provoked a slight decrease of the content of point defects and of the irradiation-induced precipitates. The content of these precipitates which are also present in the unirradiated state did not change by annealing. 
]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0022-3115(98)00013-0]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1959-1</dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:1616-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hadek, J.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1616-1</dc:identifier>
<dc:title><![CDATA[Reconstruction of Pointwise Neutron Flux Distribution in a Hexagonal Cassete - Theoretical Background and Implementation into the Code DYN3D/H1.1]]></dc:title>
<dc:source><![CDATA[Proc. oft the 7th Symposium of Atomic Energy Research, Hörnitz, 23. - 26. 09. 1997, p. 469]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The reconstruction of neutron flux density and thermal power density inside the hexagonal cassette of VVER type is described in this paper. The method of succesive smooting combined with folloing analytical solution was used for the detailed pointwise evaluation of neutron fluxes and thermal power densities diestributions in the cassette interior. The program module RECON based on the above mentioned method is presented in the next part of this paper. The results generated by the 3-dimensional reactor dynamic code DYN3D are used as input data for this subprogram. RECON can be used for methodical off-line investigation or to be implemented into the code DYN3D. This implementation is demonstrated at the end of paper.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1616-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hadek, J.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1616-2</dc:identifier>
<dc:title><![CDATA[Reconstruction of Pointwise Neutron Flux Distribution in a Hexagonal Cassete - Theoretical Background and Implementation into the Code DYN3D/H1.1]]></dc:title>
<dc:source><![CDATA[7th Symposium of Atomic Energy
Research, Hörnitz, 23. - 26. 09. 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The reconstruction of neutron flux density and thermal power density inside the hexagonal cassette of VVER type is described in this paper. The method of succesive smooting combined with folloing analytical solution was used for the detailed pointwise evaluation of neutron fluxes and thermal power densities diestributions in the cassette interior. The program module RECON based on the above mentioned method is presented in the next part of this paper. The results generated by the 3-dimensional reactor dynamic code DYN3D are used as input data for this subprogram. RECON can be used for methodical off-line investigation or to be implemented into the code DYN3D. This implementation is demonstrated at the end of paper.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1020-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1020-1</dc:identifier>
<dc:title><![CDATA[Verification of the Code DYN3D/R with the Help of International Benchmarks]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-195 October 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Different benchmarks for reactors with quadratic fuel assemblies were calculated with the code DYN3D/R. In this report comparisons with the results of the reference solutions are carried out. The results of DYN3D/R and the reference calculation for the eigenvalue keff and the power distribution are shown for the steady-state 3-dimensional IAEA-Benchmark. The results of NEACRP-Benchmarks on control rod ejections in a standard PWR were compared with the reference solutions published by the NEA Data Bank. For assessing the accuracy of DYN3D/R results in comparison to other codes the deviations to the reference solutions are considered. Detailed comparisons with the published reference solutions of the NEA-NSC Benchmarks on uncontrolled withdrawal of control rods are made. The influence of the axial nodalization is also investigated. All in all, a good agreement of the DYN3D/R results with the reference solutions can be seen for the considered benchmark problems.

]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:578-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-578-1</dc:identifier>
<dc:title><![CDATA[DYN3D - A 3-DIMENSIONAL CORE MODEL FOR STEADY STATE AND TRANSIENT ANALYSIS IN THERMAL REACTOR]]></dc:title>
<dc:source><![CDATA[Int. Conf. on Physics of Reactors, 16.-20.9.1996, Mito, Japan, Proceedings pp. J-70 - J-79]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The 3D core model DYN3D developed firstly for analyses of transients in thermal reactors with hexagonal fuel assemblies was extended by a new version DYN3D/R for reactors with quadratic fuel elements. The method used in Cartesian geometry is described. Numerical results for benchmarks as the NEACRP rod ejection benchmarks are compared with the reference solutions. Results of  uncontrolled withdrawal of control rod bank are shown. The efficiency of steady-state neutronic calculation by using multiprocessor workstation is presented. 

]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:578-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-578-7</dc:identifier>
<dc:title><![CDATA[DYN3D - A 3-DIMENSIONAL CORE MODEL FOR STEADY STATE AND TRANSIENT ANALYSIS IN THERMAL REACTOR]]></dc:title>
<dc:source><![CDATA[Int. Conf. on Physics of Reactors, 16.-20.9.1996, Mito, Japan, Proceedings pp. J-70 - J-79]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The 3D core model DYN3D developed firstly for analyses of transients in thermal reactors with hexagonal fuel assemblies was extended by a new version DYN3D/R for reactors with quadratic fuel elements. The method used in Cartesian geometry is described. Numerical results for benchmarks as the NEACRP rod ejection benchmarks are compared with the reference solutions. Results of  uncontrolled withdrawal of control rod bank are shown. The efficiency of steady-state neutronic calculation by using multiprocessor workstation is presented. 

]]></dc:description>
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<identifier>HZDR:PUBLDB:2861-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Andronenko, L.]]></dc:creator>
<dc:creator><![CDATA[Andronenko, M.]]></dc:creator>
<dc:creator><![CDATA[Kotov, A.]]></dc:creator>
<dc:creator><![CDATA[Neubert, W.]]></dc:creator>
<dc:creator><![CDATA[Petrov, G.]]></dc:creator>
<dc:creator><![CDATA[Seliverstov, D.]]></dc:creator>
<dc:creator><![CDATA[Vaishnene, L.]]></dc:creator>
<dc:creator><![CDATA[Yatsoura, V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2861-1</dc:identifier>
<dc:title><![CDATA[Measurement of Fragment Production Cross Sections in 1 GeV Proton Interactions with Carbon, Preprint]]></dc:title>
<dc:source><![CDATA[Preprint  PNPI  NP-3-1998 Nr. 2217]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Double differential cross sections of fragment production in 1 GeV proton interactions with carbon were measured with a two-arm spectrometer installed at 30° and 126° with respect to the proton beam line of the PNIP synchrocyclotron. Mass and charge identifications of the fragments were performed by time-of-flight and Bragg spectroscopy methods for both registration angles. The obtained kinetic energy spectra were reproduced by moving source fits with a Maxelllian-like emission pattern.]]></dc:description>
<dc:subject><![CDATA[Cross sections]]></dc:subject>
<dc:subject><![CDATA[isotopes]]></dc:subject>
<dc:subject><![CDATA[Bragg spectroscopy]]></dc:subject>
<dc:type>info:eu-repo/semantics/preprint</dc:type>
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<identifier>HZDR:PUBLDB:1750-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kossok, N.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Schütz, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1750-1</dc:identifier>
<dc:title><![CDATA[Identifikation und diagnostische Überwachung von Zweiphasenströmungen in Rohleitungen]]></dc:title>
<dc:source><![CDATA[IV. Kolloquium "Technische Diagnostik", Dresden, 15. 03. 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Die Analyse von Ultraschall-Transmissionssignalen zeigte, daß eine laufende Identifikation des Stromungszustandes in Rohrleitungen durch einen Aufbau von Relationen zwischen den physikalischen Parametern einer Zweiphasenströmung und den charakteristischen Mustern gemessener Signale möglich ist. Auf dieser Grundlage werden Ergebnisse eines Systems, welches aus einer Ultraschall-Meßeinheit, einer Datenbankeinheit und einer Mustererkennungseinheit besteht, vorgestellt. Dieses System liefert am Ausgang vier Parameter: einen Identifikator fur die Strömungsform, die separaten Volumenströme der flüssigen und der gasformigen Phase und den abgeleiteten Gasgehalt. Der Parametersatz dient als einer von mehreren Eingabensätzen fur das übergeordnete Überwachungs- oder Diagnosesystem. Die mit diesem System erzielten Erkennungsraten liegen zwischen 87 % und 94%.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2084-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Skaddan, M. B.]]></dc:creator>
<dc:creator><![CDATA[Wüst, F.]]></dc:creator>
<dc:creator><![CDATA[Welch, M. J.]]></dc:creator>
<dc:creator><![CDATA[Katzenellenbogen, J. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2084-1</dc:identifier>
<dc:title><![CDATA[Synthesis and biological evaluation of 7alpha Re/Tc "3+1" and cyclopentadienyltri- carbonylmetal (CpTM) estrogen mimics based on the conjugated design]]></dc:title>
<dc:source><![CDATA[13th International symposium on Radiopharmaceutical Chemistry, St. Louis, USA 
27.6.-1.7.99]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The diagnosis and staging of breast cancer could be improved by the development of imaging radiopharmaceuticals that provide a non-invasive determination of the estrogen receptor (ER) status of tumor cells. Towards this goal, we have synthesized a number of Re and Tc-labeled estradiol  (1)  mimics based on the conjugated design, which tethers a metal-containing moiety to an existing steroid. In this study, the 7alpha position of estradiol was chosen as the tether site, due to its well known
tolerance of bulky substituents. <SUP>1</SUP> The metal was stabilized using either the "3+1" design  (2,3), or the cyclopentadienyltricarbonylmetal (CpTM) approach  (4,5,6) . In the "3+1" design, a tridentate ligand and a monodentate ligand surround an oxometal core.<SUP>2</SUP> In the CpTM design, a substituted Cp and three carbonyls are coordinated to a Re/Tc(I) center.<SUP>3,4</SUP> 
The advantages of using the "3+1" and CpTM desings are the well-established stability of both systems, as well as the ability to produce both systems efficiently at the tracer level.<SUP>2,4</SUP>
 The first tether used was a hexyl spacer, and the synthesis of the precursors for targets  2-6  started with THP-protected estradiol  7  (Scheme 1). After oxidation to ketone  8  using a previously published method,<SUP8</SUP> standard alkylation conditions introduced the hexene side chain to form  9 ,  with BEt<SUB>3</SUB> as an additive to stabilize the enolate and prevent O-alkylation.
]]></dc:description>
<dc:subject><![CDATA[estrogen]]></dc:subject>
<dc:subject><![CDATA[radiotracers]]></dc:subject>
<dc:subject><![CDATA[rhenium]]></dc:subject>
<dc:subject><![CDATA[technetium]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:2084-2</identifier>
<datestamp>2019-03-04</datestamp>
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</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Skaddan, M. B.]]></dc:creator>
<dc:creator><![CDATA[Wüst, F.]]></dc:creator>
<dc:creator><![CDATA[Welch, M. J.]]></dc:creator>
<dc:creator><![CDATA[Katzenellenbogen, J. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2084-2</dc:identifier>
<dc:title><![CDATA[Synthesis and biological evaluation of 7alpha Re/Tc "3+1" and cyclopentadienyltri- carbonylmetal (CpTM) estrogen mimics based on the conjugated design]]></dc:title>
<dc:source><![CDATA[J. Labelled Cpd. Radiopharm. 42 (Suppl.1) (1999) S153-S155]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The diagnosis and staging of breast cancer could be improved by the development of imaging radiopharmaceuticals that provide a non-invasive determination of the estrogen receptor (ER) status of tumor cells. Towards this goal, we have synthesized a number of Re and Tc-labeled estradiol  (1)  mimics based on the conjugated design, which tethers a metal-containing moiety to an existing steroid. In this study, the 7alpha position of estradiol was chosen as the tether site, due to its well known
tolerance of bulky substituents. <SUP>1</SUP> The metal was stabilized using either the "3+1" design  (2,3), or the cyclopentadienyltricarbonylmetal (CpTM) approach  (4,5,6) . In the "3+1" design, a tridentate ligand and a monodentate ligand surround an oxometal core.<SUP>2</SUP> In the CpTM design, a substituted Cp and three carbonyls are coordinated to a Re/Tc(I) center.<SUP>3,4</SUP> 
The advantages of using the "3+1" and CpTM desings are the well-established stability of both systems, as well as the ability to produce both systems efficiently at the tracer level.<SUP>2,4</SUP>
 The first tether used was a hexyl spacer, and the synthesis of the precursors for targets  2-6  started with THP-protected estradiol  7  (Scheme 1). After oxidation to ketone  8  using a previously published method,<SUP8</SUP> standard alkylation conditions introduced the hexene side chain to form  9 ,  with BEt<SUB>3</SUB> as an additive to stabilize the enolate and prevent O-alkylation.
]]></dc:description>
<dc:subject><![CDATA[estrogen]]></dc:subject>
<dc:subject><![CDATA[radiotracers]]></dc:subject>
<dc:subject><![CDATA[rhenium]]></dc:subject>
<dc:subject><![CDATA[technetium]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1237-1</identifier>
<datestamp>2023-05-03</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Grigull, S.]]></dc:creator>
<dc:creator><![CDATA[Kruse, O.]]></dc:creator>
<dc:creator><![CDATA[Parascandola, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1237-1</dc:identifier>
<dc:title><![CDATA[Dynamic in Situ Diagnostics Using High-Energy Ion Beam Analysis]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 136-138 (1998) 1203-1211]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[MeV ion beam analysis (IBA) is presented as a powerful tool for in situ, real-time process diagnostics. With minor additional experimental equipment such as diferential pumping or the installation of special detectors, dynamic stoichiometric profiles can be measured during ion beam or plasma exposure. Spectrum acquisition times of the order of a few minutes or less enable the study of fast and transient diffusion effects and transient surface coverages. Examples are given addressing the diffusion and trapping of hydrogen in nickel around room temperature, the ion beam synthesis of carbon±nitrogen films, the ion beam nitriding of stainless steel, and the diagnostics of the layered structure of cubic boron nitride films. The latter example combines stoichiometric in situ analysis using dynamic ERD and structural in situ analysis using optical ellipsometry.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0168-583X(97)00813-6]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1237-1</dc:relation>
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<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2088-1</identifier>
<datestamp>2025-12-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hesse, E.]]></dc:creator>
<dc:creator><![CDATA[Naehring, F. K.]]></dc:creator>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2088-1</dc:identifier>
<dc:title><![CDATA[A lithium liquid metal ion source with narrow angle emission for writing beam lithography]]></dc:title>
<dc:source><![CDATA[Microelectronic engineering 23 (1994) 111-114]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Parameters of a lithium liquid metal ion source have been determined. The angular intensity is the higest yet reported for liquid metal ion sources. This high angular intensity and the large range of light ions suggest the liquid metal ion source to be applied for writing beam lithography. PMMA resist layers were exposed by a focused lithium ion beam.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/0167-9317(94)90116-3]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2088-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2139-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:creator><![CDATA[Artinger, R.]]></dc:creator>
<dc:creator><![CDATA[Schmeide, K.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:creator><![CDATA[Kim, J. I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2139-1</dc:identifier>
<dc:title><![CDATA[Säulenexperimente zur Untersuchung des Einflusses von Huminstoffen auf das Migrationsverhalten von Uran(VI) in einem sandigen Sediment]]></dc:title>
<dc:source><![CDATA[Vortragstagung der GDCh, FG Nuklearchemie, Dresden, 07.-09.09.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Die Untersuchung des Ausbreitungsverhaltens von Actinidionen in wäßrigen Systemen ist unabdingbar zur Erstellung von Risikoabschätzungen zur Langzeitsicherheit von ober- und untertägigen Einrichtungen des ehemaligen Uranerzbergbaus sowie von Endlagern für radioaktiven Abfall. Das Migrationsverhalten von Actinidionen in einem natürlichen Aquifer wird stark von den vorherrschenden Bedingungen beeinflußt. Dabei können Huminstoffe als ubiquitäre, organische Komplexbildner einen entscheidenden Einfluß auf die Immobilisierung bzw. Mobilisierung  der Actinidionen ausüben. 
Die vorliegende Arbeit zeigt Ergebnisse von Säulenexperimenten zur Untersuchung des Einflusses aquatischer Huminstoffe auf das Migrationsverhalten von Uran(VI) in einem sandigen Grundwasserleiter. Für die Untersuchungen wurden ein Grundwasser (GoHy-532, DOC: 30 mg C/l) sowie pleistozäner Flugsand aus dem Gebiet Gorleben verwendet. Der in Säulen (Länge 25 cm und 50 cm; Durchmesser 5 cm) eingebaute Sand wurde unter Inertgasbedingungen (Ar + 1 % CO<sub>2</sub>) mit dem Grundwasser konditioniert. Zur Bestimmung der hydraulischen Parameter der Säulen wurde tritiertes Wasser als Tracer verwendet. Die Migrationsuntersuchungen erfolgten in Abhängigkeit von der Kontaktzeit des Grundwassers mit Uran(VI) (<sup>232</sup>UO<sub>2</sub>Cl<sub>2</sub>) bis zur Injektion auf die Säule, der Grundwasserfließgeschwindigkeit sowie der Säulenlänge.
Die Uran-Durchbruchskurven der Säulenexperimente zeigen, daß ein Teil des Urans ungehindert, an Huminstoffe gebunden und dabei bis zu 5 % schneller als das Wasser durch das Sediment transportiert wird. Der Wiedererhalt an Uran liegt für die durchgeführten Experimente im Bereich zwischen 2 % und 9 %. 
Der ungehinderte, huminstoffgetragene Urantransport ist von der Kontaktzeit des Grundwassers mit Uran(VI) abhängig und steigt mit Erhöhung der Konditionierungszeit. Darüber hinaus nimmt der Wiedererhalt mit abnehmender Grundwasserfließgeschwindigkeit sowie zunehmender Säulenlänge, d.h. mit Erhöhung der Kontaktzeit mit dem Sediment, ab. Dieses Ergebnis deutet auf eine kinetisch kontrollierte Wechselwirkung des huminstoffgebundenen Urans mit der Sandoberfläche hin.
]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3123-7</dc:identifier>
<dc:title><![CDATA[Performance Ratio im Detail: PV-Generatorleistung und Anlagenertrag]]></dc:title>
<dc:source><![CDATA[Tagungsband 15. Symposium Photovoltaische Solarenergie, 15.-17. März 2000, Staffelstein, S. 331]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Das Performance Ratio (PR) als wichtigste Kenngröße einer netzgekoppelten Photovoltaikanlage wird analysiert. Durch Unterscheidung zwischen der nominalen Generatorleistung und der Nennleistung des Generators können einerseits gemessenen Werte des PR interpretiert und andererseits aus gemessenen Werten des PR auf relativ einfache Weise die Generatornennleistung ermittelt werden. Das Verfahren wird an verschiedenen Anlagen verifiziert.
Die qualifizierte Ermittlung des PR einer Anlage ist wichtige Voraussetzung für eine belastbaren Ertragsvorhersage einer PV-Anlage.]]></dc:description>
<dc:subject><![CDATA[Photovoltaik]]></dc:subject>
<dc:subject><![CDATA[Performance Ratio]]></dc:subject>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3123-2</dc:identifier>
<dc:title><![CDATA[Performance Ratio im Detail: PV-Generatorleistung und Anlagenertrag]]></dc:title>
<dc:source><![CDATA[Tagungsband 15. Symposium Photovoltaische Solarenergie, 15.-17. März 2000, Staffelstein, S. 331]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Das Performance Ratio (PR) als wichtigste Kenngröße einer netzgekoppelten Photovoltaikanlage wird analysiert. Durch Unterscheidung zwischen der nominalen Generatorleistung und der Nennleistung des Generators können einerseits gemessenen Werte des PR interpretiert und andererseits aus gemessenen Werten des PR auf relativ einfache Weise die Generatornennleistung ermittelt werden. Das Verfahren wird an verschiedenen Anlagen verifiziert.
Die qualifizierte Ermittlung des PR einer Anlage ist wichtige Voraussetzung für eine belastbaren Ertragsvorhersage einer PV-Anlage.]]></dc:description>
<dc:subject><![CDATA[Photovoltaik]]></dc:subject>
<dc:subject><![CDATA[Performance Ratio]]></dc:subject>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Borodin, V. A.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3125-1</dc:identifier>
<dc:title><![CDATA[Modeling of Ge nanocluster evolution in ion implanted Si02 layers]]></dc:title>
<dc:source><![CDATA[Nuclear Instr. Meth. B 147 (1999) 286]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<identifier>HZDR:PUBLDB:3122-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Pham, M. T.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Steiner, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3122-1</dc:identifier>
<dc:title><![CDATA[Low temperature hydroxyapatite coating of titanium via sodium ion implantation]]></dc:title>
<dc:source><![CDATA[Thin Solid Films 379 (2000) 50-56]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Na ions were implanted into pure Ti surfaces. New surface phases were shown to be incorporated into the surface: sodium titanates Na2TiO3 (in the as-implanted state) and Na2Ti6O13 (after 20 min heating at 700 °C in air). A variable level of rugged surface in porosity and roughness was observed depending on the applied ion dose and energy. Upon exposing to simulated body fluid, such ion-implanted surfaces were revealed to enhancedly elicit hydroxyapatite nucleation and growth. ]]></dc:description>
<dc:subject><![CDATA[biocompatibility]]></dc:subject>
<dc:subject><![CDATA[titanium]]></dc:subject>
<dc:subject><![CDATA[hydroxyapatite]]></dc:subject>
<dc:subject><![CDATA[surface coating]]></dc:subject>
<dc:subject><![CDATA[ion implantation]]></dc:subject>
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<identifier>HZDR:PUBLDB:2140-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:creator><![CDATA[Artinger, R.]]></dc:creator>
<dc:creator><![CDATA[Schmeide, K.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Kim, J. I.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2140-1</dc:identifier>
<dc:title><![CDATA[Investigation of the Migration Behavior of Uranium in an Aquifer System Rich in Humic Substances: Laboratory Column Experiments]]></dc:title>
<dc:source><![CDATA[FZKA 6324, Wissenschaftliche Berichte Forschungszentrum Karlsruhe, (G. Buckau, ed.). Karlsruhe 1999, p. 219.]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The migration behavior of uranium in a sandy aquifer system rich in humic substances was studied in laboratory column experiments. For the investigations we used a Pleistocene aeolian quartz sand and groundwater GoHy-532 from the Gorleben site (Germany). The column experiments were performed in a glove box under anaerobic conditions (Ar + 1 % CO<sub>2</sub>). <sup>232</sup>U(VI)  was used as a tracer. The migration behavior of uranium was investigated as a function of the uranium/groundwater equilibration time before injection into the column, the groundwater flow velocity and the column length.
From the breakthrough curves one can conclude that a part of the injected uranium migrates slightly faster than groundwater. The observed migration behavior is attributed to the association of a part of uranium with humic colloids, which move faster due to size exclusion processes. Depending on the experimental conditions the recovery of humic colloid-bound transported uranium amounts to 0.4 up to 7.6 %. The recovery of non-retarded colloid-borne uranium increases with increasing uranium/groundwater equilibration time before injection into the column. Beyond it, the recovery of humic colloid-borne uranium decreases with decreasing groundwater flow velocity and increasing column length, which corresponds to an increasing residence time in the column. 
The results refer to the fact that the migration behavior of uranium is strongly influenced by kinetically controlled interaction processes of uranium with humic colloids.
]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:creator><![CDATA[Artinger, R.]]></dc:creator>
<dc:creator><![CDATA[Schmeide, K.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Kim, J. I.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2140-2</dc:identifier>
<dc:title><![CDATA[Investigation of the Migration Behavior of Uranium in an Aquifer System Rich in Humic Substances: Laboratory Column Experiments]]></dc:title>
<dc:source><![CDATA[Fourth Project Meeting of the EU project: Effects of Humic Substances on the Migration of Radionuclides: Complexation and Actinides, Leuven, Belgium, 19.-20.11.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The migration behavior of uranium in a sandy aquifer system rich in humic substances was studied in laboratory column experiments. For the investigations we used a Pleistocene aeolian quartz sand and groundwater GoHy-532 from the Gorleben site (Germany). The column experiments were performed in a glove box under anaerobic conditions (Ar + 1 % CO<sub>2</sub>). <sup>232</sup>U(VI)  was used as a tracer. The migration behavior of uranium was investigated as a function of the uranium/groundwater equilibration time before injection into the column, the groundwater flow velocity and the column length.
From the breakthrough curves one can conclude that a part of the injected uranium migrates slightly faster than groundwater. The observed migration behavior is attributed to the association of a part of uranium with humic colloids, which move faster due to size exclusion processes. Depending on the experimental conditions the recovery of humic colloid-bound transported uranium amounts to 0.4 up to 7.6 %. The recovery of non-retarded colloid-borne uranium increases with increasing uranium/groundwater equilibration time before injection into the column. Beyond it, the recovery of humic colloid-borne uranium decreases with decreasing groundwater flow velocity and increasing column length, which corresponds to an increasing residence time in the column. 
The results refer to the fact that the migration behavior of uranium is strongly influenced by kinetically controlled interaction processes of uranium with humic colloids.
]]></dc:description>
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<dc:creator><![CDATA[Kreißig, U.]]></dc:creator>
<dc:creator><![CDATA[Grigull, S.]]></dc:creator>
<dc:creator><![CDATA[Lange, K.]]></dc:creator>
<dc:creator><![CDATA[Nitzsche, P.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2162-1</dc:identifier>
<dc:title><![CDATA[In situ ERDA studies of ion drift processes during anodic bonding of alkali-borosilicate glass to metal]]></dc:title>
<dc:source><![CDATA[Nucl. Instr. Meth. B 136 - 138 (1998) 674]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kruijer, S.]]></dc:creator>
<dc:creator><![CDATA[Nikolov, O.]]></dc:creator>
<dc:creator><![CDATA[Keune, W.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Weber, S.]]></dc:creator>
<dc:creator><![CDATA[Scherrer, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2163-1</dc:identifier>
<dc:title><![CDATA[Depth analysis of phase formation in alpha-Fe after high-dose Al ion implantation]]></dc:title>
<dc:source><![CDATA[J. Appl. Phys. 84 (1998) 6570]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kruijer, S.]]></dc:creator>
<dc:creator><![CDATA[Dobler, M.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Keune, W.]]></dc:creator>
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<dc:title><![CDATA[Depth analysis of Fe-silicide formation after Fe-implantation into Si by DCEMS]]></dc:title>
<dc:source><![CDATA[Int. Conf. Appl. Mössbauer Effect, Rio de Janeiro, Sept. 14 - 20, 1997]]></dc:source>
<dc:date>1997</dc:date>
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<dc:creator><![CDATA[Kruijer, S.]]></dc:creator>
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<dc:creator><![CDATA[Keune, W.]]></dc:creator>
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<dc:title><![CDATA[Depth analysis of Fe-silicide formation after Fe-implantation into Si by DCEMS]]></dc:title>
<dc:source><![CDATA[Hyperfine Interactions (C) 3 (1998) 149]]></dc:source>
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<dc:creator><![CDATA[Große, M.]]></dc:creator>
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<dc:title><![CDATA[SAXS Experiments with High Lateral Resolution by Using of an X-ray Micro Beam]]></dc:title>
<dc:source><![CDATA[Proc. International School and Symposium on Small-Angle Scattering, Matrahaza (Hungary), Oct. 1998, Report 02/E, 1999, S. 41]]></dc:source>
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<dc:creator><![CDATA[Große, M.]]></dc:creator>
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<dc:title><![CDATA[SAXS Experiments with High Lateral Resolution by Using of an X-ray Micro Beam]]></dc:title>
<dc:source><![CDATA[Proc. International School and Symposium on Small-Angle Scattering, Matrahaza (Hungary), Oct. 1998, Report 02/E, 1999, S. 41]]></dc:source>
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<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Hempel, A.]]></dc:creator>
<dc:creator><![CDATA[Gilles, R.]]></dc:creator>
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<dc:title><![CDATA[SANS Investigations of the Irradiation and Annealing Behaviour of the VVER-type Reactor Pressure Vessel Steel 15Xh2MFA]]></dc:title>
<dc:source><![CDATA[BENSC Experimental Reports 1997, Berichte des HMI Berlin, HMI-B552, (1998), S. 244]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Denner, V.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Goerigk, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1963-1</dc:identifier>
<dc:title><![CDATA[ASAXS-Investigations of the Structural Changes in the Reactor Pressure Vessel Steel 15Kh2MFA after Electron Irradiation]]></dc:title>
<dc:source><![CDATA[Jahresbericht HASYLAB 1997, Hamburg (1998)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:1966-1</identifier>
<datestamp>2023-05-05</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Priede, J.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1966-1</dc:identifier>
<dc:title><![CDATA[Hydrothermal wave instability of thermocapillary-driven convection in a transverse magnetic field]]></dc:title>
<dc:source><![CDATA[Journal of Fluid Mechanics (2000), vol. 404, pp. 211-250]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[We study the linear stability of a thermocapilary-driven convection in a planar unbounded layer of an electrically conducting low-Prandtl-number liquid heated from the side and subjected to a transverse magnetic field. The thresholds of convective instability for both longitudional and oblique disturbances are calculated numerically and also asymptotically by considering the Hartmann and Prandtl numbers as large and small parameters, respectively. The magnetic field has a stabilizing effect on the flow with the critical temperature gradient for the transition from steady to oscillatory convection increasing as square of the the field strength. So increases also the critical frequency, while the critical wavelength reduces inversely with field strength. These asymptotics develop in a strong enough magnetic field when the instability is entirely due to the jet of the base flow confined in the Hartmann layer at the free surface. In contrast to the base flow, the critical disturbances, having a long wavelength at small Prandtl numbers, extend from the free surface into the bulk of the liquid layer over a distance exceeding the thickness of the Hartmann layer O(Pr-1/2) times. For Ha ? Pr-1/2 the instability is influenced by the actual depth of the layer. For such moderate magnetic fields the instability threshold is sensitive to the thermal properties of the bottom of the layer and the dependences of the critical parameters on the field strength are more complicated. In the latter case, there is a number of various instability modes possible depending on the thermal boundary conditions and the relative magnitudes of Prandtl and Hartmann numbers.]]></dc:description>
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<identifier>HZDR:PUBLDB:1967-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Priede, J.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1967-1</dc:identifier>
<dc:title><![CDATA[Oscillatory and rotational instabilities in electromagnetic levitation]]></dc:title>
<dc:source><![CDATA[accepted at Symposium Fluid-Flow Phenomena in Metals Processing TMS Annual Meeting, San Diego, USA, February 27 - March 5, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Two different instability mechanisms of electromagnetically levitated bodies are analyzed. The first is due to the virtual coupling between the electric current passing through the magnetic system and the variation of position of the body. This mechanism can result in unstable mass center oscillations of a levitated solid body. Another type of instabilities may occur because of the coupling beween the motion and the electric currents induced in the body. This effect can cause a spontaneous rotation of the body setting in as the frequency of the alternating magnetic field exceeds certain critaical threshold depending on the configuration of the field. This instability can be suppressed by an axial steady magnetic field of strength comparable to that of the levitating field.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1967-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Priede, J.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1967-2</dc:identifier>
<dc:title><![CDATA[Oscillatory and rotational instabilities in electromagnetic levitation]]></dc:title>
<dc:source><![CDATA[Fluid Flow Phenomena in Metals Processing, Eds.: N.El-Kaddah, D.G.C.Robertson, S.T.Johansen, V.R.Voller, The Minerals, Metals & Materials  Society, Warrendale (USA), 1999, pp.593-601]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Two different instability mechanisms of electromagnetically levitated bodies are analyzed. The first is due to the virtual coupling between the electric current passing through the magnetic system and the variation of position of the body. This mechanism can result in unstable mass center oscillations of a levitated solid body. Another type of instabilities may occur because of the coupling beween the motion and the electric currents induced in the body. This effect can cause a spontaneous rotation of the body setting in as the frequency of the alternating magnetic field exceeds certain critaical threshold depending on the configuration of the field. This instability can be suppressed by an axial steady magnetic field of strength comparable to that of the levitating field.]]></dc:description>
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<identifier>HZDR:PUBLDB:1974-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Thess, A.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1974-1</dc:identifier>
<dc:title><![CDATA[Magnetohydrodynamik]]></dc:title>
<dc:source><![CDATA[Physikalische Blätter 54, S. 125, Februar 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Der Traum von magnetohydrodynamischen (MHD)-Generatoren und  MHD-Schiffsantrieben hat sich nicht erfüllt. Die magnetisch gesteuerte Kernfusion läßt auf sich warten. Doch die Stille trügt:; MHD-Technologien  halten erfolgreich Einzug in Metallurgie und Verfahrenstechnik,  MHD-Experimente eröffnen neue Perspektiven für die nichtlineare Physik und  Turbulenzforschung, und selbst das klassische Problem der Entstehung des  Erdmagnetfeldes scheint seiner experimentellen Verifikation nahe zu sein.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:language>ger</dc:language>
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<header>
<identifier>HZDR:PUBLDB:1978-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bojarevics, A.]]></dc:creator>
<dc:creator><![CDATA[Gelfgat, Y.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Cramer, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1978-1</dc:identifier>
<dc:title><![CDATA[The effect of a superimposed steady magnetic field on nonstationary flow driven by a high frequency AC magnetic in an open cavity]]></dc:title>
<dc:source><![CDATA[Workshop "The Use of Magnetic Fields in Crystal Growth and Metals Casting"  
Frankfurt a. M., 1.-2. April 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:531-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Beyer, M.]]></dc:creator>
<dc:creator><![CDATA[Carl, H.]]></dc:creator>
<dc:creator><![CDATA[Schikora, B.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Seidel, A.]]></dc:creator>
<dc:creator><![CDATA[Zschau, J.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-531-1</dc:identifier>
<dc:title><![CDATA[Lieferung von Investitionsgütern zur Erhöhung der Betriebssicherheit des Kernkraftwerkes Saporoshje - Betriebliche Überwachung, 2. Realisierungsstufe -]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-135 April 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Im Rahmen eines Programms des Bundesministeriums für Umwelt, Naturschutz und Reaktorsicherheit zur Zusammenarbeit mit den MOE-Staaten und der GUS auf dem Gebiet der kerntechnischen Sicherheit hat das Forschungszentrum Rossendorf, Institut für Sicherheitsforschung, im Verbund mit dem technischen Überwachungsverein TÜV Rheinland, Institut für Kerntechnik und Strahlenschutz, die einvernehmlich spezifizierten "technischen Mittel für ein System zur verbesserten betrieblichen Überwachung" an das Kernkraftwerk Saporoshje, Ukraine, geliefert und in Betrieb genommen. Im vorliegenden Bericht (Textteil) werden die Lieferungen und Leistungen nach Art und Umfang (Beschaffenheit, Abnahmeprüfung, Übergabe und Inbetriebnahme der technischen Mittel und die für das ukrainische Fachpersonal durchgeführten Schulungsmaßnahmen) bis zur Aufnahme des Probebetriebes am 30. November 1995 beschrieben. Dem Bericht ist ein Anhang A mit Vorschlägen zur Gestaltung der automatisch arbeitenden Überwachungssoftware und ein Anhang B mit wissenschaftsorganisatorischen Details beigefügt.
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:494-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Beyer, M.]]></dc:creator>
<dc:creator><![CDATA[Carl, H.]]></dc:creator>
<dc:creator><![CDATA[Schikora, B.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Seidel, A.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Zschau, J.]]></dc:creator>
<dc:creator><![CDATA[Nowak, K.]]></dc:creator>
<dc:creator><![CDATA[Tolksdorf, P.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-494-2</dc:identifier>
<dc:title><![CDATA[Ein technisches Informationssystem zur verbesserten betrieblichen Überwachung des Kernkraftwerkes Saporoshje/Ukraine]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-171 März 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[In order to improve the operational surveillance of a VVER-1000 unit of the Ukrainian nuclear power plant Zaporosh´ye a technical monitoring system has been specified. The system will enable the state regulatory and supervisory bodies to survey the unit operation independently of operators to assess its safety status, and to impose appropriate conditions. Due to its up-to-date configuration the system provides early indication of any operational incident and emission of radioactive materials connected. Based on the system an immediate warning in mergency situations is possible as well as an effective emergency management. For this purpose 49 different operational parameters of the unit, 18 radiological parameters of the unit and the plant site and 6 meteorological parameters are monitored.
The monitoring concept and its technical realization are described.
]]></dc:description>
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<identifier>HZDR:PUBLDB:494-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Beyer, M.]]></dc:creator>
<dc:creator><![CDATA[Carl, H.]]></dc:creator>
<dc:creator><![CDATA[Schikora, B.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Seidel, A.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Zschau, J.]]></dc:creator>
<dc:creator><![CDATA[Nowak, K.]]></dc:creator>
<dc:creator><![CDATA[Tolksdorf, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-494-1</dc:identifier>
<dc:title><![CDATA[Ein technisches Informationssystem zur verbesserten betrieblichen Überwachung des Kernkraftwerkes Saporoshje/Ukraine]]></dc:title>
<dc:source><![CDATA[Postervortrag zum 4. Kolloquium Technische Diagnostik, TU Dresden, 14./15. März 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[In order to improve the operational surveillance of a VVER-1000 unit of the Ukrainian nuclear power plant Zaporosh´ye a technical monitoring system has been specified. The system will enable the state regulatory and supervisory bodies to survey the unit operation independently of operators to assess its safety status, and to impose appropriate conditions. Due to its up-to-date configuration the system provides early indication of any operational incident and emission of radioactive materials connected. Based on the system an immediate warning in mergency situations is possible as well as an effective emergency management. For this purpose 49 different operational parameters of the unit, 18 radiological parameters of the unit and the plant site and 6 meteorological parameters are monitored.
The monitoring concept and its technical realization are described.
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:350-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Beyer, M.]]></dc:creator>
<dc:creator><![CDATA[Carl, H.]]></dc:creator>
<dc:creator><![CDATA[Schikora, B.]]></dc:creator>
<dc:creator><![CDATA[Seidel, A.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Zschau, J.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-350-1</dc:identifier>
<dc:title><![CDATA[Aufbau eines behördlichen Fernüberwachungssystems zur betrieblichen Überwachung des KKW Saporoshje, Block 5, 1. Realisierungsstufe]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-88 Mai 1995]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[The technical equipment required to improve the operational monitoring of the NPP Zaporozh'ye, Ukraine is represented. it includes two measuring lines for the upgrading of the operational measuring equipment and seven computer-engineering components for establishing an on-site NPP supervision and has been specified in accordance with NPP experts and specialists of the Ukrainian State Supervisory Authority. Furthermore, the results of practical tests are described to check the hard- and software suitability for the down loading of measuring data from an operational computer using an original SM-2M computer made in Russia and a simulator in the laboratory. To prove the exact function a special laboratory variant of the coupling receiver software was been developed. Conceptional proposals for the algorithmic realization of the on-site monitoring of the NPP Zaporozh'ye conclude this report.
]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:1992-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Stefani, F.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Gailitis, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1992-1</dc:identifier>
<dc:title><![CDATA[Numerical Simulation for the Riga Dynamo]]></dc:title>
<dc:source><![CDATA[Workshop "Laboratory Experiments on Dynamo Action", Jurmala (Latvia), June 13-16, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The critical magnetic Reynolds number (Rm) of the Riga dynamo experiment depends 
strongly on the shape of its velocity profiles. For given motor power ressources it is
necessary to optimize these profiles in order to achieve self-excitation of the magnetic
 field. We present a number of one- and two-dimensional calculations for a variety of
axial and azimuthal velocities. Particularly, we test velocity profiles with maximal
 helicity (Bessel function profile). For these velocity profiles the critical Rm can 
be reduced by 20 per cent compared to the value for the solid body rotation profile. 
The used two-dimensional finite difference solver allows to study the effect of 
axially varying profiles, too. In addition, we present some two-dimensional 
calculations for further dynamo experiments in cylindrical geometry, including 
the flow topologies s1t1, s2t1 and s2t2. The influence of the flow direction and
the effect of a surrounding conducting medium on the critical Rm is investigated 
in detail. ]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:2046-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Mändl, S.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2046-2</dc:identifier>
<dc:title><![CDATA[Nitrogen and boron implantation into austenitic stainless steel]]></dc:title>
<dc:source><![CDATA[4th Int. Workshop on PBII, Dearborn, June 2-4, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2046-1</identifier>
<datestamp>2025-12-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Mändl, S.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2046-1</dc:identifier>
<dc:title><![CDATA[Nitrogen and boron implantation into austenitic stainless steel]]></dc:title>
<dc:source><![CDATA[Journal of Vacuum Science and Technology B 17 (2), Mar/Apr 1999, 832-835]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1116/1.590647]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2046-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2089-1</identifier>
<datestamp>2025-12-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hesse, E.]]></dc:creator>
<dc:creator><![CDATA[Mair, G. L. R.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2089-1</dc:identifier>
<dc:title><![CDATA[Parametric investigation of current pulses in a liquid metal ion emitter]]></dc:title>
<dc:source><![CDATA[Journal of Physics D: Appl. Phys. 29 (1996) 2193-2197.]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The presence of current pulses superimposed on the dc level of the ion current in liquid metal ion sources has been known for a long time. This work investigates the behaviour of the pulses for varying temperature and working liquid metal. Attempts are made to explain the differences observed in the threshold current for the appearance of the pulses and also in their terminal, or saturation, frequency. Differences are also found between sources using the same working metal, although the pulse appearance threshold current is the same for a given metal. 
The experimental results indicate that a low source operating temperature is desirable if droplet emission is to be minimized.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1088/0022-3727/29/8/020]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2089-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2090-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Janssen, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2090-1</dc:identifier>
<dc:title><![CDATA[Time of flight corrected beam blanker for ion beam lithography systems]]></dc:title>
<dc:source><![CDATA[Optic 91, No.1 (1992) 46-48]]></dc:source>
<dc:date>1992</dc:date>
<dc:description><![CDATA[For an electrostatic beam blanker the deflection fields are calculated which prevent spurious deflections due to the ion time of flight. The beam blanker consists of two defection electrode pairs arranged symmetrically befor and after the beam cross over. The calculated deflection fields can be realized by declinated surfaces of the blanker electrodes.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2090-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2165-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kulikov, D. V.]]></dc:creator>
<dc:creator><![CDATA[Trushin, Y. V.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Pezoldt, J.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2165-1</dc:identifier>
<dc:title><![CDATA[Theoretical description of high-temperature implantation of 6H-SiC with N<SUP>+</SUP>-and Al<SUP>+</SUP>-ions]]></dc:title>
<dc:source><![CDATA[Techn. Phys. Lett. 24 (1998) 17]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2165-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2167-1</identifier>
<datestamp>2025-04-17</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Groß, B.]]></dc:creator>
<dc:creator><![CDATA[Marion, S.]]></dc:creator>
<dc:creator><![CDATA[Hempelmann, R.]]></dc:creator>
<dc:creator><![CDATA[Grambole, D.]]></dc:creator>
<dc:creator><![CDATA[Herrmann, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2167-1</dc:identifier>
<dc:title><![CDATA[Proton conducting Ba<SUB>3</SUB>Ca<SUB>1.18</SUB>Nb<SUB>1.82</SUB>O<SUB>8.73</SUB>/H<SUB>2</SUB>O: Sol-gel preparation and pressure/composition isotherms]]></dc:title>
<dc:source><![CDATA[Solid State Ionics 109 (1998) 13]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Thin films of Ba3Ca1.18Nb1.82O8.73, prepared in a sol-gel process by multiple dip-coating on silicon wafers were charged with hydrogen by dissociative water
absorption at definite values of water vapour pressures and temperatures. The hydrogen content was determined using nuclear resonance reaction analysis. From the resulting water vapour pressure/hydrogen composition isotherms the absorption enthalpies and the absorption entropy were calculated in the framework of a two site
model, based on Fermi-Dirac statistics. On Ba3Ca1.18Nb1.82O8.73 also impedance spectroscopy was performed yielding the bulk conductivity. From these data
in combination with proton transport numbers and the thermodynamic results as noted above the proton diffusion coefficient could be evaluated.
]]></dc:description>
<dc:subject><![CDATA[solid proton conductors]]></dc:subject>
<dc:subject><![CDATA[water in oxide ceramics]]></dc:subject>
<dc:subject><![CDATA[thermodynamics]]></dc:subject>
<dc:subject><![CDATA[impedance spectroscopy]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Manova, D.]]></dc:creator>
<dc:creator><![CDATA[Dimitrova, V.]]></dc:creator>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Karpuzov, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2168-1</dc:identifier>
<dc:title><![CDATA[Investigation of d.c.-reactive magnetron-sputtered AIN thin films by electron microprobe analysis, X-ray photoelectron spectroscopy and polarized infra-red reflection]]></dc:title>
<dc:source><![CDATA[Surf. Coat. Technol. 106 (1998) 205]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Mantl, S.]]></dc:creator>
<dc:creator><![CDATA[Kappius, L.]]></dc:creator>
<dc:creator><![CDATA[Antons, A.]]></dc:creator>
<dc:creator><![CDATA[Löken, M.]]></dc:creator>
<dc:creator><![CDATA[Klinkhammer, F.]]></dc:creator>
<dc:creator><![CDATA[Dolle, M.]]></dc:creator>
<dc:creator><![CDATA[Zhao, Q. T.]]></dc:creator>
<dc:creator><![CDATA[Mesters, S.]]></dc:creator>
<dc:creator><![CDATA[Buchal, C.]]></dc:creator>
<dc:creator><![CDATA[Bay, H. L.]]></dc:creator>
<dc:creator><![CDATA[Trinkaus, H.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2169-1</dc:identifier>
<dc:title><![CDATA[Growth, patterning and microelectronic applications of epitaxial cobaltdisilicide]]></dc:title>
<dc:source><![CDATA[MRS Symp. Proc. 514 (1998) 145]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Moelle, C.]]></dc:creator>
<dc:creator><![CDATA[Werner, M.]]></dc:creator>
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<dc:creator><![CDATA[Sellschop, M.]]></dc:creator>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
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<dc:creator><![CDATA[Johnston, C.]]></dc:creator>
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<dc:title><![CDATA[Specific heat of single-, poly- and nanocrystalline diamond]]></dc:title>
<dc:source><![CDATA[Diamond and Rel. Mat. 7 (1998) 499]]></dc:source>
<dc:date>1998</dc:date>
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<dc:creator><![CDATA[Noll, K.]]></dc:creator>
<dc:creator><![CDATA[Döbeli, M.]]></dc:creator>
<dc:creator><![CDATA[Grambole, D.]]></dc:creator>
<dc:creator><![CDATA[Herrmann, F.]]></dc:creator>
<dc:creator><![CDATA[Krähenbühl, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2174-1</dc:identifier>
<dc:title><![CDATA[Fluorine enrichement on the surface of antarctic C30 and H chondrites by nuclear reaction analysis (NRA) and the sources of this terrestrial fluorine]]></dc:title>
<dc:source><![CDATA[Meteoritics and Planetary Science 33 (1998) Supplement, A 118]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:creator><![CDATA[Markwitz, A.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Fröb, H.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2183-1</dc:identifier>
<dc:title><![CDATA[Strong blue and violet light emission from silicon- and germanium-implanted silicon-dioxide films]]></dc:title>
<dc:source><![CDATA[Mat. Res. Soc. Symp. Proc. 486 (1998) 175]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Behr, G.]]></dc:creator>
<dc:creator><![CDATA[Dobler, M.]]></dc:creator>
<dc:creator><![CDATA[Teresiak, A.]]></dc:creator>
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<dc:title><![CDATA[Angle dependent Mössbauer spectroscopy on ß-FeSi2 single crystals]]></dc:title>
<dc:source><![CDATA[Hyperfine Interactions (c) 3 (1998) 385]]></dc:source>
<dc:date>1998</dc:date>
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<dc:creator><![CDATA[Soltani-Farshi, M.]]></dc:creator>
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<dc:creator><![CDATA[Bethge, K.]]></dc:creator>
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<dc:title><![CDATA[Content of hydrogen in boron-, carbon-, nitrogen-, oxygen-, fluorine- and neon-implanted titanium]]></dc:title>
<dc:source><![CDATA[SMMIB 97, Gatlinburg, TE, USA, Sept. 1997]]></dc:source>
<dc:date>1997</dc:date>
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<dc:creator><![CDATA[Soltani-Farshi, M.]]></dc:creator>
<dc:creator><![CDATA[Baumann, H.]]></dc:creator>
<dc:creator><![CDATA[Rück, D.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Kreißig, U.]]></dc:creator>
<dc:creator><![CDATA[Bethge, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2188-1</dc:identifier>
<dc:title><![CDATA[Content of hydrogen in boron-, carbon-, nitrogen-, oxygen-, fluorine- and neon-implanted titanium]]></dc:title>
<dc:source><![CDATA[Surf. Coat. Technol. 103-104 (1998) 299]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Wesch, W.]]></dc:creator>
<dc:creator><![CDATA[Karmann, A.]]></dc:creator>
<dc:creator><![CDATA[Börner, H. G.]]></dc:creator>
<dc:creator><![CDATA[Jentschel, M.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2192-2</dc:identifier>
<dc:title><![CDATA[GRID spectroscopy - a new nuclear method for lattice site localization of foreign atoms]]></dc:title>
<dc:source><![CDATA[13th Int. Conf. on Ion Beam Analysis, Lissabon, Portugal, July 28 -August 2, 1997]]></dc:source>
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<dc:creator><![CDATA[Wesch, W.]]></dc:creator>
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<dc:title><![CDATA[GRID spectroscopy - a new nuclear method for lattice site localization of foreign atoms]]></dc:title>
<dc:source><![CDATA[ Nucl. Instr. Meth. B136-138 (1998) 494]]></dc:source>
<dc:date>1998</dc:date>
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<dc:date>1998</dc:date>
<dc:description><![CDATA[The OECD has defined a benchmark for coupled Cartesian neutron kinetics/thermohydraulics code systems. In the first phase, a plant simulation with point kinetics was requested. The purpose was to test the model response.
In this presentation, the dependence of the results obtained by means of the  ATHLET-code from several important parameters is investigated. It was found, that the nodalization of the steamline in the vicinity of the break has an influence on the pressure behaviour and on the time of the return-to-power.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1995-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Alemany, A.]]></dc:creator>
<dc:creator><![CDATA[Shatrov, V.]]></dc:creator>
<dc:creator><![CDATA[Krasilnikov, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1995-1</dc:identifier>
<dc:title><![CDATA[Magnetohydrodynamic flow around bluff bodies]]></dc:title>
<dc:source><![CDATA[Final Report: Januar 1995 - Dezember 1997, Dresden, September 1998, Reference number: INTA]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1995-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1997-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1997-1</dc:identifier>
<dc:title><![CDATA[Marangoni-Konvektion in einer seitlich beheizten ebenen Flüssigmetallschicht unter dem Einfluß eines Magnetfeldes]]></dc:title>
<dc:source><![CDATA[Schlussbericht, Juli 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1997-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1998-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Ulbricht, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1998-1</dc:identifier>
<dc:title><![CDATA[SANS-Investigation of the Irradiation-Induced Changes in Reactor Pressure Vessel Steels]]></dc:title>
<dc:source><![CDATA[Rapport de Experience 1998, LLB Saclay]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1998-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2000-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Kyrki-Rajamäki, R.]]></dc:creator>
<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:creator><![CDATA[Mittag, S.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-2000-1</dc:identifier>
<dc:title><![CDATA[Collection and Review of VVER Transient Measurement Data]]></dc:title>
<dc:source><![CDATA[Technical Report on CEC PHARE project SRR1-95, Forschungszentrum Rossendorf; 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Technical Reports on VVER transients were provided by IVO, NRI, KI, STCNRS and INRNE. The present report gives a survey of the transients documented by the five organisations mentioned. The main actions and effects observed during each transient are briefly described. An overview of the information contained in the five Technical Reports is provided in tabular form. The tables comprise information on the initial states, the measured parameters, and the time regime of the measurement. For each reactor type, VVER­440 and VVER­1000, respectively, one transient is recommended for coupled codes validation in the current project.]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2000-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2002-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Walle, E.]]></dc:creator>
<dc:creator><![CDATA[Valo, M.]]></dc:creator>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Gage, G.]]></dc:creator>
<dc:creator><![CDATA[Wootton, M.]]></dc:creator>
<dc:creator><![CDATA[Keim, E.]]></dc:creator>
<dc:creator><![CDATA[Debarberis, L.]]></dc:creator>
<dc:creator><![CDATA[Horsten, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2002-1</dc:identifier>
<dc:title><![CDATA[Reconstitution Techniques Qualification & Evaluation to Study Ageing Phenomena of Nuclear Pressure Vessel Materials - Resque,]]></dc:title>
<dc:source><![CDATA[Contract FI4SCT960038, Yearly Progress 
Report 1997, European Commission, Euratom Research Framework Programme 1994-1998 "Nuclear Fission Safety", June 1998, AGE-Resque(98)-P003]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2002-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:14249-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Cowan, T. E.]]></dc:creator>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, H.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Wenckstern, H.]]></dc:creator>
<dc:creator><![CDATA[Brandt, M.]]></dc:creator>
<dc:creator><![CDATA[Benndorf, G.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14249-1</dc:identifier>
<dc:title><![CDATA[Structural characterization of H plasma-doped ZnO single crystals by Hall measurements and photoluminescence studies]]></dc:title>
<dc:source><![CDATA[Physica Status Solidi (A) 207(2010), 2426-2431]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Nominally undoped, hydrothermally grown ZnO single crystals have been investigated prior to and after doping in remote H plasma. Characterizations have been made by temperature-dependent Hall effect (TDH) and low temperature photoluminescence (PL) measurements. The H content before and after the doping has been de-termined using nuclear reaction analysis and is compared to the density of shallow donors derived from the TDH measurements. 
The electrical properties of the as-grown ZnO sin-gle crystals are found to differ significantly. This is as-cribed to the density ratio of shallow donors and compen-sating acceptors. PL measurements showed that AlZn, GaZn, and interstitial zinc (Zni) are prominent shallow donors in the as-grown samples.
Remote H plasma treatment produced a metallic conducting near-surface layer thus masking the electrical properties of the bulk. The electrical properties of the in-vestigated samples are very similar after the treatment, independent of the as-grown state, because the density of shallow donors far exceeds that of compensating accep-tors in the affected near-surface region. The maximum of the broad near-band-edge emission is found to be located at 3.3595 eV due to the high doping density.]]></dc:description>
<dc:subject><![CDATA[ZnO single crystals]]></dc:subject>
<dc:subject><![CDATA[H plasma doping]]></dc:subject>
<dc:subject><![CDATA[temperature-dependent Hall effect]]></dc:subject>
<dc:subject><![CDATA[low temperature photoluminescence]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1002/pssa.201026311]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14249-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2047-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pham, M. T.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Steiner, G.]]></dc:creator>
<dc:creator><![CDATA[Oswald, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2047-1</dc:identifier>
<dc:title><![CDATA[Interface-mediated synthesis of hydroxyapatite]]></dc:title>
<dc:source><![CDATA[J. Biomed. Materials Research 59 (2002) 254-258]]></dc:source>
<dc:date>2002</dc:date>
<dc:description><![CDATA[The interface water vapour-titanium was employed for a controlled synthesis of surface-supported hydroxyapatite. In this approach, a Ti surface was doped with Ca and P by ion implantation and then subjected to a hydrothermal treatment in a water vapour autoclave. Ion implantation served to prepare a reactive blend of finely dispersed reactants in a stoichiometric ratio incorporated within the network of an outermost layer of the substrate surface. Needle-like carbonate hydroxyapatite in an overlayer was identified to deposit on the surface. The results suggest interface-mediated thin film formation and phase transformation.]]></dc:description>
<dc:subject><![CDATA[biomaterials]]></dc:subject>
<dc:subject><![CDATA[surface coating]]></dc:subject>
<dc:subject><![CDATA[hydroxyapatite]]></dc:subject>
<dc:subject><![CDATA[titanium implants]]></dc:subject>
<dc:subject><![CDATA[ion implantation]]></dc:subject>
<dc:subject><![CDATA[materials technology]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2047-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2048-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Gabriel, F.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-2048-1</dc:identifier>
<dc:title><![CDATA[Bericht der Frühjahrstagung der Studiengruppe für Elektronische Instrumentierung vom 22.-24. März 1999 in der Ruhr-Universität in Bochum]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-261 Mai 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2048-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:283-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brünig, D.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Dittmann, A.]]></dc:creator>
<dc:creator><![CDATA[Doltze, T.]]></dc:creator>
<dc:creator><![CDATA[Gassel, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-283-1</dc:identifier>
<dc:title><![CDATA[Betriebserfahrungen mit großen solarthermischen Anlagen in Sachsen]]></dc:title>
<dc:source><![CDATA[Tagungsserie Klimagipfel der Fördergesellschaft Erneuerbare Energien Berlin/Brandenburg e.V., Wildau, 20.01.1995]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Die zwei größten solarthermischen Anlagen Sachsens werden im Anlagenaufbau und hinsichtlich der bisher vorliegenden Betriebserfahrungen vorgestellt und verglichen. Dies ist zum einen eine Anlage in Freital mit 90 m² Absorberfläche zur Warmwassererzeugung und Fernwärmeeinspeisung. Zum zweiten handelt es sich um sieben Anlagen mit je 100 m² Absorberfläche zur Warmwasserbereitung in Wohnblöcken in Oederan. Beide Anlagen arbeiten störungsfrei. Die geplanten solaren Erträge konnten in der ersten Betriebsperiode nicht erreicht werden. In der Freitaler Anlage lag die Rücklauftemperatur des Fernwärmenetzes etwa 20 K über der Auslegungstemperatur, was zu schlechten Kollektorwirkungsgraden führte. In Oederan betrug der Warmwasserbedarf nur ca. 60 % des Auslegungswertes mit dem gleichen negativen energetischen Effekt.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-283-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2091-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Hesse, E.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2091-1</dc:identifier>
<dc:title><![CDATA[Ion beam synthesis of CoSi<sub>2</sub> - microstructures by means of a high current focused ion beam]]></dc:title>
<dc:source><![CDATA[Proceedings of the Ninth International Conference on Ion Beam Modification of Materials Canberra, Australia, 5-10 February, 1995]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[The bfabrication of CoSi<sub>2</sub> - structures by stoichiometric implantation of Co<sup>+</sup> (E = 30...35 keV, I<sub>ion</sub> = 1.3nA) and Co<sup>++</sup> ions (E = 60 keV, I<sub>ion</sub> = 0.6nA) at doses between 0.3 and 5x10<sup>17</sup> cm<sup>-2</sup> and a subsequent two step annealing (600°C, 60 min; 1000°C, 30 min in N<sub>2</sub>) is demonstrated. The dose dependence and the influence of the substrate temperature were studied. The quality of the silicide submicron structures was investigated by SEM, EDX and electrical measurements.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2935-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-2935-1</dc:identifier>
<dc:title><![CDATA[International Workshop on Measuring Techniques for Liquid Metal Flows (MTLM), Rossendorf, 11.-13.10.99, Proceedings]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-278 November 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The International Workshop on "Measuring Techniques in Liquid Metal Flows" (MTLM Workshop) was organised in frame of the Dresden "Innovationskolleg Magnetofluiddynamik". The subject of the MTLM Workshop was limited to methods to determine physical flow quantities such as velocity, pressure, void fraction, inclusion properties, crystallisation fronts etc. The present proceedings contain abstracts and viewgraphs of the oral presentations.
During the last decades numerical simulations have become an important tool in industry and research to study the structure of flows and the properties of heat and mass transfer. However, in case of liquid metal flows there exists a significant problem to validate the codes with experimental data due to the lack of available measuring techniques. Due to the material properties (opaque, hot, chemical aggressive) the measurement of flow quantities is much more delicate in liquid metals compared to ordinary water flows. The generalisation of results obtained by means of water models to real liquid metal flows has often to be considered as difficult due to the problems to meet the actual values of non-dimensional flow parameters (Re, Pr, Gr, Ha, etc.). Moreover, a strong need has to be noted to make measuring techniques available to monitor and to control flow processes in real industrial facilities.
]]></dc:description>
<dc:subject><![CDATA[measuring techniques]]></dc:subject>
<dc:subject><![CDATA[liquid metals]]></dc:subject>
<dc:subject><![CDATA[semiconducting melts]]></dc:subject>
<dc:subject><![CDATA[magnetic fields]]></dc:subject>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2562-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hornauer, U.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2562-1</dc:identifier>
<dc:title><![CDATA[Improvement of the high temperature oxidation resistance of Ti50Al via ion implantation]]></dc:title>
<dc:source><![CDATA[11th Int. Conf. on Ion Beam Modification of Materials, Amsterdam, the Netherlands,
Aug. 31 - Sept. 4, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1610-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Nitzsche, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1610-1</dc:identifier>
<dc:title><![CDATA[SANS investigations of the irradiation-caused structural damages in VVER 440-type reactor pressure vessel steels]]></dc:title>
<dc:source><![CDATA[Physica B 234 - 236 (1997), 997 - 998]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Small-angle neutron scattering (SANS) experiments were performed at KWS2 facility of the KFA Jülich for investigating the defect structures, which are produced by neutron irradiation in Russian Cr-Mo-V alloyed reactor pressure vessel steel. Irradiation and post-irradiation annealing considerably change both SANS intensity and its course  in the Guinier plot, which was analysed by the Glatter method. As a rule, bimodal size distribution functions were found with a first maximum at a radius of 1-2 nm and a second maximum at 6-8 nm. Irradiation increases the first maximum, annealing reduced it.
]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2096-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Böhm, A.]]></dc:creator>
<dc:creator><![CDATA[Brinkmann, K.-T.]]></dc:creator>
<dc:creator><![CDATA[Dshemuchadse, S.]]></dc:creator>
<dc:creator><![CDATA[Freiesleben, H.]]></dc:creator>
<dc:creator><![CDATA[Herrmann, P.]]></dc:creator>
<dc:creator><![CDATA[Jakob, B.]]></dc:creator>
<dc:creator><![CDATA[Koch, H.]]></dc:creator>
<dc:creator><![CDATA[Krug, J.]]></dc:creator>
<dc:creator><![CDATA[Kuhlmann, E.]]></dc:creator>
<dc:creator><![CDATA[Lange, J. S.]]></dc:creator>
<dc:creator><![CDATA[Michel, P.]]></dc:creator>
<dc:creator><![CDATA[Möller, K.]]></dc:creator>
<dc:creator><![CDATA[Schamlott, A.]]></dc:creator>
<dc:creator><![CDATA[Schönmeier, P.]]></dc:creator>
<dc:creator><![CDATA[Schülke, A.]]></dc:creator>
<dc:creator><![CDATA[Steinke, M.]]></dc:creator>
<dc:creator><![CDATA[Sun, G. Y.]]></dc:creator>
<dc:creator><![CDATA[Würschig-Pörsel, M.]]></dc:creator>
<dc:creator><![CDATA[Zielinski, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2096-1</dc:identifier>
<dc:title><![CDATA[The COSY-TOF barrel detector]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research A]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[A barrel-shaped scintillator hodoscope was developed as part of the time-of-flight spectrometer TOF operated at an external beam line of the cooler synchrotron COSY. The COSY-TOF spectrometer is used mainly to perform kinematically complete experiments on light meson production and proton-proton bremsstrahlung  in proton-proton collisions for laboratory energies up to 2.5 GeV.
The newly developed scintillator hodoscope (BARREL1), one of several detector segments of the COSY-TOF spectrometer, consists of one layer of 96 scintillator bars of 15 mm thickness arranged to form a barrel with 3 m in diameter and 2.85 m in length.
For any given interaction process the TOF spectrometer allows to determine the velocity vectors of all charged ejectiles emerging from the target by measuring the time of flight between the start and the stop detector as well as the point of impact   on the stop detector. For the BARREL1 detector the position information is obtained by two-sided light read-out of the scintillator bars. For minimum ionizing particles the spatial resolution was measured to be Delta z(FWHM) = 8 cm, corresponding to a polar angle resolution in the range  0.57 to 2.86 degrees, depending on the hit position. The binning in azimuthal angular direction amounts to 360/96 = 3.75 degrees. For the time-of-flight resolution of minimum ionizing particles a value of Delta t(FWHM) = 0.61 ns was obtained.]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:14190-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Donat, C. K.]]></dc:creator>
<dc:creator><![CDATA[Walter, B.]]></dc:creator>
<dc:creator><![CDATA[Kayser, T.]]></dc:creator>
<dc:creator><![CDATA[Deuther-Conrad, W.]]></dc:creator>
<dc:creator><![CDATA[Schliebs, R.]]></dc:creator>
<dc:creator><![CDATA[Nieber, K.]]></dc:creator>
<dc:creator><![CDATA[Bauer, R.]]></dc:creator>
<dc:creator><![CDATA[Haertig, W.]]></dc:creator>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14190-1</dc:identifier>
<dc:title><![CDATA[Effects of lateral fluid percussion injury on cholinergic markers in the newborn piglet brain]]></dc:title>
<dc:source><![CDATA[International Journal of Developmental Neuroscience 28(2010), 31-38]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Traumatic brain injury is a leading cause of death and disability in children. Studies using adult animal models showed alterations of the central cholinergic neurotransmission as a result of trauma. However, there is a lack of knowledge about consequences of brain trauma on cholinergic function in the immature brain. It is hypothesized that trauma affects the relative acetylcholine esterase activity and causes a loss of cholinergic neurons in the immature brain. Severe fluid percussion trauma (FP-TBI, 3.8  0.3 atm) was induced in 15 female newborn piglets, monitored for 6 h and compared with 12 control animals. The hemispheres ipsilateral to FP-TBI obtained from seven piglets were used for acetylcholine esterase istochemistry on frozen sagittal slices, while regional cerebral blood flow and oxygen availability was determined in the remaining eight FP-TBI animals. Post-fixed slices were immunohistochemically labelled for choline acetyltransferase as well as for lowaffinity neurotrophin receptor in order to characterize cholinergic neurons in the basal forebrain. Regional cerebral blood flow and brain oxygen availability were reduced during the first 2 h after FPTBI (P < 0.05). In addition, acetylcholine esterase activity was significantly increased in the neocortex, basal forebrain, hypothalamus and medulla after trauma (P < 0.05), whereas the number of choline acetyltransferase and low-affinity neurotrophin receptor positive cells in the basal forebrain were unaffected by the injury. Thus, traumatic brain injury evoked an increased relative activity of the acetylcholine esterase in the immature brain early after injury, without loss of cholinergic neurons in the basal forebrain. These changes may contribute to developmental impairments after immature traumatic brain injury.]]></dc:description>
<dc:subject><![CDATA[Traumatic brain injury]]></dc:subject>
<dc:subject><![CDATA[Immature brain]]></dc:subject>
<dc:subject><![CDATA[Cholinergic system]]></dc:subject>
<dc:subject><![CDATA[Acetylcholine esterase]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/j.ijdevneu.2009.10.001]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:3107-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Assmann, W.]]></dc:creator>
<dc:creator><![CDATA[Huber, H.]]></dc:creator>
<dc:creator><![CDATA[Karamian, S. A.]]></dc:creator>
<dc:creator><![CDATA[Grüner, F.]]></dc:creator>
<dc:creator><![CDATA[Mieskes, H. D.]]></dc:creator>
<dc:creator><![CDATA[Andersen, J. U.]]></dc:creator>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3107-1</dc:identifier>
<dc:title><![CDATA[Transverse cooling or heating of channeled ions by electron capture and loss]]></dc:title>
<dc:source><![CDATA[Phys. Rev. Lett. 83 (1999) 1759]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[We have measured the angular distribution of energetic heavy ions after passage through a Si crystal for an incident beam with an isotropic angular distribution over angles much larger than the critical angle for channeling. Strong redistribution of the flux has been observed, in some cases an enhancement along channeling directions, and in other cases a reduction. The phenomenon is not predicted by channeling  theory and cannot be reproduced by computer simulations. We propose a new mechanism: cooling or heating of the transverse motion of channeled ions due to repeated capture and loss of electrons. The cooling effect is analogous to Sisyphus cooling of very cold, trapped atoms in a strong laser field.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2201-2</identifier>
<datestamp>2025-04-17</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ulbricht, A.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Strunz, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2201-2</dc:identifier>
<dc:title><![CDATA[Small Angle Scattering Study Concerning the Effect of Residual Elements on the Radiation Behaviour of Iron Alloys]]></dc:title>
<dc:source><![CDATA[Physica B 276-278 (2000) 936-938]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[For better understanding of the influence of the deleterious elements on the neutron embrittlement of reactor pressure vessel steels, the microstructural evolution due to neutron irradiation was investigated by SANS experiments at ternary iron alloys with different contents of copper and phosphorus. In every case irradiation produced nanoscaled inhomogeneities. The volume fraction of the inhomogeneities incrases with the copper content but not with the phosphorus content. Surprisingly, the high-pure alloy shows a relatively high irradiation effect. The irradiation defects vary in type and kinetic of evolution for the different alloys.]]></dc:description>
<dc:subject><![CDATA[small angle scattering]]></dc:subject>
<dc:subject><![CDATA[radiation damage]]></dc:subject>
<dc:subject><![CDATA[neutron embrittlement]]></dc:subject>
<dc:subject><![CDATA[iron alloy]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0921-4526(99)01605-1]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2201-2</dc:relation>
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<header>
<identifier>HZDR:PUBLDB:2201-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ulbricht, A.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Strunz, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2201-1</dc:identifier>
<dc:title><![CDATA[Small Angle Scattering Study Concerning the Effect of Residual Elements on the Radiation Behaviour of Iron Alloys]]></dc:title>
<dc:source><![CDATA[ECNS'99, 2. European Conference on Neutron Scattering, Sept. 1999, Budapest,
PHYSICA B 276-278 (2000) 936-938]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[For better understanding of the influence of the deleterious elements on the neutron embrittlement of reactor pressure vessel steels, the microstructural evolution due to neutron irradiation was investigated by SANS experiments at ternary iron alloys with different contents of copper and phosphorus. In every case irradiation produced nanoscaled inhomogeneities. The volume fraction of the inhomogeneities incrases with the copper content but not with the phosphorus content. Surprisingly, the high-pure alloy shows a relatively high irradiation effect. The irradiation defects vary in type and kinetic of evolution for the different alloys.]]></dc:description>
<dc:subject><![CDATA[small angle scattering]]></dc:subject>
<dc:subject><![CDATA[radiation damage]]></dc:subject>
<dc:subject><![CDATA[neutron embrittlement]]></dc:subject>
<dc:subject><![CDATA[iron alloy]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2201-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<identifier>HZDR:PUBLDB:2202-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Nicolai, R.]]></dc:creator>
<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:creator><![CDATA[Bubner, M.]]></dc:creator>
<dc:creator><![CDATA[Klöcking, R.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2202-1</dc:identifier>
<dc:title><![CDATA[FTIR-Untersuchungen zur Komplexierung von Uran(VI) durch Huminsäuren]]></dc:title>
<dc:source><![CDATA[Tagung der Deutschen Gesellschaft für Moor- und Torfkunde e.V.,Sektion IV - Physik, Chemie, Biologie
Bad Elster, 07.-09.10.1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Aufgrund der nur unvollkommen erfaßbaren, keineswegs stabilen chemischen Struktur und Funktionalität von Huminsäuren aus natürlichen Recourcen haben operationell mit HS übereinstimmende, synthetische Polymere als Modellhuminsäuren in vielen Bereichen der experimentellen Wissenschaften Eingang gefunden. Sie sind vor dem Hintergrund der Umweltkontaminationen durch toxische und radiotoxische Schwermetalle besonders für Bindungsstudien mit Metallionen interessant, da ihre Funktionalität durch Variation der Precursoren und  der Synthesebedingungen in weiten Grenzen "eingestellt" werden kann.

Wir haben FTIR-spektrometrisch die festen Komplexe von Uran(VI) mit unterschiedlichen, gut charaktersierten Huminsäuren, zwei natürlichen Huminsäuren (Aldrich-Huminsäure und eine aus Moorwasser des "Kleinen Kranichsees" isolierte Huminsäure) sowie drei synthetischen Huminsäuren (zwei Melanoidinfraktionen sowie das Oxidationsprodukt von 3,4,5 Trihydroxybenzoesäure), verglichen. Trotz unterschiedlicher Herkunft der Huminsäuren, die in ihren FTIR-Spektren deutlich wird, scheint die Urananbindung an die Huminsäuren sehr ähnlich zu sein, was durch EXAFS-Untersuchungen an Uranylkomplexen natürlicher Huminsäuren und synthetischer Huminsäuren vom Melanoidintyp gestützt wird. Sowohl die asymmetrischen UO22+-Streckschwingungen im mittleren Infrarot, die wir zwischen 933.5 cm-1 und 923.1 cm-1 registrieren, als auch die UO22+-Deformationsschwingungen im fernen Infrarot zwischen 264.8 cm-1 und 260.6 cm-1 sind gut miteinander vergleichbar. 
Die Einflußnahmen der strukturellen und funktionellen Unterschiede der Huminsäuren spiegeln sich in unterschiedlichen Verschiebungen der Uranylbanden wieder. 
]]></dc:description>
<dc:subject><![CDATA[FTIR-Spektroskopie]]></dc:subject>
<dc:subject><![CDATA[Huminsäuren, Uranyl-Huminsäurekomplexe]]></dc:subject>
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<identifier>HZDR:PUBLDB:2203-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
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<dc:creator><![CDATA[Deshkovskaya, A. A.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2203-1</dc:identifier>
<dc:title><![CDATA[Ion bombardment stimulated phase formation in quartz glasses]]></dc:title>
<dc:source><![CDATA[11.th Int. Conf. on Ion Beam Modification of Materials, Amsterdam, Netherlands,  Aug. 31 - Sept. 4, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2204-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Dobler, M.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2204-1</dc:identifier>
<dc:title><![CDATA[Untersuchung der Eisendisilizidbildung nach der Implantation von Fe in Si]]></dc:title>
<dc:source><![CDATA[10. Arbeitstagung Angewandte Oberflächenanalytik AOFA 10, Kaiserslautern, Sept. 6-10, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2205-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Dobler, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2205-1</dc:identifier>
<dc:title><![CDATA[CEMS-Eisendisilizide-Ionenstrahlverfahren]]></dc:title>
<dc:source><![CDATA[IX. Mößbauerkolloquium Freiberg, Sept. 28-30, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<identifier>HZDR:PUBLDB:2207-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Fichtner, P.]]></dc:creator>
<dc:creator><![CDATA[Kaschny, J. R.]]></dc:creator>
<dc:creator><![CDATA[Behar, M.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2207-1</dc:identifier>
<dc:title><![CDATA[The effects of annealing temperature on the formation of helium filled structures in silicon]]></dc:title>
<dc:source><![CDATA[11th Int. Conf. on Ion Beam Modification of Materials (IBMM'98), Amsterdam, Aug. 31 -  Sept. 4, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:2209-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Fischer, C. G.]]></dc:creator>
<dc:creator><![CDATA[Connell, S. H.]]></dc:creator>
<dc:creator><![CDATA[Coleman, P. G.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Malik, F.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Britton, D. T.]]></dc:creator>
<dc:creator><![CDATA[Sellschop, J. P. F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2209-1</dc:identifier>
<dc:title><![CDATA[A slow positron beam investigation of positron-defect interactions in single crystalline synthetic type IB diamonds and a natural type IIB diamond]]></dc:title>
<dc:source><![CDATA[ 8th Int. Workshop on Slow Positron Beam Techniques for Solids and Surface (SLOPOS - 8), Cape Town, Sept. 6 - 12, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:2210-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2210-1</dc:identifier>
<dc:title><![CDATA[Applications of infrared spectroscopy in materials research]]></dc:title>
<dc:source><![CDATA[33. Holzhau-Meeting, March 30, April 3, 1998  (invited lecture)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2211-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2211-1</dc:identifier>
<dc:title><![CDATA[In plane anisotropy of IBAD t-BN films]]></dc:title>
<dc:source><![CDATA[Gordon Research Conference on Plasma Processing Science, Tilton School, New Hampshire, USA, Aug. 9 - 14, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2212-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2212-1</dc:identifier>
<dc:title><![CDATA[Investigation of in-plane anisotropy of IBAD t-BN films]]></dc:title>
<dc:source><![CDATA[DACH - Kolloquium, Giengen, Oct. 6-8, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<identifier>HZDR:PUBLDB:2213-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2213-1</dc:identifier>
<dc:title><![CDATA[Analysis of mechanisms in ECR-PECVD of BN films using in situ ellipsometry]]></dc:title>
<dc:source><![CDATA[DACH - Kolloquium, Giengen, Oct. 6-8, 1998]]></dc:source>
<dc:date>1998</dc:date>
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<identifier>HZDR:PUBLDB:2214-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Ganetsos, T.]]></dc:creator>
<dc:creator><![CDATA[Tsamakis, D.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Mair, G. L. R.]]></dc:creator>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Aidinis, C.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2214-2</dc:identifier>
<dc:title><![CDATA[Si<SUB>1-x</SUB>Ge<SUB>x</SUB> structures fabricated by focused ion beam implantation]]></dc:title>
<dc:source><![CDATA[J. de Phys. IV 8 (1998) Pr3 - 109]]></dc:source>
<dc:date>1998</dc:date>
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<identifier>HZDR:PUBLDB:2214-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Ganetsos, T.]]></dc:creator>
<dc:creator><![CDATA[Tsamakis, D.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Mair, G. L. R.]]></dc:creator>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Aidinis, C.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2214-1</dc:identifier>
<dc:title><![CDATA[Si<SUB>1-x</SUB>Ge<SUB>x</SUB> structures fabricated by focused ion beam implantation]]></dc:title>
<dc:source><![CDATA[Conference in Low Temperature Devices, Toscane, Italy, June 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<header>
<identifier>HZDR:PUBLDB:2215-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gong, M.]]></dc:creator>
<dc:creator><![CDATA[Beling, C. D.]]></dc:creator>
<dc:creator><![CDATA[Fung, S.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Wirth, H. D.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[You, Z.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2215-1</dc:identifier>
<dc:title><![CDATA[Ions and electron-irradiation induced deep levels in n-type and p-type 6H-SiC]]></dc:title>
<dc:source><![CDATA[MRS 1998 Spring Meeting, San Francisco, April 13-17, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:language>eng</dc:language>
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<record>
<header>
<identifier>HZDR:PUBLDB:1749-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Gebbeken, B.]]></dc:creator>
<dc:creator><![CDATA[Eggers, R.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1749-1</dc:identifier>
<dc:title><![CDATA[Entspannungsverdampfung während der Druckentlastung von Co<sub>2</sub> aus dem überkritischen Anfangszustand]]></dc:title>
<dc:source><![CDATA[GVC-Fachausschuß Mehrphasenströmungen, Vortrag 2.27, Lahnstein, 06. - 08. März 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Druckentlastungsexperimente der TU Hamburg/Harburg von überkritischem CO<sub>2</sub> aus einem Druckbehälter werden vorgestellt. Dabei wurden mit einer Gamma-Durchstrahlung axiale Dampfgehaltsprofile im System CO<sub>2</sub>-flüssig und CO<sub>2</sub>-gasförmig sowie Druck- und Temperaturverläufe gemessen. Die Experimente, insbesondere die lokalen Gasgehalte, können durch das Programm BLDN des FZR mit Erfolg nachgerechnet werden, wobei verschiedene Driftansätze auf ihre Anwendbarkeit auf CO<sub>2</sub> hin überprüft wurden.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1749-1</dc:relation>
<dc:audience>Researchers</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1783-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schäfer, F.]]></dc:creator>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1783-1</dc:identifier>
<dc:title><![CDATA[Rechnungen zum 1%-Leck an der Versuchsanlage PMK-2 mit dem Code ATHLET]]></dc:title>
<dc:source><![CDATA[Proc. Jahrestagung Kerntechnik, Nürnberg, 16. - 18. Mai 1995, S. 79 - 82]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Die ungarische Versuchsanlage PMK-2 ist ein im Volumenmaßstab 1:2070 skaliertes Modell einer Reaktoranlage vom Typ WWER-440. Das Experiment 1%-Leck im kalten Strang" ist die Wiederholung eines Experiments von 1990 mit erweiterter
Instrumentierung - insbesondere Nadelsonden aus dem FZ Rossendorf. Das Leck befindet sich am oberen Teil des Ringspalts und hat einen Durchmesser von 1 mm. Für das Experiment wird angenommen, daß zur Notkühlung nur das Hochdrucknotkühlsystem (HPIS) verfügbar ist. Im Forschungszentrum Rossendorf wurden Nachrechnungen zu dem vorgestellten Experiment mit dem Code ATHLET Mod1.1 Cycle A durchgeführt. Wie der Vergleich von Rechnung und Experiment zeigt, werden alle Phänomene des Experiments in der Rechnung gut wiedergegeben. Insbesondere konnten die beobachteten Instabilitäten im Naturumlauf sehr gut modelliert werden.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1783-1</dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:1783-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schäfer, F.]]></dc:creator>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1783-7</dc:identifier>
<dc:title><![CDATA[Rechnungen zum 1%-Leck an der Versuchsanlage PMK-2 mit dem Code ATHLET]]></dc:title>
<dc:source><![CDATA[Proc. Jahrestagung Kerntechnik, Nürnberg, 16. - 18. Mai 1995, S. 79 - 82]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Die ungarische Versuchsanlage PMK-2 ist ein im Volumenmaßstab 1:2070 skaliertes Modell einer Reaktoranlage vom Typ WWER-440. Das Experiment 1%-Leck im kalten Strang" ist die Wiederholung eines Experiments von 1990 mit erweiterter
Instrumentierung - insbesondere Nadelsonden aus dem FZ Rossendorf. Das Leck befindet sich am oberen Teil des Ringspalts und hat einen Durchmesser von 1 mm. Für das Experiment wird angenommen, daß zur Notkühlung nur das Hochdrucknotkühlsystem (HPIS) verfügbar ist. Im Forschungszentrum Rossendorf wurden Nachrechnungen zu dem vorgestellten Experiment mit dem Code ATHLET Mod1.1 Cycle A durchgeführt. Wie der Vergleich von Rechnung und Experiment zeigt, werden alle Phänomene des Experiments in der Rechnung gut wiedergegeben. Insbesondere konnten die beobachteten Instabilitäten im Naturumlauf sehr gut modelliert werden.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1783-7</dc:relation>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2004-1</identifier>
<datestamp>2025-12-03</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Gokhman, A.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2004-1</dc:identifier>
<dc:title><![CDATA[Dependence of the Ratio between Magnetic and Nuclear Small Angle Neutron Scattering on the Size of the Heterogeneities]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 160 (2000) 515-520]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The ratio between magnetic and nuclear small angle neutron scattering (SANS) can provide additional information about the composition and structure of the scattering inhomogenities. The method fails if the material system does not meet the two-phase approach. In this case, by using the indirect transformation method, the ratio can more generally be defined and related to the dependence of the scattering particle size. The method is derived and applied to model systems with two types of non-magnetic spheric inhomogenities in a ferromagnetic matrix.]]></dc:description>
<dc:subject><![CDATA[Analysis of materials]]></dc:subject>
<dc:subject><![CDATA[Neutron scattering]]></dc:subject>
<dc:subject><![CDATA[radiation damage]]></dc:subject>
<dc:subject><![CDATA[reactor pressure vessel steel]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0168-583X(99)00625-4]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2004-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:3448-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Rossberg, A.]]></dc:creator>
<dc:creator><![CDATA[Hennig, C.]]></dc:creator>
<dc:creator><![CDATA[Reich, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3448-1</dc:identifier>
<dc:title><![CDATA[Characterization of Chromium Complexes in Chrome Tannins, Leather, and Gelatin Using Extended X-ray Absorption Fine Structure (EXAFS) Spectroscopy]]></dc:title>
<dc:source><![CDATA[Journal of the American Leather Chemists Association 96, 133-147 (2001)]]></dc:source>
<dc:date>2001</dc:date>
<dc:description><![CDATA[Chrome tannage is the most intensively investigated tanning process. Nevertheless, the nature (size) of the chromium - collagen complexes has not been proofed experimentally yet.
We investigated the structure of the chromium complexes in powder and dilute solutions of chromium alum, a basic chrome(III) tannin (Chromosal B), an acetone dehydrated, Chromosal tanned Wet Blue leather, an industrial manufactured leather before and after artificial shrinkage, and gelatin by Extended X-ray Absorption Fine Structure (EXAFS) spectroscopy.
	It is shown that in solid Chromosal B every Cr atom is surrounded by approximately two other Cr atoms. In 0.2 M Chromosal B solution binuclear, in solid chromium alum and its 0.2 M solution mononuclear chromium complexes are present. In leather and gelatin the bound chromium complexes are approximately binuclear. Partial area shrinkage caused by repeated thermal treatment of the chrome leather did not lead to a significant change of the Cr complex inside the leather. These results support the current theoretical concept of chrome tanning in a direct way and demonstrate the great potential of EXAFS investigations in the leather field. 

]]></dc:description>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:276-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brünig, D.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-276-1</dc:identifier>
<dc:title><![CDATA[Solare Trinkwarmwasserbereitung und Einspeisung in ein Fernwärmenetz - Demonstrationsanlage Waldblickschule Freital]]></dc:title>
<dc:source><![CDATA[Terrarec '95, Kongreß West-Ost-Transfer Umwelt Leipzig, 1. - 3.3. 1995, Tagungsband Energie S. 156]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Im Beitrag werden erste Ergebnisse der Messungen (Zeitraum Juli-Dezember 1994) an der Solaranlage vorgestellt. Kollektorkreis, Pufferspeicherladekreis, Brauchwasserladekreis und Fernwärmeeinspeisung werden im Einzelnen analysiert. Die Betriebsergebnisse bestätigen die Auslegung, aufgrund erhöhter Rücklauftemperaturen des Fernwärmenetzes liegen die energetischen Ergebnisse der Solaranlage unter den projektierten Werten.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-276-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:276-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brünig, D.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-276-7</dc:identifier>
<dc:title><![CDATA[Solare Trinkwarmwasserbereitung und Einspeisung in ein Fernwärmenetz - Demonstrationsanlage Waldblickschule Freital]]></dc:title>
<dc:source><![CDATA[Terrarec '95, Kongreß West-Ost-Transfer Umwelt Leipzig, 1. - 3.3. 1995, Tagungsband Energie S. 156]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Im Beitrag werden erste Ergebnisse der Messungen (Zeitraum Juli-Dezember 1994) an der Solaranlage vorgestellt. Kollektorkreis, Pufferspeicherladekreis, Brauchwasserladekreis und Fernwärmeeinspeisung werden im Einzelnen analysiert. Die Betriebsergebnisse bestätigen die Auslegung, aufgrund erhöhter Rücklauftemperaturen des Fernwärmenetzes liegen die energetischen Ergebnisse der Solaranlage unter den projektierten Werten.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-276-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1988-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1988-1</dc:identifier>
<dc:title><![CDATA[Fifth Dynamic AER Benchmark - A Benchmark for Coupled Thermohydraulic System/3D Hexagonal Neutron Kinetic Core Models - Comparison of Results - Level 1]]></dc:title>
<dc:source><![CDATA[AER Working Group D Meeting, Rez (Czech Republic), May 18-20, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The fifth dynamic benchmark was defined at the 7th AER-Symposium, held in Hörnitz, Germany in 1997. It is the first benchmark for coupled thermohydraulic system/three-dimensional hexagonal neutron kinetic core models. In this benchmark the interaction between the components of a VVER-440 NPP with the reactor core has been investigated. In this presentation, the first results obtained by means of the codes DYN3D/ATHLET (Forschungszentrum Rossendorf), BIPR8/ATHLET (Kurchatov Institute Moscow) und HEXTRAN/SMABRE (VTT Energy Espoo) were compared. Both thermohydraulics and neutron kinetics parameters show dif-
ferences.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1988-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:14255-2</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pietzsch, J.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, F.-J.]]></dc:creator>
<dc:creator><![CDATA[Laube, M.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Kniess, T.]]></dc:creator>
<dc:creator><![CDATA[Wuest, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14255-2</dc:identifier>
<dc:title><![CDATA[Concomitant targeting of cyclooxygenase-2 and oxidant stress pathways for radioprotection of normal vascular tissue]]></dc:title>
<dc:source><![CDATA[European Journal of Cancer 8(2010), 211]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Background: 
Radiotherapy of various cancers is closely associated with increased cardiovascular morbidity and mortality. Arachidonic acid metabolites are supposed to play a key role in radiation-induced vascular dysfunction, inflammation, and injury. This study was designed to evaluate the effects of novel selective cyclooxygenase-2 (COX-2) inhibitors on radiation-induced formation of arachidonic acid metabolites via cyclooxygenase-2 and oxidant stress pathways in endothelial cells.

