Publications Repository - Helmholtz-Zentrum Dresden-Rossendorf

The surface layer (S-layer) protein genes of the uranium mining waste pile isolate Bacillus sphaericus JG-A12 and of its relative B. sphaericus NCTC 9602 were analyzed. The almost identical N-termini of both S-layer proteins possess a unique structure, comprising three Nterminal S-layer homologous domains (SLH). The central parts of the proteins share a high homology and are related to the S-layer proteins of B. sphaericus CCM 2177 and P-1. In contrast, the C-terminal parts of the studied S-layer proteins differ significantly between each other. Surprisingly, the C-terminal part of the S-layer protein of JG-A12 shares a high identity with that of the S-layer protein of B. sphaericus CCM 2177. In both strains the chromosomal S-layer protein genes were followed by a newly identified putative insertion element comprising three ORFs, which encode a putative transposase, a putative integrase/recombinase, a putative protein containing a DNA binding helix turn helix motif, and the S-layer protein-like gene copies sllA (9602) or sllB (JG-A12). Interestingly, both studied B. sphaericus strains were found to contain an additional, plasmid located and silent S-layer protein gene possessing the same sequence as sllA and sllB. The primary structures of the corresponding putative proteins are almost identical in both strains. The N-terminal and central parts of these S-layer proteins share a high identity with those of the chromosomally encoded functional S-layer proteins. Their C-terminal parts, however, differ significantly. These results strongly suggest that the S-layer protein genes have evolved via horizontal transfer of genetic information followed by DNA rearrangements mediated by mobile elements.

Uranium mining waste piles, heavily polluted with radionuclides and other toxic metals, are a reservoir for bacteria that have evolved special strategies to survive in these extreme environments. Understanding the mechanisms of bacterial adaptation may enable the development of novel bioremediation strategies and other technological applications. Cell isolates of Bacillus sphaericus JG-A12 from a uranium mining waste pile in Germany are able to accumulate high amounts of toxic metals such as U, Cu, Pb, Al, and Cd as well as precious metals. Some of these metals, i.e. U, Cu, Pd(II), Pt(II) and Au(III), are also bound by the highly orderd paracrystalline proteinaceous surface layer (S-layer) that envelopes the cells of this strain. These special capabilities of the cells and the S-layer proteins of B. sphaericus JG-A12 are highly interesting for the clean-up of uranium contaminated waste waters, for the recovery of precious metals from electronic wastes, and for the production of metal nanoclusters. The fabricated nanoparticles are promising for the development of novel catalysts. This work reviews the molecular biology of the S-layer of the strain JG-A12 and the S-layer dependent interactions of the bacterial cells with metals. It presents future perspectives for their application in bioremediation and nanotechnology.

¹⁸F-labeled amino acids represent a promising class of imaging agents in tumors visualized by means of positron emission tomography (PET). Because of the high uptake it is still problematic to clear differentiate between tumors and inflammation.
The high enrichment in tumor tissues assumed the uptake of the tracer via a tumor-specific amino acid transporter, which is not or different expressed in inflammatory cells suggesting a different endowment of neutral amino acids. As previously shown, L-type amino acid transporter 1 (LAT1) is playing a key role because of its high up-regulation in malignant tumors. For the functional expression of LAT1 a single membrane-spanning protein, the heavy chain of 4F2 antigen (4F2hc), essentially forms a heterodimeric complex via disulfide bonds.
The present study investigated the amino acid transport mechanism of LAT1 for 3-O-methyl-6-¹⁸F-Fluoro-L-DOPA (OMFD), a novel ¹⁸F-labeled phenylalanine derivative, into tumor cells.
For molecular characterisation of L-type amino acid transporters focusing on the LAT1-4F2hc subtype we used two different tumor cells like FaDu (squamous cell carcinoma)/HT29 (colorectal adenocarcinoma) and tumor bearing mice performing quantitative RT-PCR, Western-Blot, and immunhistochemistry. In vitro uptake assays with HT29 and FaDu were performed with OMFD under physiological amino acid concentrations.
OMFD demonstrated a saturable and sodium- and energy-independent accumulation in vitro in different tumor cell lines, suggesting its uptake to be mediated exclusively by sodium-independent LAT1.
Our data emphasize the relevance of OMFD as a PET tracer for imaging of specific amino acid transport via LAT1 in tumors. Furthermore, the identification and characterization of tumor specific amino acid transporters like LAT1 will be a helpful tool for therapeutic implications. The inhibition of LAT1 activity in tumor cells could be effective in the inhibition of tumor cell growth by depriving tumor cells of essential amino acids, too.

Hypoxia is a common feature of various human tumor entities. Hypoxic tumor tissue can be studied by nuclear medicine imaging techniques like PET and SPECT. In this study we analyzed in vitro the influence of experimental hypoxia on the radiotracer uptake of various primary endothelial cells, which play an essential part in tumor angiogenesis.
Experimental hypoxia was induced by cultivating cells for 24 hours in presence of 2% oxygen in a special incubator (Gasboy C40, Labotect). Cellular uptake of [99mTc]MIBI, [18F]MISO and [18F]FDG was determined after one or four hours incubation and measured after cell lysis with a gamma counter Cobra II (Perkin Elmer). Radiotracer uptake was normalized to the cell protein. Three types of primary endothelial cells were used: human umbilical vein endothelial cells (HUVEC), human dermal microvascular endothelial cells (HDMEC) and human aortic endothelial cells (HAEC) as well as the two tumor cell lines, being FaDu (squamous cell carcinoma) and HT29 (colorectal adenocarcinoma), respectively. Cellular expression of hypoxia-inducible factor-1a (HIF-1a) and vascular endothelial growth factor (VEGF) was monitored with quantitative PCR (RotorGene 2000).
In our experiments we found that under hypoxic conditions the uptake of [99Tc]MIBI was decreased in all cell types. The uptake of the hypoxia-specific radiotracer [18F]MISO was slightly increased in all primary endothelial cell types. Furthermore, primary endothelial cells incorporated significant higher amounts of [18F]FDG under experimental hypoxic conditions in comparison to normoxic conditions. Especially HDMECs showed a marked response to hypoxia with an approximately two-fold higher [18F]FDG uptake. Also HUVECs and HAECs responded to experimental hypoxia, whereas tumor cell lines FaDu and HT29 showed only moderate increase of [18F]FDG uptake under hypoxic conditions.
We conclude that experimental hypoxia represents a much higher stimulus for primary endothelial cells than for cultivated tumor cells to accumulate [18F]FDG and also to incorporate [18F]MISO in vitro. Our data emphasize the relevance of endothelial cells as one important part of the tumor micromilieu and stimulate further studies on the different patterns of radiotracer uptake in neoplastic or neovascularized lesions.