Materials and methods: 
Acute effects (1 d, 3 d) of X-ray radiation at moderate doses (2 to 10 Gy) without or with presence of selective COX-2 inhibitors (cyclopentene/indole/indomethacin derivatives (2 each); 1 µM, 10 µM) in human arterial (HAEC) and microvascular (HDMEC) endothelial cells compared to sham-irradiated controls were assessed. Therefore, the following parameters were measured: COX-2 induction; secretion of cytokines tumor necrosis factor-α, interleukin-6, and monocyte chemoattractant protein-1; release of prostaglandins PGE2 and PGI2; release of isoprostanes 8-iso-PGE2 and 8-iso-PGF2α; and oxidative stress (lipid peroxides).

Results: 
Irradiation of endothelial cells without presence of COX-2 inhibitors resulted in a dose-dependent augmentation of all parameters studied. When endothelial cells were exposed to COX-2 inhibitors during and for 24 h post irradiation, indole derivatives showed highest potency to inhibit release of both prostaglandins and isoprostanes. Furthermore, when irradiated cells were treated with indole derivatives a significant decrease of lipid peroxide formation and cytokine secretion could be observed, which indicates a direct interaction with oxidant stress-pathways. By contrast, both cyclopentene and indomethacin derivatives majorily inhibited prostaglandin release, but showed only slight effects on formation of isoprostanes, lipid peroxides and cytokines. Model experiments using human low density lipoproteins oxidized by radiolytically generated oxygen radicals showed that indole derivatives differently interact with peroxidation of polyunsaturated fatty acids, than the cyclopentene/indomethacin derivatives, suggesting a physico-chemical rationale for observed anti-oxidant activity.

Conclusion: 
Indole-based selective COX-2 inhibitors substantially decreased radiation-induced formation of vasoactive isoprostanes
8-iso-PGE2 and 8-iso-PGF2α by endothelial cells. These findings may have particular importance in radiation-induced processes in which COX-2 is induced and oxidant stress occurs. The reduction of radiation-induced vascular dysfunction by antioxidative COX-2 inhibitors may widen the therapeutic window of cyclooxygenase-2 targeted treatment.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:14255-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pietzsch, J.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, F.-J.]]></dc:creator>
<dc:creator><![CDATA[Laube, M.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Kniess, T.]]></dc:creator>
<dc:creator><![CDATA[Wuest, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14255-1</dc:identifier>
<dc:title><![CDATA[Concomitant targeting of cyclooxygenase-2 and oxidant stress pathways for radioprotection of normal vascular tissue]]></dc:title>
<dc:source><![CDATA[21st Meeting of the European Association for Cancer Research (EACR-21), 26.-29.06.2010, Oslo, Norway]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Background: 
Radiotherapy of various cancers is closely associated with increased cardiovascular morbidity and mortality. Arachidonic acid metabolites are supposed to play a key role in radiation-induced vascular dysfunction, inflammation, and injury. This study was designed to evaluate the effects of novel selective cyclooxygenase-2 (COX-2) inhibitors on radiation-induced formation of arachidonic acid metabolites via cyclooxygenase-2 and oxidant stress pathways in endothelial cells.

Materials and methods: 
Acute effects (1 d, 3 d) of X-ray radiation at moderate doses (2 to 10 Gy) without or with presence of selective COX-2 inhibitors (cyclopentene/indole/indomethacin derivatives (2 each); 1 µM, 10 µM) in human arterial (HAEC) and microvascular (HDMEC) endothelial cells compared to sham-irradiated controls were assessed. Therefore, the following parameters were measured: COX-2 induction; secretion of cytokines tumor necrosis factor-α, interleukin-6, and monocyte chemoattractant protein-1; release of prostaglandins PGE2 and PGI2; release of isoprostanes 8-iso-PGE2 and 8-iso-PGF2α; and oxidative stress (lipid peroxides).

Results: 
Irradiation of endothelial cells without presence of COX-2 inhibitors resulted in a dose-dependent augmentation of all parameters studied. When endothelial cells were exposed to COX-2 inhibitors during and for 24 h post irradiation, indole derivatives showed highest potency to inhibit release of both prostaglandins and isoprostanes. Furthermore, when irradiated cells were treated with indole derivatives a significant decrease of lipid peroxide formation and cytokine secretion could be observed, which indicates a direct interaction with oxidant stress-pathways. By contrast, both cyclopentene and indomethacin derivatives majorily inhibited prostaglandin release, but showed only slight effects on formation of isoprostanes, lipid peroxides and cytokines. Model experiments using human low density lipoproteins oxidized by radiolytically generated oxygen radicals showed that indole derivatives differently interact with peroxidation of polyunsaturated fatty acids, than the cyclopentene/indomethacin derivatives, suggesting a physico-chemical rationale for observed anti-oxidant activity.

Conclusion: 
Indole-based selective COX-2 inhibitors substantially decreased radiation-induced formation of vasoactive isoprostanes
8-iso-PGE2 and 8-iso-PGF2α by endothelial cells. These findings may have particular importance in radiation-induced processes in which COX-2 is induced and oxidant stress occurs. The reduction of radiation-induced vascular dysfunction by antioxidative COX-2 inhibitors may widen the therapeutic window of cyclooxygenase-2 targeted treatment.]]></dc:description>
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<identifier>HZDR:PUBLDB:1620-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1620-1</dc:identifier>
<dc:title><![CDATA[The Coupled Code Complex DYN3D/ATHLET - Application to Main Steam Line Break Analysis]]></dc:title>
<dc:source><![CDATA[Proc. Joint International Conference on Mathematical Methods and Supercomputing for Nuclear Applications, pp.1358-1366, ANS, La Grange Park, IL (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The coupling of advanced thermohydraulic codes with 3-dimensional neutron kinetic codes corresponds to the effort to replace conservative estimations by best estimate calculations. ATHLET is an advanced thermohydraulic code, developed by the German "Gesellschaft für Anlagen- und Reaktorsicherheit" (GRS). The DYN3D code, developed at Forschungszentrum Rossendorf (FZR) for the simulation of reactivity initiated accidents in nuclear reactors with hexagonal and Cartesian fuel element cross section geometry comprises 3-dimensional neutron kinetics, models for the thermohydraulics of the core and the thermomechanical fuel rod behaviour.
The reactor core model DYN3D was coupled with ATHLET according to two basically different strategies. The first way of coupling uses only the neutron kinetics part of DYN3D (internal coupling). In the second way, the whole core is cut out from the ATHLET plant model and is completely described by DYN3D (external coupling). In this case the values of pressure, mass flow rate, enthalpy and boron acid concentration at the bottom and at the top of the core have to be transferred between the codes. This way of coupling is efficiently supported by the General Control and Simulation Module (GCSM) of ATHLET.
The results of the analysis of a main steam line break scenario for a VVER-440 type reactor by the help of DYN3D-ATHLET are presented. The effect of different assumptions for the coolant mixing in downcomer and lower plenum of the reactor has been investigated.]]></dc:description>
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<identifier>HZDR:PUBLDB:1620-2</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1620-2</dc:identifier>
<dc:title><![CDATA[The Coupled Code Complex DYN3D/ATHLET - Application to Main Steam Line Break Analysis]]></dc:title>
<dc:source><![CDATA[Joint International Conference on
Mathematical Methods and Supercomputing for Nuclear Applications, ANS, La
Grange Park, IL (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The coupling of advanced thermohydraulic codes with 3-dimensional neutron kinetic codes corresponds to the effort to replace conservative estimations by best estimate calculations. ATHLET is an advanced thermohydraulic code, developed by the German "Gesellschaft für Anlagen- und Reaktorsicherheit" (GRS). The DYN3D code, developed at Forschungszentrum Rossendorf (FZR) for the simulation of reactivity initiated accidents in nuclear reactors with hexagonal and Cartesian fuel element cross section geometry comprises 3-dimensional neutron kinetics, models for the thermohydraulics of the core and the thermomechanical fuel rod behaviour.
The reactor core model DYN3D was coupled with ATHLET according to two basically different strategies. The first way of coupling uses only the neutron kinetics part of DYN3D (internal coupling). In the second way, the whole core is cut out from the ATHLET plant model and is completely described by DYN3D (external coupling). In this case the values of pressure, mass flow rate, enthalpy and boron acid concentration at the bottom and at the top of the core have to be transferred between the codes. This way of coupling is efficiently supported by the General Control and Simulation Module (GCSM) of ATHLET.
The results of the analysis of a main steam line break scenario for a VVER-440 type reactor by the help of DYN3D-ATHLET are presented. The effect of different assumptions for the coolant mixing in downcomer and lower plenum of the reactor has been investigated.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1298-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1298-1</dc:identifier>
<dc:title><![CDATA[Solution of the Fifth Dynamic AER Benchmark Using the Coupled Code DYN3D/ATHLET]]></dc:title>
<dc:source><![CDATA[Proceeding of the 8th AER-Symposium, pp. 357-367, KFKI Atomic Energy Research Institute, Budapest (1998)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The fifth dynamic benchmark is the first benchmark for coupled thermohydraulic system/three-dimensional hexagonal neutron kinetic core models. In this benchmark the interaction between the components of a VVER-440 NPP with the reactor core has been investigated.

The initiating event is a symmetrical break of the main steam header at the end of the first fuel cycle and hot shutdown conditions with one control rod group stucking. This break causes an overcooling of the primary circuit. During this overcooling the scram reactivity is compensated and the scrammed reactor becomes recritical. The calculation was continued until the highly-borated water from the high pressure injection system terminated the power excursion.

Several aspects of this very complex and complicated benchmark problem are analyzed in detail. Sensitivity studies with different hydraulic parameters are made. The influence on the course of the transient and on the solution is discussed.

]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1298-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1298-2</dc:identifier>
<dc:title><![CDATA[Solution of the Fifth Dynamic AER Benchmark Using the Coupled Code DYN3D/ATHLET]]></dc:title>
<dc:source><![CDATA[8th AER-Symposium]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The fifth dynamic benchmark is the first benchmark for coupled thermohydraulic system/three-dimensional hexagonal neutron kinetic core models. In this benchmark the interaction between the components of a VVER-440 NPP with the reactor core has been investigated.

The initiating event is a symmetrical break of the main steam header at the end of the first fuel cycle and hot shutdown conditions with one control rod group stucking. This break causes an overcooling of the primary circuit. During this overcooling the scram reactivity is compensated and the scrammed reactor becomes recritical. The calculation was continued until the highly-borated water from the high pressure injection system terminated the power excursion.

Several aspects of this very complex and complicated benchmark problem are analyzed in detail. Sensitivity studies with different hydraulic parameters are made. The influence on the course of the transient and on the solution is discussed.

]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<identifier>HZDR:PUBLDB:2443-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pezoldt, J.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Hatzopoulos, N.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Kreißig, U.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2443-1</dc:identifier>
<dc:title><![CDATA[Structural studies of buried (SiC)<SUB>1-x</SUB>(AlN)<SUB>x</SUB> layers fabricated by co-implantation of nitrogen and aluminium ions in 6H-SiC]]></dc:title>
<dc:source><![CDATA[7th Int. Conf. on Defect Recognition and Image Processing in Semiconductors (DRIP VII), Templin, Germany, Sept. 7 - 10, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2445-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Plass, M. F.]]></dc:creator>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Kolitsch, A.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2445-1</dc:identifier>
<dc:title><![CDATA[Characterization of noncubic boron nitride films grown by a nonnormal angle of ion bombardment]]></dc:title>
<dc:source><![CDATA[ICMCTF 97, San Diego, USA]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Plass, M. F.]]></dc:creator>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Kolitsch, A.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2446-1</dc:identifier>
<dc:title><![CDATA[Growth and characterization of boron nitride thin films]]></dc:title>
<dc:source><![CDATA[SMMIB 97, Gatlinburg, TE, USA, Sept. 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2447-1</dc:identifier>
<dc:title><![CDATA[Computer simulation of random-to-channeling and blocking-to-channeling transitions]]></dc:title>
<dc:source><![CDATA[Workshop on Channeling and Blocking Effects with Heavy Ion Beams, München, Germany, April 18 - 19, 1997 (invited lecture)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:14425-3</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Toepfer, T.]]></dc:creator>
<dc:creator><![CDATA[Neukum, J.]]></dc:creator>
<dc:creator><![CDATA[Hein, J.]]></dc:creator>
<dc:creator><![CDATA[Siebold, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14425-3</dc:identifier>
<dc:title><![CDATA[Very large DPSS lasers are coming]]></dc:title>
<dc:source><![CDATA[Laser Focus World 46(2010)10, 64-67]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[New alcaline-earth fluoride laser materials and ever-improving diode-laser module technology are bringing very high-energy, 	moderate-to high-repetition-rate DPSS lasers for research closer to reality.]]></dc:description>
<dc:subject><![CDATA[High-energy]]></dc:subject>
<dc:subject><![CDATA[diode-pumped]]></dc:subject>
<dc:subject><![CDATA[solid-state lasers]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:14448-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Moll, H.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14448-1</dc:identifier>
<dc:title><![CDATA[Actinide Interactions with Bacteria]]></dc:title>
<dc:source><![CDATA[Actinide and Brine Chemistry in a Salt-Based Repository (ABC-SALT) International Workshop, 15.-17.09.2010, Carlsbad, New Mexico, USA]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Microbes are widely distributed in nature also under harsh conditions (e.g., high salinity; low permeability; high and low temperatures). They can strongly influence the migration of hazardous actinides in the environment once they have been released. This is demonstrated by an increased interest in studies exploring the interaction processes involving actinides and bacteria during the last years. However, worldwide only little detailed information is available about the biodiversity and microbial influences on radionuclide migration under the conditions of a deep nuclear repository.
The presentation covers the broad topic of actinide interactions with bacteria. A short overview about the determination of the microbial diversity giving the dominant bacterial strains will be given. In more detail, the manifold interaction process of bacteria with actinides will be highlighted based on selected examples. 
With this presentation we want to point out the importance of actinide-microbe interactions for the disposal of nuclear waste.]]></dc:description>
<dc:subject><![CDATA[microbes]]></dc:subject>
<dc:subject><![CDATA[actinides]]></dc:subject>
<dc:subject><![CDATA[nuclear waste disposal]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<header>
<identifier>HZDR:PUBLDB:2448-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2448-1</dc:identifier>
<dc:title><![CDATA[Modeling of implantation damage in silicon]]></dc:title>
<dc:source><![CDATA[Int. Workshop on Challenges in Predictive Process Simulation (ChiPPS'97), Wandlitz, Germany, Aug. 17 - 20, 1997 (invited lecture)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1461-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krüssenberg, A.-K.]]></dc:creator>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1461-1</dc:identifier>
<dc:title><![CDATA[A New Criterion for the Bubble Slug Transition in Vertical Tubes]]></dc:title>
<dc:source><![CDATA[Ninth International Topical Meeting on Nuclear Reactor Thermal Hydraulics (NURETH-9), San Francisco, 5th Oct 1999, CD-ROM]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Vertical two-phase flow is normally classified into the four basic flow regimes bubble, slug, churn and annular flow. The transition between the different flow regimes does not occur suddenly and many extensions of this classification can be found in literature. For the prediction of flow patterns empirical and theoretical flow pattern maps have been developed. 
A new criterion is presented for the transition between bubble and slug flow which is based on local instantaneous conductivity measurements with a wire mesh sensor (1 kHz that means 1000 frames per second, 242 measuring points in a tube cross section area). The high resolution allows the calculation of particle size distributions.
 
The transition from homogeneous bubble flow to heterogeneous bubble flow is indicated by the appearance of a bimodal bubble size distribution. If the equivalent bubble diameter exceeds the tube diameter the transition from bubble to slug flow occurs. The new criterion is compared with different empirical (Govier & Aziz, Weisman & Kang) and theoretical flow maps (Taitel, Bornea & Dukler, Ishii & Mishima) and shows a good agreement. 
  
]]></dc:description>
<dc:subject><![CDATA[bubble size distribution]]></dc:subject>
<dc:subject><![CDATA[bubble slug flow transition criteria]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1461-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krüssenberg, A.-K.]]></dc:creator>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1461-7</dc:identifier>
<dc:title><![CDATA[A New Criterion for the Bubble Slug Transition in Vertical Tubes]]></dc:title>
<dc:source><![CDATA[Ninth International Topical Meeting on Nuclear Reactor Thermal Hydraulics (NURETH-9), San Francisco, 5th Oct 1999, CD-ROM]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Vertical two-phase flow is normally classified into the four basic flow regimes bubble, slug, churn and annular flow. The transition between the different flow regimes does not occur suddenly and many extensions of this classification can be found in literature. For the prediction of flow patterns empirical and theoretical flow pattern maps have been developed. 
A new criterion is presented for the transition between bubble and slug flow which is based on local instantaneous conductivity measurements with a wire mesh sensor (1 kHz that means 1000 frames per second, 242 measuring points in a tube cross section area). The high resolution allows the calculation of particle size distributions.
 
The transition from homogeneous bubble flow to heterogeneous bubble flow is indicated by the appearance of a bimodal bubble size distribution. If the equivalent bubble diameter exceeds the tube diameter the transition from bubble to slug flow occurs. The new criterion is compared with different empirical (Govier & Aziz, Weisman & Kang) and theoretical flow maps (Taitel, Bornea & Dukler, Ishii & Mishima) and shows a good agreement. 
  
]]></dc:description>
<dc:subject><![CDATA[bubble size distribution]]></dc:subject>
<dc:subject><![CDATA[bubble slug flow transition criteria]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1217-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Fethke, M.]]></dc:creator>
<dc:creator><![CDATA[Rossner, L.]]></dc:creator>
<dc:creator><![CDATA[Jaegers, H.]]></dc:creator>
<dc:creator><![CDATA[Hicken, E. F.]]></dc:creator>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1217-1</dc:identifier>
<dc:title><![CDATA[Experimental Investigation of the Operation Mode of Passive Safety Systems]]></dc:title>
<dc:source><![CDATA[ENC '98, Nice, France, 25-29 October 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The safety concept of the innovative boiling water reactor SWR 1000 is characterised by passive safety systems (e.g. emergency condensers, building condensers, passive initiators). The operation mode and the effectiveness of these safety systems is investigated in the multipurpose thermalhydraulic test facility NOKO at the Forschungszentrum Jülich (FZJ).
The effectiveness of the emergency condenser was determined in more than 200 experiments. Post-test calculations of the emergency condenser experiments were performed with an improved version of the ATHLET code. The comparison of the calculations and the experiments shows a good agreement.
Parallel, the performance of three different designs of the passive initiator was investigated experimentally. The experimental results are used to optimise the design of an additional passive initiator which will be tested in NOKO this year.
Additionally, more than 80 experiments were carried out in NOKO to determine the effectiveness of two different designs of the building condenser. Post-test calculations were performed using the modified computer code RALOC. The comparison of the calculations and the experiments shows a good agreement.
]]></dc:description>
<dc:subject><![CDATA[SWR1000]]></dc:subject>
<dc:subject><![CDATA[NOKO]]></dc:subject>
<dc:subject><![CDATA[emergency condenser]]></dc:subject>
<dc:subject><![CDATA[ATHLET]]></dc:subject>
<dc:subject><![CDATA[building condenser]]></dc:subject>
<dc:subject><![CDATA[passive initiator]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1217-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:1217-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Fethke, M.]]></dc:creator>
<dc:creator><![CDATA[Rossner, L.]]></dc:creator>
<dc:creator><![CDATA[Jaegers, H.]]></dc:creator>
<dc:creator><![CDATA[Hicken, E. F.]]></dc:creator>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1217-7</dc:identifier>
<dc:title><![CDATA[Experimental Investigation of the Operation Mode of Passive Safety Systems]]></dc:title>
<dc:source><![CDATA[ENC '98, Nice, France, 25-29 October 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The safety concept of the innovative boiling water reactor SWR 1000 is characterised by passive safety systems (e.g. emergency condensers, building condensers, passive initiators). The operation mode and the effectiveness of these safety systems is investigated in the multipurpose thermalhydraulic test facility NOKO at the Forschungszentrum Jülich (FZJ).
The effectiveness of the emergency condenser was determined in more than 200 experiments. Post-test calculations of the emergency condenser experiments were performed with an improved version of the ATHLET code. The comparison of the calculations and the experiments shows a good agreement.
Parallel, the performance of three different designs of the passive initiator was investigated experimentally. The experimental results are used to optimise the design of an additional passive initiator which will be tested in NOKO this year.
Additionally, more than 80 experiments were carried out in NOKO to determine the effectiveness of two different designs of the building condenser. Post-test calculations were performed using the modified computer code RALOC. The comparison of the calculations and the experiments shows a good agreement.
]]></dc:description>
<dc:subject><![CDATA[SWR1000]]></dc:subject>
<dc:subject><![CDATA[NOKO]]></dc:subject>
<dc:subject><![CDATA[emergency condenser]]></dc:subject>
<dc:subject><![CDATA[ATHLET]]></dc:subject>
<dc:subject><![CDATA[building condenser]]></dc:subject>
<dc:subject><![CDATA[passive initiator]]></dc:subject>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1217-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2216-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Andronenko, L. N.]]></dc:creator>
<dc:creator><![CDATA[Andronenko, M. N.]]></dc:creator>
<dc:creator><![CDATA[Seliverstov, D. M.]]></dc:creator>
<dc:creator><![CDATA[Neubert, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2216-1</dc:identifier>
<dc:title><![CDATA[Fragment production in proton interactions with light nuclei]]></dc:title>
<dc:source><![CDATA[7th International Conference on Clustering Aspects of Nuclear Structure and Dynamics. Rab, Croatia 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Isotopic yield ratios were derived from double-differential cross sections  measured in p+<sup>9</sup>Be and p+<sup>12</sup>C collisions at 1 GeV. Enhanced <sup>9</sup>He yields were found compared to heavier target nuclei.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2216-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1370-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1370-1</dc:identifier>
<dc:title><![CDATA[Meßtechnik für stationäre und transiente Mehrphasenströmungen]]></dc:title>
<dc:source><![CDATA[Atomwirtschaft-Atomtechnik 43 (1998), Nr. 11, S. 706-708]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Initiatoren des zweiten Workshops zum Thema „Meßtechnik für stationäre und transiente Mehrphasenströmungen" im Forschungszentrum Rossendorf (FZR) e.V. waren das Institut für Sicherheitsforschung des FZR und das Institut für Prozeßtechnik, Prozeßautomatisierung und Meßtechnik (IPM) an der Hochschule für Technik, Wirtschaft und Sozialwesen (HTWS) Zittau/Görlitz. Der Workshop wurde mit Unterstützung der Deutschen Gesellschaft für Chemisches Apparatewesen, Chemische Technik und Biotechnologie (Dechema) e.V. sowie der Kerntechnischen Gesellschaft (Fachgruppe Thermo- und Fluiddynamik) veranstaltet. In drei Haupt- sowie 13 Fachvorträgen wurden optische Meßverfahren, Impedanzverfahren und Sondergebiete zur Messung wichtiger Größen in einer Zwei- oder Mehrphasenströmung vorgestellt. ]]></dc:description>
<dc:subject><![CDATA[Meßtechnik für stationäre und transiente Mehrphasenströmungen]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>ger</dc:language>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Ahlemeyer, B.]]></dc:creator>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3082-1</dc:identifier>
<dc:title><![CDATA[Different response of cerebral and non-cerebral endothelial cells to cytotoxic hypoxia]]></dc:title>
<dc:source><![CDATA[Neurochem. Int. 31 (1997) 39-44]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Moll, H.]]></dc:creator>
<dc:creator><![CDATA[Zänker, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, W.]]></dc:creator>
<dc:creator><![CDATA[Brendler, V.]]></dc:creator>
<dc:creator><![CDATA[Kluge, A.]]></dc:creator>
<dc:creator><![CDATA[Hüttig, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3235-1</dc:identifier>
<dc:title><![CDATA[Ausscheidung von Sekundärmineralen aus Lettenwasser der Himmelfahrt Fundgrube Freiberg]]></dc:title>
<dc:source><![CDATA[6. Kolloquium im SPP "Geochemische Prozesse mit Langzeitfolgen im anthropogen beeinflussten Sickerwasser und Grundwasser", 2. und 3. März, Berlin]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Im Laufe von 10 Monaten schied sich aus dem untersuchten Lettenwasser eine makros-kopische Sekundärmineralphase aus. Es handelt sich im wesentlichen um das sulfatreiche Mineral H-Jarosit. Kleine Mengen an schlecht kristallinen Phasen, wie Schwertmannit, können nicht ausgeschlossen werden. Der H-Jarosit bindet signifikante Mengen an As und Blei. Die XRD ergab aber keine Hinweise auf Skorodit oder Bleiminerale. 
Die ultrafeinen Partikel (<5nm) in ARD Lösungen könnten ein Zwischenprodukt im Bildungsprozeß des H-Jarosits sein. Dann könnte die Charakterisierung des Niederschlags im gealterten Lettenwasser Hinweise auf die Zusammensetzung der ultrafeinen Partikel im frischen Lettenwasser geben. EXAFS-Messungen zur Aufklärung der chemischen Bindungsverhältnisse in Kolloidpartikeln (<5nm) sind in Arbeit.
]]></dc:description>
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<identifier>HZDR:PUBLDB:2007-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Höhne, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2007-2</dc:identifier>
<dc:title><![CDATA[NUMERICAL SIMULATION OF THE COOLANT FLOW IN PRESSURIZED WATER REACTORS]]></dc:title>
<dc:source><![CDATA[CFX International Users Conference, Friedrichshafen, Germany 19-24 June 1999,
CD-ROM, No. 27]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The behavior of PWRs during cold water or boron dilution transients is strongly influenced by the distribution of coolant temperature and boron concentration at the core inlet. This distribution is required as an input to 3-dimensional neutron kinetics to calculate the power distribution in the core. It mainly depends on how the plugs of cold or unborated water formed in a single loop are mixed in the downcomer and in the lower plenum [1]. The reactivity insertion due to penetration of unborated coolant into the core depends on the degree of mixing. Weak mixing can result in recriticality and possibly in significant power release. The same is true for cold water insertion into the core due to overcooling of a coolant loop in the case of a steam line break. Coolant mixing is also of interest under steady state normal operation conditions. Slight differences in the cold leg temperatures can occur due to small asymmetries in the primary circuit loops.

To simulate such mixture phenomena requires the application of 3-dimensional CFD (computational fluid dynamics) codes. The results of the simulation have to be validated against mixing experiments at scaled facilities. The calculations are accomplished using the CFD Code CFX-4.2 [2]. 

As a first step, steady state mixing conditions in the downcomer and lower plenum are considered. Qualitatively different flow fields were found in different reactor types depending from the downcomer geometry. Calculated results were compared with experiments.]]></dc:description>
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<identifier>HZDR:PUBLDB:2007-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Höhne, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2007-7</dc:identifier>
<dc:title><![CDATA[NUMERICAL SIMULATION OF THE COOLANT FLOW IN PRESSURIZED WATER REACTORS]]></dc:title>
<dc:source><![CDATA[CFX International Users Conference, Friedrichshafen, Germany 19-24 June 1999,
CD-ROM, No. 27]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The behavior of PWRs during cold water or boron dilution transients is strongly influenced by the distribution of coolant temperature and boron concentration at the core inlet. This distribution is required as an input to 3-dimensional neutron kinetics to calculate the power distribution in the core. It mainly depends on how the plugs of cold or unborated water formed in a single loop are mixed in the downcomer and in the lower plenum [1]. The reactivity insertion due to penetration of unborated coolant into the core depends on the degree of mixing. Weak mixing can result in recriticality and possibly in significant power release. The same is true for cold water insertion into the core due to overcooling of a coolant loop in the case of a steam line break. Coolant mixing is also of interest under steady state normal operation conditions. Slight differences in the cold leg temperatures can occur due to small asymmetries in the primary circuit loops.

To simulate such mixture phenomena requires the application of 3-dimensional CFD (computational fluid dynamics) codes. The results of the simulation have to be validated against mixing experiments at scaled facilities. The calculations are accomplished using the CFD Code CFX-4.2 [2]. 

As a first step, steady state mixing conditions in the downcomer and lower plenum are considered. Qualitatively different flow fields were found in different reactor types depending from the downcomer geometry. Calculated results were compared with experiments.]]></dc:description>
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<identifier>HZDR:PUBLDB:2008-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2008-1</dc:identifier>
<dc:title><![CDATA[Measurements and CFX-Simulations of a Bubbly Flow in a Vertical Pipe]]></dc:title>
<dc:source><![CDATA[CFX International Users Conference, Friedrichshafen, 21.-24.6.1999 (Conference-CD)]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[In the Forschungszentrum Rossendorf a measurements techniques test loop was constructed. Air water flow in a vertical tube was investigated using different two phase flow measuring techniques. The paper describes the used measuring techniques and some performed experiments. The code CFX-4.2 with its implemented two phase models was used, to simulate bubbly flow and to compare calculated void profiles with the measured results. ]]></dc:description>
<dc:subject><![CDATA[bubble flow]]></dc:subject>
<dc:subject><![CDATA[two-phase flow measurement techniques]]></dc:subject>
<dc:subject><![CDATA[cfd simulations]]></dc:subject>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2008-7</dc:identifier>
<dc:title><![CDATA[Measurements and CFX-Simulations of a Bubbly Flow in a Vertical Pipe]]></dc:title>
<dc:source><![CDATA[CFX International Users Conference, Friedrichshafen, 21.-24.6.1999 (Conference-CD)]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[In the Forschungszentrum Rossendorf a measurements techniques test loop was constructed. Air water flow in a vertical tube was investigated using different two phase flow measuring techniques. The paper describes the used measuring techniques and some performed experiments. The code CFX-4.2 with its implemented two phase models was used, to simulate bubbly flow and to compare calculated void profiles with the measured results. ]]></dc:description>
<dc:subject><![CDATA[bubble flow]]></dc:subject>
<dc:subject><![CDATA[two-phase flow measurement techniques]]></dc:subject>
<dc:subject><![CDATA[cfd simulations]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2011-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Aszodi, A.]]></dc:creator>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2011-1</dc:identifier>
<dc:title><![CDATA[Experimental and Numerical Investigation of One and Two-Phase Natural Convection in Storage Tanks]]></dc:title>
<dc:source><![CDATA[EUROTHERM Seminar No. 63, Single and Two- Phase Natural Circulation, Genoa September 1999, Proceedings edited by M. Misale and F. Mayinger, pp. 43-49, ISBN 88-900433-1-8]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Experiments were performed to investigate heating up processes of fluids in storage tanks under the influence of an external heat source. As a consequence of an external fire, the heat-up of the inventory may lead to the evaporation of the liquid and to release of significant quantities of dangerous gases into the environment. Several tests were performed both with heating from the bottom and with heating from the side walls. In recent tests in addition to thermocouples, the tank was equipped with needle probes for measuring of the local void fraction. The paper presents experimental and numerical investigations of single and two phase heating up processes of tanks with side wall heating. The measurement of the temperature and of the void fraction makes interesting phenomena evident. which could be explained by an own 2D model. The gained experimental results may be used for the validation of boiling models in 3-D CFD codes. ]]></dc:description>
<dc:subject><![CDATA[heating up]]></dc:subject>
<dc:subject><![CDATA[large pools]]></dc:subject>
<dc:subject><![CDATA[natural circulation]]></dc:subject>
<dc:subject><![CDATA[boiling]]></dc:subject>
<dc:subject><![CDATA[experiments]]></dc:subject>
<dc:subject><![CDATA[two-phase flow measurements]]></dc:subject>
<dc:subject><![CDATA[cfd-simulation]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2011-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Aszodi, A.]]></dc:creator>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2011-7</dc:identifier>
<dc:title><![CDATA[Experimental and Numerical Investigation of One and Two-Phase Natural Convection in Storage Tanks]]></dc:title>
<dc:source><![CDATA[EUROTHERM Seminar No. 63, Single and Two- Phase Natural Circulation, Genoa September 1999, Proceedings edited by M. Misale and F. Mayinger, pp. 43-49, ISBN 88-900433-1-8]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Experiments were performed to investigate heating up processes of fluids in storage tanks under the influence of an external heat source. As a consequence of an external fire, the heat-up of the inventory may lead to the evaporation of the liquid and to release of significant quantities of dangerous gases into the environment. Several tests were performed both with heating from the bottom and with heating from the side walls. In recent tests in addition to thermocouples, the tank was equipped with needle probes for measuring of the local void fraction. The paper presents experimental and numerical investigations of single and two phase heating up processes of tanks with side wall heating. The measurement of the temperature and of the void fraction makes interesting phenomena evident. which could be explained by an own 2D model. The gained experimental results may be used for the validation of boiling models in 3-D CFD codes. ]]></dc:description>
<dc:subject><![CDATA[heating up]]></dc:subject>
<dc:subject><![CDATA[large pools]]></dc:subject>
<dc:subject><![CDATA[natural circulation]]></dc:subject>
<dc:subject><![CDATA[boiling]]></dc:subject>
<dc:subject><![CDATA[experiments]]></dc:subject>
<dc:subject><![CDATA[two-phase flow measurements]]></dc:subject>
<dc:subject><![CDATA[cfd-simulation]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<header>
<identifier>HZDR:PUBLDB:2012-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Hoppe, D.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-2012-1</dc:identifier>
<dc:title><![CDATA[Die Verknüpfung von Teilmodellen auf der Grundlage der Dimensionsanalyse]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-263 Juni 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Für den Zweck der Modellbildung wird es im Beitrag als einfacher angesehen, erst Teilmodelle des zu beschreibenden Objektes zu erzeugen und diese nachher zu einer gesamtheitlichen Struktur miteinander zu verknüpfen, als das Objekt unmittel bar in seiner Gesamtheit zu modellieren. Aus dieser Sicht wird untersucht, wie die Verknüpfung von vorgegebenen Teilmodellen auf systematische Weise mit Hilfe der sogenannten Dimensionsanalyse durchgeführt werden kann. Das Strukturierungs problem wird dabei auf das Lösen eines linearen algebraische Gleichungssystems zurückgeführt. Strukturelle Restriktionen werden entweder durch eine geeignete Problemformulierung oder dadurch berücksichtigt, daß der formal gefundene Lö sungsraum nachträglich eingeschränkt wird. Anwendungsmöglichkeiten dieses Kon zeptes werden an verschiedenartigen Beispielen gezeigt.
]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
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<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2012-1</dc:relation>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<header>
<identifier>HZDR:PUBLDB:2014-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2014-1</dc:identifier>
<dc:title><![CDATA[Schnelle Gittersensoren für Gasgehalt, Gasgeschwindigkeit und Volumenstrom in einer Zweiphasenströmung]]></dc:title>
<dc:source><![CDATA[Seminarvortrag Universität GH Essen, 06. Mai 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Im Forschungszentrum Rossendorf wurde ein Gittersensor entwickelt, der die Ermittlung von momentanen Gasverteilungen mit einer örtlichen Auflösung von ca. 3 mm bei einer Meßfolge von derzeit 1200 Hz erlaubt. Er basiert auf der Messung der momentanen örtlichen elektrischen Leitfähigkeit des Zweiphasengemischs. Mit dem Sensor wurde eine Luft-Wasser-Strömung in einer vertikalen Rohleitung in weiten Bereichen der Leerrohrgeschwindigkeiten visualisiert und Voidanteile gemessen. Durch die gute Auflösung des Sensors werden Gasblasen in mehreren, zeitlich aufeinanderfolgenden Verteilungen abgebildet, was die Untersuchung von Blasengrößenverteilungen und deren Evolution entlang des Strömungsweges ermöglicht. Mit zwei hintereinander angeordneten Sensoren wurden durch Anwendung der Kreuzkorrelation Profile der Gasgeschwindigkeit gemessen. ]]></dc:description>
<dc:subject><![CDATA[two-phase flow]]></dc:subject>
<dc:subject><![CDATA[measurement methods]]></dc:subject>
<dc:subject><![CDATA[wire-mesh sensor]]></dc:subject>
<dc:subject><![CDATA[vertical pipe flow]]></dc:subject>
<dc:subject><![CDATA[flow pattern]]></dc:subject>
<dc:subject><![CDATA[gas fraction]]></dc:subject>
<dc:subject><![CDATA[gas velocity]]></dc:subject>
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<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
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<dc:identifier>https://www.hzdr.de/publications/Publ-1292-1</dc:identifier>
<dc:title><![CDATA[Die thermische Zersetzung von Wasserstoffperoxid als Modellreaktion für die Druckentlastung]]></dc:title>
<dc:source><![CDATA[4. Fachtagung Anlagen-, Arbeits- und Umweltsicherheit, 5.-6.11.1998, Köthen]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Für die Validierung von Computercodes zur dynamischen Simulation von Druckentlastungsvorgängen werden experimentelle Daten benötigt. Besonders geeignet sind dabei Versuchserien, bei denen einzelne Parameter variiert werden. Mit Hilfe von Parameterstudien lassen sich Rückschlüsse sowohl auf die Güte der Einzelmodelle als auch des Gesamtmodells ziehen. Solche Daten liegen jedoch meist nur für Druckentlastungen verdampfender oder gasentlösender Stoffsysteme vor. In der Praxis ist aber i.a. die Druckentlastung im Fall durchgehender exothermer Reaktionen interessant. Daher wurde eine geeignete Modellreaktion gesucht. Die thermische Zersetzung von Wasserstoffperoxid zeichnet sich dadurch aus, daß sie einfach durchführbar ist, daß mit Wasser und Sauerstoff unproblematische Reaktionsprodukte entstehen und daß die Reaktion allein durch Wärmezufuhr ausgelöst werden kann.]]></dc:description>
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<dc:title><![CDATA[Die thermische Zersetzung von Wasserstoffperoxid als Modellreaktion für die Druckentlastung]]></dc:title>
<dc:source><![CDATA[4. Fachtagung Anlagen-, Arbeits- und Umweltsicherheit, 5.-6.11.1998, Köthen]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Für die Validierung von Computercodes zur dynamischen Simulation von Druckentlastungsvorgängen werden experimentelle Daten benötigt. Besonders geeignet sind dabei Versuchserien, bei denen einzelne Parameter variiert werden. Mit Hilfe von Parameterstudien lassen sich Rückschlüsse sowohl auf die Güte der Einzelmodelle als auch des Gesamtmodells ziehen. Solche Daten liegen jedoch meist nur für Druckentlastungen verdampfender oder gasentlösender Stoffsysteme vor. In der Praxis ist aber i.a. die Druckentlastung im Fall durchgehender exothermer Reaktionen interessant. Daher wurde eine geeignete Modellreaktion gesucht. Die thermische Zersetzung von Wasserstoffperoxid zeichnet sich dadurch aus, daß sie einfach durchführbar ist, daß mit Wasser und Sauerstoff unproblematische Reaktionsprodukte entstehen und daß die Reaktion allein durch Wärmezufuhr ausgelöst werden kann.]]></dc:description>
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<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
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<dc:title><![CDATA[Coupling the Advanced Thermohydraulic Code ATHLET with the 3D-Core Model DYN3D]]></dc:title>
<dc:source><![CDATA[International Topical Meeting on VVER Safety, Prague, September 21 - 23, 1995, Proc. pp. 197 - 200]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[The coupling of advanced thermohydraulic codes with 3-dimensional neutron kinetic codes corresponds to the effort to replace conservative estimations by best estimate calculations. In the past advanced thermohydraulic codes and detailed core models were devoloped in most cases separatly. But it is often nesessary to consider the feedback between the coolant circuits and space dependent neutron kinetics. Examples for such cases are boron dilution accidents or inadverdant connection of a loop filled with cold water. 
ATHLET is an advanced thermohydraulic code, developed by the German Gesellschaft fr Anlagen- und Reaktorsicherheit (GRS). Up to now only point kinetics and 1-dimensional neutron kinetics have been included. The DYN3D code, developed in the Research Centre Rossendorf (FZR) for the improvement of the simulation of reactivity initiated accidents in VVER-type reactors comprises 3- dimensional neutron kinetics, models for the thermohydraulics of the core including heat transfer from the fuel to the coolant, a fuel rod behavior model and a mixing model for the lower plenum.]]></dc:description>
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<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
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<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1771-2</dc:identifier>
<dc:title><![CDATA[Coupling the Advanced Thermohydraulic Code ATHLET with the 3D-Core Model DYN3D]]></dc:title>
<dc:source><![CDATA[Internat Topical Meeting on VVER Safety, Prague, September 21 -23, 1995]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[The coupling of advanced thermohydraulic codes with 3-dimensional neutron kinetic codes corresponds to the effort to replace conservative estimations by best estimate calculations. In the past advanced thermohydraulic codes and detailed core models were devoloped in most cases separatly. But it is often nesessary to consider the feedback between the coolant circuits and space dependent neutron kinetics. Examples for such cases are boron dilution accidents or inadverdant connection of a loop filled with cold water. 
ATHLET is an advanced thermohydraulic code, developed by the German Gesellschaft fr Anlagen- und Reaktorsicherheit (GRS). Up to now only point kinetics and 1-dimensional neutron kinetics have been included. The DYN3D code, developed in the Research Centre Rossendorf (FZR) for the improvement of the simulation of reactivity initiated accidents in VVER-type reactors comprises 3- dimensional neutron kinetics, models for the thermohydraulics of the core including heat transfer from the fuel to the coolant, a fuel rod behavior model and a mixing model for the lower plenum.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2015-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2015-1</dc:identifier>
<dc:title><![CDATA[Untersuchungen zu möglichen Ursachen von Schwingungen des Massenstroms an der Entlastungsarmatur bei Druckentlastungsvorgängen]]></dc:title>
<dc:source><![CDATA[am Institut für Verfahrenstechnik der Universität Hannover, 30.1.1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Mewes, D.]]></dc:creator>
<dc:creator><![CDATA[Brodhagen, A.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2016-1</dc:identifier>
<dc:title><![CDATA[Simulation des transienten Verhaltens mehrphasiger Strömungsfelder in einem Blow-Down System]]></dc:title>
<dc:source><![CDATA[zum Schwerpunkt-Kolloquium der Volkswagenstiftung zur "Modellierung komplexer Systeme in der Verfahrenstechnik", Aachen, 22.-23. Februar 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2017-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2017-1</dc:identifier>
<dc:title><![CDATA[Massenstromschwankungen bei der Druckentlastung von Reaktoren]]></dc:title>
<dc:source><![CDATA[42. Sitzung des DECHEMA/GVC-Arbeitsausschuß "Sicherheitsgerechtes Auslegen von Chemieapparaten", Forschungszentrum Rossendorf, 15-16. Oktober 1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2019-1</dc:identifier>
<dc:title><![CDATA[BRICK - ein Simulationstool für Mehrphasenströmungen in einem Behälter auf der Basis einer Partikelmethode]]></dc:title>
<dc:source><![CDATA[Statement auf dem GVC-Expertengespräch "Computational Fluid Dynamics", Düsseldorf, 3. September 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Das Programm BRICK beruht auf einer neuen Lösungsmethode für die Modellierung
von Transportvorgängen in Behältern. Die Grundgedanken der Methode, welche zur Klasse der Particle-In-Cell (PIC) Methoden gehört, werden vorgestellt.

]]></dc:description>
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<identifier>HZDR:PUBLDB:14737-1</identifier>
<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Siebold, M.]]></dc:creator>
<dc:creator><![CDATA[Uecker, R.]]></dc:creator>
<dc:creator><![CDATA[Hornung, M.]]></dc:creator>
<dc:creator><![CDATA[Hein, J.]]></dc:creator>
<dc:creator><![CDATA[Sauerbrey, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14737-1</dc:identifier>
<dc:title><![CDATA[Terawatt Yb:CaF2 laser]]></dc:title>
<dc:source><![CDATA[6th International Conference on Crystal Growth ICCG-16, 08.-13.08.2010, Beijing, China]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[We present a terawatt diode-pumped laser employing single-crystalline Yb:CaF2 as the amplifying medium. A pulse energy of 197 mJ and a duration of 192 fs were obtained, corresponding to a peak power of 1 TW.]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<identifier>HZDR:PUBLDB:14773-1</identifier>
<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Frost, L.]]></dc:creator>
<dc:creator><![CDATA[Moll, H.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14773-1</dc:identifier>
<dc:title><![CDATA[Aqueous uranyl benzoate species characterized by different spectroscopic techniques]]></dc:title>
<dc:source><![CDATA[Radiochimica Acta 100(2012)5, 297-303]]></dc:source>
<dc:date>2012</dc:date>
<dc:description><![CDATA[In this study UV-vis spectroscopy as well as RT and cryo time-resolved laser-induced fluorescence spectroscopy (TRLFS) were applied to reinvestigate the complexation of uranium(VI) by benzoic acid (BA). For the first time in the liquid phase the existence of a U(VI)-BA complex with a 1:2 stoichiometry could be proven. 
RT TRLFS measurements revealed a static as well as a dynamic ligand-initiated quench process in the U(VI)-BA system. At these conditions no luminescence emission resulting from complex formation was found. Consequently cryo TRLFS was applied to increase the maximum detect-able BA:U(VI) ratio. By this for the first time a lumines-cence spectrum of the 1:2 U(VI)-BA complex could be determined. This species is characterized by emission bands at 467, 485, 505, 526, and 550 nm which are blue-shifted compared to the ones of the uranyl ion. The luminescence lifetime of the 1:2 complex amounts to 9.21 ± 0.01 µs at -18°C compared to 150.4 ± 0.5 µs for uranyl.
Stability constants of both, the 1:1 and the 1:2 species, have been calculated to be log β110 = 2.66 ± 0.18 and log β120 = 4.48 ± 0.24, respectively. UV-vis spectroscopy combined with factor analysis yielded the molar absorption spectrum of the 1:2 U(VI)-BA species which is characterized by absorption bands at 406, 418, 432.5, 447, and 461 nm and a molar absorption coefficient of 22 L•mol-1•cm-1.]]></dc:description>
<dc:subject><![CDATA[Uranium]]></dc:subject>
<dc:subject><![CDATA[Benzoic Acid]]></dc:subject>
<dc:subject><![CDATA[Complexation]]></dc:subject>
<dc:subject><![CDATA[UV-vis spectroscopy]]></dc:subject>
<dc:subject><![CDATA[Cryo TRLFS]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Körner, M.]]></dc:creator>
<dc:creator><![CDATA[Lenz, K.]]></dc:creator>
<dc:creator><![CDATA[Liedke, M. O.]]></dc:creator>
<dc:creator><![CDATA[Strache, T.]]></dc:creator>
<dc:creator><![CDATA[Keller, A.]]></dc:creator>
<dc:creator><![CDATA[Facsko, S.]]></dc:creator>
<dc:creator><![CDATA[Fassbender, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14810-1</dc:identifier>
<dc:title><![CDATA[Morphology Induced Magnetic Phenomena]]></dc:title>
<dc:source><![CDATA[group seminar, 09.06.2010, München, Germany]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:106-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
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<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
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<dc:title><![CDATA[Formation of CoSi2 wires by maskless implantation with the focused ion beam]]></dc:title>
<dc:source><![CDATA[und Proceedings MRS Fall Meeting, Boston, 29.11.-3.12.1993]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[The maskless ion implatation with the focused ion beam as as a new method for ion beam synthesis of cobalt silicide wires is presented. In order to perform the implantation a special achromatic mass seperator was implemented into the ion column, liquid alloy ion sources for cobalt ions were 30 keV Co+ and 60 keV Co++ ions. The dose dependence for room temperature implantation and the influence of the substrate temperature were investigated.]]></dc:description>
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<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Hesse, E.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
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<dc:title><![CDATA[Formation of CoSi2 wires by maskless implantation with the focused ion beam]]></dc:title>
<dc:source><![CDATA[Materials Research Society, Symposium Proceedings; Materials Synthesis and Processing Using Ion Beams; Vol. 316 (1994) pp. 741-746]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The maskless ion implatation with the focused ion beam as as a new method for ion beam synthesis of cobalt silicide wires is presented. In order to perform the implantation a special achromatic mass seperator was implemented into the ion column, liquid alloy ion sources for cobalt ions were 30 keV Co+ and 60 keV Co++ ions. The dose dependence for room temperature implantation and the influence of the substrate temperature were investigated.]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Hesse, E.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
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<dc:title><![CDATA[Formation of CoSi2 wires by maskless implantation with the focused ion beam]]></dc:title>
<dc:source><![CDATA[Materials Research Society, Symposium Proceedings; Silicides, Germanides, and Their Interfaces; Vol. 320 (1994) pp. 153-158]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[The maskless ion implatation with the focused ion beam as as a new method for ion beam synthesis of cobalt silicide wires is presented. In order to perform the implantation a special achromatic mass seperator was implemented into the ion column, liquid alloy ion sources for cobalt ions were 30 keV Co+ and 60 keV Co++ ions. The dose dependence for room temperature implantation and the influence of the substrate temperature were investigated.]]></dc:description>
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<identifier>HZDR:PUBLDB:1022-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Hausmann, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1022-2</dc:identifier>
<dc:title><![CDATA[RBS and Channeling Analysis of Cobalt Disilicide Layers Produced by Focused Ion Beam Implantation]]></dc:title>
<dc:source><![CDATA[10th Int. School on Vacuum, Electron and Ion Technologies, Varna, Bulgaria, Sept. 22 - 27, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Cobalt disilicide layers were formed by ion beam synthesis using 35 keV Co+ focused ion beam (FIB) implantation into silicon. A strong influence of the pixel dwell time on the layer formation was found. Only for short pixel dwell-times (about 1µs) closed layers with sufficient quality for device application could be formed. To understand the dwell-time effect the as-implanted samples were examined by Rutherford backscattering (RBS) and channeling analysis. A method is presented which allows quantitative measurements of samples where the implanted areas are smaller than the diameter of the RBS beam. Evidence has been obtained that the silicon crystal damage is less for short dwell-times.]]></dc:description>
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<identifier>HZDR:PUBLDB:1022-1</identifier>
<datestamp>2023-04-26</datestamp>
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<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Hausmann, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1022-1</dc:identifier>
<dc:title><![CDATA[RBS and Channeling Analysis of Cobalt Disilicide Layers Produced by Focused Ion Beam Implantation]]></dc:title>
<dc:source><![CDATA[Vacuum, Volume 51, Number 2, Pages 261-266, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Cobalt disilicide layers were formed by ion beam synthesis using 35 keV Co+ focused ion beam (FIB) implantation into silicon. A strong influence of the pixel dwell time on the layer formation was found. Only for short pixel dwell-times (about 1µs) closed layers with sufficient quality for device application could be formed. To understand the dwell-time effect the as-implanted samples were examined by Rutherford backscattering (RBS) and channeling analysis. A method is presented which allows quantitative measurements of samples where the implanted areas are smaller than the diameter of the RBS beam. Evidence has been obtained that the silicon crystal damage is less for short dwell-times.]]></dc:description>
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<identifier>HZDR:PUBLDB:2218-1</identifier>
<datestamp>2019-03-04</datestamp>
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</header>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:creator><![CDATA[Kreißig, U.]]></dc:creator>
<dc:creator><![CDATA[Kruse, O.]]></dc:creator>
<dc:creator><![CDATA[Grigull, S.]]></dc:creator>
<dc:creator><![CDATA[Parascandola, S.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2218-1</dc:identifier>
<dc:title><![CDATA[ERDA in-situ studies of atomic transport processes in various materials]]></dc:title>
<dc:source><![CDATA[Int.Conf. on Swift Heavy Ions in Materials Engeneering and Characterization (SHIMEC-98), New Delhi, Oct. 19 - 22, 1998 (invited lecture)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2219-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Andronenko, L. N.]]></dc:creator>
<dc:creator><![CDATA[Andronenko, M. N.]]></dc:creator>
<dc:creator><![CDATA[Gusev, Y. I.]]></dc:creator>
<dc:creator><![CDATA[Kotov, A. A.]]></dc:creator>
<dc:creator><![CDATA[Neubert, W.]]></dc:creator>
<dc:creator><![CDATA[Petrov, G. E.]]></dc:creator>
<dc:creator><![CDATA[Seliverstov, D. M.]]></dc:creator>
<dc:creator><![CDATA[Strakovski, I. I.]]></dc:creator>
<dc:creator><![CDATA[Vaishnene, L. A.]]></dc:creator>
<dc:creator><![CDATA[Yatsoura, V. I.]]></dc:creator>
<dc:creator><![CDATA[Zalite, A. Y.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2219-1</dc:identifier>
<dc:title><![CDATA[Fragmentation of Be induced by 1 GeV protons]]></dc:title>
<dc:source><![CDATA[Preprint NP-36-1999  Nr. 2321 , St.Petersburg Nuclear Physics Institute ,Gatchina, Russia]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Fragment yields and energy spectra of He, Li and Be isotopes have been measured in p+<sup>9</sup>Be interactions at 1 GeV incident energy at 30 deg. and 126 deg. using a two-arm
spectrometer based on Bragg chambers. The obtained yield ratio of the low abundant
<sup>8</sup>He to <sup>8</sup>Li in the spectator momentum range is compared with published data.]]></dc:description>
<dc:subject><![CDATA[fragmentation]]></dc:subject>
<dc:subject><![CDATA[cross section]]></dc:subject>
<dc:subject><![CDATA[isotope]]></dc:subject>
<dc:subject><![CDATA[proton]]></dc:subject>
<dc:type>info:eu-repo/semantics/other</dc:type>
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<identifier>HZDR:PUBLDB:2678-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Wittern, U.]]></dc:creator>
<dc:creator><![CDATA[Strähle, J.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2678-1</dc:identifier>
<dc:title><![CDATA[Synthese von Nitrenkomplexen mit N-Trimethylsilylanilin. III. Charakterisierung und Kristallstruktur von [Re(NPh)(OsiMe<SUB>3</SUB>)Cl(NH<SUB>2</SUB>Ph)(py)<SUB>2</SUB>][ReO] und <I>trans</I>-[Re<SUB>2</SUB>O<SUB>3</SUB>(py)<SUB>4</SUB>]]]></dc:title>
<dc:source><![CDATA[Z. anorg. allg. Chem. 623, 218 (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2312-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:title><![CDATA[Workshop on Measuring techniques for steady state and transient multiphase flows 1999]]></dc:title>
<dc:source><![CDATA[Kerntechnik 64 (1999) 5-6, p. 309-311]]></dc:source>
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<dc:description><![CDATA[The third workshop on Measuring Techniques for Steady State and Transient Multiphase Flows took place at the Forschungszentrum Rossendorf (FZR) at the 14 Oktober 1999. This series of meetings was initiated by the Institute for Safety Research of the FZR and by the Institute of Process Technology, Process Automation and Measuring Techniques of the University of Applied Science Zittau. The workshop was supported by the Deutsche Gesellschaft für Chemisches Apparatewesen, Chemische Technik und Biotechnologie (DECHEMA) and the Section Thermo and Fluiddynamics of the Kerntechnische Gesellschaft. Two main lectures and 9 technical papers dealt with wall thermography, acoustic and gamma source water level measurement, electro diffusion, optical tomography and velocity and mass flow measurements with wire mesh sensors.]]></dc:description>
<dc:subject><![CDATA[Measuring Techniques for Steady State and Transient Multiphase Flows]]></dc:subject>
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<dc:title><![CDATA[Erzeugung blauer Lumineszenzzentren durch Ionenstrahlsynthese]]></dc:title>
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<dc:title><![CDATA[Alloying by high dose ion implantation of iron into magnesium and aluminium]]></dc:title>
<dc:source><![CDATA[Int. Conf. Appl. Mössbauer Effect, Rio de Janeiro, Brazil, Sept. 14 - 20, 1997 (invited lecture)]]></dc:source>
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<dc:title><![CDATA[Angle dependent Mössbauer spectroscopy on beta-FeSi<SUB>2</SUB> single crystals]]></dc:title>
<dc:source><![CDATA[Int. Conf. Appl. Mössbauer Effect, Rio de Janeiro, Brazil, Sept. 14 - 20, 1997]]></dc:source>
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<dc:title><![CDATA[Investigation of Fe-Mg-alloys produced by ion implantation]]></dc:title>
<dc:source><![CDATA[10th Int. Conf. Surface Modification of Metals by Ion Beams, Gatlinburg, USA, Sept.  21 - 26, 1997]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:title><![CDATA[Analysis and Calculation of an Accident with Delayed Scram on NPP Greifswald Using the Coupled Code DYN3D/ATHLET]]></dc:title>
<dc:source><![CDATA[Proc. 7th Symposium of AER, pp.457-468, KFKI Atomic Energy Research Institute, Budapest (1997)]]></dc:source>
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<dc:description><![CDATA[Analysis and calculation of an abnormal event which occurred in 1989 at the NPP Greifswald (VVER-440/213) are reported about. This event was a scram failure at about 50% nominal power with two of six working main coolant pumps (MCP). The analysis revealed remarkable differences between the active and passive loops due to non-homogeneous coolant mixing in the downcomer and lower plenum in the initial state before the accident. An existing input data deck for the coupled code DYN3D/ATHLET was modified to carry out calculations of this accident. On account of the absence of a mixing model considering loops with forward and loops with backward flow at the same time, the six reactor loops were modeled by a 3-fold (passive), a 2-fold (active) and a single (with the MCP to be switched-off at the beginning of the transient) loop. The comparison of the stationary calculation with the reported data shows a good agreement taking into account the mentioned deviations between the loops. Most of the calculated thermohydraulic parameters during the accident are very close to the measured data. Deviations in the loop temperatures can be explained by the differences in the measured stationary data and by the fact of non-homogeneous coolant mixing in the downcomer and the lower plenum. A small, but continuous power increase was observed during the whole time in the calculation while the measured power was remaining nearly constant. The power behaviour was brought into agreement with the measured data by a correction of the moderator temperature coefficient within the accuracy recommendations of the Atomic Energy Research (AER). 
The calculation of this accident is an important contribution to the validation of the coupled code DYN3D/ATHLET. It demonstrated problems of the analysis of real abnormal events on NPP`s.]]></dc:description>
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<dc:title><![CDATA[Analysis and Calculation of an Accident with Delayed Scram on NPP Greifswald Using the Coupled Code DYN3D/ATHLET]]></dc:title>
<dc:source><![CDATA[7th Symposium of AER]]></dc:source>
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<dc:description><![CDATA[Analysis and calculation of an abnormal event which occurred in 1989 at the NPP Greifswald (VVER-440/213) are reported about. This event was a scram failure at about 50% nominal power with two of six working main coolant pumps (MCP). The analysis revealed remarkable differences between the active and passive loops due to non-homogeneous coolant mixing in the downcomer and lower plenum in the initial state before the accident. An existing input data deck for the coupled code DYN3D/ATHLET was modified to carry out calculations of this accident. On account of the absence of a mixing model considering loops with forward and loops with backward flow at the same time, the six reactor loops were modeled by a 3-fold (passive), a 2-fold (active) and a single (with the MCP to be switched-off at the beginning of the transient) loop. The comparison of the stationary calculation with the reported data shows a good agreement taking into account the mentioned deviations between the loops. Most of the calculated thermohydraulic parameters during the accident are very close to the measured data. Deviations in the loop temperatures can be explained by the differences in the measured stationary data and by the fact of non-homogeneous coolant mixing in the downcomer and the lower plenum. A small, but continuous power increase was observed during the whole time in the calculation while the measured power was remaining nearly constant. The power behaviour was brought into agreement with the measured data by a correction of the moderator temperature coefficient within the accuracy recommendations of the Atomic Energy Research (AER). 
The calculation of this accident is an important contribution to the validation of the coupled code DYN3D/ATHLET. It demonstrated problems of the analysis of real abnormal events on NPP`s.]]></dc:description>
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<dc:title><![CDATA[Structure and magnetic properties in the low temperature annealing range of FeZrBCu-base alloys]]></dc:title>
<dc:source><![CDATA[Soft Magnetic Materials 13, Grenoble, Sept. 24 - 26, 1997]]></dc:source>
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<dc:identifier>https://www.hzdr.de/publications/Publ-2435-1</dc:identifier>
<dc:title><![CDATA[Direct measurements of high-energy secondary electrons during plasma immersion ion implantation]]></dc:title>
<dc:source><![CDATA[3rd Int. Conf. Reactive Plasmas, Nara, Japan, Jan. 21 - 24, 1997]]></dc:source>
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<dc:creator><![CDATA[Nicht, E.-M.]]></dc:creator>
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<dc:title><![CDATA[Positron annihilation spectroscopy, electrical resistivity, and microstructural transmission electron microscopy studies of the CuMn system]]></dc:title>
<dc:source><![CDATA[11th Int. Conf. on Positron Annihilation (ICPA-11), Kansas City, USA, May 25-30, 1997]]></dc:source>
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<dc:creator><![CDATA[Obara, K.]]></dc:creator>
<dc:creator><![CDATA[Yiji, P.]]></dc:creator>
<dc:creator><![CDATA[Chiba, K.]]></dc:creator>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2437-1</dc:identifier>
<dc:title><![CDATA[Surface excitation processes of adsorbed gas molecules on metal surface]]></dc:title>
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]]></dc:description>
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<dc:identifier>https://www.hzdr.de/publications/Publ-2256-1</dc:identifier>
<dc:title><![CDATA[Wear properties of TiN coated cutting tools implanted with nitrogen ions]]></dc:title>
<dc:source><![CDATA[ION´98, Kazimierz Dolny, Poland, June 16-19, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Näser, A.]]></dc:creator>
<dc:creator><![CDATA[Gelhoff, W.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2258-1</dc:identifier>
<dc:title><![CDATA[Paramagnetische Störstellen in Si nach Implantation von Pd]]></dc:title>
<dc:source><![CDATA[DPG-Tagung, Regensburg, Germany,  March 23, 1998]]></dc:source>
<dc:date>1998</dc:date>
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<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Neelmeijer, C.]]></dc:creator>
<dc:creator><![CDATA[Mäder, M.]]></dc:creator>
<dc:creator><![CDATA[Pietsch, U.]]></dc:creator>
<dc:creator><![CDATA[Ulbricht, H.]]></dc:creator>
<dc:creator><![CDATA[Walcha, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2259-1</dc:identifier>
<dc:title><![CDATA[Johann Gregorius Höroldt fecit?]]></dc:title>
<dc:source><![CDATA[Jahrestagung der GDCh, Archäometrie und Denkmalpflege, Würzburg, Sept. 23 - 25, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA["J. G. Höroldt fec. et inv": Gemacht und erdacht von Johann Gregorius Höroldt - findet man als Signatur auf dem Boden der prachtvoll dekorierten "Höroldt-Vase" in der Porzellansammlung im Zwinger. Das typische Höroldt-Motiv findet sich wieder auf einem Walzenkrug, ebenfalls aus weißem Porzellan als Träger. Mittels Ionenstrahlanalyse an Luft gelang es am 5 MV Tandembeschleuniger des FZ Rossendorf, zerstörungsfrei aufzuklären, dass die Pigmente der Schmelzfarben auf der Vase der überlieferten "Höroldt'schen Palette" entsprechen. Im Gegensatz dazu wurde z.B. Chrom-Grün am Walzenkrug gefunden, was eindeutig auf eine Kopie hinweist.]]></dc:description>
<dc:subject><![CDATA[Ionenstrahlanalyse an Luft]]></dc:subject>
<dc:subject><![CDATA[zerstörungsfrei]]></dc:subject>
<dc:subject><![CDATA[PIXE]]></dc:subject>
<dc:subject><![CDATA[Malfarben]]></dc:subject>
<dc:subject><![CDATA[Porzellan]]></dc:subject>
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<identifier>HZDR:PUBLDB:2259-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Neelmeijer, C.]]></dc:creator>
<dc:creator><![CDATA[Mäder, M.]]></dc:creator>
<dc:creator><![CDATA[Pietsch, U.]]></dc:creator>
<dc:creator><![CDATA[Ulbricht, H.]]></dc:creator>
<dc:creator><![CDATA[Walcha, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2259-2</dc:identifier>
<dc:title><![CDATA[Johann Gregorius Höroldt fecit?]]></dc:title>
<dc:source><![CDATA[Archäometrie und Denkmalpflege - Kurzberichte 1998, S. 78 - 80]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA["J. G. Höroldt fec. et inv": Gemacht und erdacht von Johann Gregorius Höroldt - findet man als Signatur auf dem Boden der prachtvoll dekorierten "Höroldt-Vase" in der Porzellansammlung im Zwinger. Das typische Höroldt-Motiv findet sich wieder auf einem Walzenkrug, ebenfalls aus weißem Porzellan als Träger. Mittels Ionenstrahlanalyse an Luft gelang es am 5 MV Tandembeschleuniger des FZ Rossendorf, zerstörungsfrei aufzuklären, dass die Pigmente der Schmelzfarben auf der Vase der überlieferten "Höroldt'schen Palette" entsprechen. Im Gegensatz dazu wurde z.B. Chrom-Grün am Walzenkrug gefunden, was eindeutig auf eine Kopie hinweist.]]></dc:description>
<dc:subject><![CDATA[Ionenstrahlanalyse an Luft]]></dc:subject>
<dc:subject><![CDATA[zerstörungsfrei]]></dc:subject>
<dc:subject><![CDATA[PIXE]]></dc:subject>
<dc:subject><![CDATA[Malfarben]]></dc:subject>
<dc:subject><![CDATA[Porzellan]]></dc:subject>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Neelmeijer, C.]]></dc:creator>
<dc:creator><![CDATA[Mäder, M.]]></dc:creator>
<dc:creator><![CDATA[Pietsch, U.]]></dc:creator>
<dc:creator><![CDATA[Ulbricht, H.]]></dc:creator>
<dc:creator><![CDATA[Walcha, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2259-7</dc:identifier>
<dc:title><![CDATA[Johann Gregorius Höroldt fecit?]]></dc:title>
<dc:source><![CDATA[Archäometrie und Denkmalpflege - Kurzberichte 1998, S. 78 - 80]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA["J. G. Höroldt fec. et inv": Gemacht und erdacht von Johann Gregorius Höroldt - findet man als Signatur auf dem Boden der prachtvoll dekorierten "Höroldt-Vase" in der Porzellansammlung im Zwinger. Das typische Höroldt-Motiv findet sich wieder auf einem Walzenkrug, ebenfalls aus weißem Porzellan als Träger. Mittels Ionenstrahlanalyse an Luft gelang es am 5 MV Tandembeschleuniger des FZ Rossendorf, zerstörungsfrei aufzuklären, dass die Pigmente der Schmelzfarben auf der Vase der überlieferten "Höroldt'schen Palette" entsprechen. Im Gegensatz dazu wurde z.B. Chrom-Grün am Walzenkrug gefunden, was eindeutig auf eine Kopie hinweist.]]></dc:description>
<dc:subject><![CDATA[Ionenstrahlanalyse an Luft]]></dc:subject>
<dc:subject><![CDATA[zerstörungsfrei]]></dc:subject>
<dc:subject><![CDATA[PIXE]]></dc:subject>
<dc:subject><![CDATA[Malfarben]]></dc:subject>
<dc:subject><![CDATA[Porzellan]]></dc:subject>
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<identifier>HZDR:PUBLDB:2036-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2036-1</dc:identifier>
<dc:title><![CDATA[BRICK - ein Simulationstool für Mehrphasenströmungen in Behältern auf der Basis einer Partikelmethode]]></dc:title>
<dc:source><![CDATA[1. Chemnitzer Verfahrenstechnisches Kolloquium, 25.-26. November 1998, TU Chemnitz]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[In dem neu entwickelten 1-D-Behältermodell BRICK werden die Transportvorgänge in
Behältern auf der Grundlage einer neu entwickelten Partikelmethode gelöst. 
Die Methode zielt auf die Vermeidung numerischer Diffusion, was insbesondere bei der Berücksichtigung von Diskontinuitäten, wie z.B. dem Gemischspiegel, von 
Vorteil ist. Die implizite Wiedergabe der aktuellen Position des Gemischspiegels sowie ein spezielles Interface ermöglichen die Beachtung der Entwicklung einer 
Schaumkrone am Übergang zwischen dem Zweiphasengemisch und dem Gasraum.

]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2036-2</dc:identifier>
<dc:title><![CDATA[BRICK - ein Simulationstool für Mehrphasenströmungen in Behältern auf der Basis einer Partikelmethode]]></dc:title>
<dc:source><![CDATA[1. Chemnitzer Verfahrenstechnisches Kolloquium, 25.-26. November 1998, TU Chemnitz]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[In dem neu entwickelten 1-D-Behältermodell BRICK werden die Transportvorgänge in
Behältern auf der Grundlage einer neu entwickelten Partikelmethode gelöst. 
Die Methode zielt auf die Vermeidung numerischer Diffusion, was insbesondere bei der Berücksichtigung von Diskontinuitäten, wie z.B. dem Gemischspiegel, von 
Vorteil ist. Die implizite Wiedergabe der aktuellen Position des Gemischspiegels sowie ein spezielles Interface ermöglichen die Beachtung der Entwicklung einer 
Schaumkrone am Übergang zwischen dem Zweiphasengemisch und dem Gasraum.

]]></dc:description>
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<identifier>HZDR:PUBLDB:2018-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2018-1</dc:identifier>
<dc:title><![CDATA[Dynamische Simulation von Druckentlastungsvorgängen mit dem Programm BRICK]]></dc:title>
<dc:source><![CDATA[45. Sitzung des DECHEMA/GVC-Arbeitsausschuß "Sicherheitsgerechtes Auslegen von Chemieapparaten", Frankfurt am Main, 21./22. April 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Das Programm BRICK gestattet die Berechnung des zeitlichen Verlaufs wichtiger Größen (Druck, Temperatur, Massenaustrag) bei der Druckentlastung chemischer Reaktoren auf Grundlage einer Particle-In-Cell (PIC) Methode. Die wichtigsten Einzelmodelle des Programms werden erläutert. Beispiele zur Validierung werden diskutiert.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:14413-2</identifier>
<datestamp>2025-06-05</datestamp>
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</header>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krause-Rehberg, R.]]></dc:creator>
<dc:creator><![CDATA[Butterling, M.]]></dc:creator>
<dc:creator><![CDATA[Jungmann, M.]]></dc:creator>
<dc:creator><![CDATA[Krille, A.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Rogov, A.]]></dc:creator>
<dc:creator><![CDATA[Noack, K.]]></dc:creator>
<dc:creator><![CDATA[Cowan, T.]]></dc:creator>
<dc:creator><![CDATA[Wagner, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14413-2</dc:identifier>
<dc:title><![CDATA[The EPOS system at the radiation source ELBE at For-schungszentrum Dresden-Rossendorf]]></dc:title>
<dc:source><![CDATA[Proceedings of the International School of Physics "E. Fermi" - Physics with many positrons, 07.-17.07.2009, Varenna, Italia<br>The EPOS system at the radiation source ELBE at For-schungszentrum Dresden-Rossendorf, Amsterdam: IOS Press Amsterdam]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The heart of the radiation source ELBE at the Forschungszentrum Dresden-Rossendorf (FZD) is a 40-MeV LINAC with an average current of 1 mA. Due to its superconducting technology, the time structure is different from conventional LINACs. Electron bunches as short as 2 ps with a 26 MHz repetition rate can be used in continuous operation (cw) mode. This is an ideal host for an intense positron source. After organizing SLOPOS-9 in Rossendorf, it was decided to add EPOS (ELBE Positron Source) to the existing experiments at ELBE. EPOS consists of two LINAC-based setups, Gamma-induced Positron Spectroscopy (GiPS) and Monoenergetic Positron Spectroscopy (MePS). The GiPS setup, where positrons are produced inside the whole sample volume by pair production using a pulsed gamma beam, is unique so far. Here, bulky samples such as coarse powders, dispersions, but also liquids or whole devices of non-destructive testing can be investigated by all positron techniques important for materials science (lifetime spectroscopy, age-momentum correlation, and coincidence Doppler broadening spectroscopy). The same techniques will be applied at the MePS setup, where slow, mono-energetic positrons will be generated by moderation to study near-surface layers. This system is still under construction. The EPOS system will be completed by two conventional setups, a continuous slow positron beam and a positron lifetime/ Doppler spectrometer, both operated by 22Na sources.]]></dc:description>
<dc:subject><![CDATA[Positron spectroscopy]]></dc:subject>
<dc:subject><![CDATA[Positron Annihilation]]></dc:subject>
<dc:subject><![CDATA[Monoenergetic Positrons]]></dc:subject>
<dc:subject><![CDATA[Gamma-induced Positrons]]></dc:subject>
<dc:subject><![CDATA[LINAC-based]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:2050-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:creator><![CDATA[Hornauer, U.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2050-1</dc:identifier>
<dc:title><![CDATA[Inhibition of the Oxidation of Intermetallic TiAl by Ion Implantation]]></dc:title>
<dc:source><![CDATA[8th Week of Doctoral Students (WDS), Charles University, Prag 1999, 24.06.1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The effect of ion beam implantation and plasma immersion ion implantation of chlorine on the high temperature oxidation of titanium aluminides above 800 °C in air was investigated. Thermogravimetric oxidation tests (TGA) were performed to examine the long term protection. Depth profiling with Auger electron spectroscopy (AES) was used to investigate Cl diffusion and oxide formation during the first stage of oxidation. A microscopic model of the chlorine effect will be discussed. A systematic variation of the implantation energy and fluence shows that there is a narrow regime of the Cl concentration for optimum protective effect at 900°C in air. The oxidation rate after this incubation time is reduced by about 2 orders of magnitude compared to untreated Ti50Al and is nearly independent of the fluence. The effect is almost independent of the implantation energy in the range of 15 keV to 1 MeV. First results of plasma immersion ion implantation of chlorine show that it is possible to use this technique to implant also large and complex surfaces.]]></dc:description>
<dc:subject><![CDATA[Implantation]]></dc:subject>
<dc:subject><![CDATA[TiAl]]></dc:subject>
<dc:subject><![CDATA[Intermetallics]]></dc:subject>
<dc:subject><![CDATA[Oxidation]]></dc:subject>
<dc:subject><![CDATA[high temperature oxidation]]></dc:subject>
<dc:subject><![CDATA[Plasma immersion ion implantation]]></dc:subject>
<dc:subject><![CDATA[PSI]]></dc:subject>
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<identifier>HZDR:PUBLDB:1063-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1063-1</dc:identifier>
<dc:title><![CDATA[Main Steam Line Break Analysis of a NPP with VVER by Means of the Coupled Code DYN3D/ATHLET]]></dc:title>
<dc:source><![CDATA[Tagungsband Jahrestagung Kerntechnik '98, S. 15-19]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The coupling of advanced thermohydraulic codes with 3-dimensional neutron kinetic codes corresponds to the effort to replace conservative estimations by best estimate calculations. ATHLET is an advanced thermohydraulic code, developed by the German "Gesellschaft für Anlagen- und Reaktorsicherheit" (GRS). The DYN3D code, developed at Forschungszentrum Rossendorf (FZR) for the simulation of reactivity initiated accidents in nuclear reactors with hexagonal and Cartesian fuel element cross section geometry comprises 3-dimensional neutron kinetics, models for the thermohydraulics of the core and the thermomechanical fuel rod behaviour.

Both versions of DYN3D for hexagonal and Cartesian fuel element geometry were coupled with ATHLET according to two basically different strategies. The first way of coupling uses only the neutron kinetics part of DYN3D (internal coupling). In the second way, the whole core is cut out from the ATHLET plant model and is completely described by DYN3D (external coupling). In this case the values of pressure, mass flow rate, enthalpy and boron acid concentration at the bottom and at the top of the core have to be transferred between the codes. This way of coupling is efficiently supported by the General Control and Simulation Module (GCSM) of ATHLET.

The coupled code DYN3D/ATHLET was used to investigate the possibility of recriticality during an asymmetrical overcooling of the reactor core of a NPP with VVER-440 after a main steam line break (MSLB). This MSLB analysis was performed for hot zero power and end of fuel cycle conditions. Different coolant mixing conditions in the lower plenum of the reactor were simulated. The results show the importance of these conditions. In case of a realistic mixing model and without consideration of mixing, i.e. where each loop is connected to a particular 1/6 sector of the core, a recriticality after reactor scram was predicted. For ideal mixing only, recriticality can be avoided.

]]></dc:description>
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<identifier>HZDR:PUBLDB:1063-3</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1063-3</dc:identifier>
<dc:title><![CDATA[Main Steam Line Break Analysis of a NPP with VVER by Means of the Coupled Code DYN3D/ATHLET]]></dc:title>
<dc:source><![CDATA[Proc. TOPSAFE `98, Session TSC-1a, ENS, Valencia (Spain), 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The coupling of advanced thermohydraulic codes with 3-dimensional neutron kinetic codes corresponds to the effort to replace conservative estimations by best estimate calculations. ATHLET is an advanced thermohydraulic code, developed by the German "Gesellschaft für Anlagen- und Reaktorsicherheit" (GRS). The DYN3D code, developed at Forschungszentrum Rossendorf (FZR) for the simulation of reactivity initiated accidents in nuclear reactors with hexagonal and Cartesian fuel element cross section geometry comprises 3-dimensional neutron kinetics, models for the thermohydraulics of the core and the thermomechanical fuel rod behaviour.

Both versions of DYN3D for hexagonal and Cartesian fuel element geometry were coupled with ATHLET according to two basically different strategies. The first way of coupling uses only the neutron kinetics part of DYN3D (internal coupling). In the second way, the whole core is cut out from the ATHLET plant model and is completely described by DYN3D (external coupling). In this case the values of pressure, mass flow rate, enthalpy and boron acid concentration at the bottom and at the top of the core have to be transferred between the codes. This way of coupling is efficiently supported by the General Control and Simulation Module (GCSM) of ATHLET.

The coupled code DYN3D/ATHLET was used to investigate the possibility of recriticality during an asymmetrical overcooling of the reactor core of a NPP with VVER-440 after a main steam line break (MSLB). This MSLB analysis was performed for hot zero power and end of fuel cycle conditions. Different coolant mixing conditions in the lower plenum of the reactor were simulated. The results show the importance of these conditions. In case of a realistic mixing model and without consideration of mixing, i.e. where each loop is connected to a particular 1/6 sector of the core, a recriticality after reactor scram was predicted. For ideal mixing only, recriticality can be avoided.

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<identifier>HZDR:PUBLDB:1063-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1063-2</dc:identifier>
<dc:title><![CDATA[Main Steam Line Break Analysis of a NPP with VVER by Means of the Coupled Code DYN3D/ATHLET]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik '98]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The coupling of advanced thermohydraulic codes with 3-dimensional neutron kinetic codes corresponds to the effort to replace conservative estimations by best estimate calculations. ATHLET is an advanced thermohydraulic code, developed by the German "Gesellschaft für Anlagen- und Reaktorsicherheit" (GRS). The DYN3D code, developed at Forschungszentrum Rossendorf (FZR) for the simulation of reactivity initiated accidents in nuclear reactors with hexagonal and Cartesian fuel element cross section geometry comprises 3-dimensional neutron kinetics, models for the thermohydraulics of the core and the thermomechanical fuel rod behaviour.

Both versions of DYN3D for hexagonal and Cartesian fuel element geometry were coupled with ATHLET according to two basically different strategies. The first way of coupling uses only the neutron kinetics part of DYN3D (internal coupling). In the second way, the whole core is cut out from the ATHLET plant model and is completely described by DYN3D (external coupling). In this case the values of pressure, mass flow rate, enthalpy and boron acid concentration at the bottom and at the top of the core have to be transferred between the codes. This way of coupling is efficiently supported by the General Control and Simulation Module (GCSM) of ATHLET.

The coupled code DYN3D/ATHLET was used to investigate the possibility of recriticality during an asymmetrical overcooling of the reactor core of a NPP with VVER-440 after a main steam line break (MSLB). This MSLB analysis was performed for hot zero power and end of fuel cycle conditions. Different coolant mixing conditions in the lower plenum of the reactor were simulated. The results show the importance of these conditions. In case of a realistic mixing model and without consideration of mixing, i.e. where each loop is connected to a particular 1/6 sector of the core, a recriticality after reactor scram was predicted. For ideal mixing only, recriticality can be avoided.

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<header>
<identifier>HZDR:PUBLDB:1063-4</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1063-4</dc:identifier>
<dc:title><![CDATA[Main Steam Line Break Analysis of a NPP with VVER by Means of the Coupled Code DYN3D/ATHLET]]></dc:title>
<dc:source><![CDATA[TOPSAFE `98, Session TSC-1a, ENS, Valencia (Spain), 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The coupling of advanced thermohydraulic codes with 3-dimensional neutron kinetic codes corresponds to the effort to replace conservative estimations by best estimate calculations. ATHLET is an advanced thermohydraulic code, developed by the German "Gesellschaft für Anlagen- und Reaktorsicherheit" (GRS). The DYN3D code, developed at Forschungszentrum Rossendorf (FZR) for the simulation of reactivity initiated accidents in nuclear reactors with hexagonal and Cartesian fuel element cross section geometry comprises 3-dimensional neutron kinetics, models for the thermohydraulics of the core and the thermomechanical fuel rod behaviour.

Both versions of DYN3D for hexagonal and Cartesian fuel element geometry were coupled with ATHLET according to two basically different strategies. The first way of coupling uses only the neutron kinetics part of DYN3D (internal coupling). In the second way, the whole core is cut out from the ATHLET plant model and is completely described by DYN3D (external coupling). In this case the values of pressure, mass flow rate, enthalpy and boron acid concentration at the bottom and at the top of the core have to be transferred between the codes. This way of coupling is efficiently supported by the General Control and Simulation Module (GCSM) of ATHLET.

The coupled code DYN3D/ATHLET was used to investigate the possibility of recriticality during an asymmetrical overcooling of the reactor core of a NPP with VVER-440 after a main steam line break (MSLB). This MSLB analysis was performed for hot zero power and end of fuel cycle conditions. Different coolant mixing conditions in the lower plenum of the reactor were simulated. The results show the importance of these conditions. In case of a realistic mixing model and without consideration of mixing, i.e. where each loop is connected to a particular 1/6 sector of the core, a recriticality after reactor scram was predicted. For ideal mixing only, recriticality can be avoided.

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<header>
<identifier>HZDR:PUBLDB:981-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-981-1</dc:identifier>
<dc:title><![CDATA[Definition of the Fifth Dynamic AER Benchmark Problem - A Benchmark for Coupled Thermohydraulic/ Three-Dimensional Hexagonal Neutron Kinetic Codes]]></dc:title>
<dc:source><![CDATA[Proc. 7th Symposium of AER, pp.429-438 , KFKI Atomic Energy Research Institute, Budapest (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The fifth dynamic benchmark defined in this paper is the first benchmark for coupled thermohydraulic system/three-dimensional neutron kinetic core models. In this benchmark the interaction between the components of a VVER-440 NPP with the reactor core should be investigated.

The initiating event is a symmetrical break of the main steam header (MSH) at the end of the first fuel cycle and hot shutdown conditions with one stuck out control rod group. The main purpose is the investigation of recriticality. For this reason, the calculation should be continued until the power excursion is eventually terminated by high-borated water from the high pressure injection system.

The participants of the benchmark should use own input data decks developed according to the needs of their own codes. The main geometrical parameters and characteristics of control and safety systems to be considered in this benchmark will be given to bring into agreement the data decks. Own best estimate nuclear cross section data should be used in the calculation. Only the initial subcriticality at the beginning of the transient will be given to made the results more comparable. ]]></dc:description>
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<identifier>HZDR:PUBLDB:981-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kliem, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-981-2</dc:identifier>
<dc:title><![CDATA[Definition of the Fifth Dynamic AER Benchmark Problem - A Benchmark for Coupled Thermohydraulic/ Three-Dimensional Hexagonal Neutron Kinetic Codes]]></dc:title>
<dc:source><![CDATA[7th Symposium of AER]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The fifth dynamic benchmark defined in this paper is the first benchmark for coupled thermohydraulic system/three-dimensional neutron kinetic core models. In this benchmark the interaction between the components of a VVER-440 NPP with the reactor core should be investigated.

The initiating event is a symmetrical break of the main steam header (MSH) at the end of the first fuel cycle and hot shutdown conditions with one stuck out control rod group. The main purpose is the investigation of recriticality. For this reason, the calculation should be continued until the power excursion is eventually terminated by high-borated water from the high pressure injection system.