Aim:

Hypoxia is a common feature of various human tumor entities and the enhanced uptake of specific radiotracers in hypoxic tissues can be visualized by means of positron emission tomography (PET). In this study we analyzed the influence of experimental hypoxia on the [¹⁸F]FDG uptake of various primary endothelial cells and tumor cell lines.
Material and Methods:
Experimental hypoxia was induced by cultivating cells for 24 hours in presence of 2% oxygen in a special incubator (Gasboy C40, Labotect). Cellular [¹⁸F]FDG uptake was determined after one hour incubation and measured after cell lysis with a Cobra II spectrometer (Packard). [¹⁸F]FDG uptake was correlated to protein concentration. Three types of primary endothelial cells were used: human umbilical cord endothelial cells (HUVEC), human dermal microvascular endothelial cells (HDMEC) and human aortic endothelial cells (HAEC) as well as the two tumor cell lines, being FaDu (squamous cell carcinoma) and HT29 (colorectal adenocarcinoma), respectively.
Results:
In our experiments we found that primary endothelial cells incorporate significant higher amounts of [¹⁸F]FDG under experimental hypoxic conditions in comparison to normoxic conditions. Especially HDMECs showed a marked response to hypoxia with an approximately two-fold higher [¹⁸F]FDG uptake. Also HUVECs and HAECs responded to experimental hypoxia, whereas tumor cell lines FaDu and HT29 showed only moderate increase of [¹⁸F]FDG uptake under hypoxic conditions.
Conclusion:
Experimental hypoxia represents a much higher stimulus for primary endothelial cells than for cultivated tumor cells to incorporate [¹⁸F]FDG. Our data emphasize the relevance of endothelial cells as one important part of the tumor micromilieu and stimulate further studies on the different patterns of radiotracer uptake in neoplastic or neovascularized lesions.

During the archaeological work in summer 2000 a spectacular hoard of silver coins could be excavated at the medieval site Becin, next to Ephesos / Turkey. This hoard, whose total weight amounted to approximately 30 kg, includes about 60.000 Islamic coins as well as 830 European coins and represents the largest finding of coins ever made in Turkey. One of the most outstanding features of the Becin hoard is the fact that almost all mint places recorded for the Ottoman Empire and all rulers of the second half of the 16th century up to the beginning of the 17th century are represented in this treasure. Thus, the numismatic evaluation and the material analysis of the coins will provide a general insight in the monetary and economic history of the Ottoman Empire in this time.
In a first step of the investigations a collection of 450 samples was analyzed quantitatively. Photon, electron and proton induced X-ray analysis provide complementary information on the chemical composition of the coins. Using EDXRF, the content of both the major constituent Ag and the minor elements Cu and Pb were determined. The advantage of SEM/EDX is the ability to analyze small areas of the cross-sections. Finally, PIXE measurements were carried out in order to characterize also the trace elements, like Au, Bi, Fe, Ni. The initial results show on the one hand an arrangement in different groups of coins concerning their chemical composition. On the other hand the findings illustrate frequent devaluations in the fineness of the silver coins described in the Ottoman written sources.

The role of hydrogen in hydrogenated amorphous silicon (a-Si:H) has been studied from the viewpoint of its specific contribution to mechanical stress in the material. Hydrogen ion implantation has been used to increase the hydrogen concentration. In order to distinguish the effect of the changed hydrogen concentration/bonding configuration from the accompanying implantation-induced defects, a-Si:H samples with corresponding number of displacements have been studied, created using proper doses of silicon ion implantation. The experimental results have shown that it is the silicon-bonded hydrogen that essentially affects the stress, as the major contribution has its clustered bonding configuration.

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The γ decay of the 12+ yrast trap in 52Fe has been measured for the first time. The two E4 γ-branches to the 8+ states are hindered with respect to other B(E4) reduced transition probabilities measured in the f 7/2 schel. The interpretation of the data is given in the full pf shell model framework, comparing the results obtained with different residual interactions. It is shown that measurements of hexadecapole transition probabilities constitute a powerful tool in discriminationg the correct configurration of the involved wavefunctions.

Die Sorption von Uran (VI) an das komplexe Gestein Phyllit wurde gründlich untersucht. Dominierender Prozess der Sorption ist die Bindung an das Sekundärmaterial Ferrihydrit. Anhand der gewonnenen experimentellen Daten gelang die Bestimmung von Oberflächenkomplexbildungskonstanten für die mineralischen Bestandteile Quarz, Muskovit, Albit und Chlorit. Diese log K-Werte können in chemischen Transportprogrammen Verwendung finden.

Diese Arbeit beschäftigt sich mit der Entfernung von organischen Stoffen aus Wässern durch Anionenaustauscher. Dabei werden C-14-markierte Modellsubstanzen eingesetzt. Die Aufnahme von Durchbruchskurven erfolgt bei verschiedenen Bedingungen (Variation von Beladungstemperatur, Salzgehalt und Organikakonzentration).

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Flash lamp annealing of heteroepitaxial silicon carbide on silicon structures involves melting the silicon below the SiC layer but the facetted nature of the liquid-solid interface leads to unacceptable surface roughness. This paper describes a method of controlling melting by using a melt stop created at a controlled depth below the Si / SiC interface by implanting a high dose of carbon, which significantly increases the silicon melting temperature. Results confirm the effectiveness of the technique in reducing roughness.

Swirling flows generated by the application of a rotating magnetic field (RMF) during the solidification significantly modify the heat and mass transport in the melt. Their enormous potential to modify the microstructure is known since long but was systematically studied only recently [1,2]. However, the understanding of flow field driven by the RMF in the solidifying melt and the corresponding temperature and concentration distributions is far from being complete. By means of a combination of experiments and numerical simulations important relations shall be established.
To calculate the flow field we use a code based on the SIMPLE algorithm which has been carefully validated on the isothermal problem of the RMF-driven acceleration of a melt from rest [3,4]. The solidification is treated by using a mixture-theory-model following Voller et al. [Int. J. Heat Mass Transfer 32 (1989), 1719]. The geometry studied is a Pb-Sn melt in a cylindrical cavity directionally solidified from below. The simulations cover Taylor numbers, Ta, up to 2*106 where Ta determines the magnitude of the bulk flow.
The solidification in the RMF depends on the degree of development of the forced convection (spin-up problem). The flow fields belonging to characteristic stages are discussed. Generally, the RMF significantly modifies the solidification as soon as the average flow velocity of the meridional flow becomes comparable or larger as the velocity of the solidification front. We discuss the impact of the flow on heat transfer in the melt thereby providing a detailed comparison of experimental and numerical date with respect to cooling rates and temperature gradients. Emphasis is given to the temperature gradients in vicinity of the solidication front which are hardly accessible in experiments. Their tendency with growing Ta is examined and linked with the accelerated onset of the transition from columnar to equiaxed growth (CET) found in the experiments [2]. Furthermore the macrosegregation to be expected in the RMF case are discussed.