The participants of the benchmark should use own input data decks developed according to the needs of their own codes. The main geometrical parameters and characteristics of control and safety systems to be considered in this benchmark will be given to bring into agreement the data decks. Own best estimate nuclear cross section data should be used in the calculation. Only the initial subcriticality at the beginning of the transient will be given to made the results more comparable. ]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2051-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Enghardt, W.]]></dc:creator>
<dc:creator><![CDATA[Gabriel, F.]]></dc:creator>
<dc:creator><![CDATA[Gippner, P.]]></dc:creator>
<dc:creator><![CDATA[Grosse, E.]]></dc:creator>
<dc:creator><![CDATA[Guratzsch, H.]]></dc:creator>
<dc:creator><![CDATA[Janssen, D.]]></dc:creator>
<dc:creator><![CDATA[Michel, P.]]></dc:creator>
<dc:creator><![CDATA[Nething, U.]]></dc:creator>
<dc:creator><![CDATA[Neubert, W.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Schilling, K.-D.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Seidel, W.]]></dc:creator>
<dc:creator><![CDATA[Steegmüller, U.]]></dc:creator>
<dc:creator><![CDATA[Stein, P.]]></dc:creator>
<dc:creator><![CDATA[Wagner, W.]]></dc:creator>
<dc:creator><![CDATA[Wenzel, M.]]></dc:creator>
<dc:creator><![CDATA[Wolf, A.]]></dc:creator>
<dc:creator><![CDATA[Wünsch, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2051-1</dc:identifier>
<dc:title><![CDATA[The ELBE Radiation Source Project]]></dc:title>
<dc:source><![CDATA[Acta Physica Polonica B, No. 5, Vol. 30 (1999), pp. 1639-1645]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2057-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Römer, J.]]></dc:creator>
<dc:creator><![CDATA[Füchtner, F.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2057-2</dc:identifier>
<dc:title><![CDATA[SYNTHESIS OF A NEW TRACER FOR CANCER IMAGING: 16alpha-[<SUP>18</SUP>F]FLUOROESTRADIOL-3,17beta-DISULPHAMATE]]></dc:title>
<dc:source><![CDATA[8<SUP>th</SUP> Conference of Central European Division of International Isotope Society, Bad Soden, 10.-11.6.1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The synthesis of 16alpha-[<SUP>18</SUP>F]fluoroestradiol-3,17beta-disulphamate ([<SUP>18</SUP>F]FESDS) being a new potential radiotracer for investigations in positron emission tomography  is described. 16alpha-[<SUP>18</SUP>F]Fluoroestradiol ([<SUP>18</SUP>F]FES) is converted with excessive sulphamoyl chloride in absolute acetonitrile in presence of an alkali. Using kryptofix 2.2.2 and K<SUB>2</SUB>CO<SUB>3</SUB> as alkali, [<SUP>18</SUP>F]FESDS was obtained in yields of 50 - 60%.]]></dc:description>
<dc:subject><![CDATA[Synthesis]]></dc:subject>
<dc:subject><![CDATA[<SUP>18</SUP>F labelling]]></dc:subject>
<dc:subject><![CDATA[radiotracer]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:326-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Hesse, E.]]></dc:creator>
<dc:creator><![CDATA[Schneider, P.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Geßner, T.]]></dc:creator>
<dc:creator><![CDATA[Löbner, B.]]></dc:creator>
<dc:creator><![CDATA[Zichner, N.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-326-1</dc:identifier>
<dc:title><![CDATA[Comparision of CoSi2 Interconnection Lines on Crystalline and Noncrystalline Silicon Fabricated by Writing Focused Ion Beam Implantation]]></dc:title>
<dc:source><![CDATA[Applied Surface Science 91 (1995) pp. 44-49]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[A focused beam of Co+ ions has been used to produce CoSi2 interconnects by means of ion beam synthesis. Investigations have been performed using polysilicon, amorphous and crystalline silicon substrates. The influence of implantation dose and annealing temperature on the resistivity has been studied. For room temperature implantation and annealing 600°C for 1h, a resistivity of about 60µ(*cm has been obtained independent of the subtrate type. The CoSi2 layers have been found to be stable up to 700°C. CoSi2 interconnects have been fabricated on the slope walls of 200µm deep anisotropically etched grooves using a dynamic focus control of the focused ion beam.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:326-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Hesse, E.]]></dc:creator>
<dc:creator><![CDATA[Schneider, P.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Geßner, T.]]></dc:creator>
<dc:creator><![CDATA[Löbner, B.]]></dc:creator>
<dc:creator><![CDATA[Zichner, N.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-326-2</dc:identifier>
<dc:title><![CDATA[Comparision of CoSi2 Interconnection Lines on Crystalline and Noncrystalline Silicon Fabricated by Writing Focused Ion Beam Implantation]]></dc:title>
<dc:source><![CDATA[MAM '95]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[A focused beam of Co+ ions has been used to produce CoSi2 interconnects by means of ion beam synthesis. Investigations have been performed using polysilicon, amorphous and crystalline silicon substrates. The influence of implantation dose and annealing temperature on the resistivity has been studied. For room temperature implantation and annealing 600°C for 1h, a resistivity of about 60µ(*cm has been obtained independent of the subtrate type. The CoSi2 layers have been found to be stable up to 700°C. CoSi2 interconnects have been fabricated on the slope walls of 200µm deep anisotropically etched grooves using a dynamic focus control of the focused ion beam.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:3146-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Jäger, H.-U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3146-1</dc:identifier>
<dc:title><![CDATA[Computer simulation of defect evolution during high-energy ion implantation and subsequent annealing]]></dc:title>
<dc:source><![CDATA[IUMRS-ICAM99 Conference, Symposium M: Si-based Materials and Devices, Beijing, China, June 13- 18, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1605-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hausmann, S.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:creator><![CDATA[Fuhrmann, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1605-2</dc:identifier>
<dc:title><![CDATA[Dwell-time effects in focused ion beam synthesis of cobalt disilicide: reflectivity measurements]]></dc:title>
<dc:source><![CDATA[11th  Int. Conf. on Ion Beam Modification of Materials, Amsterdam, Aug. 31  Sept. 4,1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Cobalt disilicide layers were produced by 70 keV Co2+ focused ion beam implantation into Si(111) at temperatures of about 400°C and subsequent annealing. The CoSi2 layer quality depends on pixel dwell-time and subtrate temperature. Only properly chosen parameters result in a continuous layer. The dwell-time (1-250 µs) and substrate temperature (355-400°C) dependence was investigated by scanning electron microscopy, reflectivity measurements and Rutherford backscattering spectroscopy/channeling. The results show that the irradiation damage increases with dwell-time and decreases with temperature, indicating an interplay between the damage creation rate and the dynamic annealing rate. Already after implantation of less than a tenth part of the dose required for continuous layer formation, the quality of the resulting CoSi2 layer is predertermined.]]></dc:description>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<header>
<identifier>HZDR:PUBLDB:1605-1</identifier>
<datestamp>2023-05-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hausmann, S.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:creator><![CDATA[Fuhrmann, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1605-1</dc:identifier>
<dc:title><![CDATA[Dwell-time effects in focused ion beam synthesis of cobalt disilicide: reflectivity measurements]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B, 148 (1999) 610-614]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Cobalt disilicide layers were produced by 70 keV Co2+ focused ion beam implantation into Si(111) at temperatures of about 400°C and subsequent annealing. The CoSi2 layer quality depends on pixel dwell-time and subtrate temperature. Only properly chosen parameters result in a continuous layer. The dwell-time (1-250 µs) and substrate temperature (355-400°C) dependence was investigated by scanning electron microscopy, reflectivity measurements and Rutherford backscattering spectroscopy/channeling. The results show that the irradiation damage increases with dwell-time and decreases with temperature, indicating an interplay between the damage creation rate and the dynamic annealing rate. Already after implantation of less than a tenth part of the dose required for continuous layer formation, the quality of the resulting CoSi2 layer is predertermined.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0168-583X(98)00786-1]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1605-1</dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:366-2</identifier>
<datestamp>2020-12-09</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-366-2</dc:identifier>
<dc:title><![CDATA[Submicron CoSi<SUB>2</SUB>-structures fabricated by focused ion beam implantation and local flash lamp melting]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 112 (1996) pp. 201-205]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[A new way to fabricate submicron CoSi2 structures on Si wafers is presented. The method consists of a combination of focused ion beam (FIB) implantation of Co+ ions and subsequent flash lamp irradiation. With our FIB equipment IMSA-100 one- and two dimensional structures were implanted by writing with a 35 keV Co+ beam which was focused to a spot diameter of 200nm. However, for the porposed method the spot size is not the crucial dimension because the final structure size is controlled by a local melting  and recrystallization process in the implanted regions. Here the structure size is determined by the amount of implanted atoms which can be concentrated by the local melting process into the submicron CoSi2 structures. The local melting is caused by heteronucleation at the Si wafer surface during the short period of superheating, which is obtained by intense flash lamp irradiation of 3 or 20 ms duration. Disintegration of implanted CoSi2 wires by precipitate formation during thermal annealing, which was reported by Liddle et al. (Mater. Res. Soc. Symp. Proc. 279 (1993) 881), can be avoided by this method. The CoSi2 structures were analysed by scanning electron microscopy (SEM) and energy dispersiv X-ray analysis (EDX). Dots and wires of about 200 nm diameter and width, respectively, have been fabricated during these first experiments, whilst smaller dimensions seem to be possible in future.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/0168-583X(95)01250-8]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-366-2</dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:409-1</identifier>
<datestamp>2020-12-09</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Driesel, W.]]></dc:creator>
<dc:creator><![CDATA[Dietzsch, C.]]></dc:creator>
<dc:creator><![CDATA[Hesse, E.]]></dc:creator>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-409-1</dc:identifier>
<dc:title><![CDATA[In situ observation of the tip shape of Co-Ge liquid alloy ion sources in a high-voltage transmission electron microscope]]></dc:title>
<dc:source><![CDATA[Journal of Vacuum Science and Technology Part B 14 (1996) 3 pp. 1621-29]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[For in situ observation in a 1 MeV TEM Co-Ge liquid alloy ion soures (LAISs) were mountet to a special specimen holder revealing the formation of the field-stabilizes Co-Ge liquid alloy cone, the change in the tip shape as a function of the ion emission current, spatial shifts of the liquid alloy cone, and microdroplet emission from Co-Ge LAISs. This has facilitated the better understanding of the ion and microdroplet emission process from  Co-Ge LAISs in a large range of ion current. Below the onset voltage the shape of the tip covered with the liquid Co-Ge alloy is spherical. At the onset voltage the Tayler cone is formed. A jetlike protrusion at the cone vertex. The cone half-angle a decreases and the jet length l increases with increasing emission current le. Linear dependences of a and l on Ie are found. Emission of microdroplets is observed at the shanks behind the Tayler cone. The radius of microdroplets varied between 0.035 and 10 µm. These microdroplets are emitted in time intervals of about 0.1 s and more.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1116/1.589201]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-409-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:446-1</identifier>
<datestamp>2021-11-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Hesse, E.]]></dc:creator>
<dc:creator><![CDATA[Prewett, P. D.]]></dc:creator>
<dc:creator><![CDATA[Watson, J. G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-446-1</dc:identifier>
<dc:title><![CDATA[Cluster beams from a Co-Nd liquid alloy ion source]]></dc:title>
<dc:source><![CDATA[Microelectronic Engineering 30 (1996) pp. 245-248]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[A Cobalt-Neodymium Liquid Alloy Ion Source (LAIS) is investigated with respect to ist cluster emission behaviour. Clusters and molecular ions were found. The influence of the source emission current on the cluster emission intensity and also on the cluster mass distributationis studied. The Co-Nd LAIS was used for writing patterning (implantation, sputtering) in a mass-selecting Focused Cluster Beam (FCB) system. Theoretical estimations were carried out concerning the use of the FCB for direct deposition at landing energies of about 100 eV / atom. First experimental results of cobalt FCBs are presented.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/0167-9317(95)00237-5]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-446-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:446-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Hesse, E.]]></dc:creator>
<dc:creator><![CDATA[Prewett, P. D.]]></dc:creator>
<dc:creator><![CDATA[Watson, J. G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-446-2</dc:identifier>
<dc:title><![CDATA[Cluster beams from a Co-Nd liquid alloy ion source]]></dc:title>
<dc:source><![CDATA[MNE'95]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[A Cobalt-Neodymium Liquid Alloy Ion Source (LAIS) is investigated with respect to ist cluster emission behaviour. Clusters and molecular ions were found. The influence of the source emission current on the cluster emission intensity and also on the cluster mass distributationis studied. The Co-Nd LAIS was used for writing patterning (implantation, sputtering) in a mass-selecting Focused Cluster Beam (FCB) system. Theoretical estimations were carried out concerning the use of the FCB for direct deposition at landing energies of about 100 eV / atom. First experimental results of cobalt FCBs are presented.]]></dc:description>
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<dc:title><![CDATA[High current FIB system for micromechanics application]]></dc:title>
<dc:source><![CDATA[Microelectronic Engineering 21 (1993) pp. 197-200]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[A high current Focused Ion Beam (FIB) system, designd to achieve current dendities above 10 A/cm2 is presented. The system parameters and properties are discussed and first applications in the field of micromechanics are shown.]]></dc:description>
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<dc:source><![CDATA[30th Polish Seminar on Positron Annihilation, Jarnoltowek, Sept. 17-21, 1998]]></dc:source>
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<dc:title><![CDATA[Correlation of electrical and microstructural properties after high dose aluminium implantation into 6H-SiC]]></dc:title>
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<dc:title><![CDATA[Formation of surface Pd-Ti alloys using pulsed plasma beams]]></dc:title>
<dc:source><![CDATA[ION'98, Kazimierz Dolny, Poland, June 16-19, 1998]]></dc:source>
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<dc:title><![CDATA[Pulsed plasma beam mixing of Ti and Mo on Al<SUB>2</SUB>O<SUB>3</SUB> substrates]]></dc:title>
<dc:source><![CDATA[11th Int. Conf. on Ion Beam Modification of Materials, Amsterdam, The Netherlands, 
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<dc:title><![CDATA[Microscopic processes of damage production during ion implantation studied by combining time-ordered BCA with MD simulations]]></dc:title>
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<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
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<dc:title><![CDATA[Is there still any hope for blue luminescence from silicon?]]></dc:title>
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<dc:date>1998</dc:date>
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<dc:title><![CDATA[Charakterisierung von durch Ionenimplantation hergestellten Fe-Al-Schichten mittels Augerelektronen- und Mößbauerspektroskopie]]></dc:title>
<dc:source><![CDATA[10. Arbeitstagung Angewandte Oberflächenanalytik AOFA 10, Kaiserslautern, Sept. 6-10, 1998]]></dc:source>
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<dc:title><![CDATA[Temperaturverhalten von durch Hochdosisimplantation hergestellten Al-Fe-Legierungen]]></dc:title>
<dc:source><![CDATA[IX. Mößbauerkolloquium, Freiberg, Sept. 28-30, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2276-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Sendezera, E. J.]]></dc:creator>
<dc:creator><![CDATA[Davidson, A. T.]]></dc:creator>
<dc:creator><![CDATA[Fischer, C. G.]]></dc:creator>
<dc:creator><![CDATA[Connell, S. H.]]></dc:creator>
<dc:creator><![CDATA[Sellschop, J. P. F.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Nicht, E.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2276-1</dc:identifier>
<dc:title><![CDATA[Characterisation of Al-implanted LiF by a monoenergetic positron beam]]></dc:title>
<dc:source><![CDATA[8th Int. Workshop on Slow Positron Beam Techniques for Solids and Surfaces (SLOPOS-8), Cape Town, Sept. 6 - 12, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2277-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Serre, C.]]></dc:creator>
<dc:creator><![CDATA[Perez-Rodriguez, A.]]></dc:creator>
<dc:creator><![CDATA[Romano-Rodriguez, A.]]></dc:creator>
<dc:creator><![CDATA[Morante, J. R.]]></dc:creator>
<dc:creator><![CDATA[Fonseca, L.]]></dc:creator>
<dc:creator><![CDATA[Acero, M. C.]]></dc:creator>
<dc:creator><![CDATA[Esteve, J.]]></dc:creator>
<dc:creator><![CDATA[Kögler, R.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2277-1</dc:identifier>
<dc:title><![CDATA[Bonding and etch-back of ion beam synthesized beta-SiC for SiCOI formation]]></dc:title>
<dc:source><![CDATA[NATO Advanced Workshop "Perspectives, Science and Technologies for Novel Silicon on Insulator Devices", Kiev, Ukraine, Oct. 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2279-1</identifier>
<datestamp>2019-03-04</datestamp>
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            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2279-1</dc:identifier>
<dc:title><![CDATA[Ion beam processing for silicon-based light emission]]></dc:title>
<dc:source><![CDATA[XIIth Int. Conf. Ion Implantation Technology (IIT´98), Kyoto, Japan, June 22-26, 1998]]></dc:source>
<dc:date>1998</dc:date>
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<identifier>HZDR:PUBLDB:2280-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hauschild, T.]]></dc:creator>
<dc:creator><![CDATA[Jentschel, M.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Börner, H. G.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2280-1</dc:identifier>
<dc:title><![CDATA[Study of Interatomic Potentials in ZnS using Crystal-GRID high-precision gamma spectroscopy and MD simulations]]></dc:title>
<dc:source><![CDATA[ICACS-18, Odense, Denmark, August 3-8, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Crystal-GRID measurements have been performed with ZnS single crystals. A new Crystal-GRID potential could be determined by splining a Stillinger-Weber like equilibrium potential to screened Coulomb potentials. The new potential is fitted to experimental data containing information about the energy range of about 10 to 500 eV and differs significantly from the screened Coulomb potentials. The nuclear level life time of the 3221 keV level in 33S has been determined to be (48.8 +/- 0.7) fs. Furthermore the predicted asymmetry of a Crystal-GRID line shape could be observed for the first time. ]]></dc:description>
<dc:subject><![CDATA[Crystal-GRID]]></dc:subject>
<dc:subject><![CDATA[gamma ray spectroscopy]]></dc:subject>
<dc:subject><![CDATA[interatomic potential]]></dc:subject>
<dc:subject><![CDATA[Molecular Dynamics simulation]]></dc:subject>
<dc:subject><![CDATA[nuclear level lifetime]]></dc:subject>
<dc:subject><![CDATA[ZnS]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:14511-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Battistoni, G.]]></dc:creator>
<dc:creator><![CDATA[Broggi, F.]]></dc:creator>
<dc:creator><![CDATA[Brugger, M.]]></dc:creator>
<dc:creator><![CDATA[Campanella, M.]]></dc:creator>
<dc:creator><![CDATA[Carboni, M.]]></dc:creator>
<dc:creator><![CDATA[Empl, A.]]></dc:creator>
<dc:creator><![CDATA[Fassò, A.]]></dc:creator>
<dc:creator><![CDATA[Gadioli, E.]]></dc:creator>
<dc:creator><![CDATA[Cerutti, F.]]></dc:creator>
<dc:creator><![CDATA[Ferrari, A.]]></dc:creator>
<dc:creator><![CDATA[Ferrari, A.]]></dc:creator>
<dc:creator><![CDATA[Garzelli, M.]]></dc:creator>
<dc:creator><![CDATA[Lantz, M.]]></dc:creator>
<dc:creator><![CDATA[Mairani, A.]]></dc:creator>
<dc:creator><![CDATA[Margiotta, A.]]></dc:creator>
<dc:creator><![CDATA[Morone, C.]]></dc:creator>
<dc:creator><![CDATA[Muraro, S.]]></dc:creator>
<dc:creator><![CDATA[Parodi, K.]]></dc:creator>
<dc:creator><![CDATA[Patera, V.]]></dc:creator>
<dc:creator><![CDATA[Pelliccioni, M.]]></dc:creator>
<dc:creator><![CDATA[Pinsky, L.]]></dc:creator>
<dc:creator><![CDATA[Ranft, J.]]></dc:creator>
<dc:creator><![CDATA[Roesler, S.]]></dc:creator>
<dc:creator><![CDATA[Rollet, S.]]></dc:creator>
<dc:creator><![CDATA[Sala, P. R.]]></dc:creator>
<dc:creator><![CDATA[Santana, M.]]></dc:creator>
<dc:creator><![CDATA[Sarchiapone, L.]]></dc:creator>
<dc:creator><![CDATA[Sioli, M.]]></dc:creator>
<dc:creator><![CDATA[Smirnov, G.]]></dc:creator>
<dc:creator><![CDATA[Sommerer, F.]]></dc:creator>
<dc:creator><![CDATA[Theis, C.]]></dc:creator>
<dc:creator><![CDATA[Trovati, S.]]></dc:creator>
<dc:creator><![CDATA[Villari, R.]]></dc:creator>
<dc:creator><![CDATA[Vincke, H.]]></dc:creator>
<dc:creator><![CDATA[Vincke, H.]]></dc:creator>
<dc:creator><![CDATA[Vlachoudis, V.]]></dc:creator>
<dc:creator><![CDATA[Vollaire, J.]]></dc:creator>
<dc:creator><![CDATA[Zapp, N.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14511-1</dc:identifier>
<dc:title><![CDATA[The application of the Monte Carlo code FLUKA in radiation protection studies for the Large Hadron Collider]]></dc:title>
<dc:source><![CDATA[Joint International Conference on Supercomputing in Nuclear Applications and Monte Carlo 2010 (SNA + MC2010), 17.-21.10.2010, Tokyo, Japan<br>Progress in Nuclear Science and Technology 2(2011), 358-364]]></dc:source>
<dc:date>2011</dc:date>
<dc:description><![CDATA[The multi-purpose particle interaction and transport code FLUKA is integral part of all radiation protection studies for the design and operation of the Large Hadron Collider (LHC) at CERN. It is one of the very few codes available for this type of calculations which is capable to calculate in one and the same simulation proton-proton and heavy ion collisions at LHC energies as well as the entire hadronic and electromagnetic particle cascade initiated by secondary particles in detectors and beam-line components from TeV energies down to energies of thermal neutrons. The present paper reviews these capabilities of FLUKA in giving details of relevant physics models along with examples of radiation protection studies for the LHC such as shielding studies for underground areas occupied by personnel during LHC operation and the simulation of induced radioactivity around beam loss points. Integral part of the FLUKA development is a careful benchmarking of specific models as well as the code performance in complex, real life applications which is demonstrated with examples of studies relevant to radiation protection at the LHC.]]></dc:description>
<dc:subject><![CDATA[radiation protection]]></dc:subject>
<dc:subject><![CDATA[shielding calculations]]></dc:subject>
<dc:subject><![CDATA[activation]]></dc:subject>
<dc:subject><![CDATA[FLUKA]]></dc:subject>
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<identifier>HZDR:PUBLDB:2997-1</identifier>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hoppe, D.]]></dc:creator>
<dc:creator><![CDATA[Giera, H.-D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2997-1</dc:identifier>
<dc:title><![CDATA[Anordnung zur akustischen Volumenbestimmung]]></dc:title>
<dc:source><![CDATA[DE 198 30 442 A1]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Mit der Erfindung soll die Anwendung eines passiven Resonanzverfahrens auch ohne determinierte Anregung ermöglicht werden.
Die technische Lösung baut auf der Anwendung bekannter Schallaufnehmer und eines Signalvergleichers auf.]]></dc:description>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Lindau, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2998-1</dc:identifier>
<dc:title><![CDATA[Vorrichtung zum Fördern von Schüttgut mittels Vibrationsförderung]]></dc:title>
<dc:source><![CDATA[DE 198 35 530A1]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Aufgabe der Erfindung ist es, einen Vibrationsförderer dahingehend zu verändern, daß insbesondere an der Abwurfstelle auch bei kleinen Förderstömen schwerfließender Schüttgüter ein kontinuierlicher Transport erreichbar ist.]]></dc:description>
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<identifier>HZDR:PUBLDB:2999-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Förster, E.]]></dc:creator>
<dc:creator><![CDATA[Eisold, B.]]></dc:creator>
<dc:creator><![CDATA[Hiller, B.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2999-1</dc:identifier>
<dc:title><![CDATA[Vorrichtung zum Öffnen von Glasampullen]]></dc:title>
<dc:source><![CDATA[DE 198 41 722 A1]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Aufgabe der Erfindung ist eine Vorrichtung, die ein sicheres und rationelles Öffnen der Glasampullen unterschiedlicher Größe und Bauform mit geringem Aufwand ermöglicht,  wobei ein  möglichst vollständiges Verwenden des Inhalts der Glasampullen erfolgen soll.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:230-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-230-2</dc:identifier>
<dc:title><![CDATA[Coupling of the Thermohydraulic Code ATHLET with the Neutron Kinetic Core Model DYN3D]]></dc:title>
<dc:source><![CDATA[Int. Conf. on Mathematics and Computations, Reactor Physics and Environmental Analysis, April 30. - May 5., 1995, Portland, Oregon, USA, Proc., Vol. 1, pp. 257 - 263]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[ The coupling of advanced thermohydraulic codes with 3-dimensional neutron kinetic codes corresponds to the effort to replace conservative estimations by best estimate calculations. ATHLET is an advanced thermohydraulic code, developed by the German Gesellschaft fr Anlagen- und Reaktorsicherheit (GRS). Up to now only point kinetics and 1-dimensional neutron kinetics have been included. The DYN3D code, developed in the Research Centre Rossendorf (RCR) for the improvement of the simulation of reactivity initiated accidents in nuclear reactors with hexagonal fuel elements comprises 3-dimensional neutron kinetics, models for the thermohydraulics of the core including heat transfer from the fuel to the coolant and a fuel rod behavior model.

     The reactor core model DYN3D was coupled with the ATHLET code on two basically different ways. The first way of coupling uses only the neutron kinetics part of the DYN3D code (internal coupling). This coupling along the core is very close and demands an high effort of programming due to the high number of coupling parameters.

     In the second way the whole core is cut out from the ATHLET plant model. The core is completly modeled by the DYN3D code (external coupling). In this case the interfaces are located at the bottom and at the top of the core. At this interfaces the pressures, mass flow rates, enthalpies and concentrations of boron acid have to be transferred. This way of coupling is easy to realize by interconnection of an interface routine. It is effectively supported by the General Control and Simulation Modul (GCSM) of the ATHLET code. Almost no changes of the single programs are necessary. Another advantage of this coupling is that the complete DYN3D model can be used.

     The disadvantage of this method is the splitting of the thermohydraulics. A closed implicit time integration of the whole system of thermohydraulic equations like in the ATHLET code would demand strong changes of the single programs o ...]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:230-3</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-230-3</dc:identifier>
<dc:title><![CDATA[Coupling of the Thermohydraulic Code ATHLET with the Neutron Kinetic Core Model DYN3D]]></dc:title>
<dc:source><![CDATA[Int. Conf. on Mathematics and Computations, Reactor Physics and Environmental Analysis, April 30. - May 5., 1995, Portland, Oregon, USA, Proc., Vol. 1, pp. 257 - 263]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[ The coupling of advanced thermohydraulic codes with 3-dimensional neutron kinetic codes corresponds to the effort to replace conservative estimations by best estimate calculations. ATHLET is an advanced thermohydraulic code, developed by the German Gesellschaft fr Anlagen- und Reaktorsicherheit (GRS). Up to now only point kinetics and 1-dimensional neutron kinetics have been included. The DYN3D code, developed in the Research Centre Rossendorf (RCR) for the improvement of the simulation of reactivity initiated accidents in nuclear reactors with hexagonal fuel elements comprises 3-dimensional neutron kinetics, models for the thermohydraulics of the core including heat transfer from the fuel to the coolant and a fuel rod behavior model.

     The reactor core model DYN3D was coupled with the ATHLET code on two basically different ways. The first way of coupling uses only the neutron kinetics part of the DYN3D code (internal coupling). This coupling along the core is very close and demands an high effort of programming due to the high number of coupling parameters.

     In the second way the whole core is cut out from the ATHLET plant model. The core is completly modeled by the DYN3D code (external coupling). In this case the interfaces are located at the bottom and at the top of the core. At this interfaces the pressures, mass flow rates, enthalpies and concentrations of boron acid have to be transferred. This way of coupling is easy to realize by interconnection of an interface routine. It is effectively supported by the General Control and Simulation Modul (GCSM) of the ATHLET code. Almost no changes of the single programs are necessary. Another advantage of this coupling is that the complete DYN3D model can be used.

     The disadvantage of this method is the splitting of the thermohydraulics. A closed implicit time integration of the whole system of thermohydraulic equations like in the ATHLET code would demand strong changes of the single programs o ...]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:591-2</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-591-2</dc:identifier>
<dc:title><![CDATA[Schwankungen des Massenstroms bei Druckentlastungsvorgängen]]></dc:title>
<dc:source><![CDATA[3. Fachtagung "Anlagen-, Arbeits- und Umweltsicherheit", Köthen, 7.-8.11.1996, Preprints, S. 233-240]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Bei der linearen Stabilitätsanalyse des Abblaseprozesses aus Druckbehältern mit zweiphasigem, aufwallendem Medium wurden Instabilitätsbereiche mit starken Massenstrompulsationen in der Abblaseleitung gefunden. Entscheidender Mechanismus ist die Rückkopplung zwischen Gemischspiegelschwankung, kritischer Ausströmrate und Druckabfallgeschwindigkeit. Für die Stabilitätsanalyse wurden analytische Modelle zur Beschreibung des bertragungsverhaltens aufgestellt. Es wurden Nyquist-Diagramme für verschiedene Parameterkombinationen untersucht und so die Instabilitätsbereiche identifiziert. Die Schwingneigung wird durch hohe Gasgehalte an der Entlastungsarmatur, eine große Verzögerungszeit (Länge der Abblaseleitung) und geringe Höhen der Schaumzone befördert.]]></dc:description>
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<identifier>HZDR:PUBLDB:591-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-591-1</dc:identifier>
<dc:title><![CDATA[Schwankungen des Massenstroms bei Druckentlastungsvorgängen]]></dc:title>
<dc:source><![CDATA[3. Fachtagung "Anlagen-, Arbeits- und Umweltsicherheit", Köthen, 7.-8.11.1996]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Bei der linearen Stabilitätsanalyse des Abblaseprozesses aus Druckbehältern mit zweiphasigem, aufwallendem Medium wurden Instabilitätsbereiche mit starken Massenstrompulsationen in der Abblaseleitung gefunden. Entscheidender Mechanismus ist die Rückkopplung zwischen Gemischspiegelschwankung, kritischer Ausströmrate und Druckabfallgeschwindigkeit. Für die Stabilitätsanalyse wurden analytische Modelle zur Beschreibung des bertragungsverhaltens aufgestellt. Es wurden Nyquist-Diagramme für verschiedene Parameterkombinationen untersucht und so die Instabilitätsbereiche identifiziert. Die Schwingneigung wird durch hohe Gasgehalte an der Entlastungsarmatur, eine große Verzögerungszeit (Länge der Abblaseleitung) und geringe Höhen der Schaumzone befördert.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2059-1</identifier>
<datestamp>2025-12-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Seifert, S.]]></dc:creator>
<dc:creator><![CDATA[Leibnitz, P.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2059-1</dc:identifier>
<dc:title><![CDATA[Nitridorhenium(V)-Komplexe mit Dimercaptobernsteinsäuredimethylester. Präparation, Charakterisierung und Kristallstruktur von [Re{NC(CH<SUB>3</SUB>)<SUB>2</SUB>PPhMe<SUB>2</SUB>}(DMSMe<SUB>2</SUB>)<SUB>2</SUB>]]]></dc:title>
<dc:source><![CDATA[Zeitschrift fuer anorganische und allgemeine Chemie 1999, 625, 1037-1040]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Die Reaktion von [ReNCl<SUB>2</SUB>(Me<SUB>2</SUB>PhP)<SUB>3</SUB>] 1 mit zwei Äquivalenten Dimercaptobernsteinsäuredimethylester (DMSMe<SUB>2</SUB>) in Aceton führt zur Bildung eines neutralen, diamagnetischen Rhenium(V)-DMSMe<SUB>2</SUB>-Komplexes unter Anlagerung einer Phenyldimethylphosphanisopropyl-Gruppierung am nukleophilen Nitrid-Stickstoff. Der entstehende Komplex 2 [Re{NC(CH<SUB>3</SUB>)<SUB>2</SUB>(Me<SUB>2</SUB>PhP)}(DMSMe<SUB>2</SUB>)<SUB>2</SUB>] kristallisiert triklin in der Raumgruppe P1, a = 12,334(7), b = 12,412(7), c = 12,414(8) Å; alpha = 60,14(3)°, beta = 67,98(3)°, gamma = 80,63(6)°; Z = 2. Das Rhenium befindet sich in einer quadratisch-pyramidalen Anordnung der Donoratome. Die beiden meso-DMSMe<SUB>2</SUB>-Liganden sind in syn-endo-Stellung angeordnet. Die Rhenium-Stickstoff-Bindung ist mit 1,697(12) Å nur wenig länger als in Nitridokomplexen und vergleichbar mit anderen Re-N-C-Bindungsabständen. Der Angriff des Lösungsmittels am Nitridostickstoffatom wird in Aceton (2) und Methylethylketon unter Bildung von 3 beobachtet. Massenspektrometrisch wird darüberhinaus nachgewiesen, daß auch eine Reaktion des Nitridostickstoffatoms mit dem Kondensationsprodukt des Methylethylketons erfolgt unter Bildung von [ReN{C(CH<SUB>3</SUB>)(C<SUB>2</SUB>H<SUB>5</SUB>)CH<SUB>2</SUB>C(O)C<SUB>2</SUB>H<SUB>5</SUB>(Me<SUB>2</SUB>PhP)}(DMSMe<SUB>2</SUB>)<SUB>2</SUB>]) 4. ]]></dc:description>
<dc:subject><![CDATA[Rhenium complexes]]></dc:subject>
<dc:subject><![CDATA[nitrido compounds]]></dc:subject>
<dc:subject><![CDATA[DMS complexes]]></dc:subject>
<dc:subject><![CDATA[X-ray diffraction]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2060-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Lucas, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2060-1</dc:identifier>
<dc:title><![CDATA[A new one-dimensional Particle-In-Cell model for multiphase vessel flow]]></dc:title>
<dc:source><![CDATA[Journal of Thermal Sciences 38 (1999) 758-768]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[A new one-dimensional Particle-In-Cell transport model for multiphase flow in a vessel is presented. The model aims at the consistent simulation of discontinuities as the top level of a multi-phase mixture. That makes it possible to include models for the transient behaviour of a foam layer on top of a mixture for example. The transport model, which is the basic component of a new computer code will be described. Flexible interfaces allow the implementation of models, constitutive laws or correlations for extra effects like phase transfer, generation and coalescence of bubbles or drops, foam behaviour, heat transfer, discharge from the vessel a.s.o. Due to these interfaces and a transparent code structure the code is a suitable basis for the development, test and validation of models. It allows the completion or the replacement of such models according to the specific application. 

]]></dc:description>
<dc:subject><![CDATA[transient simulation]]></dc:subject>
<dc:subject><![CDATA[multiphase flow particle method]]></dc:subject>
<dc:subject><![CDATA[numerical diffusion]]></dc:subject>
<dc:subject><![CDATA[chemical reactor depressurisation]]></dc:subject>
<dc:subject><![CDATA[foam discontinuity]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2061-1</identifier>
<datestamp>2025-12-02</datestamp>
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<dc:creator><![CDATA[Beuthien-Baumann, B.]]></dc:creator>
<dc:creator><![CDATA[Hamacher, K.]]></dc:creator>
<dc:creator><![CDATA[Oberdorfer, F.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2061-1</dc:identifier>
<dc:title><![CDATA[Preparation of Fluorine-18 labelled Sugars and Derivatives and their Application as Tracer for Positron-Emission-Tomography]]></dc:title>
<dc:source><![CDATA[Carbohydrate Research 327 (2000) 107-118]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The usefulness of <SUP>18</SUP>F-labelled carbohydrates, especially 2-deoxy-2-[<SUP>18</SUP>F]fluoro-D-glucose, to study pathophysiological processes in man non-invasively using positron-emission-tomography (PET) led to a widespread investigation of different <SUP>18</SUP>F-labelled sugars and sugar derivatives. In consideration of the short half-life of fluorine-18 (T<SUB>1/2</SUB>=110 min) synthetic strategies concerning precursor design, labelling conditions and deprotection of the intermediate compounds were developed to guarantee an efficient high radiochemical yield synthesis for diagnostic purposes. Besides some aspects of medical application of 2-deoxy-2-[<SUP>18</SUP>F]fluoro-D-glucose, a few synthetic strategies are described reflecting development work on promising <SUP>18</SUP>F-labelled sugars for diagnostic purposes during the last two decades]]></dc:description>
<dc:subject><![CDATA[Positron-emission-tomography]]></dc:subject>
<dc:subject><![CDATA[<SUP>18</SUP>F-Labelled carbohydrates]]></dc:subject>
<dc:subject><![CDATA[Medical application]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:384-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-384-1</dc:identifier>
<dc:title><![CDATA[Solar heat feeding into a district heating network]]></dc:title>
<dc:source><![CDATA[2. Deutsch-Italienische Konferenz über die Nutzung erneuerbare Energien, Brescia, Italien, 13.-16.6.1995, Tagungsband S. 241]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[After one year of operation the main results of the pilot system are summerized:
- mean collector efficiency 30%
- produced solar heat 30 MWh
- system losses 15%
The reasons for the deviations of the measured values from the projected values are discussed.
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:384-7</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-384-7</dc:identifier>
<dc:title><![CDATA[Solar heat feeding into a district heating network]]></dc:title>
<dc:source><![CDATA[2. Deutsch-Italienische Konferenz über die Nutzung erneuerbare Energien, Brescia, Italien, 13.-16.6.1995, Tagungsband S. 241]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[After one year of operation the main results of the pilot system are summerized:
- mean collector efficiency 30%
- produced solar heat 30 MWh
- system losses 15%
The reasons for the deviations of the measured values from the projected values are discussed.
]]></dc:description>
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<identifier>HZDR:PUBLDB:601-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Allen, P. G.]]></dc:creator>
<dc:creator><![CDATA[Bucher, J. J.]]></dc:creator>
<dc:creator><![CDATA[Clark, D. L.]]></dc:creator>
<dc:creator><![CDATA[Edelstein, N. M.]]></dc:creator>
<dc:creator><![CDATA[Ekberg, S. A.]]></dc:creator>
<dc:creator><![CDATA[Gohdes, J. W.]]></dc:creator>
<dc:creator><![CDATA[Hudson, E. A.]]></dc:creator>
<dc:creator><![CDATA[Kaltsoyannis, N.]]></dc:creator>
<dc:creator><![CDATA[Lukens, W. W.]]></dc:creator>
<dc:creator><![CDATA[Neu, M. P.]]></dc:creator>
<dc:creator><![CDATA[Palmer, P. D.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Shuh, D. K.]]></dc:creator>
<dc:creator><![CDATA[Tait, C. D.]]></dc:creator>
<dc:creator><![CDATA[Zwick, B. D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-610-1</dc:identifier>
<dc:title><![CDATA[Multinuclear NMR, Raman, EXAFS, and X-ray diffraction studies of uranyl carbonate complexes in near-neutral aqueous solution. X-ray structure of [C(NH2)3]6[(UO2)3(CO3)6].cntdot.6.5H2O]]></dc:title>
<dc:source><![CDATA[Inorganic Chemistry 34 (1995) pp 4797-4807]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:771-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Pham, T.]]></dc:creator>
<dc:creator><![CDATA[Zyganow, V.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Oswald, S.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-771-1</dc:identifier>
<dc:title><![CDATA[Corrosion Behavior and Microstructure of Titanium implanted with alpha and beta stabilizing elements]]></dc:title>
<dc:source><![CDATA[Thin Solid Films 310 (1997) 251-259]]></dc:source>
<dc:date>1997</dc:date>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-787-1</dc:identifier>
<dc:title><![CDATA[Advances in technetium chemistry towards 99m Tc receptor imaging agents]]></dc:title>
<dc:source><![CDATA[Transition Metal Chemistry, 22. 318-320 (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2928-1</identifier>
<datestamp>2025-12-03</datestamp>
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<dc:creator><![CDATA[Nock, B.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Tisato, F.]]></dc:creator>
<dc:creator><![CDATA[Maina, T.]]></dc:creator>
<dc:creator><![CDATA[Leibnitz, P.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Chiotellis, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2928-1</dc:identifier>
<dc:title><![CDATA[Oxorhenium mixed-ligand complexes with the 2,6-dimercaptomethylpyridine ligand. Crystal structure of [2,6-dimercaptomethylpyridinato][p-methoxybenzenethiolato]oxorhenium(V)]]></dc:title>
<dc:source><![CDATA[Inorg. Chim. Acta 304 (2000) 26-32]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Two novel oxorhenium complexes containing the 2,6-dithiomethylpyridine ligand were synthesized according to the '3 + 1' and the '3 + 2' approaches, respectively, and characterized by classical methods of analysis. The [2,6-dithiomethylpyridinato][p-methoxybenzenethiolato]oxorhenium complex, 1, was produced by simultaneous action of equimolar quantities of 2,6-dithiomethylpyridine and p-methoxybenzenethiol on the precursor [(n-C<SUB>4</SUB>H<SUB>9</SUB>)<SUB>4</SUB>N][ReOCl<SUB>4</SUB>] in EtOH. As revealed by spectroscopic data as well as X-ray structure analysis, complex 1 adopts a distorted square pyramidal geometry around the metal with the SNS/S donors forming the basal plane and the oxygen occupying the apex of the pyramid. When the same tridentate ligand reacts with [(n-C<SUB>4</SUB>H<SUB>9</SUB>)<SUB>4</SUB>N][ReOCl<SUB>3</SUB>(PO)] (PO = o-diphenylphosphinophenolato) as a precursor, complex 2a, [2,6-dithiomethylpyridinato][o-diphenylphosphinophenolato]oxorhenium, is obtained. The latter is a six-coordinate rhenium species to which the distorted octahedral geometry is assigned, according to the analytical findings. In this case, the SNS/P donors occupy the equatorial plane and the two oxygen atoms the apices of the distorted octahedron positioned trans to each other.]]></dc:description>
<dc:subject><![CDATA[Oxorhenium complexes]]></dc:subject>
<dc:subject><![CDATA[mixed ligand complexes]]></dc:subject>
<dc:subject><![CDATA[NMR spectroscopy]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<identifier>HZDR:PUBLDB:2283-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Smirnov, V. K.]]></dc:creator>
<dc:creator><![CDATA[Kibalov, D. S.]]></dc:creator>
<dc:creator><![CDATA[Krivlevich, S. A.]]></dc:creator>
<dc:creator><![CDATA[Lepshin, P. A.]]></dc:creator>
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<dc:creator><![CDATA[Ynakov, R. A.]]></dc:creator>
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<dc:title><![CDATA[Wave-ordered nanostructures formed on silicon-on-insulator wafers by means of reactive ion beams]]></dc:title>
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<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Soltani-Farshi, M.]]></dc:creator>
<dc:creator><![CDATA[Baumann, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Kreißig, U.]]></dc:creator>
<dc:creator><![CDATA[Bethge, K.]]></dc:creator>
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<dc:title><![CDATA[The behaviour of hydrogen in titanium after ion implantation]]></dc:title>
<dc:source><![CDATA[CAARI´98, Denton, USA, December 1998]]></dc:source>
<dc:date>1998</dc:date>
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<dc:creator><![CDATA[Strobel, M.]]></dc:creator>
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<dc:title><![CDATA[Computer simulation studies of the competition between nucleation and ion mixing in ion beam synthesis of nanoclusters]]></dc:title>
<dc:source><![CDATA[4th Int. Conf. on Computer Simulation of Radiation Effects in Solids, Okayama, Japan, 
Sept. 15-19, 1998]]></dc:source>
<dc:date>1998</dc:date>
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<dc:creator><![CDATA[Turos, A.]]></dc:creator>
<dc:creator><![CDATA[Gawlik, D.]]></dc:creator>
<dc:creator><![CDATA[Jagielski, J.]]></dc:creator>
<dc:creator><![CDATA[Stonert, A.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
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<dc:title><![CDATA[Ion Beam Mixing of the ZrO<SUB>2</SUB>/Fe System]]></dc:title>
<dc:source><![CDATA[11Int. Conf. on Ion Beam Modification of Materials, Amsterdam,The Netherlands,
Aug. 31 - Sept. 4, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Kachurin, G. A.]]></dc:creator>
<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2290-1</dc:identifier>
<dc:title><![CDATA[Room temperature visible photoluminescence from Ar<SUP>+</SUP>- and Ge<SUP>+</SUP>-implanted Si<SUB>3</SUB>N<SUB>4</SUB>- and SiO<SUB>x</SUB>N<SUB>y</SUB>-films]]></dc:title>
<dc:source><![CDATA[E-MRS´98, Strasbourg, June 16-19, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2291-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Kachurin, G. A.]]></dc:creator>
<dc:creator><![CDATA[Zhuravlev, K. S.]]></dc:creator>
<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2291-1</dc:identifier>
<dc:title><![CDATA[Effect of hydrostatic pressure annealing on visible photoluminescence from Si<SUP>+</SUP>- and Ge<SUP>+</SUP>-implanted SiO<SUB>2</SUB> films]]></dc:title>
<dc:source><![CDATA[11th Int. Conf. on Ion Beam Modification of Materials, Amsterdam, The Netherlands, 
Aug. 31 - Sept. 4, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Waidmann, S.]]></dc:creator>
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<dc:creator><![CDATA[Arnold, B.]]></dc:creator>
<dc:creator><![CDATA[Knupfer, M.]]></dc:creator>
<dc:creator><![CDATA[Leonhardt, A.]]></dc:creator>
<dc:creator><![CDATA[Fink, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2293-1</dc:identifier>
<dc:title><![CDATA[Electron energy-loss spectroscopy in transmission of undoped and doped diamond films]]></dc:title>
<dc:source><![CDATA[E-MRS'98, Strasbourg, France, June 16 - 19, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2295-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Walterfang, M.]]></dc:creator>
<dc:creator><![CDATA[Kruijer, S.]]></dc:creator>
<dc:creator><![CDATA[Keune, W.]]></dc:creator>
<dc:creator><![CDATA[Dobler, M.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2295-1</dc:identifier>
<dc:title><![CDATA[Tiefenselektive Phasenanalyse Si-ionenimplantierter "-Fe-Oberflächen mittels DCEMS]]></dc:title>
<dc:source><![CDATA[DPG-Frühjahrstagung, Regensburg, March 23-27,1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2296-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Koch, T.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Jentschel, M.]]></dc:creator>
<dc:creator><![CDATA[Börner, H. G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2296-1</dc:identifier>
<dc:title><![CDATA[Study of Interatomic Potentials in ZnS - Crystal-GRID Experiments versus ab initio Calculations]]></dc:title>
<dc:source><![CDATA[Applications of high-precision gamma-spectroscopy, Notre Dame, USA, July 1-3, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Crystal-GRID measurements have been performed with ZnS single crystals. For the first time, an asymmetric Crystal-GRID line shape could be observed. The preliminary data evaluation indicates that the reported lifetime of the 3221 keV level in 33 is too short. A value of about 60 fs has been found. Due to this ``long'' lifetime the line shape is much less structured than calculated with the reported lifetime.]]></dc:description>
<dc:subject><![CDATA[atomic collisions]]></dc:subject>
<dc:subject><![CDATA[Crystal-GRID]]></dc:subject>
<dc:subject><![CDATA[gamma ray spectroscopy]]></dc:subject>
<dc:subject><![CDATA[interatomic potentials]]></dc:subject>
<dc:subject><![CDATA[Molecular Dynamics simulations]]></dc:subject>
<dc:subject><![CDATA[nuclear lifetimes]]></dc:subject>
<dc:subject><![CDATA[ZnS]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<identifier>HZDR:PUBLDB:2296-2</identifier>
<datestamp>2025-04-16</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Koch, T.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Jentschel, M.]]></dc:creator>
<dc:creator><![CDATA[Börner, H. G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2296-2</dc:identifier>
<dc:title><![CDATA[Study of Interatomic Potentials in ZnS - Crystal-GRID Experiments versus ab initio Calculations]]></dc:title>
<dc:source><![CDATA[J. Res. Natl. Inst. Stand. Technol. 105 (2000) 81-87]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Crystal-GRID measurements have been performed with ZnS single crystals. For the first time, an asymmetric Crystal-GRID line shape could be observed. The preliminary data evaluation indicates that the reported lifetime of the 3221 keV level in 33 is too short. A value of about 60 fs has been found. Due to this ``long'' lifetime the line shape is much less structured than calculated with the reported lifetime.]]></dc:description>
<dc:subject><![CDATA[atomic collisions]]></dc:subject>
<dc:subject><![CDATA[Crystal-GRID]]></dc:subject>
<dc:subject><![CDATA[gamma ray spectroscopy]]></dc:subject>
<dc:subject><![CDATA[interatomic potentials]]></dc:subject>
<dc:subject><![CDATA[Molecular Dynamics simulations]]></dc:subject>
<dc:subject><![CDATA[nuclear lifetimes]]></dc:subject>
<dc:subject><![CDATA[ZnS]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.6028/jres.105.010]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2296-2</dc:relation>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:2297-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Wang, X.]]></dc:creator>
<dc:creator><![CDATA[Kolitsch, A.]]></dc:creator>
<dc:creator><![CDATA[Zhao, J. P.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2297-1</dc:identifier>
<dc:title><![CDATA[Similarity of energetic depositions of cubic boron nitride and titanium nitride thin films]]></dc:title>
<dc:source><![CDATA[MRS Fall Meeting 1998, Boston, USA, Nov. 30 - Dec.4, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<identifier>HZDR:PUBLDB:2298-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Wirth, H.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Gonzalez-Varona, O.]]></dc:creator>
<dc:creator><![CDATA[Perez-Rodriguez, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2298-1</dc:identifier>
<dc:title><![CDATA[Ion-implantation induced damage In 6H-SiC: the influence of substrate temperature]]></dc:title>
<dc:source><![CDATA[40th Electronic Materials Conference (EMC'98), Charlottesville, Virginia, USA, June 24-26, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:2299-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Zappe, S.]]></dc:creator>
<dc:creator><![CDATA[Obermeier, E.]]></dc:creator>
<dc:creator><![CDATA[Stoemenos, J.]]></dc:creator>
<dc:creator><![CDATA[Möller, H.]]></dc:creator>
<dc:creator><![CDATA[Krötz, G.]]></dc:creator>
<dc:creator><![CDATA[Wirth, H.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2299-1</dc:identifier>
<dc:title><![CDATA[Stabilisation of the 3C-SiC/SOI system by an intermediate Si<SUB>3</SUB>N<SUB>4</SUB> layer]]></dc:title>
<dc:source><![CDATA[ECSCRM '98 (2nd European Conf. on Silicon Carbide and Related Materials), Montpellier, Sept. 2 - 4, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:2300-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Zuhr, R. A.]]></dc:creator>
<dc:creator><![CDATA[Budai, J. D.]]></dc:creator>
<dc:creator><![CDATA[Datskos, P. G.]]></dc:creator>
<dc:creator><![CDATA[Meldrum, A.]]></dc:creator>
<dc:creator><![CDATA[Thomas, K. A.]]></dc:creator>
<dc:creator><![CDATA[Warmack, R. J.]]></dc:creator>
<dc:creator><![CDATA[White, C. W.]]></dc:creator>
<dc:creator><![CDATA[Feldman, L. C.]]></dc:creator>
<dc:creator><![CDATA[Strobel, M.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2300-1</dc:identifier>
<dc:title><![CDATA[Nanostructured arrays formed by finely focused ion beams]]></dc:title>
<dc:source><![CDATA[MRS Fall Meeting, Boston, USA, Nov. 30 - Dec. 4, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:type>Text</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:2286-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Stölzel, M.]]></dc:creator>
<dc:creator><![CDATA[Born, R.]]></dc:creator>
<dc:creator><![CDATA[Scharnweber, D.]]></dc:creator>
<dc:creator><![CDATA[Worch, H.]]></dc:creator>
<dc:creator><![CDATA[Pham, M. T.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2286-1</dc:identifier>
<dc:title><![CDATA[In vitro Charakterisierung modifizierter ionenimplantierter Titanoberflächen]]></dc:title>
<dc:source><![CDATA[Werkstoffwoche,  München, Germany, Oct. 12-15, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
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<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2286-1</dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:2189-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Spaeth, C.]]></dc:creator>
<dc:creator><![CDATA[Richter, F.]]></dc:creator>
<dc:creator><![CDATA[Grigull, S.]]></dc:creator>
<dc:creator><![CDATA[Kreißig, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2189-1</dc:identifier>
<dc:title><![CDATA[Conversion algorithm for ERDA multielement spectra and its application to thin-film problems]]></dc:title>
<dc:source><![CDATA[Nucl. Instr. Meth. B140 (1998) 243]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[A computer program was designed for the conversion of element-resolved energy spectra obtained from elastic recoil
detection analysis into composition depth profles. The algorithm is described in detail. An important feature of the
program is that the contribution of the analyzed elements to the stopping power is accounted for self-consistently. Extensions of the algorithm address the problem of the simultaneous analysis of recoil and forward scattering events, respectively, and of distortions in the recoil spectra due to the presence of target constituents with isotopic distributions that cannot be resolved when using standard ionization chambers for recoil detection. Two examples are given to demonstrate how one may benefit from the capabilities of the conversion program in the context of specifc thin film problems. The first example addresses compositional changes in Si3N4/C bilayers due to N-ion implantation, while the second one is dealing with the problem of impurity accumulation at the hexagonal-to-cubic phase boundary in BN films.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2189-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<header>
<identifier>HZDR:PUBLDB:2022-1</identifier>
<datestamp>2026-01-15</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Scheunemann, M.]]></dc:creator>
<dc:creator><![CDATA[Kretzschmar, M.]]></dc:creator>
<dc:creator><![CDATA[Elz, S.]]></dc:creator>
<dc:creator><![CDATA[Pertz, H. H.]]></dc:creator>
<dc:creator><![CDATA[Seifert, S.]]></dc:creator>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Syhre, R.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2022-1</dc:identifier>
<dc:title><![CDATA[Synthesis and Autoradiographic Evaluation of a Novel High-Affinity Tc-99m Ligand for the 5-HT<SUB>2A</SUB> Receptor]]></dc:title>
<dc:source><![CDATA[13. Intern. Symposium on Radiopharmaceutical Chemistry, Saint Louis, USA 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The successful development of [<SUP>99m</SUP>Tc]TRODAT as ligand for the dopamine transporter has shown the feasibility to image specific transporters in the brain with radiotracers based on Tc-99m (1). In contrast to this achievement and despite the efforts many groups have devoted so far, the search for Tc-99m complexes with affinity to post-synaptic CNS receptors have not yet reached the same stage of development (2). As one of the consequences for the design of serotonin-5-HT<SUB>2A</SUB> receptor binding Tc-99m complexes an affinity of < 1nM is believed to be a prerequisite for further progress. Aiming at such a high affinity, we have pursued our design concept starting from ketanserin as lead structure for 5-HT<SUB>2A</SUB> receptor binding ligands (3, 4).
Here we report on the synthesis of a new high-affinity Tc-99m ligand that meets the requirement of picomolar affinity. The complex is evaluated in various receptor binding assays and by in vitro autoradiography.
]]></dc:description>
<dc:subject><![CDATA[Serotonin-5-HT<SUB>2A</SUB> receptor]]></dc:subject>
<dc:subject><![CDATA[Tc-99m receptor ligand]]></dc:subject>
<dc:subject><![CDATA[ketanserin analogue]]></dc:subject>
<dc:subject><![CDATA[ligand synthesis]]></dc:subject>
<dc:subject><![CDATA[in vitro autoradiography]]></dc:subject>
<dc:subject><![CDATA[receptor binding assay]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2022-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2022-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Scheunemann, M.]]></dc:creator>
<dc:creator><![CDATA[Kretzschmar, M.]]></dc:creator>
<dc:creator><![CDATA[Elz, S.]]></dc:creator>
<dc:creator><![CDATA[Pertz, H. H.]]></dc:creator>
<dc:creator><![CDATA[Seifert, S.]]></dc:creator>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Syhre, R.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2022-2</dc:identifier>
<dc:title><![CDATA[Synthesis and Autoradiographic Evaluation of a Novel High-Affinity Tc-99m Ligand for the 5-HT<SUB>2A</SUB> Receptor]]></dc:title>
<dc:source><![CDATA[J. Labelled Cpd. Radiopharm. 42 (1999) S345-S347]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The successful development of [<SUP>99m</SUP>Tc]TRODAT as ligand for the dopamine transporter has shown the feasibility to image specific transporters in the brain with radiotracers based on Tc-99m (1). In contrast to this achievement and despite the efforts many groups have devoted so far, the search for Tc-99m complexes with affinity to post-synaptic CNS receptors have not yet reached the same stage of development (2). As one of the consequences for the design of serotonin-5-HT<SUB>2A</SUB> receptor binding Tc-99m complexes an affinity of < 1nM is believed to be a prerequisite for further progress. Aiming at such a high affinity, we have pursued our design concept starting from ketanserin as lead structure for 5-HT<SUB>2A</SUB> receptor binding ligands (3, 4).
Here we report on the synthesis of a new high-affinity Tc-99m ligand that meets the requirement of picomolar affinity. The complex is evaluated in various receptor binding assays and by in vitro autoradiography.
]]></dc:description>
<dc:subject><![CDATA[Serotonin-5-HT<SUB>2A</SUB> receptor]]></dc:subject>
<dc:subject><![CDATA[Tc-99m receptor ligand]]></dc:subject>
<dc:subject><![CDATA[ketanserin analogue]]></dc:subject>
<dc:subject><![CDATA[ligand synthesis]]></dc:subject>
<dc:subject><![CDATA[in vitro autoradiography]]></dc:subject>
<dc:subject><![CDATA[receptor binding assay]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2022-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:3069-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-3069-1</dc:identifier>
<dc:title><![CDATA[Lumineszenzeigenschaften ionenimplantierter nanokristalliner SiO<SUB>2</SUB>-Schichten]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-279]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/doctoralThesis</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-3069-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1132-1</identifier>
<datestamp>2023-05-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1132-1</dc:identifier>
<dc:title><![CDATA[Pre- and Posttest Calculations to Natural Circulation Experiments at the Integral Test Facility ISB-VVER Using the Thermalhydraulic Code ATHLET]]></dc:title>
<dc:source><![CDATA[Nuclear Engineering and Design 190(1999)341-346]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[In 1995 at the integral test facility ISB-VVER in Elektrogorsk near Moscow natural circulation experiments were performed, which were scientifically accompanied by the Forschungszentrum Rossendorf. These experiments were the first of this kind at a test facility, which models VVER-1000 thermalhydraulics. Using the code ATHLET which is being developed by "Gesellschaft für Anlagen- und Reaktorsicherheit", pre- and posttest calculations were done to determine the thermalhydraulic events to be expected and to define and tune the boundary conditions of the test. The conditions found for natural circulation instabilities and cold leg loop seal clearing could be confirmed by the tests. Besides the thermalhydraulic standard measuring system, the facility was equipped with needle shaped conductivity probes for measuring the local void fractions.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0029-5493(99)00083-7]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1132-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1280-1</identifier>
<datestamp>2023-05-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1280-1</dc:identifier>
<dc:title><![CDATA[Natural circulation experiments at the ISB-VVER integral test facility and calculations using the thermal-hydraulic code ATHLET]]></dc:title>
<dc:source><![CDATA[Nuclear Technology 128(October 1999) No. 1, pp. 75-86]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[In 1995 at the integral test facility ISB-VVER in Elektrogorsk near Moscow, natural circulation experiments were performed, that were scientifically supported by the Forschungszentrum Rossendorf. These experiments were the first of this kind at a test facility, that models VVER-1000 thermal-hydraulics. Using the code ATHLET, which is being developed by Gesellschaft für Anlagen- und Reaktorsicherheit, pre- and posttest calculations were done to determine the thermal-hydraulic events to be expected and to define and tune the boundary conditions of the test. The conditions found for natural circulation instabilities and cold-leg loop-seal clearing could be confirmed by the tests. In the paper, the experimental results are presented, analysed and compared with ATHLET calculations. The main thermal-hydraulic phenomena were identified and compared with the results gained during similar experiments on VVER-440 test facilities. Besides the thermal-hydraulic standard measurin!
g system, the facility was equipped with needle-shaped conductivity probes for measuring the local void fractions.


]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.13182/NT99-A3015]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1280-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:3103-1</identifier>
<datestamp>2025-12-09</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Andronenko, M.]]></dc:creator>
<dc:creator><![CDATA[Andronenko, L.]]></dc:creator>
<dc:creator><![CDATA[Neubert, W.]]></dc:creator>
<dc:creator><![CDATA[Seliverstov, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3103-1</dc:identifier>
<dc:title><![CDATA[Pecularities of isotopic temperatures obtained from p + A collisions at 1 GeV]]></dc:title>
<dc:source><![CDATA[Eur. Phys. J. A, Vol. 8, Nr. 1, pp.9-13]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The nuclear temperatures obtained from inclusive measurements of double isotopic yield ratios of fragments produced in 1 GeV p+A collisions amount to about 4 MeV nearly independent from the target mass.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1007/s10050-000-4501-2]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-3103-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:14193-2</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Eichler, S.]]></dc:creator>
<dc:creator><![CDATA[Fahmy, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14193-2</dc:identifier>
<dc:title><![CDATA[Water repartitioning at the water lipid protein interface controls receptor activation in G-Protein coupled receptors]]></dc:title>
<dc:source><![CDATA[Annual Meeting of the German Biophysical Society, 03.-06.10.2010, Bochum, Deutschland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[G-Protein coupled receptors (GPCRs) play a fundamental role in many physiological processes. High ligand specifity of rhodopsin-like GPCRs in contrast to the highly conserved and class defining D(E)RY motif undergoing a protonation upon receptor activation suggests a general local activation mechanism acting as an autonomous functional module.  
It has been shown that the D(E)RY motif positioned at the phase boundary acts as a pH-dependent switch which is governed by side chain partitioning between the aqueous and lipidic phase [1].
Here we have addressed the putative reverse effect, i.e. restructuring of the water lipid interface upon side chain protonation to elucidate the functional implication of water lipid protein interactions in the control of protein conformation. We have studied a TM3 derived transmembrane segment where a fluorescence reporter resides below the D(E)RY motif inside the helix. By fluorescence spectroscopy, FRET studies and FTIR-Fluorescence cross correlation experiments we show the pH dependent hydration site N-terminally of the D(E)RY motif. Thus the ionized D(E) side chain attracts water that dissolves the TM-sequence even beyond the two preceding hydrophobic residues. 
These results argue for a key role of the rearrangement of the water lipid protein microstructure upon GPCR activation as it effects not only the phase boundary but even  more hydrophobic environment inside the lipidic phase. 
[1] S. Madathil, K.Fahmy, J Biol Chem 284, 28801-28809 (2009)]]></dc:description>
<dc:subject><![CDATA[membrane transport]]></dc:subject>
<dc:subject><![CDATA[protonation]]></dc:subject>
<dc:subject><![CDATA[FTIR spectroscopy]]></dc:subject>
<dc:subject><![CDATA[fluorescence spectroscopy]]></dc:subject>
<dc:subject><![CDATA[FRET]]></dc:subject>
<dc:subject><![CDATA[charge stabilization]]></dc:subject>
<dc:subject><![CDATA[bilayer]]></dc:subject>
<dc:subject><![CDATA[water reorganization]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14193-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2097-1</identifier>
<datestamp>2025-12-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Jungclaus, A.]]></dc:creator>
<dc:creator><![CDATA[Kast, D.]]></dc:creator>
<dc:creator><![CDATA[Lieb, K. P.]]></dc:creator>
<dc:creator><![CDATA[Teich, C.]]></dc:creator>
<dc:creator><![CDATA[Weiszflog, M.]]></dc:creator>
<dc:creator><![CDATA[Härtlein, T.]]></dc:creator>
<dc:creator><![CDATA[Ender, C.]]></dc:creator>
<dc:creator><![CDATA[Köck, F.]]></dc:creator>
<dc:creator><![CDATA[Schwalm, D.]]></dc:creator>
<dc:creator><![CDATA[Johnstone, I. P.]]></dc:creator>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Peusquens, R.]]></dc:creator>
<dc:creator><![CDATA[Dewald, A.]]></dc:creator>
<dc:creator><![CDATA[Eberth, J.]]></dc:creator>
<dc:creator><![CDATA[Thomas, H. G.]]></dc:creator>
<dc:creator><![CDATA[Gorska, M.]]></dc:creator>
<dc:creator><![CDATA[Grawe, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2097-1</dc:identifier>
<dc:title><![CDATA[Lifetime study of particle-hole excitations in the semimagic nucleus <SUP>94</SUP>Ru]]></dc:title>
<dc:source><![CDATA[Physical Review C, Volume 60, 014309]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevC.60.014309]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2097-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:870-1</identifier>
<datestamp>2022-11-11</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brandolini, F.]]></dc:creator>
<dc:creator><![CDATA[Ionescu-Bujor, M.]]></dc:creator>
<dc:creator><![CDATA[Medina, N. H.]]></dc:creator>
<dc:creator><![CDATA[Ribas, R. V.]]></dc:creator>
<dc:creator><![CDATA[Bazzacco, D.]]></dc:creator>
<dc:creator><![CDATA[Poli, M.]]></dc:creator>
<dc:creator><![CDATA[Pavan, P.]]></dc:creator>
<dc:creator><![CDATA[Alvarez, C. R.]]></dc:creator>
<dc:creator><![CDATA[Angelis, G.]]></dc:creator>
<dc:creator><![CDATA[Lunardi, S.]]></dc:creator>
<dc:creator><![CDATA[Acuna, D.]]></dc:creator>
<dc:creator><![CDATA[Napoli, D. R.]]></dc:creator>
<dc:creator><![CDATA[Frauendorf, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-870-1</dc:identifier>
<dc:title><![CDATA[Lifetimes of a shears band in<SUP>139</SUP>Sm]]></dc:title>
<dc:source><![CDATA[Physics Letters B 388 (1996) pp. 468-474]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0370-2693(96)01202-6]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-870-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1731-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:title><![CDATA[Application of the ECR slot antenna plasma source for ion implantation]]></dc:title>
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<dc:title><![CDATA[Doping of 3C-SiC by implantation of nitrogen at high temperatures]]></dc:title>
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<dc:title><![CDATA[Defects in detwinned LaGaO<SUB>3</SUB> substrates]]></dc:title>
<dc:source><![CDATA[Acta Physica Polonica A92 (1997) 205]]></dc:source>
<dc:date>1997</dc:date>
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<dc:title><![CDATA[Sensitization of silicon nitride surfaces for Ag<SUP>+</SUP> ions by ion implantation]]></dc:title>
<dc:source><![CDATA[Sensors and Actuators B43 (1997) 110]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
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<dc:title><![CDATA[Verifikation des ATHLET-Rechenprogramms im Rahmen der externen Verifikationsgruppe ATHLET BETHSY Test 5.2c- Totalverlust des Speisewassers]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-231 August 1998]]></dc:source>
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<dc:description><![CDATA[Im Rahmen der externen Validierung des von der Gesellschaft für Anlagen- und Reaktorsicherheit entwickelten Störfallcodes ATHLET, der in der Version Mod 1.1 Cycle D vorlag, wurden zwei Experimente nachgerechnet und anlaysiert, die an der französischen Versuchsanlage BETHSY durchgeführt wurden.
Das Experiment 5.2c dient der Untersuchung der Notfallprozeduren beim Totalausfall der Speisewasserversorgung auf der Dampferzeugersekundärseite. Spezielles Interesse gilt hierbei den Möglichkeiten der Notkühlung durch primäres Bleed and Feed, dem Verhalten der Dampferzeuger bei sekundärseitiger Austrocknung und dem Langzeitverhalten der Anlage bis zum Einspeisen der einzelnen Notkühlsysteme. Im Verlauf der Transiente erfolgt die Einspeisung sowohl aus dem Hochdrucknotkühlsystem als auch aus den Druckspeichern und dem Niederdrucknotkühlsystem.
Die Auswertung der Rechnungen zeigt, daß praktisch alle wesentlichen Phänome im Verlauf der Transiente korrekt wiedergegeben werden. Als ein wesentlicher Einflußfaktor auf die Qualität der Rechnungen hat sich die Modellierung der Wärmeverluste, welche an der Versuchsanlage teilweise durch eine Zusatzheizung (Trace Heating) kompensiert werden, herausgestellt. Werden die Wärmeverluste im Primärkreis falsch berechnet, so ergeben sich signifikante Abweichungen im Verlauf des Primärdrucks. Da alle Prozesse im weiteren druckgesteuert erfolgen, wirken sich Abweichungen im Primärdruck besonders stark auf den Verlauf der Transiente aus.
Die Ergebnisse der Rechnungen zeigen darüberhinaus, daß die sicherheitsrelevante Aussage des Experiments durch den Code ATHLET reproduziert wird.
]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:title><![CDATA[Finite Volume and Finite Element Code Calculations to an IAHR-Benchmark Test]]></dc:title>
<dc:source><![CDATA[7th International Conference on Nuclear Engineering (ICONE-7), Tokyo April 1999 
Conference CD, ICONE-7072]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[New reactor designs comprise passive elements for decay heat removal. Computational-Fluid-Dynamics codes are an appropriate tool for the assessment of the efficiency of those components. Most of these codes are based either on the Finite-Volume or the Finite-Element method. Because of the importance for reactor safety these numerical tools have to be thoroughly validated using results from experimental setups.
The governing mechanism in passive components for decay heat removal is natural convection and heat transfer with internal heating. To assess the capability describing mixed convection flow, post test calculations of an IAHR benchmark exercise were performed (Kamide et. al, 1991). The commercial codes CFX-4® and ANSYS/FLOTRAN® were used, representing the Finite-Volume Method and the Finite-Element Method respectively.
This paper presents a discussion of the problems and capabilities of each code to calculate complex flow regimes and temperature fields.
]]></dc:description>
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<dc:identifier>https://www.hzdr.de/publications/Publ-1374-7</dc:identifier>
<dc:title><![CDATA[Finite Volume and Finite Element Code Calculations to an IAHR-Benchmark Test]]></dc:title>
<dc:source><![CDATA[7th International Conference on Nuclear Engineering (ICONE-7), Tokyo April 1999 
Conference CD, ICONE-7072]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[New reactor designs comprise passive elements for decay heat removal. Computational-Fluid-Dynamics codes are an appropriate tool for the assessment of the efficiency of those components. Most of these codes are based either on the Finite-Volume or the Finite-Element method. Because of the importance for reactor safety these numerical tools have to be thoroughly validated using results from experimental setups.
The governing mechanism in passive components for decay heat removal is natural convection and heat transfer with internal heating. To assess the capability describing mixed convection flow, post test calculations of an IAHR benchmark exercise were performed (Kamide et. al, 1991). The commercial codes CFX-4® and ANSYS/FLOTRAN® were used, representing the Finite-Volume Method and the Finite-Element Method respectively.
This paper presents a discussion of the problems and capabilities of each code to calculate complex flow regimes and temperature fields.
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Schäfer, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1386-3</dc:identifier>
<dc:title><![CDATA[Post-Test Analysis of the Experiment 5.2c- Total Loss of Feedwater at the BETHSY Test Facility]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik '99, Tagungsbericht S. 99-102, Karlsruhe, 18.-20. Mai 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[In the framework of the external validation of the thermohydraulic code ATHLET Mod 1.1 Cycle D, which has been developed by the GRS, post test analyses of two experiments were done, which were performed at the french integral test facility BETHSY.
The BETHSY experiment 5.2c investigates the accident procedures in case of a total loss of feedwater at the steam generator secondary side, [3]. In such an accident the emergency cooling of the reactor core with primary bleed and feed, the behaviour of the steam generators in case of dry out and the long time behaviour of the test facility are special subjects of interest. During the experiment the high pressure injection system, the hydroaccumulators and the low pressure injection system were available.
The evaluation of the calculated results shows, that all main phenomena can be calculated in a good quality compared with the experiment. Resulting from various calculations it should be noticed that the quality of the results strongly depends on the modelling of the heat losses of the facility, which were partly compensated by the trace heating. This trace heating was changed several times in the experiment to compensate the changing heat losses. The exact modelling of the resulting heat losses has a strong influence on the course of the whole transient. In this test the unsufficient modelling of the resulting heat losses may be the reason for deviations of the calculated transient from the observed transient.
The results show, that the safety relevant statement of the experiment could be reproduced by the code ATHLET.
]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Schäfer, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1386-7</dc:identifier>
<dc:title><![CDATA[Post-Test Analysis of the Experiment 5.2c- Total Loss of Feedwater at the BETHSY Test Facility]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik '99, Tagungsbericht S. 99-102, Karlsruhe, 18.-20. Mai 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[In the framework of the external validation of the thermohydraulic code ATHLET Mod 1.1 Cycle D, which has been developed by the GRS, post test analyses of two experiments were done, which were performed at the french integral test facility BETHSY.
The BETHSY experiment 5.2c investigates the accident procedures in case of a total loss of feedwater at the steam generator secondary side, [3]. In such an accident the emergency cooling of the reactor core with primary bleed and feed, the behaviour of the steam generators in case of dry out and the long time behaviour of the test facility are special subjects of interest. During the experiment the high pressure injection system, the hydroaccumulators and the low pressure injection system were available.
The evaluation of the calculated results shows, that all main phenomena can be calculated in a good quality compared with the experiment. Resulting from various calculations it should be noticed that the quality of the results strongly depends on the modelling of the heat losses of the facility, which were partly compensated by the trace heating. This trace heating was changed several times in the experiment to compensate the changing heat losses. The exact modelling of the resulting heat losses has a strong influence on the course of the whole transient. In this test the unsufficient modelling of the resulting heat losses may be the reason for deviations of the calculated transient from the observed transient.
The results show, that the safety relevant statement of the experiment could be reproduced by the code ATHLET.
]]></dc:description>
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<identifier>HZDR:PUBLDB:1918-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
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<dc:title><![CDATA[Nachrechnung eines Abblase-Experimentes mit den thermohydraulischen Störfallprogrammen ATHLET und RELAP]]></dc:title>
<dc:source><![CDATA[1. ATHLET-Anwenderseminar, GRS Garching, Mai 1992]]></dc:source>
<dc:date>1992</dc:date>
<dc:description><![CDATA[Der Bericht beschreibt Nachrechnungen eines Abblaseexperiments, das vor etwa 10 Jahren am Moskauer Energetischen Institut durchgef|hrt wurde und für das experimentelle Daten des zeitlichen Verlaufes der Druckentlastung im
Abblasebehälter und des Dampfgehaltes in verschiedenen Gefäßhöhen vorliegen.
Es wurden die Programme RELAP5/mod2 und ATHLET 1.0 Version E eingesetzt. Wie es sich zeigt, hat die richtige Beschreibung der Zweiphasenströmung an der
Ausströmöffnung den größten Einfluß auf die Genauigkeit der Nachrechnung.
Hierfür bietet das stationdre 1D-FD-Modell für kritisches Ausströmen des
Programms ATHLET die bessere Anpassungsfähigkeit an die gegebenen
Versuchsbedingungen.
]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1603-1</dc:identifier>
<dc:title><![CDATA[Solarenergie - Photovoltaik]]></dc:title>
<dc:source><![CDATA[Tagung der Evangelischen Akademie Meißen, 12. - 14. Juni 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Anhand ausgewählter Ergebnisse wird der aktuelle Stand der Nutzung der Photovoltaik vorgestellt. Trotz einer Reihe bemerkenswerter technischer Fortschritte bei den Hauptkomponenten und einer Vielzahl errichteter Demonstrationsanlagen liegen die Kosten von Solarstrom noch einen Faktor 10 zu hoch. Deshalb besteht nach wie vor ein erheblicher Forschungsbedarf, um diese Technologie zur Marktreife zu bringen.]]></dc:description>
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<dc:creator><![CDATA[Jenkins, D. G.]]></dc:creator>
<dc:creator><![CDATA[Juutinen, S.]]></dc:creator>
<dc:creator><![CDATA[Kelsall, N.]]></dc:creator>
<dc:creator><![CDATA[Krücken, R.]]></dc:creator>
<dc:creator><![CDATA[Lane, G. J.]]></dc:creator>
<dc:creator><![CDATA[Lee, I. Y.]]></dc:creator>
<dc:creator><![CDATA[Macchiavelli, A. O.]]></dc:creator>
<dc:creator><![CDATA[Macleod, R. W.]]></dc:creator>
<dc:creator><![CDATA[Schmid, G.]]></dc:creator>
<dc:creator><![CDATA[Sears, J. M.]]></dc:creator>
<dc:creator><![CDATA[Smith, J. F.]]></dc:creator>
<dc:creator><![CDATA[Stephens, F. S.]]></dc:creator>
<dc:creator><![CDATA[Vetter, K.]]></dc:creator>
<dc:creator><![CDATA[Wadsworth, R.]]></dc:creator>
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<dc:identifier>https://www.hzdr.de/publications/Publ-2344-1</dc:identifier>
<dc:title><![CDATA[Shears Mechanism in the A ~ 110 Region]]></dc:title>
<dc:source><![CDATA[Physical Review Letters, Volume 82, Number 16, 19 April 1999, 3220-3223]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Jenkins, D. G.]]></dc:creator>
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<dc:creator><![CDATA[Cameron, J.]]></dc:creator>
<dc:creator><![CDATA[Clark, R. M.]]></dc:creator>
<dc:creator><![CDATA[Fossan, D. B.]]></dc:creator>
<dc:creator><![CDATA[Hibbert, I. M.]]></dc:creator>
<dc:creator><![CDATA[Janzen, V. P.]]></dc:creator>
<dc:creator><![CDATA[Krücken, R.]]></dc:creator>
<dc:creator><![CDATA[Lane, G. J.]]></dc:creator>
<dc:creator><![CDATA[Lee, I. Y.]]></dc:creator>
<dc:creator><![CDATA[Macchiavelli, A. O.]]></dc:creator>
<dc:creator><![CDATA[Parry, C. M.]]></dc:creator>
<dc:creator><![CDATA[Sears, J. M.]]></dc:creator>
<dc:creator><![CDATA[Smith, J. F.]]></dc:creator>
<dc:creator><![CDATA[Frauendorf, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2359-1</dc:identifier>
<dc:title><![CDATA[Magnetic rotational bands in <SUP>108</SUP>Sb]]></dc:title>
<dc:source><![CDATA[Physical Review C, Volume 58, Number 5, November 1998, 2703-2709]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<identifier>HZDR:PUBLDB:442-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:identifier>https://www.hzdr.de/publications/Publ-442-7</dc:identifier>
<dc:title><![CDATA[Stand und Wirtschaftlichkeit von Sonnen- und Windenergienutzung zur Stromerzeugung in Sachsen]]></dc:title>
<dc:source><![CDATA[XXVII Kraftwerkstechnisches Kolloquium der TU Dresden, 24./25.10.1995, Tagungsband Teil I, S. 45]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[In den letzten Jahren war in Sachsen eine dynamische Entwicklung bei der Nutzung der Wind- und Sonnenenergie zu Erzeugung von Elektroenergie zu verzeichnen. Derzeit sind in Sachsen etwa Windenergieanlagen mit einer Leistung von insgesamt 20 MW und netzgekoppelte Photovoltaikanlagen mit einer Leistung von knapp 600 kW in Betrieb. Die Windenergienutzung befindet sich derzeit an der Schwelle zur Wirtschaftlichkeit (Stromgestehungskosten etwa 17 Pf/kWh), bis zum Jahr 2000 kann mit einer installierten Leistung bis zu 200 MW gerechnet werden. Demgegenüber ist Strom aus Photovoltaikanlagen noch um den Faktor 10 zu teuer.]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-442-1</dc:identifier>
<dc:title><![CDATA[Stand und Wirtschaftlichkeit von Sonnen- und Windenergienutzung zur Stromerzeugung in Sachsen]]></dc:title>
<dc:source><![CDATA[XXVII Kraftwerkstechnisches Kolloquium der TU Dresden, 24./25.10.1995, Tagungsband Teil I, S. 45]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[In den letzten Jahren war in Sachsen eine dynamische Entwicklung bei der Nutzung der Wind- und Sonnenenergie zu Erzeugung von Elektroenergie zu verzeichnen. Derzeit sind in Sachsen etwa Windenergieanlagen mit einer Leistung von insgesamt 20 MW und netzgekoppelte Photovoltaikanlagen mit einer Leistung von knapp 600 kW in Betrieb. Die Windenergienutzung befindet sich derzeit an der Schwelle zur Wirtschaftlichkeit (Stromgestehungskosten etwa 17 Pf/kWh), bis zum Jahr 2000 kann mit einer installierten Leistung bis zu 200 MW gerechnet werden. Demgegenüber ist Strom aus Photovoltaikanlagen noch um den Faktor 10 zu teuer.]]></dc:description>
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<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Tameshige, Y.]]></dc:creator>
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<dc:creator><![CDATA[Shimbara, Y.]]></dc:creator>
<dc:creator><![CDATA[Fujita, H.]]></dc:creator>
<dc:creator><![CDATA[Wakasa, T.]]></dc:creator>
<dc:creator><![CDATA[Brown, B. A.]]></dc:creator>
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<dc:title><![CDATA[High-precision ( p,t) reaction to determine 25Al( p,γ )26Si reaction rates]]></dc:title>
<dc:source><![CDATA[Physical Review C 82(2010), 025807-01-025807-12]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Since the identification of ongoing 26Al production in the universe, the reaction sequence 24Mg(p,γ )25Al(β+ν)25Mg(p,γ )26Al has been studied intensively. At temperatures where the radiative capture on 25Al (t1/2 = 7.2 s) becomes faster than the β+ decay, the production of 26Al can be reduced due to the depletion of 25Al. To determine the resonances relevant for the 25Al(p,γ )26Si bypass reaction, we measured the 28Si(p,t )26Si reaction with high-energy precision using the Grand Raiden spectrometer at the Research Center for Nuclear Physics, Osaka. Several new energy levels were found above the p threshold and for known states excitation energies were determined with smaller uncertainties. The calculated stellar rates of the bypass reaction agree well with previous results, suggesting that these rates are well established.]]></dc:description>
<dc:subject><![CDATA[26Al 24Mg(p]]></dc:subject>
<dc:subject><![CDATA[γ )25Al(β+ν)25Mg(p]]></dc:subject>
<dc:subject><![CDATA[γ )26Al Grand Raiden spectrometer]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:14457-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:creator><![CDATA[Enghardt, W.]]></dc:creator>
<dc:creator><![CDATA[Golnik, C.]]></dc:creator>
<dc:creator><![CDATA[Kormoll, T.]]></dc:creator>
<dc:creator><![CDATA[Wüstemann, J.]]></dc:creator>
<dc:creator><![CDATA[Fiedler, F.]]></dc:creator>
<dc:creator><![CDATA[Müller, A.]]></dc:creator>
<dc:creator><![CDATA[Schöne, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14457-1</dc:identifier>
<dc:title><![CDATA[A Compton Imager for in-vivo Dosimetry of Proton Beams]]></dc:title>
<dc:source><![CDATA[WP 3 Meeting, ENVISION, 04.09.2010, Stockholm, Schweden]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:subject><![CDATA[in-vivo dosimetry]]></dc:subject>
<dc:subject><![CDATA[proton irradiation]]></dc:subject>
<dc:subject><![CDATA[ion irradiation]]></dc:subject>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<identifier>HZDR:PUBLDB:415-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Kljukin, A.]]></dc:creator>
<dc:creator><![CDATA[Kolesnikov, Y.]]></dc:creator>
<dc:creator><![CDATA[Lielausis, O.]]></dc:creator>
<dc:creator><![CDATA[Platacis, E.]]></dc:creator>
<dc:creator><![CDATA[Skopis, M.]]></dc:creator>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-415-1</dc:identifier>
<dc:title><![CDATA[Local properties of a Hg/N2 bubbly flow injected by a single orifice in a longitudinal magnetic field]]></dc:title>
<dc:source><![CDATA[Int. Riga Conference on MHD, August 1995, Riga]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:664-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Dittes, F.-M.]]></dc:creator>
<dc:creator><![CDATA[Doron, E.]]></dc:creator>
<dc:creator><![CDATA[Smilansky, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-664-1</dc:identifier>
<dc:title><![CDATA[Long-time behavior of the semiclassical baker's map]]></dc:title>
<dc:source><![CDATA[Physical Review E 49 (1994) pp. R963]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:332-1</identifier>
<datestamp>2020-12-10</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schell, N.]]></dc:creator>
<dc:creator><![CDATA[Simmons, R. O.]]></dc:creator>
<dc:creator><![CDATA[Burkel, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-332-1</dc:identifier>
<dc:title><![CDATA[First observation of inelastic X-ray scattering from condensed <SUP>4</SUP>He using high energy resolution]]></dc:title>
<dc:source><![CDATA[Journal of Synchrotron Radiation (1996). 3, 316-317]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Recently, the suitability of inelastic X-ray scattering for the investigation of solid and fluid <SUP>4</SUP>HE has been demonstraded. For the text experiments an energy resolution of the order of 10-15 meV was used at the backscattering spectrometer INELAX at the storage ring DORIS of DESY, Hamburg. Lattice excitations were observed for momentum transfers along the c axis of h.c.p. helium crystals which were grown in situ at pressures of 54-63 Mpa and at temperatures of 4.2-6.4 K. At 10 k abowve the melting point, engery-loss signals could also be detected from the liquid helium at equivalent momentum transfers.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1107/S0909049596008941]]></dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:2105-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Fülle, R.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-2105-1</dc:identifier>
<dc:title><![CDATA[Jahresbericht 1997/98 und 1. Halbjahr 1999 Abteilung Kommunikation und Datenverarbeitung]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-274 Juli 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Bericht der Abteilung Kommunikation und Datenverarbeitung des FZR über ihre Tätigkeit in den Jahren 1997, 1998 und im 1. Halbjahr 1999]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2104-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Stefani, F.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2104-1</dc:identifier>
<dc:title><![CDATA[A contactless method for velocity reconstruction in electrically conducting fluids]]></dc:title>
<dc:source><![CDATA[Measurement science and technology 11 (2000) 758-765]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[A contactless method for velocity determination in electrically conducting fluids is presented. The method is based on the fact that an additional magnetic field is induced if the moving fluid is exposed to a primary magnetic field. Applying the primary  magnetic field in two different directions and measuring the corresponding induced magnetic fields the fluid velocity can be reconstructed if some kind of regularization for the velocity field is used. For a spherical shaped conducting fluid analytical expressions for the connection between spherical harmonics expansion coefficients of the induced magnetic fields on one side and of the defining scalars of the velocity on the other side are given. For other geometries a general method for numerical treatment is proposed.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:2098-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Naumann, B.]]></dc:creator>
<dc:creator><![CDATA[Neubert, W.]]></dc:creator>
<dc:creator><![CDATA[Pröhl, D.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-2098-1</dc:identifier>
<dc:title><![CDATA[Entwicklung von Strahlfängern für maximale Elektronenenergie am Beschleuniger ELBE]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-267 Juli 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[A design study of beam dumps is presented for the 40 MeV superconducting Electron-Linearaccelerator ELBE.  Nuclear physical and thermal properties of selected materials are considered. Energy deposition and neutron production were calculated for a special design of the beam dump. For those  Monte-Carlo simulations the particle transport rogram packages  GEANT, MCNP and FLUKA have been used. The expected activation under  beam conditions was estimated for selected dump materials.]]></dc:description>
<dc:subject><![CDATA[beam dump]]></dc:subject>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2101-1</identifier>
<datestamp>2025-12-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Seifert, S.]]></dc:creator>
<dc:creator><![CDATA[Drews, A.]]></dc:creator>
<dc:creator><![CDATA[Gupta, A.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2101-1</dc:identifier>
<dc:title><![CDATA[Stability Studies on <SUP>99m</SUP>Technetium(III) Complexes with Tridentate/Monodentate Thiol Ligands and Phosphine ("3+1+1" Complexes)]]></dc:title>
<dc:source><![CDATA[Appl. Radiat. Isot. 53 (2000) 431-438]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The preparation and characterisation of "3+1+1" technetium complexes of the gen-eral formula [Tc(SES)(RS)(PMe<SUB>2</SUB>Ph)] (SES = tridentate dithiol ligand, E = S, O, NMe; RSH = monothiol ligand) at the no carrier added level is described. The Tc(III) com-plexes are prepared in a one-step procedure starting from pertechnetate in yields of 85 - 95 % of radiochemical purity. A comparison of their chromatographic data with the fully characterised <SUP>99</SUP>Tc complexes indicate the identity of the investigated com-pounds. Stability studies show that the <SUP>99m</SUP>Tc complexes undergo some alteration in solution. They are oxidised to the 3+1 oxotechnetium(V) complexes and/or decom-pose in aqueous solution. In challenge experiments performed with glutathione, ex-change of the monothiolato ligand occurs in the same manner as known for the 3+1 complexes.]]></dc:description>
<dc:subject><![CDATA[3+1+1 <SUP>99m</SUP>Tc complexes]]></dc:subject>
<dc:subject><![CDATA[preparation]]></dc:subject>
<dc:subject><![CDATA[stability]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0969-8043(99)00169-4]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2101-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2333-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Mändl, S.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2333-1</dc:identifier>
<dc:title><![CDATA[Plasma-Immersions-Ionenimplantation für große Oberflächen]]></dc:title>
<dc:source><![CDATA[JOT 37 (1997) II-IV]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2333-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2334-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Nangia, A.]]></dc:creator>
<dc:creator><![CDATA[Kim, J. H.]]></dc:creator>
<dc:creator><![CDATA[Weiß, A. H.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2334-2</dc:identifier>
<dc:title><![CDATA[Experimental determination of positron related surface characteristics of 6H-SiC]]></dc:title>
<dc:source><![CDATA[American Physical Society Meeting, Kansas City, USA, March 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2334-3</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Nangia, A.]]></dc:creator>
<dc:creator><![CDATA[Kim, J. H.]]></dc:creator>
<dc:creator><![CDATA[Weiß, A. H.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2334-3</dc:identifier>
<dc:title><![CDATA[Experimental determination of positron related surface characteristics of 6H-SiC]]></dc:title>
<dc:source><![CDATA[11th Int. Conf. on Positron Annihilation (ICPA-11), Kansas City, USA, May 25-30,1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2334-4</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
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<dc:creator><![CDATA[Nangia, A.]]></dc:creator>
<dc:creator><![CDATA[Kim, J. H.]]></dc:creator>
<dc:creator><![CDATA[Weiß, A. H.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2334-4</dc:identifier>
<dc:title><![CDATA[Experimental determination of positron related surface characteristics of 6H-SiC]]></dc:title>
<dc:source><![CDATA[American Vacuum Society - Texas Chapter (Symp. on Electronic Materials, Processing and Characteri-zation), Austin, TX, USA, June 3 - 4, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2334-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Nangia, A.]]></dc:creator>
<dc:creator><![CDATA[Kim, J. H.]]></dc:creator>
<dc:creator><![CDATA[Weiß, A. H.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2334-1</dc:identifier>
<dc:title><![CDATA[Experimental determination of positron related surface characteristics of 6H-SiC]]></dc:title>
<dc:source><![CDATA[Mat. Sci. Forum 255-257 (1997) 711]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2336-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
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<dc:creator><![CDATA[Nicht, E.-M.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Cieslar, M.]]></dc:creator>
<dc:creator><![CDATA[Vostry, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2336-1</dc:identifier>
<dc:title><![CDATA[Positron annihilation spectroscopy, electrical resistivity, and microstructural transmission electron microscopy studies of the CuMn system]]></dc:title>
<dc:source><![CDATA[Mat. Sci. Forum 255-257 (1997) 572]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:2339-1</identifier>
<datestamp>2019-03-04</datestamp>
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</header>
<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Nomura, N.]]></dc:creator>
<dc:creator><![CDATA[Shiozawa, H.]]></dc:creator>
<dc:creator><![CDATA[Takada, T.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2339-1</dc:identifier>
<dc:title><![CDATA[Gas-sensor properties of SnO<SUB>2</SUB> films implanted with gold and iron ions]]></dc:title>
<dc:source><![CDATA[J. Mat. Sci.: Materials in Electronics 8 (1997) 301]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:2340-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Reichert, W.]]></dc:creator>
<dc:creator><![CDATA[Lossy, R.]]></dc:creator>
<dc:creator><![CDATA[Gonzalez Sirgo, M.]]></dc:creator>
<dc:creator><![CDATA[Obermeier, E.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2340-1</dc:identifier>
<dc:title><![CDATA[Investigation of the effects of high temperature implantation and post implantation annealing on the electrical behaviour of nitrogen implanted $-SiC films]]></dc:title>
<dc:source><![CDATA[Diam. Relat. Mater. 6 (1997) 1445]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:2341-1</identifier>
<datestamp>2025-04-16</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Frauendorf, S.]]></dc:creator>
<dc:creator><![CDATA[Sheikh, J. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2341-1</dc:identifier>
<dc:title><![CDATA[Rotational alignment near N=Z and proton-neutron correlations]]></dc:title>
<dc:source><![CDATA[Physical Review C, Volume 59, Number 3, March 1999, 1400-1404]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevC.59.1400]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2341-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2342-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2342-1</dc:identifier>
<dc:title><![CDATA[Härten von Edelstahl durch Stickstoff-Plasma-Immersions-Ionenimplantation]]></dc:title>
<dc:source><![CDATA[Ingenieur-Werkstoffe 6 (1997) 44]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:2345-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Guratzsch, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2345-1</dc:identifier>
<dc:title><![CDATA[Astatine-211 production at the Rossendorf cyclotron]]></dc:title>
<dc:source><![CDATA[Meeting on 211-At in anti-cancer therapy, Ispra, June 7th / 8th, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The production of Astatine-211 with the 120 cm Rossendorf cyclotron U-120 has been going on for two decades. Natural Bismuth evaporated on an Aluminium backing, a specially constructed water cooled target-block, is irradiated by 28 MeV Alpha-particles: 209Bi(Alpha, 2n)211At. For safety reasons the beam current is limited to 10 µA. The irradiated target is transported to the user who extracts the Astatine by himself. He also prepares the target with Bismuth for the next irradiation.]]></dc:description>
<dc:subject><![CDATA[Isotope production]]></dc:subject>
<dc:subject><![CDATA[Astatine-211]]></dc:subject>
<dc:subject><![CDATA[cyclotron]]></dc:subject>
<dc:subject><![CDATA[target construction]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:1665-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Höhne, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1665-1</dc:identifier>
<dc:title><![CDATA[CFD-Anwendungen zur Kühlmittelvermischung in Druckwasserreaktoren]]></dc:title>
<dc:source><![CDATA[CFX-Anwendertreffen, Bad Dürkheim, 16./17. September 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Um sich ein besseres Bild über die Strömungsvorgänge im Downcomer und im   unteren Plenum eines Druckwasserreaktors machen zu können, wurde mit einem CFD-Code (CFX 4.1) die Strömung unter möglichst realen Randbedingungen nachgerechnet. Hierfür wurden uns freundlicherweise Meßdaten des Anfahrvorganges der Hauptkühlmittelpumpe des DWR Konvoi zur Verfügung gestellt. Die Nachrechnung realer Anfahrvorgänge des DWR Konvoi mit Hilfe von IBS-Meßdaten zeigten eine relativ gute Durchmischung des Kühlmittels im unteren Plenum. Interessant war es festzustellen, daß das Geschwindigkeitsmaximum im unteren Downcomerbereich wie ein Halbkreis um den angefahrenen Stutzen liegt. Unterhalb dieses Stutzens ist die Geschwindigkeit vermindert.

]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:2925-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Iwasa, N.]]></dc:creator>
<dc:creator><![CDATA[Boue, F.]]></dc:creator>
<dc:creator><![CDATA[Surowka, G.]]></dc:creator>
<dc:creator><![CDATA[Sümmerer, K.]]></dc:creator>
<dc:creator><![CDATA[Baumann, T.]]></dc:creator>
<dc:creator><![CDATA[Blank, B.]]></dc:creator>
<dc:creator><![CDATA[Czajkowski, S.]]></dc:creator>
<dc:creator><![CDATA[Förster, A.]]></dc:creator>
<dc:creator><![CDATA[Gai, M.]]></dc:creator>
<dc:creator><![CDATA[Geissel, H.]]></dc:creator>
<dc:creator><![CDATA[Grosse, E.]]></dc:creator>
<dc:creator><![CDATA[Hellström, M.]]></dc:creator>
<dc:creator><![CDATA[Koczon, P.]]></dc:creator>
<dc:creator><![CDATA[Kohlmeyer, B.]]></dc:creator>
<dc:creator><![CDATA[Kulessa, R.]]></dc:creator>
<dc:creator><![CDATA[Laue, F.]]></dc:creator>
<dc:creator><![CDATA[Marchand, C.]]></dc:creator>
<dc:creator><![CDATA[Motobayashi, T.]]></dc:creator>
<dc:creator><![CDATA[Oeschler, H.]]></dc:creator>
<dc:creator><![CDATA[Ozawa, A.]]></dc:creator>
<dc:creator><![CDATA[Pravikoff, M. S.]]></dc:creator>
<dc:creator><![CDATA[Schwab, E.]]></dc:creator>
<dc:creator><![CDATA[Schwab, W.]]></dc:creator>
<dc:creator><![CDATA[Senger, P.]]></dc:creator>
<dc:creator><![CDATA[Speer, J.]]></dc:creator>
<dc:creator><![CDATA[Sturm, C.]]></dc:creator>
<dc:creator><![CDATA[Surowiec, A.]]></dc:creator>
<dc:creator><![CDATA[Teranishi, T.]]></dc:creator>
<dc:creator><![CDATA[Uhlig, F.]]></dc:creator>
<dc:creator><![CDATA[Wagner, A.]]></dc:creator>
<dc:creator><![CDATA[Walus, W.]]></dc:creator>
<dc:creator><![CDATA[Bertulani, C.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2925-1</dc:identifier>
<dc:title><![CDATA[Measurement of the Coulomb Dissociation of 8B at 254 MeV/nucleon and the 8B Solar Neutrino Flux.]]></dc:title>
<dc:source><![CDATA[Physical Review Letters 83, 2910-2913]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[We have measured the Coulomb dissociation of 8B into 7Be and a proton at 254 MeV/nucleon using a large-acceptance focusing spectrometer.
The astrophysical S17-factor for the 7Be(p, gamma)8B reaction at Ec.m. = 0.25-2.78  MeV is deduced yielding S17(0) = 20.6±1.2 (expt)
±1.0(theor)  eV b. This result agrees with the presently adopted zero-energy S17-factor obtained in direct-reaction measurements and with the
results of other Coulomb-dissociation studies performed at 46.5 and 51.2 MeV/nucleon.]]></dc:description>
<dc:subject><![CDATA[Coulomb Dissociation 8B Solar Neutrino Flux]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:14245-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hilger, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14245-1</dc:identifier>
<dc:title><![CDATA[Chiral symmetry and medium modifications of mesons]]></dc:title>
<dc:source><![CDATA[EMMI workshop "Quarkonium and the deconfined matter in the LHC era", 15.-20.06.2010, Martina Franca, Italien]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Using QCD sum rules we investigate the in-medium behavior of pseudo-scalar and vector mesons. The rho meson is considered within a scenario of pure chiral restoration by dropping the chirally odd condensates. The interplay of mass shift and broadening of the spectral function is highlighted. We apply finite density QCD sum rules to mesons consisting of a heavy and a light quark (D, Ds and B) and investigate their sensitivity to the chiral condensate and consider the splitting of particle and antiparticle spectral functions with increasing density of the ambient nuclear matter. In order to gain a more direct dependence on the chiral condensate and other potential order parameters of chiral symmetry we present a series of Weinberg-Shuryak type sum rules for heavy-light systems at finite densities. Furthermore, the special role of the gluon condensates for systems consisting of two heavy quarks (e.g. J/Psi) and the QCD trace anomalie allows an extension of the method to large temperatures at non-zero baryon densities using the Rossendorf quasi-particle model.]]></dc:description>
<dc:subject><![CDATA[QCD sum rules]]></dc:subject>
<dc:subject><![CDATA[chiral symmetry]]></dc:subject>
<dc:subject><![CDATA[rho meson]]></dc:subject>
<dc:subject><![CDATA[D meson]]></dc:subject>
<dc:subject><![CDATA[open charm]]></dc:subject>
<dc:subject><![CDATA[chiral partner]]></dc:subject>
<dc:subject><![CDATA[J/Psi]]></dc:subject>
<dc:subject><![CDATA[Dyson-Schwinger equation]]></dc:subject>
<dc:subject><![CDATA[Bethe-Salpeter equation]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:14245-2</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hilger, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14245-2</dc:identifier>
<dc:title><![CDATA[Chiral symmetry and medium modifications of mesons]]></dc:title>
<dc:source><![CDATA[QCD 10 - 15th high-energy physics international conference in quantum, 28.06.-3.7.2010, Montpellier, Frankreich]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Using QCD sum rules we investigate the in-medium behavior of pseudo-scalar and vector mesons. The rho meson is considered within a scenario of pure chiral restoration by dropping the chirally odd condensates. The interplay of mass shift and broadening of the spectral function is highlighted. We apply finite density QCD sum rules to mesons consisting of a heavy and a light quark (D, Ds and B) and investigate their sensitivity to the chiral condensate and consider the splitting of particle and antiparticle spectral functions with increasing density of the ambient nuclear matter. In order to gain a more direct dependence on the chiral condensate and other potential order parameters of chiral symmetry we present a series of Weinberg-Shuryak type sum rules for heavy-light systems at finite densities. Furthermore, the special role of the gluon condensates for systems consisting of two heavy quarks (e.g. J/Psi) and the QCD trace anomalie allows an extension of the method to large temperatures at non-zero baryon densities using the Rossendorf quasi-particle model.]]></dc:description>
<dc:subject><![CDATA[QCD sum rules]]></dc:subject>
<dc:subject><![CDATA[chiral symmetry]]></dc:subject>
<dc:subject><![CDATA[rho meson]]></dc:subject>
<dc:subject><![CDATA[D meson]]></dc:subject>
<dc:subject><![CDATA[open charm]]></dc:subject>
<dc:subject><![CDATA[chiral partner]]></dc:subject>
<dc:subject><![CDATA[J/Psi]]></dc:subject>
<dc:subject><![CDATA[Dyson-Schwinger equation]]></dc:subject>
<dc:subject><![CDATA[Bethe-Salpeter equation]]></dc:subject>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14245-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:14245-3</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hilger, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14245-3</dc:identifier>
<dc:title><![CDATA[Chiral symmetry and medium modifications of mesons]]></dc:title>
<dc:source><![CDATA[QCHS 9 - IX Quark Confinement and the Hadron Spectrum, 30.08.-03.09.2010, Madrid, Spanien]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Using QCD sum rules we investigate the in-medium behavior of pseudo-scalar and vector mesons. The rho meson is considered within a scenario of pure chiral restoration by dropping the chirally odd condensates. The interplay of mass shift and broadening of the spectral function is highlighted. We apply finite density QCD sum rules to mesons consisting of a heavy and a light quark (D, Ds and B) and investigate their sensitivity to the chiral condensate and consider the splitting of particle and antiparticle spectral functions with increasing density of the ambient nuclear matter. In order to gain a more direct dependence on the chiral condensate and other potential order parameters of chiral symmetry we present a series of Weinberg-Shuryak type sum rules for heavy-light systems at finite densities. Furthermore, the special role of the gluon condensates for systems consisting of two heavy quarks (e.g. J/Psi) and the QCD trace anomalie allows an extension of the method to large temperatures at non-zero baryon densities using the Rossendorf quasi-particle model.]]></dc:description>
<dc:subject><![CDATA[QCD sum rules]]></dc:subject>
<dc:subject><![CDATA[chiral symmetry]]></dc:subject>
<dc:subject><![CDATA[rho meson]]></dc:subject>
<dc:subject><![CDATA[D meson]]></dc:subject>
<dc:subject><![CDATA[open charm]]></dc:subject>
<dc:subject><![CDATA[chiral partner]]></dc:subject>
<dc:subject><![CDATA[J/Psi]]></dc:subject>
<dc:subject><![CDATA[Dyson-Schwinger equation]]></dc:subject>
<dc:subject><![CDATA[Bethe-Salpeter equation]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2034-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Höhne, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2034-1</dc:identifier>
<dc:title><![CDATA[Modellierung der Kühlmittelvermischung im Ringraum von Druckwasser- reaktoren mit Hilfe von Methoden der numerischen Fluiddynamik]]></dc:title>
<dc:source><![CDATA[Workshop Kompetenzerhaltung Kerntechnik, KTG-Jahrestagung, München, 28.5. 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[
Es wurden für die Simulation die DWR Konvoi und WWER-440 ausgewählt, wobei hierbei sich auf die Netzgenerierung des Downcomerbereiches und des untereren Plenums beschränkt wurde. Hierbei wurde das dreidimensionale Strömungsberechnungsprogramm CFX 4.1 eingesetzt, welches die Navier-Stokes-Gleichungen löst. Das verwendete Turbulenzmodell war das k-Epsilon-Modell. Die Strömung des Kühlmittels wurde inkompressibel gerechnet. Es wurde Wert auf eine möglichst originalgetreue Gestaltung des Stutzenbereiches / Schrägen bzw. Erweiterungen im Downcomer und Rundungen der Stutzenpartien gelegt. Der Bereich hoher Geschwindigkeitsgradienten wurde mit einem dichteren Grid generiert.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2034-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1934-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1934-1</dc:identifier>
<dc:title><![CDATA[Nachrechnung eines Abblaseexperimentes mit den thermohydraulischen Störfallprogrammen ATHLET und RELAP]]></dc:title>
<dc:source><![CDATA[FSS 08/92, Mai 1992]]></dc:source>
<dc:date>1992</dc:date>
<dc:description><![CDATA[Der Bericht beschreibt Nachrechnungen eines Abblaseexperiments, das vor etwa 10 Jahren am Moskauer Energetischen Institut durchgef|hrt wurde und für das experimentelle Daten des zeitlichen Verlaufes der Druckentlastung im Abblasebehälter und des Dampfgehaltes in verschiedenen Gefäßhöhen vorliegen.
Es wurden die Programme RELAP5/mod2 und ATHLET 1.0 Version E eingesetzt. Wie es sich zeigt, hat die richtige Beschreibung der Zweiphasenströmung an der Ausströmöffnung den größten Einfluß auf die Genauigkeit der Nachrechnung. Hierfür bietet das stationdre 1D-FD-Modell für kritisches Ausströmen des Programms ATHLET die bessere Anpassungsfähigkeit an die gegebenen Versuchsbedingungen.
]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1934-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:14533-2</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Niemietz, K.]]></dc:creator>
<dc:creator><![CDATA[Galindo, V.]]></dc:creator>
<dc:creator><![CDATA[Pätzold, O.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Stelter, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14533-2</dc:identifier>
<dc:title><![CDATA[Flow modelling with relevance to Vertical Gradient Freeze crystal growth under the Influence of a travelling magnetic field]]></dc:title>
<dc:source><![CDATA[The 16th International Conference on Crystal Growth(ICCG-16), 08.-13.08.2010, Beijing, China]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Results on the experimental and numerical modelling of the melt flow typically observed in Vertical Gradient Freeze (VGF) crystal growth with a Travelling Magnetic Field (TMF) are presented. Particular attention is paid on the transition from a laminar to a time-dependent flow, which represents a crucial problem in VGF growth. Low-temperature model experiments at around 80°C were performed using a GaInSn melt in a resistance furnace with concentric, separately adjustable heating zones. The TMF was created by an external coil system, and the flow velocity was measured by means of the Ultrasonic Doppler Velocimetry (UDV). The melt flow was simulated numerically using a finite volume code based on the open source code library OpenFOAM. As a criterion for the stability of the flow the turbulent kinetic energy was calculated under the influence of the TMF and thermal buoyancy. The results obtained are compared to isothermal TMF flow modelling at ambient temperature. The stability limit of the melt flow is found to be significantly influenced by the mutual interaction of buoyant and TMF-driven flows. Both experimental and numerical results show the stabilizing effect of a natural, VGF-type buoyancy on the TMF-induced flow.]]></dc:description>
<dc:subject><![CDATA[fluid flows]]></dc:subject>
<dc:subject><![CDATA[magnetic fields]]></dc:subject>
<dc:subject><![CDATA[stirring]]></dc:subject>
<dc:subject><![CDATA[vertical gradient freeze technique]]></dc:subject>
<dc:subject><![CDATA[numerical simulation]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<header>
<identifier>HZDR:PUBLDB:14533-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Niemietz, K.]]></dc:creator>
<dc:creator><![CDATA[Galindo, V.]]></dc:creator>
<dc:creator><![CDATA[Pätzold, O.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Stelter, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14533-1</dc:identifier>
<dc:title><![CDATA[Flow modelling with relevance to Vertical Gradient Freeze crystal growth under the Influence of a travelling magnetic field]]></dc:title>
<dc:source><![CDATA[Journal of Crystal Growth 318(2011), 150-155]]></dc:source>
<dc:date>2011</dc:date>
<dc:description><![CDATA[Results on the experimental and numerical modelling of the melt flow typically observed in Vertical Gradient Freeze (VGF) crystal growth with a Travelling Magnetic Field (TMF) are presented. Particular attention is paid on the transition from a laminar to a time-dependent flow, which represents a crucial problem in VGF growth. Low-temperature model experiments at around 80°C were performed using a GaInSn melt in a resistance furnace with concentric, separately adjustable heating zones. The TMF was created by an external coil system, and the flow velocity was measured by means of the Ultrasonic Doppler Velocimetry (UDV). The melt flow was simulated numerically using a finite volume code based on the open source code library OpenFOAM. As a criterion for the stability of the flow the turbulent kinetic energy was calculated under the influence of the TMF and thermal buoyancy. The results obtained are compared to isothermal TMF flow modelling at ambient temperature. The stability limit of the melt flow is found to be significantly influenced by the mutual interaction of buoyant and TMF-driven flows. Both experimental and numerical results show the stabilizing effect of a natural, VGF-type buoyancy on the TMF-induced flow.]]></dc:description>
<dc:subject><![CDATA[fluid flows]]></dc:subject>
<dc:subject><![CDATA[magnetic fields]]></dc:subject>
<dc:subject><![CDATA[stirring]]></dc:subject>
<dc:subject><![CDATA[vertical gradient freeze technique]]></dc:subject>
<dc:subject><![CDATA[numerical simulation]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/j.jcrysgro.2010.10.077]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14533-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:14503-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schade, H.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14503-1</dc:identifier>
<dc:title><![CDATA[Strangeness - phi mesons in pA reactions]]></dc:title>
<dc:source><![CDATA[International Workshop on Hot and Cold Baryonic Matter, 15.-19.08.2010, Budapest, Ungarn]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Recent experiments of the ANKE collaboration concerning the phi meson production in pA-reactions p (2.83 GeV) + C, Cu, Ag and Au are appropriate for the absorptive phi-N interaction within the trancparency ratio. With the aim of analyzing the amount of phi absorption we applied our well confirmed transport model of Boltzmann-Ühling-Uhlenbeck (BUU) type on this scenario. The results seem to point to an absorption cross section of 18 \pm 3 mb only when accounting for secundary phi production processes as well as isospin asymmetry and ANKE acceptance conditions.]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14503-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1599-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hirsch, W.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Brünig, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1599-1</dc:identifier>
<dc:title><![CDATA[Windpotentiale in Sachsen]]></dc:title>
<dc:source><![CDATA[Hrg.: Sächsisches Staatsministerium für Umwelt und Landesentwicklung, Reihe: Materialien zum Klimaschutz, Heft I/1997, 70 Seiten]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Im Bericht werden großflächige Untersuchungen zu windhöffigen Gebieten Sachsens vorgestellt. Für etwa 2/3 der Fläche Sachsens wurden die Windverhältnisse flächendeckend mit dem Programm WASP berechnet. Etwa 5% der Fläche Sachsens kann danach als windhöffig gelten. Als realistisches technisches Potential (Berücksichtigung von Bebauung, Naturschutzgebieten usw.) werden 5 TWh/a angesehen. Bis zum Jahr 2010 wird ein Erwartungspotential von 2 TWh/a geschätzt.]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Becker, H.]]></dc:creator>
<dc:creator><![CDATA[Kiefer, K.]]></dc:creator>
<dc:creator><![CDATA[Hoffmann, V. U.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Heilscher, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1596-7</dc:identifier>
<dc:title><![CDATA[5 Years of Operational Experience in the German 1000-Roof-Programme: Results of Monitoring and Inspection]]></dc:title>
<dc:source><![CDATA[Proceedings of the 14th European Photovoltaic Solar Energy Conference and Exhibition, Barcelona (Spain), 30 June - 4 July 1997, Volume II, p. 1677]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Within the framework of the German 1000-Roofs-PV-Programme, a total of 2011 grid connected PV systems with a total output of approximately 5.3 MWp were installed on the roofs of private houses. In addition to the recording and evaluation of the system data, another primary objective of the programme is the technical inspection of the PV systems and, in particular, the components used such as solar modules, cables, wires, diodes, fuses, terminals, overvoltage protection devices,DC isolating device and inverters. As some of the PV systems have now been in operation for as long as five years, it has been possible to gain valuable experience with regard to material time-to-failure, installation, environmental influences, maintenance, user behavior as well as on the stability and long term performance of the components used.]]></dc:description>
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<dc:creator><![CDATA[Becker, H.]]></dc:creator>
<dc:creator><![CDATA[Kiefer, K.]]></dc:creator>
<dc:creator><![CDATA[Hoffmann, V. U.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Heilscher, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1596-1</dc:identifier>
<dc:title><![CDATA[5 Years of Operational Experience in the German 1000-Roof-Programme: Results of Monitoring and Inspection]]></dc:title>
<dc:source><![CDATA[Proceedings of the 14th European Photovoltaic Solar Energy Conference and Exhibition, Barcelona (Spain), 30 June - 4 July 1997, Volume II, p. 1677]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Within the framework of the German 1000-Roofs-PV-Programme, a total of 2011 grid connected PV systems with a total output of approximately 5.3 MWp were installed on the roofs of private houses. In addition to the recording and evaluation of the system data, another primary objective of the programme is the technical inspection of the PV systems and, in particular, the components used such as solar modules, cables, wires, diodes, fuses, terminals, overvoltage protection devices,DC isolating device and inverters. As some of the PV systems have now been in operation for as long as five years, it has been possible to gain valuable experience with regard to material time-to-failure, installation, environmental influences, maintenance, user behavior as well as on the stability and long term performance of the components used.]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Alberto, R.]]></dc:creator>
<dc:creator><![CDATA[Dilwort, J.]]></dc:creator>
<dc:creator><![CDATA[Zheng, Y.]]></dc:creator>
<dc:creator><![CDATA[Ortner, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2064-1</dc:identifier>
<dc:title><![CDATA[Rhenium and Technetium Complexes with Pyridylphosphines]]></dc:title>
<dc:source><![CDATA[37. IUPAC-Kongress, Berlin, August 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Technetium and rhenium co-ordination chemistry is of particular interest due to the favourable nuclear properties of 99mTc (Eg = 140 keV, half-life t1/2 = 6.02 h) which makes this isotope the workhorse for diagnostic nuclear medicine. The b-emitting rhenium nuclides 186Re and 188Re are under investigation for possible applications in radioimmunotherapy. Fundamental co-ordination chemical studies form the basis for the development of new Tc and Re radiopharmaceuticals. 
Diphenyl(2-pyridyl)phosphine (PPh2py) and tris(2-pyridyl)phosphine (Ppy3) are a versatile ligands which can co-ordinate as a monodentate or chelating ligands depending on the requirements of the metal center.
The potentially bidentate ligand PPh2py reacted with (NEt4)2[MI(CO)3X3] complexes (M = Re, Tc) to give (NEt4)[MI(CO)3X2(PPh2py-P)] or [MI(CO)3X(PPh2py-P)2] depending on the amount of the ligand used. The reaction with (NBu4)[TcVINCl4] yielded [TcVNCl2(PPh2py-P)2] whereas from the reaction with (NBu4)[ReOCl4] the complexes [ReVOCl3(PPh2py-P,N)], [ReVOCl3(OPPh2py-O,N)], [ReIVCl4(OPPh2py-O,N) and [ReIVCl3(OH)(OPPh2py-O,N)] have been isolated. Reduction of the metal center and formation of diphenyl(2-pyridyl)phosphine oxide (OPPh2py) occurs using an excess of PPh2py and heating of the reaction mixtures under reflux. 
All products have been characterised spectroscopically and by X-ray structure analysis. Monodentate co-ordination via phosphorus has been found for the rhenium(I) carbonyl complexes and [TcVNCl2(PPh2py-P)2]. In the latter compound a trigonal-bipyramidal coordination sphere is formed with the phosphines as axial ligands. The chelated complexes show small N-Re-P and N-Re-O bite angles due to the 4-membered or 5-membered chelate rings. The pyridine nitrogen occupies the axial position (trans to "O2-") in [ReOCl3-(PPh2py-P,N)] whereas equatorial co-ordination is found in [ReOCl3(OPPh2py-O,N)].
The reaction of (NEt4)2[ReI(CO)3Br3] with Ppy3 gave [Re(CO)3Br(Ppy3-N,N')] whereas with o ...]]></dc:description>
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<identifier>HZDR:PUBLDB:1471-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1471-1</dc:identifier>
<dc:title><![CDATA[Auslegung und Erträge von netzgekoppelten Photovoltaik-Anlagen]]></dc:title>
<dc:source><![CDATA[Energie und Umwelt '99, 24.-25. März 1999, Freiberg, Tagungsband S. 81]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Im Vortrag werden ausgewählte Ergebnisse des 1000-Dächer-Programms zusammengefaßt, die für den Entwurf und die Energieerträge künftiger netzgekoppelter Anlagen relevant sind. Eine kritische Auswertung der Ergebnisse im hier relevanten Leistungsbereich (1-5 kWp) führt relativ zwangsläufig zum Konzept der Einstrang-Anlage. Der DC-Trennschalter kann - ebenso wie die Überspannungsableiter - in das Netzeinspeisegerät integriert werden. Ein künftiges integriertes Netzeinspeisegerät sollte neben dem Wechselrichter noch eine Diagnose- sowie Anzeigeeinheit, die neben Strom-, Spannungs-und Leistungswerten mittels eines einfachen Solarimeters das Performance Ratio errechnet und anzeigt, enthalten. Neben dem Anlagenkonzept ist die Auswahl der Komponenten entscheidend für die erreichbaren Erträge. Bei Nutzung von Modulen mit garantierter STC-Leistung und von Wechselrichtern mit hohem Jahresnutzungsgrad kann ein jährlicher Ertrag von 800 bis 850 kWh pro installierte Generatorleistung von 1 kW erwartet werden. Eine Anlage mit einer Leistung von 5 kW kann demnach den Bedarf eines Durchschnittshaushaltes rechnerisch decken.]]></dc:description>
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<identifier>HZDR:PUBLDB:1471-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1471-7</dc:identifier>
<dc:title><![CDATA[Auslegung und Erträge von netzgekoppelten Photovoltaik-Anlagen]]></dc:title>
<dc:source><![CDATA[Energie und Umwelt '99, 24.-25. März 1999, Freiberg, Tagungsband S. 81]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Im Vortrag werden ausgewählte Ergebnisse des 1000-Dächer-Programms zusammengefaßt, die für den Entwurf und die Energieerträge künftiger netzgekoppelter Anlagen relevant sind. Eine kritische Auswertung der Ergebnisse im hier relevanten Leistungsbereich (1-5 kWp) führt relativ zwangsläufig zum Konzept der Einstrang-Anlage. Der DC-Trennschalter kann - ebenso wie die Überspannungsableiter - in das Netzeinspeisegerät integriert werden. Ein künftiges integriertes Netzeinspeisegerät sollte neben dem Wechselrichter noch eine Diagnose- sowie Anzeigeeinheit, die neben Strom-, Spannungs-und Leistungswerten mittels eines einfachen Solarimeters das Performance Ratio errechnet und anzeigt, enthalten. Neben dem Anlagenkonzept ist die Auswahl der Komponenten entscheidend für die erreichbaren Erträge. Bei Nutzung von Modulen mit garantierter STC-Leistung und von Wechselrichtern mit hohem Jahresnutzungsgrad kann ein jährlicher Ertrag von 800 bis 850 kWh pro installierte Generatorleistung von 1 kW erwartet werden. Eine Anlage mit einer Leistung von 5 kW kann demnach den Bedarf eines Durchschnittshaushaltes rechnerisch decken.]]></dc:description>
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<identifier>HZDR:PUBLDB:1296-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Futterschneider, H.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1296-1</dc:identifier>
<dc:title><![CDATA[Modul-Untersuchungen im FZR-Testfeld]]></dc:title>
<dc:source><![CDATA[Sonnenenergie 5/1998, S. 36]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Seit 1993 wird im Institut für Sicherheitsforschung des FZR ein Photovoltaik-Experimentierfeld betrieben. Neben einer kleinen netzgekoppelten PV-Anlage besteht die Gesamtanlage aus einem Strahlungsmeßfeld und einem Modulmeßfeld. Durch kontinuierliche mehrjährige Kennlinienvermessung wurden die ertragsrelevanten Parameter von Modulen ermittelt. Die jährlichen Energieerträge unterschiedlich orientierter Module entsprechen den Berechnungen der jeweiligen Einstrahlungssummen nach dem PEREZ-Modell.
Die STC-Leistung verschiedener Module wurde nach einem Outdoor-Verfahren bestimmt. Dabei wurden Minderleistungen zwischen 15 und 25 % gegenüber Datenblattangaben gefunden. Das auf den DC-Ertrag bezogene Performance Ratio der einzelnen Module lag zwischen 89 und 94 %. Ein mittleres jährliches Leistungsspektrum -gültig für große Teile Deutschlands und kristalline Module- wurde ermittelt.
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1210-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:creator><![CDATA[Teichmann, G.]]></dc:creator>
<dc:creator><![CDATA[Futterschneider, H.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1210-1</dc:identifier>
<dc:title><![CDATA[Langzeituntersuchungen an netzgekoppelten Photovoltaikanlagen in Sachsen]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-221 Mai 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Zwischen 1993 und 1997 wurden 50 kleine netzgekoppelte Photovoltaikanlagen in Sachsen im Rahmen des 1000-Dächer-Photovoltaik-Programms systematisch untersucht. Neben der kontinuierlichen Auswertung der monatlichen Einstrahlung und der Energieerzeugung wurden alle Anlagen mittels eines PV-Anlagen-Analysators vermessen. An 5 Anlagen wurde ein erweitertes Messprogramm durchgeführt.
Die mittlere jährliche Einstrahlung auf geneigte Dachflächen in urbanen Gebieten Sachsens wurde zu 1050 kWh/m² bestimmt. Davon fallen 75 % während der Tageslastspitzen im Sommerhalbjahr an. Die ermittelten Kennlinien der eingesetzten Hauptkomponenten (Module, Wechselrichter) wichen teilweise erheblich von den Datenblattangaben ab. Gut ausgelegte und installierte Anlagen können bei einem Performance Ratio von 80 % einen jährlichen Ertrag von 840 kWh/kWp bringen. Künftig sollten  Anlagen im kleinen Leistungsbereich (bis 5 kWp) als Einstranganlagen errichtet werden. Der Energieverbrauch der einbezogenen Haushalte war überraschend hoch. Bei solaren Deckungsgraden von etwa 100 % konnten nur 25 % des erzeugten Stromes direkt in den Haushalten verbraucht werden. Bei Deckungsgraden von kleiner 20 % erreichte der Direktnutzungsgrad etwa 70 %.
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:239-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brünig, D.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-239-1</dc:identifier>
<dc:title><![CDATA[Einbindung ins Fernnetz wird in Sachsen erprobt]]></dc:title>
<dc:source><![CDATA[Sonnenenergie & Wärmetechnik  5/1994, S.21]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Solarwärme - Einbindung ins Fernwärmenetz wird in Sachsen erprobt
Die im Juni 1994 in Betrieb genommene solarthermische Anlage mit 100 m2 Kollektorfläche ist ein sächsisches Modellvorhaben. Neben der üblichen solaren Trinkwarmwasserbereitung - hier für die Schule - steht die Einspeisung von Solarwärme in ein neugeschaffenes gasbeheiztes Fernwärmenetz im Mittelpunkt eines Langzeitmeß- und analyseprogramms des Forschungszentrums Rossendorf. Die Solaranlage arbeitet nach dem Low-Flow-Prinzip der Kollektordurchströmung in Verbindung mit einer selbstregelnden Speicherschichtbeladung. Regelung und Meßdatenerfassung werden durch eine DDC-Anlage realisiert. 
]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:227-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brünig, D.]]></dc:creator>
<dc:creator><![CDATA[Naehring, F.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-227-1</dc:identifier>
<dc:title><![CDATA[Einspeisung von Solarwärme in konventionelle Fern- und Nahwärmenetze]]></dc:title>
<dc:source><![CDATA[Energieanwendung, Energie- und Umwelttechnik 43 (1994), 445]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[In der Arbeit werden unterschiedliche Konzepte der Einbindung großer Solaranlagen in konventionelle Wärmesysteme untersucht. Am Beispiel der Solaranlagen in Oederan und Freital wird die dezentrale Einbindung und die Einkopplung in Fernwärmenetze mit den entsprechenden Vor- und Nachteilen diskutiert. Als entscheidender Parameter für den zu erwartenden Ertrag erweist sich das Temperaturniveau des aufnehmenden Netzes.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:type>doc-type:article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1928-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Bergner, F.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1928-1</dc:identifier>
<dc:title><![CDATA[Zähigkeitsprüfung intermetallischer Phasen - Studie]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-92-07 May 1992]]></dc:source>
<dc:date>1992</dc:date>
<dc:description><![CDATA[In der vorliegenden Studie werden Ergebnisse zur Bruchzähigkeit intermetallischer Phasen sowie Erfahrungen bei deren experimentellen Bestimmung aus der Literatur zusammengetragen und diskutiert, ohne dabei Anspruch auf Vollständigkeit zu erheben. Da es für diese Kombination von Prüfaufgabe und Werkstoff bisher kaum gesicherte Erkenntnisse gibt, liegt der Schwerpunkt darauf, bevorzugt angewendete Verfahren herauszuarbeiten und die Gründe für diese Bevorzugung zu machen.
]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
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<dc:type>doc-type:report</dc:type>
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<identifier>HZDR:PUBLDB:853-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Denecke, M. A.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Bubner, M.]]></dc:creator>
<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:creator><![CDATA[Allen, P. G.]]></dc:creator>
<dc:creator><![CDATA[Bucher, J. J.]]></dc:creator>
<dc:creator><![CDATA[Edelstein, N. M.]]></dc:creator>
<dc:creator><![CDATA[Shuh, D. K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-853-1</dc:identifier>
<dc:title><![CDATA[Determination of Structural Parameters od Uranyl Ions Complexed with Organic Acids using EXAFS]]></dc:title>
<dc:source><![CDATA[ACTINIDES '97, 21.-26. September 1997 in Baden-Baden]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-853-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1072-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Panak, P.]]></dc:creator>
<dc:creator><![CDATA[Mack, B.]]></dc:creator>
<dc:creator><![CDATA[Baraniak, L.]]></dc:creator>
<dc:creator><![CDATA[Denecke, M. A.]]></dc:creator>
<dc:creator><![CDATA[Hennig, C.]]></dc:creator>
<dc:creator><![CDATA[Roßberg, A.]]></dc:creator>
<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1072-1</dc:identifier>
<dc:title><![CDATA[Determination of U(VI) Reduction after Bacterial Metabolization by Uranium L<SUB>III</SUB>-Edge Xanes Spectroscopy]]></dc:title>
<dc:source><![CDATA[HASYLAB Jahresbericht 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<record>
<header>
<identifier>HZDR:PUBLDB:3450-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, U.]]></dc:creator>
<dc:creator><![CDATA[Teschendorff, V.]]></dc:creator>
<dc:creator><![CDATA[Burtak, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3450-1</dc:identifier>
<dc:title><![CDATA[Aufgabenstellung - Validierung - Anwendung von gekoppelten 3D-Kernmodellen und Systemcodes]]></dc:title>
<dc:source><![CDATA[atw 45. Jg. (2000) Heft 6 - Juni]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[100 Wissenschaftler und Ingenieure aus elf europäischen Ländern und den USA waren der Einladung des Institutes für Sicherheitsforschung des Forschungszentrums Rossendorf (FZR) zum Fachtag "Wechselwirkungen zwischen Thermofluiddynamik und Neutronenkinetik" gefolgt. Die Tagung fand vom 31. Januar bis 1. Februar 2000 am FZR statt und wurde gemeinsam von den Fachgruppen "Reaktorphysik" und Thermofluiddynamik" der Kerntechnischen Gesellschaft veranstaltet. In 19 Vorträgen wurden Anforderungen an Sicherheitsanalysen aus der Sicht der Wissenschaft, der Industrie und der Gutachter formuliert. Programmschwerpunkte waren die Entwicklung von Methoden zur Kopplung von 3D Neutronenkinetik und Thermohydraulik, die Validierung der Modelle an Hand von Experimenten und die Anwendung für Sicherheitsanalysen von Leichtwasserreaktoren. Am Ende konnte festgestellt werden, dass mit den gekoppelten neutronenkinetisch-thermohydraulischen Systemcodes eine fortgeschrittene Simulationstechnik zur Verfügung steht, die eine wesentliche Erhöhung der Aussagesicherheit von Störfallsimulationen ermöglicht.]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:1976-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Weier, T.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Mutschke, G.]]></dc:creator>
<dc:creator><![CDATA[Fey, U.]]></dc:creator>
<dc:creator><![CDATA[Posdziech, O.]]></dc:creator>
<dc:creator><![CDATA[Lielausis, E.]]></dc:creator>
<dc:creator><![CDATA[Platacis, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1976-1</dc:identifier>
<dc:title><![CDATA[Some results on electromagnetic control of flow around bodies]]></dc:title>
<dc:source><![CDATA[Proc. of the International Symposium on  SEAWATER DRAG REDUCTION, pp. 395-400, Newport, Rhode Island (USA), 22.-24. Juli 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The flow around bodies (cylinder, plate) can be controlled by applying electromagnetic forces originating from electrodes and permanent magnets suitably placed on the surface of the body. There is a large variety for applying those forces with respect to the geometrical arrangement and the electrical current feeding the electrodes. The goals of this approach are flow stabilization, drag reduction or manoeuvrability of the body in an electrically low-conducting fluid like seawater. We present experimental and numerical results for a low Reynolds-number range of 200 < Re < 4000. Experiments were performed using a copper sulphate electrolytic solution and a sodium hydroxide loop. Flows are considered around a cylinder and over a plate, with
Lorentz forces being parallel to the body surface. Experimental results will be presented for the body drag and the wake flow structures depending on different
regimes of electromagnetic forcing. In particular, we distinguish between the
regimes of direct, frequency-variable sinusoidal or pulsed electric currents. Numerical results confirm the physical tendencies at least for lower Reynolds numbers.  Parameter ranges will be given for an optimal electromagnetic flow control in terms of drag reduction and flow laminarization. The energetic balance will be discussed. ]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2661-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:creator><![CDATA[Jankowsky, R.]]></dc:creator>
<dc:creator><![CDATA[Noll, B.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:creator><![CDATA[Dinkelborg, L. M.]]></dc:creator>
<dc:creator><![CDATA[Hilger, C. S.]]></dc:creator>
<dc:creator><![CDATA[Semmler, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2661-1</dc:identifier>
<dc:title><![CDATA[Technetium Coordination Ability of Cysteine-containing Peptides: X-ray Absorption Spectroscopy of a <SUP>99</SUP>Tc Labeled Endothelin Derivate]]></dc:title>
<dc:source><![CDATA[Applied Radiation and Isotopes 48,1045 (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2661-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2662-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kuhn, N.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Maichle-Mößmer, C.]]></dc:creator>
<dc:creator><![CDATA[Wiethoff, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2662-1</dc:identifier>
<dc:title><![CDATA[[Li<SUB>12</SUB>O<SUB>2</SUB>Cl<SUB>2</SUB>(ImN)<SUB>8</SUB>(THF)<SUB>4</SUB>] x 8 THF: ein Peroxokomplex des Lithiums mit neuartiger Käfigstruktur]]></dc:title>
<dc:source><![CDATA[Zeitschrift für anorganische und allgemeine Chemie 623, 1121 (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2662-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:3081-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Zessin, J.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3081-1</dc:identifier>
<dc:title><![CDATA[Triphenylarsonium-[<SUP>11</SUP>C]Methylid - Ein neuer <SUP>11</SUP>C-Präkursor zur Synthese von <SUP>11</SUP>C-Indolderivaten]]></dc:title>
<dc:source><![CDATA[36. Intern. Jahrestagung DGN, Leipzig, 01.-04.04.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Derivate des Indols sind Verbindungen mit vielfältigen physiologischen Funktionen und daher als Radiotracer von Interesse. Für die Synthese solcher <SUP>11</SUP>C-Verbindungen kann man die Umsetzung von Arsoniumyliden mit o-Aminobenzoylverbindungen  zu Indolen (Bravo, 1970) nutzen.
Methyltriphenylarsoniumiodid (MTPAI) als Vorstufe des Triphenylarsoniummethylids (TPAM) kann ausgehend von Methyliodid hergestellt werden. Mit [<SUP>11</SUP>C]Methyliodid ermöglicht dieser reaktionsweg die direkte Darstellung von <SUP>11</SUP>C-markierten Indolen.

Der erste syntheseschritt umfasst die Quaternisierung  von Triphenylarsin mit [<SUP>11</SUP>C]Methyliodid zu [<SUP>11</SUP>C]MTPAI. Ausreichende Reaktionsgeschwindigkeiten werden nur in Gegenwart stark polarer Lösungsmittel erreicht. Innerhalb von 10 min bei 120°C wurden in THF/DMSO (3:1) radiochemische Ausbeuten von 67% (bezogen auf [<SUP>11</SUP>C]CH<SUB>3</SUB>I, zerfallskorrigiert) und in Ethanol 76% erreicht.
Im zweiten Schritt erfolgt die in situ Generierung von [<SUP>11</SUP>C]TPAM durch Butyllithium und nachfolgend die Umsetzung mit o-Aminobenzaldehyd zu [2-<SUP>11</SUP>C]Indol.
Durch Verwendung von Alkyl-o-aminophenylketonen können 3-alkylierte [2-<SUP>11</SUP>C]Indole  hergestellt werden. O-Aminoacetophenon ergibt 3-Methyl-[2-<SUP>11</SUP>C]Indol und o-Aminopropiophenon 3-Etyl-[2-<SUP>11</SUP>C]Indol.
Ausgehend von dem neuen <SUP>11</SUP>C-Präkursor Triphenylarsonium[<SUP>11</SUP>C]methylid sind <SUP>11</SUP>C-kernmarkierte Indole mit radiochemischen Ausbeuten von 23 - 31% (bezogen auf [<SUP>11</SUP>C]CH<SUB>3</SUB>I, zerfallskorrigiert) herstellbar. 
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:3081-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Zessin, J.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3081-2</dc:identifier>
<dc:title><![CDATA[Triphenylarsonium-[<SUP>11</SUP>C]Methylid - Ein neuer <SUP>11</SUP>C-Präkursor zur Synthese von <SUP>11</SUP>C-Indolderivaten]]></dc:title>
<dc:source><![CDATA[Nuklearmedizin 37 (1998) A44]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Derivate des Indols sind Verbindungen mit vielfältigen physiologischen Funktionen und daher als Radiotracer von Interesse. Für die Synthese solcher <SUP>11</SUP>C-Verbindungen kann man die Umsetzung von Arsoniumyliden mit o-Aminobenzoylverbindungen  zu Indolen (Bravo, 1970) nutzen.
Methyltriphenylarsoniumiodid (MTPAI) als Vorstufe des Triphenylarsoniummethylids (TPAM) kann ausgehend von Methyliodid hergestellt werden. Mit [<SUP>11</SUP>C]Methyliodid ermöglicht dieser reaktionsweg die direkte Darstellung von <SUP>11</SUP>C-markierten Indolen.

Der erste syntheseschritt umfasst die Quaternisierung  von Triphenylarsin mit [<SUP>11</SUP>C]Methyliodid zu [<SUP>11</SUP>C]MTPAI. Ausreichende Reaktionsgeschwindigkeiten werden nur in Gegenwart stark polarer Lösungsmittel erreicht. Innerhalb von 10 min bei 120°C wurden in THF/DMSO (3:1) radiochemische Ausbeuten von 67% (bezogen auf [<SUP>11</SUP>C]CH<SUB>3</SUB>I, zerfallskorrigiert) und in Ethanol 76% erreicht.
Im zweiten Schritt erfolgt die in situ Generierung von [<SUP>11</SUP>C]TPAM durch Butyllithium und nachfolgend die Umsetzung mit o-Aminobenzaldehyd zu [2-<SUP>11</SUP>C]Indol.
Durch Verwendung von Alkyl-o-aminophenylketonen können 3-alkylierte [2-<SUP>11</SUP>C]Indole  hergestellt werden. O-Aminoacetophenon ergibt 3-Methyl-[2-<SUP>11</SUP>C]Indol und o-Aminopropiophenon 3-Etyl-[2-<SUP>11</SUP>C]Indol.
Ausgehend von dem neuen <SUP>11</SUP>C-Präkursor Triphenylarsonium[<SUP>11</SUP>C]methylid sind <SUP>11</SUP>C-kernmarkierte Indole mit radiochemischen Ausbeuten von 23 - 31% (bezogen auf [<SUP>11</SUP>C]CH<SUB>3</SUB>I, zerfallskorrigiert) herstellbar. 
]]></dc:description>
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<datestamp>2025-12-05</datestamp>
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</header>
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Rami, F.]]></dc:creator>
<dc:creator><![CDATA[Crochet, P.]]></dc:creator>
<dc:creator><![CDATA[Dona, R.]]></dc:creator>
<dc:creator><![CDATA[Schauenburg, B.]]></dc:creator>
<dc:creator><![CDATA[Wagner, P.]]></dc:creator>
<dc:creator><![CDATA[Alard, J. P.]]></dc:creator>
<dc:creator><![CDATA[Andronic, A.]]></dc:creator>
<dc:creator><![CDATA[Basrak, Z.]]></dc:creator>
<dc:creator><![CDATA[Bastid, N.]]></dc:creator>
<dc:creator><![CDATA[Belyaev, I.]]></dc:creator>
<dc:creator><![CDATA[Bendarag, A.]]></dc:creator>
<dc:creator><![CDATA[Berek, G.]]></dc:creator>
<dc:creator><![CDATA[Best, D.]]></dc:creator>
<dc:creator><![CDATA[Caplar, R.]]></dc:creator>
<dc:creator><![CDATA[Devismes, A.]]></dc:creator>
<dc:creator><![CDATA[Dupieux, P.]]></dc:creator>
<dc:creator><![CDATA[Dzelalija, M.]]></dc:creator>
<dc:creator><![CDATA[Eskef, M.]]></dc:creator>
<dc:creator><![CDATA[Fodor, Z.]]></dc:creator>
<dc:creator><![CDATA[Gobbi, A.]]></dc:creator>
<dc:creator><![CDATA[Grishkin, Y.]]></dc:creator>
<dc:creator><![CDATA[Herrmann, N.]]></dc:creator>
<dc:creator><![CDATA[Hildenbrand, K. D.]]></dc:creator>
<dc:creator><![CDATA[Hong, B.]]></dc:creator>
<dc:creator><![CDATA[Kecskemeti, J.]]></dc:creator>
<dc:creator><![CDATA[Kirejczyk, M.]]></dc:creator>
<dc:creator><![CDATA[Korolija, M.]]></dc:creator>
<dc:creator><![CDATA[Kotte, R.]]></dc:creator>
<dc:creator><![CDATA[Lebedev, A.]]></dc:creator>
<dc:creator><![CDATA[Leifels, Y.]]></dc:creator>
<dc:creator><![CDATA[Merlitz, H.]]></dc:creator>
<dc:creator><![CDATA[Mohren, S.]]></dc:creator>
<dc:creator><![CDATA[Moisa, D.]]></dc:creator>
<dc:creator><![CDATA[Neubert, W.]]></dc:creator>
<dc:creator><![CDATA[Pelte, D.]]></dc:creator>
<dc:creator><![CDATA[Petrovici, M.]]></dc:creator>
<dc:creator><![CDATA[Pinkenburg, C.]]></dc:creator>
<dc:creator><![CDATA[Plettner, C.]]></dc:creator>
<dc:creator><![CDATA[Reisdorf, W.]]></dc:creator>
<dc:creator><![CDATA[Schüll, D.]]></dc:creator>
<dc:creator><![CDATA[Seres, Z.]]></dc:creator>
<dc:creator><![CDATA[Sikora, B.]]></dc:creator>
<dc:creator><![CDATA[Simion, V.]]></dc:creator>
<dc:creator><![CDATA[Siwek-Wilczynska, K.]]></dc:creator>
<dc:creator><![CDATA[Stoicea, G.]]></dc:creator>
<dc:creator><![CDATA[Stockmeier, M.]]></dc:creator>
<dc:creator><![CDATA[Vasiliev, M.]]></dc:creator>
<dc:creator><![CDATA[Wisniewski, K.]]></dc:creator>
<dc:creator><![CDATA[Wohlfarth, D.]]></dc:creator>
<dc:creator><![CDATA[Yushmanov, I.]]></dc:creator>
<dc:creator><![CDATA[Zhilin, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2886-1</dc:identifier>
<dc:title><![CDATA[Flow Angle from Intermediate Mass Fragments]]></dc:title>
<dc:source><![CDATA[Nucl. Phys. A 646 (1999) 367]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Directed sideward flow of light charged particles and intermediate mass fragments was measured in different symmetric reactions at bombarding energies from 90 to 800 AMeV. The flow parameter is found to increase with the charge of the detected fragment up to Z=3-4 and turns into saturation for heavier fragments. Guided by simple simulations of an anisotropic expanding thermal source, we show that the value at saturation can provide a good estimate of the flow angle, Θ<sub>flow,</sub> in the participant region. It is found that Θ<sub>flow,</sub> depends strongly on the impact parameter. The excitation function of Θ<sub>flow,</sub> reveals striking deviations from the ideal hydrodynamical scaling. The data exhibit a steep rise of Θ<sub>flow,</sub> to a maximum at around 250-400 AMeV, followed by a moderate decrease as the bombarding energy increases further.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0375-9474(98)00641-1]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2886-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2895-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Rettig, D.]]></dc:creator>
<dc:creator><![CDATA[Adam, R.]]></dc:creator>
<dc:creator><![CDATA[Merker, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2895-1</dc:identifier>
<dc:title><![CDATA[Aerosol Formation by UV Irradiation of Paraffin and Silicone Vapors]]></dc:title>
<dc:source><![CDATA[European Aerosol Conference EAC´99,  Prag]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:3474-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Merroun, M.]]></dc:creator>
<dc:creator><![CDATA[Tzvetkova, Z.]]></dc:creator>
<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3474-1</dc:identifier>
<dc:title><![CDATA[Complexation of uranium by three different Acidithiobacillus Ferrooxidans types]]></dc:title>
<dc:source><![CDATA[BMRI-2 Euroconference on Bacterial-Metal/Radionuclide Interaction, Rossendorf bei Dresden, 30.8.-1.9. 2000]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[In uranium mining piles a number of acidophilic chemolithoautotrophic bacteria has been identified, which are able to oxidize sulphide minerals, elemental sulfur, ferrous iron, and, in presence of uranium minerals, also U(IV). Especially one representative of this group, Acidithiobacillus ferrooxidans, is of particular interest. This organism has been used commercially in metal leaching from ores and decontamination of industrial wastes [1].
Sequence analysis of the 16S rRNA genes of several reference strains and uranium mining waste pile isolates of this bacterium revealed specific signatures which distinguish three types within the species. This allowed to develop a technique for analysis of the distribution of the A. ferrooxidans eco-types in the soil samples of a uranium mining waste pile. 
The technique is based on amplification of 16S rDNA fragments in total soil DNA by the use of two A. ferrooxidans species specific primers 16S458F and 16S1473R [2]. The resulting amplicons were then digested with a frequently cutting enzyme RsaI  which produced three different type-specific profiles [3; 4]. Using this direct approach we have demonstrated that one of the A. ferrooxidans types (type I) was predominant in the soil samples studied and was found in more polluted sites, whereas the type II was found in less contaminated samples. The type III was found mostly to coexist with the type II.
The objectives of the present work were to determine whether these eco-types differ in their capability to tolerate and accumulate uranium, and also to study the structural complexes formed at the surfaces of A. ferrooxidans eco-types using different spectroscopic techniques as Extended X-ray Absorption Fine Structure (EXAFS), Infra Red (IR) and time-resolved laser-induced fluorescence spectroscopy (TRLFS). In addition, the most efficient desorbing agent for the accumulated uranium was selected.
The uranium accumulation by the above mentioned three types of A. ferrooxidans was studied at different metal concentrations and different pH values (1.5 and 4). The results obtained (Fig.1) demonstrated that the strains from the different types possess different capability to accumulate uranium. The amount of uranium biosorbed by the three types increased with increasing concentration of uranium.
Fig.1: Biosorption of uranium by different  types of A. ferrooxidans 

Interestingly, the strains W1 (type I) and D2 (type III) are resistant to 8 and 9 mM of uranium, respectively, whereas the strain ATCC 33020 (type II) does not tolerate more than 2 mM of uranium (Table 1).


Strains
	
Uranium (mM)
	Tolerated
	MICs
A. ferrooxidans W1 
	8	9
A. ferrooxidans ATCC 33020 
	2	4
A. ferrooxidans D2 
	9	10
Table 1: Minimum Inhibitory Concentrations (MICs) of uranium for the growth of A. ferrooxidans type

On the basis of these results, one may speculate that the strains of the types I and III are more resistant to uranium, probably because they possess a mechanism which limits the uranium binding below the lethal amounts. 

The desorption of the accumulated uranium from the bacterial cells was investigated using different desorbing agents as sodium carbonate, sodium citrate and EDTA at different concentrations. The results obtained demonstrated that the sodium carbonate is able to recuperate up to 97% of the uranium sorbed from the cells of A. ferrooxidans type III, and 88.33 and 88.50% from the cells of the types I and II, respectively.

Using EXAFS analysis we have found that no significant structural differences were observed between the uranium complexes formed by the 3 types of A. ferrooxidans. However, the EXAFS spectra are indicating formation of uranium complexes which are different from those formed by bacilli [5; 6].


Acknowledgements
This work was supported by grant 7531.50-03-FZR/607 from the Sächsisches Staatsministerium für Wissenschaft und Kunst, Dresden, Germany

]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:3380-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3380-1</dc:identifier>
<dc:title><![CDATA[A novel approach to robust Tc(III) mixed-ligand chelates as tools for conjugating biologically active molecules]]></dc:title>
<dc:source><![CDATA[Meeting der COST B12 Action, WG 5, Rom, 29.05.2000]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[To meet the need for small and "robust" chelates we focussed our recent investigations on new types of technetium(III) chelates, their synthesis and evaluation of molecular properties. Here we report  on five-coordinated compounds with "3+1+1", "3+2", and  "4+1" donor arrangements.
Such species, all belonging to the family of "n+1"mixed-ligand technetium complexes, were developed and characterized towards versatility, lipophilicity and stability.
The "3+2" approach make use of the combination of a tridentate HS-E-SH ligands with a PR<SUB>2</SUB>-SH chelator, common action of the tripodal nitrilotris(ethanethiol) with isocyanide co-ligands leads to 
trigonal-bipyramidal "4+1" Tc(III) complexes.
Both types enables easy functionalization and thus a fine-tuning of physicochemical properties of the complexes or to link the chelate unit to biomolecules.
The sterically well shielded oxo-free species are non-polar, showing higher logP values as the "3+1" oxotechnetium(V) compounds. The "3+2" and "4+1" complexes are stable towards re-oxidation and transchelation in challenge experiments with glutathione. The "3+2" type is the most versatile one while the compact "4+1" seems to be the most stable arrangement.
The presented "3+2" and "4+1" complex types  are useful tools in designing of <SUP>99m</SUP>Tc or <SUP>186/188</SUP>Re radiopharmaceuticals.
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2080-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Nebelung, C.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2080-1</dc:identifier>
<dc:title><![CDATA[Stillegung und Rückbau: Direktmessung alpha-aktiver Nuklide in Bauschutt zur Freigabeentscheidung, Schlußbericht zum Fördervorhaben 02 S 7655 und 02S7655A, Laufzeit: 01.05.1996 bis 31.10.1998]]></dc:title>
<dc:source><![CDATA[Abschlußbericht BMBF Projekt 02S7655 und 02S7655A Juli 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Beim Abriß von Nuklearanlagen fallen große Mengen Bauschutt an, die mit Radionukliden kontaminiert sein können. Da diese Kontaminationen häufig nahe der Freigrenze liegen, ist für die Entscheidung, ob das Material als radioaktiver Abfall behandelt werden muß oder freigegeben werden kann, eine schnelle und exakte Methode notwendig. Die Bestimmung der ( - und $ - Aktivivtät ist mit in-situ Messungen möglich. Eine direkte Messung der " - aktiven Nuklide im stehenden Gebäude ist auf Grund der geringen Reichweite der " -Strahlung und ihrer Absorption im Beton nicht möglich. Die übliche chemische Analyse der " - aktiven Nuklide ist sehr zeitaufwendig. 
Im Rahmen dieses Projektes wurde eine Methode der direkten " - Spektrometrie nach nur mechanischer Präparation des Betons entwickelt. In einem aus zwei Schritten bestehendem Zerkleinerungsprozeß wurden Suspensionen mit mittleren Partikeldurchmessern von 0,5 µm erhalten. Die Meßproben mit einem Durchmesser von 20 cm und Schichtdicken zwischen 0,6 und 5 µm wurden durch Gießen oder Sprühen auf die Probenträger und anschließendes Trocknen hergestellt. Die Spektren dieser Proben wurden in einer Gitterionisationskammer aufgenommen. Durch die Verwendung von Standardbeton mit dotierten Actiniden konnten die Selbstabsorption der " - Strahlung und die Peakform in Abhängigkeit der Schichtdicke ermittelt werden. Unbekannte Betonproben gleicher Geometrie konnten mit Hilfe dieser ermittelten Peakform entfaltet werden. 
Das für diese Arbeit entwickelte Programm WINKRUM basiert auf einem geometrischen Modell für Partikelgröße, Partikelverteilung und Packungsdichte. Mit Strahlungstransportberechnungen können Spektren simuliert werden, die ebenfalls eine Peakentfaltung von Multielementspektren ermöglichen.
Mit dieser Direktmessung dünner Meßproben können " - aktive Nuklide bis zu 0,02 Bq/g in Multielementspektren innerhalb von 30 h bestimmt werden.
 
]]></dc:description>
<dc:subject><![CDATA[Actinide]]></dc:subject>
<dc:subject><![CDATA[Alpha-aktive Nuklide]]></dc:subject>
<dc:subject><![CDATA[Alpha-Spektrometrie]]></dc:subject>
<dc:subject><![CDATA[Bauschutt]]></dc:subject>
<dc:subject><![CDATA[Beton]]></dc:subject>
<dc:subject><![CDATA[Dünne Schichten]]></dc:subject>
<dc:subject><![CDATA[Freigaberegelung]]></dc:subject>
<dc:subject><![CDATA[Freimessung]]></dc:subject>
<dc:subject><![CDATA[Kontamination]]></dc:subject>
<dc:subject><![CDATA[Nuklearanlagen]]></dc:subject>
<dc:subject><![CDATA[Stillegung]]></dc:subject>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2080-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:1382-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Friedrich, A.]]></dc:creator>
<dc:creator><![CDATA[Krizbai, I. A.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Roux, F.]]></dc:creator>
<dc:creator><![CDATA[Ganapathy, V.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1382-1</dc:identifier>
<dc:title><![CDATA[Functional expression of the serotonin transporter in immortalized rat brain microvessel endothelial cells]]></dc:title>
<dc:source><![CDATA[J.Neurochem. 74, (2000) 1241-1248]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[There is evidence from recent studies that the brain endothelium (of capillaries and/or larger vessels) may serve as a specific target for serotonin (5-HT). This neurotransmitter is expected to be involved in the regulation of the BBB permeability and/or of the cerebral blood flow via receptor-mediated mechanisms. Effective control of these processes depends on a speedy uptake and metabolism of released 5-HT molecules. To realise this, a similar mechanism of 5-HT uptake as in brain may exist at the BBB. In this study, we have demonstrated using reverse transcriptase-polymerase chain reaction (RT-PCR) that 5-HT transporter mRNA is present in the brain endothelium and that a saturable transport system for 5-HT is functionally expressed at immortalized rat brain endothelial cells (RBE4 cells). These cells take up [<SUP>3</SUP>H]5-HT by an active saturable process with a <I>K</I><SUB>m</SUB>-value of 397± 64 nmol/L and a transport capacity of 51.7 ± 3.5 pmolg<SUP>-1</SUP>min<SUP>-1</SUP>. The 5-HT uptake depends on Na<SUP>+</SUP>, as indicated by the replacement of NaCl by LiCl. The 5-HT uptake was sensitive to specific 5-HT transport inhibitors such as paroxetine, clomipramine, fluoxetine and citalopram, but not to inhibitors of the vesicular amine transporter such as reserpine or tetrabenazine. Our results demonstrate that cerebral endothelial cells are able to participate actively in the removal and metabolism of the released 5-HT, which supports the concept of direct serotonergic regulation of the BBB function.
]]></dc:description>
<dc:subject><![CDATA[Blood-brain barrier]]></dc:subject>
<dc:subject><![CDATA[gene expression]]></dc:subject>
<dc:subject><![CDATA[serotonin]]></dc:subject>
<dc:subject><![CDATA[transporter]]></dc:subject>
<dc:subject><![CDATA[clomipramine]]></dc:subject>
<dc:subject><![CDATA[citalopram]]></dc:subject>
<dc:subject><![CDATA[fluoxetine]]></dc:subject>
<dc:subject><![CDATA[paroxetine]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1382-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1382-2</identifier>
<datestamp>2023-05-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Friedrich, A.]]></dc:creator>
<dc:creator><![CDATA[Krizbai, I. A.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Roux, F.]]></dc:creator>
<dc:creator><![CDATA[Ganapathy, V.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1382-2</dc:identifier>
<dc:title><![CDATA[Functional expression of the serotonin transporter in immortalized rat brain microvessel endothelial cells]]></dc:title>
<dc:source><![CDATA[Journal of Cerebral Blood Flow and Metabolism, Vol. 19 (Suppl.1), 245]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[There is evidence from recent studies that the brain endothelium (of capillaries and/or larger vessels) may serve as a specific target for serotonin (5-HT). This neurotransmitter is expected to be involved in the regulation of the BBB permeability and/or of the cerebral blood flow via receptor-mediated mechanisms. Effective control of these processes depends on a speedy uptake and metabolism of released 5-HT molecules. To realise this, a similar mechanism of 5-HT uptake as in brain may exist at the BBB. In this study, we have demonstrated using reverse transcriptase-polymerase chain reaction (RT-PCR) that 5-HT transporter mRNA is present in the brain endothelium and that a saturable transport system for 5-HT is functionally expressed at immortalized rat brain endothelial cells (RBE4 cells). These cells take up [<SUP>3</SUP>H]5-HT by an active saturable process with a <I>K</I><SUB>m</SUB>-value of 397± 64 nmol/L and a transport capacity of 51.7 ± 3.5 pmolg<SUP>-1</SUP>min<SUP>-1</SUP>. The 5-HT uptake depends on Na<SUP>+</SUP>, as indicated by the replacement of NaCl by LiCl. The 5-HT uptake was sensitive to specific 5-HT transport inhibitors such as paroxetine, clomipramine, fluoxetine and citalopram, but not to inhibitors of the vesicular amine transporter such as reserpine or tetrabenazine. Our results demonstrate that cerebral endothelial cells are able to participate actively in the removal and metabolism of the released 5-HT, which supports the concept of direct serotonergic regulation of the BBB function.
]]></dc:description>
<dc:subject><![CDATA[Blood-brain barrier]]></dc:subject>
<dc:subject><![CDATA[gene expression]]></dc:subject>
<dc:subject><![CDATA[serotonin]]></dc:subject>
<dc:subject><![CDATA[transporter]]></dc:subject>
<dc:subject><![CDATA[clomipramine]]></dc:subject>
<dc:subject><![CDATA[citalopram]]></dc:subject>
<dc:subject><![CDATA[fluoxetine]]></dc:subject>
<dc:subject><![CDATA[paroxetine]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1046/j.1471-4159.2000.741241.x]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1382-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1664-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Krynkov, A.]]></dc:creator>
<dc:creator><![CDATA[Nikolaev, Y. A.]]></dc:creator>
<dc:creator><![CDATA[Korolev, Y.]]></dc:creator>
<dc:creator><![CDATA[Erak, D. Y.]]></dc:creator>
<dc:creator><![CDATA[Gerashenke, S.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1664-1</dc:identifier>
<dc:title><![CDATA[Einfluß der Zusammensetzung auf die Strahlenversprödung von Eisenlegierungen]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-255 Februar 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The radiation embrittlement of the reactor pressure vessel is highly safety-relevant for VVER-type pressure vessels. The sensitivity against radiation embrittlement depends on the chemical composition of the pressure vessel steel. Using an irradiation experiment at surveillance positions in two Russian VVER 440-type reactors the effects of copper, phosphorus and nickel on the radiation embrittlement should be investigated. For that, eight mock-up alloys were selected. Their chemical composition varied between 0.015 and 0.42 % Cu, 0.002 and 0.039 % P, 0.01 and 1.98 % Ni, 0.09 and 0.37 % Si, and 0.35 and 0.49 % Mn. Charpy-V impact tests and tensile tests were performed with specimens machined from these alloys. The specimens were tested in the as-received state, in the irradiated state (fluence: 1x10<sup>19</sup> and 8x10<sup>19</sup>  /cm<sup>2</sup> [E>0.5 MeV]) an in the post-irradiation annealed state. In the as-received state, the alloys have a ferritic microstructure. Apart from Cu, the alloyed elements are solved in the matrix.
Irradiation produces strong hardening and embrittlement. The effect increases with the Cu and P content. Ni causes an additional embrittlement. It is independent on the Ni concentration within the range of 1.1 to 2 % Ni and results in a shift of the ductile-brittle transition temperature of about 120 °C after a fluence of 1x10<sup>19</sup> /cm<sup>2</sup> by a flux of 4x10<sup>11</sup> /cm<sup>2</sup>s. The shift does not depend on the Cu or P content. Furthermore the upper shelf energy is especially reduced by the Ni-rich alloys. For very low content of Cu and P these relations are not valid. The irradiation effect can be eliminated by annealing at 475 °C /100 h. For high content of Cu or P the recovery is incomplete, it remains a residue of 20 to 25 % of the irradiation effect. Ni has no influence on the recovery.
Comparing the results of this study with the ones of the surveillance programmes of the VVER 440-type reactors, the alloys with low Ni content show the same irradiation behaviour as the weld metal. For the Ni rich alloys such well-walidated references are missing.
The experiment is part of an extended research programme. It supposed to continue in order to gain information about the synergistic effects of these elements. ]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1664-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:355-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Barz, H.-U.]]></dc:creator>
<dc:creator><![CDATA[Böhmer, B.]]></dc:creator>
<dc:creator><![CDATA[Konheiser, J.]]></dc:creator>
<dc:creator><![CDATA[Stephan, I.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-355-1</dc:identifier>
<dc:title><![CDATA[Ermittlung der Neutronendosis von bestrahlten WWER-Reaktordruckbehältermaterialien]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-87 Juni 1995]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[In this report is described the theoretical and experimental determination of all needed parameters  for the neutron exposure of the different specimens that were irradiated in the Rheinsberg reactor within the period from 1984 until 1988 to obtain data for neutron embrittlement studies.
The methodical approach is represented, possible sources of errors are discussed and all the needed results are collected. The work can be divided into a pure calculation part, into the description of the extraction of the monitors and their gamma spectrometric analysis and into the discussion of the spectrum adjustment procedure which combines experimental and theoretical results. Therefore, this representation deals not only with this special task but gives also a survey about the methodical approach and the state of art in Rossendorf for the general problem of determination of neutron fluences, because the developed methods are generally applicable and not limited to the special problem of neutron embrittlement. Different  problems with respect of neutron fluences exist also in Germany.
The calculation of fluences is based on an accurate description of the history of the reactor for all irradiation periods, i.e. the time and space dependence of burnup, power and fisson sources. This information was given for a time and space grid of all fuel elements. 
For the calculation of the fluences were not used time dependent fluxes, but at first  integral sources of fission neutrons are calculated for different fissionable isotopes. Using these given integral source distributions the fluences were calculated and the results from the different fissionable source were composed. For the improvement of the comparison between experimental and theoretical results a special method was used calculating special integral sources for the given detector, because each detector according to its decay notes another integral source resp. flux distribution, which has to be theoretically corrected. 
The basis of all transport calculations was the Monte Carlo method in a special problem adjusted kind.  Special procedures were developed and successfully applicated for the reduction of statistical errors. Therefore, also for single specimens results with small statistical errors were obtained. It is remarkable that this accurate method which allows a realistic 3-dimensional description of the system reactor-surroundings could be applied with reasonable calculation times for the great number of needed calculations.]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-355-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:2552-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Guttek, B.]]></dc:creator>
<dc:creator><![CDATA[Stechemesser, H.]]></dc:creator>
<dc:creator><![CDATA[Lielausis, O.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2552-1</dc:identifier>
<dc:title><![CDATA[Investigation of liquid metal two phase flow characteristics by means of local resistivity probes and X-ray screening technique]]></dc:title>
<dc:source><![CDATA[International Workshop on Measuring Techniques for Liquid Metal Flows (MTLM), Dresden, October 11-13, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[In many technologies such as the refinement of metallic melts the injection of gas bubbles is used to drive some liquid motion, enhance transport processes or to control the rate of chemical reactions. The resulting flow structure strongly depends on two phase flow parameters such as bubble size, bubble distribution or the local void fraction. Magnetic fields can be used to control the characteristics of a liquid metal bubbly flow. 
We present experimental investigations of the bubble formation in heavy liquid metals as well as the influence of external magnetic fields on the turbulent dispersion of gas bubbles and the slip ratio in liquid metal bubbly flows, respectively.

a) Bubble formation
If gas bubbles are injected into a liquid metal characterised by a large surface tension one should be care to get a good wetting between the fluid and the surface of the gas injector. Otherwise, the gas would try to spread out along this interface to form gas layers. A control of the bubble size and formation rate becomes difficult. The comparison between experiment and theoretical models describing bubble formation processes requires an ideal wetted gas injector. 
The bubble formation in mercury and the eutectic alloy InGaSn has been studied by means of several methods of gas injection, for instance through single orifices or injectors made from sintered metals with a mean porosity of a few microns. X-ray measurements have been used to directly observe the resulting gas bubbles rising in the liquid metal. In the case of an single orifce the influence of electromagnetic forces on the bubble frequency has been demonstrated. 