The application of time varying magnetic fields can be considered as an effective tool to organize a well-defined flow structure in the liquid phase affecting the nucleation and solidification parameters. Main goal of our activities is to elucidate a strategy to control the microstructure of castings by an optimal combination of magnetic field intensity, field frequency and cooling rate. The development of fine, globular grains is preferred. Structures containing textured columnar grains and zones of macrosegregation should be avoided.
Solidification experiments as well as numerical simulations were carried out dealing with Pb Sn alloys solidified directionally from a water cooled copper chill. A rotating magnetic field (RMF) was chosen for melt agitation, because the essential features of an RMF-driven flow have already been intensively investigated for the isothermal case. The magnitude of the bulk flow in the melt generated by the RMF varies with the magnetic Taylor number Ta. The forced convection causes distinct modifications of the temperature and concentration field such as a reduction of the temperature gradient ahead of the solidification front. Without electromagnetic stirring the alloy solidifies solely in form of dendrites aligned parallel to the heat flow direction. In contrast, a transition from a columnar to an equiaxed growth (CET) is observed if the solidifying ingot is exposed to an RMF. The position of the CET is shifted towards the bottom of the casting by increasing the Ta number. The CET was found to occur for a cooling rate of about 0.4 K/s and temperature gradients in the range between 0.6 and 1.0 K/mm
The ultrasound Doppler velocimetry (UDV) was applied to measure the bulk flow during solidification. Our results show that the velocity profiles undergo distinct modifications during solidification indicating the occurrence of more sophisticated flow patterns as known from the isothermal case. Furthermore, the UDV data allow an assessment of the current position of the columnar solidification front.

Bubble driven flows have found wide applications in industrial technologies. In metallurgical processes gas bubbles are injected into a bulk liquid metal to drive the liquid into motion, to homogenize the physical and chemical properties of the melt or to refine the melt. For such gas-liquid metal two-phase flows, external magnetic fields provide a possibility to control the bubble motion in a contactless way.
Compared to the numerous experimental studies on the movement of bubbles in transparent liquids , especially in water, the number of publications dealing with gas bubbles rising in liquid metals is comparatively small. The shortage of suitable measuring techniques can be considered as one reason for the slow progress in the investigations of gas-liquid metal flows. Powerful optical methods are obviously not available for measurements in liquid metals. The majority of measurements in liquid metal two-phase flows published until now was obtained using local conductivity probes, hot wire anemometer or optical fiber probes to determine quantities such as void fraction, bubble and liquid velocity or the bubble size. However, measurements with any local probe disturb the flow in a significant way, especially if the structures to be investigated reach dimensions comparable to the probes. In the case of opaque liquids the application of acoustic or ultrasonic sensors offers a possibility to get information about the flow structure and bubble quantities. We applied the Ultrasound Doppler Velocimetry (UDV) for measurements of the velocity structure in liquid metal bubbly flows. Because of the ability to work non-invasively in opaque fluids and to deliver complete velocity profiles in real time it is very attractive for liquid metal applications.
In our experiments we investigated the consequence of an application of a DC magnetic field on both the bubble and the liquid velocity. The motion of single argon bubbles rising in GaInSn were analyzed in terms of the terminal velocity, the drag coefficient, the oscillation frequency of the bubble velocity and the Strouhal number. Because the gas bubble is electrically non-conducting, it does not experience the effect of the electromagnetic force directly. However, the bubble behaviour is influenced by the magnetically induced modifications in the liquid flow structure around the bubble. The measurements reveal a distinct effect of the magnetic field on the bubble velocity as well as the bubble wake. The magnetic field application leads to a mitigation of the horizontal components of the bubble velocity resulting in a more rectilinear bubble path. A restructuring of the entire flow field can be observed if a bubble plume is exposed to a DC magnetic field. As a result of the interaction between magnetic field and liquid flow electric currents were induced inside the liquid causing a damping of the flow by Joule dissipation. However, a characteristic feature of the electromagnetic dissipation is the anisotropy. Thus, the application of a transverse field leads not only to a general damping of the flow, but also favours the occurrence of vortices aligned parallel to the magnetic field direction.

Bakterien sind winzig klein, sehr leistungsfähig und es gibt keinen noch so extremen Lebensraum, den sie nicht besiedeln könnten. Als wahre Alleskönner liefern sie der Bionik (Verbindung aus Biologie und Technik) viele neue Impulse. Am Beispiel faszinierender Hüllstrukturen verschiedener Bakterien wird dies exemplarisch aufgezeigt.

Nanowires have fascinating properties. Also the kind and strength of driving forces for their structural evolution differ from macroscopic systems, thus opening new routes for their synthesis. And, with respect to interface energy, nanowires are unstable, during their decay new selforganized 1D structures evolve.
This presentation summarizes reaction pathways of the formation and decay of 1D nanostructures predicted by atomistic computer simulations. It will be shown that nanowire synthesis by phase separation from supersaturated 1D traces relies on different time scales of different processes involved: (i) phase separation is faster than long-range diffusion, thus, initially small nanodroplets form. (ii) Short-range diffusion is fast, thus, lateron the minority phase is concentrated/unified to a wire (ripening, coalescence). (iii) On a long time scale, the wire lowers its surface energy by peristaltic undulations and decays finally into large droplets (Rayleigh instability). Each process can be governed in order to fabricated functional structures. For instance, crosspoints of nanowires accelerates the wire instability locally, which leads to a nanodot separated by nm gaps from the four nanowires. Such a Si structure embedded in SiO2 might operate as a room temperature single electron transistor.