b) Turbulent bubble dispersion, slip ratio
The transport properties of small argon bubbles have been studied in turbulent upwards channel flows of sodium and mercury. The bubbles were injected by a single orifice located in the centre of the channel cross section. After a distinct distance the local void fraction and the bubble velocity has been measured by means of electrical resistivity probes. The flow has been exposed to external magnetic fields directed transverse or longitudinal to the mean flow direction. 
We will present and discuss measuring results showing the effect of the magnetic field strength and direction on the horizontal gas distribution and the ratio between gas and liquid velocity. ]]></dc:description>
<dc:subject><![CDATA[two-phase flow]]></dc:subject>
<dc:subject><![CDATA[bubbly regime]]></dc:subject>
<dc:subject><![CDATA[liquid metals]]></dc:subject>
<dc:subject><![CDATA[void fraction measurements]]></dc:subject>
<dc:subject><![CDATA[electric resistivity probe]]></dc:subject>
<dc:subject><![CDATA[X-ray imaging]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2552-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2553-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2553-1</dc:identifier>
<dc:title><![CDATA[Rossendorfer Beamline an der ESRF]]></dc:title>
<dc:source><![CDATA[Phys. Bl. 54 (1998) Nr. 9, 785]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2553-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:2554-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Schell, N.]]></dc:creator>
<dc:creator><![CDATA[Funke, H.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2554-1</dc:identifier>
<dc:title><![CDATA[ROBL (German Beamline) on BM20: Structural and radiochemical investigations]]></dc:title>
<dc:source><![CDATA[ESRF- Newsletter 30 (1998) 45]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:14453-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bürger, D.]]></dc:creator>
<dc:creator><![CDATA[Seeger, M.]]></dc:creator>
<dc:creator><![CDATA[Zhou, S.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Helm, M.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14453-1</dc:identifier>
<dc:title><![CDATA[Thermodynamical limits of diluted (magnetic) semiconductors]]></dc:title>
<dc:source><![CDATA[30th International Conference on the Physics of Semiconductors (ICPS 2010), 25.-30.07.2010, Seoul, Südkorea]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The incorporation of transition metal dopants in semiconductors above their solubility limit is the main challenge for the fabrication of diluted magnetic semiconductors. Dietl et al. have predicted the Curie temperature of different p-type conducting semiconductors alloyed with 5 at. % Mn [1]. This work motivated experimental efforts focused on the fabrication of highly diluted magnetic semiconductors. Unfortunately, such highly diluted magnetic semiconductors are metastable alloys and try to reach their thermodynamical equilibrium by the diffusion of the incorporated magnetic dopants leading to spinodal decomposition and secondary phase formation. There exist classical models which describe the kinetics of phase transitions and secondary phase formation for large clusters consisting of 100, 1000 or more atoms. However, electronic properties like carrier concentration strongly depend on the fraction of unclustered dopant atoms. Especially, in diluted magnetic semiconductors the formation of such clusters has to be prevented and growth techniques far from thermodynamical equilibrium are necessary.
Besides the LT-MBE process, the magnetic dopant implantation followed by pulsed laser annealing (PLA) appears to be a promising route for the fabrication of ferromagnetic semiconductors. The fast temperature quenching during PLA suppresses the diffusion of magnetic dopant atoms, i.e. diffusion via random hopping of these dopants is frozen and metastable diluted magnetic semiconductors are formed. 
In this contribution we present the results from combined random-walk simulations and heat-flow calculations to describe the initial cluster formation for different magnetic semiconductors being characterized by a large variation of diffusion coefficients of the magnetic dopants. Under the assumption that the de-clustering probability of neighbouring dopants is lower than the clustering probability, we can explain the successful fabrication of GaAs:Mn and the impossibility to fabricate diluted ferromagnetic Si:Mn with LT-MBE or Mn implantation followed by PLA. Especially, our modelling approach can be used to estimate first clustering events during the re-crystallization after PLA. Within this picture, we conclude that for the preparation of diluted ferromagnetic semiconductors the basic diffusion parameters and the room temperature solubility of the magnetic dopants are reasonable parameters to estimate the chance for a successful preparation of different kinds of diluted systems.
[1] T. Dietl et al. Science 287 1019 (2000)]]></dc:description>
<dc:subject><![CDATA[ferromagnetic semiconductors]]></dc:subject>
<dc:subject><![CDATA[pulsed laser annealing]]></dc:subject>
<dc:subject><![CDATA[metastable]]></dc:subject>
<dc:subject><![CDATA[manganese]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<header>
<identifier>HZDR:PUBLDB:14531-2</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Massarczyk, R.]]></dc:creator>
<dc:creator><![CDATA[Birgersson, E.]]></dc:creator>
<dc:creator><![CDATA[Schramm, G.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Belgya, T.]]></dc:creator>
<dc:creator><![CDATA[Beyer, R.]]></dc:creator>
<dc:creator><![CDATA[Grosse, E.]]></dc:creator>
<dc:creator><![CDATA[Hannaske, R.]]></dc:creator>
<dc:creator><![CDATA[Junghans, A. R.]]></dc:creator>
<dc:creator><![CDATA[Matic, A.]]></dc:creator>
<dc:creator><![CDATA[Szentimiklosi, L.]]></dc:creator>
<dc:creator><![CDATA[Weil, J.]]></dc:creator>
<dc:creator><![CDATA[Wagner, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14531-2</dc:identifier>
<dc:title><![CDATA[Photon strength function deduced from photon scattering and neutron capture]]></dc:title>
<dc:source><![CDATA[EFNUDAT Users and Collaboration Workshop "Measurement and Models of Nuclear Reactions", 25.-27.05.2010, Paris, France]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The dipole strength function of 78Se and 196Pt are investigated by two different experimental methods, capture of cold neutrons in 77Se and 195Pt, and photon scattering experiments on 78Se and 196Pt. Considering the different ways of excitation, the strength function deduced from the results are expected to agree. The report shows the status of the data analysis and presents first preliminary results.]]></dc:description>
<dc:subject><![CDATA[Nuclear structure]]></dc:subject>
<dc:subject><![CDATA[gamma-ray spectroscopy]]></dc:subject>
<dc:subject><![CDATA[gamma-ray strength functions]]></dc:subject>
<dc:subject><![CDATA[neutron capture]]></dc:subject>
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<identifier>HZDR:PUBLDB:14531-1</identifier>
<datestamp>2025-06-05</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Massarczyk, R.]]></dc:creator>
<dc:creator><![CDATA[Birgersson, E.]]></dc:creator>
<dc:creator><![CDATA[Schramm, G.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Belgya, T.]]></dc:creator>
<dc:creator><![CDATA[Beyer, R.]]></dc:creator>
<dc:creator><![CDATA[Grosse, E.]]></dc:creator>
<dc:creator><![CDATA[Hannaske, R.]]></dc:creator>
<dc:creator><![CDATA[Junghans, A. R.]]></dc:creator>
<dc:creator><![CDATA[Matic, A.]]></dc:creator>
<dc:creator><![CDATA[Szentimiklosi, L.]]></dc:creator>
<dc:creator><![CDATA[Weil, J.]]></dc:creator>
<dc:creator><![CDATA[Wagner, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14531-1</dc:identifier>
<dc:title><![CDATA[Photon strength function deduced from photon scattering and neutron capture]]></dc:title>
<dc:source><![CDATA[EFNUDAT Users and Collaboration Workshop "Measurement and Models of Nuclear Reactions", 25.-27.05.2010, Paris, France<br>European Physics Journal Web Conferences 8 (2010), 07008]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The dipole strength function of 78Se and 196Pt are investigated by two different experimental methods, capture of cold neutrons in 77Se and 195Pt, and photon scattering experiments on 78Se and 196Pt. Considering the different ways of excitation, the strength function deduced from the results are expected to agree. The report shows the status of the data analysis and presents first preliminary results.]]></dc:description>
<dc:subject><![CDATA[Nuclear structure]]></dc:subject>
<dc:subject><![CDATA[gamma-ray spectroscopy]]></dc:subject>
<dc:subject><![CDATA[gamma-ray strength functions]]></dc:subject>
<dc:subject><![CDATA[neutron capture]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14531-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:1725-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Nitzsche, P.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Goerigk, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1725-1</dc:identifier>
<dc:title><![CDATA[ASAXS-Investigation of the Structural Changes in Laboratory Heats of the Reactor Pressure Vessel Steel 15 Kh2MFA after Irradation in a Nuclear Power Plant]]></dc:title>
<dc:source><![CDATA[DESY, Jahresbericht 1995, HASYLAB am Deutschen Elektronen-Synchrotron, Annual Report II, Jan. 1996, S. 833]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1725-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2326-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kögler, R.]]></dc:creator>
<dc:creator><![CDATA[Kaschny, J. R.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Werner, P.]]></dc:creator>
<dc:creator><![CDATA[Danilin, A. B.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2326-1</dc:identifier>
<dc:title><![CDATA[Metal gettering by defective regions in carbon-implanted silicon]]></dc:title>
<dc:source><![CDATA[Solid State Phenomena 57/58 (1997) 63]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2326-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2328-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kruijer, S.]]></dc:creator>
<dc:creator><![CDATA[Keune, W.]]></dc:creator>
<dc:creator><![CDATA[Dobler, M.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2328-1</dc:identifier>
<dc:title><![CDATA[Depth analysis of phase formation in Si after high-dose Fe ion implantation by depth-selective conversion-electron Mössbauer spectroscopy]]></dc:title>
<dc:source><![CDATA[Appl. Phys. Lett. 70 (1997) 2696]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2328-1</dc:relation>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2556-1</identifier>
<datestamp>2025-12-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krepper, E.]]></dc:creator>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Aszódi, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2556-1</dc:identifier>
<dc:title><![CDATA[Numerical Simulation of the Emergency Condenser of the SWR1000]]></dc:title>
<dc:source><![CDATA[Kerntechnik 64 (1999) 5-6, p. 243-252]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The SWR1000 is a new innovative boiling water reactor concept, which is developed by Siemens AG. This concept is characterized in particular by passive safety systems (e.g. four emergency condensers, four building condensers, eight passive pressure pulse transmitters, six gravity-driven core flooding lines). In the framework of BWR Physics and Thermohydraulic Complementary Action (BWR-CA) to the EU BWR R&D Cluster emergency condenser tests were performed by Forschungszentrum Jülich at the NOKO test facility. In this paper post test calculations with ATHLET are presented, which aim at the determination of the removable power of the emergency condenser and its operation mode. The 1D thermal-hydraulic code ATHLET was extended by the module KONWAR for the calculation of the heat transfer coefficient during condensation in horizontal tubes. In addition, results of CFD-calculations using the code CFX-4 are presented, which investigate the natural convection during the heat up process at the secondary side of the NOKO test facility. ]]></dc:description>
<dc:subject><![CDATA[BWR]]></dc:subject>
<dc:subject><![CDATA[emergency condenser]]></dc:subject>
<dc:subject><![CDATA[condensation inside horizontal tubes]]></dc:subject>
<dc:subject><![CDATA[natural convection]]></dc:subject>
<dc:subject><![CDATA[CFD]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.13182/NSE00-A2139]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2556-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:2557-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krüssenberg, A.-K.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2557-1</dc:identifier>
<dc:title><![CDATA[A New Criterion for the Bubble Slug Transition in Vertical Tubes]]></dc:title>
<dc:source><![CDATA[Kerntechnik 65/1 (2000) 7-13]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Vertical two-phase flow is normally classified into the four basic flow regimes bubble, slug, churn and annular flow. The transition between the different flow regimes does not occur suddenly and many extensions of this classification can be found in literature. For the prediction of flow patterns empirical and theoretical flow pattern maps have been developed. 
A new criterion is presented for the transition between bubble and slug flow which is based on local instantaneous conductivity measurements with a wire mesh sensor (1 kHz that means 1000 frames per second, 242 measuring points in a tube cross section area). The high resolution allows the calculation of particle size distributions. 
The transition from homogeneous bubble flow to heterogeneous bubble flow is indicated by the appearance of a bimodal bubble size distribution. If the equivalent bubble diameter exceeds the tube diameter the transition from bubble to slug flow occurs. The new criterion is compared with different empirical (Govier & Aziz, Weisman & Kang) and theoretical flow maps (Taitel, Bornea & Dukler, Ishii & Mishima) and shows a good agreement. 
]]></dc:description>
<dc:subject><![CDATA[Bubble Size Distribution]]></dc:subject>
<dc:subject><![CDATA[Bubble Slug Flow Transition Criteria]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2557-1</dc:relation>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:2557-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Krüssenberg, A.-K.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2557-2</dc:identifier>
<dc:title><![CDATA[A New Criterion for the Bubble Slug Transition in Vertical Tubes]]></dc:title>
<dc:source><![CDATA[NURETH-9, San Francisco, California, USA, October 3-8, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Vertical two-phase flow is normally classified into the four basic flow regimes bubble, slug, churn and annular flow. The transition between the different flow regimes does not occur suddenly and many extensions of this classification can be found in literature. For the prediction of flow patterns empirical and theoretical flow pattern maps have been developed. 
A new criterion is presented for the transition between bubble and slug flow which is based on local instantaneous conductivity measurements with a wire mesh sensor (1 kHz that means 1000 frames per second, 242 measuring points in a tube cross section area). The high resolution allows the calculation of particle size distributions. 
The transition from homogeneous bubble flow to heterogeneous bubble flow is indicated by the appearance of a bimodal bubble size distribution. If the equivalent bubble diameter exceeds the tube diameter the transition from bubble to slug flow occurs. The new criterion is compared with different empirical (Govier & Aziz, Weisman & Kang) and theoretical flow maps (Taitel, Bornea & Dukler, Ishii & Mishima) and shows a good agreement. 
]]></dc:description>
<dc:subject><![CDATA[Bubble Size Distribution]]></dc:subject>
<dc:subject><![CDATA[Bubble Slug Flow Transition Criteria]]></dc:subject>
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<identifier>HZDR:PUBLDB:2651-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Bonsdorf, G.]]></dc:creator>
<dc:creator><![CDATA[Denecke, M. A.]]></dc:creator>
<dc:creator><![CDATA[Schäfer, K.]]></dc:creator>
<dc:creator><![CDATA[Christen, S.]]></dc:creator>
<dc:creator><![CDATA[Langbein, H.]]></dc:creator>
<dc:creator><![CDATA[Gunßer, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2651-1</dc:identifier>
<dc:title><![CDATA[X-Ray Absorption Spectroscopic and Mössbauer Studies of Redox and Cation-Ordering Processes in Manganese Ferrite]]></dc:title>
<dc:source><![CDATA[HASYLAB-Annual Report 1996 I, 834 (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2652-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Dilworth, J. R.]]></dc:creator>
<dc:creator><![CDATA[Hübener, R.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2652-1</dc:identifier>
<dc:title><![CDATA[Synthesis and Characterization of Bis(tetrabutylammonium)bis(isotrithionedithiolato-S,S')-nitrido technetate(V), (Bu<SUB>4</SUB>N)<SUB>2</SUB>[TcN(dmit)<SUB>2</SUB>]]]></dc:title>
<dc:source><![CDATA[Zeitschrift für anorganische und allgemeine Chemie 623, 880 (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Dressler, R.]]></dc:creator>
<dc:creator><![CDATA[Schumann, D.]]></dc:creator>
<dc:creator><![CDATA[Taut, S.]]></dc:creator>
<dc:creator><![CDATA[Fischer, S.]]></dc:creator>
<dc:creator><![CDATA[Binder, R.]]></dc:creator>
<dc:creator><![CDATA[Yakushev, A. B.]]></dc:creator>
<dc:creator><![CDATA[Buklanov, G.]]></dc:creator>
<dc:creator><![CDATA[Dinh, T. L.]]></dc:creator>
<dc:creator><![CDATA[Domanov, V. P.]]></dc:creator>
<dc:creator><![CDATA[Szeglowski, Z.]]></dc:creator>
<dc:creator><![CDATA[Kubica, B.]]></dc:creator>
<dc:creator><![CDATA[Guseva, L. I.]]></dc:creator>
<dc:creator><![CDATA[Thikhomirova, G. S.]]></dc:creator>
<dc:creator><![CDATA[Gäggeler, H. W.]]></dc:creator>
<dc:creator><![CDATA[Bruchertseifer, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2653-1</dc:identifier>
<dc:title><![CDATA[First Observation of -Ray Emission Assigned to the Decay of <SUP>164</SUP>W]]></dc:title>
<dc:source><![CDATA[Radiochimica Acta 77, 241-244 (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Eichler, B.]]></dc:creator>
<dc:creator><![CDATA[Hübener, S.]]></dc:creator>
<dc:creator><![CDATA[Erdmann, N.]]></dc:creator>
<dc:creator><![CDATA[Eberhardt, K.]]></dc:creator>
<dc:creator><![CDATA[Funk, H.]]></dc:creator>
<dc:creator><![CDATA[Herrmann, G.]]></dc:creator>
<dc:creator><![CDATA[Köhler, S.]]></dc:creator>
<dc:creator><![CDATA[Trautmann, N.]]></dc:creator>
<dc:creator><![CDATA[Passler, G.]]></dc:creator>
<dc:creator><![CDATA[Urban, F.-J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2655-1</dc:identifier>
<dc:title><![CDATA[An Atomic Beam Source for Actinide Elements: Concept and Realization]]></dc:title>
<dc:source><![CDATA[Radiochimica Acta 79, 221-233 (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:1618-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Vorst, K.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Neumann, J.]]></dc:creator>
<dc:creator><![CDATA[Schlüter, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1618-1</dc:identifier>
<dc:title><![CDATA[Fault Diagnostics in Chemical Semibatch Reactors Using Neural Networks]]></dc:title>
<dc:source><![CDATA[Proc. of the 5th European Congress on Intelligent Techniques and Soft Computing EUFIT 97, Aachen, Germany, September 8 - 11, 1997, pp. 1704 - 1708]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[This paper presents a neural-network approach to early identifying dangerous states in chemical semibatch reactors. Data sets which were supplied both from a process simulator and from measurements in a laboratory reactor were used to train and test  neural networks and a fuzzy pattern classifier for different normal and faulty states. Three-layer perceptron networks were found to be best suited for classifying different normal and abnormal process states. Even multiple fault states can be recognized by the perceptron network correctly.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1618-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Vorst, K.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Neumann, J.]]></dc:creator>
<dc:creator><![CDATA[Schlüter, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1618-7</dc:identifier>
<dc:title><![CDATA[Fault Diagnostics in Chemical Semibatch Reactors Using Neural Networks]]></dc:title>
<dc:source><![CDATA[Proc. of the 5th European Congress on Intelligent Techniques and Soft Computing EUFIT 97, Aachen, Germany, September 8 - 11, 1997, pp. 1704 - 1708]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[This paper presents a neural-network approach to early identifying dangerous states in chemical semibatch reactors. Data sets which were supplied both from a process simulator and from measurements in a laboratory reactor were used to train and test  neural networks and a fuzzy pattern classifier for different normal and faulty states. Three-layer perceptron networks were found to be best suited for classifying different normal and abnormal process states. Even multiple fault states can be recognized by the perceptron network correctly.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2657-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Tefera, N.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Neumann, J.]]></dc:creator>
<dc:creator><![CDATA[Deerberg, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2657-1</dc:identifier>
<dc:title><![CDATA[Identifikation und Bewertung prozeßrelevanter Zustände in Semibatch-Reaktoren mit neuronalen Netzen]]></dc:title>
<dc:source><![CDATA[DECHEMA-Jahrestagungen '99, Jahrestagung Sicherheitstechnik, 27. - 29. April 1999, Wiesbaden, Band II, S. 143]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Die Anwendungsmöglichkeiten neuronaler Netze zur Operatorberatung bei der Prozeßführung exothermer Reaktionen werden am Beispiel einer säurekatalysierten Veresterung gezeigt. Um auch die potentielle Gefahr der verschiedenen Fehlerzustände bewerten zu können, wurden separate Perceptron-Netze zur Gefahrenbewertung und zur Fehleridentifikation angewendet. Die Ergebnisse zeigten, daß durch geeignete Trainingsdaten und Merkmalsextraktion aus den Prozeßdaten die Perceptron-Netze auch Fehler in Prozeßabläufen erkannten und richtig bewerteten, deren Daten nicht zum Netztraining benutzt wurden.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2657-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Tefera, N.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Neumann, J.]]></dc:creator>
<dc:creator><![CDATA[Deerberg, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2657-7</dc:identifier>
<dc:title><![CDATA[Identifikation und Bewertung prozeßrelevanter Zustände in Semibatch-Reaktoren mit neuronalen Netzen]]></dc:title>
<dc:source><![CDATA[DECHEMA-Jahrestagungen '99, Jahrestagung Sicherheitstechnik, 27. - 29. April 1999, Wiesbaden, Band II, S. 143]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Die Anwendungsmöglichkeiten neuronaler Netze zur Operatorberatung bei der Prozeßführung exothermer Reaktionen werden am Beispiel einer säurekatalysierten Veresterung gezeigt. Um auch die potentielle Gefahr der verschiedenen Fehlerzustände bewerten zu können, wurden separate Perceptron-Netze zur Gefahrenbewertung und zur Fehleridentifikation angewendet. Die Ergebnisse zeigten, daß durch geeignete Trainingsdaten und Merkmalsextraktion aus den Prozeßdaten die Perceptron-Netze auch Fehler in Prozeßabläufen erkannten und richtig bewerteten, deren Daten nicht zum Netztraining benutzt wurden.]]></dc:description>
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<identifier>HZDR:PUBLDB:1219-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Dohrmann, F.]]></dc:creator>
<dc:creator><![CDATA[Bethge, K.]]></dc:creator>
<dc:creator><![CDATA[Enghardt, W.]]></dc:creator>
<dc:creator><![CDATA[Fateev, O.]]></dc:creator>
<dc:creator><![CDATA[Garabatos, C.]]></dc:creator>
<dc:creator><![CDATA[Grosse, E.]]></dc:creator>
<dc:creator><![CDATA[Müntz, C.]]></dc:creator>
<dc:creator><![CDATA[Karig, W.]]></dc:creator>
<dc:creator><![CDATA[Koenig, W.]]></dc:creator>
<dc:creator><![CDATA[Smykov, L.]]></dc:creator>
<dc:creator><![CDATA[Sobiella, M.]]></dc:creator>
<dc:creator><![CDATA[Steigerwald, A.]]></dc:creator>
<dc:creator><![CDATA[Stelzer, H.]]></dc:creator>
<dc:creator><![CDATA[Stroth, J.]]></dc:creator>
<dc:creator><![CDATA[Wüstenfeld, J.]]></dc:creator>
<dc:creator><![CDATA[Zanevsky, Y.]]></dc:creator>
<dc:creator><![CDATA[Zentek, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1219-1</dc:identifier>
<dc:title><![CDATA[A Low-Mass Drift Chamber System for the HADES-Spectrometer]]></dc:title>
<dc:source><![CDATA[Acta Physica Polonica B No 11, Vol. 29 (1998), 3189-3193]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[A new high resolution (D M/M < 1 %) and high acceptance (45 %) di-electron spectrometer (HADES) has been designed to investigate in-medium properties of hadrons. For tracking of all charged particles (in particular with sufficient resolution for electrons) a system of 24 low-mass drift chambers (Helium based counting gas and Aluminum field and cathode wires), arranged in four tracking planes, is used.
Design aspects of the chambers are reported. Results of performance optimization using various prototype detectors are discussed, including results of an ageing test. Stable operation in the high-multiplicity environment of heavy ion collisions, and a spatial resolution of 70 mm (s) over 80 % of a cell have been demonstrated in two beam experiments.]]></dc:description>
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<identifier>HZDR:PUBLDB:505-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-505-2</dc:identifier>
<dc:title><![CDATA[A Neural Network Approach for Acoustic Leak Monitoring at Pressurized Plants with Complicated Topology]]></dc:title>
<dc:source><![CDATA[Preprints of the IFAC Workshop on On-line Fault Detection and Supervision in the Chemical Process Industries, Newcastle (England), June 12 - 13th 1995, pp. 98 - 102]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Gross, C. J.]]></dc:creator>
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<dc:creator><![CDATA[Kabadiyski, M. K.]]></dc:creator>
<dc:creator><![CDATA[Roth, H. A.]]></dc:creator>
<dc:creator><![CDATA[Rudolph, D.]]></dc:creator>
<dc:creator><![CDATA[Simpson, J.]]></dc:creator>
<dc:creator><![CDATA[Skeppstedt, Ö.]]></dc:creator>
<dc:creator><![CDATA[Varley, B. J.]]></dc:creator>
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<dc:identifier>https://www.hzdr.de/publications/Publ-597-1</dc:identifier>
<dc:title><![CDATA[A new type of band crossing at large deformation]]></dc:title>
<dc:source><![CDATA[Physics Letters B 374 (1996) pp. 277-282]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Buchanan, B. B.]]></dc:creator>
<dc:creator><![CDATA[Bucher, J. J.]]></dc:creator>
<dc:creator><![CDATA[Carlson, D. E.]]></dc:creator>
<dc:creator><![CDATA[Edelstein, N. M.]]></dc:creator>
<dc:creator><![CDATA[Hudson, E. A.]]></dc:creator>
<dc:creator><![CDATA[Kaltsoyannis, N.]]></dc:creator>
<dc:creator><![CDATA[Leighton, T.]]></dc:creator>
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<dc:creator><![CDATA[Shuh, D. K.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
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<dc:creator><![CDATA[Woicik, J.]]></dc:creator>
<dc:creator><![CDATA[Yang, W.-S.]]></dc:creator>
<dc:creator><![CDATA[Yee, A.]]></dc:creator>
<dc:creator><![CDATA[Yee, B. C.]]></dc:creator>
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<dc:title><![CDATA[A XANES and EXAFS Investigation of the Speciation of Selenite following Bacterial Metabolization]]></dc:title>
<dc:source><![CDATA[Inorganic Chemistry 34 (1995) pp. 1617]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2663-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Mack, J.]]></dc:creator>
<dc:creator><![CDATA[Ortner, K.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Parish, R. V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2663-1</dc:identifier>
<dc:title><![CDATA[Gold(III)-Komplexe mit 2-(N,N-Dimethylaminomethyl)phenyl (damp<SUP>-</SUP>). Darstellung und Kristall-strukturen von [Au(damp-C,N)Cl<SUB>2</SUB>], [Au(damp-C,N)(OOCCH<SUB>3</SUB>)<SUB>2</SUB>] und [Au(damp-C,N)(mnt)] (mnt<SUP>2-</SUP> = 1,2-Dicyanoethene-1,2-dithiolat)]]></dc:title>
<dc:source><![CDATA[Zeitschrift für anorganische und allgemeine Chemie. 623, 873 (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2693-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2693-1</dc:identifier>
<dc:title><![CDATA[Koordinierte Nitridoliganden - Lewis-Säuren für den Komplexchemiker]]></dc:title>
<dc:source><![CDATA[Universität Potsdam, Institut für Anorganische Chemie, Potsdam, Germany, 06.11.1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2694-1</dc:identifier>
<dc:title><![CDATA[Technetium - ein künstliches Element erobert das Krankenhaus]]></dc:title>
<dc:source><![CDATA[Johannes-Gutenberg-Universität Mainz, Institut für Kernchemie
Mainz, Germany, 26.11.1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Abram, U.]]></dc:creator>
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<dc:title><![CDATA[Nitrido Ligands as Bridges between Main Group and Transition Metals]]></dc:title>
<dc:source><![CDATA[St. Annes Conference 1997 Oxford, Oxford, England, 17.12.1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Allen, P. G.]]></dc:creator>
<dc:creator><![CDATA[Shuh, D. K.]]></dc:creator>
<dc:creator><![CDATA[Bucher, J. J.]]></dc:creator>
<dc:creator><![CDATA[Edelstein, N. M.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2696-1</dc:identifier>
<dc:title><![CDATA[An XAFS Investigation of the Formation of Actinide Aquo and Chloro Complexes]]></dc:title>
<dc:source><![CDATA[214th American Chemical Society National Meeting, Las Vegas, NV, USA, 07.-11.9.1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2697-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Arnold, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2697-1</dc:identifier>
<dc:title><![CDATA[Identification of an uranium surface species sorbed onto ferrihydrite by TRLFS (Time-resolved Laser-induced Fluorescence Spectroscopy)]]></dc:title>
<dc:source><![CDATA[Workshop: The Münster workshop on Mineral Surface Science, Münster, Germany, 02.-04.04.1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:961-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Albe, K.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-961-1</dc:identifier>
<dc:title><![CDATA[Modelling of boron nitride: atomic scale simulations on thin film growth]]></dc:title>
<dc:source><![CDATA[Computational Materials Science 10 (1998) 111]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Molecular-dynamics simulations on ion-beam deposition
of boron nitride are presented. A realistic Tersoff-like potential energy
function for boron nitride, which was specially fitted to ab initio-data,
has been used. The impact of energetic boron and nitrogen atoms on a c-BN
target is simulated with energies ranging from 10 to 600 eV. The structural
analysis of the grown films shows, that a loose, dominantly sp<SUP>2</SUP>-bonded
structure arises at high ion flux. In no case the formation of a sp<SUP>3</SUP>-bonded
phase is observed, but the obtained films partially reveal textured basal
planes as found in experiment. Two different growth regimes are identified
for ion energies above and below 100 eV.]]></dc:description>
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<identifier>HZDR:PUBLDB:961-2</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Albe, K.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-961-2</dc:identifier>
<dc:title><![CDATA[Modelling of boron nitride: atomic scale simulations on thin film growth]]></dc:title>
<dc:source><![CDATA[E-MRS Spring Meeting, Symp. D: Computational Modeling of Issues in Materials Science, Strasbourg, France, June 16 - 20, 1997 (invited lecture)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Molecular-dynamics simulations on ion-beam deposition
of boron nitride are presented. A realistic Tersoff-like potential energy
function for boron nitride, which was specially fitted to ab initio-data,
has been used. The impact of energetic boron and nitrogen atoms on a c-BN
target is simulated with energies ranging from 10 to 600 eV. The structural
analysis of the grown films shows, that a loose, dominantly sp<SUP>2</SUP>-bonded
structure arises at high ion flux. In no case the formation of a sp<SUP>3</SUP>-bonded
phase is observed, but the obtained films partially reveal textured basal
planes as found in experiment. Two different growth regimes are identified
for ion energies above and below 100 eV.]]></dc:description>
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<dc:title><![CDATA[Mikrokapillare mit integrierten chemischen Mikrosensoren und Verfahren zu ihrer Herstellung]]></dc:title>
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<dc:description><![CDATA[Mit der Erfindung wird die Mikrokapillare ( 1 ) so konfiguriert, daß die in die Mikrokapillare integrierten chemischen Mikrosensoren, d.h. deren empfindliche Membrangebiete ( 3 ) von dem zu analysierenden Meßfluid zwangsumspült und damit zwangsbenetzt werden. Diese Zwangsumspülung wird konstruktiv durch Einführung sogenannter Kanalstopper ( 2 ) realisiert, welche die Entstehung von Totvolumina minimieren. 
Die erfindungsgemäße Mikrokapillare mit integrierten chemischen Mikrosensoren bietet dabei den Vorteil, daß unter Verwendung der Kanalstopper das Meßfluid auf optimale Weise zum Auftreffen auf das sensitive Gebiet des Sensors geführt wird, wodurch ein verbessertes Ansprechen im dynamischen Betrieb erreicht wird. 
Zum Aufbau der Mikrokapillare wird eine anisotrope Silicium-Strukturierungstechnologie angewendet, die je nach Anwendungsfall die geometrisch ideale Gestaltung der Kapillare und des Kanalstoppers im Bereich der chemisch sensitiven Membran zur optimalen Strömungsführung gestattet.
Durch Nutzung des Reflowlötens mit niedrig schmelzendem Lot bzw. der Verwendung kaltaushärtender Klebstoffe bei der Montage der Mikrosensoren wird eine schonende Montage  unter Vermeidung hoher Temperatur- oder Spannungsbelastungen gewährleistet und ein flexibles Auswechseln von Ausfallsensoren ermöglicht. ]]></dc:description>
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Die erfindungsgemäße Mikrokapillare mit integrierten chemischen Mikrosensoren bietet dabei den Vorteil, daß unter Verwendung der Kanalstopper das Meßfluid auf optimale Weise zum Auftreffen auf das sensitive Gebiet des Sensors geführt wird, wodurch ein verbessertes Ansprechen im dynamischen Betrieb erreicht wird. 
Zum Aufbau der Mikrokapillare wird eine anisotrope Silicium-Strukturierungstechnologie angewendet, die je nach Anwendungsfall die geometrisch ideale Gestaltung der Kapillare und des Kanalstoppers im Bereich der chemisch sensitiven Membran zur optimalen Strömungsführung gestattet.
Durch Nutzung des Reflowlötens mit niedrig schmelzendem Lot bzw. der Verwendung kaltaushärtender Klebstoffe bei der Montage der Mikrosensoren wird eine schonende Montage  unter Vermeidung hoher Temperatur- oder Spannungsbelastungen gewährleistet und ein flexibles Auswechseln von Ausfallsensoren ermöglicht. ]]></dc:description>
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<dc:description><![CDATA[Ion implantation of Ca and/or P into Ti or Ti alloys is of interest in order  to enhance mechanical properties and  biocompatibility for medical applications . With this motivation the microstructural changes of the implanted surface layer were studied. Surface near implantation of high doses of calcium results in an oxidation of the modified layer and the formation of CaO. For deeper calcium implantations, precipitation of the metastable hexagonal modification of calcium has been observed instead of the cubic equilibrium phase. Beside these new phases partial amporphization is observed. High dose implantation of phosphorus leads mainly to amorphization of the implanted layer. This hinders the reaction with oxygen during implantation and room temperature aging. High dose double implantation with P followed by Ca also leads to partial amorphization. No indication for new phases containing Ca and P is found.]]></dc:description>
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Marburg, Germany, September 9-14, 2001]]></dc:source>
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<dc:description><![CDATA[Ion implantation of Ca and/or P into Ti or Ti alloys is of interest in order  to enhance mechanical properties and  biocompatibility for medical applications . With this motivation the microstructural changes of the implanted surface layer were studied. Surface near implantation of high doses of calcium results in an oxidation of the modified layer and the formation of CaO. For deeper calcium implantations, precipitation of the metastable hexagonal modification of calcium has been observed instead of the cubic equilibrium phase. Beside these new phases partial amporphization is observed. High dose implantation of phosphorus leads mainly to amorphization of the implanted layer. This hinders the reaction with oxygen during implantation and room temperature aging. High dose double implantation with P followed by Ca also leads to partial amorphization. No indication for new phases containing Ca and P is found.]]></dc:description>
<dc:subject><![CDATA[Titanium alloys]]></dc:subject>
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Erfindungsgemäß erfolgt dies derart, daß ein (100)-p-Siliciumeinkristall  im Energiebereich von 300keV bis zu einigen MeV gestaffelt mit N+- und O+-Ionen beschossen und nachfolgend definierten Temper- und Diffusionsprozessen ausgesetzt wird. Dadurch wird eine Lagedefinition des Stapelisolators im Siliciumsubstrat, eine Lage- und Strukturdefinition innerhalb des Isolatorstapels SiO2-Si-xOxNz-Si2N3 und die ideale Ausbildung des  elektronischen Interfaces zwischen der einkristallinen (100)-p-Si-Deckschicht und dem Isolatorstapel erreicht. Nach dieser Isolatorvergrabung erfolgt in der einkristallinen Si-Deckschicht die vollständige ISFET-Präparation. Das Freilegen der chemisch empfindlichen Membran erfolgt im letzten Schritt durch simultanes anisotropes Ätzen im Full-Wafer-Prozeß, hierbei wirkt die Si3N4-Membranschicht als ideale Ätzstoppschicht, das Bauelement ist sofort einsetzbar.  
]]></dc:description>
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<dc:title><![CDATA[Flüssigmetall-Ionenquelle zur Erzeugung von Kobalt-Ionenstrahlen]]></dc:title>
<dc:source><![CDATA[DE 43 12 028 A 1]]></dc:source>
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<dc:description><![CDATA[Die Erfindung betrifft eine Flüssigmetall-Ionenquelle zur Erzeugung von Kobaltionenstrahlen, insbesondere das den Emitter benetzende Quellenmaterial einer derartigen Ionenquelle. 

Die Erfindung beinhaltet Flüssigmetall-Ionenquellen, deren Emitter mit einer definierten Legierung aus Kobalt und einem oder mehreren Elementen aus der Gruppe der Seltenen Erden als Quellenmaterial benetzt ist. Mit derart ausgestatteten Flüssigmetall-Ionenquellen ist es möglich, langzeitig einen stabilen Ionenstrom, der im ausreichendem Ma e aus Kobaltionen besteht, zu erhalten.
Die Bestandteile der Legierung im Zusammenspiel mit dem niedrigen Schmelzpunkt führen dazu, da  keine chemischen Reaktionen mit dem Emitter- und Heizermaterial auftreten. ]]></dc:description>
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<dc:title><![CDATA[Flüssigmetall-Ionenquelle zur Erzeugung von Kobalt-Ionenstrahlen]]></dc:title>
<dc:source><![CDATA[EP 0 620 582 B 1]]></dc:source>
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<dc:description><![CDATA[Die Erfindung betrifft eine Flüssigmetall-Ionenquelle zur Erzeugung von Kobaltionenstrahlen, insbesondere das den Emitter benetzende Quellenmaterial einer derartigen Ionenquelle. 

Die Erfindung beinhaltet Flüssigmetall-Ionenquellen, deren Emitter mit einer definierten Legierung aus Kobalt und einem oder mehreren Elementen aus der Gruppe der Seltenen Erden als Quellenmaterial benetzt ist. Mit derart ausgestatteten Flüssigmetall-Ionenquellen ist es möglich, langzeitig einen stabilen Ionenstrom, der im ausreichendem Ma e aus Kobaltionen besteht, zu erhalten.
Die Bestandteile der Legierung im Zusammenspiel mit dem niedrigen Schmelzpunkt führen dazu, da  keine chemischen Reaktionen mit dem Emitter- und Heizermaterial auftreten. ]]></dc:description>
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Extended calculations of the deuteron's static properties, based on the numerical solution of the Bethe-Salpeter equation,.are presented. A formalism is developed, which provides a comparative analysis of the covariant amplitudes in various representations and nonrelativistic wave functions. The magnetic and quadrupole moments of the deuteron are calculated in the Bethe-Salpeter formalism and tlie role of relativistic corrections is discussed.]]></dc:description>
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Extended calculations of the deuteron's static properties, based on the numerical solution of the Bethe-Salpeter equation,.are presented. A formalism is developed, which provides a comparative analysis of the covariant amplitudes in various representations and nonrelativistic wave functions. The magnetic and quadrupole moments of the deuteron are calculated in the Bethe-Salpeter formalism and tlie role of relativistic corrections is discussed.]]></dc:description>
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<dc:title><![CDATA[Actinides in the Environment]]></dc:title>
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<dc:title><![CDATA[Basic Research for Environmental Remediation: Speciation and Complexation of Aqueous Uranium]]></dc:title>
<dc:source><![CDATA[LLNL, Glenn T. Seaborg Institute tor Transactinium Science, Livermore, CA, USA, January 1997, invited]]></dc:source>
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<dc:title><![CDATA[lnterdisciplinary Nuclear Chemistry: Applications to Actinide Environmental Chemistry and Studies of the Chemical Properties of the Heaviest Elements]]></dc:title>
<dc:source><![CDATA[University of California Berkeley, Chemistry Department, Berkeley, CA, USA, January 1997, invited]]></dc:source>
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<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
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<dc:title><![CDATA[Melanoidine als definierte Huminsäureanaloga für Komplexbildungsuntersuchungen]]></dc:title>
<dc:source><![CDATA[Workshop:Geochemische Modellierung radiotoxische und chemisch-toxische Stoffe in natürlichen aquatischen Systemen, Forschungszentrum Karlsruhe, Institut für Nukleare Entsorgungstechnik, Karlsruhe, Germany, 23.-24.04.1997]]></dc:source>
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<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
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<dc:title><![CDATA[Erste Stabilitätsuntersuchungen an synthetischen und natürlichen Huminsäuren]]></dc:title>
<dc:source><![CDATA[Workshop zum Forschungsvorhaben: Einfluß von Huminstoffen auf das Migrationsverhalten radioaktiver und nichtradioaktiver Schadstoffe unter naturnahen Bedingungen, Saarbrücken, Germany, 10.07.1997]]></dc:source>
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<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2719-1</dc:identifier>
<dc:title><![CDATA[Fortschrittsbericht über die Synthese von Huminsäuren und deren Komplexbildungsverhalten gegenüber Uranylionen]]></dc:title>
<dc:source><![CDATA[Workshop zum Forschungsvorhaben: Einfluß von Huminstoffen auf das Migrationsverhalten
radioaktiver und nichtradioaktiver Schadstoffe unter naturnahen Bedingungen, Saarbrücken, Germany, 10.07.1997]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:creator><![CDATA[Strecker, N.]]></dc:creator>
<dc:creator><![CDATA[Feudel, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2721-1</dc:identifier>
<dc:title><![CDATA[Atomistic simulation of ion implantation into real 2d structures]]></dc:title>
<dc:source><![CDATA[Int. Workshop on Challenges in Predictive Process Simulation (ChiPPS'97), Wandlitz, Germany, Aug. 17 - 20, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Paul, E. S.]]></dc:creator>
<dc:creator><![CDATA[Fossan, D. B.]]></dc:creator>
<dc:creator><![CDATA[Hauschild, K.]]></dc:creator>
<dc:creator><![CDATA[Hibbert, I. M.]]></dc:creator>
<dc:creator><![CDATA[Nolan, P. J.]]></dc:creator>
<dc:creator><![CDATA[Schnare, H.]]></dc:creator>
<dc:creator><![CDATA[Sears, J. M.]]></dc:creator>
<dc:creator><![CDATA[Thorslund, I.]]></dc:creator>
<dc:creator><![CDATA[Wadsworth, R.]]></dc:creator>
<dc:creator><![CDATA[Wilson, A. N.]]></dc:creator>
<dc:creator><![CDATA[Wilson, J. N.]]></dc:creator>
<dc:creator><![CDATA[Ragnarsson, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2885-1</dc:identifier>
<dc:title><![CDATA[High-Fold γ-ray spectroscopy of <sup>117</sup>I: Coexistence of Collective and Noncollective Structures]]></dc:title>
<dc:source><![CDATA[Phys. Rev. C 59 (1999) 1984-1998]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[High spin states have been populated in <sup>117</sup><sub> 53</sub>I via the <sup>90</sup>Zr(<sup>31</sup>P,2p2n) reaction at 150 MeV, using the EUROGAM II γ-ray spectrometer to record high-fold γ-ray coincidences. A quadruples γ-ray analysis (γ<sup>4</sup>) has been used to extend the known level scheme. In addition to several aligned noncollective states, a new high-spin band showing  characteristics of smooth termination has been established at and linked into the low-spin level scheme. Its structure has been inferred through comparison with cranked Nilsson-Strutinsky calculations.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2722-1</dc:identifier>
<dc:title><![CDATA[Actinide Chemistry at the Dedicated Rossendorf Beamline (ROBL) at the ESRF]]></dc:title>
<dc:source><![CDATA[27. Jounees des Actinides, Dijon, France, 26.-29.4.1997, invited]]></dc:source>
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<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:creator><![CDATA[Noll, B.]]></dc:creator>
<dc:creator><![CDATA[Leibnitz, P.]]></dc:creator>
<dc:creator><![CDATA[Reck, G.]]></dc:creator>
<dc:creator><![CDATA[Noll, S.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-128-1</dc:identifier>
<dc:title><![CDATA[Occurence and Nature of Different Tc(V) and Re(V) Complexes with Mercapto/Amide Ligands]]></dc:title>
<dc:source><![CDATA[Radiochimica Acta 63 (1993) pp. 133-137]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2728-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Shuh, D. K.]]></dc:creator>
<dc:creator><![CDATA[Allen, P. G.]]></dc:creator>
<dc:creator><![CDATA[Bucher, J. J.]]></dc:creator>
<dc:creator><![CDATA[Edelstein, N. M.]]></dc:creator>
<dc:creator><![CDATA[Denecke, M. A.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2728-1</dc:identifier>
<dc:title><![CDATA[X-ray Absorption Fine Structure of Actinides in Concentrated Electrolytes]]></dc:title>
<dc:source><![CDATA[Actinides'97, Baden-Baden, Germany, 21.-26.09.1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2733-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Zänker, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2733-1</dc:identifier>
<dc:title><![CDATA[Colloid Chemistry of Humic Acid]]></dc:title>
<dc:source><![CDATA[First Project Meeting of the FU project "Effects of Humic Substances on the Migration of Radionuclides: Complexation and Transport of Actinides", Forschungszentrum Karlsruhe, Institut f. Nukleare Entsorgungstechnik; Karlsruhe, Germany, 03.-04.03.1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<dc:title><![CDATA[Characterization of the Submicron Particles in the Kranichsee Moor Water]]></dc:title>
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<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Pavlenko, O. P.]]></dc:creator>
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<dc:title><![CDATA[Photon production in an expanding and chemically equilibrating gluon-enriched plasma]]></dc:title>
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<dc:description><![CDATA[Abstract  Photon production in a longitudinally and transversely expanding gluon plasma with initially little quark admixture is considered. Chemical equilibration of quarks and gluons is followed by rate equations. The yields of hard photons withE2 GeV are insensitive to chemical equilibration and depend mainly on the initial thermalized state. Medium-energy photons withE1 GeV are more frequently produced in case of faster equilibration, despite of faster cooling. For an assumed fast equilibration we follow the evolution of matter through mixed and hadron phases. The transverse momentum kick, due to transverse expansion, of photons from hadron matter is shown to be reduced for an equation of state with reduced latent heat. The photon yield in the regionE>1 GeV from deconfined matter dominates for conditions, estimated to be achieved at RHIC, in case of a weakly first-order confinement transition.]]></dc:description>
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<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
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<dc:creator><![CDATA[Brutscher, J.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
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<dc:title><![CDATA[Sheath Dynamics in Plasma Immersion Ion Implantation]]></dc:title>
<dc:source><![CDATA[Surface & Coatings Technology 85 (1996) pp. 98-104]]></dc:source>
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<dc:creator><![CDATA[Abraham, A.]]></dc:creator>
<dc:creator><![CDATA[Mack, B.]]></dc:creator>
<dc:creator><![CDATA[Baraniak, L.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
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<dc:title><![CDATA[Vergleich der Sorption von Eisen und Uran an Erzgebirgsmetamorphiten und Elbtalsedimenten unter aeroben und anaeroben Bedingungen und unter dem Einfluß organischer Grubenwasserinhaltsstoffe]]></dc:title>
<dc:source><![CDATA[GDCh-Fachtagung, FG Nuklearchemie
Dresden, Germany, 07.-09.09.1998]]></dc:source>
<dc:date>1998</dc:date>
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<dc:creator><![CDATA[Bubner, M.]]></dc:creator>
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<dc:title><![CDATA[Die Synthese isotopmarkierter Modellhuminsäuren]]></dc:title>
<dc:source><![CDATA[GDCh-Fachtagung, FG Nuklearchemie
Dresden, Germany, 07.-09.09.1998]]></dc:source>
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Dresden, Germany, 07.-09.09.1998]]></dc:source>
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<dc:title><![CDATA[FTIR-Untersuchungen zur Komplexierung von Uran(V) durch huminsäureähnliche Melanoidine]]></dc:title>
<dc:source><![CDATA[GDCh-Fachtagung, FG Nuklearchemie
Dresden, Germany, 07.-09.09.1998]]></dc:source>
<dc:date>1998</dc:date>
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<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
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<dc:title><![CDATA[Huminsäureforschung im FZR - Melanoidine als Modell-Huminsäuren]]></dc:title>
<dc:source><![CDATA[Uranium Mining and Hydrogeology II
Freiberg, Germany, 15.-17.09.1998]]></dc:source>
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<dc:creator><![CDATA[Hennig, C.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2803-1</dc:identifier>
<dc:title><![CDATA[Korrektur der Koordinationszahlbestimmung für die Uranylgruppe aus EXAFS-Messungen pulverförmiger Proben]]></dc:title>
<dc:source><![CDATA[GDCh-Fachtagung, FG Nuklearchemie
Dresden, Germany, 07.-09.09.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2804-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hennig, C.]]></dc:creator>
<dc:creator><![CDATA[Kraus, W.]]></dc:creator>
<dc:creator><![CDATA[Nolze, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2804-1</dc:identifier>
<dc:title><![CDATA[The Problem of Preferred Orientation in EXAFS Measurements - Solvable with X-ray Diffraction?]]></dc:title>
<dc:source><![CDATA[Euroconference and NEA Workshop: Actinide-XAS-98
Grenoble, France, 04.-06.10.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:3013-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Jankowsky, R.]]></dc:creator>
<dc:creator><![CDATA[Friebe, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3013-1</dc:identifier>
<dc:title><![CDATA[Verfahren zur Auftrennung von Substanzgemischen]]></dc:title>
<dc:source><![CDATA[DE 197 50 832 A 1]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Die Erfindung betrifft ein Verfahren zur Auftrennung von Substanzgemischen unter Verwendung der Kapillarelektrophorese.

Mit der Erfindung soll die Kapillarelektrophorese dahingehend modifiziert werden, daß der die Auftrennung von Substanzgemischen beeinträchtigende Einfluß der Parameter gesenkt und der Prozeß der Auftrennung insbesondere bei niedrigem pH-Wert beschleunigt wird.

Erfindungsgemäß wird die Aufgabe dadurch gelöst, daß während des analytischen Trennlaufs bei der Kapillarelektrophorese das Einlaßgefäß mit einem extern erzeugten Luftüberdruck beaufschlagt wird. Abhängig von der Gräße der Kapillare und den elektrischen Bedingungen wird der Luftüberdruck zwischen 5 und 80 mbar gewählt.
]]></dc:description>
<dc:type>info:eu-repo/semantics/patent</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:patent</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:1477-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1477-2</dc:identifier>
<dc:title><![CDATA[Integrated high voltage modulator for plasma immersion ion implantation]]></dc:title>
<dc:source><![CDATA[4th Int. Workshop on PBII, Dearborn, June 2-4, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Plasma immersion ion implantation (PIII) on an industrial scale requires negative high voltage pulses in the kA range with voltages up to 200 kV. Hence, the equipment to produce suitable high voltage pulses is rather expensive and shares a considerable part of the total costs of PIII equipment. Reducing the costs of equipment is therefore still a challenge to promote the commercial use of PIII.
A new high voltage modulator is presented, which will meet the above requirements. 
The basic idea of the new modulator is that in case of two floating electrodes, immersed into a plasma and connected to both plates of a charged capacitor, the anode potential will be close to the plasma potential, whereas the cathode potential will become negative compared to the plasma potential. 
The new modulator works as a triode system, consisting of anode, cathode and grid, all located inside of the working chamber. The plasma is discharged between cathode and grid. As usual in PIII, the sample is immersed into the plasma and works as the cathode in the system. The grid is mounted between plasma and anode, in such a way that ions or electrons from the plasma can get to the anode by passing the grid plane only. Further a capacitor is connected to anode and cathode with both plates and the anode is additionally linked to a positive high voltage source. If the grid is negatively biased, the anode is isolated from the plasma, as electrons from the plasma are reflected by the grid bias, whereas the ions are reflected by the positive potential of the anode. As far as the grid is negatively biased the cathode is at plasma floating potential, and the capacitor may be charged by the positive high voltage source to the capacitor voltage. When the grid potential is switched to ground potential electrons from the plasma can reach the anode and will shift the anode potential to plasma potential. At the same time the cathode is switched to negative high voltage potential  . 
As the performance of the integrated modulator depends on the maximum of the electron current which can be extracted from the plasma by the anode, the basic considerations concerning the anode current and the revealing design parameters of the integrated modulator are given. The experimental results of modulating 20 kV at a maximum current of 4 A confirm the theory.  ]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1477-1</identifier>
<datestamp>2025-02-06</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1477-1</dc:identifier>
<dc:title><![CDATA[Integrated high voltage modulator for plasma immersion ion implantation]]></dc:title>
<dc:source><![CDATA[Journal of Vacuum Science and Technology B 17(2), Mar/Apr 1999, 895-899]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Plasma immersion ion implantation (PIII) on an industrial scale requires negative high voltage pulses in the kA range with voltages up to 200 kV. Hence, the equipment to produce suitable high voltage pulses is rather expensive and shares a considerable part of the total costs of PIII equipment. Reducing the costs of equipment is therefore still a challenge to promote the commercial use of PIII.
A new high voltage modulator is presented, which will meet the above requirements. 
The basic idea of the new modulator is that in case of two floating electrodes, immersed into a plasma and connected to both plates of a charged capacitor, the anode potential will be close to the plasma potential, whereas the cathode potential will become negative compared to the plasma potential. 
The new modulator works as a triode system, consisting of anode, cathode and grid, all located inside of the working chamber. The plasma is discharged between cathode and grid. As usual in PIII, the sample is immersed into the plasma and works as the cathode in the system. The grid is mounted between plasma and anode, in such a way that ions or electrons from the plasma can get to the anode by passing the grid plane only. Further a capacitor is connected to anode and cathode with both plates and the anode is additionally linked to a positive high voltage source. If the grid is negatively biased, the anode is isolated from the plasma, as electrons from the plasma are reflected by the grid bias, whereas the ions are reflected by the positive potential of the anode. As far as the grid is negatively biased the cathode is at plasma floating potential, and the capacitor may be charged by the positive high voltage source to the capacitor voltage. When the grid potential is switched to ground potential electrons from the plasma can reach the anode and will shift the anode potential to plasma potential. At the same time the cathode is switched to negative high voltage potential  . 
As the performance of the integrated modulator depends on the maximum of the electron current which can be extracted from the plasma by the anode, the basic considerations concerning the anode current and the revealing design parameters of the integrated modulator are given. The experimental results of modulating 20 kV at a maximum current of 4 A confirm the theory.  ]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1116/1.590658]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:1027-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Baraniak, L.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, M.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1027-1</dc:identifier>
<dc:title><![CDATA[Complexation of Uranium(VI) with the Main Components of Mine-Wood Degradation. Part 1. Complexation with Protocatehuic Acid, Vanillic Acid and Vanillin]]></dc:title>
<dc:source><![CDATA[6th International Conference on Chemistry and Migration Behaviour of Actinides and Fission Products in the Geosphere: MIGRATION '97, Sendai, Japan, October 26-31, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[<P>To consider the process of mine wood degradation and its concequences on the contaminant migration via aquatic path in risk assessments, e.g. for uranium mine restoration in the southern region of Saxony (Germany), the complexation of U(VI) with 3,4-dihydroxybenzoic acid (proto-catechuic acid), 4-hydroxy-3-methoxy-cinnamic acid (ferulic acid), 4-hydroxy-3-methoxybenzoic acid (vanillic acid) and 4-hydroxy-3-methoxybenzaldehyde (vanillin) was studied by potentiometric pH titration in carbonate-free solutions of 0.1 M NaClO<SUB>4</SUB>. These four complexants are reasonably stable monomeric intermediates in the microbial or hydrothermally driven spruce-wood lignin degradation and therefore play a role in natural water chemistry.</P>
<P>The evaluation of the pH titration curves was carried out with the classical theory of stepwise complex formation, analyzing Bjerrums formation function [1] and by non-linear fitting of the pH titration curve with Sayces multi-equilibria program "SCOGS" [2], considering hydrolysis  and mixed-ligand complexation.</P>
<P>In the case of protocatechuic acid, a series of very stable (1:1) to (1:3) complexes are formed (log ß: 14.8/25.9/33.2). The constants calculated by Bjerrums formation function are in full agreement with the values of the SCOGS curve fitting, i.e. U(VI) hydrolysis is surpressed in the presence of this ligand. The complexes with ferulic acid and vanillic acid have a much lower stability: log ß<SUB>11</SUB> values are to 6.88 and 7.16, respectively. In the case of ferulic acid, the assumption of the acidic species [UO<SUB>2</SUB>H(fer)]<SUP>+</SUP> with log ß<SUB>111</SUB> =11.9 improves the pH curve fit. Vanillin as complexant leads to pH curves that can be best fitted with the species [UO<SUB>2</SUB>(van)]<SUP>+</SUP> and [UO<SUB>2</SUB>(van)<SUB>2</SUB>(OH)<SUB>2</SUB>]<SUP>2-</SUP> with log ß values of 4.47 and -3.95, respectively.</P>
<P>Using these data speciation calculations for some calcite-rich mine waters show that the strong U(VI)-carbonato complexes predominate. Under certain conditions only protocatechuic acid complexes can be formed.</P>
]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:2320-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Jentschel, M.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Börner, H. G.]]></dc:creator>
<dc:creator><![CDATA[Doll, C.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2320-1</dc:identifier>
<dc:title><![CDATA[Crystal-GRID investigations of atomic collision cascades in ionic compounds]]></dc:title>
<dc:source><![CDATA[Mat. Sci. Forum  248-249 (1997) 49]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2320-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1108-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1108-1</dc:identifier>
<dc:title><![CDATA[Damage in silicon carbide induced by Rutherford backscattering analysis]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B135-138 (1998) 460]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1108-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2855-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grahn, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2855-1</dc:identifier>
<dc:title><![CDATA[Chemische Reaktion an der Phasengrenze nichtmischbarer Flüssigkeiten]]></dc:title>
<dc:source><![CDATA[29. Sitzung des DECHEMA/GVC-Arbeitsausschusses "Reaktionstechnik sicherheitstechnisch schwieriger Prozesse"]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Im Vortrag werden Versuche zum reaktiven Stoffübergang über die Phasengrenze zweier nicht mischbarer Lösungsmittel und die dabei auftretenden hydrodynamischen Instabilitäten sowie die numerische Simulation dieser Vorgänge in einer vertikalen Spaltgeometrie vorgestellt.]]></dc:description>
<dc:subject><![CDATA[hydrodynamische Instabilität]]></dc:subject>
<dc:subject><![CDATA[fluide Phasengrenze]]></dc:subject>
<dc:subject><![CDATA[Grenzflächenreaktion]]></dc:subject>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2855-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:3012-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3012-1</dc:identifier>
<dc:title><![CDATA[Verfahren zur Erzeugung einer dotierten Schicht in Siliziumkarbid]]></dc:title>
<dc:source><![CDATA[DE 197 41 725 A 1]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Die Erfindung betrifft ein Verfahren zur Dotierung von Halbleiterbauelementen, deren Substrat aus Siliziumkarbid besteht.
Der Erfindung liegt die Aufgabe zugrunde, in Siliziumkarbid-Substraten p-leitende Schichten herzustellen, deren Schichtwiderstand kleiner als 10 k /  ist und in denen die Löcherbeweglichkeit größer als 10 cm²/Vs ist.
Erfindungsgemäß wird die Aufgabe dadurch gelöst, daß zusätzlich zu den Akzeptor-Ionen Kohlenstoff-Ionen in einer Konzentration von mehr als 5 Atom% implantiert werden. Dabei können die Kohlenstoff-Ionen vor, während oder nach dem Einbringen der Akzeptor-Ionen implantiert werden.In vorteilhafter Ausgestaltung der Erfindung erfolgt eine Ausheilung der Schicht mit mindestens 500°C. Die Implantationsdosis kann auch in mehreren Teilschritten eingebracht werden. Die Ausheilung soll dann nach jedem Teilschritt erfolgen.
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:3012-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3012-2</dc:identifier>
<dc:title><![CDATA[Verfahren zur Erzeugung einer dotierten Schicht in Siliziumkarbid]]></dc:title>
<dc:source><![CDATA[Patent DE 197 41 725 C2]]></dc:source>
<dc:date>2003</dc:date>
<dc:description><![CDATA[Die Erfindung betrifft ein Verfahren zur Dotierung von Halbleiterbauelementen, deren Substrat aus Siliziumkarbid besteht.
Der Erfindung liegt die Aufgabe zugrunde, in Siliziumkarbid-Substraten p-leitende Schichten herzustellen, deren Schichtwiderstand kleiner als 10 k /  ist und in denen die Löcherbeweglichkeit größer als 10 cm²/Vs ist.
Erfindungsgemäß wird die Aufgabe dadurch gelöst, daß zusätzlich zu den Akzeptor-Ionen Kohlenstoff-Ionen in einer Konzentration von mehr als 5 Atom% implantiert werden. Dabei können die Kohlenstoff-Ionen vor, während oder nach dem Einbringen der Akzeptor-Ionen implantiert werden.In vorteilhafter Ausgestaltung der Erfindung erfolgt eine Ausheilung der Schicht mit mindestens 500°C. Die Implantationsdosis kann auch in mehreren Teilschritten eingebracht werden. Die Ausheilung soll dann nach jedem Teilschritt erfolgen.
]]></dc:description>
<dc:type>info:eu-repo/semantics/patent</dc:type>
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<identifier>HZDR:PUBLDB:856-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kögler, R.]]></dc:creator>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Kaschny, J.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Danilin, A. B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-856-1</dc:identifier>
<dc:title><![CDATA[Detection of metastable defective regions in ion-implanted Silicon by means of metall gettering]]></dc:title>
<dc:source><![CDATA[MRS '97, Spring Meeting, San Francisco, March 31-April 4, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2682-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Simoen, E.]]></dc:creator>
<dc:creator><![CDATA[Vanhellemont, J.]]></dc:creator>
<dc:creator><![CDATA[Alaerts, A.]]></dc:creator>
<dc:creator><![CDATA[Claeys, C.]]></dc:creator>
<dc:creator><![CDATA[Gaubas, E.]]></dc:creator>
<dc:creator><![CDATA[Kaniava, A.]]></dc:creator>
<dc:creator><![CDATA[Ohyama, H.]]></dc:creator>
<dc:creator><![CDATA[Sunaga, H.]]></dc:creator>
<dc:creator><![CDATA[Nashiyama, I.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2682-1</dc:identifier>
<dc:title><![CDATA[Proton irradiation effects in silicon devices]]></dc:title>
<dc:source><![CDATA[Proc. of the 7.Int.Symp. on "Recent progress in Accelerator Beam Applications", Takasaki, Japan, JAERI-Conf. 97-003, p. 224]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:824-1</identifier>
<datestamp>2022-11-11</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barz, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Bondorf, J. P.]]></dc:creator>
<dc:creator><![CDATA[Gaardhoje, J. J.]]></dc:creator>
<dc:creator><![CDATA[Heiselberg, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-824-1</dc:identifier>
<dc:title><![CDATA[Freeze-Out Time in Ultrarelativistic Heavy Ion Collisions from Coulomb Effects in Transverse Pion Spectra]]></dc:title>
<dc:source><![CDATA[Physical Review C 56, No. 3, September 1997, 1553-1556]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Abstract:
The influence of the nuclear Coulomb field on transverse spectra of  λ <sup>+</sup> and λ<sup>-</sup> measured in Pb + Pb reactions at 158 A GeV has been investigated. Pion trajectories are calculated in the field of an expanding fireball. The observed enhancement of the λ<sup>-</sup>/λ<sup>+</sup> ratio at small momenta depends on the temperature and transverse expansion velocity of the source, the rapidity distribution of the net positive charge, and mainly the time of the freeze-out.]]></dc:description>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevC.56.1553]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-824-1</dc:relation>
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<header>
<identifier>HZDR:PUBLDB:824-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Barz, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Bondorf, J. P.]]></dc:creator>
<dc:creator><![CDATA[Gaardhoje, J. J.]]></dc:creator>
<dc:creator><![CDATA[Heiselberg, H.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-824-2</dc:identifier>
<dc:title><![CDATA[Freeze-Out Time in Ultrarelativistic Heavy Ion Collisions from Coulomb Effects in Transverse Pion Spectra]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-168 Preprint]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Abstract:
The influence of the nuclear Coulomb field on transverse spectra of  λ <sup>+</sup> and λ<sup>-</sup> measured in Pb + Pb reactions at 158 A GeV has been investigated. Pion trajectories are calculated in the field of an expanding fireball. The observed enhancement of the λ<sup>-</sup>/λ<sup>+</sup> ratio at small momenta depends on the temperature and transverse expansion velocity of the source, the rapidity distribution of the net positive charge, and mainly the time of the freeze-out.]]></dc:description>
<dc:type>info:eu-repo/semantics/preprint</dc:type>
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<dc:type>doc-type:report</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1287-1</identifier>
<datestamp>2023-05-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ortner, K.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1287-1</dc:identifier>
<dc:title><![CDATA[Gold(III) Complexes with Diphenylthiocarbazonate. Synthesis and Structures of [Au(Hdamp-C<SUP>1)</SUP>{PhNHNC(S)NNPh}Cl]ClxH<SUB>2</SUB>O and ...]]></dc:title>
<dc:source><![CDATA[Polyhedron 18 (1999) 749-754]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0277-5387(98)00349-0]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1287-1</dc:relation>
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<header>
<identifier>HZDR:PUBLDB:2723-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Turos, A.]]></dc:creator>
<dc:creator><![CDATA[Wieteska, K.]]></dc:creator>
<dc:creator><![CDATA[Wierzchowski, W. K.]]></dc:creator>
<dc:creator><![CDATA[Wendler, E.]]></dc:creator>
<dc:creator><![CDATA[Wesch, W.]]></dc:creator>
<dc:creator><![CDATA[Strupinski, W.]]></dc:creator>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2723-1</dc:identifier>
<dc:title><![CDATA[Ion bombardment induced relaxation of strained AlGaAs/GaAs heterostructures studied by the complementary use of RBS-channeling and X-ray synchrotron radiation]]></dc:title>
<dc:source><![CDATA[13th Int. Conf. on Ion Beam Analysis (IBA-13), Lisboa, Portugal, July 27 - Aug. 1, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1206-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Scheffel, U.]]></dc:creator>
<dc:creator><![CDATA[Szabo, Z.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1206-1</dc:identifier>
<dc:title><![CDATA[Radioligands for the Study of the 5-HT Transporter in Vivo]]></dc:title>
<dc:source><![CDATA[IDrugs 1999 Vol 2 No 2 , Review Radioligands 129-145]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Loss of 5-HT transporter (SERT) sites has been implicated in various neurodegenerative diseases and users of some amphetamine derivatives such as MDMA. Therefore, the development of suitable radioligands for neuroimaging of the SERT in the human brain is important. A large number of drugs have been labeled with <SUP>11</SUP>C, <SUP>18</SUP>F or <SUP>123</SUP>I over the last ten years in order to achieve such radioligands. Despite these attempts most of the compounds were found unsuitable because of low target-to-nontarget ratios. Some cocaine-derived radioligands allow SERT imaging of the human brain using positron emission tomography (PET) although they have a limited selectivity. Among the various specific 5-HT uptake inhibitors only [<SUP>123</SUP>I]iodonitroquipazine for single photon emission computed tomography (SPECT) and [<SUP>11</SUP>C](+)McN5652 for PET appear to meet the criteria of a useful radioligand. There is still a need for the development of new radioligands for SERT imaging. Advances in tracer synthetic methodologies may bring further progress in this field.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:969-1</identifier>
<datestamp>2023-04-28</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Pavlenko, O. P.]]></dc:creator>
<dc:creator><![CDATA[Peshier, A.]]></dc:creator>
<dc:creator><![CDATA[Hentschel, M.]]></dc:creator>
<dc:creator><![CDATA[Soff, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-969-1</dc:identifier>
<dc:title><![CDATA[Thermal Open Charm Signals Versus Hard Initial Yields in ultrarelativistic Heavy-Ion Collisions]]></dc:title>
<dc:source><![CDATA[Journal of Physics G: Nucl. Part. Phys. 23 (1997) 2001-2011]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Abstract. 

Exploiting a unique set of parton distribution functions we estimate hard processes for open charm, dilepton and mini-jet production. Assuming rapid thermalization within the mini-jet plasma we follow the evolution (expansion and chemical equilibration) of the parton matter and calculate the energy loss of charm quarks in this environment. A substantial part of charm is espected to thermalize. We try to estimate the thermalized open charm component in the final hadron spectra.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1088/0954-3899/23/12/025]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-969-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:969-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Pavlenko, O. P.]]></dc:creator>
<dc:creator><![CDATA[Peshier, A.]]></dc:creator>
<dc:creator><![CDATA[Hentschel, M.]]></dc:creator>
<dc:creator><![CDATA[Soff, G.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-969-2</dc:identifier>
<dc:title><![CDATA[Thermal Open Charm Signals Versus Hard Initial Yields in ultrarelativistic Heavy-Ion Collisions]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-189]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Abstract. 

Exploiting a unique set of parton distribution functions we estimate hard processes for open charm, dilepton and mini-jet production. Assuming rapid thermalization within the mini-jet plasma we follow the evolution (expansion and chemical equilibration) of the parton matter and calculate the energy loss of charm quarks in this environment. A substantial part of charm is espected to thermalize. We try to estimate the thermalized open charm component in the final hadron spectra.]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-969-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:14264-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Constantinescu, B.]]></dc:creator>
<dc:creator><![CDATA[Bugoi, R.]]></dc:creator>
<dc:creator><![CDATA[Munnik, F.]]></dc:creator>
<dc:creator><![CDATA[Pichon, L.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14264-1</dc:identifier>
<dc:title><![CDATA[Micro-pixe studies for archaeological gold identification  the case of transylvanian gold and of dacian gold staters (kosons)]]></dc:title>
<dc:source><![CDATA[ICNMTA 2010 - 12th International Conference on Nuclear Microprobe Technology and Applications, 26.-30.07.2010, Leipzig, Germany]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Trace elements are more significant for provenance of archaeological metallic artifacts than the main components. For gold, the most promising elements are Platinum Group Elements (PGE), Sb, Hg, Pb, and, especially for alluvial (panned) gold, Sn and Pt. Several small fragments of ancient gold objects from some Bronze Age objects and Greek and Dacian (KOSON  type) coins were analyzed. To check if the Transylvanian gold was used, some fragments of nuggets from Transylvanian mines and alluvial gold were also studied. The measurements were performed by using the AGLAE accelerator of the Centre de Recherche et de Restauration des Musees de France. The samples were bombarded with a 3 MeV proton micro-beam (roughly 50 µm diameter). The employed   beam current was around 10 nA. We also used the micro-PIXE technique at the nuclear microprobe facility of the Forschungszentrum Dresden-Rossendorf. A 3 MeV proton beam was employed; the beam diameter was roughly 150 μm. The total accumulated charge was around 3 μC. 
As conclusions of the performed experiments, one can quote the following findings: 
- Sn was detected as a trace-element in all the KOSON without monogram coins; in one of them we could acquire spectra in several spots; in one of them a very high concentration of Sn was found but not in the surrounding areas, most probably a cassiterite grain; 
- No trace-elements were detected in the KOSON with monogram coins and the pseudo-Lysimach staters issued by the Greek colonies at the Black Sea coast; it was concluded that highly refined gold was used to manufacture these coins; the above findings led us to the idea that the two kind of KOSON coins were manufactured by using different gold sources 
- Sn was also found as trace element in a fragment taken from a Early Bronze Age bracelet from Tauteu, hoard (Transylvania) and in a fragment from the Vulchitrun-like disk (Late Bronze Age) found in Calarasi, Oltenia; we could conclude that alluvial gold was most likely used to manufacture these Bronze Age objects; 
- Te was found in several geological samples (e.g. in the ones from Rosia Montana), a fact that is of particular importance, since this element appears to be a characteristic of the Transylvanian gold minerals, but it is easily evaporated during the native gold melting, so, its presence in gold objects is very improbable; 
- A very interesting finding was the presence of Pd traces in one of the alluvial gold samples, the one coming from Mures river.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:14359-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Wosnitza, J.]]></dc:creator>
<dc:creator><![CDATA[Bergk, B.]]></dc:creator>
<dc:creator><![CDATA[Ignatchik, O.]]></dc:creator>
<dc:creator><![CDATA[Polyakov, A.]]></dc:creator>
<dc:creator><![CDATA[Gumeniuk, R.]]></dc:creator>
<dc:creator><![CDATA[Leithe-Jasper, A.]]></dc:creator>
<dc:creator><![CDATA[Schnelle, W.]]></dc:creator>
<dc:creator><![CDATA[Nicklas, M.]]></dc:creator>
<dc:creator><![CDATA[Rosner, H.]]></dc:creator>
<dc:creator><![CDATA[Grin, Y.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14359-1</dc:identifier>
<dc:title><![CDATA[Electronic band structure of superconducting PrPt<sub>4</sub>Ge<sub>12</sub>]]></dc:title>
<dc:source><![CDATA[Strongly Correlated Electron Systems 2010 (SCES2010), 27.06.-02.07.2010, Santa Fe, USA]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Recently, the new skutterudite superconductor PrPt<sub>4</sub>Ge<sub>12</sub> with the comparably high transition temperature of T<sub>c</sub> = 7.9 K was discovered [1]. First experiments gave evidence for strong coupling and hint at point-like nodes of the order parameter [2]. The Sommerfeld coefficient is rather low and indicates that PrPt<sub>4</sub>Ge<sub>12</sub> is not a heavy-fermion superconductor. Here, we present results of a de Haas-van Alphen (dHvA) study performed on a high-quality single crystal. Several dHvA frequencies could be resolved over a broad angular range. The small band-resolved effective masses (less than half the free-electron mass) confirm the non-heavy-fermion character of the electron system. To get insight into the nature of the mass renormalization, the experimental data are compared with state-of-the-art band-structure calculations]]></dc:description>
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<dc:language>eng</dc:language>
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<record>
<header>
<identifier>HZDR:PUBLDB:1619-1</identifier>
<datestamp>2023-05-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bauer, R.]]></dc:creator>
<dc:creator><![CDATA[Bergmann, R.]]></dc:creator>
<dc:creator><![CDATA[Walter, B.]]></dc:creator>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Zwiener, U.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1619-1</dc:identifier>
<dc:title><![CDATA[Regional distribution of cerebral blood volume and cerebral blood flow in newborn piglets - effect of hypoxia / hypercapnia]]></dc:title>
<dc:source><![CDATA[Developmental Brain Research 112 (1999) 89-98]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The relationship between regional parenchymal cerebral blood volume (CBV), regional cerebral blood flow (CBF) and the calculated mean transit time (MTT) was investigated in 14 newborn piglets. The effects of combined hypoxic hypoxia (p<SUB>a</SUB>O<SUB>2</SUB> = 32 ± 5 mm Hg) and hypercapnia ((p<SUB>a</SUB>CO<SUB>2</SUB> = 68 ± 5 mm Hg) were measured in seven animals. Remaining animals served as the control group. During baseline conditions the highest CBF and CVB values were found in the lower brainstem and cerebellum, whereas white matter exhibited the lowest values (p<0.05). MTT was prolonged within the cerebral cortex (2.34 ± 0.42 s<SUP>-1</SUP>) compared with the thalamic MTT (1.53 ± 0,38 s<SUP>-1</SUP>) (p<0.05). Under moderate hypoxia/hypercapnia, a CBF increase to the forebrain (p<0.05) resulted in an elevated brain oxygen delivery (p<0.05) and so CMRO<SUB>2</SUB> remained unchanged. Moreover, a moderate increase of CBV and a marked shortening of MTT occurred (p<0.05). The CBV increase was higher in structures with lowest baseline values, i.e., thalamus (66% increase) and white matter (62% increase) (p<0.05). MTT was between 22% of baseline in the lower brainstem and 49% in white matter (p<0.05). We conclude that under normoxic and normocapnic conditions the newborn piglets exhibit a comparatively enlarged intraparenchymal CBV. Moderate hypoxia and hypercapnia induced a marked increase in cerebral blood flow which appears to be  caused by an increased perfusion velocity, expressed by a strongly reduced mean transit time and by a concomitant CBV increase. ]]></dc:description>
<dc:subject><![CDATA[Cerebral blood flow]]></dc:subject>
<dc:subject><![CDATA[Cerebral blood volume]]></dc:subject>
<dc:subject><![CDATA[Colored microspheres]]></dc:subject>
<dc:subject><![CDATA[<SUP>99m</SUP>Technetium pertechnetate]]></dc:subject>
<dc:subject><![CDATA[Newborn piglet]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0165-3806(98)00167-9]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1619-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:2905-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Kryk, H.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Seiler, T.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Deerberg, G.]]></dc:creator>
<dc:creator><![CDATA[Neumann, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2905-1</dc:identifier>
<dc:title><![CDATA[Assessment and Identification of Undesired States in Chemical Semibatch Reactors Using Neural Networks]]></dc:title>
<dc:source><![CDATA[Proceedings of IFAC Symposium on Fault Detection, Supervision and Safety for Technical Processes - SAFEPROCESS'2000, Budapest, 14-16 June, 2000, pp. 458-461]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[This paper presents a neural-network approach to operator-independent assessing the operational states of chemical semibatch reactors. The suitability of neural networks for process monitoring was investigated in a miniplant in which strongly exothermic chemical reference processes were carried out. Before being applied to state classification, the neural network classifiers first have be trained using process data of normal and abnormal sequences of reaction to establish a nonlinear decision model between process parameters and state classification. Afterwards, the trained classifiers can be used for process monitoring. Best results were reached with three-layer perceptron networks. For assessing the danger potential of fault states, separate perceptron networks for danger classification and for fault isolation were used.]]></dc:description>
<dc:subject><![CDATA[Fault diagnosis]]></dc:subject>
<dc:subject><![CDATA[Process identification]]></dc:subject>
<dc:subject><![CDATA[Supervision]]></dc:subject>
<dc:subject><![CDATA[Artificial intelligence]]></dc:subject>
<dc:subject><![CDATA[Classifiers]]></dc:subject>
<dc:subject><![CDATA[Neural networks]]></dc:subject>
<dc:subject><![CDATA[Chemical industry]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:2905-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:creator><![CDATA[Kryk, H.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Seiler, T.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Deerberg, G.]]></dc:creator>
<dc:creator><![CDATA[Neumann, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2905-7</dc:identifier>
<dc:title><![CDATA[Assessment and Identification of Undesired States in Chemical Semibatch Reactors Using Neural Networks]]></dc:title>
<dc:source><![CDATA[Proceedings of IFAC Symposium on Fault Detection, Supervision and Safety for Technical Processes - SAFEPROCESS'2000, Budapest, 14-16 June, 2000, pp. 458-461]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[This paper presents a neural-network approach to operator-independent assessing the operational states of chemical semibatch reactors. The suitability of neural networks for process monitoring was investigated in a miniplant in which strongly exothermic chemical reference processes were carried out. Before being applied to state classification, the neural network classifiers first have be trained using process data of normal and abnormal sequences of reaction to establish a nonlinear decision model between process parameters and state classification. Afterwards, the trained classifiers can be used for process monitoring. Best results were reached with three-layer perceptron networks. For assessing the danger potential of fault states, separate perceptron networks for danger classification and for fault isolation were used.]]></dc:description>
<dc:subject><![CDATA[Fault diagnosis]]></dc:subject>
<dc:subject><![CDATA[Process identification]]></dc:subject>
<dc:subject><![CDATA[Supervision]]></dc:subject>
<dc:subject><![CDATA[Artificial intelligence]]></dc:subject>
<dc:subject><![CDATA[Classifiers]]></dc:subject>
<dc:subject><![CDATA[Neural networks]]></dc:subject>
<dc:subject><![CDATA[Chemical industry]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2906-1</identifier>
<datestamp>2025-12-03</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Herzberg, R.-D.]]></dc:creator>
<dc:creator><![CDATA[Fransen, C.]]></dc:creator>
<dc:creator><![CDATA[Brentano, P.]]></dc:creator>
<dc:creator><![CDATA[Eberth, J.]]></dc:creator>
<dc:creator><![CDATA[Enders, J.]]></dc:creator>
<dc:creator><![CDATA[Fitzler, A.]]></dc:creator>
<dc:creator><![CDATA[Käubler, L.]]></dc:creator>
<dc:creator><![CDATA[Kaiser, H.]]></dc:creator>
<dc:creator><![CDATA[Neumann-Cosel, P.]]></dc:creator>
<dc:creator><![CDATA[Pietralla, N.]]></dc:creator>
<dc:creator><![CDATA[Ponomarev, V. Y.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, A.]]></dc:creator>
<dc:creator><![CDATA[Schnare, H.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Skoda, S.]]></dc:creator>
<dc:creator><![CDATA[Thomas, H. G.]]></dc:creator>
<dc:creator><![CDATA[Tiesler, H.]]></dc:creator>
<dc:creator><![CDATA[Weisshaar, D.]]></dc:creator>
<dc:creator><![CDATA[Wiedenhöver, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2906-1</dc:identifier>
<dc:title><![CDATA[Resolved dipole strength below the giant resonance in <SUP>138</SUP>Ba]]></dc:title>
<dc:source><![CDATA[Physical Review C, Volume 60, 051307]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevC.60.051307]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2906-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2996-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Rettig, D.]]></dc:creator>
<dc:creator><![CDATA[Merker, P.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:creator><![CDATA[Rudolph, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2996-1</dc:identifier>
<dc:title><![CDATA[Verfahren und Einrichtung zur Herstellung von Kieselsäureaerosolen]]></dc:title>
<dc:source><![CDATA[DE 198 25 193 A1]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[wird nachgereicht]]></dc:description>
<dc:type>info:eu-repo/semantics/patent</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:patent</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2996-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2984-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Lielausis, O.]]></dc:creator>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2984-1</dc:identifier>
<dc:title><![CDATA[Verfahren und Anordnung zur Steuerung der Gasblasenbildung in elektrisch leitfähigen Flüssigkeiten]]></dc:title>
<dc:source><![CDATA[Patentanmeldung Az 199 48 879.7]]></dc:source>
<dc:date>2001</dc:date>
<dc:description><![CDATA[Der Erfindung liegt die Aufgabe zugrunde, ein Verfahren und eine Anordnung vorzuschlagen, mit der die Steuerung der Blasengröße ermöglicht wird. Eine spezielle Aufgabenstellung besteht in der Generierung möglichst kleiner Gasblasen. ]]></dc:description>
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<dc:title><![CDATA[Verfahren und Anordnung zur Steuerung der Gasblasenbildung in elektrisch leitfähigen Flüssigkeiten]]></dc:title>
<dc:source><![CDATA[Patentschrift DE 199 48 879 C1]]></dc:source>
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<dc:description><![CDATA[Der Erfindung liegt die Aufgabe zugrunde, ein Verfahren und eine Anordnung vorzuschlagen, mit der die Steuerung der Blasengröße ermöglicht wird. Eine spezielle Aufgabenstellung besteht in der Generierung möglichst kleiner Gasblasen. ]]></dc:description>
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<dc:title><![CDATA[Elektrisch steuerbare Mikro-Pipette]]></dc:title>
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<dc:description><![CDATA[Die Erfindung betrifft eine elektrisch steuerbare Mikro-Pipette zur Handhabung kleinster Fluidvolumina im Bereich von einigen hundert pl bis zu einigen µl.  Die Mikro-Pipette ermöglicht die Aufnahme von Fluiden, Fluidgemischen oder den gegebenenfalls in ihnen enthaltenen Mikropartikeln, deren Abtransport in das Innere komplexer Systeme sowie die zielgerichtete Abgabe der aufgenommenen Stoffe an den Ort einer Probenweiterverarbeitung bzw. eines Probenabfalls. 
Die elektrisch steuerbare Mikro-Pipette besteht aus einer mit einer inerten Trägerflüssigkeit befüllten Mikroejektionspumpe, welche aus einer mikrotechnisch hergestellten Kammer mit einer einen elektrisch ansteuerbaren Aktuator aufweisenden elastischen Kammerwand  (Mikromembranpumpe) aufgebaut ist,  deren Mikroauslaufkapillare als Pipettenspitze ausgebildet ist
Die erfindungsgemäße, elektrisch ansteuerbaren Mikro-Pipette wird mittels der Technologien der Mikrosystemtechnik hergestellt, sie kann als Hybridaufbau aus mehreren Einzelchips zum System Mikro-Pipette integriert werden, oder auch kompakt in nur einen Silizium-Chip integriert sein. Grundsätzlich eignen sich beide Fertigungsalternativen für die Massenproduktion und zeichnen sich durch extrem hohe Genauigkeit und Reproduzierbarkeit aus. Der Einsatz der erfindungsgemäßen Mikro-Pipette führt je nach Anwendung zu einer Verringerung des Totvolumens bzw. des Medienverbrauchs. Aufgrund des Fehlens mechanisch bewegter Teile weist sie eine  extrem hohe Zuverlässigkeit und wartungsfreie Standzeit auf. ]]></dc:description>
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<dc:title><![CDATA[Elektrisch steuerbare Mikro-Pipette]]></dc:title>
<dc:source><![CDATA[EP 0 725 267 A 3]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Die Erfindung betrifft eine elektrisch steuerbare Mikro-Pipette zur Handhabung kleinster Fluidvolumina im Bereich von einigen hundert pl bis zu einigen µl.  Die Mikro-Pipette ermöglicht die Aufnahme von Fluiden, Fluidgemischen oder den gegebenenfalls in ihnen enthaltenen Mikropartikeln, deren Abtransport in das Innere komplexer Systeme sowie die zielgerichtete Abgabe der aufgenommenen Stoffe an den Ort einer Probenweiterverarbeitung bzw. eines Probenabfalls. 
Die elektrisch steuerbare Mikro-Pipette besteht aus einer mit einer inerten Trägerflüssigkeit befüllten Mikroejektionspumpe, welche aus einer mikrotechnisch hergestellten Kammer mit einer einen elektrisch ansteuerbaren Aktuator aufweisenden elastischen Kammerwand  (Mikromembranpumpe) aufgebaut ist,  deren Mikroauslaufkapillare als Pipettenspitze ausgebildet ist
Die erfindungsgemäße, elektrisch ansteuerbaren Mikro-Pipette wird mittels der Technologien der Mikrosystemtechnik hergestellt, sie kann als Hybridaufbau aus mehreren Einzelchips zum System Mikro-Pipette integriert werden, oder auch kompakt in nur einen Silizium-Chip integriert sein. Grundsätzlich eignen sich beide Fertigungsalternativen für die Massenproduktion und zeichnen sich durch extrem hohe Genauigkeit und Reproduzierbarkeit aus. Der Einsatz der erfindungsgemäßen Mikro-Pipette führt je nach Anwendung zu einer Verringerung des Totvolumens bzw. des Medienverbrauchs. Aufgrund des Fehlens mechanisch bewegter Teile weist sie eine  extrem hohe Zuverlässigkeit und wartungsfreie Standzeit auf. ]]></dc:description>
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<dc:creator><![CDATA[Fan, J.]]></dc:creator>
<dc:creator><![CDATA[Ding, G.]]></dc:creator>
<dc:creator><![CDATA[Fung, S.]]></dc:creator>
<dc:creator><![CDATA[Xie, Z.]]></dc:creator>
<dc:creator><![CDATA[Zhong, Y.]]></dc:creator>
<dc:creator><![CDATA[Wong, K.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Grambole, D.]]></dc:creator>
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<dc:title><![CDATA[Shallow acceptor and hydrogen impurity in p-type arsenic-doped ZnMgO films grown by radio frequency magnetron sputtering]]></dc:title>
<dc:source><![CDATA[Semiconductor Science and Technology 25(2010)8, 085009]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Arsenic-doped ZnMgO films were fabricated on SiO<sub>2</sub> by the radio frequency magnetron sputtering technique at different substrate temperatures during growth. The yielded films were characterized by room temperature Hall measurement, x-ray diffraction, x-ray photoelectron spectroscopy, scanning electron microscopy, secondary ion mass spectroscopy, nuclear reaction analysis and low-temperature photoluminescence. As-doped samples grown at low substrate temperature (350 degrees C) were n-type conducting (n similar to 10<sup>18</sup> cm<sup>-3</sup>), with evidence showing that the hydrogen impurity was an important shallow donor associated with the observed n-type conduction. Conversion of n-type to p-type conduction being observed at the substrate temperature of similar to 400 degrees C was associated with the formation of the As<sub>Zn</sub>(V<sub>Zn</sub>)<sub>2</sub> shallow acceptor complex and the drastic reduction of the hydrogen content.]]></dc:description>
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<dc:creator><![CDATA[Kögler, R.]]></dc:creator>
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<dc:title><![CDATA[Spatial distribution of gettering centres in ion-implanted and annealed silicon]]></dc:title>
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Aug.  31 - Sept. 4, 1998]]></dc:source>
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<dc:creator><![CDATA[Hensel, F.]]></dc:creator>
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<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
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<dc:title><![CDATA[Verfahren zur Messung der integralen Massenfeuchte in Zweiphasenströmungen]]></dc:title>
<dc:source><![CDATA[DE P 4 423 665 A1]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[Es wird ein Verfahren zur Messung der Massenfeuchte von in Rohrleitungen geführten Zweiphasenströmungen (gasförmig/flüssig) mit kleinem Massenstromanteil der flüssigen Phase (<30%) beschrieben, dadurch gekennzeichnet, dass die Positronen in die Strömung emittiert werden und die bei der Annihilation der in die Strömung emittierten Positronen entstehende Gamma-Strahlung in Abhängigkeit von der Entfernung des Annihilationsortes von der Positronenquelle gemessen wird und dadurch, dass die Form der Reichweitenverteilung der Positronen zur Bestimmung der Massenfeuchte verwendet wird.]]></dc:description>
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<identifier>HZDR:PUBLDB:765-1</identifier>
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<dc:creator><![CDATA[Böhmer, B.]]></dc:creator>
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<dc:title><![CDATA[Influence of Input Neutron Spectrum Covariances on Results of Pressure Vessel Neutron Spectrum Adjustments]]></dc:title>
<dc:source><![CDATA[9th International Symposium on Reactor Dosimetry, Sept. 2-6, 1996, Prague
Eds H. Ait Abderrahim, P. D'hondt, B. Osmera, World Scientific Publishing, Singapore (1998) ISBN 981-02-3346-9, pp 294-301]]></dc:source>
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<dc:description><![CDATA[One of the most critical problems in practical applications of spectrum adjustment in pressure vessel dosimetry is the insufficient knowledge of the input spectrum covariance matrix. Usually very crude approximations for this covariance matrix are used in adjustment procedures and, moreover, it is not clear to which extent these approximations influence the final results. Therefore it appeared useful to calculate this matrix as carefully as possible for a typical system and in positions for which a sufficient amount of activation measurements and precise transport calculations was available. The paper presents and discusses results of such calculations for a VVER-1000 type reactor. They base on the one hand on sensitivity coefficients estimated in transport calculations by means of the ANISN code and on the other hand on cross section covariance data taken from the Obninsk ABBN-93 data library. The results of spectrum adjustments based on the estimated covariance matrix are compared with results based on formerly used matrices. The obtained differences are discussed. ]]></dc:description>
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<dc:title><![CDATA[Influence of Input Neutron Spectrum Covariances on Results of Pressure Vessel Neutron Spectrum Adjustments]]></dc:title>
<dc:source><![CDATA[9th International Symposium on Reactor Dosimetry, Sept. 2-6, 1996, Prague
Eds H. Ait Abderrahim, P. D'hondt, B. Osmera, World Scientific Publishing, Singapore (1998) ISBN 981-02-3346-9, pp 294-301]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[One of the most critical problems in practical applications of spectrum adjustment in pressure vessel dosimetry is the insufficient knowledge of the input spectrum covariance matrix. Usually very crude approximations for this covariance matrix are used in adjustment procedures and, moreover, it is not clear to which extent these approximations influence the final results. Therefore it appeared useful to calculate this matrix as carefully as possible for a typical system and in positions for which a sufficient amount of activation measurements and precise transport calculations was available. The paper presents and discusses results of such calculations for a VVER-1000 type reactor. They base on the one hand on sensitivity coefficients estimated in transport calculations by means of the ANISN code and on the other hand on cross section covariance data taken from the Obninsk ABBN-93 data library. The results of spectrum adjustments based on the estimated covariance matrix are compared with results based on formerly used matrices. The obtained differences are discussed. ]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Böhmer, B.]]></dc:creator>
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<dc:title><![CDATA[Neutron Spectrum Covariances and their Influence on Results of Pressure Vessel Neutron Spectrum Adjustments]]></dc:title>
<dc:source><![CDATA[Voprosy Atomnoi Nauki i Techniki, Seriya Jadernye Konstanty, 1998, Vypusk 1, p. 28-34, Ed. ZNIIatominform, Moscow]]></dc:source>
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<dc:title><![CDATA[Computer-simulation and RBS/C studies of high-dose N<SUP>+</SUP> and Al<SUP>+</SUP> co-implantation in 6H-SiC]]></dc:title>
<dc:source><![CDATA[Techn. Phys. Lett. 23 (1997) 617
(Russian version - Pis'ma v ZhTF 23 (No 16) (1997) 6)]]></dc:source>
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<dc:title><![CDATA[Vergleichende Untersuchungen der Funktionalität von synthetischen Huminsäuren und Aldrich-Huminsäure]]></dc:title>
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<dc:title><![CDATA[Laser lnduced Photoacoustic Spectroscopy using Solid State Tunable Lasers (OPO)]]></dc:title>
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<dc:title><![CDATA[XAS-Datenanalyse mit Hilfe von FEFF-Rechnungen]]></dc:title>
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<dc:creator><![CDATA[Dementjev, A. P.]]></dc:creator>
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<dc:title><![CDATA[Electron spectroscopy for chemical analysis Investigation of the Interaction of uranyl and calcium ions with humic acids]]></dc:title>
<dc:source><![CDATA[Inorganica Chimica Acta 273 (1998) 234-237]]></dc:source>
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<dc:creator><![CDATA[Hackstein, G.]]></dc:creator>
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<dc:title><![CDATA[Elektroenergieerzeugung aus erneuerbaren Energiequellen in Sachsen]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-193 August 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Im Bericht werden die Potentiale zur Elektroenergieerzeugung aus verschiedenen erneuerbaren Energiequellen in Sachsen zusammengestellt. Dabei werden natürliche Potentiale und - wo möglich - technische Potentiale sowie wirtschaftliche Potentiale unterschieden. Das ermittelte technische Potential (ohne Biomasse) entspricht etwa einer Elektroenergieproduktion von 7400 GWh jährlich. Davon entfallen etwa 2/3 auf die Windenergie und der Rest zu gleichen Teilen auf die Wasserkraft und die Photovoltaik.
Die Erschließung der Potentiale seit 1990 wird im Einzelnen dargestellt. Neben der seit langem genutzten Wasserkraft entwickelt sich insbesondere die Windenergie sehr dynamisch. Die Windenergie wird noch 1997 die Wasserkraft als bedeutendste erneuerbare Energie in Sachsen ablösen. Die weitere Nutzung dieser beiden Energiequellen stößt allerdings auf zunehmende ökologische Bedenken bzw. Widerstände.
Der Anteil der erneuerbaren Energiequellen am Elektroenergieverbrauch in Sachsen erreichte 1996 etwa 1,3 %. Bis zum Jahr 2000 erscheint eine Vergrößerung dieses Anteils auf ca. 5 % möglich.
]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Shuh, D. K.]]></dc:creator>
<dc:creator><![CDATA[Kaltsoyannis, N.]]></dc:creator>
<dc:creator><![CDATA[Bucher, J. J.]]></dc:creator>
<dc:creator><![CDATA[Edelstein, N. M.]]></dc:creator>
<dc:creator><![CDATA[Clark, D. L.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Hudson, E. A.]]></dc:creator>
<dc:creator><![CDATA[Mahamid, A.]]></dc:creator>
<dc:creator><![CDATA[Torretto, P.]]></dc:creator>
<dc:creator><![CDATA[Lukens, W. W.]]></dc:creator>
<dc:creator><![CDATA[Roberts, K.]]></dc:creator>
<dc:creator><![CDATA[Yee, B. C.]]></dc:creator>
<dc:creator><![CDATA[Carlson, D. E.]]></dc:creator>
<dc:creator><![CDATA[Yee, A.]]></dc:creator>
<dc:creator><![CDATA[Buchanan, B. B.]]></dc:creator>
<dc:creator><![CDATA[Leighton, T.]]></dc:creator>
<dc:creator><![CDATA[Yang, W.-S.]]></dc:creator>
<dc:creator><![CDATA[Bryan, J. C.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-617-1</dc:identifier>
<dc:title><![CDATA[Environmental Applications of XANES: Speciation of Tc in Cement after Chemical Treatment and Se after Bacterial Uptake]]></dc:title>
<dc:source><![CDATA[Mater. Res. Soc. Symp. Proc. 344 (1995)]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:language>eng</dc:language>
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<header>
<identifier>HZDR:PUBLDB:2257-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Näser, A.]]></dc:creator>
<dc:creator><![CDATA[Gehlhoff, W.]]></dc:creator>
<dc:creator><![CDATA[Overhof, H.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2257-1</dc:identifier>
<dc:title><![CDATA[EPR identification of a shallow donor state of cadmium in silicon]]></dc:title>
<dc:source><![CDATA[8th Int. Conf. on Shallow Level Centres in Semiconductors, Montpellier, France, July 27-30, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:857-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-857-1</dc:identifier>
<dc:title><![CDATA[Nachweis verformungsbedingter Strukturschädigung in Rißnähe durch Röntgenkleinwinkelstreuung]]></dc:title>
<dc:source><![CDATA[29. DVM-Tagung Bruchvorgänge, Februar 1997, Stuttgart, S. 299 ff.]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:857-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-857-7</dc:identifier>
<dc:title><![CDATA[Nachweis verformungsbedingter Strukturschädigung in Rißnähe durch Röntgenkleinwinkelstreuung]]></dc:title>
<dc:source><![CDATA[29. DVM-Tagung Bruchvorgänge, Februar 1997, Stuttgart, S. 299 ff.]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1005-1</identifier>
<datestamp>2023-04-26</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Enghardt, W.]]></dc:creator>
<dc:creator><![CDATA[Debus, J.]]></dc:creator>
<dc:creator><![CDATA[Haberer, T.]]></dc:creator>
<dc:creator><![CDATA[Hasch, B.-G.]]></dc:creator>
<dc:creator><![CDATA[Hinz, R.]]></dc:creator>
<dc:creator><![CDATA[Jäkel, O.]]></dc:creator>
<dc:creator><![CDATA[Krämer, M.]]></dc:creator>
<dc:creator><![CDATA[Lauckner, K.]]></dc:creator>
<dc:creator><![CDATA[Pawelke, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1005-1</dc:identifier>
<dc:title><![CDATA[The application of PET to quality assurance of heavy-ion tumour therapy.]]></dc:title>
<dc:source><![CDATA[Strahlentherapie und Onkologie, Vol. 175, Suppl. II (1999) 33-36]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[At the new heavy ion tumor therapy facility of the Gesellschaft für Schwerionenforschung at Darmstadt positron emission tomography (PET) has been implemented for in-beam and in-situ therapy control, i.e. during the tumor irradiation. The components necessary for this dedicated PET-imaging and their integration into the framework of therapy planning and quality assurance of heavy ion cancer treatments are presented. Results of the first application of this PET-method to patient treatments are reported.]]></dc:description>
<dc:subject><![CDATA[heavy-ion therapy]]></dc:subject>
<dc:subject><![CDATA[positron emission tomography]]></dc:subject>
<dc:subject><![CDATA[treatment planning]]></dc:subject>
<dc:subject><![CDATA[quality assurance]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1007/BF03038884]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1005-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:3186-1</identifier>
<datestamp>2025-12-09</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Nock, B.]]></dc:creator>
<dc:creator><![CDATA[Maina, T.]]></dc:creator>
<dc:creator><![CDATA[Tsortos, A.]]></dc:creator>
<dc:creator><![CDATA[Pelecanou, M.]]></dc:creator>
<dc:creator><![CDATA[Raptopoulou, C. P.]]></dc:creator>
<dc:creator><![CDATA[Papadopoulos, M.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Stassinopoulou, C.]]></dc:creator>
<dc:creator><![CDATA[Terzis, A.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Nounesis, G.]]></dc:creator>
<dc:creator><![CDATA[Chiotellis, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3186-1</dc:identifier>
<dc:title><![CDATA[Glutathione interaction with SNS/S mixed ligand complexes of oxorhenium(V): Kinetic aspects and characterization of the products]]></dc:title>
<dc:source><![CDATA[Inorganic Chemistry 39 (2000) 4433-4441]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[A series of oxorhenium(V) SNS/S mixed ligand complexes [ReO(L<SUP>n</SUP>/L)] carrying different types of tridentate ligand [L<SUP>1</SUP>: C<SUB>2</SUB>H<SUB>5</SUB>N(CH<SUB>2</SUB>CH<SUB>2</SUB>S)<SUB>2</SUB>, L<SUP>2</SUP>: (C<SUB>2</SUB>H<SUB>5</SUB>)<SUB>2</SUB>NCH<SUB>2</SUB>CH<SUB>2</SUB>N(CH<SUB>2</SUB>CH<SUB>2</SUB>S)<SUB>2</SUB>, L<SUP>3</SUP>: C<SUB>2</SUB>H<SUB>5</SUB>SCH<SUB>2</SUB>CH<SUB>2</SUB>N(CH<SUB>2</SUB>CH<SUB>2</SUB>S)<SUB>2</SUB> and L<SUP>4</SUP>: 2,6-(SCH<SUB>2</SUB>)<SUB>2</SUB>NC<SUB>5</SUB>H<SUB>3</SUB>] and the same monodentate coligand (L: C<SUB>6</SUB>H<SUB>5</SUB>S) have been synthesized and characterized by spectroscopic methods and elemental analyses. X-ray structure determination was performed for complexes 3 and 4. Complex 3 adopts the expected distorted trigonal bipyramidal geometry around the metal in a syn configuration, while complex 4, due to the aromatic character of the nitrogen of the SNS donor-atom set, exhibits a distorted square pyramidal geometry. The interaction of complexes 1 - 4 with glutathione (GSH) was studied by high performance liquid chromatography (HPLC), revealing the rapid formation of the respective daughter complexes 5 - 8, wherein the L coligand has been substituted by GS. The daughter complexes 5 - 8 have been characterized by ES-MS and a battery of NMR measurements involving HETCOR, COSY and NOESY procedures. Kinetic aspects of the interaction of complexes 1 ¾ 3 with GSH have been studied by isothermal titration microcalorimetry providing direct measurements of the interaction rate constants as well as the total enthalpy change. The reaction of complex 1 is characterized by the slowest and that of complex 2 by the fastest rate. This is in agreement with previously reported trends for analogous <SUP>99m</SUP>Tc complexes.]]></dc:description>
<dc:subject><![CDATA[oxorhenium complexes]]></dc:subject>
<dc:subject><![CDATA[X-ray structure determination]]></dc:subject>
<dc:subject><![CDATA[glutathion exchange]]></dc:subject>
<dc:subject><![CDATA[kinetic and thermodynamic investigations]]></dc:subject>
<dc:subject><![CDATA[microcalorimetry]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:3539-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grants, I.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Pätzold, O.]]></dc:creator>
<dc:creator><![CDATA[Wunderwald, U.]]></dc:creator>
<dc:creator><![CDATA[Jenkner, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3539-1</dc:identifier>
<dc:title><![CDATA[Linearization approaches in VGF models: decoupling global radiation transfer and the Stefan problem]]></dc:title>
<dc:source><![CDATA[DGKK-Jahrestagung, Freiberg, 11-12.10.2000]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Simplified theoretical models are presented for the highly coupled phenomena of heat transfer, convection and solidification during VGF crystal growth. The models are essential in order to inverse the general approach: optimal conditions at the solidification front can be translated into temperature conditions at the heaters and the corresponding heater regimes. The Stefan problem of the unknown geometry of the solidification front is solved in a simplified analytical way in good approximation with the full numerical solution.]]></dc:description>
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<dc:language>eng</dc:language>
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<header>
<identifier>HZDR:PUBLDB:2571-1</identifier>
<datestamp>2025-12-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Denner, V.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Mathon, M.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2571-1</dc:identifier>
<dc:title><![CDATA[Irradiation-induced structural changes in surveillance material of VVER 440-type weld metal]]></dc:title>
<dc:source><![CDATA[Journal of Nuclear Materials 277 (2000) 280-287]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The irradiation-induced microstructural changes in surveillance materials of the VVER 
440-type weld metal Sv-10KhMFT were investigated by small angle neutron scattering 
(SANS) and anomalous small angle X-ray scattering (SAXS). Due to the high fluence 
a strong effect was found in the SANS experiment. No significant effect of the irradiationis detected by SAXS. The reason of this discrepancy is the different 
scattering contrast of irradiation-induced defects for neutron and X-rays. An analysis 
of the small angle X-ray scattering shows that the scattering intensity is mainly caused by vanadium-containing precipitates and grain boundaries. Both types of scattering defects are hardly changed by irradiation. Neutron irradiation rather produces additional scattering defects of few nanometers in size. Assuming these defects are clusters containing copper and other foreign atoms with a composition according to results of atom probe field ion microscopy investigations, both the high SANS and the low SAXS effect can be explained. ]]></dc:description>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1524/ract.2000.88.9-11.723]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:2572-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2572-1</dc:identifier>
<dc:title><![CDATA[Anlagentechnik für die Plasmaimmersions-Ionenimplantation]]></dc:title>
<dc:source><![CDATA[Anwenderforum AWS, Meisdorf, December 12, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2572-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1019-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Werner, M.]]></dc:creator>
<dc:creator><![CDATA[Bulavin, V.]]></dc:creator>
<dc:creator><![CDATA[Pavelko, V.]]></dc:creator>
<dc:creator><![CDATA[Gutsev, D.]]></dc:creator>
<dc:creator><![CDATA[Anikin, G.]]></dc:creator>
<dc:creator><![CDATA[Usanov, A.]]></dc:creator>
<dc:creator><![CDATA[Dodonov, V.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-1019-1</dc:identifier>
<dc:title><![CDATA[Entwicklung von theoretischen Schwingungsmodellen für WWER-Reaktoren auf der Grundlage der Finite-Elemente-Methode]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-196 Oktober 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[In diesem Abschlußbericht wird ein Fördervorhaben beschrieben, welches auf die Unterstützung von 6 russischen Wissenschaftlern aus drei unterschiedlichen Institutionen abzielte. Ihre Arbeiten zur Anlagendiagnostik / Schadensfrüherkennung dienen der Erhöhung der Sicherheit von WWER-Reaktoren.
	Das Vorhaben leistet einen Beitrag zur verbesserten Beurteilung der mechanischen Integrität von Reaktoren der russischen WWER-440 und WWER-1000 Baureihe, insbesondere zur empfindlichen Früherkennung und Lokalisation mechanischer Schädigungen an Reaktorkomponenten mit Hilfe schwingungsdiagnostischer Methoden. Zu diesem Zweck wurde das Finite-Element-Modell zur Simulation des mechanischen Schwingungsverhaltens aller Primärkreiskomponenten eines WWER-1000 erstellt. Dafür wurde das Programmpaket ANSYS® genutzt.
	Das Berechnungsmodell zum WWER-440 wurde mit neueren Ergebnissen experimenteller Schwingungsuntersuchungen weiter justiert.  Das Modell kann in der Hauptsache genutzt werden, um zu klären, wie sich unterstellte mechanische Defekte von Reaktoreinbauten auf die Schwingungen der Gesamtanlage auswirken. Diese Schadenssimulation ist besonders geeignet, empfindliche Meßpositionen für die on-line Überwachung zu finden und physikalisch fundierte Grenzwerte zu definieren. ]]></dc:description>
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<dc:creator><![CDATA[Möller, W.]]></dc:creator>
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<dc:title><![CDATA[Neue Technologien der Ionenimplantation]]></dc:title>
<dc:source><![CDATA[Ruhr-Universität Bochum, Fakultät für Physik, April 20, 1998]]></dc:source>
<dc:date>1998</dc:date>
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<dc:creator><![CDATA[Fietz, J.]]></dc:creator>
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<dc:title><![CDATA[Environmentel radioactive contamination caused by the uranium extraction industry and problems of site remediation in the East European countries]]></dc:title>
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<dc:title><![CDATA[Plasma immersion and low-energy ion implantation for the nitriding of metal surfaces]]></dc:title>
<dc:source><![CDATA[Charles University Prag, Dept. of Polymer Physics, Oct. 26, 1998]]></dc:source>
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<dc:creator><![CDATA[Fietz, J.]]></dc:creator>
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<dc:title><![CDATA[Der Unfall von Tschernobyl und seine Folgen - eine Bilanz aus heutiger Sicht]]></dc:title>
<dc:source><![CDATA[Zentrumskollqium des FZR, Rossendorf, 27.3.1996]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Mrotschek, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2597-1</dc:identifier>
<dc:title><![CDATA[Oberflächenmodifizierung von Hartmetallen mittels Bor-Implantation]]></dc:title>
<dc:source><![CDATA[Weißrussische Universität Minsk, July 28, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Hebert, J. P.]]></dc:creator>
<dc:creator><![CDATA[Daroussin, J. L.]]></dc:creator>
<dc:creator><![CDATA[Michel, P.]]></dc:creator>
<dc:creator><![CDATA[Perih, C.]]></dc:creator>
<dc:creator><![CDATA[Lozano Martinez, F.]]></dc:creator>
<dc:creator><![CDATA[Lopez Romero, A.]]></dc:creator>
<dc:creator><![CDATA[Fietz, J.]]></dc:creator>
<dc:creator><![CDATA[Langer, L.]]></dc:creator>
<dc:creator><![CDATA[Kahn, A.]]></dc:creator>
<dc:creator><![CDATA[Litvin, V.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2598-1</dc:identifier>
<dc:title><![CDATA[Decommissioning of old uranium ore extraction and traetment installations]]></dc:title>
<dc:source><![CDATA[Contract No FI2D/CT93/0083, Final Report, EUR 16885 EN, ISBN 92-827-6823-6, ECSC-EC-EAEC, Brussels-Luxembourg 1996]]></dc:source>
<dc:date>1996</dc:date>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Neelmeijer, C.]]></dc:creator>
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<dc:title><![CDATA[The scientific analysis of Böttger stoneware at the Research Center Rossendorf (Dresden, Germany)]]></dc:title>
<dc:source><![CDATA[1st Int. Workshop on the non-destructive characterisation of Böttger stoneware, J. Paul Getty Museum - Los Angeles/Cal., Nov. 1998]]></dc:source>
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<dc:creator><![CDATA[Fietz, J.]]></dc:creator>
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<dc:creator><![CDATA[Niese, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2600-1</dc:identifier>
<dc:title><![CDATA[LOWRAD 96, Methods and Applications of Low-Level Radioactivity Measurements]]></dc:title>
<dc:source><![CDATA[Proceedings of a Workshop, Rossendorf / Dresden, 7 - 8 November 1996]]></dc:source>
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<dc:creator><![CDATA[Fietz, J.]]></dc:creator>
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<dc:title><![CDATA[LOWRAD 96, Methods and Applications of Low-Level Radioactivity Measurements]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-170, March 1997]]></dc:source>
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<dc:creator><![CDATA[Fietz, J.]]></dc:creator>
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<dc:title><![CDATA[The Rossendorf Research Site]]></dc:title>
<dc:source><![CDATA[LOWRAD 96, Methods and Applikations of Low-Level Radioactivity Measurements, Rossendorf / Dresden, 7 - 8 November 1996]]></dc:source>
<dc:date>1996</dc:date>
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<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2987-1</dc:identifier>
<dc:title><![CDATA[Blue Light Emission from Ion Beam Synthesized Semiconductor Nanoclusters in SiO<SUB>2</SUB> Films]]></dc:title>
<dc:source><![CDATA[25th Annual Conference of the IEEE Industrial Electronics Society, IECON '99,
Nov. 29 - Dec. 3, 1999, San Jose, USA]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Due to quantum confinement and surface effects semiconductor nanoparticles exhibit properties, which considerably differ to that of the bulk material. The topic of light emission from ion beam synthesized semiconductor nanoclusters is focused on recent success in extracting strong violet / blue photo- and electroluminescence from Si- or Ge- implanted SiO<SUB>2</SUB> layers on Si.]]></dc:description>
<dc:subject><![CDATA[luminescence]]></dc:subject>
<dc:subject><![CDATA[ion beam synthesis]]></dc:subject>
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<dc:subject><![CDATA[optoelectronics]]></dc:subject>
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<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-466-1</dc:identifier>
<dc:title><![CDATA[Erweitertes Überwachungsprogramm der Strahlenversprödung durch Probenrekonstitution]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik 1996, Mannheim, 1996, Tagungsbericht, S. 172 ff.]]></dc:source>
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<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-466-7</dc:identifier>
<dc:title><![CDATA[Erweitertes Überwachungsprogramm der Strahlenversprödung durch Probenrekonstitution]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik 1996, Mannheim, 1996, Tagungsbericht, S. 172 ff.]]></dc:source>
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<dc:creator><![CDATA[Poggi, G.]]></dc:creator>
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<dc:creator><![CDATA[Belayev, I. M.]]></dc:creator>
<dc:creator><![CDATA[Berger, L.]]></dc:creator>
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<dc:creator><![CDATA[Boussange, S.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-650-1</dc:identifier>
<dc:title><![CDATA[Evidence for collective expansion in light-particle emission following Au + Au collisions at 100, 150 and 250 A MeV]]></dc:title>
<dc:source><![CDATA[Nuclear Physics A 586 (1995) pp. 755]]></dc:source>
<dc:date>1995</dc:date>
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<dc:creator><![CDATA[Lips, V.]]></dc:creator>
<dc:creator><![CDATA[Barth, R.]]></dc:creator>
<dc:creator><![CDATA[Oeschler, H.]]></dc:creator>
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<dc:creator><![CDATA[Karnaukhov, V. A.]]></dc:creator>
<dc:creator><![CDATA[Kuznetsov, L. A.]]></dc:creator>
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<dc:creator><![CDATA[Karcz, W.]]></dc:creator>
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<dc:creator><![CDATA[Norbeck, E.]]></dc:creator>
<dc:creator><![CDATA[Gross, C. J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-675-1</dc:identifier>
<dc:title><![CDATA[Evidence for simultaneous breakup in reactions with relativistic alpha-projectiles]]></dc:title>
<dc:source><![CDATA[Physics Letters B 338 (1994) pp.141]]></dc:source>
<dc:date>1994</dc:date>
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<header>
<identifier>HZDR:PUBLDB:980-1</identifier>
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<dc:creator><![CDATA[Denecke, M. A.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:creator><![CDATA[Bubner, M.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:creator><![CDATA[Allen, P. G.]]></dc:creator>
<dc:creator><![CDATA[Bucher, J. J.]]></dc:creator>
<dc:creator><![CDATA[Edelstein, N. M.]]></dc:creator>
<dc:creator><![CDATA[Shuh, D. K.]]></dc:creator>
<dc:creator><![CDATA[Czerwinski, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-980-1</dc:identifier>
<dc:title><![CDATA[EXAFS Investigations of the Interaction of Humic Acids and Model Compounds with Uranyl Cations in Solid Complexes]]></dc:title>
<dc:source><![CDATA[Migration '97 Konferenz, 26.-31. Oktober, Sendai, Japan]]></dc:source>
<dc:date>1997</dc:date>
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<header>
<identifier>HZDR:PUBLDB:980-2</identifier>
<datestamp>2023-04-27</datestamp>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Denecke, M. A.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:creator><![CDATA[Bubner, M.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:creator><![CDATA[Allen, P. G.]]></dc:creator>
<dc:creator><![CDATA[Bucher, J. J.]]></dc:creator>
<dc:creator><![CDATA[Edelstein, N. M.]]></dc:creator>
<dc:creator><![CDATA[Shuh, D. K.]]></dc:creator>
<dc:creator><![CDATA[Czerwinski, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-980-2</dc:identifier>
<dc:title><![CDATA[EXAFS Investigations of the Interaction of Humic Acids and Model Compounds with Uranyl Cations in Solid Complexes]]></dc:title>
<dc:source><![CDATA[Radiochim. Acta 82, 103 (1998)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1524/ract.1998.82.special-issue.103]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:86-1</identifier>
<datestamp>2020-11-05</datestamp>
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<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Winter, G.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:creator><![CDATA[Reif, J.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Döring, J.]]></dc:creator>
<dc:creator><![CDATA[Wirowski, R.]]></dc:creator>
<dc:creator><![CDATA[Nicolay, N.]]></dc:creator>
<dc:creator><![CDATA[Brentano, P.]]></dc:creator>
<dc:creator><![CDATA[Grawe, H.]]></dc:creator>
<dc:creator><![CDATA[Schubart, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-86-1</dc:identifier>
<dc:title><![CDATA[Excited states built on the 6- isomer in ...]]></dc:title>
<dc:source><![CDATA[Physical Review C 49 (1994) pp. 2427]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevC.49.2427]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:2911-1</identifier>
<datestamp>2019-03-04</datestamp>
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</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Höfgen, A.]]></dc:creator>
<dc:creator><![CDATA[Heera, V.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2911-1</dc:identifier>
<dc:title><![CDATA[Ion beam induced nanocrystallization of SiC]]></dc:title>
<dc:source><![CDATA[Mat. Sci. Forum 388 (2000) 897]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Ion-beam-induced crystallization (IBIC) was used to produce nanocrystals in the preamorphized region of a 6H-SiC bulk crystal. The precipitation was stimulated by high dose implantation with Al and Si at temperatures between 300 °C and 700 °C. The morphology of the nanocrystalline phase and its dependence on the implantation parameters were investigated by cross-sectional transmission electron microscopy (XTEM). Above a certain threshold dose, randomly oriented grains of 3C-SiC with almost spherical shape and mean diameters ranging from 4 to 25 nm are formed. The recrystallization is completed within a very narrow time window. Therefore, in our experiments the nucleation and growth process could not be observed directly. From the extrapolation of the kinetics of the secondary grain growth to zero time the window of suitable parameters for the observation of nucleation and primary grain growth was estimated. A critical temperature (TC  300 °C) as well as an incubation time (tI  300 s below 700°C) for the beginning of the recrystallization were found.]]></dc:description>
<dc:subject><![CDATA[ion implantation]]></dc:subject>
<dc:subject><![CDATA[amorphization]]></dc:subject>
<dc:subject><![CDATA[recrystallization]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:3093-1</identifier>
<datestamp>2019-03-04</datestamp>
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</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Schmidt-Brücken, B.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3093-1</dc:identifier>
<dc:title><![CDATA[Rhenium Compounds Containing Heterocyclic Thiols - Syntheses and Structures]]></dc:title>
<dc:source><![CDATA[Anorganische allg. Chemie]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Reactions of trans-[ReOCl3(PPh3)2] with 1,3-thiazoline-2-thiol (thiazSH), pyridine-2-thiol (pyrSH) or pyrimidine-2-thiol (pyrmSH) result in the formation of rhenium(V) oxo complexes or rhenium(III) species depending on the conditions applied. mer-[ReOCl3(thiazSH)(OPPh3)], trans-[ReCl3(PPh3)(thiazSH)2], [ReO(2-propO)(PPh3)Cl(pyrS-S,N)], cis-[ReCl2(PPh3)2(pyrS-S,N)] and [ReCl2(PPh3)2(pyrmS-S,N)] have been isolated from such reactions and structurally characterized.
cis-[ReCl2(PPh3)2(pyrS-S,N)] and [ReCl2(PPh3)2(pyrmS-S,N)] are obtained in better yields by ligand substitution on trans-[ReCl3(MeCN)(PPh3)2]. The reaction between (n-Bu4N)[ReOCl4] and purine-6-thiole (purinSH) results in the formation of the oxo-bridged [O{ReO(purinS-S,N)2}2].]]></dc:description>
<dc:subject><![CDATA[Rhenium Complexes]]></dc:subject>
<dc:subject><![CDATA[Heterocyclic Thiols]]></dc:subject>
<dc:subject><![CDATA[Crystal Structures]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2929-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2929-1</dc:identifier>
<dc:title><![CDATA[Development of <SUP>99m</SUP>Tc complexes for imaging the serotonin-5HT<SUB>1A</SUB> and -5HT<SUB>2A</SUB> receptors in the Central Nervous System]]></dc:title>
<dc:source><![CDATA[Meeting COST B12 Action, WG5, Barcelona, 14.10.1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<identifier>HZDR:PUBLDB:2926-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Stephan, H.]]></dc:creator>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:creator><![CDATA[Seidel, J.]]></dc:creator>
<dc:creator><![CDATA[Wolf, G.]]></dc:creator>
<dc:creator><![CDATA[Vögtle, F.]]></dc:creator>
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<dc:title><![CDATA[Entwicklung und Charakterisierung Funktionaler Supramolekularer Systeme]]></dc:title>
<dc:source><![CDATA[2. Workshop "Kontaktforum Chemieforschung", VCI Nordost, Dresden, 26./27.10.1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Supramolekulare Systeme mit spezifischen, wohldefinierten Funktionen ermöglichen eine hochselektive Erkennung und Bindung unterschiedlicher Spezies und erschließen damit neue Anwendungsfelder in der Medizin, Analytik, Informations- und Energietechnik sowie in der chemischen Technik. 
Möglichkeiten der selektiven Bindung und gezielten Freisetzung von medizinisch und biologisch relevanten Anionen wie Pertechnetat, Perrhenat und ATP werden am Beispiel photo- und pH-schaltbarer Dendrimere diskutiert. Über die Bildung von Einschlussverbindungen natürlicher helicaler Amyloseeinheiten mit anionischen, kationischen und nichtionischen Tensiden wird berichtet. Die eingesetzten Methoden wie Flüssig-Flüssig-Extraktion, Lipophiliebestimmung und Kalorimetrie gestatten die Charakterisierung kleinster Substanzmengen.

]]></dc:description>
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<datestamp>2025-12-09</datestamp>
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<dc:creator><![CDATA[Pham, M. T.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Reuther, H.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Steiner, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3021-1</dc:identifier>
<dc:title><![CDATA[Hydroxyapatite nucleation on Na ion implanted Ti surfaces]]></dc:title>
<dc:source><![CDATA[Mater. Sci.Lett. 19 (2000) 1029-1031]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Na ions were implanted into pure Ti surfaces. New surface phases were shown to be incorporated into the surface: sodium titanates Na2TiO3 (in the as-implanted state) and Na2Ti6O13 (after 20 min heating at 700 °C in air). A variable level of the surface porosity and roughness was observed depending on the applied ion dose and energy. Upon exposing to simulated body fluid, such ion-implanted surfaces were revealed to enhance hydroxyapatite nucleation and growth.]]></dc:description>
<dc:subject><![CDATA[biomaterial]]></dc:subject>
<dc:subject><![CDATA[titanium]]></dc:subject>
<dc:subject><![CDATA[hydroxyapatite]]></dc:subject>
<dc:subject><![CDATA[surface coating]]></dc:subject>
<dc:subject><![CDATA[ion implantation]]></dc:subject>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Cumblidge, S. E.]]></dc:creator>
<dc:creator><![CDATA[Catchen, G. L.]]></dc:creator>
<dc:creator><![CDATA[Motta, A. T.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
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<dc:title><![CDATA[Effects of Neutron Irradiation and Thermal Annealing on Model Alloys using Positron Annihilation Techniques]]></dc:title>
<dc:source><![CDATA[Effects of Radiation on Materials: 20th International Symposium, ASTM STP 1405, S. T. Rosinski, M. L. Grossbeck, T. R. Allen and A. S. Kumar (Eds.), American Society for Testing and Materials, West Conshohocken, PA, 2001, pp. 247-261]]></dc:source>
<dc:date>2001</dc:date>
<dc:description><![CDATA[We present the results of a systematic investigation of neutron-irradiated and thermally-annealed model alloys using positron annihilation spectroscopy (PAS), including both lifetime and Doppler broadening techniques. The objective of this work is to use PAS to provide information on the irradiation-induced microstructural features that are thought to cause embrittlement in pressure-vessel steels. Such information could complement the results obtained by other techniques, especially small-angle neutron scattering (SANS) and atomic probe field ion microscopy (APFIM). We examined a series of model Fe-based alloys, in which the Cu, P and Ni concentration were systematically varied. These alloys were examined in the as-fabricated state, after irradiation to 1 x 10 19 nxcm-2, and to 8 x 10 19 nxcm-2, and after successive post-irradiation 30-minute isochronal anneals at temperatures ranging from 200 to 600 °C. In each case, we measured the positron annihilation lifetime distribution, the Doppler broadening (S-parameter), and the 15 N Rockwell hardness for the samples. ]]></dc:description>
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<datestamp>2025-12-08</datestamp>
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<dc:creator><![CDATA[Cumblidge, S. E.]]></dc:creator>
<dc:creator><![CDATA[Catchen, G. L.]]></dc:creator>
<dc:creator><![CDATA[Motta, A. T.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3379-7</dc:identifier>
<dc:title><![CDATA[Effects of Neutron Irradiation and Thermal Annealing on Model Alloys using Positron Annihilation Techniques]]></dc:title>
<dc:source><![CDATA[Effects of Radiation on Materials: 20th International Symposium, ASTM STP 1405, S. T. Rosinski, M. L. Grossbeck, T. R. Allen and A. S. Kumar (Eds.), American Society for Testing and Materials, West Conshohocken, PA, 2001, pp. 247-261]]></dc:source>
<dc:date>2001</dc:date>
<dc:description><![CDATA[We present the results of a systematic investigation of neutron-irradiated and thermally-annealed model alloys using positron annihilation spectroscopy (PAS), including both lifetime and Doppler broadening techniques. The objective of this work is to use PAS to provide information on the irradiation-induced microstructural features that are thought to cause embrittlement in pressure-vessel steels. Such information could complement the results obtained by other techniques, especially small-angle neutron scattering (SANS) and atomic probe field ion microscopy (APFIM). We examined a series of model Fe-based alloys, in which the Cu, P and Ni concentration were systematically varied. These alloys were examined in the as-fabricated state, after irradiation to 1 x 10 19 nxcm-2, and to 8 x 10 19 nxcm-2, and after successive post-irradiation 30-minute isochronal anneals at temperatures ranging from 200 to 600 °C. In each case, we measured the positron annihilation lifetime distribution, the Doppler broadening (S-parameter), and the 15 N Rockwell hardness for the samples. ]]></dc:description>
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<dc:creator><![CDATA[Schmeide, K.]]></dc:creator>
<dc:creator><![CDATA[Geipel, G.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2781-1</dc:identifier>
<dc:title><![CDATA[Case-Study: Uranium-Mining Rock Pile No. 250 in the Region Schlema/Alberoda (Saxony, Germany)]]></dc:title>
<dc:source><![CDATA[4<SUP>th</SUP> EU Project Meeting "Effects of Humic Substances on the Migration of Radionuclides: Complexation and Transport of Actinides"
Leuven, Belgium, 19.-20.11.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2780-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Schmeide, K.]]></dc:creator>
<dc:creator><![CDATA[Zorn, T.]]></dc:creator>
<dc:creator><![CDATA[Zänker, H.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2780-1</dc:identifier>
<dc:title><![CDATA[Effect of Humic Substances on the Sorption of Uranium(VI) onto Site-Specific Rock Material]]></dc:title>
<dc:source><![CDATA[EC Project Meeting, Centre d´Etudes de Saclay
Paris, France, 11.-12.05.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2782-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Schmeide, K.]]></dc:creator>
<dc:creator><![CDATA[Pompe, P.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2782-1</dc:identifier>
<dc:title><![CDATA[Effect of Humic Acid on the Uranium Sorption on Phyllite and its Constituents]]></dc:title>
<dc:source><![CDATA[4<SUP>th</SUP> EU Project Meeting "Effects of Humic Substances on the Migration of Radionuclides: Complexation and Transport of Actinides"
Leuven, Belgium, 19.-20.11.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2783-1</dc:identifier>
<dc:title><![CDATA[Analysis of the culturable members of the natural bacterial communities in uranium waste piles]]></dc:title>
<dc:source><![CDATA[Dept. of Geomicrobiology, University of Sofia
Sofia, Bulgaria, 06.06.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<identifier>HZDR:PUBLDB:2784-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2784-1</dc:identifier>
<dc:title><![CDATA[Selective accumulation of heavy metals in drain waters of a uranium waste pile by three indigenous Bacillis strains]]></dc:title>
<dc:source><![CDATA[Institute of Microbiology, Bulgarian Academy of Sciences
Sofia, Bulgaria, 25.06.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<identifier>HZDR:PUBLDB:2785-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2785-1</dc:identifier>
<dc:title><![CDATA[Diversity in natural bacterial populations in the uranium wastes as examined by a 16S rDNA retrieval]]></dc:title>
<dc:source><![CDATA[Inst. of Molecular Biology, Bulgarian Academy of Sciences
Sofia, Bulgaria, 07.10.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<identifier>HZDR:PUBLDB:2786-1</identifier>
<datestamp>2025-12-03</datestamp>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Jungclaus, A.]]></dc:creator>
<dc:creator><![CDATA[Kast, D.]]></dc:creator>
<dc:creator><![CDATA[Lieb, K. P.]]></dc:creator>
<dc:creator><![CDATA[Lingk, C.]]></dc:creator>
<dc:creator><![CDATA[Teich, C.]]></dc:creator>
<dc:creator><![CDATA[Iordanov, O.]]></dc:creator>
<dc:creator><![CDATA[Härtlein, T.]]></dc:creator>
<dc:creator><![CDATA[Schwalm, D.]]></dc:creator>
<dc:creator><![CDATA[Johnstone, I. P.]]></dc:creator>
<dc:creator><![CDATA[Schwengner, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2786-1</dc:identifier>
<dc:title><![CDATA[Magnetic moment measurements in the semi-magic nuclei <SUP>94</SUP>Ru and <SUP>95</SUP>Rh after recoil implantation into iron and nickel]]></dc:title>
<dc:source><![CDATA[European Physical Journal A, 6, 29-36, (1999)]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1007/s100500050313]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2786-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:3400-1</identifier>
<datestamp>2025-12-08</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hennig, C.]]></dc:creator>
<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Panak, P.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Roßberg, A.]]></dc:creator>
<dc:creator><![CDATA[Raff, J.]]></dc:creator>
<dc:creator><![CDATA[Bucher, J.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3400-1</dc:identifier>
<dc:title><![CDATA[EXAFS investigation of uranium(VI) complexes formed at Bacillus cereus and Bacillus sphaericus surfaces]]></dc:title>
<dc:source><![CDATA[Radiochimica Acta 89 (2001), 625-631]]></dc:source>
<dc:date>2001</dc:date>
<dc:description><![CDATA[
Uranium(VI) complex formation at vegetative cells and spores of Bacillus cereus and Bacillus sphaericus was studied using uranium LII-edge and LIII-edge extended x-ray absorption fine structure (EXAFS) spectroscopy. A comparison of the measured equatorial U-O distances and other EXAFS structural parameters of uranyl complexes formed at the Bacillus strains with those of the uranyl structure family indicates that the uranium is predominantly bound as uranyl phosphate.
]]></dc:description>
<dc:subject><![CDATA[EXAFS]]></dc:subject>
<dc:subject><![CDATA[uranium complexation]]></dc:subject>
<dc:subject><![CDATA[bioaccumulation]]></dc:subject>
<dc:subject><![CDATA[Bacillus cereus]]></dc:subject>
<dc:subject><![CDATA[Bacillus sphaericus]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1524/ract.2001.89.10.625]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:3109-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3109-1</dc:identifier>
<dc:title><![CDATA[Ion beam induced nanocrystals - an introduction to nanocrystal session]]></dc:title>
<dc:source><![CDATA[Gordon Research Conference on Materials Processes Far From
Equilibrium, Plymouth, NH, USA, July 11-16, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<header>
<identifier>HZDR:PUBLDB:3110-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Strobel, M.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3110-1</dc:identifier>
<dc:title><![CDATA["Inverse" Ostwald ripening due to ion irradiation: An athermal process studied by Monte Carlo simulations]]></dc:title>
<dc:source><![CDATA[Gordon Research Conference on Materials Processes Far From Equilibrium, Plymouth, NH, USA, July 11-16, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:3111-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hauschild, T.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Jentschel, M.]]></dc:creator>
<dc:creator><![CDATA[Börner, H. G.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3111-1</dc:identifier>
<dc:title><![CDATA[Crystal-GRID: Study of orientation-dependent slowing-down in single-crystalline ZnS]]></dc:title>
<dc:source><![CDATA[14th  Int. Conf. on Ion Beam Analysis (IBA-14) and 6th European Conf. on Accelerators in Applied Research and Technology (ECAART-6),Dresden, Germany, July 26-30, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Crystal-GRID is a direct method to study orientation-dependent slowing down of recoil atoms in mono-crystals at intermediate recoil velocities of up to 1 Angstrom/fs. The method is based on the excitation of nuclei by neutron capture and their deexcitation by successive photon emissions. A first photon emission leads to a recoil of a few 100 eV. Special deexcitation channels are considered where the recoiling nucleus is not yet at rest when the second photon is emitted. The Doppler shifted energy of this second gamma quantum is measured. When observing many deexcitations a Doppler broadened gamma line shape is obtained.

The slowing down of recoiling atoms is anisotropic due to the regular and discrete positions of the collision partners in a lattice. The use of single-crystalline targets allows to observe this anisotropy via a pronounced structure of the Doppler broadened gamma line. As the Doppler shift only depends on the projection of recoil velocities on the axis of observation, different line shapes can be obtained when performing various measurements with crystals aligned differently.

Measurements have been carried out with the high-precision gamma spectrometers GAMS 4 and GAMS 5 at the ILL. Doppler broadened line shapes could be obtained using ZnS single crystals in three orientations. They are compared to predictions from molecular dynamics (MD) simulations. Thereby, parameters of classical interatomic potentials describing the slowing down have been extracted.

Detailed results will be presented for ZnS, showing that the universal screened Coulomb potentials (ZBL, KrC) have to be modified in the examined energy region. Using the modified potentials, effects such as channelling and blocking have been studied by computer simulations. It will be discussed to which extent the potential corrections are important for simulations of ion beam techniques.]]></dc:description>
<dc:subject><![CDATA[Crystal-GRID]]></dc:subject>
<dc:subject><![CDATA[gamma ray spectroscopy]]></dc:subject>
<dc:subject><![CDATA[interatomic potential]]></dc:subject>
<dc:subject><![CDATA[Molecular Dynamics simulation]]></dc:subject>
<dc:subject><![CDATA[nuclear level lifetime]]></dc:subject>
<dc:subject><![CDATA[ZnS]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-3111-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:3111-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hauschild, T.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Jentschel, M.]]></dc:creator>
<dc:creator><![CDATA[Börner, H. G.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3111-2</dc:identifier>
<dc:title><![CDATA[Crystal-GRID: Study of orientation-dependent slowing-down in single-crystalline ZnS]]></dc:title>
<dc:source><![CDATA[8th  Int. Conf. on Atomic Collisions in Solids (ICACS18), Odense, Denmark, August 3-8, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Crystal-GRID is a direct method to study orientation-dependent slowing down of recoil atoms in mono-crystals at intermediate recoil velocities of up to 1 Angstrom/fs. The method is based on the excitation of nuclei by neutron capture and their deexcitation by successive photon emissions. A first photon emission leads to a recoil of a few 100 eV. Special deexcitation channels are considered where the recoiling nucleus is not yet at rest when the second photon is emitted. The Doppler shifted energy of this second gamma quantum is measured. When observing many deexcitations a Doppler broadened gamma line shape is obtained.

The slowing down of recoiling atoms is anisotropic due to the regular and discrete positions of the collision partners in a lattice. The use of single-crystalline targets allows to observe this anisotropy via a pronounced structure of the Doppler broadened gamma line. As the Doppler shift only depends on the projection of recoil velocities on the axis of observation, different line shapes can be obtained when performing various measurements with crystals aligned differently.

Measurements have been carried out with the high-precision gamma spectrometers GAMS 4 and GAMS 5 at the ILL. Doppler broadened line shapes could be obtained using ZnS single crystals in three orientations. They are compared to predictions from molecular dynamics (MD) simulations. Thereby, parameters of classical interatomic potentials describing the slowing down have been extracted.

Detailed results will be presented for ZnS, showing that the universal screened Coulomb potentials (ZBL, KrC) have to be modified in the examined energy region. Using the modified potentials, effects such as channelling and blocking have been studied by computer simulations. It will be discussed to which extent the potential corrections are important for simulations of ion beam techniques.]]></dc:description>
<dc:subject><![CDATA[Crystal-GRID]]></dc:subject>
<dc:subject><![CDATA[gamma ray spectroscopy]]></dc:subject>
<dc:subject><![CDATA[interatomic potential]]></dc:subject>
<dc:subject><![CDATA[Molecular Dynamics simulation]]></dc:subject>
<dc:subject><![CDATA[nuclear level lifetime]]></dc:subject>
<dc:subject><![CDATA[ZnS]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:3112-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Assmann, W.]]></dc:creator>
<dc:creator><![CDATA[Huber, H.]]></dc:creator>
<dc:creator><![CDATA[Karamian, S. A.]]></dc:creator>
<dc:creator><![CDATA[Andersen, J. U.]]></dc:creator>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3112-1</dc:identifier>
<dc:title><![CDATA[Transverse cooling or heating of channeled ions by electron capture and loss]]></dc:title>
<dc:source><![CDATA[8th  Int. Conf. on Atomic Collisions in Solids (ICACS18), Odense, Denmark, August 3-8, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:3113-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ostwald, S.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3113-1</dc:identifier>
<dc:title><![CDATA[XPS investigations for the study of Ge clustering in SiO2]]></dc:title>
<dc:source><![CDATA[8th European Conf. on Appl. of Surface and Interface Analysis (ECASIA´99), Sevilla, Spain, October 4-8, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:14283-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Philipp, P.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Zier, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14283-1</dc:identifier>
<dc:title><![CDATA[SWOP—Charge Carrier Depth Profiling of Boron Doped Single Crystalline Silicon]]></dc:title>
<dc:source><![CDATA[The 18th International Conference on Ion Implantation Technology (IIT 2010), 06.-11.06.2010, Kyoto, Japan]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[According to the subsequently continued shrinking of semiconductor device dimensions the fabrication of ultra shallow pn-junctions is the essential requirement for modern CMOS technology. Therefore the importance of measurement techniques for dopant depth profiles is rising and the demands in resolution and accuracy are increasing. The established methods like SIMS and spreading resistance profiling become less suitable for these applications because of their disadvantages at measurements near the silicon surface.
Stepwise Oxidation Profiling was applied to boron doped p+ layers as a new measurement technique for ultra shallow doped layers. Single crystalline n-type silicon (110 Ohmcm) with <100>- orientation was used as base material. One sample type was implanted with boron at an ion energy of 1 keV and an implantation fluence of 3x1014 cm<sup>-2</sup>. After implantation the samples were annealed by rapid thermal annealing (RTA) at 1000 °C and 10 s annealing time. On the other sample type boron was deposited by e-beam evaporation. Following, a 400 keV Si pre-implant was done to avoid transient enhanced diffusion and then a flash lamp diffusion (FLD) was carried out with 600 °C preheating and a 1300 °C Xe flash of about 3 ms duration. The two sample types were fabricated as planar van der Pauw (VDP) test structures.
Compared to the Continuous Anodic Oxidation Technique (CAOT) developed by S. Prussin the measurement procedure of SWOP is similar and the dopant depth profiles are measured by altering between an electrical VDP measurement of the sheet resistance and the electrochemical growth of thin anodic SiO2 layers (in steps of 1 nm and below). The SWOP measurement can be done in one apparatus without removing the sample for anodic oxidation or electrical VDP measurement. The values of the active boron concentration are calculated using the hole mobility values based on the Thurber expression.]]></dc:description>
<dc:subject><![CDATA[anodic oxidation]]></dc:subject>
<dc:subject><![CDATA[boron implantation]]></dc:subject>
<dc:subject><![CDATA[ultra shallow junction]]></dc:subject>
<dc:subject><![CDATA[depth profiling]]></dc:subject>
<dc:subject><![CDATA[van-der-Pauw]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14283-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
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<record>
<header>
<identifier>HZDR:PUBLDB:14283-2</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Philipp, P.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Zier, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14283-2</dc:identifier>
<dc:title><![CDATA[SWOP—Charge Carrier Depth Profiling of Boron Doped Single Crystalline Silicon]]></dc:title>
<dc:source><![CDATA[AIP Conference Proceedings 1321(2010), 216-219]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[According to the subsequently continued shrinking of semiconductor device dimensions the fabrication of ultra shallow pn-junctions is the essential requirement for modern CMOS technology. Therefore the importance of measurement techniques for dopant depth profiles is rising and the demands in resolution and accuracy are increasing. The established methods like SIMS and spreading resistance profiling become less suitable for these applications because of their disadvantages at measurements near the silicon surface.
Stepwise Oxidation Profiling was applied to boron doped p+ layers as a new measurement technique for ultra shallow doped layers. Single crystalline n-type silicon (110 Ohmcm) with <100>- orientation was used as base material. One sample type was implanted with boron at an ion energy of 1 keV and an implantation fluence of 3x1014 cm<sup>-2</sup>. After implantation the samples were annealed by rapid thermal annealing (RTA) at 1000 °C and 10 s annealing time. On the other sample type boron was deposited by e-beam evaporation. Following, a 400 keV Si pre-implant was done to avoid transient enhanced diffusion and then a flash lamp diffusion (FLD) was carried out with 600 °C preheating and a 1300 °C Xe flash of about 3 ms duration. The two sample types were fabricated as planar van der Pauw (VDP) test structures.
Compared to the Continuous Anodic Oxidation Technique (CAOT) developed by S. Prussin the measurement procedure of SWOP is similar and the dopant depth profiles are measured by altering between an electrical VDP measurement of the sheet resistance and the electrochemical growth of thin anodic SiO2 layers (in steps of 1 nm and below). The SWOP measurement can be done in one apparatus without removing the sample for anodic oxidation or electrical VDP measurement. The values of the active boron concentration are calculated using the hole mobility values based on the Thurber expression.]]></dc:description>
<dc:subject><![CDATA[anodic oxidation]]></dc:subject>
<dc:subject><![CDATA[boron implantation]]></dc:subject>
<dc:subject><![CDATA[ultra shallow junction]]></dc:subject>
<dc:subject><![CDATA[depth profiling]]></dc:subject>
<dc:subject><![CDATA[van-der-Pauw]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1063/1.3548353]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14283-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1971-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Hicken, E. F.]]></dc:creator>
<dc:creator><![CDATA[Jaegers, H.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1971-1</dc:identifier>
<dc:title><![CDATA[Results of Experimente at the NOKO Pilot Plant]]></dc:title>
<dc:source><![CDATA[VGB-Power Tech 78 (1998), Nr. 5, S. 79-84]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[On the NOKO (emergency condenser) test station constructed at Jülich Research Centre, the operating performance and
effectiveness of the emergency condenser of the boiling water reactor 1000 have been determined in well over 200 tests. It has been
possible to check that the tests were in close agreement with a modified version of ATHLET ]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1975-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1975-1</dc:identifier>
<dc:title><![CDATA[Specimen Reconstitution Technique and Verification Testing for Charpy Size SENB Specimens]]></dc:title>
<dc:source><![CDATA[Small Specimen Test Techniques, ASTM STP 1329, W.R. Corwin, S.T. Rosinski, E. van Walle, Eds., American Society for Testing and Materials, July 1998, pp. 420]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Specimen reconstitution, i.e. the incorporation of a small piece from a previously tested specimen into a compound specimen, allows to multiply the number of tests. That is especially important if the available material is restricted and new parameters have to be measured. For this purpose a technique was developed to reconstitute Charpy size single-edge notch specimens (SENB) from broken halves of Charpy V-notch specimens. The essential tools for producing reconstituted specimens are a stud arc welding set-up and an electric wire discharge machine. The reconstitution technique applied is in accordance with the ASTM- guideline E-1253. The fraction of the insert that is affected by the reconstitution technique is determined by measurements of temperature and hardness gradients and by metallographic examination. The specimen reconstitution technique has been validated for SENB specimens of Charpy geometry. The test methods comprised instrumented impact testing of Charpy V specimens and elastic- plastic fracture toughness testing with precracked and side grooved SENB specimens.
]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
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<dc:type>doc-type:bookPart</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1975-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:2466-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:creator><![CDATA[Strecker, N.]]></dc:creator>
<dc:creator><![CDATA[Feudel, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2466-1</dc:identifier>
<dc:title><![CDATA[Atomistic modeling of ion implantation within a 2d process simulator]]></dc:title>
<dc:source><![CDATA[MRS Fall Meeting, Boston, USA, Dec. 1 - 5, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2466-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2466-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:creator><![CDATA[Strecker, N.]]></dc:creator>
<dc:creator><![CDATA[Feudel, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2466-2</dc:identifier>
<dc:title><![CDATA[Atomistic modeling of ion implantation within a 2d process simulator]]></dc:title>
<dc:source><![CDATA[Mat. Res. Soc. Symp. Proc. 490 (1998) 21]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:bookPart</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2466-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:2467-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Seifarth, H.]]></dc:creator>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:creator><![CDATA[Markwitz, A.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, P.]]></dc:creator>
<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2467-1</dc:identifier>
<dc:title><![CDATA[Abscheidung von Si/SiO<SUB>2</SUB>-Cluster-Schichten durch reaktives Magnetron-Sputtern]]></dc:title>
<dc:source><![CDATA[8. Bundesdeutsche Fachtagung Plasmatechnologie, Dresden, Sept. 14 - 17, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2467-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2986-2</identifier>
<datestamp>2025-12-03</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Thees, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Wittmaack, M.]]></dc:creator>
<dc:creator><![CDATA[Stegemann, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Gebel, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2986-2</dc:identifier>
<dc:title><![CDATA[Microstructure and electrical properties of gate-SiO\sub{2} containing Ge-nanoclusters for memory applications]]></dc:title>
<dc:source><![CDATA[Microelectronics Reliability 40 (2000) 867-871]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[MOSFET´s with gateoxides containing nanoclusters (Si, Ge, Sn, Sb) fabricated with different techniques (implantation, LPCVD, sputtering) are a very promising approach for future memories. This contribution reports on results obtained on Ge-implanted MOS capacitors. By varying the implantation and annealing parameters the Ge depth profile and the cluster size and distribution can be controlled. The experimental results are explained by a theoretical model, which is based on TRIM calculations, rate-equation studies and 3D kinetic Monte Carlo simulations. The electrical properties of gate-SiO\sub{2} containing Ge-nanoclusters are investigated in detail with emphasis on its feasibility for memory applications. ]]></dc:description>
<dc:subject><![CDATA[ion beam synthesis]]></dc:subject>
<dc:subject><![CDATA[nanoclusters]]></dc:subject>
<dc:subject><![CDATA[nonvolatile merory]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0026-2714(99)00330-3]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2986-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:2986-1</identifier>
<datestamp>2025-12-03</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Thees, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Wittmaack, M.]]></dc:creator>
<dc:creator><![CDATA[Stegemann, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Gebel, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2986-1</dc:identifier>
<dc:title><![CDATA[Microstructure and electrical properties of gate-SiO\sub{2} containing Ge-nanoclusters for memory applications]]></dc:title>
<dc:source><![CDATA[10th Workshop on Dielectrics in Microelectronics Barcelona, November 3-5, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[MOSFET´s with gateoxides containing nanoclusters (Si, Ge, Sn, Sb) fabricated with different techniques (implantation, LPCVD, sputtering) are a very promising approach for future memories. This contribution reports on results obtained on Ge-implanted MOS capacitors. By varying the implantation and annealing parameters the Ge depth profile and the cluster size and distribution can be controlled. The experimental results are explained by a theoretical model, which is based on TRIM calculations, rate-equation studies and 3D kinetic Monte Carlo simulations. The electrical properties of gate-SiO\sub{2} containing Ge-nanoclusters are investigated in detail with emphasis on its feasibility for memory applications. ]]></dc:description>
<dc:subject><![CDATA[ion beam synthesis]]></dc:subject>
<dc:subject><![CDATA[nanoclusters]]></dc:subject>
<dc:subject><![CDATA[nonvolatile merory]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2986-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2988-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Lindau, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2988-1</dc:identifier>
<dc:title><![CDATA[Verfahren zur Bestimmung der Festigkeit von dispersem Material]]></dc:title>
<dc:source><![CDATA[DE 198 13 065 A 1]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Die Bestimmung der Festigkeit von dispersem Material ist für dessen Handhabbarkeit in Transport- und Verarbeitungsprozessen von Bedeutung und beschreibt Fließverhalten, innere Reibung und Wandreibung disperser Materialien, zu denen Schüttgut, Granulat und feines Pulver gehören.
Die Festigkeit soll möglichst einfach und umfassend erfaßt werden.
Erfindungsgemäß wird die Aufgabe dadurch gelöst, daß in einem selbsterregten schwingenden mechanischen System sowohl die Verlustleistung als auch die Eigenfrequenz zuerst mit einem mit dem System fest verbundenen, starren Referenzkörper und nachfolgend für das zu bestimmende disperse Material, das die gleiche Masse wie der Referenzkörper aufweist, ermittelt werden und daß die Festigkeit des dispersen Materials durch einen relativen Dämpfungsfaktor b nach der Formel

b=(T<sub>M</sub>*f<sub>R</sub>)/(T<sub>R</sub>*f<sub>M</sub>)

und durch einen relativen Ankopplungsfaktor k nach der Formel

k=1-(f<sub>R</sub>-f<sub>M</sub>)/f<sub>R</sub>

bestimmt wird, wobei
f<sub>R</sub>	die Eigenfrequenz bei Belegung des Systems mit dem Referenzkörper,
f<sub>M</sub>	die Eigenfrequenz bei Belegung des Systems mit dem dispersen Material,
T<sub>R</sub>	die Pulsbreite der Ansteuerspannung für den Referenzkörper und
T<sub>M</sub>	die Pulsbreite der Ansteuerspannung für das disperse Material
bedeuten.]]></dc:description>
<dc:type>info:eu-repo/semantics/patent</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:patent</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:1662-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Denner, V.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Mathon, M.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1662-1</dc:identifier>
<dc:title><![CDATA[SANS Investigations of the Irradiation-induced Microstructural Changes in Surveillance Specimes of VVER-440-Type Reactor Pressure Vessel Steel 15Kh2MFA and Weld Metal Sv-10MFT]]></dc:title>
<dc:source><![CDATA[Table Ronde LLB Saclay, November 1997, Posterbeitrag]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Two mechanisms are proposed for the theoretical description of the dilational viscoelasticity on a liquid surface. Possible relaxations of the temperature and electric charges induced due to the passage of the transverse-longitudinal surface waves are discussed. The dilational viscosity of the liquid metal surface can be realistically estimated from the charge oscillations model.]]></dc:description>
<dc:subject><![CDATA[Liquid surface]]></dc:subject>
<dc:subject><![CDATA[Surface tension]]></dc:subject>
<dc:subject><![CDATA[Viscoelaticity]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1662-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1632-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:creator><![CDATA[Elkin, I.]]></dc:creator>
<dc:creator><![CDATA[Kalinenko, V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1632-1</dc:identifier>
<dc:title><![CDATA[Analysis of a boron dilution accident for WWER-440 combining the use of the codes DYN3D and SiTAP]]></dc:title>
<dc:source><![CDATA[Nuclear Engineering and Design 170 (1997), pp. 95 - 99]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[A boron dilution scenario caused by the connection of a previously disconnected primary circuit loop in a Russian WWER­440 type reactor is considered. The scenario is specific for this reactor type because of the existence of Main Isolating Valves in the loops. The additional failure of safety systems during the connection procedure was assumed. The analysis was carried out by the combined use of SiTAP and DYN3D. By the help of the fast running plant simulator code SiTAP several modifications of the scenario were considered. The scenario with the most dangerous consequences was identified and has been analysed using the three­dimensional core model DYN3D including a coolant mixing model for the lower plenum. The boundary conditions for the DYN3D analysis were obtained from SiTAP calculation. Comparing the results of both codes, a similar behaviour of the mean reactor parameters can be observed, but in the 3D analysis local exceeding of safety relevant parameters was obtained. Thus, the point kinetics model is not conservative, but by using SiTAP more realistic time­dependent boundary conditions for the 3D model could be provided than in previous analyses. The strong consequences of the considered scenario suggest the nessecity of additional measures for preventing this type of accidents.

]]></dc:description>
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<identifier>HZDR:PUBLDB:2575-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:creator><![CDATA[Seifert, S.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-2575-1</dc:identifier>
<dc:title><![CDATA[Institute of Bioinorganic and Radiopharmaceutical Chemistry; Report January 1998 - Juni 1999]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf, FZR-270 September 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[FOREWORD]]></dc:description>
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<identifier>HZDR:PUBLDB:2577-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2577-1</dc:identifier>
<dc:title><![CDATA[Comparative study of ion implanted SiC by slow positron implantation and Rutherford backscattering/ channeling spectroscopies]]></dc:title>
<dc:source><![CDATA[Texas Christian University (Department of Physics), Ft. Worth/TX, 02.11.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2577-2</dc:identifier>
<dc:title><![CDATA[Comparative study of ion implanted SiC by slow positron implantation and Rutherford backscattering/ channeling spectroscopies]]></dc:title>
<dc:source><![CDATA[University of Texas at Arlington (Physics Department), Arlington/TX, 03.11.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
<dc:type>Text</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2578-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2578-1</dc:identifier>
<dc:title><![CDATA[Charakterisierung leerstellenartiger Defekte in ionenimplantiertem SiC mit Positronen]]></dc:title>
<dc:source><![CDATA[FZ Rossendorf, Zentrumsseminar, 10.12.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<identifier>HZDR:PUBLDB:2579-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Fontaine, F.]]></dc:creator>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2579-1</dc:identifier>
<dc:title><![CDATA[Hochtemperatur-Implantation von Diamant]]></dc:title>
<dc:source><![CDATA[2. Statusseminar zum BMBF-Verbundprojekt 'Sensorcluster für extreme Umgebungsbedingungen', Fernuniversität Hagen, 2./3. Juni 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<identifier>HZDR:PUBLDB:2580-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2580-1</dc:identifier>
<dc:title><![CDATA[In-situ -Ionenstrahlanalytik während der Ionenstrahlmodifikation dünner Schichten]]></dc:title>
<dc:source><![CDATA[ETH Zürich, 9.6.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2581-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2581-1</dc:identifier>
<dc:title><![CDATA[Verschleißfester Edelstahl durch Plasmaimmersions-Ionenimplantation]]></dc:title>
<dc:source><![CDATA[Robert Bosch AG, Crailsheim, March 9, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2582-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2582-1</dc:identifier>
<dc:title><![CDATA[Nanokristalle: Ein neues Material der Opto- und Halbleiterelektronik?]]></dc:title>
<dc:source><![CDATA[Physikalisches Institut der Universität Kaiserslautern, Jan. 19, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2584-1</identifier>
<datestamp>2019-03-04</datestamp>
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</header>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2584-1</dc:identifier>
<dc:title><![CDATA[Ion beam synthesis of nanocrystals in SiO2: experiments, modeling and computer simulations]]></dc:title>
<dc:source><![CDATA[Vanderbilt University, Nashville, TN, USA, June 29, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2585-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Herrmann, F.]]></dc:creator>
<dc:creator><![CDATA[Grambole, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2585-1</dc:identifier>
<dc:title><![CDATA[Anwendungen der Rossendorfer Kernmikrosonde als Schwerionenmikroskop]]></dc:title>
<dc:source><![CDATA[Arbeitstreffen Forschung mit nuklearen Sonden und Ionenstrahlen, Leipzig, 5. - 7. Okt. 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<header>
<identifier>HZDR:PUBLDB:367-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Richter, K.]]></dc:creator>
<dc:creator><![CDATA[Weiß, R.]]></dc:creator>
<dc:creator><![CDATA[Zimmermann, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-367-1</dc:identifier>
<dc:title><![CDATA[Experimentelle Modalanalyse an einer Kühlschleife eines Druckwasserreaktors]]></dc:title>
<dc:source><![CDATA[TUD - Sonderdruck zum Vortrag in Schmochtitz]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/other</dc:type>
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<identifier>HZDR:PUBLDB:2350-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Beyer, M.]]></dc:creator>
<dc:creator><![CDATA[Carl, H.]]></dc:creator>
<dc:creator><![CDATA[Schumann, P.]]></dc:creator>
<dc:creator><![CDATA[Seidel, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2350-1</dc:identifier>
<dc:title><![CDATA[Fernüberwachung ukrainischer Kernkraftwerke (in Russisch)]]></dc:title>
<dc:source><![CDATA[Atomnaja Technika sa rubeshom, Nr.8 (1999), page 3-8]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Die zu Beginn der neunziger Jahre in der Ukraine praktizierte Überwachung der Kernkraftwerke ermöglichte der Genehmigungs- und Aufsichtsbehörde nur einen unzureichenden Zugang zu Informationen über den jeweils aktuellen betrieblichen Sicherheitszustand.
Deshalb wurde für den 5. Block des KKW Saporoshje (WWER-1000/W-320) ein modernes betriebliches Überwachungssystem als Pilotprojekt konzipiert, eingerichtet und Ende 1995 in den Probebetrieb überführt. Es ergänzt die vorhandenen betrieblichen Kontroll- und Überwachungseinrichtungen durch Einbeziehung moderner informationstechnischer Mittel. Das System ermöglicht schwerpunktmäßig eine kontinuierliche Beobachtung des Zustandes vom Block 5 bei Normalbetrieb und bei Betriebsstörungen bzw. Störfällen, so daß bei erkennbaren Abweichungen vom bestimmungsgemäßen Anlagenbetrieb frühzeitig durch Nachfrage und Anordnung darauf reagiert werden kann.
Ein ähnliches Überwachungssystem konnte 1998 für den ersten und zweiten Block des KKW Rovno (WWER-440/W-213) eingerichtet und an das Informations- und Krisenzentrum in Kiew angeschlossen werden.
]]></dc:description>
<dc:subject><![CDATA[ukrainische Kernkraftwerke]]></dc:subject>
<dc:subject><![CDATA[KKW]]></dc:subject>
<dc:subject><![CDATA[Fernüberwachung]]></dc:subject>
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<dc:title><![CDATA[Response to Comment on "Interstitial-type defects away of the projected ion range in high energy ion implanted and annealed silicon"]]></dc:title>
<dc:source><![CDATA[Appl. Phys. Lett. 77, 1251 (2000)]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[see abstract of the above mentioned publication in APL 75, 9, 1279 (1999)]]></dc:description>
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<dc:title><![CDATA[Generation of radiation defects in high resistivity silicon at cyclic irradiation and annealing]]></dc:title>
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<dc:title><![CDATA[Molecular studies of the culturable and non-culturable bacteria in uranium wastes]]></dc:title>
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<dc:title><![CDATA[Institute of Bioinorganic and Radiopharmaceutical Chemistry; Annual Report 1992]]></dc:title>
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<identifier>HZDR:PUBLDB:2790-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Zänker, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2790-1</dc:identifier>
<dc:title><![CDATA[Photonenkorrelationsspektroskopie und Rasterkraftmikroskopie an Huminsäure.]]></dc:title>
<dc:source><![CDATA[TU Dresden, Institut für Werkstoffwissenschaft
Dresden, Germany, 17.12.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:14333-1</identifier>
<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Cornelius, S.]]></dc:creator>
<dc:creator><![CDATA[Vinnichenko, M.]]></dc:creator>
<dc:creator><![CDATA[Kolitsch, A.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14333-1</dc:identifier>
<dc:title><![CDATA[Electrical transport in Al doped ZnO grown by reactive pulsed magnetron sputtering]]></dc:title>
<dc:source><![CDATA[5th Forum on New Materials (in the framework of 12th International Conference on Modern Materials and Technologies - CIMTEC 2010), 13.-18.06.2010, Montecatini Terme, Italien]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The synthesis of transparent conductive oxides (TCO) with high transmittance in the near infrared (IR) spectral range is a key requirement for increasing the power conversion efficiency in thin film solar cells. As the absorption at energies close to the Si band gap (1.1 eV) is caused by the free electron plasma it is necessary to maximize their mobility at moderate densities (~5x10<sup>20</sup> cm<sup>-3</sup>) in order to simultaneously reach low resistivities of ~2x10<sup>-4</sup> Ohm*cm and improve the IR transmittance.
Therefore a reactive magnetron sputtering method using metallic Zn/Al alloy targets was developed to achieve high carrier mobilities (~45 cm<sup>2</sup>/Vs) in ZnO:Al thin films. The influence of growth temperature, oxygen partial pressure and target Al concentration on the electrical film properties has been investigated systematically by Hall effect measurements.
Additionally XRD, X-TEM, AFM, ERDA, RBS and spectroscopic ellipsometry were employed to reveal film structure, composition and optical properties. The experimentally observed limit of mobility in polycrystalline ZnO:Al is discussed in terms of ionized impurity scattering and clustering as well as grain boundary limited transport.]]></dc:description>
<dc:subject><![CDATA[transparent conductive oxides]]></dc:subject>
<dc:subject><![CDATA[TCO]]></dc:subject>
<dc:subject><![CDATA[reactive magnetron sputtering]]></dc:subject>
<dc:subject><![CDATA[ZnO:Al]]></dc:subject>
<dc:subject><![CDATA[AZO]]></dc:subject>
<dc:subject><![CDATA[electrical properties]]></dc:subject>
<dc:subject><![CDATA[mobility]]></dc:subject>
<dc:subject><![CDATA[ionized impurity scattering]]></dc:subject>
<dc:subject><![CDATA[grain boundary limited transport]]></dc:subject>
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<identifier>HZDR:PUBLDB:2883-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Grosse, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2883-1</dc:identifier>
<dc:title><![CDATA[Die Strahlungsquelle ELBE am Forschungszentrum Rossendorf]]></dc:title>
<dc:source><![CDATA[Phys. Bl. 54 (1998) 342-344]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[In einigen Wochen wird der Grundstein für die Strahlungsquelle ELBE am Forschungszentrum Rossendorf (FZR) bei Dresden gelegt. Das Kernstück dieser neuen Anlage wird ein supraleitender Elektronen-Linearbeschleuniger hoher Brillanz sein, der in seiner kombination von hoher Strahlintensität und guter Strahlqualität (d. h. niedriger Emittanz) alle in Europa existierenden Anlagen übertreffen soll (das Akronym ELBE wurde aber nicht nur deshalb gewählt).]]></dc:description>
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<identifier>HZDR:PUBLDB:2884-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Stefani, F.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2884-1</dc:identifier>
<dc:title><![CDATA[Velocity reconstruction in electrically conducting fluids from external electromagnetic measurements]]></dc:title>
<dc:source><![CDATA[APS Bulletin vol. 44, no. 4, pp. 106 (1999)]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[A possibility for the determination of velocity fields in electrically conducting fluids is presented. Applying an external magnetic field, electric and magnetic fields are induced by the fluid motion. The electric potential can be measured at the walls and the magnetic field outside the fluid volume. The inverse problem of reconstructing the velocity from the measured quantities is solved using Tikhonov regularization. Several examples will be given to illustrate the potential of such type of velocity reconstruction. The problem of uniqueness is treated in detail for the spherical geometry. Our ultimate aim is to develop a fully contactless velocity measurement technique whereby measuring the electric potential at the wall can be avoided. ]]></dc:description>
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<dc:creator><![CDATA[Geipel, G.]]></dc:creator>
<dc:creator><![CDATA[Rutsch, M.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Brendler, V.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2758-1</dc:identifier>
<dc:title><![CDATA[Speciation of Uranium - Determination and Calculation under Natural Conditions Uranium Mining and Hydrogeology II]]></dc:title>
<dc:source><![CDATA[Freiberg, Germany, 15.-17.09.1998]]></dc:source>
<dc:date>1998</dc:date>
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<identifier>HZDR:PUBLDB:2757-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Funke, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2757-1</dc:identifier>
<dc:title><![CDATA[The Radiochemistry Safety System at ROBL]]></dc:title>
<dc:source><![CDATA[14th CRG Club Meeting
Grenoble, France, 19.-20.10.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Bubner, M.]]></dc:creator>
<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2759-1</dc:identifier>
<dc:title><![CDATA[Synthetic Humic Acids for Radioecological Environmental Research]]></dc:title>
<dc:source><![CDATA[Joint European International Isotope Society Conference
Bad Soden, Germany, 24.-26.06.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2760-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hennig, C.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2760-1</dc:identifier>
<dc:title><![CDATA[A Monochromator Feedback System]]></dc:title>
<dc:source><![CDATA[14th CRG Club Meeting
Grenoble, France, 19.-20.10.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2469-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2469-1</dc:identifier>
<dc:title><![CDATA[MeV-Implantation in Silicium]]></dc:title>
<dc:source><![CDATA[20. Dt. Nutzertreffen Ionenimplantation, SIMEC-Werk der Siemens AG, Dresden, Oct. 29 -30, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2470-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Späth, C.]]></dc:creator>
<dc:creator><![CDATA[Kühn, M.]]></dc:creator>
<dc:creator><![CDATA[Richter, F.]]></dc:creator>
<dc:creator><![CDATA[Falke, U.]]></dc:creator>
<dc:creator><![CDATA[Hietschold, M.]]></dc:creator>
<dc:creator><![CDATA[Kilper, R.]]></dc:creator>
<dc:creator><![CDATA[Kreißig, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2470-1</dc:identifier>
<dc:title><![CDATA[A comparative study of ERDA, EELS and XPS for structural analysis of amorphous carbon nitride films]]></dc:title>
<dc:source><![CDATA[Int. Conf. Diamond '97]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2586-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Höfgen, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2586-1</dc:identifier>
<dc:title><![CDATA[Ionenstrahlinduzierte Rekristallisation von amorphen SiC-Schichten]]></dc:title>
<dc:source><![CDATA[Institut für Physik, TU Chemnitz, May 11, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<identifier>HZDR:PUBLDB:2587-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:title><![CDATA[18F-Radiotracer und deren Verwendung zum Monitoring der Expression der Cytosin-Deaminase nach Gentransfer sowie Verfahren zur Herstellung der 18F-Radiotracer]]></dc:title>
<dc:source><![CDATA[Patentschrift 199 51 715 C1]]></dc:source>
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<dc:description><![CDATA[Aufgabe der Erfindung ist es, eine Substanz vorzuschlagen, die bei der Verwendung zum Monitoring der Expression von Cytosin-Deaminase mit 18F-Tracer genügend lange Zeit in der Zelle verbleibt sowie ein Verfahren zur Herstellung der Substanz anzugeben.]]></dc:description>
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Die derzeitig bei chemischen Mikroanalysesystemen erkennbaren Probleme bezüglich Membranpumpen und mikromechanischer Ventile werden  bei der  Konstruktion des erfindungsgemäßen Mikroanalysators dadurch gelöst, daß zur Bewältigung des Fluidhandlings ausschließlich Mikrofluidmanipulatoren, das sind Mikrotropfen-Emitter und Mikro-Fluiddioden, eingesetzt sind, welche mittels mikrotechnischer Verfahren und mikrosystemtechnischer Aufbau- und Verbindungstechniken herstellbar und als modulare Komponenten flexibel koppelbar an Mikrofluidiksystem und Mikrosensoren zum Systemaufbau sind. Der erfindungsgemäße Mikroanalysator mit einem neu konzipierten Fluid-Handlingsystem zeichnet sich in besonderer Weise durch eine absolute Leckfreiheit, eine einfache Konstruktion, einen geringen Platzbedarf und eine kostengünstige Herstellung aus.]]></dc:description>
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Die derzeitig bei chemischen Mikroanalysesystemen erkennbaren Probleme bezüglich Membranpumpen und mikromechanischer Ventile werden  bei der  Konstruktion des erfindungsgemäßen Mikroanalysators dadurch gelöst, daß zur Bewältigung des Fluidhandlings ausschließlich Mikrofluidmanipulatoren, das sind Mikrotropfen-Emitter und Mikro-Fluiddioden, eingesetzt sind, welche mittels mikrotechnischer Verfahren und mikrosystemtechnischer Aufbau- und Verbindungstechniken herstellbar und als modulare Komponenten flexibel koppelbar an Mikrofluidiksystem und Mikrosensoren zum Systemaufbau sind. Der erfindungsgemäße Mikroanalysator mit einem neu konzipierten Fluid-Handlingsystem zeichnet sich in besonderer Weise durch eine absolute Leckfreiheit, eine einfache Konstruktion, einen geringen Platzbedarf und eine kostengünstige Herstellung aus.]]></dc:description>
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<dc:creator><![CDATA[Remskar, M.]]></dc:creator>
<dc:creator><![CDATA[Mrzel, A.]]></dc:creator>
<dc:creator><![CDATA[Virsek, M.]]></dc:creator>
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<dc:creator><![CDATA[Krause, M.]]></dc:creator>
<dc:creator><![CDATA[Kolitsch, A.]]></dc:creator>
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<dc:title><![CDATA[The MoS<SUB>2</SUB> nanotubes with defect-controlled electric properties]]></dc:title>
<dc:source><![CDATA[Nanoscale Research Letters 6(2011), 26]]></dc:source>
<dc:date>2011</dc:date>
<dc:description><![CDATA[We describe a two-step synthesis of pure multiwall MoS<SUB>2</SUB> nanotubes with a high degree of homogeneity in size. The Mo<SUB>6</SUB>S<SUB>4</SUB>I<SUB>6</SUB> nanowires grown directly from elements under temperature gradient conditions in hedgehog-like assemblies were used as precursor material. Transformation in argon-H<SUB>2</SUB>S/H<SUB>2</SUB> mixture leads to the MoS<SUB>2</SUB> nanotubes still grouped in hedgehog-like morphology. The described method enables a large scale production of MoS<SUB>2</SUB> nanotubes and their size control. X-ray diffraction, optical absorption and Raman spectroscopy, scanning electron microscopy with wave dispersive analysis, and transmission electron microscopy were used to characterize the starting Mo<SUB>6</SUB>S<SUB>4</SUB>I<SUB>6</SUB> nanowires and the MoS<SUB>2</SUB> nanotubes. The unit cell parameters of the Mo<SUB>6</SUB>S<SUB>4</SUB>I<SUB>6</SUB> phase are proposed. Blue shift in optical absorbance and metallic behaviour of MoS<SUB>2</SUB> nanotubes in two-probe measurement are explained by a high defect concentration.]]></dc:description>
<dc:subject><![CDATA[inorganic fullerenes]]></dc:subject>
<dc:subject><![CDATA[layered compounds]]></dc:subject>
<dc:subject><![CDATA[nanotubes]]></dc:subject>
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<dc:title><![CDATA[Spatial distribution of defects in ion-implanted and annealed Si: the R<SUB>p</SUB>/2 effect]]></dc:title>
<dc:source><![CDATA[Fed. Univ. of Rio Grande dol Sul, Porto Alegre, Brasilien, Oct.27, 1998]]></dc:source>
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<dc:title><![CDATA[Verfahren zur Herstellung von Kontakten und Leitbahnen in oder auf kristallinen Siliziumkarbid-Halbleitersubstraten]]></dc:title>
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<dc:title><![CDATA[Verfahren zur Herstellung von Kontakten und Leitbahnen in oder auf kristallinen Siliziumkarbid-Halbleitersubstraten]]></dc:title>
<dc:source><![CDATA[Patentschrift DE 199 44 144 C2]]></dc:source>
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<dc:description><![CDATA[Der Erfindung liegt die Aufgabe zugrunde, Kontakte und Leitbahnen in oder auf kristallinen SiC-Halbleitersubstraten mit geringerem Kosten- und Herstellungsaufwand sowie gutem Grenzflächenverhalten herzustellen, wenn eine Schicht über den Kontakten bzw. Leitbahnen aus SiC erforderlich ist.]]></dc:description>
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The mixing of the doorway components of a giant resonance due to the interaction via the common decay channels influences significantly the distribution of the multipole strength and the energy spectrum of the decay products of the giant resonance. The photoemission turns out to be most sensitive to the overlapping of the doorway states. At high excitation energies, the interference between the doorway states leads to a restructuring towards lower energies and apparent quenching of the dipole strength.]]></dc:description>
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The mixing of the doorway components of a giant resonance due to the interaction via the common decay channels influences significantly the distribution of the multipole strength and the energy spectrum of the decay products of the giant resonance. The photoemission turns out to be most sensitive to the overlapping of the doorway states. At high excitation energies, the interference between the doorway states leads to a restructuring towards lower energies and apparent quenching of the dipole strength.]]></dc:description>
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coefficient, strongly depending on the ion energy and the surface composition.
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High voltage pulses of eU0 = 5, 10, 15 and 20 kV were applied to a spherical
target with a small orifice. The ions were collected in the high vacuum
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coefficient, strongly depending on the ion energy and the surface composition.
In this work direct time-resolved ion flux measurements are presented.
High voltage pulses of eU0 = 5, 10, 15 and 20 kV were applied to a spherical
target with a small orifice. The ions were collected in the high vacuum
region behind this orifice and their energy distribution function exhibits
a sharp peak at the nominal energy eU0 with the height decreasing during
the voltage pulse, in agreement with the theoretical predictions for a
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<dc:creator><![CDATA[Meyer, G. J.]]></dc:creator>
<dc:creator><![CDATA[Matzke, K. H.]]></dc:creator>
<dc:creator><![CDATA[Hamacher, K.]]></dc:creator>
<dc:creator><![CDATA[Füchtner, F.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:creator><![CDATA[Notohamiprodjo, G.]]></dc:creator>
<dc:creator><![CDATA[Zijlstra, S.]]></dc:creator>
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<dc:title><![CDATA[The stability of 2-[<SUP>18</SUP>F]fluoro-deoxy-D-glucose towards epimerisation under alkaline conditions]]></dc:title>
<dc:source><![CDATA[Applied Radiation and Isotopes 51 (1999) 37-41]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Alkaline hydrolysis of 1,3,4,6-tetraacetyl-2-(<SUP>18</SUP>F]fluoro-deoxy-D-glucose in the course of 2-[<SUP>18</SUP>F]fluoro-deoxy-D-glucose (<SUP>18</SUP>FDG) synthesis offers special advantages over acidic hydrolytic procedures, because the reaction time is short and thermal requirements are very mild. In view of the possible epimerization of  2-[<SUP>18</SUP>F]fluoro-deoxy-D-glucose a multi-centre study has been performed to check the safety of this method for routine production of <SUP>18</SUP>FDG in view of the quality standards set by the European Pharmacopoeia. The study revealed that in using 0.33 M NaOH for the hydrolysis, a limitation of the reaction temperature to 40°C and a restriction of the reaction time to 5 min represent reaction conditions, which reliably limit the epimerization of <SUP>18</SUP>FDG to <SUP>18</SUP>FDM to 0.5%. Regarding the quality requirements on FDG as set forth by pharmacopoeial standards, alkaline hydrolysis of the intermediate in routine <SUP>18</SUP>FDG production is a safe and efficient reaction pathway, which furthermore obviates the requirement to check for other 2-substituted deoxy-D-glucose derivatives.]]></dc:description>
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<dc:creator><![CDATA[Türler, A.]]></dc:creator>
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<dc:title><![CDATA[Evidence for relativistic effects in the chemistry of element 104]]></dc:title>
<dc:source><![CDATA[Actinides'97, Baden-Baden, Germany, 21.-26.09.1997]]></dc:source>
<dc:date>1997</dc:date>
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<dc:title><![CDATA[Computersimulationen zur Evolution von Nanoclustern]]></dc:title>
<dc:source><![CDATA[Frühjahrstagung der DPG, Münster, Germany, March 17-21, 1997]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:creator><![CDATA[Barz, H.-U.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
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<dc:title><![CDATA[Consideration of Neutron Flux Gradients for Sophisticated Evaluation of Irradiation Experiments]]></dc:title>
<dc:source><![CDATA[IAEA Specialist's Meeting on Irradiation Effects and Mitigation, Vladimir, Russia, 15 - 19 September, 199, IWG-LMNPP-97/2, Vienna 1997, p. 230]]></dc:source>
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<dc:description><![CDATA[A joint Russian/German irradiation experiment was performed at the pressurized water reactor VVER 2 of the Rheinsberg NPP (Germany). The experiment comprises about 800 Charpy V-notch,  SENB and CT specimens made from 24 different heats of Russian type RPV base and weld metals.
Comprehensive calculations of the neutron fluence were carried out. A multigroup Monte Carlo method allows the calculation of the neutron fluence of each specimen or of different points within a large specimen under consideration of the details of the geometric arrangement. As the calculations shown the neutron fluence considerably varies over the cross section of an irradiation rig. Therefore, influence of the flux gradients on testing of Charpy V-notch and CT-specimens is evaluated.
Methods taking into account a fluence correction of the measured absorbed energies are presented and discussed]]></dc:description>
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<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
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<dc:title><![CDATA[Consideration of Neutron Flux Gradients for Sophisticated Evaluation of Irradiation Experiments]]></dc:title>
<dc:source><![CDATA[IAEA Specialist's Meeting on Irradiation Effects and Mitigation, Vladimir, Russia, 15 - 19 September, 199, IWG-LMNPP-97/2, Vienna 1997, p. 230]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[A joint Russian/German irradiation experiment was performed at the pressurized water reactor VVER 2 of the Rheinsberg NPP (Germany). The experiment comprises about 800 Charpy V-notch,  SENB and CT specimens made from 24 different heats of Russian type RPV base and weld metals.
Comprehensive calculations of the neutron fluence were carried out. A multigroup Monte Carlo method allows the calculation of the neutron fluence of each specimen or of different points within a large specimen under consideration of the details of the geometric arrangement. As the calculations shown the neutron fluence considerably varies over the cross section of an irradiation rig. Therefore, influence of the flux gradients on testing of Charpy V-notch and CT-specimens is evaluated.
Methods taking into account a fluence correction of the measured absorbed energies are presented and discussed]]></dc:description>
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<identifier>HZDR:PUBLDB:1960-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Große, M.]]></dc:creator>
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<dc:title><![CDATA[Additional Information about the Chemistry of Precipitates by Variation of the Scattering Contrast in the SANS and SAXS Experiment]]></dc:title>
<dc:source><![CDATA[Proc. International School and Symposium on Small-Angle Scattering, Matrahaza (Hungary), Oct. 1998, Report 02/E, 1999, S. 38]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Small-angle neutron scattering (SANS) experiments were performed at KWS2 facility of the KFA Jülich for investigating the defect structures, which are produced by neutron irradiation in Russian Cr-Mo-V alloyed reactor pressure vessel steel. Irradiation and post-irradiation annealing considerably change both SANS intensity and its course in the Guinier plot, which was analysed by the Glatter method. As a rule, bimodal size distribution functions were found with a first maximum at a radius of 1-2 nm and a second maximum at 6-8 nm. Irradiation increases the first maximum annealing reduces it. ]]></dc:description>
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<identifier>HZDR:PUBLDB:1960-7</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Große, M.]]></dc:creator>
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<dc:title><![CDATA[Additional Information about the Chemistry of Precipitates by Variation of the Scattering Contrast in the SANS and SAXS Experiment]]></dc:title>
<dc:source><![CDATA[Proc. International School and Symposium on Small-Angle Scattering, Matrahaza (Hungary), Oct. 1998, Report 02/E, 1999, S. 38]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Small-angle neutron scattering (SANS) experiments were performed at KWS2 facility of the KFA Jülich for investigating the defect structures, which are produced by neutron irradiation in Russian Cr-Mo-V alloyed reactor pressure vessel steel. Irradiation and post-irradiation annealing considerably change both SANS intensity and its course in the Guinier plot, which was analysed by the Glatter method. As a rule, bimodal size distribution functions were found with a first maximum at a radius of 1-2 nm and a second maximum at 6-8 nm. Irradiation increases the first maximum annealing reduces it. ]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Stephan, J.]]></dc:creator>
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<dc:title><![CDATA[Spindelmutterhalterung für ein Spindelgetriebe zum Antrieb von Hebeln]]></dc:title>
<dc:source><![CDATA[Patentanmeldung Az 199 48 050.8]]></dc:source>
<dc:date>2001</dc:date>
<dc:description><![CDATA[Der Erfindung liegt die Aufgabe zugrunde, eine Spindelmutterhalterung für ein Hebel antreibendes Spindelgetriebe vorzuschlagen, das auch unter extremen Bedingungen 
wie im Vakuum, unter Strahlenbelastung und bei einer Temperatur nahe dem absoluten Nullpunkt sicher funktioniert und dauerhaft eine exakte Wegauflösung im Nanometer-Bereich realisiert. ]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Stephan, J.]]></dc:creator>
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<dc:title><![CDATA[Spindelmutterhalterung für ein Spindelgetriebe zum Antrieb von Hebeln]]></dc:title>
<dc:source><![CDATA[Patentschrift DE 199 48 050 C1]]></dc:source>
<dc:date>2001</dc:date>
<dc:description><![CDATA[Der Erfindung liegt die Aufgabe zugrunde, eine Spindelmutterhalterung für ein Hebel antreibendes Spindelgetriebe vorzuschlagen, das auch unter extremen Bedingungen 
wie im Vakuum, unter Strahlenbelastung und bei einer Temperatur nahe dem absoluten Nullpunkt sicher funktioniert und dauerhaft eine exakte Wegauflösung im Nanometer-Bereich realisiert. ]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2608-1</dc:identifier>
<dc:title><![CDATA[Computersimulation der Ionenimplantation in der Si-Technologie: Wechselspiel zwischen Kanalisierung und Defektbildung]]></dc:title>
<dc:source><![CDATA[Physikalisches Institut der Universität Münster, July, 3, 1998]]></dc:source>
<dc:date>1998</dc:date>
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<identifier>HZDR:PUBLDB:1398-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Schneider, C.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1398-1</dc:identifier>
<dc:title><![CDATA[Fluidmechanics of Electrolytic Cells]]></dc:title>
<dc:source><![CDATA[2nd intern. symposium "Two-Phase Flow Modelling and Experimentation", Pisa, Italy, 23-26 May 1999, proceedings vol. 2, pp. 1085-1092.]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The process in the anode chamber of an alkaline chloride electrolysis cell was modelled by hydrogen peroxide decomposition at a platinum surface, which replaces the anode. Bubble size measurements and shutdown experiments have shown the ap-plicability of this model reaction. In the anode chamber regions of bubble flow, spherical foam and a transition to cell foam at the top were found. Gas fraction distributions were measured by the differential pressure method and gamma densitometry. LDA and PDPA were used to obtain velocity and bubble size distributions. For the bubble flow region, the correct consideration of the bubble size distribution was identified as determining factor to reproduce the volume flow rate of the gaseous phase from the measured gas fraction. Minor contributions to the gas flow rate are caused by bubbles of several millimetres magnitude generated in the ribs of the anode and by a liquid circulation driven by the lateral gas supply, which is characteristic for the design of membrane cells. In the foam region, large bubbles appearing as a result of coalescence carry a significant part of the gas flow rate.]]></dc:description>
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<dc:title><![CDATA[Fluidmechanics of Electrolytic Cells]]></dc:title>
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<dc:description><![CDATA[The process in the anode chamber of an alkaline chloride electrolysis cell was modelled by hydrogen peroxide decomposition at a platinum surface, which replaces the anode. Bubble size measurements and shutdown experiments have shown the ap-plicability of this model reaction. In the anode chamber regions of bubble flow, spherical foam and a transition to cell foam at the top were found. Gas fraction distributions were measured by the differential pressure method and gamma densitometry. LDA and PDPA were used to obtain velocity and bubble size distributions. For the bubble flow region, the correct consideration of the bubble size distribution was identified as determining factor to reproduce the volume flow rate of the gaseous phase from the measured gas fraction. Minor contributions to the gas flow rate are caused by bubbles of several millimetres magnitude generated in the ribs of the anode and by a liquid circulation driven by the lateral gas supply, which is characteristic for the design of membrane cells. In the foam region, large bubbles appearing as a result of coalescence carry a significant part of the gas flow rate.]]></dc:description>
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<dc:title><![CDATA[Photoluminescence and electroluminescence investigations at Ge-rich SiO<SUB>2</SUB> layers]]></dc:title>
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<dc:title><![CDATA[Nitrierung von Leichtmetallen durch Ionenimplantation]]></dc:title>
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<dc:description><![CDATA[Beim Schließen einer schnellwirkenden Absperrarmatur in einer Rohrleitung, in der eine Flüssigkeit strömt, kann es zu Kavitationsschlägen kommen. In vielen technischen Anwendungen ist ein möglichst rasches Absperren von Rohrleitungen erforderlich, insbesondere wenn es um die Beherrschung von Störungen geht. Es wird eine Methode zur Verhinderung des Kondensationsschlages vorgeschlagen. Sie besteht in der Einführung einer Hilfsarmatur, die sich hinter der eigentlichen Absperrarmatur befindet. Diese Hilfsarmatur wird zu dem Zeitpunkt geschlossen, an dem die Kavitationsblase ihre größte Ausdehnung in der Rohrleitung erreicht hat. Die Blase wird dadurch zwischen den beiden Armaturen eingeschlossen und so am Kollabieren gehindert. Im Vortrag werden die Meßergebnisse vorgestellt, die Rohrleitungs-Versuchsfeld von Fraunhofer UMSICHT mit Zweiphasen-Meßtechnik aus Rossendorf erhalten wurden. Die Auslegungskriterien für eine solche Anordnung werden diskutiert.]]></dc:description>
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<dc:title><![CDATA[Ion beam processing of single crystalline SiC]]></dc:title>
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<dc:title><![CDATA[Ion beam processing of single crystalline SiC]]></dc:title>
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<dc:title><![CDATA[Ion beam processing of single crystalline SiC]]></dc:title>
<dc:source><![CDATA[Fed. Univ. of Rio Grande dol Sul, Porto Alegre, Brasilien, Nov.5, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:title><![CDATA[Advanced ion beam processing of semiconductor materials]]></dc:title>
<dc:source><![CDATA[Advanced Lectureship Program, Dept. of Appl. Phys., Univ. of Barcelona, Spain, May 11, 1998]]></dc:source>
<dc:date>1998</dc:date>
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<identifier>HZDR:PUBLDB:1769-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Gaschenko, M. P.]]></dc:creator>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Zippe, W.]]></dc:creator>
<dc:creator><![CDATA[et. al.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1769-1</dc:identifier>
<dc:title><![CDATA[Experimental Investigation of Accidental Thermohydraulic Processes under Circuit Depressurization at ISB-VVER Safety Integral Test Facility]]></dc:title>
<dc:source><![CDATA[International Symposium on Two-Phase Flow Modelling and Experimentation, Rom, Italy, October 09 - 11, 1995, p. 537]]></dc:source>
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<dc:description><![CDATA[The paper presents the results of small-break loss-of-coolant tests carried out at the test facility ISB-VVER located in Elektrogorsk, Russia. Presently, it is the only operating integral model of the Sovjet type VVER-1000 reactor suitable for thermalhydraulic investigations. A small leak in the upper plenum of the reactor vessel was chosen for the test scenario. Different emergency core cooling (ECC) injection modes were applied and compared. It was show that the best results of ECC injection are obtained by a combined injection into both hot and cold leg. It is possible to maintain a reliable core cooling even without an injection by the safety injection tanks, which were assumed to be not available. The tests provided data suitable for code verification. Applied needle shaped void fraction probes delivered detailed information about the two-phase flow in the primary circuit.]]></dc:description>
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<dc:creator><![CDATA[Gaschenko, M. P.]]></dc:creator>
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<dc:creator><![CDATA[et. al.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1769-2</dc:identifier>
<dc:title><![CDATA[Experimental Investigation of Accidental Thermohydraulic Processes under Circuit Depressurization at ISB-VVER Safety Integral Test Facility]]></dc:title>
<dc:source><![CDATA[International Symposium on Two-Phase Flow Modelling and Experimentation, Rom, Italy, October 09 - 11, 1995]]></dc:source>
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<dc:description><![CDATA[The paper presents the results of small-break loss-of-coolant tests carried out at the test facility ISB-VVER located in Elektrogorsk, Russia. Presently, it is the only operating integral model of the Sovjet type VVER-1000 reactor suitable for thermalhydraulic investigations. A small leak in the upper plenum of the reactor vessel was chosen for the test scenario. Different emergency core cooling (ECC) injection modes were applied and compared. It was show that the best results of ECC injection are obtained by a combined injection into both hot and cold leg. It is possible to maintain a reliable core cooling even without an injection by the safety injection tanks, which were assumed to be not available. The tests provided data suitable for code verification. Applied needle shaped void fraction probes delivered detailed information about the two-phase flow in the primary circuit.]]></dc:description>
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<dc:title><![CDATA[Photo- and electroluminescence studies at ion beam synthesized Ge-rich SiO<SUB>2</SUB>-layers]]></dc:title>
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<dc:title><![CDATA[The mechanism of diffusional transport during ion nitriding of aluminium]]></dc:title>
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<dc:description><![CDATA[The mechanism of thermal transport during low-energy ion nitriding of aluminium has been investigated using marker and isotope sequence techniques in  connection whit ion beam analysis. For an ion energy of 1 keV and a temperature of 400°C, it is shown that stoichiometric nitride grows at the surface with aluminium being supplied by diffusion from the underlying bulk.]]></dc:description>
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<dc:title><![CDATA[Measurements of random and channeling stopping powers and charge state distributions in silicon for 0.2 - 1.2 MeV/u heavy ions]]></dc:title>
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<dc:title><![CDATA[Microscopic analysis of two-body correlations in light nuclei]]></dc:title>
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<datestamp>2025-12-03</datestamp>
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<dc:creator><![CDATA[Panak, P.]]></dc:creator>
<dc:creator><![CDATA[Hard, B. C.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, K.]]></dc:creator>
<dc:creator><![CDATA[Kutschke, S.]]></dc:creator>
<dc:creator><![CDATA[Röske, K.]]></dc:creator>
<dc:creator><![CDATA[Selenska-Pobell, S.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
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<dc:title><![CDATA[Bacteria from uranium mining waste pile: Interactions with U(VI)]]></dc:title>
<dc:source><![CDATA[J. Alloys and Compounds 271-273, 262 (1998)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<identifier>HZDR:PUBLDB:2740-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<dc:creator><![CDATA[Schuster, G.]]></dc:creator>
<dc:creator><![CDATA[Bubner, M.]]></dc:creator>
<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2740-1</dc:identifier>
<dc:title><![CDATA[Thermoanalytical Investigations on the Oxidizing Degradation of Natural and Synthetic Humic Acids and their Calcium and Uranyl Complexes]]></dc:title>
<dc:source><![CDATA[12. Ulm-Freiberger Kalorimetrietage, Freiberg, Germany, 19.-21.3.1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2741-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Woedtke, F.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Denecke, M. A.]]></dc:creator>
<dc:creator><![CDATA[Nitsche, H.]]></dc:creator>
<dc:creator><![CDATA[Oppermann, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2741-1</dc:identifier>
<dc:title><![CDATA[Strukturuntersuchungen an Mischkristallen V<SUB>1-x</SUB>Nb<SUB>x</SUB>O<SUB>2</SUB>]]></dc:title>
<dc:source><![CDATA[9. Tagung Festkörperanalytik, Chemnitz, Germany, 23.-26.06.1997]]></dc:source>
<dc:date>1997</dc:date>
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<identifier>HZDR:PUBLDB:2846-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Fitz, C.]]></dc:creator>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Kolitsch, A.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2846-1</dc:identifier>
<dc:title><![CDATA[An instrument for in-situ stress measurement in thin films during growth]]></dc:title>
<dc:source><![CDATA[Surface and Coatings Technology 128-129 (2000) 474-478]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[An improved stress-measuring technique based on the cantilever bending principle is presented. Thermal shift of the sample holder position that results in errors in the stress data is minimised by evaluating the difference in the deflection of two laser beams. The film thickness is calculated from the reflected laser intensity or from ellipsometry data recorded simultaneously during film growth. Without using a lock-in technique or image processing, the resolution in bending force-per-unit-width is 0.02 N/m for a 50 µm thick cantilever. The system represents an easy, versatile and cheap technique to measure intrinsic and thermal stresses in thin films. The system has been employed to record the instantaneous stress during ion beam assisted deposition of BN films and the global stress during ion induced amorphisation of silicon. ]]></dc:description>
<dc:subject><![CDATA[cantilever]]></dc:subject>
<dc:subject><![CDATA[intrinsic stress]]></dc:subject>
<dc:subject><![CDATA[thin films]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2637-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:creator><![CDATA[Abram, S.]]></dc:creator>
<dc:creator><![CDATA[Maichle-Mößmer, C.]]></dc:creator>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2637-1</dc:identifier>
<dc:title><![CDATA[Synthesis and characterization of indium(III) complexes with tri- and pentadentate thiosemicarbazones. Crystal and molecular structure of [InCl2(HDAPTSC)] _ 2 DMSO, {O[In(HDAPTSC)(OH)]2} _ 5 MeOH, [InCl2-(APTSC)(MeOH)], [In(APTSC)2]PF6 and (H2APTSC)][InCl(APTSC)(mnt)] _ 0.5 H2O (H2DAPTSC = 2,6-diacetylpyridine-bis(thiosemicarbazone), HAPTSC = 2-acetylpyridine-thiosemicarbazone, mnt<SUP>2-</SUP> = 1,2-dicyanoethene-1,2-dithiolate)]]></dc:title>
<dc:source><![CDATA[Polyhedron 17 (1) 131 (1998)]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:2860-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Neumann, J.]]></dc:creator>
<dc:creator><![CDATA[Deerberg, G.]]></dc:creator>
<dc:creator><![CDATA[Schlüter, S.]]></dc:creator>
<dc:creator><![CDATA[Schmitt, W.]]></dc:creator>
<dc:creator><![CDATA[Hessel, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2860-1</dc:identifier>
<dc:title><![CDATA[Early Detection and Identification of Undesirable States in Chemical Plants Using Neural Networks]]></dc:title>
<dc:source><![CDATA[Keil, F., Mackens, W., Voß, H., Werther, J. (eds): Scientific Computing in Chemical Engineering II - Simulation, Image Processing, Optimization and Control, Springer-Verlag Berlin, Heidelberg, New York, 1999, S. 380-387, LSBN: 3-540-65851-3]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The suitability of pattern recognition for safety diagnosis of chemical plants is discussed. Experiments in a miniplant and with a process simulator are carried out. The process characteristics are treated with different recognition methods and classified with the aid of expert know how. Afterwards, the trained system can be used for process diagnosis. The capability of neural networks for this problem can be shown.]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
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<header>
<identifier>HZDR:PUBLDB:1740-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Valo, M.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Estorff, U.]]></dc:creator>
<dc:creator><![CDATA[Törrönen, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1740-1</dc:identifier>
<dc:title><![CDATA[Proposed Post Service Investigation on Decommissioned Greifswald Units]]></dc:title>
<dc:source><![CDATA[Proc. of the CSNI/CEC Workshop on Aged and Decommissioned Material Collection and Testing for Structural Integrity Purposes, Mol (Belgium), June 1995, OECD/GD !1996) 10, pp. 131 - 146]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The first four Greifswald reactor units belong to the WWER 440/230 reactor family and they are the only ones permanently shut-down. The status of the WWER 440 units as concerns the plant specific material data is shortly described in the paper. The lack of material data is a real problem of the 230 model reactors and the high lead factor in the surveillance irradiations of the more modern 213 units is an essential uncertainty  in the safety assessment of the units. In addition most aof the 230 units have been and some of the 213 units will be annealed. Greifswald units are fully representative WWER 440 units and they represent irradiated, irradiated-annealed and irradiated-annealed-reirradiated material conditions. In this paper a basic material research programme is proposed, which can greatly support the operating WWER units.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1740-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Valo, M.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Estorff, U.]]></dc:creator>
<dc:creator><![CDATA[Törrönen, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1740-7</dc:identifier>
<dc:title><![CDATA[Proposed Post Service Investigation on Decommissioned Greifswald Units]]></dc:title>
<dc:source><![CDATA[Proc. of the CSNI/CEC Workshop on Aged and Decommissioned Material Collection and Testing for Structural Integrity Purposes, Mol (Belgium), June 1995, OECD/GD !1996) 10, pp. 131 - 146]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The first four Greifswald reactor units belong to the WWER 440/230 reactor family and they are the only ones permanently shut-down. The status of the WWER 440 units as concerns the plant specific material data is shortly described in the paper. The lack of material data is a real problem of the 230 model reactors and the high lead factor in the surveillance irradiations of the more modern 213 units is an essential uncertainty  in the safety assessment of the units. In addition most aof the 230 units have been and some of the 213 units will be annealed. Greifswald units are fully representative WWER 440 units and they represent irradiated, irradiated-annealed and irradiated-annealed-reirradiated material conditions. In this paper a basic material research programme is proposed, which can greatly support the operating WWER units.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<header>
<identifier>HZDR:PUBLDB:14196-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Ankiewicz, A. O.]]></dc:creator>
<dc:creator><![CDATA[Martins, J. S.]]></dc:creator>
<dc:creator><![CDATA[Carmo, M. C.]]></dc:creator>
<dc:creator><![CDATA[Grundmann, M.]]></dc:creator>
<dc:creator><![CDATA[Zhou, S.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, H.]]></dc:creator>
<dc:creator><![CDATA[Sobolev, N. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14196-1</dc:identifier>
<dc:title><![CDATA[Ferromagnetic resonance on metal nanocrystals in Fe and Ni implanted ZnO]]></dc:title>
<dc:source><![CDATA[Journal of Applied Physics 107(2010), 09B518]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[We studied the angular dependence of the ferromagnetic resonance (FMR) spectra of (0001)ZnO single crystals implanted with Ni and Fe ions and compared the results to the data obtained by other experimental techniques, especially, x-ray diffraction (XRD) and superconducting quantum interference device magnetometry. The FMR revealed the formation of metal nanocrystals (NCs) embedded in the ZnO lattice in an oriented way. Whereas in the case of Ni, the conclusions drawn from the FMR studies corroborated the XRD and magnetometry results with respect to the alignment of the NCs in the host lattice, in the case of the Fe NCs, the FMR clearly shows that the hard magnetization axis (which is < 111 > in bcc Fe) is oriented perpendicular to the sample surface (parallel to the [0001]ZnO axis), at variance with the former XRD observations.]]></dc:description>
<dc:subject><![CDATA[ferromagnetic resonance]]></dc:subject>
<dc:subject><![CDATA[II-VI semiconductors]]></dc:subject>
<dc:subject><![CDATA[ion implantation]]></dc:subject>
<dc:subject><![CDATA[iron]]></dc:subject>
<dc:subject><![CDATA[magnetisation]]></dc:subject>
<dc:subject><![CDATA[nanostructured materials]]></dc:subject>
<dc:subject><![CDATA[nickel]]></dc:subject>
<dc:subject><![CDATA[X-ray diffraction]]></dc:subject>
<dc:subject><![CDATA[zinc compounds]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1063/1.3357999]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:825-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bergmann, U.]]></dc:creator>
<dc:creator><![CDATA[Bergner, F.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-825-2</dc:identifier>
<dc:title><![CDATA[Rißfortschrittsmessung an Dreipunkt-Biegeproben mit Ultraschall]]></dc:title>
<dc:source><![CDATA[Vortrags- und Diskussionstagung "Werkstoffprüfung 1996", 5.-6.12.96, Bad Nauheim, Tagungsband S. 143-151]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Ein Ultraschall-Laufzeit-Beugungsverfahren wurde zur Messung des Rißfortschritts im quasistatischen Dreipunkt-Biegeversuch an Proben unterschiedlicher Werkstoffe eingesetzt. Der mit diesem Verfahren bestimmte Gesamtrißfortschritt steht in guter Übereinstimmung mit dem jeweiligen fraktografisch bestimmten Wert. 
Durch eine geeignete Darstellungsweise der Ultraschallsignale konnte die Aussagekraft der Messungen deutlich erhöht werden. Insbesondere für Gußeisen zeigt sich ein ausgeprägter Übergang von Rißspitzenabstumpfung zu Rißausbreitung. Durch Ausnutzen der Bildinformationen kann der Rißfortschritt auch dann gemessen werden, wenn das Rißspitzenecho durch ein anderes Echo überlagert wird. 
Es wurde gezeigt, daß Rißfortschrittsmessungen prinzipiell auch auf der Grundlage von rißspitzengebeugten Longitudinalwellen möglich ist. ]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:825-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bergmann, U.]]></dc:creator>
<dc:creator><![CDATA[Bergner, F.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-825-1</dc:identifier>
<dc:title><![CDATA[Rißfortschrittsmessung an Dreipunkt-Biegeproben mit Ultraschall]]></dc:title>
<dc:source><![CDATA[Werkstoffprüfung '96, 5.-6.12.1996, Bad Nauheim, Deutscher Verband für Materialforschung und -prüfung e.V.]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Ein Ultraschall-Laufzeit-Beugungsverfahren wurde zur Messung des Rißfortschritts im quasistatischen Dreipunkt-Biegeversuch an Proben unterschiedlicher Werkstoffe eingesetzt. Der mit diesem Verfahren bestimmte Gesamtrißfortschritt steht in guter Übereinstimmung mit dem jeweiligen fraktografisch bestimmten Wert. 
Durch eine geeignete Darstellungsweise der Ultraschallsignale konnte die Aussagekraft der Messungen deutlich erhöht werden. Insbesondere für Gußeisen zeigt sich ein ausgeprägter Übergang von Rißspitzenabstumpfung zu Rißausbreitung. Durch Ausnutzen der Bildinformationen kann der Rißfortschritt auch dann gemessen werden, wenn das Rißspitzenecho durch ein anderes Echo überlagert wird. 
Es wurde gezeigt, daß Rißfortschrittsmessungen prinzipiell auch auf der Grundlage von rißspitzengebeugten Longitudinalwellen möglich ist. ]]></dc:description>
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<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:579-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Richter, H.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-579-1</dc:identifier>
<dc:title><![CDATA[Determination of Crack-Initiation Toughness by Impact and Dynamic Testing]]></dc:title>
<dc:source><![CDATA[Proc. of the 11th European Conference on Fracture - ECF 11, Poitiers-Futurscope, France, Sept. 1996, Vol. III, pp. 2001 - 2006]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The critical J-integral (Jid) can be useful as toughness parameter at initiation of stable crack growth. Under the condition of the impact bending test the critical step for evaluating of Jid is the detection of the crack initiation point on the impact load displacement curve. In this paper the crack initiation is determined by using emission of acoustic waves (AE). The experimental techniques used to evaluate Jid include both instrumented impact testing based on 300 J pendulum impact tester with a piezoelectric broadband AE sensor within the impact tup and dynamic 3 point bending loading with a servohydraulic test machine and additional AE sensors on the specimen.
Different kind of pulses of the AE signals can be observed. One of them corresponds with crack initiation. The evidence of initiation at this point was confirmed by single and multiple specimen methods. ]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:579-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Richter, H.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Viehrig, H.-W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-579-7</dc:identifier>
<dc:title><![CDATA[Determination of Crack-Initiation Toughness by Impact and Dynamic Testing]]></dc:title>
<dc:source><![CDATA[Proc. of the 11th European Conference on Fracture - ECF 11, Poitiers-Futurscope, France, Sept. 1996, Vol. III, pp. 2001 - 2006]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[The critical J-integral (Jid) can be useful as toughness parameter at initiation of stable crack growth. Under the condition of the impact bending test the critical step for evaluating of Jid is the detection of the crack initiation point on the impact load displacement curve. In this paper the crack initiation is determined by using emission of acoustic waves (AE). The experimental techniques used to evaluate Jid include both instrumented impact testing based on 300 J pendulum impact tester with a piezoelectric broadband AE sensor within the impact tup and dynamic 3 point bending loading with a servohydraulic test machine and additional AE sensors on the specimen.
Different kind of pulses of the AE signals can be observed. One of them corresponds with crack initiation. The evidence of initiation at this point was confirmed by single and multiple specimen methods. ]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:14270-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Deuther-Conrad, W.]]></dc:creator>
<dc:creator><![CDATA[Becker, G.]]></dc:creator>
<dc:creator><![CDATA[Fischer, S.]]></dc:creator>
<dc:creator><![CDATA[Hiller, A.]]></dc:creator>
<dc:creator><![CDATA[Østergaard Nielsen, E.]]></dc:creator>
<dc:creator><![CDATA[Brunicardi Timmermann, D.]]></dc:creator>
<dc:creator><![CDATA[Patt, M.]]></dc:creator>
<dc:creator><![CDATA[Sabri, O.]]></dc:creator>
<dc:creator><![CDATA[Peters, D.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14270-1</dc:identifier>
<dc:title><![CDATA[In Vivo Binding of [18F]NS10743 on α7 Nicotinic Acetylcholine Receptors (α7-nAChR) in Pig Brain]]></dc:title>
<dc:source><![CDATA[23rd Annual Congress of the European Association of Nuclear Medicine (EANM), 09.-13.10.2010, Wien, Österreich]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Aim: Alterations of α7-nAChR have been observed in schizophrenia, brain trauma and neurodegenerative diseases. For PET imaging of α7 nAChR [18F]NS10743 has been successfully developed and evaluated in mice by tissue distribution and specificity studies. Here we report on baseline and blocking PET studies with [18F]NS10743 in pig brain. 