Nanowires (NWs) and chains of nanocrystals (NCs) embedded in dielectrics or semiconductors are intensively studied regarding their potential application in nanoelectronics. CoSi2 nanostructures in Si are particularly interesting because of the full compatibility of CoSi2 with CMOS technology.
Here, we present predictive atomistic computer simulations on the ion beam synthesis of CoSi2 NWs in Si and their decay into chains of CoSi2 NCs which are applicable as plasmon waveguides. In order to simulate the Co implantation, the binary collision codes TRIDYN and TRIM were adapted to the particular experimental situation of a finely-focused Co ion beam of 50nm in width. The resulting 3D implantation profile serves as input for a kinetic lattice Monte-Carlo code by means of which nucleation and growth of CoSi2 precipitates and their coalescence into a CoSi2 NW are described. From an evolutionary viewpoint, NW synthesis and decay proceed on different time scales. The NW decay into a NC chain (Rayleigh instability) is driven by the minimization of interfacial free energy. In this regard, it will be demonstrated that the orientation of the Co implantation profile to the single crystalline Si matrix influences the stability of the synthesized CoSi2 NW. Since the system energetically favors the CoSi2(111)/Si(111) interface, driving faceting forces may occur which accelerate the NW decay into a NC chain.

An abstract was not required.

Nanowires (NWs) and chains of nanocrystals (NCs) embedded in dielectrics or semiconductors are intensively studied for photonic and nanoelectronic applications. In this respect, CoSi2 NWs and NC chains are of particular interest because of their full CMOS compatibility, the low damping of surface plasmons at the CoSi2-Si interface, and the transparency of Si at the plasmon frequency.
Here, we present results of atomistic computer simulations which describe the ion beam synthesis of CoSi2 NWs in Si and their thermally activated decay into chains of CoSi2 NCs. The Co implantation is simulated with the binary collision codes TRIDYN and TRIM adapted to the particular experimental situation of a finely focused Co ion beam of a few tens of nanometers in width. The resulting 3D implantation profile serves as input for a kinetic lattice Monte-Carlo code by means of which nucleation and growth of CoSi2 precipitates and their coalescence into a CoSi2 NW are described. From an evolutionary viewpoint, NW synthesis proceeds on a shorter time scale than its decay. The NW decay into a NC chain (Rayleigh instability) is driven by the minimization of interfacial free energy. Moreover, we demonstrate that the orientation of the Co implantation profile to the single crystalline Si matrix strongly influences the stability of the synthesized CoSi2 NW. Since the system energetically favors the CoSi2(111)-Si(111) interface, driving faceting forces may occur which accelerate the NW decay into a NC chain. Thus, intentional misalignment between the focused Co ion beam and the Si substrate is suggested as way to a controlled decay of the ion beam synthesized CoSi2 NW into a chain of monodisperse and equidistant CoSi2 NCs.

An abstract was not required.

Series of carbon steels with various contents of carbon were irradiated with high intensity 5-6 J cm-2, short (µs range) nitrogen and argon plasma pulses. In all samples the near surface layer of the thickness in µm range was melted. The paper reports the results of investigation of changes induced by such treatment. The identified phases, profiles of retained nitrogen concentration, microhardness and wear resistance of the modified layer are presented and discussed.

The experiments to synthesize thin MgB2 inter-metallic compound with the use of ion implantation and plasma pulse treatment are presented. Mg was implanted with 3e18 cm-2 of 80 keV and 5e18 cm-2 of 100 keV B+ ions and next treated with hydrogen and argon plasma pulses of duration of about 1 mu s and fluence between 2 and 4 J/cm2. Superconducting properties were examined by magnetically modulated microwave absorption (MMMA), magnetic moment and electrical conductivity measurements. The structural properties of the implanted and pulse-treated samples were examined by the X-ray diffraction (XRD) and Rutherford backscattering (RBS) methods. The main result consists in observation of MMMA hysteresis loop demonstrating the existence of superconducting regions with T-c as high as 32 K. However, the zero-resistance effect has not been obtained due to incomplete global connectivity between the superconducting regions.

Neutron and gamma field functionals were studied by means of deterministic Sn and stochastic Monte Carlo calculations and by neutron activation measurements that were carried out in the ex-vessel cavity of the VVER-440 reactor Greifswald-1. The paper presents and analyses the results. The influence of different numbers of energy groups for the description of the cross sections is pointed out. A good agreement was found both between the results of deterministic and Monte Carlo calculation and between numerical and measurement results.

Laser-Induced spectroscopic methods were often used in actinide chemistry as tool to study the speciation of these elements in aquatic environments. The main goal of the application of time-resolved laser-induced fluorescence spectroscopy (TRLFS) and laser-induced photoacoustic spectroscopy (LIPAS) is to achieve detection limits of the actinide species as low as possible or in concentration ranges expected under environmental conditions.
With laser sources can it is possible to provide any wavelength from the near UV to the NIR (Near Infrared) wavelength range. The development of tunable solid-state lasers overcame some disadvantages of the dye laser systems as short tunable wavelength range and the use of hazardous chemicals. The application of low temperatures for samples measured with fluorescence spectroscopic methods brought effort especially in the detection of carbonate species.
In this contribution the focus will be mainly on the fluorescence spectroscopy of lower actinides, as it is not possible to include all literature in this field.

The processes of electro- (EL) and photoluminescence (PL) and charge trapping in Er-implanted SiO2 containing silicon nanoclusters have been studied. It is shown that in Er-doped SiO2 with an excess of silicon nanoclusters of 10 at. %, a strong energy transfer from silicon nanoclusters results in a ten-fold increase of the PL peak at 1540 nm from Er luminescent centers, whereas the EL is strongly quenched by the excess silicon nanoclusters. It is further shown that the implantation of Er creates in the oxide positive charge traps with a giant cross section (σ(h0) > 10(-13) cm(2)). Introducing subsequent silicon nanocrystals in the oxide leads to the formation of negative charge traps of a giant cross section (σ(e0) > 10(-13) cm(2)). The possible reason for the EL quenching in the Er-doped SiO2 by silicon nanoclusters is discussed. (C) 2005 American Institute of Physics.

The oxygen concentration in Nd-Fe-B alloy was determined with secondary ion mass spectrometry (SIMS) using Cs+-ions. The SIMS measurements were calibrated with oxygen-implanted single crystals. The depth profile of Nd2Fe14B single crystals displays a 0.5 μ m thick surface layer with elevated oxygen concentration which can be distinguished from the matrix with an oxygen content c(O) = 0.006± 0.002 at%. Polycrystalline samples can exceed this value by far and are sensitive to processing parameters and sample handling. SIMS measurements revealed the oxygen content of the Nd2Fe14B phase considerably lower than the total oxygen content of Nd-Fe-B samples. © 2004 Elsevier B.V. All rights reserved.

The complexation of Cm(III) and Eu(III) with n-C3H7-BTP in non-aqueous organic solution was studied with extended X-ray absorption spectroscopy. Bond lengths are the same in both complexes. Quantum chemical calculations performed at different levels support this finding. On the other hand, the Cm•(n-C3H7-BTP)3 complex is formed at much lower metal-to-ligand concentration ratio than the Eu•(n-C3H7-BTP)3 complex, as shown by time-resolved laser-induced fluorescence spectroscopy. This is in good agreement with n-C3H7-BTP’s high selectivity for trivalent actinides over lanthanides in liquid-liquid extraction.

Electromagnetic processing comprises the influence of Lorentz forces in the molten state. Whereas the action of static magnetic fields is solely damping in most cases, alternating fields offer the potentiality of active control mechanisms such as pumping, stirring, homogenization, and the like. Among the latter, various field types have to be distinguished based on the number of poles and geometric arrangement. Neither for one type, and more than ever for a combination thereof, might the resulting flow tagged well known.
Numerous, often non-validated numerical simulations overwhelm the few experiments done on liquid metals. In the present work, the ultrasonic Doppler velocimetry (UDV) and local potential probes have been employed to study the flow of an alloy in single-phase, traveling, and rotating fields. The area-wide results conveyed by the UDV technique will be presented as flow visualization whereas potential probe measurements may answer questions of more quantitative nature regarding turbulence characteristics.

At the experimental carbon ion tumour therapy facility at GSI Darmstadt, in-beam positron emissions tomography (PET) is used to monitor the dose delivery precision. A dual head positron camera has been assembled from commercial detector components in order to measure the β+-activity, induced by the irradiation, simultaneously to the dose application. Despite the positive clinical impact, the image quality is limited by the low counting statistics, orders of magnitude below that in standart PET applications to nuclear medicine. This paper investigates the origin for the noisy acquisition during particle extraction from the synchrottron of GSI. The results demonstrate the failure of standard random correction techniques due to a γ-ray background correlated in time with the carbon ion beam microstructure. This prevents the use of data acquired during beam extraction for imaging. The loss of counting statistics is expected to rise further at the future hospital-based facility at Heidelberg, due to a more efficient utilisation of the accelerator resulting in shorter beam pauses and a reduced treatment time. In respect, this paper provides the basis for a new data acquísition concept tailored to the unconventional application of in-beam PET imaging to therapy monitoring at radiofrequency pulsed radiation sources.

The subjects of electromagnetic flow control and ship propulsion are reviewed, and possibilities for further developments are sketched.

The possibilities for local velocity measurements in liquid metal flows are reviewed. Special emphasis is put on local potential probes and the ultrasonic velocimetry.

Ausgehend von den physikochemischen Grundlagen der Grignard-Chemie werden Einflussfaktoren für eine sichere Prozessführung beschrieben. Bei Grignard-Synthesen tritt das größte Gefahrenpotential in der ersten Reaktionsstufe, der Herstellung der Grignard-Reagenz, auf. Insbesondere muss das Anspringen der Reaktion bei einer unzulässig großen Akkumulation von organischem Halogenid verhindert werden, wenn keine ausreichende, schnell wirksam werdende Kühlleistungsreserve vorhanden ist.
Vor der Überführung einer neuen Grignard-Synthese in den großtechnischen Maßstab sollten umfassende Untersuchungen der Grignard-Reaktionsstufe in Laborreaktoren durchgeführt werden. Mit Hilfe isothermer und adiabatischer kalorimetrischer Messungen konnten die wichtigsten Prozessparameter, wie molare Reaktionsenthalpie, adiabatische Temperaturerhöhung, Induktionszeit, Anstiegsgeschwindigkeit der Wärmeleistung und Dauer der Startphase, ermittelt werden. Sie sind notwendig, um die maximal zulässige Akkumulation des organischen Halogenids für die verfügbare Kühlleistung der Produktionsanlage bestimmen zu können.
Die Untersuchungen zeigten, dass gleiche Werte der molaren Reaktionsenthalpie sowohl bei isothermer als auch adiabatischer Kalorimetrie gemessen wurden. Als Ursache für die gemessenen größeren Enthalpiewerte während der isotherme Startreaktionsphase konnten noch vorhandene Wasser-Restmengen identifiziert werden, die infolge ihrer exothermen Folgereaktion mit der gebildeten Grignard-Reagenz einen zusätzlichen Wärmebeitrag lieferten. Eine Temperaturabhängigkeit der molaren Reaktionsenthalpie konnte im Temperaturbereich von 25°C bis 120°C nicht festgestellt werden.
Um subjektive Fehleinschätzungen des Anspringens der Grignard-Reaktion zu vermeiden, wurden die Anwendungsmöglichkeiten verschiedener Messmethoden zur Online-Überwachung getestet. Mit der in situ-Infrarotspektroskopie ließ sich das Anspringen der Grignard-Reaktion eindeutig und empfindlich detektieren. Ebenso könnte das spätere Einschlafen der Reaktion infolge zudosierter oder eindringender Verunreinigungen erkannt werden. Das Leistungsvermögen der Stoff- und Energiebilanzen als Methode zur Online-Überwachung konnte sowohl für die Startphase als auch für die Hauptreaktionsphase im Vergleich mit der Infrarotspektroskopie nachgewiesen werden. Die Wärmebilanzierung liefert eine viel versprechende Alternative zur in situ-Infrarotspektroskopie für den Einsatz an Produktionsanlagen, weil sie mit einer ausreichend empfindlichen Betriebsmesstechnik realisiert werden kann, quasi im Echtzeitbetrieb arbeitet und wesentlich kostengünstiger ist. Der Vorteil der in situ-Infrarotspektroskopie ist die parallele Online-Messung von störenden Wasseranteilen im Reaktionsmedium. Beispielsweise könnte das Nichtstarten der Grignard-Reaktion aufgrund von zu großen Wasserrestmengen in der Mehrzweckanlage erkannt werden. Durch geeignete Sicherheitsmaßnahmen und Sicherheitsverriegelungen sollte die Überdosierung von organischem Halogenid und das Eindringen stark exothermer Verunreinigungen (wie z. B. Wasser) während der ersten Grignard-Reaktionsstufe unbedingt verhindert werden. Aus Sicherheitsgründen sollte Wasser durch Öl als Kühlmedium möglichst ersetzt werden.