Materials and Methods: Dynamic PET scanning (2h) was performed in anesthetized female piglets (13-15 kg), intravenously injected with ~ 330 MBq [18F]NS10743 (specific activity >150 GBq/µmol). Three animals additionally received 5 mg/kg of the α7 nAChR antagonist NS6740. Plasma samples were taken and metabolite-corrected input functions were estimated. Individual regions of interest were defined using an MRI-based template of pig brain.  SUV, distribution volume (VT= K1/k2) and binding potential (BPND = (VT region - VT reference)/VT reference) were estimated. 

Results: [18F]NS10743 readily passed the blood-brain barrier and the uptake of radioactivity peaked with SUV = 2.23±0.71 at 8-10 min in the baseline scan while in NS6740-blocking studies the radioactivity levels peaked significantly earlier (SUV = 3.02 ± 1.28 at 6 min)  and decreased faster. At the end of study (between 90 and 120 min pi) SUV was significantly decreased by NS6740 in all investigated brain regions except olfactory bulb, which was chosen as reference region for calculation of BPND. At baseline, a mean VT value of 6.07±1.54 was estimated with the highest radiotracer accumulation in temporal, parietal, and occipital lobe, thalamus, striatum, and middle cortex (VT = 7.27±1.95  7.10±1.58). Intermediate binding was observed in hippocampus, colliculi, midbrain, frontal lobe, and ventral cortex (VT = 6.76±1.71  6.09±1.05), and lowest values were assessed in the cerebellum, pons, and olfactory bulb (VT = 5.71±1.18  4.11±0.96). Baseline BPND values for high (temporal lobe), median (hippocampus) and low specific binding (cerebellum) were  0.76±0.07, 0.54±0.08, and 0.39±0.08, respectively. NS6740 significantly reduced the binding potential BPND in regions with high [18F]NS10743 binding (temporal lobe: -29 %, p = 0.01; midbrain: -35 %, p = 0.02) while the decrease in regions with low binding was not significant (cerebellum: -16 %, p = 0.2). 

Conclusion: The data provide clear evidence of in vivo binding of [18F]NS10743 at α7 nAChR. However, with regard to the low density of α7 nAChR expression in the brain further modifications of the NS10743 core structure are needed to increase the target affinity of the tracer compound.]]></dc:description>
<dc:subject><![CDATA[α7-nAChR]]></dc:subject>
<dc:subject><![CDATA[neurodegenerative diseases]]></dc:subject>
<dc:subject><![CDATA[[18F]NS10743]]></dc:subject>
<dc:subject><![CDATA[PET]]></dc:subject>
<dc:subject><![CDATA[blood-brain barrier]]></dc:subject>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:14270-2</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brust, P.]]></dc:creator>
<dc:creator><![CDATA[Deuther-Conrad, W.]]></dc:creator>
<dc:creator><![CDATA[Becker, G.]]></dc:creator>
<dc:creator><![CDATA[Fischer, S.]]></dc:creator>
<dc:creator><![CDATA[Hiller, A.]]></dc:creator>
<dc:creator><![CDATA[Østergaard Nielsen, E.]]></dc:creator>
<dc:creator><![CDATA[Brunicardi Timmermann, D.]]></dc:creator>
<dc:creator><![CDATA[Patt, M.]]></dc:creator>
<dc:creator><![CDATA[Sabri, O.]]></dc:creator>
<dc:creator><![CDATA[Peters, D.]]></dc:creator>
<dc:creator><![CDATA[Steinbach, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14270-2</dc:identifier>
<dc:title><![CDATA[In Vivo Binding of [18F]NS10743 on α7 Nicotinic Acetylcholine Receptors (α7-nAChR) in Pig Brain]]></dc:title>
<dc:source><![CDATA[European Journal of Nuclear Medicine and Molecular Imaging 37(2010)2, 198-311]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Aim: Alterations of α7-nAChR have been observed in schizophrenia, brain trauma and neurodegenerative diseases. For PET imaging of α7 nAChR [18F]NS10743 has been successfully developed and evaluated in mice by tissue distribution and specificity studies. Here we report on baseline and blocking PET studies with [18F]NS10743 in pig brain. 

Materials and Methods: Dynamic PET scanning (2h) was performed in anesthetized female piglets (13-15 kg), intravenously injected with ~ 330 MBq [18F]NS10743 (specific activity >150 GBq/µmol). Three animals additionally received 5 mg/kg of the α7 nAChR antagonist NS6740. Plasma samples were taken and metabolite-corrected input functions were estimated. Individual regions of interest were defined using an MRI-based template of pig brain.  SUV, distribution volume (VT= K1/k2) and binding potential (BPND = (VT region - VT reference)/VT reference) were estimated. 

Results: [18F]NS10743 readily passed the blood-brain barrier and the uptake of radioactivity peaked with SUV = 2.23±0.71 at 8-10 min in the baseline scan while in NS6740-blocking studies the radioactivity levels peaked significantly earlier (SUV = 3.02 ± 1.28 at 6 min)  and decreased faster. At the end of study (between 90 and 120 min pi) SUV was significantly decreased by NS6740 in all investigated brain regions except olfactory bulb, which was chosen as reference region for calculation of BPND. At baseline, a mean VT value of 6.07±1.54 was estimated with the highest radiotracer accumulation in temporal, parietal, and occipital lobe, thalamus, striatum, and middle cortex (VT = 7.27±1.95  7.10±1.58). Intermediate binding was observed in hippocampus, colliculi, midbrain, frontal lobe, and ventral cortex (VT = 6.76±1.71  6.09±1.05), and lowest values were assessed in the cerebellum, pons, and olfactory bulb (VT = 5.71±1.18  4.11±0.96). Baseline BPND values for high (temporal lobe), median (hippocampus) and low specific binding (cerebellum) were  0.76±0.07, 0.54±0.08, and 0.39±0.08, respectively. NS6740 significantly reduced the binding potential BPND in regions with high [18F]NS10743 binding (temporal lobe: -29 %, p = 0.01; midbrain: -35 %, p = 0.02) while the decrease in regions with low binding was not significant (cerebellum: -16 %, p = 0.2). 

Conclusion: The data provide clear evidence of in vivo binding of [18F]NS10743 at α7 nAChR. However, with regard to the low density of α7 nAChR expression in the brain further modifications of the NS10743 core structure are needed to increase the target affinity of the tracer compound.]]></dc:description>
<dc:subject><![CDATA[α7-nAChR]]></dc:subject>
<dc:subject><![CDATA[neurodegenerative diseases]]></dc:subject>
<dc:subject><![CDATA[[18F]NS10743]]></dc:subject>
<dc:subject><![CDATA[PET]]></dc:subject>
<dc:subject><![CDATA[blood-brain barrier]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14270-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
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<record>
<header>
<identifier>HZDR:PUBLDB:3073-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Lielausis, O.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3073-1</dc:identifier>
<dc:title><![CDATA[The behaviour of gas bubbles in a turbulent liquid metal MHD flow, Part II: The influence of an external magnetic field on the slip ratio in a liquid metal bubbly flow]]></dc:title>
<dc:source><![CDATA[International Journal of Multiphase Flow (2000),
Vol. 26/1, 67-82]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The influence of an steady, homogeneous magnetic field on the slip ratio in a liquid metal bubbly flow is investigated. An one-dimensional model has been developed describing the motion of an ensemble of bubbles in a MHD flow. Calculations are presented for magnetic fields aligned transverse and parallel to the mean flow direction. While in the longitudinal case the slip decreases monotonously with growing field strength, it passes a minimum and increases again for large fields if B is directed transverse to the flow. In order to prove the theoretical predictions experiments are performed in a sodium-argon flow exposed to a transverse field and a mercury-nitrogen flow with a longitudinal magnetic field.]]></dc:description>
<dc:subject><![CDATA[liquid metal-gas flow]]></dc:subject>
<dc:subject><![CDATA[bubble]]></dc:subject>
<dc:subject><![CDATA[magnetic field]]></dc:subject>
<dc:subject><![CDATA[void fraction]]></dc:subject>
<dc:subject><![CDATA[drag coefficient]]></dc:subject>
<dc:subject><![CDATA[slip ratio]]></dc:subject>
<dc:subject><![CDATA[resistivity probe]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:1625-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Böttger, A.]]></dc:creator>
<dc:creator><![CDATA[Zschau, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1625-2</dc:identifier>
<dc:title><![CDATA[A New Wire-Mesh Tomograph for Gas-Liquid Flows]]></dc:title>
<dc:source><![CDATA[Conference Frontiers in Industrial Process Tomography II, Delft, The Nederlands, April 9 - 12, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[A wire-mesh tomograph for gas-liquid two-phase flows is presented. It is based on the measurement of the conductivity distribution over the cross section of the flow. Two planes of wire grids are placed into the flow in a short distance from each other. The angle between the wires of both grids is 90 °. The conductivity is measured at all cross points of the wires of the two planes. An imaging rate of 1000 frames per second was achieved, the measured data is directly transformed into local volumetric gas fractions without image reconstruction efforts. The minimal conductivity of the liquid necessary for applying the sensor is very low. Pure water (s » 0.5 µS/cm) can be measured without any problems. Up to now, the 2 x 16 wire mesh sensor was tested in a vertical air-water flow.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1625-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<dc:title><![CDATA[Pd diffusion in ZnTe and CdTe]]></dc:title>
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<dc:title><![CDATA[Sequences around the fragmentation sites of the large subunit rRNA in the family Rhizobiaceae]]></dc:title>
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<dc:source><![CDATA[Radiochim. Acta 80, 1 (1998)]]></dc:source>
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<dc:title><![CDATA[Zur Problematik der Bestimmung dynamischer Festigkeitswerte im instrumentierten Kerbschlagbiegeversuch]]></dc:title>
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<dc:description><![CDATA[Zur Bewertung der strukturellen Integrität von Bauteilen werden auch Festigkeitskennwerte unter schlagartigen Belastungsbedingungen benötigt.
Eine Möglichkeit dynamische Festigkeitskennwerte abzuschätzen, bietet die Berechnung der dynamischen Fließ- und Biegebruchspannungen aus den nach ISO/CD 14 556 im instrumentierten Kerbschlagbiegeversuch bestimmten charakteristischen Kräften. Üblicherweise werden die Festigkeitswerte unter Schlagbiegebelastung nach einem Vorschlag von SERVER (1978) berechnet. Dieser Vorschlag wurde aus einer Lösung der Fließlinientheorie nach EWING (1968) abgeleitet.
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<dc:title><![CDATA[Evidence for Relativistic Effects in the Chemistry of Element 104]]></dc:title>
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<dc:source><![CDATA[Workshop Institut für Kernchemie der Universität Mainz, Mainz, Germany, 13. 03. 1998]]></dc:source>
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<dc:creator><![CDATA[Strobel, M.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
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<dc:title><![CDATA[Formation and self-organization of nanoclusters by ion beam synthesis: a combined atomistic and continuum description]]></dc:title>
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<dc:creator><![CDATA[Trushin, Y. V.]]></dc:creator>
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<dc:creator><![CDATA[Kulikov, D. V.]]></dc:creator>
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<dc:creator><![CDATA[Kreißig, U.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Pezoldt, J.]]></dc:creator>
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<dc:title><![CDATA[A computational model of the formation of (SiC)<SUB>1-x</SUB>(AlN)<SUB>x</SUB> structures by hot, high-dose N<SUP>+</SUP> and Al<SUP>+</SUP> coimplants in 6H-SiC]]></dc:title>
<dc:source><![CDATA[Int. Conf. on Silicon Carbide, III-Nitrides and Related Materials, Stockholm, Sweden, 
Aug. 31 - Sept. 5, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Kachurin, G. A.]]></dc:creator>
<dc:creator><![CDATA[Zhuravlev, K. S.]]></dc:creator>
<dc:creator><![CDATA[Pazdnikov, N. A.]]></dc:creator>
<dc:creator><![CDATA[Volodin, V. A.]]></dc:creator>
<dc:creator><![CDATA[Gutakovsky, A. K.]]></dc:creator>
<dc:creator><![CDATA[Leier, A. F.]]></dc:creator>
<dc:creator><![CDATA[Fröb, H.]]></dc:creator>
<dc:creator><![CDATA[Leo, K.]]></dc:creator>
<dc:creator><![CDATA[Böhme, T.]]></dc:creator>
<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
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<dc:title><![CDATA[Blue photoluminescence from high-dose Si<SUP>+</SUP>- and Ge<SUP>+</SUP>-implanted silicon-dioxide layers]]></dc:title>
<dc:source><![CDATA[Int. Workshop des Innovationskollegs der TU Chemnitz "Methoden und Materialsysteme für den Nanometerbereich", Schöneck/Vogtl., March 3 - 5, 1997]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
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<dc:creator><![CDATA[Scheffler, M.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
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<dc:title><![CDATA[A Finite Element Based Vibration Model for VVER-440 Type Reactors Considering the Fluid-Structure-Interaction]]></dc:title>
<dc:source><![CDATA[Proc. Jahrestagung Kerntechnik '95, Nürnberg, 16. - 18. Mai 1995, S. 227 - 230]]></dc:source>
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Grunwald, G.]]></dc:creator>
<dc:creator><![CDATA[Scheffler, M.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-437-1</dc:identifier>
<dc:title><![CDATA[A Finite Element Based Vibration Model for VVER-440 Type Reactors Considering the Fluid-Structure-Interaction]]></dc:title>
<dc:source><![CDATA[Jahrestagung Kerntechnik 1995]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Hensel, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-812-1</dc:identifier>
<dc:title><![CDATA[Dichtemessung mit Positronenstrahlung]]></dc:title>
<dc:source><![CDATA[ACHEMA 97: Int. Treffen für chem. Technik, Umweltschutz und Biotechnologie, 25. Ausstellungstagung, 9.-14. Juni 1997, Frankfurt/Main]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[Ein berührungsloses Dichtemeßverfahren für Medien geringer Dichte wird vorgestellt, das auf der Abhängigkeit der Reichweite von Positronenstrahlung von der Dichte des Meßmediums beruht. Die Positronen werden von einem Radionuklid in einer festen Quelle erzeugt und in das zu untersuchende Volumen emittiert. Seitlich angeordnete Detektoren registrieren die bei der Annihilation der Positronen entstehenden Gammaquanten. Das Verfahren wurde in einem Dichtebereich von 15 kg/m<SUP>3</SUP> bis 38 kg/m<SUP>3</SUP> getestet, eine Erweiterung des Meßbereichs von 5 kg/m<SUP>3</SUP> bis 300 kg/m<SUP>3</SUP> ist möglich. 

Einsatzfelder sind mehrphasige Strömungen mit hohem Massenstromanteil der gasförmigen Phase (Schäume und Dämpfe) sowie unter Druck stehende Gase. Der Vorteil des Verfahrens besteht in einer Kombination der hohen Dichtesensitivität der Betastrahlung mit der geringen Absorption der bei der Annihilation entstehenden Gammastrahlung in Rohr- bzw. Behälterwänden. ]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Wieteska, K.]]></dc:creator>
<dc:creator><![CDATA[Wierzchowski, W.]]></dc:creator>
<dc:creator><![CDATA[Turos, A.]]></dc:creator>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2476-1</dc:identifier>
<dc:title><![CDATA[Synchrotron X-ray studies of AlGaAs/GaAs epitaxial layers implanted with Se ions]]></dc:title>
<dc:source><![CDATA[4th Symp. on Synchrotron Radiation, Krakow, PL, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Wirth, H.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Coleman, P. G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2477-1</dc:identifier>
<dc:title><![CDATA[Investigation of ion-implantation induced damage in 6H-SiC by RBS/C and Positron Annihilation Spectroscopy]]></dc:title>
<dc:source><![CDATA[Int. Conf. on Silicon Carbide, III-Nitrides and Related Materials, Stockholm, Sweden,
Aug. 31 - Sept. 5, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Wirth, H.]]></dc:creator>
<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2478-1</dc:identifier>
<dc:title><![CDATA[Kristallgitter-Einbau implantierter Ionen in 6H-SiC]]></dc:title>
<dc:source><![CDATA[DPG-Frühjahrstagung, Münster, March 17 - 21, 1997]]></dc:source>
<dc:date>1997</dc:date>
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<identifier>HZDR:PUBLDB:2922-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Wagner, A.]]></dc:creator>
<dc:creator><![CDATA[Müntz, C.]]></dc:creator>
<dc:creator><![CDATA[Oeschler, H.]]></dc:creator>
<dc:creator><![CDATA[Sturm, C.]]></dc:creator>
<dc:creator><![CDATA[Barth, R.]]></dc:creator>
<dc:creator><![CDATA[Cieslak, M.]]></dc:creator>
<dc:creator><![CDATA[Debowski, M.]]></dc:creator>
<dc:creator><![CDATA[Grosse, E.]]></dc:creator>
<dc:creator><![CDATA[Koczon, P.]]></dc:creator>
<dc:creator><![CDATA[Mang, M.]]></dc:creator>
<dc:creator><![CDATA[Miskowiec, D.]]></dc:creator>
<dc:creator><![CDATA[Schicker, R.]]></dc:creator>
<dc:creator><![CDATA[Schwab, E.]]></dc:creator>
<dc:creator><![CDATA[Senger, P.]]></dc:creator>
<dc:creator><![CDATA[Beckerle, P.]]></dc:creator>
<dc:creator><![CDATA[Brill, D.]]></dc:creator>
<dc:creator><![CDATA[Shin, Y.-H.]]></dc:creator>
<dc:creator><![CDATA[Ströbele, H.]]></dc:creator>
<dc:creator><![CDATA[Walus, W.]]></dc:creator>
<dc:creator><![CDATA[Kohlmeyer, B.]]></dc:creator>
<dc:creator><![CDATA[Pühlhofer, F.]]></dc:creator>
<dc:creator><![CDATA[Speer, J.]]></dc:creator>
<dc:creator><![CDATA[Völkel, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2922-1</dc:identifier>
<dc:title><![CDATA[Evidence for Different Freeze-out Radii of High- and Low-energy Pions Emitted in Au+Au Collisions at 1 AGeV.]]></dc:title>
<dc:source><![CDATA[Physics Letters B 420 (1998) 20-24]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Double differential production cross sections of pi- and pi+ mesons and the number of participating protons have been measured
in central Au+Au collisions at 1 GeV/nucleon.
At low pion energies the pi- yield is strongly enhanced over the pi+ yield.
The energy dependence of the pi-/pi+ ratio is assigned to the Coulomb interaction of the charged pions with the protons in the reaction zone.
The deduced Coulomb potential increases with increasing pion c.m. energy.
This behavior indicates different freeze-out radii for different pion energies in the c.m. frame.]]></dc:description>
<dc:subject><![CDATA[pi- pi+ meson Au+Au 1 AGeV Coulomb]]></dc:subject>
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<identifier>HZDR:PUBLDB:2479-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Witke, W.]]></dc:creator>
<dc:creator><![CDATA[Siemroth, P.]]></dc:creator>
<dc:creator><![CDATA[Brückner, J.]]></dc:creator>
<dc:creator><![CDATA[Brutscher, J.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2479-1</dc:identifier>
<dc:title><![CDATA[Ionenimplantation aus Vakuumbogenplasmen]]></dc:title>
<dc:source><![CDATA[8. Bundesdeutsche Fachtagung Plasmatechnologie, Dresden, Sept. 14 - 17, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<header>
<identifier>HZDR:PUBLDB:1281-1</identifier>
<datestamp>2023-05-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Kaschny, J. R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1281-1</dc:identifier>
<dc:title><![CDATA[Cavities in helium implanted and annealed silicon characterized by spectroscopic ellipsometry]]></dc:title>
<dc:source><![CDATA[Journal of Applied Physics, October 15, 1999, Volume 86, Issue 8, pp. 4067-4713]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The formation of helium induced cavities in silicon during short-time annealing is analyzed by spectroscopic ellipsometry. Specimens implanted with 40 keV He+ ions to a dose of 5×1016 cm2 are heat treated at 800 °C for times of 11200 s by rapid thermal annealing. Spectroscopic ellipsometry is employed to obtain quantitative information on the cavity volume depth profiles. A newly developed formula is used to model the optical multilayer depth profiles. The cavity volume is found to increase during annealing for about 300 s and to decrease for longer annealing times. Over this characteristic time a marked change in the He loss occurs, which has been reported only recently. Swelling of the helium implanted and annealed silicon is analyzed using an atomic force microscope. Step heights are consistent with the cavity volume per unit area obtained from spectroscopic ellipsometry data analysis. The number density of cavities after annealing for 600 s is calculated to be 1.16±0.27×1017 cm3 and is found to be largely independent of depth in the central part of the cavity layer.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1063/1.371341]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:1272-1</identifier>
<datestamp>2023-05-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Küchler, R.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1272-1</dc:identifier>
<dc:title><![CDATA[Ultrasonic Surface Waves for Studying the Properties of Thin Films]]></dc:title>
<dc:source><![CDATA[Thin Solid Films 315 (1998) 29-34]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The change of the spreading velocity of ultrasonic surface waves by thin film deposition is descibed by an approximation of the nonlinear equations of motion. The effect of residual stress in deposited films on the spreading velocity is considered. As an example for practical applications, the velocity change of surface waves after TiN-film desposition on steel bars in investigated.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0040-6090(97)00457-4]]></dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:14287-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Akhmadaliev, C.]]></dc:creator>
<dc:creator><![CDATA[Ridgway, M.]]></dc:creator>
<dc:creator><![CDATA[Kluth, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14287-1</dc:identifier>
<dc:title><![CDATA[Swift Heavy Ion Beam Shaping of Au and Ge Nanoparticles in SiO2]]></dc:title>
<dc:source><![CDATA[21st International Conference on the Application of Accelerators in Research and Industry (CAARI 2010), 08.-13.08.2010, Dallas/Fortworth, Texas, USA]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Lasers can process materials at spatiotemporal µm and ps scales. Here it will be shown that swift heavy ions can be used for materials processing at even shorter length and time scales.  Swift-heavy-ion-induced deformation of spherical Au and Ge nanoclusters (NCs) embedded in SiO2 was studied experimentally and theoretically. Ge NC shaping is size dependent under  irradiation with 38 MeV iodine ions and with 89 and 185 MeV gold ions. Large NCs dont deform, smaller ones become discus-shaped, and very small ones show Ge loss at their equator. Small Au NCs deform into rods and wires, and, rather exotic, at critical NC size Au wires are squeezed out of the poles of the Au spheres.
Modeling and atomistic computer simulations identified the main driving forces: (i) The materials dependent electronic stopping power, (ii) the volume change upon melting, (iii) the asymmetric hydrodynamic flow due to stress field hysteresis, as well as (iv) far-from-equilibrium steady-state solubilities and strongly anisotropic diffusion. The latter one leads to Ostwald ripening of deformed NCs. The NC size distributions, shapes and anisotropies can be tailored by appropriate tuning of the driving forces. Our model describes the ion-induced shape evolution of different elements for different ion species, energies and fluences even quantitatively, where only one fit parameter describes all experiments. It is based on classical thermodynamics and hydrodynamics only. An even stronger proof is the shape change of nanospheres of critical size under swift heavy ion irradiation. For such particles, exclusively central ion impacts induce shaping, where Au is squeezed out of the poles. Using an unimodal size distributions and changing the ion impact angle during irradiation, tailoring of very exotic nanoparticle shapes become feasible.]]></dc:description>
<dc:subject><![CDATA[swift heavy ion irradiation]]></dc:subject>
<dc:subject><![CDATA[nanoparticles]]></dc:subject>
<dc:subject><![CDATA[silicon dioxide]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:2430-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hensel, F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2430-1</dc:identifier>
<dc:title><![CDATA[Positronen-Emissions-Tomographie zur Untersuchung von Zweiphasenströmungen]]></dc:title>
<dc:source><![CDATA[Workshop "Meßtechnik für stationäre und transiente Mehrphasenströmungen", Rossendorf, 24.-25.September 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Die Technik der Positronen-Emissions-Tomographie (Positron Emission Tomography, PET) ist ein bildgebendes Verfahren, das für die Nuklearmedizin entwickelt wurde. Im medizinischen Bereich wird diese Technik hauptsächlich als nichtinvasives Untersuchungsverfahren für die quantitative Erfassung von Stoffwechselvorgängen in-vivo genutzt. Hierzu werden die interessierenden Stoffsysteme mit Positronen emittierenden Nukliden wie <SUP>11</SUP>C, <SUP>13</SUP>N, <SUP>15</SUP>O oder <SUP>18</SUP>F markiert. Die Halbwertszeiten dieser Nuklide liegen im Bereich einiger Minuten bis zu einigen Stunden. In einer Vielzahl von organischen Verbindungen können damit die natürlich vorkommenden Nuklide durch ein β<SUP>+</SUP>-instabiles Isotop ersetzt werden.
<P>Die Methode Verfahren PET wurde zur Untersuchung von Zweiphasenströmungen gasförmig / flüssig angewendet. Inhalt des Vortrages sind die Darstellung von Ergebnissen der Messung des Dispersionskoeffizienten in einer turbulenten Blasenströmung und die Vorstellung geplanter Anwendungen dieser Tracertechnik in einem derzeit in Aufbau befindlichen PET-Tomographen für Schaumuntersuchungen. </P>]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2430-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hensel, F.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-2430-2</dc:identifier>
<dc:title><![CDATA[Positronen-Emissions-Tomographie zur Untersuchung von Zweiphasenströmungen]]></dc:title>
<dc:source><![CDATA[Prasser, Horst-Michael: (Hrsg.): Workshop "Meßtechnik für stationäre und transiente Mehrphasenströmungen", Forschungszentrum Rossendorf; FZR-241, 1998, 91-96]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Die Technik der Positronen-Emissions-Tomographie (Positron Emission Tomography, PET) ist ein bildgebendes Verfahren, das für die Nuklearmedizin entwickelt wurde. Im medizinischen Bereich wird diese Technik hauptsächlich als nichtinvasives Untersuchungsverfahren für die quantitative Erfassung von Stoffwechselvorgängen in-vivo genutzt. Hierzu werden die interessierenden Stoffsysteme mit Positronen emittierenden Nukliden wie <SUP>11</SUP>C, <SUP>13</SUP>N, <SUP>15</SUP>O oder <SUP>18</SUP>F markiert. Die Halbwertszeiten dieser Nuklide liegen im Bereich einiger Minuten bis zu einigen Stunden. In einer Vielzahl von organischen Verbindungen können damit die natürlich vorkommenden Nuklide durch ein β<SUP>+</SUP>-instabiles Isotop ersetzt werden.
<P>Die Methode Verfahren PET wurde zur Untersuchung von Zweiphasenströmungen gasförmig / flüssig angewendet. Inhalt des Vortrages sind die Darstellung von Ergebnissen der Messung des Dispersionskoeffizienten in einer turbulenten Blasenströmung und die Vorstellung geplanter Anwendungen dieser Tracertechnik in einem derzeit in Aufbau befindlichen PET-Tomographen für Schaumuntersuchungen. </P>]]></dc:description>
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<dc:language>ger</dc:language>
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<header>
<identifier>HZDR:PUBLDB:2480-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Kaschny, J. R.]]></dc:creator>
<dc:creator><![CDATA[Fichtner, P. L. F.]]></dc:creator>
<dc:creator><![CDATA[Mücklich, A.]]></dc:creator>
<dc:creator><![CDATA[Kreißig, U.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2480-1</dc:identifier>
<dc:title><![CDATA[Impurity gettering effects in separation-by-implanted-oxygen (SIMOX) structures - what getters what, where and how]]></dc:title>
<dc:source><![CDATA[10th Biennial Conf. on Insulating Films on Semiconductors, Stenungsund, Sweden, June 11 - 14, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2481-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Betzl, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2481-1</dc:identifier>
<dc:title><![CDATA[Neutronenstreuung am RFR]]></dc:title>
<dc:source><![CDATA[Vortrag auf Kolloquium des VKTA - 40 Jahre Rossendorfer Forschungsreaktor RFR, Rossendorf, Dec. 16, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:2482-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2482-1</dc:identifier>
<dc:title><![CDATA[Zusammenarbeit mit industriellen Einrichtungen (Industriekooperation)]]></dc:title>
<dc:source><![CDATA[Vortrag zur Evaluierung durch den Wissenschaftlichen Beirat des FZR, Rossendorf, Apr. 29, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2482-1</dc:relation>
<dc:audience>Researchers</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2483-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2483-1</dc:identifier>
<dc:title><![CDATA[Ionenstrahlphysik und Technik im Forschungszentrum Rossendorf]]></dc:title>
<dc:source><![CDATA[FernUniversität Hagen, FB Elektrotechnik, Jan. 31, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:1148-1</identifier>
<datestamp>2023-05-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Böttger, A.]]></dc:creator>
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<dc:description><![CDATA[The paper presents an electrode-mesh tomograph for the high-speed visualisation of transient gas fraction distributions in two-phase flows in pipes. It is based on the measurement of the local instantaneous conductivity of the two-phase mixture. The time resolution of the device is 1024 frames per second. The sensor consists of two electrode grids with 16 electrodes each. This results in 16 x 16 sensitive points, which are equally distributed over the cross section. The sensor is available in two designs: (1) wire-mesh sensor for lab applications and (2) sensor with enforced electrode rods for high mechanical loads. The device was recently tested in a vertical and a horizontal air-water flow in a pipe of 51.2 mm diameter.]]></dc:description>
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<dc:description><![CDATA[Six different types of boron nitride films were investigated by polarized infrared reflection spectroscopy. Films with a highly cubic, mixed cubic and non-cubic, and exclusively non-cubic phase composition were synthesized using ion beam assisted deposition. Additionally, post-deposition argon ion irradiated cubic and non-cubic boron nitride films as well as nitrogen implanted boron sample were analyzed. Using this technique, besides the cubic phase, two different non-cubic modifications, layered anisotropic and amorphous, could be distinguished. A preferentional orientation of the normal axis of the sp2-bonded basal planes parallel to the substrate surface was observed.]]></dc:description>
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<br>
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<br>
Proceedings, Vol. 2(1993)321-324]]></dc:source>
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<br>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Taut, S.]]></dc:creator>
<dc:creator><![CDATA[Hübener, S.]]></dc:creator>
<dc:creator><![CDATA[Eichler, B.]]></dc:creator>
<dc:creator><![CDATA[Gäggeler, H. W.]]></dc:creator>
<dc:creator><![CDATA[Schädel, M.]]></dc:creator>
<dc:creator><![CDATA[Zvara, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2675-1</dc:identifier>
<dc:title><![CDATA[Thermochromatography of Heavy Actinides - Determination of the Sublimation Enthalpy of Es]]></dc:title>
<dc:source><![CDATA[Radiochimica Acta 78, 33-38 (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2676-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Janssen, D.]]></dc:creator>
<dc:creator><![CDATA[Buettig, H.]]></dc:creator>
<dc:creator><![CDATA[Bushuev, A.]]></dc:creator>
<dc:creator><![CDATA[Karliner, M.]]></dc:creator>
<dc:creator><![CDATA[Konstantinov, S.]]></dc:creator>
<dc:creator><![CDATA[Kruchkov, J.]]></dc:creator>
<dc:creator><![CDATA[Myskin, O.]]></dc:creator>
<dc:creator><![CDATA[Petrov, V.]]></dc:creator>
<dc:creator><![CDATA[Sedlyarov, I.]]></dc:creator>
<dc:creator><![CDATA[Tribendis, A.]]></dc:creator>
<dc:creator><![CDATA[Volkov, V.]]></dc:creator>
<dc:creator><![CDATA[Stein, P.]]></dc:creator>
<dc:creator><![CDATA[Vogel, H. P.]]></dc:creator>
<dc:creator><![CDATA[Matheisen, A.]]></dc:creator>
<dc:creator><![CDATA[Pekeler, M.]]></dc:creator>
<dc:creator><![CDATA[Sandner, W.]]></dc:creator>
<dc:creator><![CDATA[Will, I.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2676-1</dc:identifier>
<dc:title><![CDATA[A superconducting RF gun: Current status of the Drossel cooperation]]></dc:title>
<dc:source><![CDATA[European Conference on Application of Accelerators in Research and Technology, Dresden, July 1999; P1 - 159]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The Drossel collaboration was established for the development of a low emittance high average current injector for the ELBE project. The injector is based on a photocathode RF gun with a superconducting cavity. The high average current is especially important for applied research and other  applications. First tests of the gun cavity has been done at DESY TTF.                                                                 ]]></dc:description>
<dc:subject><![CDATA[Drossel cooperation]]></dc:subject>
<dc:subject><![CDATA[superconducting RF gun]]></dc:subject>
<dc:subject><![CDATA[DESY TTF]]></dc:subject>
<dc:subject><![CDATA[applied research]]></dc:subject>
<dc:subject><![CDATA[photocathode]]></dc:subject>
<dc:subject><![CDATA[high average current]]></dc:subject>
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<identifier>HZDR:PUBLDB:132-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Große, M.]]></dc:creator>
<dc:creator><![CDATA[Böhmert, J.]]></dc:creator>
<dc:creator><![CDATA[Eichhorn, F.]]></dc:creator>
<dc:creator><![CDATA[Haubold, H.-G.]]></dc:creator>
<dc:creator><![CDATA[Goerik, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-132-1</dc:identifier>
<dc:title><![CDATA[Resonante Röntgenkleinwinkelstreuung zur Untersuchung bestrahlungsinduzierter Ausscheidungen im Stahl 15Ch2MFA]]></dc:title>
<dc:source><![CDATA[Jahresbericht 1993 des HASYLAB]]></dc:source>
<dc:date>1993</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
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<header>
<identifier>HZDR:PUBLDB:14400-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Facsko, S.]]></dc:creator>
<dc:creator><![CDATA[Pilz, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14400-1</dc:identifier>
<dc:title><![CDATA[Self-organization of Ge nanopattern under erosion with heavy Bi monomer and cluster ions]]></dc:title>
<dc:source><![CDATA[17th International Conference on Ion Beam Modification of Material - IBMM 2010, 22.-27.08.2010, Montreal, Canada]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[The self-organisation of periodic pattern on (001)Ge by bombardment with different heavy ion species (Bi+, Bi++, Bi2+, Bi3+, Bi3++) obtained from a liquid metal ion source in a mass separating 30 kV FIB system was studied. Aspect ratios exceeding values reported so far for elemental semiconductors substantially were found after cluster irradiation. An excellent regular self-ordering of dot (40 nm in height, interdistance of ~50 nm) and ripple pattern was achieved. Despite of high ion fluence, Raman measurements prove a crystalline surface layer. This result deviates drastically from monomer irradiation, where similar to former ion irradiation of Ge a spongy amorphous surface layer is formed. For the transition from the usual behaviour to the unexpected pronounced pattern formation a threshold of the energy density deposited by the collision cascade was identified: If the deposited energy density exceeds the melting threshold, dot or ripple pattern appear. In our model we assume that the ion-impact-induced deposition of energy per volume (estimated by SRIM) must exceed the energy needed for melting. Thus, Bi segregation during re-solidification of the melted pool and the 5% volume difference between molten and solid Ge can cause the observed Bi separation and Ge patterning, respectively. A consistent, qualitative model will be discussed.]]></dc:description>
<dc:subject><![CDATA[Bi-cluster]]></dc:subject>
<dc:subject><![CDATA[germanium]]></dc:subject>
<dc:subject><![CDATA[FIB]]></dc:subject>
<dc:subject><![CDATA[nanopattern]]></dc:subject>
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<header>
<identifier>HZDR:PUBLDB:14400-2</identifier>
<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Facsko, S.]]></dc:creator>
<dc:creator><![CDATA[Pilz, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14400-2</dc:identifier>
<dc:title><![CDATA[Self-organization of Ge nanopattern under erosion with heavy Bi monomer and cluster ions]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 272(2012), 198-201]]></dc:source>
<dc:date>2012</dc:date>
<dc:description><![CDATA[The self-organisation of periodic pattern on (001)Ge by bombardment with different heavy ion species (Bi+, Bi++, Bi2+, Bi3+, Bi3++) obtained from a liquid metal ion source in a mass separating 30 kV FIB system was studied. Aspect ratios exceeding values reported so far for elemental semiconductors substantially were found after cluster irradiation. An excellent regular self-ordering of dot (40 nm in height, interdistance of ~50 nm) and ripple pattern was achieved. Despite of high ion fluence, Raman measurements prove a crystalline surface layer. This result deviates drastically from monomer irradiation, where similar to former ion irradiation of Ge a spongy amorphous surface layer is formed. For the transition from the usual behaviour to the unexpected pronounced pattern formation a threshold of the energy density deposited by the collision cascade was identified: If the deposited energy density exceeds the melting threshold, dot or ripple pattern appear. In our model we assume that the ion-impact-induced deposition of energy per volume (estimated by SRIM) must exceed the energy needed for melting. Thus, Bi segregation during re-solidification of the melted pool and the 5% volume difference between molten and solid Ge can cause the observed Bi separation and Ge patterning, respectively. A consistent, qualitative model will be discussed.]]></dc:description>
<dc:subject><![CDATA[Bi-cluster]]></dc:subject>
<dc:subject><![CDATA[germanium]]></dc:subject>
<dc:subject><![CDATA[FIB]]></dc:subject>
<dc:subject><![CDATA[nanopattern]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/j.nimb.2011.01.064]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:2856-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Bubner, M.]]></dc:creator>
<dc:creator><![CDATA[Pompe, S.]]></dc:creator>
<dc:creator><![CDATA[Schmeide, K.]]></dc:creator>
<dc:creator><![CDATA[Amayri, S.]]></dc:creator>
<dc:creator><![CDATA[Reich, T.]]></dc:creator>
<dc:creator><![CDATA[Nevedov, V.]]></dc:creator>
<dc:creator><![CDATA[Heise, K.-H.]]></dc:creator>
<dc:creator><![CDATA[Bernhard, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2856-1</dc:identifier>
<dc:title><![CDATA[Untersuchungen zur Bildung fester Metall-Huminsäure-Komplexe]]></dc:title>
<dc:source><![CDATA[Arbeitstagung der Sekt. IV der DGMT 7.-8.10.1999 Bad Elster]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[

Durch Reaktion fester, vorwiegend ungelöster natürlicher und synthetischer Huminsäuren mit wässerigen Metallsalzlösungen wurden in heterogener Phase feste Huminsäurekomplexe synthetisiert. Hierfür wurden als natürliche Huminsäuren die aufgereinigte Huminsäure der Fa. Aldrich und die aus dem "Kleinen Kranichsee" (Johanngeorgenstadt, Erzgebirge) gewonnene, aquatische Huminsäure eingesetzt. Als synthetische Huminsäure wurde eine Melanoidinfraktion mit huminsäureartigen Eigenschaften (M1) verwendet /1/. Die Komplexierungen erfolgten  mit den umweltrelevanten Metallionen UO22+, Fe3+, Ca+ und Mg2+ sowie mit natürlich vorkommenden Mineralen, in denen Uran(VI), Calcium und Magnesium als Carbonatokomplex vorliegt.
Es  wurden Humate mit unterschiedlicher Metallbeladung gewonnen, indem der pH-Wert des Reaktionsgemisches und die stöchiometrischen Verhältnisse der Reaktionspartner variiert wurden. Die Konzentration der Huminsäure wurde dabei auf die COOH-Äquivalente bezogen. Durch Konkurrenzreaktionen mit Gemischen unterschiedlicher Metallkationen und Kationenaustausch-reaktionen an definierten Metallhumaten mit "freien" Kationen konnte die unterschiedliche Affinität von Eisen gegenüber natürlichen und synthetischen Huminsäuren nachgewiesen werden.
Am Beispiel der Umsetzung freier Huminsäuren mit den gemischten Carbonatokomplexen von Uran(VI) und Calcium (Liebigit) bzw. Uran(VI) und Magnesium (Bayleyit) wurden natürliche Komplexierungsvorgänge simuliert.
An den synthetisierten Metall-Humat-Komplexen wurden Strukturuntersuchungen mit Hilfe von FTIR /2/ sowie EXAFS /3/ und ESCA /4/ durchgeführt und die thermische Stabilität durch Thermische Analyse /5/ bestimmt.

 ]]></dc:description>
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<identifier>HZDR:PUBLDB:2878-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Barz, H. W.]]></dc:creator>
<dc:creator><![CDATA[Bondorf, J. P.]]></dc:creator>
<dc:creator><![CDATA[Gaardhøje, J. J.]]></dc:creator>
<dc:creator><![CDATA[Heiselberg, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2878-1</dc:identifier>
<dc:title><![CDATA[Coulomb Effects on Particle Spectra in Relativistic Nuclear Collisions]]></dc:title>
<dc:source><![CDATA[Phys. Rev. C 57 (1998) 2536]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Coulomb effects on π<sup>±</sup> and K<sup>±</sup> spectra in relativistic nuclear collisions are investigated. At collision energies around 1 GeV the ratio of π<sup>-</sup> to π<sup>+</sup> is enhanced several times at low transverse momenta but less at ultrarelativistic energies. We describe the ratios at SIS, AGS, and SPS energies with simple analytic models as well as more elaborate numerical models incorporating the expansion dynamics. The Coulomb effect
depends on the properties of the source after the violent collision phase and provides information on source sizes, freeze-out times, and expansion velocities. Comparison with results from HBT analyses are made. Predictions for π<sup>±</sup> and K<sup>±</sup> at RHIC and LHC energies are given.]]></dc:description>
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<identifier>HZDR:PUBLDB:2484-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2484-1</dc:identifier>
<dc:title><![CDATA[Ionenstrahlsynthese von Nanoclustern für elektrooptische Anwendungen]]></dc:title>
<dc:source><![CDATA[1. Materialwissenschaftliche Tagung der WGL, Berlin, Oct. 14, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<identifier>HZDR:PUBLDB:2485-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2485-1</dc:identifier>
<dc:title><![CDATA[Positron studies of defects in ion-implanted and annealed SiC]]></dc:title>
<dc:source><![CDATA[Lawrence Livermore National Lab, Physics and Space Technology, Livermore, USA, May 22, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2486-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:title><![CDATA[The Rossendorf electrostatic accelerator]]></dc:title>
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<dc:title><![CDATA[Implantationsdotierung von Diamant]]></dc:title>
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<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
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<dc:title><![CDATA[Materialforschung mittels Positronen-Annihilationsspektroskopie]]></dc:title>
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Der Erfindung liegt die Aufgabe zugrunde, ein Verfahren  zur Herstellung  von 3-0-Methyl-6-[18F]Fluor-DOPA, (3-0-Methyl-6-[ 18F]Fluor-L-4-hydroxyphenylalanin, 3-(2-[  18F]Fluor-4-hydroxy-5-methoxy-phenyl)-2-amino-propansäure) vorzuschlagen, das eine höhere radioaktive Ausbeute bei einer kürzeren Verfahrensdauer ermöglicht.]]></dc:description>
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<dc:title><![CDATA[Verfahren zur Herstellung von 3-0-Methyl-6-[18F]Fluor-DOPA, (3-0-Methyl-6-[18F]Fluor-L-4-hydroxyphenylalanin, 3-(2-[18F]Fluor-4-hydroxy-5-methoxy-phenyl)-2-amino-propansäure)]]></dc:title>
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Der Erfindung liegt die Aufgabe zugrunde, ein Verfahren  zur Herstellung  von 3-0-Methyl-6-[18F]Fluor-DOPA, (3-0-Methyl-6-[ 18F]Fluor-L-4-hydroxyphenylalanin, 3-(2-[  18F]Fluor-4-hydroxy-5-methoxy-phenyl)-2-amino-propansäure) vorzuschlagen, das eine höhere radioaktive Ausbeute bei einer kürzeren Verfahrensdauer ermöglicht.]]></dc:description>
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<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
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<dc:title><![CDATA[Abschlußbericht 'PAS-Untersuchungen an 2024-Blechen' (Stand: 18.12.1998)]]></dc:title>
<dc:source><![CDATA[Industrie-Projekt Nr. 3448109]]></dc:source>
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<dc:creator><![CDATA[Rück, D. M.]]></dc:creator>
<dc:creator><![CDATA[Schminke, A.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, H.]]></dc:creator>
<dc:creator><![CDATA[Soltani-Farshi, M.]]></dc:creator>
<dc:creator><![CDATA[Baumann, H.]]></dc:creator>
<dc:creator><![CDATA[Fink, U.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2623-1</dc:identifier>
<dc:title><![CDATA[Tribological investigations of surface treated Ti6Al4V]]></dc:title>
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<dc:description><![CDATA[]]></dc:description>
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<dc:creator><![CDATA[Bischoff, L.]]></dc:creator>
<dc:creator><![CDATA[Teichert, J.]]></dc:creator>
<dc:creator><![CDATA[Hausmann, S.]]></dc:creator>
<dc:creator><![CDATA[Ganetsos, T.]]></dc:creator>
<dc:creator><![CDATA[Mair, G. L. R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2624-1</dc:identifier>
<dc:title><![CDATA[Temperature and energy spread investigations of alloy LMIS]]></dc:title>
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September 21 - 23, 1999, Rome, Italy 
Microelectronic Engineering 53 (2000) 613 - 616]]></dc:source>
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<dc:description><![CDATA[Emitters wetted with Ga, Au<SUB>73</SUB>Ge<SUB>27</SUB>, Au<SUB>77</SUB>Ge<SUB>14</SUB>Si<SUB>9</SUB> and Co<SUB>36</SUB>Nd<SUB>64</SUB> alloys were investigated with regard to the influence of the source temperature on the current-voltage characteristics and the energy spread of the different emitted ions. The latter was measured using a system that includes an ExB mass filter and a retarding field energy analyser. The energy spread significantly affects the available FIB spot size and depends also on the emission current, the charge state, and the mass of the ions or clusters. The influence of the source parameters, temperature and energy spread, on the beam performance in terms of spot size measurements is demonstrated with a 70 keV Ge<SUP>2+</SUP> beam using the FIB system IMSA - 100.]]></dc:description>
<dc:subject><![CDATA[alloy liquid metal ion source]]></dc:subject>
<dc:subject><![CDATA[focused ion beam]]></dc:subject>
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<dc:subject><![CDATA[energy spread]]></dc:subject>
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<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
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<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2625-1</dc:identifier>
<dc:title><![CDATA[Aufwallen und Austragen von zweiphasigen Gemischen]]></dc:title>
<dc:source><![CDATA[DECHEMA-Jahrestagung 1995, 30.05.-01.06.1995, Wiesbaden]]></dc:source>
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<dc:title><![CDATA[Vorrichtung zum Abbremsen von Ionen an einer II-Anlage zur Niederenergie-Implantation]]></dc:title>
<dc:source><![CDATA[EP 1 037 254 A2]]></dc:source>
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<dc:creator><![CDATA[Serfling, V.]]></dc:creator>
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<dc:creator><![CDATA[Fritz, S.]]></dc:creator>
<dc:creator><![CDATA[Gaff, S. J.]]></dc:creator>
<dc:creator><![CDATA[Groß, C.]]></dc:creator>
<dc:creator><![CDATA[Immé, G.]]></dc:creator>
<dc:creator><![CDATA[Iori, I.]]></dc:creator>
<dc:creator><![CDATA[Kleinevoß, U.]]></dc:creator>
<dc:creator><![CDATA[Kunde, G. J.]]></dc:creator>
<dc:creator><![CDATA[Kunze, W. D.]]></dc:creator>
<dc:creator><![CDATA[Lynen, U.]]></dc:creator>
<dc:creator><![CDATA[Maddalena, V.]]></dc:creator>
<dc:creator><![CDATA[Mahi, M.]]></dc:creator>
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<dc:creator><![CDATA[Nociforo, C.]]></dc:creator>
<dc:creator><![CDATA[Ocker, B.]]></dc:creator>
<dc:creator><![CDATA[Odeh, T.]]></dc:creator>
<dc:creator><![CDATA[Petruzzelli, F.]]></dc:creator>
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<dc:creator><![CDATA[Romano, F. P.]]></dc:creator>
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<dc:creator><![CDATA[Schüttauf, A.]]></dc:creator>
<dc:creator><![CDATA[Seidel, W.]]></dc:creator>
<dc:creator><![CDATA[Sfienti, C.]]></dc:creator>
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<dc:title><![CDATA[Temperatures of Exploding Nuclei]]></dc:title>
<dc:source><![CDATA[Phys. Rev. Lett. 80 (1998) 3928-3931]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Breakup temperatures in central collisions of <sup>197</sup> Au + <sup>197</sup>Au at bombarding energies E/A = 50 to  200 MeV were determined with two methods. Isotope temperatures, deduced from double ratios of hydrogen, helium, and lithium isotopic yields, increase monotonically with bombarding energy from 5 to 12 MeV, in qualitative agreement with a scenario of chemical freeze-out after adiabatic expansion. Excited-state temperatures, derived from yield ratios of states in <sup>4</sup>He, <sup>5,6</sup>Li, and <sup>8</sup>Be, are about 5 MeV, independent of projectile energy, and seem to reflect the internal temperature of fragments at their final separation from system.]]></dc:description>
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<dc:creator><![CDATA[Vogel, O.]]></dc:creator>
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<dc:creator><![CDATA[Gableske, J.]]></dc:creator>
<dc:creator><![CDATA[Krücken, R.]]></dc:creator>
<dc:creator><![CDATA[Nicolay, N.]]></dc:creator>
<dc:creator><![CDATA[Gelberg, A.]]></dc:creator>
<dc:creator><![CDATA[Petkov, P.]]></dc:creator>
<dc:creator><![CDATA[Gizon, A.]]></dc:creator>
<dc:creator><![CDATA[Gizon, J.]]></dc:creator>
<dc:creator><![CDATA[Bazzacco, D.]]></dc:creator>
<dc:creator><![CDATA[Rossi Alvarez, C.]]></dc:creator>
<dc:creator><![CDATA[Lunardi, S.]]></dc:creator>
<dc:creator><![CDATA[Pavan, P.]]></dc:creator>
<dc:creator><![CDATA[Napoli, D. R.]]></dc:creator>
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<dc:title><![CDATA[Lowest Four-Quasiparticle Magnetic Dipole Band in <sup>128</sup><b>Ba</b>]]></dc:title>
<dc:source><![CDATA[Phys. Rev. C 56 (1998) 1338-1343]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The four-quasiparticle magnetic dipole band in <sup>128</sup>Ba has been investigated with the <sup>96</sup>Zr(<sup>36</sup>S,4n)<sup>128</sup>Ba reaction at the GASP spectrometer of the Laboratori Nazionali di Legnaro. Linking transitions to the previously known positive parity states have been observed for the first time in this mass region and new transitions on top of the band have been found. The experimental results are compared to previously made tilted axis cranking calculations.]]></dc:description>
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<dc:source><![CDATA[Nuclear Physics A 587 (1995) pp. 802]]></dc:source>
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<dc:creator><![CDATA[Martin, H. P.]]></dc:creator>
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<dc:title><![CDATA[Silicon Carbide Derived from Silica Sol and Sugar]]></dc:title>
<dc:source><![CDATA[Journal of Materials Science Letters 14 (1995) pp. 620]]></dc:source>
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<dc:creator><![CDATA[Jäger, H.-U.]]></dc:creator>
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<dc:title><![CDATA[Simulation of high-dose ion implantation-induced transient diffusion and of electrical activation of boron in crystalline silicon]]></dc:title>
<dc:source><![CDATA[Simulation of Semiconductor Devices and Processes, vol. 5, editors: S. Selberherr, H. Stippel and E. Strasser, Springer-Verlag Wien, 1993, p. 137-140]]></dc:source>
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<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Parascandola, S.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
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<dc:identifier>https://www.hzdr.de/publications/Publ-2144-1</dc:identifier>
<dc:title><![CDATA[Slow positron implantation spectroscopy of high current ion nitrided austenitic stainless steel]]></dc:title>
<dc:source><![CDATA[Nucl. Instr. Meth. B 136-138 (1998) 768-772]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Surface modification of austenitic stainless steel by high current ion nitriding at 400°C has been studied by Slow Positron Implantation Spectroscopy (SPIS). In addition, Nuclear Reaction Analysis (NRA) has been applied to obtain information about the nitrogen depth profile. The results obtained from both methods are compared and discussed with respect to the nature of defects produced by high current ion nitriding and their influence on the formation of a surface layer, called expanded austenite.]]></dc:description>
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<dc:creator><![CDATA[Wadsworth, R.]]></dc:creator>
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<dc:identifier>https://www.hzdr.de/publications/Publ-719-1</dc:identifier>
<dc:title><![CDATA[Smooth band termination in 108Sn]]></dc:title>
<dc:source><![CDATA[Physical Review C 53 (1996) 6 pp. 2763-2769]]></dc:source>
<dc:date>1996</dc:date>
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<dc:creator><![CDATA[Schnare, H.]]></dc:creator>
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<dc:title><![CDATA[Smooth termination of intruder bands in <SUP>109</SUP><SUB>51</SUB>Sb]]></dc:title>
<dc:source><![CDATA[Physical Review C 54 (1996) 4 pp. 1598-1609]]></dc:source>
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<dc:creator><![CDATA[Moll, H.]]></dc:creator>
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<dc:creator><![CDATA[Moll, H.]]></dc:creator>
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<dc:title><![CDATA[Solubility and Speciation of (UO2)2SiO4 2H2O in Aqueous Systems]]></dc:title>
<dc:source><![CDATA[Migration '95]]></dc:source>
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<dc:creator><![CDATA[Kozulin, E. M.]]></dc:creator>
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<dc:title><![CDATA[Spontaneous fission of 244Cm studied by the two-velocities method at the FOBOS spectrometer]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-99]]></dc:source>
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<dc:creator><![CDATA[Bucenieks, I.]]></dc:creator>
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<dc:title><![CDATA[Stabilisation of thin liquid metal jets by magnetic field]]></dc:title>
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<dc:title><![CDATA[Stand der Projektvorhaben BMFT 02 S 7442 2 und Ziele des Neuantrages]]></dc:title>
<dc:source><![CDATA[5. Sitzg. Arbeitskreis "Freimessg. v. Anlageteilen u. Bauschutt aus dem Abbau kerntechn. Anlagen des Brennstoffkreislaufes" TU München, 15.3.96]]></dc:source>
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<dc:creator><![CDATA[Gebel, T.]]></dc:creator>
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<dc:creator><![CDATA[Thees, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Wittmaack, M.]]></dc:creator>
<dc:creator><![CDATA[Stegemann, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3084-1</dc:identifier>
<dc:title><![CDATA[Non-volatile memory effects of ion-beam synthesized Ge and Si nanoclusters in thin SiO2 layers: electrical characterization vs. microstructure]]></dc:title>
<dc:source><![CDATA[MRS Fall Meeting, Symposium T,
Boston, Nov. 29 - Dec. 3, 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Nanocluster memories are promising for future non-volatile memory applications. In this work thin SiO2 films were implanted with Ge+ and Si+ and annealed subsequently. Charge storage effects of the MOS capacitors have been studied through I-V and high frequency C-V measurements. Positive voltage pulses lead to a positive flatband voltage shift of the C-V curve. Detrapping by applying negative voltage pulses leads to a negative shift. The achieved programming window using 6 V / 100 ms pulses for Ge based structures is higher than that for Si (2.0 V vs. 0.2 V). However the retention times for Si based memories are longer. For dedicated process parameters microstructural investigations (RBS, XTEM) of Ge+ implanted SiO2 layers showed two bands of clusters, one near the interface SiO2/Si and one in the center of the SiO2 layer. ]]></dc:description>
<dc:subject><![CDATA[nanocluster]]></dc:subject>
<dc:subject><![CDATA[nanocrystal]]></dc:subject>
<dc:subject><![CDATA[non-volatile memory]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
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<dc:creator><![CDATA[Gebel, T.]]></dc:creator>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:creator><![CDATA[Thees, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Wittmaack, M.]]></dc:creator>
<dc:creator><![CDATA[Stegemann, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3084-2</dc:identifier>
<dc:title><![CDATA[Non-volatile memory effects of ion-beam synthesized Ge and Si nanoclusters in thin SiO2 layers: electrical characterization vs. microstructure]]></dc:title>
<dc:source><![CDATA[Mat. Res. Soc. Symp. Proc. 592, T6.10.1 (2000)]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Nanocluster memories are promising for future non-volatile memory applications. In this work thin SiO2 films were implanted with Ge+ and Si+ and annealed subsequently. Charge storage effects of the MOS capacitors have been studied through I-V and high frequency C-V measurements. Positive voltage pulses lead to a positive flatband voltage shift of the C-V curve. Detrapping by applying negative voltage pulses leads to a negative shift. The achieved programming window using 6 V / 100 ms pulses for Ge based structures is higher than that for Si (2.0 V vs. 0.2 V). However the retention times for Si based memories are longer. For dedicated process parameters microstructural investigations (RBS, XTEM) of Ge+ implanted SiO2 layers showed two bands of clusters, one near the interface SiO2/Si and one in the center of the SiO2 layer. ]]></dc:description>
<dc:subject><![CDATA[nanocluster]]></dc:subject>
<dc:subject><![CDATA[nanocrystal]]></dc:subject>
<dc:subject><![CDATA[non-volatile memory]]></dc:subject>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-3084-2</dc:relation>
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<identifier>HZDR:PUBLDB:1002-1</identifier>
<datestamp>2023-04-26</datestamp>
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<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Fröb, H.]]></dc:creator>
<dc:creator><![CDATA[Leo, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1002-1</dc:identifier>
<dc:title><![CDATA[Strong Blue and Violet Photo- and Electroluminescence from Germanium- and Silicon-Implanted Silicon Dioxide Layers]]></dc:title>
<dc:source><![CDATA[Applied Physics Letters, Vol. 71, Nr. 19, S. 2809-2811]]></dc:source>
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<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2450-1</identifier>
<datestamp>2019-03-04</datestamp>
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<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Rebohle, L.]]></dc:creator>
<dc:creator><![CDATA[Borany, J.]]></dc:creator>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:creator><![CDATA[Markwitz, A.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Tyschenko, I. E.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:creator><![CDATA[Fröb, H.]]></dc:creator>
<dc:creator><![CDATA[Leo, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2450-1</dc:identifier>
<dc:title><![CDATA[Strong blue photo-and electroluminescence from ion beam synthesized Ge-rich SiO<SUB>2</SUB>-layers]]></dc:title>
<dc:source><![CDATA[II. Int. Workshop on Light Emitting Low Dimensional Silicon Structures, Lagonissi-Attiki, Greece, June 23 - 25, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:2879-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Bilger, R.]]></dc:creator>
<dc:creator><![CDATA[Böhm, A.]]></dc:creator>
<dc:creator><![CDATA[Brand, H.]]></dc:creator>
<dc:creator><![CDATA[Brand, S.]]></dc:creator>
<dc:creator><![CDATA[Brinkmann, K.-T.]]></dc:creator>
<dc:creator><![CDATA[Clement, H.]]></dc:creator>
<dc:creator><![CDATA[Cloth, P.]]></dc:creator>
<dc:creator><![CDATA[Dahmen, M.]]></dc:creator>
<dc:creator><![CDATA[Dshemuchadse, S.]]></dc:creator>
<dc:creator><![CDATA[Eyrich, W.]]></dc:creator>
<dc:creator><![CDATA[Filges, D.]]></dc:creator>
<dc:creator><![CDATA[Freiesleben, H.]]></dc:creator>
<dc:creator><![CDATA[Fritsch, M.]]></dc:creator>
<dc:creator><![CDATA[Geyer, R.]]></dc:creator>
<dc:creator><![CDATA[Hassan, A.]]></dc:creator>
<dc:creator><![CDATA[Hauffe, J.]]></dc:creator>
<dc:creator><![CDATA[Herrmann, P.]]></dc:creator>
<dc:creator><![CDATA[Hübner, B.]]></dc:creator>
<dc:creator><![CDATA[Jahn, P.]]></dc:creator>
<dc:creator><![CDATA[Kilian, K.]]></dc:creator>
<dc:creator><![CDATA[Koch, H.]]></dc:creator>
<dc:creator><![CDATA[Kress, J.]]></dc:creator>
<dc:creator><![CDATA[Krug, J.]]></dc:creator>
<dc:creator><![CDATA[Kuhlmann, E.]]></dc:creator>
<dc:creator><![CDATA[Lange, J. S.]]></dc:creator>
<dc:creator><![CDATA[Metzger, A.]]></dc:creator>
<dc:creator><![CDATA[Michel, P.]]></dc:creator>
<dc:creator><![CDATA[Möller, K.]]></dc:creator>
<dc:creator><![CDATA[Morsch, H. P.]]></dc:creator>
<dc:creator><![CDATA[Nake, C.]]></dc:creator>
<dc:creator><![CDATA[Nann, H.]]></dc:creator>
<dc:creator><![CDATA[Naumann, B.]]></dc:creator>
<dc:creator><![CDATA[Naumann, L.]]></dc:creator>
<dc:creator><![CDATA[Ringe, P.]]></dc:creator>
<dc:creator><![CDATA[Roderburg, E.]]></dc:creator>
<dc:creator><![CDATA[Rogge, M.]]></dc:creator>
<dc:creator><![CDATA[Schamlott, A.]]></dc:creator>
<dc:creator><![CDATA[Schönmeier, P.]]></dc:creator>
<dc:creator><![CDATA[Schülke, A.]]></dc:creator>
<dc:creator><![CDATA[Steinke, M.]]></dc:creator>
<dc:creator><![CDATA[Stinzing, F.]]></dc:creator>
<dc:creator><![CDATA[Turek, P.]]></dc:creator>
<dc:creator><![CDATA[Wagner, G. J.]]></dc:creator>
<dc:creator><![CDATA[Wirth, S.]]></dc:creator>
<dc:creator><![CDATA[Zielinski, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2879-1</dc:identifier>
<dc:title><![CDATA[Proton-Proton Bremsstrahlung at 797 MeV/c]]></dc:title>
<dc:source><![CDATA[Phys. Lett. B. 429 (1998) 195-200]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[At COSY pp-bremsstrahlung was measured at a beam momentum of 797 MeV/c using an external proton beam. Data were taken with a wide angle spectrometer covering a solid angle of  approximately 1 sr. The complete data set is presented in a series of c.m. angular distributions as well as a single Dalitz plot. The absence of final state interaction effects is understood as being due to a general insensitivity of the  pp γ reaction to the spin-singlet component of the NN  interaction. Coplanar angular distributions (in the laboratory system) are well reproduced by recent model calculations; also  good agreement is found with the original TRIUMF data  [K. Michaelian et al., Phys. Rev. D 41 (1990) 286] when omitting the rescaling factor of 2/3.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2879-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:3203-1</identifier>
<datestamp>2025-12-09</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Turos, A.]]></dc:creator>
<dc:creator><![CDATA[Gawlik, G.]]></dc:creator>
<dc:creator><![CDATA[Jagielski, J.]]></dc:creator>
<dc:creator><![CDATA[Stonert, A.]]></dc:creator>
<dc:creator><![CDATA[Matz, W.]]></dc:creator>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3203-1</dc:identifier>
<dc:title><![CDATA[Ion beam mixing of the ZrO2/Fe system]]></dc:title>
<dc:source><![CDATA[Nucl. Instr. and Meth. B 148 (1999) 778-782]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[ZrO2 layers stabilized with 9mol% Y2O3 of 35-100 nmthickness were deposited by sputtering on 200 nm thick Fe layers on Si/SiO2. Ion beam mixing induced by 300 keV Kr ions and 1.5 MeV Br ions bombardement was studied at temperatures ranging from 100 to 300 K. Samples were analysed by means of RBS, GXRD, and SEM techniques. RBS analysis revealed important atomic transport across the ZrO2/Fe interface. The amount of intermixed atoms increases with increasing ion dose. Ion beam mixing was observed at low temperaturesw. Upon 300 keV Kr-ion bombardment the tetragonal structure of as-deposited ZrO2(Y2O3) layers was transformed into the cubic one. High energy ion bombardment produces only transformations of the crystalline structure without any visible atomic transport and the formation of the rare FeO-wuestite phase. Kr blistering was observed from samples implanted with 300 keV Kr ions to fluences exceeding 1e16 at/cm2 at 100 K and 5e16 at/cm2 at RT.]]></dc:description>
<dc:subject><![CDATA[ion beam mixing]]></dc:subject>
<dc:subject><![CDATA[ceramic-metalsystem]]></dc:subject>
<dc:subject><![CDATA[RBS]]></dc:subject>
<dc:subject><![CDATA[GXRD]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0168-583X(98)00831-3]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-3203-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2489-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grambole, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2489-1</dc:identifier>
<dc:title><![CDATA[Möglichkeiten der Oberflächenanalytik mit Ionenstrahlverfahren im Forschungszentrum Rossendorf]]></dc:title>
<dc:source><![CDATA[TU Dresden, Inst. f. Werkstoffwissenschaften, Aug. 13, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2489-1</dc:relation>
<dc:audience>Researchers</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2490-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2490-1</dc:identifier>
<dc:title><![CDATA[Grundlagen der Ionenstrahlanalytik]]></dc:title>
<dc:source><![CDATA[TU Chemnitz, Graduiertenkolleg, Jan./Feb., 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2490-1</dc:relation>
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<record>
<header>
<identifier>HZDR:PUBLDB:2491-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Grötzschel, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2491-1</dc:identifier>
<dc:title><![CDATA[Recent developments of in situ ion beam analysis at Rossendorf]]></dc:title>
<dc:source><![CDATA[Faure, South Africa, Nov. 19, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2491-1</dc:relation>
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<header>
<identifier>HZDR:PUBLDB:2492-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<header>
<identifier>HZDR:PUBLDB:2882-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Brinkmann, K.-T.]]></dc:creator>
<dc:creator><![CDATA[Bilger, R.]]></dc:creator>
<dc:creator><![CDATA[Böhm, A.]]></dc:creator>
<dc:creator><![CDATA[Clement, H.]]></dc:creator>
<dc:creator><![CDATA[Dennert, H.]]></dc:creator>
<dc:creator><![CDATA[Dshemuchadse, S.]]></dc:creator>
<dc:creator><![CDATA[Dutz, H.]]></dc:creator>
<dc:creator><![CDATA[Eyrich, W.]]></dc:creator>
<dc:creator><![CDATA[Fanara, C.]]></dc:creator>
<dc:creator><![CDATA[Filges, D.]]></dc:creator>
<dc:creator><![CDATA[Filippi, A.]]></dc:creator>
<dc:creator><![CDATA[Freiesleben, H.]]></dc:creator>
<dc:creator><![CDATA[Fritsch, M.]]></dc:creator>
<dc:creator><![CDATA[Geyer, R.]]></dc:creator>
<dc:creator><![CDATA[Hassan, A.]]></dc:creator>
<dc:creator><![CDATA[Hauffe, J.]]></dc:creator>
<dc:creator><![CDATA[Herrmann, P.]]></dc:creator>
<dc:creator><![CDATA[Hesselbarth, D.]]></dc:creator>
<dc:creator><![CDATA[Hübner, B.]]></dc:creator>
<dc:creator><![CDATA[Jahn, P.]]></dc:creator>
<dc:creator><![CDATA[Kilian, K.]]></dc:creator>
<dc:creator><![CDATA[Koch, H.]]></dc:creator>
<dc:creator><![CDATA[Kress, J.]]></dc:creator>
<dc:creator><![CDATA[Krug, J.]]></dc:creator>
<dc:creator><![CDATA[Kuhlmann, E.]]></dc:creator>
<dc:creator><![CDATA[Marcello, S.]]></dc:creator>
<dc:creator><![CDATA[Marwinski, S.]]></dc:creator>
<dc:creator><![CDATA[Metzger, A.]]></dc:creator>
<dc:creator><![CDATA[Meyer, W.]]></dc:creator>
<dc:creator><![CDATA[Michel, P.]]></dc:creator>
<dc:creator><![CDATA[Möller, K.]]></dc:creator>
<dc:creator><![CDATA[Morsch, H. P.]]></dc:creator>
<dc:creator><![CDATA[Nann, H.]]></dc:creator>
<dc:creator><![CDATA[Naumann, B.]]></dc:creator>
<dc:creator><![CDATA[Naumann, L.]]></dc:creator>
<dc:creator><![CDATA[Raimondo, A.]]></dc:creator>
<dc:creator><![CDATA[Roderburg, E.]]></dc:creator>
<dc:creator><![CDATA[Rogge, M.]]></dc:creator>
<dc:creator><![CDATA[Schamlott, A.]]></dc:creator>
<dc:creator><![CDATA[Schönmeier, P.]]></dc:creator>
<dc:creator><![CDATA[Schröder, W.]]></dc:creator>
<dc:creator><![CDATA[Schulte-Wissermann, M.]]></dc:creator>
<dc:creator><![CDATA[Steinke, M.]]></dc:creator>
<dc:creator><![CDATA[Stinzing, F.]]></dc:creator>
<dc:creator><![CDATA[Sun, G. Y.]]></dc:creator>
<dc:creator><![CDATA[Wächter, J.]]></dc:creator>
<dc:creator><![CDATA[Wagner, G. J.]]></dc:creator>
<dc:creator><![CDATA[Wagner, M.]]></dc:creator>
<dc:creator><![CDATA[Wirth, S.]]></dc:creator>
<dc:creator><![CDATA[Zielinski, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2882-1</dc:identifier>
<dc:title><![CDATA[Three-Particle Final States Measured at the Pion threshold with COSY-TOF]]></dc:title>
<dc:source><![CDATA[Acta Phys. Polon. B 29 (1998) 2993]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The production of pions in pp collisions at beam energies of   ≤  300 MeV has been studied with the COSY-TOF spectrometer, which was recently extended to flight paths of <font face=symbol> ~ </font>3 m for charged particles through the addition of a barrel section. Together with the bremsstrahlung channel, which was investigated in an earlier
experiment, pion production exhausts the inelastic pp cross section at these energies. TOF allows the simultaneous study of
 all channels, the measurement of pnπ<sup>+</sup> being facilitated by the neutron detector COSYnus. In this contribution, preliminary results on the pionic three-body final states are discussed.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:language>eng</dc:language>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2629-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2629-1</dc:identifier>
<dc:title><![CDATA[Erfassung schneller Verdampfungs- und Kondensationsprozesse mit dem Gittersensor, Seminar Druckstöße]]></dc:title>
<dc:source><![CDATA[Dampfschläge und Pulsationen in Rohrleitungen, Organisator: Haus der Technik e.V., Oberhausen, 20.-21.10.1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Speziell für die Druckstoßuntersuchungen an der Druckstoß-Versuchsanlage von Fraunhofer UMSICHT in Oberhausen wurde vom Forschungszentrum Rossendorf ein Gittersensor zur schnellen Visualisierung der Verdampfungs- und Kondensationsvorgänge hinter einer schnellschließenden Armatur entwickelt. Er basiert auf der Messung der momentanen örtlichen elektrischen Leitfähigkeit des Zweiphasengemischs. Die Zeitauflösung des Geräts beträgt 1024 Messungen in der Sekunde. Der Sensor besteht aus zwei dicht hintereinander angeordneten Elektrodengittern mit jeweils 16 Elektroden. Die Messung erfolgt an den Kreuzungspunkten der Elektroden, d.h. an 16 x 16 Meßpunkten, die gleichmäßig über die Querschnittsfläche des Strömungskanals verteilt sind. Der Sensor ist in zwei Ausführungen verfügbar: (1) als Drahtgittersensor für Laboranwendungen und (2) als "schwerer" Sensor mit verstärkten Elektrodenstäbchen für höhere strömungsmechanische Belastungen. Letzterer wurde bei einer Vielzahl von Experimenten in Oberhausen erfolgreich eingesetzt. Eines der Ergebnisse ist ein neuartiges Verfahren zur Verhinderung des Kaviattionsschlages hinter einer Schnellschlußklappe. Durch Anordnung einer Hilfsarmatur hinter der eigentlichen Absperrarmatur ist eine Schnellabsperrung der Rohrleitung ohne Kavitationsschläge möglich. Der Einsatz von Rückschlagklappen stellt hierbei eine kostengünstige Variante dar. Um sekundäre Kavitationsschläge zu vermeiden, muß der Abstand zwischen Absperr- und Hilfsarmatur ausreichend bemessen sein. Die Hilfsarmatur muß einen möglichst geringen Druckverlust aufweisen. Durch geeignete technische oder organisatorische Maßnahmen muß sichergestellt werden, daß die Absperrarmatur nicht oder nur hinreichend langsam geöffnet werden kann, solange zwischen Absperr- und Hilfsarmatur eine Kavitationsblase eingeschlossen ist.]]></dc:description>
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<record>
<header>
<identifier>HZDR:PUBLDB:14485-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Wolf, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14485-1</dc:identifier>
<dc:title><![CDATA[3D-observation of heterogeneous transport and comparison to Lattice-Boltzmann modelling]]></dc:title>
<dc:source><![CDATA[FZD Doktorandenseminar, 22.-24.09.2010, Krögis (Meissen), Deutschland]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[This thesis is located at the Institute of Radiochemistry, FZD Research Site Leipzig for Interdisciplinary Isotope Research, Reactive Transport Division (FWRT). The main focus of this division is the investigation of transport processes in geosystems by means of radiotracer applications. The main topic of the thesis is the visualization of transport processes in geologic material by means of the in-house development of the GeoPET-method. This work is conducted as part of the scientific joint venture: Dynamik abgesoffener oder gefluteter Salzbergwerke und ihres Deckgebirgsstockwerks (Dynamic of drowned or flooded salt mines and their overburden), coordinated by the Bundesanstalt für Geowissenschaften und Rohstoffe (BGR).