The impact of organic matter on the migration of actinides in argillaceous media is relevant for the risk assessment of future nuclear waste repositories. The diffusion of a 14C-labelled synthetic humic acid in compacted Georgia kaolinite and its influence on the uranium(VI) migration was studied.
The migration of humic acid in clay is governed by diffusion. The colloidal properties of humic acid result in a size exclusion from small pores. Thus the accessible pore space decreases and the tortuosity of the diffusion path increases compared to a conservative tracer. Furthermore, the compacted clay filters large humic colloids. Both effects restrict the diffusive flux of humic acid in the clay.
Diffusion experiments on the time scale of several weeks could not demonstrate a humic colloid-borne migration of uranium(VI) in the clay system. The competition of the humate and surface binding sites for uranium as well as the kinetics and reversibility of the complexation govern the actinide migration in this system.

We propose scanning near-field optical microscopy as a novel technique for characterizing the ion-implanted patterns fabricated in amorphous silicon carbide (a-SiC:H). Different patterns have been fabricated in a-SiC:H films with a focused Ga+-ion beam system and examined with scanning near-field optical microscopy and atomic force microscopy. Although a considerable thickness change (thinning tendency) has been observed in the ion-irradiated areas, the near-field measurements confirm increases of optical absorption in these areas. The observed values of the optical contrast modulation are sufficient to justify the efficiency of the method for optical data recording using focused ion beams.

Optical patterns as small as 200nm width have been fabricated in a thin film of amorphous silicon carbide (a–SiC:H)using a focused ion beam microscope, (FIB). Because of the low electric conductivity of a–SiC:H, the diameter of the writing ion beam is broadened by the effect of surface charging which was overcome by depositing a thin layer of gold onto the a–SiC:H film. The topographic and optical contrasts of the patterned thin films have been mapped with
scanning near-field optical microscopy. The optical contrast corresponding to nanostructures is 0.2 with an overall increase of the optical density contrast of 0.5 in the irradiated areas. The results of the fabrication of patterns created with FIB on aluminium-coated a-SiC:H films are also briefly presented.

The write performance of a multidot memory is investigated in MOS (metal-oxide-semiconductor) capacitors. The oxide of the MOS structure on p-type Si contains a layer of ion beam synthesized Ge nanocrystals (NC's) very close to the Si/SiO2 interface. This structure is modeled in a floating gate-like approach, where the NC's are considered as individual storage nodes and charged by direct tunneling of holes. Quantum confinement and Coulomb blockade effects of small Ge NC's (1-6 nm) are discussed and found to be negligible for the present structure. A close agreement between the calculated write characteristics and experimental data clearly confirms the validity of the model. From the simulation results it is predicted that a flatband voltage shift ΔVfb = -1V could be gathered with programming times tprog < 1µs. The write parameters (pulse voltage and duration) for a given ΔVfb value are mainly determined by the distance of the NCs' to the substrate.

The nanostructural evolution during heat treatments of DC magnetron-sputtered Ag films, deposited at room temperature at different substrate bias voltages, was experimentally studied. A growth chamber equipped with a magnetron and Kapton windows for in-situ x-ray diffraction was mounted on a six circle goniometer at a synchrotron beam line. Bragg-Brentano x-ray diffraction was used to monitor the (111) Bragg peak during thermal annealing of the Ag films. In addition, to investigate the <111> fiber texture one-dimensional pole figures were measured ex situ. The thermal stability of the nanostructure was sensitively dependent on the substrate bias voltage. Increasing the bias voltage resulted in significantly lower rates of grain growth, which we ascribe mainly to the formation of Ar bubbles. Furthermore, the grain size in the as-deposited films decreased with increasing bias voltage while the width of the one-dimensional pole figures increased.

Abstract wird nachgereicht

Gamma and neutron flux spectra were measured inside and behind various combined iron, steel and water slabs, which were set up in the radial beams of the zero-power training and research reactors AKR of the Technical University Dresden and ZLFR of the University of Applied Sciences Zittau/Görlitz. The measurements were carried out with a liquid NE-213 scintillation spectrometer in the energy ranges 0.23-10 MeV for photons and 1-20 MeV for neutrons. These experiments were simulated with help of the Monte Carlo transport codes MCNP-4C2 and TRAMO. With MCNP the energy point-wise representation of the nuclear data from ENDF/B-VI library, release 8, was used but with TRAMO effective group cross sections prepared by means of NJOY from the same data library. The paper describes the experiments and calculations and exemplarily presents and compares some results.

Bio-activation of titanium surface by Na plasma immersion ion implantation and deposition (Pllf&D) is illustrated by precipitation of calcium phosphate and cell culture. The bioactivity of the plasma-implanted titanium is compared to that of the untreated. Na beam-line implanted and NaOH-treated titanium samples. Our data show that the samples can be classified into two groups: non-bioactive (untreated titanium and beam-line Na implanted titanium) and bioactive (Na-PIII&D and NaOH-treated titanium). None of the four types of surfaces exhibited major cell toxicity as determined by lactate dehydrogenase (LDH) release. However. the LDH release was higher oil the more bioactive PIII and NaOH-treated surfaces. From a morphological point of view, cell adherence on the NaOH-treated titanium is the best. On the other hand, the cell activity and protein production were higher on the non-bioactive surfaces. The high alkaline phosphatase activity per cell Suggests that the active surfa! ces support an osteogenic differentiation of the bone marrow cells at the expense of lower proliferation. The use of Na-PIII&D provides an environmentally cleaner technology to improve the bioactivity of Ti compared to conventional wet chemical processes. The technique is also particularly useful for the uniform and conformal treatment of medical implants that typically possess an irregular shape and are difficult to treat by conventional ion beam techniques. (c) 2005 Elsevier Ltd. All rights reserved.

We report on the fermosecond time-resolved detection of coherent phonons in single-crystal tellurium. For different crystallographic faces a detection scheme is employed which is sensitive to the anisotropic part of the Raman tensor. In this scheme we observe all three Raman allowed phonons, i.e. one of A(1) and two of E symmetry. Furthermore, for both doubly degenerate E-symmetry modes obtained from different crystallographic faces, longitudinal optical-transverse optical splitting is observed. In addition, we show that even in the low fluence regime the frequency of the fully symmetric phonon in Te is chirped and that it demonstrates an anomalous dependence on the pump fluence.

The IBR-2 is a small fast reactor with plutonium oxide fuel and liquid sodium cooling. A ro-tating two-reflector system periodically closes and opens a non-reflected side of the reactor and leads it through the prompt super critical state in a time of about 500 microseconds. During this time a burst of fast neutrons is generated in the core of the reactor, which spreads out through moderators. Channels lead the neutrons to measurement instruments.
Certain reactivity parameters of the rotating reflector system determine essential parameters of the reactor as a pulsed neutron source. Just now a new reflector system, the so-called PO-3, has been installed. For this reason the important reactivity effects of the reflector were newly calcu-lated with help of the MCNP-4C2 code. The contribution presents numerical results, which were obtained in different ways and compares results of calculations and measurements. The special in-terest consisted in studying the effect of neglecting the fission source effect, as assumed by the PERT option of the code, on the calculation results. The comparison of numerical with measure-ment results showed agreements in some cases but also considerable discrepancies, which could not yet be explained. Therefore, no final conclusion on the applicability of the PERT method for the calculation of total and displacement reactivity effects of the rotating reflector system of the IBR-2 reactor could be drawn.

2D simulations of isothermal liquid-liquid mass transfer subject to surface tension and buoyancy driven hydrodynamic instabilities have been carried out. Simulation is based on the numerical solution of two-dimensional equations of momentum and mass transport, using a combination of finite difference and finite volume methods. Two different cases have been considered: (1) buoyancy stable mass transfer, only surface tension driven convection occurs; (2) surface tension driven instability superseeded by buoyant convection. The faster attenuation of mass transfer coefficients in buoyancy stable situations is attributed to the merging of convection cells leading to a reduction in the number of renewal zones along the interface. Concentration profiles next to the interface reveal the diffusional nature of the mass transfer.

It could be shown that both, the introduction of a melt stop layer as well as the introduction of a layer with reduced melting temperature are usefull methods for the homogenisation of the melting depth at the bulk silicon surface in FLASIC structures.

Wir wollen auf diese Weise äußerst stabile Stabile Komplexe darstellen in denen Re perfekt eingekapselt ist. Ein aktives Zentrum in der Brücke soll eine gerichtete WW zum Re ausbilden und die Komplexe zusätzlich stabilisieren.

CFD pre-calculations have been performed for the themalhydraulic benchmark V1000CT-2.
The numerical grid model was generated with the grid generator IC4C (ICEM-CFD) and the preprocessor CFX-5 and contains 4.7 Mio. tetrahedral elements.The output of the Best Practice Guidelines for optimizing the numerical studies in different reactor types was used in the numerical simulation. The agreement with the Kozloduy experiment at the core inlet is very good. The results show a clear sector formation of the affected loop at the downcomer, lower plenum and core inlet. The maximum local values of the relative temperature rise in the experiment amount 97.7% and in the calculation 97.4%.

Transient CFD calculations have been performed for the thermal-hydraulic benchmark V1000CT-1, exercise 3
The numerical grid model was generated with the grid generator IC4C (ICEM-CFD) and the preprocessor CFX-5 and contains 4.7 Mio. tetrahedral elements. The output of the Best Practice Guidelines for optimizing the numerical studies in different reactor types was used in the numerical simulation. Data from a coupled code calculation with DYN3D/ATHLET were used as inlet boundary conditions. 4 different Mixing Scalars were utilized to obtain information about the contribution of each loop during the transient. The results show a clear sector formation of the affected loops at the downcomer and core inlet. At the beginning of the start-up of loop 3 the sectors of loop 1,2,4 cover a bigger area.

The plug flow was simulated with a transient CFD simulation in the horizontal channel using time dependent inlet boundary conditions. The qualitative structure of the simulated slug front and tail are similar to the experiment, while the slug length is increasing in the calculation and remains constant in the experiment. The slug propagation velocities are in good agreement.

The project was aimed at describing the mixing phenomena relevant for both safety analysis, particularly in steam line break and boron dilution scenarios, and mixing phenomena of interest for economical operation and the structural integrity. Measurement data from a set of mixing experiments, gained by using advanced measurement techniques with enhanced resolution in time and space help to improve the basic understanding of turbulent mixing and to provide data for Computational Fluid Dynamics (CFD) code validation. Slug mixing tests simulating the start-up of the first main circulation pump are performed with two 1:5 scaled facilities: The Rossendorf coolant mixing model ROCOM and the VATTENFALL test facility, modelling a German Konvoi type and a Westinghouse type three-loop PWR, respectively. Additional data on slug mixing in a VVER-1000 type reactor gained at a 1:5 scaled metal mock-up at EDO Gidropress are provided. Experimental results on mixing of fluids with density differences obtained at ROCOM and the FORTUM PTS test facility are made available.
Concerning mixing phenomena of interest for operational issues and thermal fatigue, flow distribution data available from commissioning tests (Sizewell-B for PWRs, Loviisa and Paks for VVERs) are used together with the data from the ROCOM facility as a basis for the flow distribution studies. The test matrix on flow distribution and steady state mixing performed at ROCOM comprises experiments with various combinations of running pumps and various mass flow rates in the working loops.
Computational fluid dynamics calculations are accomplished for selected experiments with two different CFD codes (CFX-5, FLUENT). Best practice guidelines (BPG) are applied in all CFD work when choosing computational grid, time step, turbulence models, modelling of internal geometry, boundary conditions, numerical schemes and convergence criteria. The BPG contain a set of systematic procedures for quantifying and reducing numerical errors. The knowledge of these numerical errors is a prerequisite for the proper judgement of model errors. The strategy of code validation based on the BPG and a matrix of CFD code validation calculations have been elaborated. Besides of the benchmark cases, additional experiments were calculated by new partners and observers, joining the project later.
Based on the “best practice solutions”, conclusions on the applicability of CFD for turbulent mixing problems in PWR were drawn and recommendations on CFD modelling were given. The high importance of proper grid generation was outlined. In general, second order discretization schemes should be used to minimise numerical diffusion. First order schemes can provide physically wrong results. With optimised “production meshes” reasonable results were obtained, but due to the complex geometry of the flow domains, no fully grid independent solutions were achieved. Therefore, with respect to turbulence models, no final conclusions can be given. However, first order turbulence models like K-e or SST K-w are suitable for momentum driven slug mixing. For buoyancy driven mixing (PTS scenarios), Reynolds stress models provide better results.