Since the late 19. century drowned salt mines cause severe mining damages in the city of Stassfurt (Saxony-Anhalt). Sink hole depressions and subsidence of the surface below the groundwater table destroyed large parts of the down town. The general causation was lack of experience with salt mines and mining in gypsum karst in the 19. century.  The causation in detail why and how exactly salt rock has washed out is more complicated to identify, as streaming mechanisms at the small scale level are partly still unclear; the general fluid dynamics at small scales is partly unknown.

To reveal these processes and mechanisms the behaviour of salt brines at the millimetre scale in drilling cores of the different geological units of the salt rock and its surrounding is examined by three-dimensional visualization of the distribution of radioactive labelled water measured with PET. Mechanisms at millimetre scale control mechanisms at the kilometre scale and are of utmost importance for the principal understanding of fluid dynamics. In the laboratory you can have a look into the rock. In the field this is not possible this way.

Combining PET data with high resolution CT-scans of the samples (conducted by the cooperation partners JGU Mainz and BAM Berlin) allows an alignment of processes of the fluid flow and its associated hydraulic pathway structures. This matching is important for understanding and for generalized conclusion about ongoing processes and is a necessary preparatory work for computer modelling.

Lattice-Boltzmann-simulations of velocity fields and streaming patterns based on CT-data are compared with PET-data derived from the same samples. This comparison of the flow patterns is done by means of geostatistic methods that allows scale independant spatial correlation of the patterns and therefore provide scale indpendant parameters like correlation lengths that are a necessity for upscaling.

Short term objective is the improvement and validation of parameters and fluid flow concepts derived from small scale simulations. Long term objective is the improvement of upscaling of parameters and concepts to the field scale and a better understanding and prediction of mining damages and groundwater behaviour.]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2912-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Höhne, T.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:creator><![CDATA[Weiss, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2912-1</dc:identifier>
<dc:title><![CDATA[Experimental and numerical investigation of the coolant mixing during fast deboration transients]]></dc:title>
<dc:source><![CDATA[9th  AER symposium on VVER reactor physics and reactor safety, October 4-8 1999,
Hotel Repiska, Dämenovska Dolina,
Slovakia, Proceedings pp. 327]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[For the analysis of boron dilution transients and main steam line break scenarios the modeling of the coolant mixing inside the reactor vessel is important, because the reactivity insertion strongly depends on boron acid concentration or the coolant temperature distribution. 

Calculations for steady state flow conditions for the VVER-440 were performed with a CFD code (CFX-4). For this calculation the RPV from the cold legs inlet through the downcomer, the lower plenum and the lower core support plate was nodalized in detail. The comparison with experimental data and an analytical mixing model which is implemented in the neutron-kinetic code DYN3D showed a good agreement for near-nominal condi-tions (all MCPs are running). The comparison between the CFD-results and the analytical model revealed differences for MSLB conditions [1].

After investigating coolant mixing under steady-state nominal flow conditions, first experiments at the Rossendorf Mixing Test Facility ROCOM were performed simulating the start-up of the first main coolant pump. The reference reactor for the geo-metrically 1:5 scaled Plexiglas model is the German Konvoi type PWR. This transient is impor-tant in the case of the existence of plugs of lower borated water in one of the loops. The travelling of plugs of different size from the inlet nozzle of the started loop to the core inlet and the resulting parameter distribution at the core inlet were investigated. CFD calculations for these experiments show the same qualitative parameter distribution picture with typical maxima, which are located at the opposite of the reactor from the started loop, as it was observed in the experiments. After demonstrating the capability of the CFD code to simulate these complicated flow transients, calculations were performed for the start-up of the first pump in a VVER-440 type reactor. However, no data from transient experiments are available at the moment for this reactor type. Therefore the calculations are a first step of understanding the coolant mixing in the RPV of a VVER-440 type reactor under transient conditions.

The results of the calculation show a very complex flow in the downcomer. The injection is distributed into two main jets, the so called butterfly distribution. In addition several secondary flows are seen in various parts of the downcomer. Especially strong vortices occur in the areas below the non operating loop nozzles and also below the injection loop. The results show that a high downcomer of VVER-440 and the existence of the lower control rod chamber support coolant mixing.
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:2912-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Höhne, T.]]></dc:creator>
<dc:creator><![CDATA[Rohde, U.]]></dc:creator>
<dc:creator><![CDATA[Weiss, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2912-7</dc:identifier>
<dc:title><![CDATA[Experimental and numerical investigation of the coolant mixing during fast deboration transients]]></dc:title>
<dc:source><![CDATA[9th  AER symposium on VVER reactor physics and reactor safety, October 4-8 1999,
Hotel Repiska, Dämenovska Dolina,
Slovakia, Proceedings pp. 327]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[For the analysis of boron dilution transients and main steam line break scenarios the modeling of the coolant mixing inside the reactor vessel is important, because the reactivity insertion strongly depends on boron acid concentration or the coolant temperature distribution. 

Calculations for steady state flow conditions for the VVER-440 were performed with a CFD code (CFX-4). For this calculation the RPV from the cold legs inlet through the downcomer, the lower plenum and the lower core support plate was nodalized in detail. The comparison with experimental data and an analytical mixing model which is implemented in the neutron-kinetic code DYN3D showed a good agreement for near-nominal condi-tions (all MCPs are running). The comparison between the CFD-results and the analytical model revealed differences for MSLB conditions [1].

After investigating coolant mixing under steady-state nominal flow conditions, first experiments at the Rossendorf Mixing Test Facility ROCOM were performed simulating the start-up of the first main coolant pump. The reference reactor for the geo-metrically 1:5 scaled Plexiglas model is the German Konvoi type PWR. This transient is impor-tant in the case of the existence of plugs of lower borated water in one of the loops. The travelling of plugs of different size from the inlet nozzle of the started loop to the core inlet and the resulting parameter distribution at the core inlet were investigated. CFD calculations for these experiments show the same qualitative parameter distribution picture with typical maxima, which are located at the opposite of the reactor from the started loop, as it was observed in the experiments. After demonstrating the capability of the CFD code to simulate these complicated flow transients, calculations were performed for the start-up of the first pump in a VVER-440 type reactor. However, no data from transient experiments are available at the moment for this reactor type. Therefore the calculations are a first step of understanding the coolant mixing in the RPV of a VVER-440 type reactor under transient conditions.

The results of the calculation show a very complex flow in the downcomer. The injection is distributed into two main jets, the so called butterfly distribution. In addition several secondary flows are seen in various parts of the downcomer. Especially strong vortices occur in the areas below the non operating loop nozzles and also below the injection loop. The results show that a high downcomer of VVER-440 and the existence of the lower control rod chamber support coolant mixing.
]]></dc:description>
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<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<record>
<header>
<identifier>HZDR:PUBLDB:2910-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Oswald, S.]]></dc:creator>
<dc:creator><![CDATA[Schmidt, B.]]></dc:creator>
<dc:creator><![CDATA[Heinig, K.-H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2910-1</dc:identifier>
<dc:title><![CDATA[XPS investigation with factor analysis for the study of Ge clustering in SiO2]]></dc:title>
<dc:source><![CDATA[Surface and Interface Analysis 29 (2000) 249-254]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The change of the depth profile and chemical bond character of Ge in Ge+ ion implanted SiO2 layers during annealing in O2 atmophere has been studied by x-ray photoelectron spectroscopy (XPS). The Ge depth profiles in as-implanted and annealed samples as measured by XPS are in agreement with profiles measured by Rutherford backscattering spectroscopy (RBS). At interfaces XPS gives more information about the Ge depth distribution than RBS. Thus, other than RBS, XPS could proof that the fraction of implanted Ge, with moves during annealing to the SiO2/Si interface region, resides on the Si side of this interface. Additionally, the high and low contrast nanoclusters in Ge implanted samples, which have been found recently in cross-section transmission electron microscopy (XTEM) images, could be identified by XPS, in combination with data analysis by factor analysis, to consist mainly of elemental Ge and GeO2, respectively.]]></dc:description>
<dc:subject><![CDATA[XPS]]></dc:subject>
<dc:subject><![CDATA[depth profiling]]></dc:subject>
<dc:subject><![CDATA[factor analysis]]></dc:subject>
<dc:subject><![CDATA[Ge]]></dc:subject>
<dc:subject><![CDATA[cluster formation]]></dc:subject>
<dc:subject><![CDATA[nanocrystals]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2972-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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<dc:creator><![CDATA[Stefani, F.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Priede, J.]]></dc:creator>
<dc:creator><![CDATA[Thess, A.]]></dc:creator>
<dc:creator><![CDATA[Cramer, A.]]></dc:creator>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
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<dc:creator><![CDATA[Eberth, J.]]></dc:creator>
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<dc:creator><![CDATA[Huxel, N.]]></dc:creator>
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<dc:creator><![CDATA[Prade, H.]]></dc:creator>
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<dc:creator><![CDATA[Wiedenhöver, I.]]></dc:creator>
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<dc:creator><![CDATA[Zilges, A.]]></dc:creator>
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<dc:title><![CDATA[Photon Scattering of <SUP>52</SUP>Cr: Two-Phonon E1 Strength at the N = 28 Shell Closure?*]]></dc:title>
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<dc:creator><![CDATA[Förster, E.]]></dc:creator>
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<dc:title><![CDATA[Verfahren zur elektrochemischen Mineralisierung von insbesondere C-14-markierten organischen Abfallstoffen]]></dc:title>
<dc:source><![CDATA[DE 196 46 049 A 1]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Die Erfindung betrifft ein Verfahren zur elektrochemischen Mineralisierung von schwer entsorgbaren, insbesondere C-14-markierten organischen Abfallstoffen, wie Sie sowohl in der Industrie als auch Laboratorien anfallen.
Mit der Erfindung wird ein allgemein anwendbares Verfahren zur vollständigen Mineralisierung von organischen Kohlenstoff-Verbindungen, insbesondere solchen, die mit dem radioaktiven Isotop Kohlenstoff-14 markiert sind, vorgestellt, das gleichzeitig die Entstehung von weiteren Problemabfällen vermeidet.
Das erfindungsgemäße Verfahren zur Mineralisierung von insbesondere C-14-markierten organischen Abfallstoffen ist dadurch gekennzeichnet, daß der Abfallstoff in Gegenwart von katalytische Mengen Silbersalz enthaltender Chromschwefelsäure im Anodenraum einer Elektrolysezelle vollständig oxidiert wird.
Es ist dabei auch möglich, die zu oxidierende Substanz samt des Sie enthaltenden Glasgefäßes oder mehrerer Gefäße in einem "Korb" in den Anodenraum einzubringen.
Bei der Mineralisierung C-14-haltiger Abfälle fällt das C-14 mit Ausbeuten größer 90% als 14CO2 an, welches beispielsweise in einer wäßriges Alkali enthaltenden Gaswaschflasche absorbiert, durch Zusatz von Bariumchlorid als Ba14CO3 ausgefällt und in dieser Form sicher entsorgt werden kann.]]></dc:description>
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<dc:creator><![CDATA[Kampf, G.]]></dc:creator>
<dc:creator><![CDATA[Knop, G.]]></dc:creator>
<dc:creator><![CDATA[Wenzel, U.]]></dc:creator>
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<dc:title><![CDATA[Studies of radiometal uptake by cultured normal and tumor cells]]></dc:title>
<dc:source><![CDATA[European Journal of Nuclear Medicine 21 (1994) pp. 874]]></dc:source>
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<dc:creator><![CDATA[Wang, X.]]></dc:creator>
<dc:creator><![CDATA[Charlamov, V.]]></dc:creator>
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<dc:creator><![CDATA[Posselt, M.]]></dc:creator>
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<dc:creator><![CDATA[Möller, W.]]></dc:creator>
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<dc:title><![CDATA[Study of Ion Beam Assisted Deposition of Al/AlN Multilayers by Comparison of Computer Simulation and Experiment]]></dc:title>
<dc:source><![CDATA[Journal of Physics D: Applied Physics 31 (1998) 2241-2244]]></dc:source>
<dc:date>1998</dc:date>
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<dc:title><![CDATA[Study of the different stages of damage induced by 200 keV Ge+ ion implantation in 6H-SiC]]></dc:title>
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<dc:date>1995</dc:date>
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<dc:creator><![CDATA[Schaffrath, A.]]></dc:creator>
<dc:creator><![CDATA[Krüssenberg, A.-K.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Hicken, E. F.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-4047-1</dc:identifier>
<dc:title><![CDATA[TOPFLOW - eine neue Mehrzweckthermohydraulikversuchsanlage zur Untersuchung transienter Zweiphasenströmungen]]></dc:title>
<dc:source><![CDATA[Seminar des Lehrstuhls für Nukleare und Neue Energiesysteme, Ruhr-Universität Bochum, 03.07.2001]]></dc:source>
<dc:date>2001</dc:date>
<dc:description><![CDATA[In dem Vortrag wird der Stand der Arbeiten zur Errichtung der Versuchsanlage TOPFLOW (Transient Two Phase Flow Test Facility) präsentiert. Hierbei werden u.a. das Design der Anlage, die geplanten Experimente, die Dokumentation, das Internetprotal sowie der Zeitplan im Detail vorgestellt.   ]]></dc:description>
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<dc:creator><![CDATA[Klein, C.]]></dc:creator>
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<dc:title><![CDATA[Charge State Distributions of Heavy Ions after Scattering at Surface atoms]]></dc:title>
<dc:source><![CDATA[Proceedings of the 15th International Conference on Ion Beam Analysis, Cairns, Australia, 15-20 July 2001, published as a special volume of Nuclear Instruments and Methods in Physics Research B]]></dc:source>
<dc:date>2001</dc:date>
<dc:description><![CDATA[The charge-state distributions of Li, C, and F ions after a single collision with Au atoms deposited at a sub-monolayer coverage on Si were measured at energies below 500 keV/amu and compared to the equilibrium charge-state distributions.  The influence of the surface on the charge state of the outgoing ions is demonstrated for Li ions at 3 MeV. It is found that the charge state distribution does not generally reach equilibrium after a single collision.]]></dc:description>
<dc:subject><![CDATA[Ion-atom collisions]]></dc:subject>
<dc:subject><![CDATA[Charge exchange]]></dc:subject>
<dc:subject><![CDATA[Charge State Distribution]]></dc:subject>
<dc:subject><![CDATA[High resolution RBS]]></dc:subject>
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<dc:title><![CDATA[Charge State Distributions of Heavy Ions after Scattering at Surface atoms]]></dc:title>
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<dc:description><![CDATA[The charge-state distributions of Li, C, and F ions after a single collision with Au atoms deposited at a sub-monolayer coverage on Si were measured at energies below 500 keV/amu and compared to the equilibrium charge-state distributions.  The influence of the surface on the charge state of the outgoing ions is demonstrated for Li ions at 3 MeV. It is found that the charge state distribution does not generally reach equilibrium after a single collision.]]></dc:description>
<dc:subject><![CDATA[Ion-atom collisions]]></dc:subject>
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<dc:subject><![CDATA[High resolution RBS]]></dc:subject>
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<dc:creator><![CDATA[Dönau, F.]]></dc:creator>
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<dc:title><![CDATA[Institute of Nuclear and Hadron Physics; Annual Report 2000]]></dc:title>
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<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Stoemenos, J.]]></dc:creator>
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<dc:creator><![CDATA[Voelskow, M.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-4050-1</dc:identifier>
<dc:title><![CDATA[The beneficial role of flash lamp annealing on the epitaxial growth of the 3C-SiC on Si]]></dc:title>
<dc:source><![CDATA[Applied Surface Science 184 (2001) 377-382]]></dc:source>
<dc:date>2001</dc:date>
<dc:description><![CDATA[For the realization of good quality 3C-SiC films epitaxially grown on Si the perfection of the film during the early stage of growth is substantial. In this paper the beneficial role of Flash Lamp Annealing (FLA) for the elimination of the defects in the SiC film and the strain reduction at the SiC/Si interface is discussed. FLA is a highly transient process, having a flash duration of a few milliseconds. When the energy density is sufficient high, it melts the silicon at the SiC/Si interface increasing the temperature there well above the melting point of the silicon. The melted Si dissolves the 3C-SiC near the interface. Additionally, the uppermost part of the 3C-SiC film is annealed due to the heat dissipation during the flash duration and the solidification of the molten region. During the solidification of the C-rich Si melt SiC grows by liquid phase epitaxy  at the annealed uppermost 3C-SiC film which act as a seed. This process results in a substantial improvement of the SiC film, eliminating also the cavities and the stress at the interface.]]></dc:description>
<dc:subject><![CDATA[3C-SiC interface]]></dc:subject>
<dc:subject><![CDATA[Flash lamp annealing]]></dc:subject>
<dc:subject><![CDATA[TEM]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2171-1</identifier>
<datestamp>2025-11-26</datestamp>
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</header>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Mieskes, H. D.]]></dc:creator>
<dc:creator><![CDATA[Assmann, W.]]></dc:creator>
<dc:creator><![CDATA[Brodale, M.]]></dc:creator>
<dc:creator><![CDATA[Dobler, M.]]></dc:creator>
<dc:creator><![CDATA[Glückler, H.]]></dc:creator>
<dc:creator><![CDATA[Hartung, P.]]></dc:creator>
<dc:creator><![CDATA[Stenzel, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2171-1</dc:identifier>
<dc:title><![CDATA[Measuring sputtering yields of high energy heavy ions on metals]]></dc:title>
<dc:source><![CDATA[Nucl. Instr. Meth. B 146 (1998) 162]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[For measuring sputtering yields with MeV heavy ions only low current densities can be used in order to avoid excessive target heating. Consequently self-cleaning of the target surface during the irradiation cannot be achieved and a contamination free surface has to be maintained by means of UHV conditions. A UHV-setup including a differential pumping system has been designed and operated at a vacuum of 10<sup>-10</sup> mbar during experiments. Sputtered particles were collected on Si catchers and subsequently measured by two different surface analysis methods: Total Reflection X-Ray Fluorescence (TXRF), and Heavy Ion Rutherford Backscattering Spectrometry (HI-RBS). In-situ surface cleaning by 8 keV Xe ions as well as online monitoring by ERDA were found to be essential. With sufficient precautions on the surface conditions reproducible sputtering yields were obtained. First  measurements for 230 MeV Au ions on Au, Zr, and Ti targets are presented.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0168-583X(98)00444-3]]></dc:relation>
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<header>
<identifier>HZDR:PUBLDB:3279-1</identifier>
<datestamp>2025-12-11</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Watanabe, H.]]></dc:creator>
<dc:creator><![CDATA[Takahashi, K.]]></dc:creator>
<dc:creator><![CDATA[Iwaki, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3279-1</dc:identifier>
<dc:title><![CDATA[Raman spectroscopic study Ag-, W- and Pd-Ions implanted polyimide films]]></dc:title>
<dc:source><![CDATA[Mat. Res. Soc. Symp. Proc. Vol. 354, p. 369-373, 1995 Materials Research Society]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/bookPart</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2527-1</identifier>
<datestamp>2025-12-05</datestamp>
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<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Shin, Y.]]></dc:creator>
<dc:creator><![CDATA[Ahner, W.]]></dc:creator>
<dc:creator><![CDATA[Barth, R.]]></dc:creator>
<dc:creator><![CDATA[Beckerle, P.]]></dc:creator>
<dc:creator><![CDATA[Brill, D.]]></dc:creator>
<dc:creator><![CDATA[Cieslak, M.]]></dc:creator>
<dc:creator><![CDATA[Debowski, M.]]></dc:creator>
<dc:creator><![CDATA[Grosse, E.]]></dc:creator>
<dc:creator><![CDATA[Koczon, P.]]></dc:creator>
<dc:creator><![CDATA[Kohlmeyer, B.]]></dc:creator>
<dc:creator><![CDATA[Mang, M.]]></dc:creator>
<dc:creator><![CDATA[Miskowiec, D.]]></dc:creator>
<dc:creator><![CDATA[Müntz, C.]]></dc:creator>
<dc:creator><![CDATA[Oeschler, H.]]></dc:creator>
<dc:creator><![CDATA[Pühlhofer, F.]]></dc:creator>
<dc:creator><![CDATA[Schwab, E.]]></dc:creator>
<dc:creator><![CDATA[Schicker, R.]]></dc:creator>
<dc:creator><![CDATA[Senger, P.]]></dc:creator>
<dc:creator><![CDATA[Speer, J.]]></dc:creator>
<dc:creator><![CDATA[Ströbele, H.]]></dc:creator>
<dc:creator><![CDATA[Sturm, C.]]></dc:creator>
<dc:creator><![CDATA[Völkel, K.]]></dc:creator>
<dc:creator><![CDATA[Wagner, A.]]></dc:creator>
<dc:creator><![CDATA[Walus, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2527-1</dc:identifier>
<dc:title><![CDATA[Enhanced Out-of-Plane Emission of K<SUP>+</SUP> Mesons Observed in Au + Au Collisions at 1 A GeV]]></dc:title>
<dc:source><![CDATA[Physical Review Letters, Volume 81, Number 8, 24 August 1998, 1576-1579]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1103/PhysRevLett.81.1576]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2527-1</dc:relation>
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<header>
<identifier>HZDR:PUBLDB:2530-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Hensel, F.]]></dc:creator>
<dc:creator><![CDATA[Schütz, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2530-1</dc:identifier>
<dc:title><![CDATA[Verfahren zur Minimierung des Einflusses von Resonanzfluktuationen auf das Meßsignal bei Ultraschall-Durchschallungsuntersuchungen]]></dc:title>
<dc:source><![CDATA[DE 4333645 A1]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Das Patent beschreibt ein Verfahren zur Minimierung des Einflusses von Resonanzfluktuationen des Meßmediums bei Ultraschall-Durchschallungsuntersuchungen an in Rohrleitungen geführten Zwei- und Mehrphasenströmungen durch eine schnelle Variation der Arbeitsfrequenz des Senders der Meßeinrichtung.]]></dc:description>
<dc:subject><![CDATA[ultrasonic transmission measurement]]></dc:subject>
<dc:subject><![CDATA[wobbling]]></dc:subject>
<dc:subject><![CDATA[Wobbeln]]></dc:subject>
<dc:subject><![CDATA[Ultraschall-Transmissionsmessung]]></dc:subject>
<dc:type>info:eu-repo/semantics/patent</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:patent</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2530-1</dc:relation>
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<dc:format><![CDATA[application/pdf]]></dc:format>
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<header>
<identifier>HZDR:PUBLDB:2530-2</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Prasser, H.-M.]]></dc:creator>
<dc:creator><![CDATA[Hensel, F.]]></dc:creator>
<dc:creator><![CDATA[Schütz, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2530-2</dc:identifier>
<dc:title><![CDATA[Verfahren zur Minimierung des Einflusses von Resonanzfluktuationen auf das Meßsignal bei Ultraschall-Durchschallungsuntersuchungen]]></dc:title>
<dc:source><![CDATA[EP 0721572 B1]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Das Patent beschreibt ein Verfahren zur Minimierung des Einflusses von Resonanzfluktuationen des Meßmediums bei Ultraschall-Durchschallungsuntersuchungen an in Rohrleitungen geführten Zwei- und Mehrphasenströmungen durch eine schnelle Variation der Arbeitsfrequenz des Senders der Meßeinrichtung.]]></dc:description>
<dc:subject><![CDATA[ultrasonic transmission measurement]]></dc:subject>
<dc:subject><![CDATA[wobbling]]></dc:subject>
<dc:subject><![CDATA[Wobbeln]]></dc:subject>
<dc:subject><![CDATA[Ultraschall-Transmissionsmessung]]></dc:subject>
<dc:type>info:eu-repo/semantics/patent</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2531-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Wirth, H.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2531-1</dc:identifier>
<dc:title><![CDATA[Effekte bei der Implantationsdotierung von Bor und Aluminium in 6H-SiC]]></dc:title>
<dc:source><![CDATA[Daimler-Benz-AG, FZ Frankfurt/M., Oct. 29, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:lecture</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2532-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Yankov, R. A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2532-1</dc:identifier>
<dc:title><![CDATA[Proximity gettering of transition-metal impurities in separation-by-implanted-oxygen (SIMOX) structures using buried carbon- and helium-implanted layers]]></dc:title>
<dc:source><![CDATA[Naval Res. Lab, Electronics Division, Washington D.C., USA, Nov. 26, 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/lecture</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2284-1</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:creator><![CDATA[Soltani-Farshi, M.]]></dc:creator>
<dc:creator><![CDATA[Baumann, H.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Coleman, P. G.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Kreißig, U.]]></dc:creator>
<dc:creator><![CDATA[Bethge, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2284-1</dc:identifier>
<dc:title><![CDATA[Positron studies of defects in nitrogen and carbon implanted titanium]]></dc:title>
<dc:source><![CDATA[1998 Spring Meeting, San Francisco/CA, April 13-17, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
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<header>
<identifier>HZDR:PUBLDB:2316-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Hatzopoulos, N.]]></dc:creator>
<dc:creator><![CDATA[Suder, S.]]></dc:creator>
<dc:creator><![CDATA[Berg, J. A.]]></dc:creator>
<dc:creator><![CDATA[Donelly, S. E.]]></dc:creator>
<dc:creator><![CDATA[Armour, D. G.]]></dc:creator>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Fukarek, W.]]></dc:creator>
<dc:creator><![CDATA[Frey, L.]]></dc:creator>
<dc:creator><![CDATA[Foad, M. A.]]></dc:creator>
<dc:creator><![CDATA[Moffat, S.]]></dc:creator>
<dc:creator><![CDATA[Bailey, P.]]></dc:creator>
<dc:creator><![CDATA[Naakes, C. T. Q.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2316-1</dc:identifier>
<dc:title><![CDATA[Range and damage distribution in ultra low energy boron ion implantation]]></dc:title>
<dc:source><![CDATA[Proc. 11th Int. Conf. Ion Implantation Technology; The Institute of Electrical and Electronics Engineers, Piscataway, USA, 1997, p. 527]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2325-1</identifier>
<datestamp>2025-12-02</datestamp>
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<dc:title><![CDATA[Recriticality Calculations for Uraniumdioxide-Water Systems with MCNP]]></dc:title>
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<dc:description><![CDATA[With the aim of generating a certain feeling for the general dependencies of the multiplication factor k<sub>∞</sub> the first section provides some results for two classes of deformations of the original fuel pins. The main part examines UO<sub>2</sub>-structures of increasing disorder, beginning with the hexagonal close package of fuel spheres and ending up with stochastic geometries. Among these structures the worst case, i.e. the one with the highest k<sub>∞</sub> but preserving mechanical stability is identified. The composition and geometric parameter of this case is used to calculate the critical thickness of a slab and critical radius of a sphere.]]></dc:description>
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<dc:subject><![CDATA[Spin]]></dc:subject>
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<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-377-1</dc:identifier>
<dc:title><![CDATA[Technetium(V) and Rhenium(V) Complexes for 5-HT2A Serotonin Receptor Binding: Structure-Affinity Considerations]]></dc:title>
<dc:source><![CDATA[Journal of Nuclear Medicine and Biology 23 (1996) 429-438]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:1958-2</identifier>
<datestamp>2019-03-04</datestamp>
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<oai_dc:dc
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Eckert, S.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Lielausis, O.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1958-2</dc:identifier>
<dc:title><![CDATA[The behaviour of gas bubbles in a turbulent liquid metal MHD flow - Part I: Dispersion in quasi-two-dimensional MHD turbulence.]]></dc:title>
<dc:source><![CDATA[International Journal of Multiphase Flow (2000), Vol. 26/1, 45-66]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[We investigate the dispersion of gas bubbles injected from a single orifice into a liquid metal flow subjected to transverse and longitudinal magnetic fields. The local void fraction is detected by means of resistivity probes. The results show a damping of velocity fluctuations corresponding to a decrease in the bubble dispersion with increasing magnetic field. An isotropic distribution of the gas phase is preserved if a longitudinal field is applied,  while an anisotropic distribution is observed in case the applied magnetic field is transverse to the flow indicating the existence of quasi-two-dimensional vortices as typical of turbulent MHD flows. 

]]></dc:description>
<dc:subject><![CDATA[liquid metal-gas flow]]></dc:subject>
<dc:subject><![CDATA[bubble]]></dc:subject>
<dc:subject><![CDATA[magnetic field]]></dc:subject>
<dc:subject><![CDATA[MHD turbulence]]></dc:subject>
<dc:subject><![CDATA[void fraction]]></dc:subject>
<dc:subject><![CDATA[resistivity probe]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
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<identifier>HZDR:PUBLDB:2378-2</identifier>
<datestamp>2023-12-19</datestamp>
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<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Wendler, W.]]></dc:creator>
<dc:creator><![CDATA[Büttig, H.]]></dc:creator>
<dc:creator><![CDATA[Gabriel, F.]]></dc:creator>
<dc:creator><![CDATA[Gippner, P.]]></dc:creator>
<dc:creator><![CDATA[Gläser, W.]]></dc:creator>
<dc:creator><![CDATA[Grosse, E.]]></dc:creator>
<dc:creator><![CDATA[Guratzsch, H.]]></dc:creator>
<dc:creator><![CDATA[Dönau, F.]]></dc:creator>
<dc:creator><![CDATA[Höhnel, G.]]></dc:creator>
<dc:creator><![CDATA[Janssen, D.]]></dc:creator>
<dc:creator><![CDATA[Nething, U.]]></dc:creator>
<dc:creator><![CDATA[Pobell, F.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Pröhl, D.]]></dc:creator>
<dc:creator><![CDATA[Schilling, K.-D.]]></dc:creator>
<dc:creator><![CDATA[Schlenk, R.]]></dc:creator>
<dc:creator><![CDATA[Seidel, W.]]></dc:creator>
<dc:creator><![CDATA[Stephan, J.]]></dc:creator>
<dc:creator><![CDATA[Stein, P.]]></dc:creator>
<dc:creator><![CDATA[Wenzel, M.]]></dc:creator>
<dc:creator><![CDATA[Wustmann, B.]]></dc:creator>
<dc:creator><![CDATA[Zahn, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2378-2</dc:identifier>
<dc:title><![CDATA[The ELBE radiation source project at the Research Center Rossendorf]]></dc:title>
<dc:source><![CDATA[Mat. Sci. Forum 255-257 (1997) 732]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<identifier>HZDR:PUBLDB:2378-1</identifier>
<datestamp>2023-12-19</datestamp>
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<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Wendler, W.]]></dc:creator>
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<dc:creator><![CDATA[Gabriel, F.]]></dc:creator>
<dc:creator><![CDATA[Gippner, P.]]></dc:creator>
<dc:creator><![CDATA[Gläser, W.]]></dc:creator>
<dc:creator><![CDATA[Grosse, E.]]></dc:creator>
<dc:creator><![CDATA[Guratzsch, H.]]></dc:creator>
<dc:creator><![CDATA[Dönau, F.]]></dc:creator>
<dc:creator><![CDATA[Höhnel, G.]]></dc:creator>
<dc:creator><![CDATA[Janssen, D.]]></dc:creator>
<dc:creator><![CDATA[Nething, U.]]></dc:creator>
<dc:creator><![CDATA[Pobell, F.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Pröhl, D.]]></dc:creator>
<dc:creator><![CDATA[Schilling, K.-D.]]></dc:creator>
<dc:creator><![CDATA[Schlenk, R.]]></dc:creator>
<dc:creator><![CDATA[Seidel, W.]]></dc:creator>
<dc:creator><![CDATA[Stephan, J.]]></dc:creator>
<dc:creator><![CDATA[Stein, P.]]></dc:creator>
<dc:creator><![CDATA[Wenzel, M.]]></dc:creator>
<dc:creator><![CDATA[Wustmann, B.]]></dc:creator>
<dc:creator><![CDATA[Zahn, R.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2378-1</dc:identifier>
<dc:title><![CDATA[The ELBE radiation source project at the Research Center Rossendorf]]></dc:title>
<dc:source><![CDATA[11th Int. Conf. on Positron Annihilation (ICPA-11), Kansas City, USA, May 25-30, 1997]]></dc:source>
<dc:date>1997</dc:date>
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<header>
<identifier>HZDR:PUBLDB:3005-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Priede, J.]]></dc:creator>
<dc:creator><![CDATA[Gerbeth, G.]]></dc:creator>
<dc:creator><![CDATA[Gelfgat, Y.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3005-1</dc:identifier>
<dc:title><![CDATA[Verfahren und Vorrichtung zur Herstellung von Einkristallen in Ampullen unter Magnetfeldeinfluß]]></dc:title>
<dc:source><![CDATA[DE 197 04 075 A 1]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[Gegenstand der Erfindung ist ein Verfahren sowie eine Vorrichtung zur Herstellung von Einkristallen nach der Methode der gerichteten Erstarrung in einer Ampulle unter Nutzung elektromagnetischer Wirkungen auf die Schmelze und die Erstarrungsfront. Das Verfahren kann für die Produktion hochreiner Halbleiter-Einkristalle genutzt werden mit einem sehr geringen Gehalt an Makro- und Mikrodefekten und einer hohen Homogenität der Dotierverteilung sowohl entlang des Kristalls als auch über dem Kristallquerschnitt.
Die Erfindung besteht darin, daß die Schmelze während des Kristallwachstums durch Überlagerung eines statischen und eines rotierenden Magnetfeldes gezielt beeinflußt wird. Dabei wird ein rotierendes Magnetfeld der Polzahl 2p = 2 mit einer Amplitude im Bereich 0.5 bis 50 mT eingesetzt, wobei das Verhältnis der Induktivitäten von statischem und rotierendem Magnetfeld durch die Beziehung

Ha*(1+(Ha/(1+(Ha(δ<sub>ω</sub>*σ/σ*R)))))<sup>-1/2</sup>>k*Ta<sup>1/6</sup>

festgelegt wird. Bezüglich des angelegten Temperaturgradienten muß die Beziehung      Ta / Ha > Gr 1 / 2    erfüllt sein.
Diese Parameter werden während des Züchtungsprozesses nahezu konstant gehalten.]]></dc:description>
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<identifier>HZDR:PUBLDB:605-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Pochodzalla, J.]]></dc:creator>
<dc:creator><![CDATA[Immé, G.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:creator><![CDATA[Begemann-Blaich, M.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:creator><![CDATA[Möhlenkamp, T.]]></dc:creator>
<dc:creator><![CDATA[Seidel, W.]]></dc:creator>
<dc:creator><![CDATA[Kunze, W. D.]]></dc:creator>
<dc:creator><![CDATA[Schüttauf, A.]]></dc:creator>
<dc:creator><![CDATA[Kunde, G. J.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:creator><![CDATA[Bassini, R.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:creator><![CDATA[Trzcinski, A.]]></dc:creator>
<dc:creator><![CDATA[Zwieglinski, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-605-1</dc:identifier>
<dc:title><![CDATA[The nuclear liquid-gas phase transition: Present status and future perspectives]]></dc:title>
<dc:source><![CDATA[GSI-Preprint-96-31]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:234-1</identifier>
<datestamp>2020-09-02</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Spies, H.]]></dc:creator>
<dc:creator><![CDATA[Fietz, T.]]></dc:creator>
<dc:creator><![CDATA[Gläser, M.]]></dc:creator>
<dc:creator><![CDATA[Pietzsch, H.-J.]]></dc:creator>
<dc:creator><![CDATA[Johannsen, B.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-234-1</dc:identifier>
<dc:title><![CDATA[The n+1 -concept in the synthesis strategy of novel technetium and rhenium tracers]]></dc:title>
<dc:source><![CDATA[Technotium and rhenium in chemistry and nuclear medicine, Edited by Nicolini, M.; Bandoli, G, and Mazzi, U., SGEDITORIALI Padova 4 (1995) 243-246]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:3280-1</identifier>
<datestamp>2025-12-11</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Crochet, P.]]></dc:creator>
<dc:creator><![CDATA[Rami, F.]]></dc:creator>
<dc:creator><![CDATA[Gobbi, A.]]></dc:creator>
<dc:creator><![CDATA[Donà, R.]]></dc:creator>
<dc:creator><![CDATA[Coffin, J. P.]]></dc:creator>
<dc:creator><![CDATA[Fintz, P.]]></dc:creator>
<dc:creator><![CDATA[Guillaume, G.]]></dc:creator>
<dc:creator><![CDATA[Jundt, F.]]></dc:creator>
<dc:creator><![CDATA[Kuhn, C.]]></dc:creator>
<dc:creator><![CDATA[Roy, C.]]></dc:creator>
<dc:creator><![CDATA[Schauenburg, B.]]></dc:creator>
<dc:creator><![CDATA[Tizniti, L.]]></dc:creator>
<dc:creator><![CDATA[Wagner, P.]]></dc:creator>
<dc:creator><![CDATA[Alard, J. P.]]></dc:creator>
<dc:creator><![CDATA[Amouroux, V.]]></dc:creator>
<dc:creator><![CDATA[Andronic, A.]]></dc:creator>
<dc:creator><![CDATA[Basrak, Z.]]></dc:creator>
<dc:creator><![CDATA[Bastid, N.]]></dc:creator>
<dc:creator><![CDATA[Belyaev, I.]]></dc:creator>
<dc:creator><![CDATA[Best, D.]]></dc:creator>
<dc:creator><![CDATA[Biegansky, J.]]></dc:creator>
<dc:creator><![CDATA[Buta, A.]]></dc:creator>
<dc:creator><![CDATA[Caplar, R.]]></dc:creator>
<dc:creator><![CDATA[Cindro, N.]]></dc:creator>
<dc:creator><![CDATA[Dupieux, P.]]></dc:creator>
<dc:creator><![CDATA[Delalija, M.]]></dc:creator>
<dc:creator><![CDATA[Fan, Z. G.]]></dc:creator>
<dc:creator><![CDATA[Fodor, Z.]]></dc:creator>
<dc:creator><![CDATA[Fraysse, L.]]></dc:creator>
<dc:creator><![CDATA[Freifelder, R. P.]]></dc:creator>
<dc:creator><![CDATA[Herrmann, N.]]></dc:creator>
<dc:creator><![CDATA[Hildenbrand, K. D.]]></dc:creator>
<dc:creator><![CDATA[Hong, B.]]></dc:creator>
<dc:creator><![CDATA[Jeong, S. C.]]></dc:creator>
<dc:creator><![CDATA[Kecskemeti, J.]]></dc:creator>
<dc:creator><![CDATA[Kirejczyk, M.]]></dc:creator>
<dc:creator><![CDATA[Koncz, P.]]></dc:creator>
<dc:creator><![CDATA[Korolija, M.]]></dc:creator>
<dc:creator><![CDATA[Kotte, R.]]></dc:creator>
<dc:creator><![CDATA[Lebedev, A.]]></dc:creator>
<dc:creator><![CDATA[Leifels, Y.]]></dc:creator>
<dc:creator><![CDATA[Manko, V.]]></dc:creator>
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<dc:creator><![CDATA[Neubert, W.]]></dc:creator>
<dc:creator><![CDATA[Pelte, D.]]></dc:creator>
<dc:creator><![CDATA[Petrovici, M.]]></dc:creator>
<dc:creator><![CDATA[Pinkenburg, C.]]></dc:creator>
<dc:creator><![CDATA[Pras, P.]]></dc:creator>
<dc:creator><![CDATA[Ramillien, V.]]></dc:creator>
<dc:creator><![CDATA[Reisdorf, W.]]></dc:creator>
<dc:creator><![CDATA[Ritman, J. L.]]></dc:creator>
<dc:creator><![CDATA[Sadchikov, A. G.]]></dc:creator>
<dc:creator><![CDATA[Schüll, D.]]></dc:creator>
<dc:creator><![CDATA[Seres, Z.]]></dc:creator>
<dc:creator><![CDATA[Sikora, B.]]></dc:creator>
<dc:creator><![CDATA[Simion, V.]]></dc:creator>
<dc:creator><![CDATA[Siwek-Wilczyska, K.]]></dc:creator>
<dc:creator><![CDATA[Sodan, U.]]></dc:creator>
<dc:creator><![CDATA[Teh, K. M.]]></dc:creator>
<dc:creator><![CDATA[Trzaska, M.]]></dc:creator>
<dc:creator><![CDATA[Vasiliev, M.]]></dc:creator>
<dc:creator><![CDATA[Wang, G. S.]]></dc:creator>
<dc:creator><![CDATA[Wessels, J. P.]]></dc:creator>
<dc:creator><![CDATA[Wienold, T.]]></dc:creator>
<dc:creator><![CDATA[Wisniewski, K.]]></dc:creator>
<dc:creator><![CDATA[Wohlfarth, D.]]></dc:creator>
<dc:creator><![CDATA[Zhilin, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3280-1</dc:identifier>
<dc:title><![CDATA[Onset of nuclear matter expansion in Au+Au collisions]]></dc:title>
<dc:source><![CDATA[Nuclear Physics A 624(4) (1997) 755-772]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[

Using the FOPI detector at GSI Darmstadt, excitation functions of collective flow components were measured for
the Au+Au system, in the reaction plane and out of this plane, at seven incident energies ranging from 100A MeV
to 800A MeV. The threshold energies, corresponding to the onset of sideward-flow (balance energy) and
squeeze-out effect (transition energy), are extracted from extrapolations of these excitation functions toward
lower beam energies for charged products with Z>= 2. The transition energy is found to be larger than the balance
energy. The impact parameter dependence of both balance and transition energies, when extrapolated to central
collisions, suggests comparable although slightly higher values than the threshold energy for the radial flow. The
relevant parameter seems to be the energy deposited into the system in order to overcome the attractive nuclear
forces.]]></dc:description>
<dc:subject><![CDATA[Heavy ion collisions]]></dc:subject>
<dc:subject><![CDATA[Nuclear matter expansion]]></dc:subject>
<dc:subject><![CDATA[Sideward-flow]]></dc:subject>
<dc:subject><![CDATA[Squeeze-out]]></dc:subject>
<dc:subject><![CDATA[Radial flow]]></dc:subject>
<dc:subject><![CDATA[Balance energy]]></dc:subject>
<dc:subject><![CDATA[Transition energy]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0375-9474(97)00464-8]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-3280-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:14189-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Donat, C. K.]]></dc:creator>
<dc:creator><![CDATA[Walter, B.]]></dc:creator>
<dc:creator><![CDATA[Deuther-Conrad, W.]]></dc:creator>
<dc:creator><![CDATA[Nieber, K.]]></dc:creator>
<dc:creator><![CDATA[Brust, R.]]></dc:creator>
<dc:creator><![CDATA[Bauer, P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14189-1</dc:identifier>
<dc:title><![CDATA[Alterations of cholinergic receptors and the vesicular acetylcholine transporter after lateral fluid percussion injury in newborn piglets]]></dc:title>
<dc:source><![CDATA[Neuropathology and Applied Neurobiology 36(2010), 225-236]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Aims: Traumatic brain injury (TBI) is one of the leading causes of death and disability in children. Adult animal models of TBI showed cholinergic alterations. However, there is no comparable data on immature animals. Therefore, this study investigates cholinergic markers in a large animal model of juvenile TBI. Methods: Twenty-seven female newborn piglets were subjected to lateral fluid percussion (FP) injury and compared with 12 untreated animals. After 6 h, animals were sacrificed and the brains removed.The hemispheres ipsilateral to FP-TBI from seven piglets and corresponding hemispheres from six control animals were used for autoradiography. Receptor density was determined with [3H]epibatidine (nicotinic acetylcholine receptors) or [3H]QNB (muscarinic acetylcholine receptors). The density of the vesicular acetylcholine transporter (vAChT) was assessed with (-)-[3H]vesamicol. Cerebral blood flow was measured by coloured microsphere method. Results: Cerebral blood flow and brain oxygen delivery were transiently reduced early after FP-TBI (P < 0.05). TBI caused reductions of muscarinic acetylcholine receptor density (fmol/mg) in the basal forebrain (sham: 10797  1339, TBI: 8791  1031), while nicotinic acetylcholine receptor remained stable. Significant increases in vAChT density (fmol/mg) were observed in the basal forebrain (sham: 2347  171, TBI: 2884  544), putamen (sham: 2276  181, TBI: 2961  386), cortex (sham: 1928  262, TBI: 2377  294), thalamic areas (sham: 2133  272, TBI: 2659  413), hippocampus (sham: 2712  145, TBI: 3391  501) and hypothalamus (sham: 2659  139, TBI: 3084  304). Conclusions: Cholinergic markers are altered after mildto- moderate TBI in the immature brain.Whereas the ACh receptors are stable in almost any brain region after TBI, vAChT expression increases after trauma at the employed severity of this specific trauma model.]]></dc:description>
<dc:subject><![CDATA[muscarinic]]></dc:subject>
<dc:subject><![CDATA[newborn pig]]></dc:subject>
<dc:subject><![CDATA[nicotinic]]></dc:subject>
<dc:subject><![CDATA[receptor]]></dc:subject>
<dc:subject><![CDATA[traumatic brain injury]]></dc:subject>
<dc:subject><![CDATA[vesicular transporter]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1111/j.1365-2990.2009.01050.x]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14189-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2116-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Anikeev, A. V.]]></dc:creator>
<dc:creator><![CDATA[Noack, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2116-1</dc:identifier>
<dc:title><![CDATA[Energy confinement of the Finite ß Plasmas in the Gas Dynamic Trap]]></dc:title>
<dc:source><![CDATA[25th EPS Conference on Controlled Fusion and Plasma Physics, June 29 - July 3, 1998, Prague, Czech Republic, Proceedings Vol. 22C, pp. 627-630]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The Gas Dynamic Trap (GDT) is an axisymmetric mirror device with a high mirror ratio to confine a collisional plasma and a minority of fast ions. The latter are produced in the trap by oblique, high-power neutral beam (NB) injection into the collisional target plasma. The recent upgrade of the NB system resulted in an increase of the power maximum during the pulse from 2.5 to almost 4.5 MW. Under the new experimental situation were studied: the transport and stability of the high-ß plasma, the cross-field tranport and the detailed energy balance of the fast ions. 
The paper reports on the measurement techniques used and on the results achieved.]]></dc:description>
<dc:subject><![CDATA[plasma physics]]></dc:subject>
<dc:subject><![CDATA[gas dynamic trap]]></dc:subject>
<dc:subject><![CDATA[high-ß plasmas]]></dc:subject>
<dc:subject><![CDATA[stability]]></dc:subject>
<dc:subject><![CDATA[cross-field transport]]></dc:subject>
<dc:subject><![CDATA[neutral beam ijection]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2116-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2116-7</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Anikeev, A. V.]]></dc:creator>
<dc:creator><![CDATA[Noack, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2116-7</dc:identifier>
<dc:title><![CDATA[Energy confinement of the Finite ß Plasmas in the Gas Dynamic Trap]]></dc:title>
<dc:source><![CDATA[25th EPS Conference on Controlled Fusion and Plasma Physics, June 29 - July 3, 1998, Prague, Czech Republic, Proceedings Vol. 22C, pp. 627-630]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[The Gas Dynamic Trap (GDT) is an axisymmetric mirror device with a high mirror ratio to confine a collisional plasma and a minority of fast ions. The latter are produced in the trap by oblique, high-power neutral beam (NB) injection into the collisional target plasma. The recent upgrade of the NB system resulted in an increase of the power maximum during the pulse from 2.5 to almost 4.5 MW. Under the new experimental situation were studied: the transport and stability of the high-ß plasma, the cross-field tranport and the detailed energy balance of the fast ions. 
The paper reports on the measurement techniques used and on the results achieved.]]></dc:description>
<dc:subject><![CDATA[plasma physics]]></dc:subject>
<dc:subject><![CDATA[gas dynamic trap]]></dc:subject>
<dc:subject><![CDATA[high-ß plasmas]]></dc:subject>
<dc:subject><![CDATA[stability]]></dc:subject>
<dc:subject><![CDATA[cross-field transport]]></dc:subject>
<dc:subject><![CDATA[neutral beam ijection]]></dc:subject>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2116-7</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1066-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1066-1</dc:identifier>
<dc:title><![CDATA[Finite Element Based Vibration Analysis of WWER-440 Reactors]]></dc:title>
<dc:source><![CDATA[ICONE98, International Conference on Nuclear Engineering, San Diego, May 10-15, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[A finite-element-model describing the mechanical vibrations of the whole
WWER-440 primary circuit was established to support the early detection of mechanical component faults. A special fluid-structure module was developed to consider the reaction forces of the fluid in the downcomer upon the moving core barrel and the rector pressure vessel. This fluid-structure interaction module is based on an approximated analytical 2D-solution of the coupled system of 3D fluid equations and the structural equations of motions. By means of the vibration model all eigenfrequencies up to 30 Hz and the corresponding mode shapes were calculated. It is shown that the fluid-structure interaction strongly influences those modes that lead to a relative displacement between reactor pressure vessel and core barrel. Moreover, by means of the model the shift of eigenfrequencies due to the degradation or to the failure of internal clamping and spring elements was investigated.Comparing the frequency spectra of the normal and the faulty structure, it could be proved that a 
recognition of such degradations and failures even inside the reactor pressure vessel is possible by pure excore vibration measurements.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1066-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:1066-2</identifier>
<datestamp>2023-05-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-1066-2</dc:identifier>
<dc:title><![CDATA[Finite Element Based Vibration Analysis of WWER-440 Reactors]]></dc:title>
<dc:source><![CDATA[Proceedings of the 6th International Conference on Nuclear Engineering (ICONE-6) San Diego, May 10-15, 1998]]></dc:source>
<dc:date>1998</dc:date>
<dc:description><![CDATA[A finite-element-model describing the mechanical vibrations of the whole
WWER-440 primary circuit was established to support the early detection of mechanical component faults. A special fluid-structure module was developed to consider the reaction forces of the fluid in the downcomer upon the moving core barrel and the rector pressure vessel. This fluid-structure interaction module is based on an approximated analytical 2D-solution of the coupled system of 3D fluid equations and the structural equations of motions. By means of the vibration model all eigenfrequencies up to 30 Hz and the corresponding mode shapes were calculated. It is shown that the fluid-structure interaction strongly influences those modes that lead to a relative displacement between reactor pressure vessel and core barrel. Moreover, by means of the model the shift of eigenfrequencies due to the degradation or to the failure of internal clamping and spring elements was investigated.Comparing the frequency spectra of the normal and the faulty structure, it could be proved that a 
recognition of such degradations and failures even inside the reactor pressure vessel is possible by pure excore vibration measurements.]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:conferenceObject</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.13182/NT99-A3013]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-1066-2</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:821-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Grunwald, G.]]></dc:creator>
<dc:creator><![CDATA[Scheffler, M.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-821-1</dc:identifier>
<dc:title><![CDATA[Analytische Modellierung mechanischer Schwingungen von Primärkreiskomponenten des Druckwasserreaktors WWER-440 mit finiten Elementen]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-172 April 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[The project contributes to the improved evaluation of the mechanical integrity of the soviet-type VVER-440 reactors especially, to a sensitive early failure detection and to the localization of mechanical damages of reactor components by means of vibration monitoring. For that purpose the mechanical vibration of all primary circuit
components was modelled by finite elements. Modeling was built on the finite element code ANSYS. The interaction between the coolant flowing in the downcomer and the vibrating components has been considered by a fluid-structure element, which describes additional mode selective damping and intertia due to the coolant displacement when the downcomer geometry changes. The calculation model was adjusted using results from experimental vibration investigations. To some extent data from earlier measurements were available. But additionally dedicated experiments had to be performed at original VVERs. Now, the model can be regarded to be widely verified. Mainly it was applied to clarify how hypothetical damages of reactor internals influence the vibration signature of the primary circuit. Such kind of damage simulation is an appropriate means to find sensitive measuring positiones for on-line monitoring and to define physically based threshold values. In principle, the model is even suited to estimate the loads of reactor components which might be imposed by external events (explosion, earthquake).
]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>ger</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-821-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2908-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Panknin, D.]]></dc:creator>
<dc:creator><![CDATA[Wirth, H.]]></dc:creator>
<dc:creator><![CDATA[Anwand, W.]]></dc:creator>
<dc:creator><![CDATA[Brauer, G.]]></dc:creator>
<dc:creator><![CDATA[Skorupa, W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2908-1</dc:identifier>
<dc:title><![CDATA[High concentration doping of 6H-SiC by ion implantation: flash versus furnace annealing]]></dc:title>
<dc:source><![CDATA[Mat. Sci. Forum 338-342 (2000) 877]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The electrical properties of high concentration aluminum and nitrogen implanted layers have been investigated after furnace as well as flash lamp annealing. For Al doped layers the electrical efficiency is enhanced using flash lamp annealing. For highest Al concentrations the doped layer shows metal like conductivity. For N doped layers the flash lamp annealing effects no increase of the carrier concentration. Due to the short annealing time only the nitrogen on hexagonal sites is electrically active. Flash lamp annealing produced no extra damage of the vacancy type as proved by Positron Annihilation Spectroscopy.]]></dc:description>
<dc:subject><![CDATA[aluminum]]></dc:subject>
<dc:subject><![CDATA[nitrogen]]></dc:subject>
<dc:subject><![CDATA[ion implantation]]></dc:subject>
<dc:subject><![CDATA[annealing]]></dc:subject>
<dc:subject><![CDATA[electrical activation]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2908-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2909-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
            xsi:schemaLocation="http://www.openarchives.org/OAI/2.0/oai_dc/
            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:creator><![CDATA[Rindelhardt, U.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-2909-1</dc:identifier>
<dc:title><![CDATA[Institute of Safety Research; Report January 1998-June 1999]]></dc:title>
<dc:source><![CDATA[Wissenschaftlich-Technische Berichte / Forschungszentrum Rossendorf; FZR-273 September 1999]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[The report gives an overview on the scientific work of the Institute of Safety Research between January 1998 and June 1999. ]]></dc:description>
<dc:type>info:eu-repo/semantics/report</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:report</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2909-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
</oai_dc:dc>
</metadata>
</record>
<record>
<header>
<identifier>HZDR:PUBLDB:2631-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:creator><![CDATA[Schulz-Lang, E.]]></dc:creator>
<dc:creator><![CDATA[Abram, S.]]></dc:creator>
<dc:creator><![CDATA[Wegmann, J.]]></dc:creator>
<dc:creator><![CDATA[Dilworth, J. R.]]></dc:creator>
<dc:creator><![CDATA[Kirmse, R.]]></dc:creator>
<dc:creator><![CDATA[Woolins, J. D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2631-1</dc:identifier>
<dc:title><![CDATA[Technetium(V) and Rhenium(V) Nitrido Complexes with Tetraphenylimidodithiodiphosphinate, [(Ph<SUB>2</SUB>PS)<SUB>2</SUB>N]<SUP>- </SUP>]]></dc:title>
<dc:source><![CDATA[J. Chem. Soc. Dalton Trans. 623 (1997)]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<header>
<identifier>HZDR:PUBLDB:3523-2</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Hornauer, U.]]></dc:creator>
<dc:creator><![CDATA[Günzel, R.]]></dc:creator>
<dc:creator><![CDATA[Richter, E.]]></dc:creator>
<dc:creator><![CDATA[Wieser, E.]]></dc:creator>
<dc:creator><![CDATA[Möller, W.]]></dc:creator>
<dc:creator><![CDATA[Schumacher, G.]]></dc:creator>
<dc:creator><![CDATA[Dettenwanger, F.]]></dc:creator>
<dc:creator><![CDATA[Schütze, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3523-2</dc:identifier>
<dc:title><![CDATA[Improvement of the High Temperature Oxidation Behaviour of TiAl Alloy by Cl Implantation using PIII]]></dc:title>
<dc:source><![CDATA[PSE 2000, Garmisch Partenkirchen, Germany, 17-21.9.2000]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The intermetallic compound TiAl is very interesting for high temperature application due to its high temperature strength and low density. Above 700 °C, the use in e.g. aircraft engines is hindered because of a low oxidation resistance. Even though the compound contains 50at% Al, this is not sufficient to form a protective Al2O3 scale. Instead, a mixed oxide scale composed of TiO2 and Al2O3 is formed. Extended alloy development has shown, that additional elements which are beneficial for the oxidation often have a bad influence on the mechanical bulk properties. Cl doping has a strong effect even in very low concentrations of about 500 ppm ("Microalloy"). Ion Implantation of 1016 Cl/cm2 protects TiAl at 900 °C for up to 1000 h against oxidation in a wide range of implantation energies. 

In order to apply this effect for complicated shaped parts, the high temperature oxidation behavior after plasma immersion ion implantation of chlorine into different TiAl alloys was investigated. A specialized chamber has been setup up for the strongly etching Cl plasma. Particularly with regard to contaminations, the chamber and the RF- antenna had to be made from aluminum. Since it is known that the Cl effect in TiAl requires a well defined Cl concentration, a variation of the implantation parameters has been performed. The resulting depth profiles of Cl are investigated using depth profiling with Auger electron spectroscopy (AES). After treatment (3*105 to 3*106 30 kV pulses of 5µs at a repetition rate from 150 Hz to 1500 Hz), the Cl is located close to the surface. The process is governed by the interplay between etching and implanting during the HV pulses. Therefore the retained dose depends mainly on the temperature during implantation, which is controlled by the repetition rate of the pulses. Oxidation tests at 900°C in air for 100 h showed a strong reduction of the oxidation, which are comparable to conventional beam line im-plantations of Cl. 
]]></dc:description>
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<header>
<identifier>HZDR:PUBLDB:141-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
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<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Neubert, W.]]></dc:creator>
<dc:creator><![CDATA[Mösner, J.]]></dc:creator>
<dc:creator><![CDATA[Kotte, R.]]></dc:creator>
<dc:creator><![CDATA[Wohlfarth, D.]]></dc:creator>
<dc:creator><![CDATA[Barz, H.-W.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-141-1</dc:identifier>
<dc:title><![CDATA[The reaction Au + Au at 150 AMeV simulated by the Copenhagen Statistical Multifragmentation Model]]></dc:title>
<dc:source><![CDATA[XXXII International Winter Meeting on Nuclear Physics, Bormio, Italy, 24.-29.1.1994]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/conferenceObject</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:477-2</identifier>
<datestamp>2021-11-02</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/openAccess</dc:rights>
<dc:creator><![CDATA[Titov, A. I.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Reznik, B. L.]]></dc:creator>
<dc:creator><![CDATA[Shklyar, V.]]></dc:creator>
<dc:publisher>Helmholtz-Zentrum Dresden-Rossendorf / HZDR</dc:publisher>
<dc:identifier>https://www.hzdr.de/publications/Publ-477-2</dc:identifier>
<dc:title><![CDATA[The reaction NN -> NNgamma in the 1 GeV region within an effective one-boson exchange model]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; FZR-118 Preprint]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[Abstract
Within an effective one- boson exchange parametrization of the T matrix of NN interactions we calculate cross sections for the reactions pp → ppγ and pn → pnγ for proton incidence energies in the order of 1 GeV. Besides bremsstrahlung processes we consider photons from ∆ decays and contributions from the η → γγ process, where the η is excited via the N<sub>1535</sub> resonance. At beam energies above 700 MeV the ∆ decay channiel dsminates for large photon energies, while above the η threshold the η decay photons ähsw up only in a narrow window. The low energy photons stem frorn pure bremsstrahlunig processes.]]></dc:description>
<dc:type>info:eu-repo/semantics/preprint</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
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<dc:language>eng</dc:language>
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<header>
<identifier>HZDR:PUBLDB:477-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
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            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Titov, A. I.]]></dc:creator>
<dc:creator><![CDATA[Kämpfer, B.]]></dc:creator>
<dc:creator><![CDATA[Reznik, B. L.]]></dc:creator>
<dc:creator><![CDATA[Shklyar, V.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-477-1</dc:identifier>
<dc:title><![CDATA[The reaction NN -> NNgamma in the 1 GeV region within an effective one-boson exchange model]]></dc:title>
<dc:source><![CDATA[Physics Letters B 372 (1996) pp. 15-19]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[Abstract
Within an effective one- boson exchange parametrization of the T matrix of NN interactions we calculate cross sections for the reactions pp → ppγ and pn → pnγ for proton incidence energies in the order of 1 GeV. Besides bremsstrahlung processes we consider photons from ∆ decays and contributions from the η → γγ process, where the η is excited via the N<sub>1535</sub> resonance. At beam energies above 700 MeV the ∆ decay channiel dsminates for large photon energies, while above the η threshold the η decay photons ähsw up only in a narrow window. The low energy photons stem frorn pure bremsstrahlunig processes.]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-477-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:666-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Fomichev, A. S.]]></dc:creator>
<dc:creator><![CDATA[David, I.]]></dc:creator>
<dc:creator><![CDATA[Lukyanov, S. M.]]></dc:creator>
<dc:creator><![CDATA[Penionzhkevich, Y. E.]]></dc:creator>
<dc:creator><![CDATA[Skobelev, N. K.]]></dc:creator>
<dc:creator><![CDATA[Tarasov, O. B.]]></dc:creator>
<dc:creator><![CDATA[Matthies, A.]]></dc:creator>
<dc:creator><![CDATA[Ortlepp, H.-G.]]></dc:creator>
<dc:creator><![CDATA[Wagner, W.]]></dc:creator>
<dc:creator><![CDATA[Lewitowicz, M.]]></dc:creator>
<dc:creator><![CDATA[Saint-Laurent, M. G.]]></dc:creator>
<dc:creator><![CDATA[u. a.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-666-1</dc:identifier>
<dc:title><![CDATA[The response of a large CsI(Tl) detector particles and heavy ions in the intermediate energy range]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research A 344 (1994) pp. 378]]></dc:source>
<dc:date>1994</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
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<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:828-1</identifier>
<datestamp>2022-11-11</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Wilhelm, M.]]></dc:creator>
<dc:creator><![CDATA[Eberth, J.]]></dc:creator>
<dc:creator><![CDATA[Pascovici, G.]]></dc:creator>
<dc:creator><![CDATA[Radermacher, E.]]></dc:creator>
<dc:creator><![CDATA[Thomas, H. G.]]></dc:creator>
<dc:creator><![CDATA[Brentano, P.]]></dc:creator>
<dc:creator><![CDATA[Prade, H.]]></dc:creator>
<dc:creator><![CDATA[Lieder, R. M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-828-1</dc:identifier>
<dc:title><![CDATA[The response of the Euroball Cluster detector to gamma-radiation up to 10 MeV]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research A 381 (1996) pp. 462-465]]></dc:source>
<dc:date>1996</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1016/S0168-9002(96)00793-0]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-828-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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</record>
<record>
<header>
<identifier>HZDR:PUBLDB:14252-1</identifier>
<datestamp>2025-06-05</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Liu, S.-P.]]></dc:creator>
<dc:creator><![CDATA[Weisbrod, S.]]></dc:creator>
<dc:creator><![CDATA[Tang, Z.]]></dc:creator>
<dc:creator><![CDATA[Marx, A.]]></dc:creator>
<dc:creator><![CDATA[Scheer, E.]]></dc:creator>
<dc:creator><![CDATA[Erbe, A.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14252-1</dc:identifier>
<dc:title><![CDATA[Direct Measurement of Electrical Transport Through G-Quadruplex DNA with Mechanically Controllable Break Junction Electrodes]]></dc:title>
<dc:source><![CDATA[Angewandte Chemie - International Edition (2010)]]></dc:source>
<dc:date>2010</dc:date>
<dc:description><![CDATA[Here we report on direct transport measurements on a G-quadruplex covalently wired between two gold electrodes realized by the mechanically controllable break junction technique. We found that the G-quadruplex shows a rather high conductance. Interestingly, when the distance of both electrodes was reversibly varied over a several nm-span this conductance behavior persists reproducibly. These hitherto unprecedented properties make G-quadruplexes interesting candidates for nanoelectronic applications where varied distances between electrodes need bridging without loss of conductance.]]></dc:description>
<dc:subject><![CDATA[molecular electronics]]></dc:subject>
<dc:subject><![CDATA[DNA]]></dc:subject>
<dc:subject><![CDATA[mechanically controlled break junctions]]></dc:subject>
<dc:subject><![CDATA[nanoelectronics]]></dc:subject>
<dc:type>info:eu-repo/semantics/article</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:article</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation><![CDATA[info:eu-repo/semantics/altIdentifier/doi/10.1002/anie.201000022]]></dc:relation>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-14252-1</dc:relation>
<dc:audience>Researchers</dc:audience>
<dc:audience>Students</dc:audience>
<dc:format><![CDATA[application/pdf]]></dc:format>
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<record>
<header>
<identifier>HZDR:PUBLDB:2864-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
            xmlns:dc="http://purl.org/dc/elements/1.1/"
            xmlns:xsi="http://www.w3.org/2001/XMLSchema-instance"
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            http://www.openarchives.org/OAI/2.0/oai_dc.xsd">
<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Abram, U.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2864-1</dc:identifier>
<dc:title><![CDATA[Trinuclear rhenium complexes with bridging nitrido ligands]]></dc:title>
<dc:source><![CDATA[Anorganische allg. Chemie]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[Trinuclear complexes with bridging nitrido ligands between the rhenium atoms are formed when [ReN(Et2dtc)2(Me2PhP)] (Et2dtc- = N,N-diethyldithio-carbamate) reacts with TlCl or Pr(O3SCF3)3. [Cl(Me2PhP)2(Et2dtc)ReºN-Re(N)Cl2(Me2PhP)-NºRe(Et2dtc)(Me2PhP)2Cl] and [(Et2dtc)2(Me2PhP)ReºN-Re(N)-(Et2dtc)(Me2PhP)-NºRe(Me2PhP)(Et2dtc)2]+ contain two almost linear, asymmetric nitrido bridges. Additional, terminal nitrido ligands are located at the middle rhenium atoms.




]]></dc:description>
<dc:subject><![CDATA[Keywords: Rhenium complexes]]></dc:subject>
<dc:subject><![CDATA[Nitrido bridges]]></dc:subject>
<dc:subject><![CDATA[Crystal structure]]></dc:subject>
<dc:subject><![CDATA[Oligomerization]]></dc:subject>
<dc:type>info:eu-repo/semantics/contributionToPeriodical</dc:type>
<dc:type>info:eu-repo/semantics/publishedVersion</dc:type>
<dc:type>doc-type:contributionToPeriodical</dc:type>
<dc:type>Text</dc:type>
<dc:language>eng</dc:language>
<dc:relation>info:eu-repo/semantics/altIdentifier/purl/https://www.hzdr.de/publications/Publ-2864-1</dc:relation>
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<dc:audience>Students</dc:audience>
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<record>
<header>
<identifier>HZDR:PUBLDB:2867-1</identifier>
<datestamp>2019-03-04</datestamp>
<setSpec>HZDR:Publications</setSpec>
</header>
<metadata>
<oai_dc:dc
            xmlns:oai_dc="http://www.openarchives.org/OAI/2.0/oai_dc/"
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Geist, V.]]></dc:creator>
<dc:creator><![CDATA[Hennig, C.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2867-1</dc:identifier>
<dc:title><![CDATA[Kristallographische Untersuchungen an meteoritischem (Fe,Ni)-Phosphid]]></dc:title>
<dc:source><![CDATA[Zeitschrift für Kristallographie, Suppl. 15, 106 (1998)]]></dc:source>
<dc:date>1998</dc:date>
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<dc:creator><![CDATA[Hennig, C.]]></dc:creator>
<dc:creator><![CDATA[Hallmeier, K. H.]]></dc:creator>
<dc:creator><![CDATA[Zahn, G.]]></dc:creator>
<dc:creator><![CDATA[Tschwatschal, F.]]></dc:creator>
<dc:creator><![CDATA[Hennig, H.]]></dc:creator>
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<dc:title><![CDATA[Conformational Influence of Dithiocarbazinic Acid Bishydrazone Ligands on the Structure of Zinc(II) Complexes: A Comparative XANES Study]]></dc:title>
<dc:source><![CDATA[Inorganic Chemistry 1999, 38, 38-43]]></dc:source>
<dc:date>1999</dc:date>
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<dc:creator><![CDATA[Jäger, H.-U.]]></dc:creator>
<dc:creator><![CDATA[Albe, K.]]></dc:creator>
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<dc:title><![CDATA[Molecular-dynamics simulations of steady-state growth of ion-deposited tetrahedral amorphous carbon films]]></dc:title>
<dc:source><![CDATA[TRANSDIAM", 5 - 7 June 2000, Amiens, France]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Molecular-dynamics calculations were performed to simulate ion beam deposition of diamond-like carbon films. Using the computationally efficient analytical potentials of Tersoff and Brenner we are able to simulate more than 10<sup>3</sup> carbon atom impacts on {111} diamond, so that steady-state film properties can be computed and analyzed. For the Tersoff potential, we achieve <i>sp<sup>3</sup></i> fractions of approximately half of the experimentally observed values. For the more refined hydrocarbon potentials of Brenner the fraction of tetrahedrally coordinated atoms is much too low, even if structures with densities close to diamond are obtained. We show, that the <i>sp<sup>3</sup></i> contents calculated with Tersoff's potential are an artifact related to the overbinding of specific bonding configurations between three- and fourfold coordinated sites. On the other hand we can prove, that the range for the binding orbitals represented by the cutoff-function is too short in Brenner's parametrization.  If an increased C-C interaction cutoff value is chosen, we achieve a distinct improvement in modeling the <i>sp<sup>3</sup></i> content of deposited ta-C films. As a result, we compute <i>sp<sup>3</sup></i> fractions which lie between 52 and 95% for the C<sup>+</sup> ion energies <i>E</i> = 30-80eV and are in reasonable agreement to recent experimental studies.
]]></dc:description>
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<dc:creator><![CDATA[Jäger, H.-U.]]></dc:creator>
<dc:creator><![CDATA[Albe, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2871-2</dc:identifier>
<dc:title><![CDATA[Molecular-dynamics simulations of steady-state growth of ion-deposited tetrahedral amorphous carbon films]]></dc:title>
<dc:source><![CDATA[Journal of Applied Physics 88 (2000) 1129-35]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[Molecular-dynamics calculations were performed to simulate ion beam deposition of diamond-like carbon films. Using the computationally efficient analytical potentials of Tersoff and Brenner we are able to simulate more than 10<sup>3</sup> carbon atom impacts on {111} diamond, so that steady-state film properties can be computed and analyzed. For the Tersoff potential, we achieve <i>sp<sup>3</sup></i> fractions of approximately half of the experimentally observed values. For the more refined hydrocarbon potentials of Brenner the fraction of tetrahedrally coordinated atoms is much too low, even if structures with densities close to diamond are obtained. We show, that the <i>sp<sup>3</sup></i> contents calculated with Tersoff's potential are an artifact related to the overbinding of specific bonding configurations between three- and fourfold coordinated sites. On the other hand we can prove, that the range for the binding orbitals represented by the cutoff-function is too short in Brenner's parametrization.  If an increased C-C interaction cutoff value is chosen, we achieve a distinct improvement in modeling the <i>sp<sup>3</sup></i> content of deposited ta-C films. As a result, we compute <i>sp<sup>3</sup></i> fractions which lie between 52 and 95% for the C<sup>+</sup> ion energies <i>E</i> = 30-80eV and are in reasonable agreement to recent experimental studies.
]]></dc:description>
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<dc:creator><![CDATA[Behrisch, R.]]></dc:creator>
<dc:creator><![CDATA[Linden, W.]]></dc:creator>
<dc:creator><![CDATA[Toussaint, U.]]></dc:creator>
<dc:creator><![CDATA[Grambole, D.]]></dc:creator>
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<dc:title><![CDATA[Surface layer destruction during ion beam analysis]]></dc:title>
<dc:source><![CDATA[Nuclear Instruments and Methods in Physics Research B 155 (1999) 440-446]]></dc:source>
<dc:date>1999</dc:date>
<dc:description><![CDATA[In ion beam analysis the decrease of the measuring signal with a number of incident ions, due to a destruction of the surface layer being analysed, depends critically
on the lateral intensity distribution in the analysing ion beam. For the assumption of destruction in one step, the decrease was calculated and the obtained analytical
formulae was fitted to the decrease as measured in ERDA and PIXE analyses. This allows to obtain values for the destruction cross sections for the ions and the
samples in the analysis, as well as information about the lateral intensity distribution in the analysing ion beam.]]></dc:description>
<dc:subject><![CDATA[Hydrogen]]></dc:subject>
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Grunwald, G.]]></dc:creator>
<dc:creator><![CDATA[Scheffler, M.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-340-1</dc:identifier>
<dc:title><![CDATA[Theoretical Vibration Model of VVER Reactors Considering Fluid-Structure-Interaction]]></dc:title>
<dc:source><![CDATA[Tagung: SMORN VII, Avignon, France, 19 - 23 June 1995]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[A finite-element-model describing the mechanical vibrations of the whole VVER-440 primary circuit is being developed to support the early detection of mechanical component faults. A special fluid-structure-element was developed to consider the reaction forces of the fluid in the downcomer upon the moving core barrel and the rector pressure vessel. It was derived from an approximated analytical 2D-solution of the coupled system of 3D fluid equations and the structural equations of motions. By means of the vibration model all eigenfrequencies up to 30 Hz and the corresponding mode shapes were calculated. It is shown that the fluid-structure-interaction strongly influences those modes exhibiting a relative displacement between reactor pressure vessel and core barrel. Moreover, by means of the model the shift of eigenfrequencies due to the degradation or to the failure of internal clamping and spring elements was investigated. By comparing the frequency spectra of the normal and of the faulty structure, it could be shown that a recognition of such degradations and failures even inside the reactor pressure vessel is possible by pure excore vibration measurements.]]></dc:description>
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Grunwald, G.]]></dc:creator>
<dc:creator><![CDATA[Scheffler, M.]]></dc:creator>
<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-340-2</dc:identifier>
<dc:title><![CDATA[Theoretical Vibration Model of VVER Reactors Considering Fluid-Structure-Interaction]]></dc:title>
<dc:source><![CDATA[Tagung: SMORN VII, Avignon, France, 19 - 23 June 1995, Vol. 2, 9.7]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[A finite-element-model describing the mechanical vibrations of the whole VVER-440 primary circuit is being developed to support the early detection of mechanical component faults. A special fluid-structure-element was developed to consider the reaction forces of the fluid in the downcomer upon the moving core barrel and the rector pressure vessel. It was derived from an approximated analytical 2D-solution of the coupled system of 3D fluid equations and the structural equations of motions. By means of the vibration model all eigenfrequencies up to 30 Hz and the corresponding mode shapes were calculated. It is shown that the fluid-structure-interaction strongly influences those modes exhibiting a relative displacement between reactor pressure vessel and core barrel. Moreover, by means of the model the shift of eigenfrequencies due to the degradation or to the failure of internal clamping and spring elements was investigated. By comparing the frequency spectra of the normal and of the faulty structure, it could be shown that a recognition of such degradations and failures even inside the reactor pressure vessel is possible by pure excore vibration measurements.]]></dc:description>
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<identifier>HZDR:PUBLDB:340-3</identifier>
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<dc:creator><![CDATA[Altstadt, E.]]></dc:creator>
<dc:creator><![CDATA[Grunwald, G.]]></dc:creator>
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<dc:creator><![CDATA[Weiß, F.-P.]]></dc:creator>
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<dc:title><![CDATA[Theoretical Vibration Model of VVER Reactors Considering Fluid-Structure-Interaction]]></dc:title>
<dc:source><![CDATA[Forschungszentrum Rossendorf; März 1995, Preprint of SMORN VII]]></dc:source>
<dc:date>1995</dc:date>
<dc:description><![CDATA[A finite-element-model describing the mechanical vibrations of the whole VVER-440 primary circuit is being developed to support the early detection of mechanical component faults. A special fluid-structure-element was developed to consider the reaction forces of the fluid in the downcomer upon the moving core barrel and the rector pressure vessel. It was derived from an approximated analytical 2D-solution of the coupled system of 3D fluid equations and the structural equations of motions. By means of the vibration model all eigenfrequencies up to 30 Hz and the corresponding mode shapes were calculated. It is shown that the fluid-structure-interaction strongly influences those modes exhibiting a relative displacement between reactor pressure vessel and core barrel. Moreover, by means of the model the shift of eigenfrequencies due to the degradation or to the failure of internal clamping and spring elements was investigated. By comparing the frequency spectra of the normal and of the faulty structure, it could be shown that a recognition of such degradations and failures even inside the reactor pressure vessel is possible by pure excore vibration measurements.]]></dc:description>
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<identifier>HZDR:PUBLDB:2543-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Grigull, S.]]></dc:creator>
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<dc:title><![CDATA[Transport und Strukturmodifikation bei der Stickstoffimplantation in amorphen Kohlenstoff]]></dc:title>
<dc:source><![CDATA[TU Dresden, July 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/doctoralThesis</dc:type>
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<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Jentschel, M.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2545-1</dc:identifier>
<dc:title><![CDATA[Crystal-GRID: Eine neue nukleare Sonde zur Untersuchung atomarer Bewegung im Festkörper]]></dc:title>
<dc:source><![CDATA[TU Dresden, April 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/doctoralThesis</dc:type>
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<identifier>HZDR:PUBLDB:2546-1</identifier>
<datestamp>2019-03-04</datestamp>
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<dc:rights>info:eu-repo/semantics/closedAccess</dc:rights>
<dc:creator><![CDATA[Möller, D.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-2546-1</dc:identifier>
<dc:title><![CDATA[Synthese schwermetallionensensitiver Membranen für ISFETs mittels Ionenimplantation]]></dc:title>
<dc:source><![CDATA[TU Dresden, July 1997]]></dc:source>
<dc:date>1997</dc:date>
<dc:description><![CDATA[]]></dc:description>
<dc:type>info:eu-repo/semantics/doctoralThesis</dc:type>
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<dc:title><![CDATA[TRIDYN-Computersimulationen zur Schicht-Deposition von BN und zur Hochdosisimplantation in Si]]></dc:title>
<dc:source><![CDATA[Friedrich-Schiller-Universität Jena, April 1997]]></dc:source>
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<datestamp>2019-03-04</datestamp>
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<dc:creator><![CDATA[Repp, T.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-3101-1</dc:identifier>
<dc:title><![CDATA[Acoustic waterhammer simulations with consideration of fluid-structure interaction (FSI)]]></dc:title>
<dc:source><![CDATA[Sammelband Workshop Kompetenzerhalt Kerntechnik, Jahrestagung Kerntechnik 2000, Bonn, 23.-25. Mai]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The results (maximum pressure amplitude and tangential stresses) of acoustic waterhammer simulations with consideration of fluid-structure interaction in straight and bended pipes are shown and compared with analytical results for some ratios of wall thickness to diameter and bending radius to diameter. A adjusted formula is described for the maximum dynamic tangential stress.   ]]></dc:description>
<dc:subject><![CDATA[waterhammer]]></dc:subject>
<dc:subject><![CDATA[fluid-structure interaction]]></dc:subject>
<dc:subject><![CDATA[acoustic simulation]]></dc:subject>
<dc:subject><![CDATA[pipe]]></dc:subject>
<dc:subject><![CDATA[pipe bend]]></dc:subject>
<dc:subject><![CDATA[wave]]></dc:subject>
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<dc:title><![CDATA[Acoustic waterhammer simulations with consideration of fluid-structure interaction (FSI)]]></dc:title>
<dc:source><![CDATA[Sammelband Workshop Kompetenzerhalt Kerntechnik, Jahrestagung Kerntechnik 2000, Bonn, 23.-25. Mai]]></dc:source>
<dc:date>2000</dc:date>
<dc:description><![CDATA[The results (maximum pressure amplitude and tangential stresses) of acoustic waterhammer simulations with consideration of fluid-structure interaction in straight and bended pipes are shown and compared with analytical results for some ratios of wall thickness to diameter and bending radius to diameter. A adjusted formula is described for the maximum dynamic tangential stress.   ]]></dc:description>
<dc:subject><![CDATA[waterhammer]]></dc:subject>
<dc:subject><![CDATA[fluid-structure interaction]]></dc:subject>
<dc:subject><![CDATA[acoustic simulation]]></dc:subject>
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<datestamp>2025-06-05</datestamp>
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<dc:creator><![CDATA[Fahmy, K.]]></dc:creator>
<dc:identifier>https://www.hzdr.de/publications/Publ-14313-2</dc:identifier>
<dc:title><![CDATA[Fourier Transform Infrared Spectroscopy for Biophysical Applications: Technical Aspects]]></dc:title>
<dc:source><![CDATA[Gordon C. K. Roberts: Encyclopedia of Biophysics, Berlin: Springer, 2013, 978-3-642-16711-9, 844-852]]></dc:source>
<dc:date>2013</dc:date>
<dc:description><![CDATA[FTIR spectroscopy has become an important non-destructive tool in gathering structural information of biological macromolecules at atomic resolution and under functional conditions. Modern instrumentation allows recording high resolution IR spectra of biomolecules in liquids, thin films, and adsorbed monolayers without chemical modification. The time-course of structural changes of biomolecules can be followed easily down to ~20 ms time resolution with rapidly scanning interferometers.  If such reactions are highly reproducible, molecular mechanisms can be studied at a time resolution down to ns by step scan interferometers. Despite the advanced user-friendliness in operating modern FTIR spectrometers, the use of the adequate detector type, the correct adjustment of the signal to noise ratio, the setting of optical and electronic filters to physically restrict the band width and the corresponding choice of the interferometer scanning speed are crucial parameters in the hand of the user. Their prudential use is essential for gaining high quality spectra by proper signal averaging procedures in static as well as time-resolved experiments and for avoiding spectral artefacts inherent to improper sampling of both the optical path and the intensity of the IR interferogram.]]></dc:description>
<dc:subject><![CDATA[FTIR]]></dc:subject>
<dc:subject><![CDATA[difference spectroscopy]]></dc:subject>
<dc:subject><![CDATA[time-resolved]]></dc:subject>
<dc:subject><![CDATA[step scan]]></dc:subject>
<dc:subject><![CDATA[rapid scan]]></dc:subject>
<dc:subject><![CDATA[bacteriorhodopsin]]></dc:subject>
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<dc:title><![CDATA[Metabolism of L-6-[<SUP>18</SUP>F]fluoro-3,4-dihydroxyphenylalanine (FDOPA) in plasma and brain of neonatal pigs under the conditions of asphyxia.]]></dc:title>
<dc:source><![CDATA[J. Cereb. Blood Flow Metab. 17 (1997) S159]]></dc:source>
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<dc:title><![CDATA[HPLC-Analyse des Metabolismus von 6-[<SUP>18</SUP>F]Fluor-L-DOPA (FDOPA) im neonatalen Schweinehirn.]]></dc:title>
<dc:source><![CDATA[35. Intern. Jahrestagung der Deutschen Gesellschaft für Nuklearmedizin e.V., Kassel 16.4.-19.4.1997.]]></dc:source>
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<dc:title><![CDATA[HPLC-Analyse des Metabolismus von 6-[<SUP>18</SUP>F]Fluor-L-DOPA (FDOPA) im neonatalen Schweinehirn.]]></dc:title>
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<dc:title><![CDATA[Structure of Chlorobis(dimethylphenylphosphine)bis(imidotetraphenyldithiophosphinatoS,S') nitridorhenium(V)]]></dc:title>
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<dc:title><![CDATA[Indium(III) Complexes with Tridentate Nitrogen Donor Ligands. Synthesis, Characterization and Crystal Structures of Complexes with 2,6-Bis(acetyloxime)pyridine and 2,6-Bis(1-phenylimino ethyl)pyridine]]></dc:title>
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<dc:title><![CDATA[Mixed-Ligand Complexes of Indium (III). Reactions of [InCl<SUB>3</SUB>(L<SUP>1</SUP>)(MeOH)] with bidentate Ligands. Synthesis, Characterization and Crystal Structures of [In(L<SUP>1</SUP>)Cl(ox)(OH<SUB>2</SUB>)] 2 H<SUB>2</SUB>O, [In(L<SUP>1</SUP>)Cl(mnt)] MeOH and [In(pythio)<SUB>3</SUB>] (L<SUP>1</SUP> = Pyridine-2,6-bis(acetyloxime), ox<SUP>2-</SUP> = oxalate, mnt<SUP>2-</SUP> = l,2-dicyano ethene-1,2-dithiolate, pythio = pyridine-2-thiolate)]]></dc:title>
<dc:source><![CDATA[Polyhedron 16, 2291 (1997)]]></dc:source>
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<dc:title><![CDATA[2-[1-(Thiosemicarbazono)ethyl]pyridinium Chloride]]></dc:title>
<dc:source><![CDATA[Acta Cryst. C53, 360 (1997)]]></dc:source>
<dc:date>1997</dc:date>
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