The flow distribution in the primary circuit of the pressurized water reactor was studied with experiments and Computational Fluid Dynamics (CFD) simulations. The main focus was on the flow field and mixing in the downcomer of the pressure vessel: how the different factors like the orientation of operating loops, the total loop flow rate and the asymmetry of the loop flow rates affect the outcome. In addition to the flow field studies the overall applicability of CFD methods for primary circuit thermal-hydraulic analysis was evaluated based on the CFD simulations of the mixing experiments of the ROCOM (Rossendorf Coolant Mixing Model) test facility and the mixing experiments of the Paks NPP.
The experimental part of the work in work package 3 included series of steady state mixing experiments with the ROCOM test facility and the publication of results of Paks VVER-440 NPP thermal mixing experiments. The ROCOM test facility models a 4-loop KONVOI type reactor. In the steady-state mixing experiments the velocity field in the downcomer was measured using laser Doppler anemometry and the concentration of the tracer solution fed from one loop was measured at the downcomer and at the core inlet plane. The varied parameters were the number and orientation of the operating loops, the total flow rate and the (asymmetric) flow rate of individual loops.
The Paks NPP thermal mixing experiments took place during commissioning tests of replaced steam generator safety valves in 1987-1989. It was assumed that in the reactor vessels of Paks VVER-440 NPP equipped with six loops the mixing of the coolant is not ideal. For the realistic determination of the active core inlet temperature field for the transients and accidents associated with different level temperature asymmetry a set of mixing factors were determined. Based on data from the online core monitoring system and a separate mathematical model the mixing factors for loop flows at the core inlet were determined.

In the numerical simulation part of the work package 3 the detailed measurements of ROCOM tests were used for the validation of CFD methods for primary circuit studies. The selected steady state mixing experiments were simulated with CFD codes CFX-4, CFX-5 and FLUENT. The velocity field in the downcomer and the mixing of the scalar were compared between CFD simulations and experiments. The CFD simulations of full scale PWR included the simulation of Paks VVER-440 mixing experiment and the simulation of Loviisa VVER-440 downcomer flow field. In the simulations of Paks experiments the experimental and simulated concentration field at the core inlet were compared and conclusions made concerning the results overall and the VVER-440 specific geometry modelling aspects like how to model the perforated elliptic bottom plate and what is the effect of the cold leg bends to the flow field entering to the downcomer. With Loviisa simulations the qualitative comparison was made against the original commissioning experiments but the emphasis was on the CFD method validation and testing.

The overall conclusion concerning the CFD modelling of the flow field and mixing in the PWR primary circuit could be that the current computation capacity and physical models also in commercial codes is beginning to be sufficient for simulations giving reliable and useful results for many real primary circuit applications. However the misuse of CFD methods is easy, and the general as well as the nuclear power specific modelling guidelines should be followed when the CFD simulations are made.

The goal of the work described in this report was the experimental investigation of the mixing of coolant with different quality (temperature, boron concentration) in nuclear reactors on the way from the cold leg through the downcomer and lower plenum to the core inlet in a systematic way. The obtained data were used for the clarification of the mixing mechanisms and form a data basis for the validation of computational fluid dynamics (CFD) codes.
For these purposes, experiments on slug mixing have been performed at two test facilities, modelling different reactor types in scale 1:5, the Rossendorf and Vattenfall test facilities. The corresponding accident scenario is the start-up of first main coolant pump (MCP) after formation of a slug of lower borated water during the reflux-condenser mode phase of a small break loss of coolant accident (LOCA). The matrices for the experiments were elaborated on the basis of the key phenomena, being responsible for the coolant mixing during pump start-up. Slug mixing tests have also been performed at the VVER-1000 facility of EDO Gidropress to meet the specifics of this reactor type.
The mixing of slugs of water of different quality is also very important for pre-stressed thermal shock (PTS) situations. In emergency core cooling (ECC) situations after a LOCA, cold ECC water is injected into the hot water in the cold leg and downcomer. Due to the large temperature differences, thermal shocks are induced at the reactor pressure vessel (RPV) wall. Temperature distributions near the wall and temperature gradients in time are important to be known for the assessment of thermal stresses.
One of the important phenomena in connection with PTS is thermal stratification, a flow condition with a vertical temperature profile in a horizontal pipe. Due to the fluctuating character of the flow, this may cause thermal fatigue in the pipe. Besides of thermal fatigue, a single thermal shock can also be relevant for structural integrity, if it is large enough, especially in the case, that the brittle fracture temperature of the RPV material is reduced due to radiation embrittlement. Therefore, additional to the investigations of slug mixing during re-start of coolant circulation, the mixing of slugs or streams of water with higher density with the ambient fluid in the RPV was investigated. The aim of these investigations was to study the process of turbulent mixing under the influence of buoyancy forces caused by the temperature differences. Heat transfer to the wall and thermal conductivity in the wall material have not been considered.
Experiments on density driven mixing were carried out at the Rossendorf and the Fortum PTS facilities.

We discuss the coaxial power input in normal and superconducting RF (SRF) photoinjector cavities. Upstream coaxial power input has been previously used at the PITZ facility where the output beam tube is an intrinsic part of the coaxial transmission line into the gun. In this paper, we describe coaxial coupling from the cathode side of the gun. For normal conducting RF guns, in addition to the advantage from symmetric coupling, an emittance compensation solenoid can now be positioned close to the gun cavity to deliver optimal transverse emittance. Beam dynamics calculations demonstrate 0.8 mm-mrad at 1 nC in X-band. For an SRF gun, we present a design for coaxial input around the cathode using a superconducting coupling cell. This cell matches the external quality factor of the gun for different beam powers and there is no RF loss associated with the axial gap of the cathode. The heat input into the coaxial feed and the surface field of the coupler are discussed. For a 1.3 GHz half-cell gun cavity with stored energy of 6.6 J, a 2.5 MeV electron beam can be delivered with a peak accelerating field of 50 MV/m. At 10 mA, the external Q is 2.1 x 106 and the coaxial line power loss that must be cooled is 28 W.

The spectra of self-adjoint operators in Krein spaces are known to possess real sectors as well as sectors of pair-wise complex conjugate eigenvalues. Transitions from one spectral sector to the other are a rather generic feature and they usually occur at exceptional points of square root branching type. For certain parameter configurations two or more such exceptional points may happen to coalesce and to form a higher order branch point. We study the coalescence of two square root branch points semi-analytically for a PT-symmetric 4×4 matrix toy model and illustrate numerically its occurrence in the spectrum of the 2×2 operator matrix of the magnetohydrodynamic α²-dynamo and of an extended version of the hydrodynamic Squire equation.

The long history of laboratory experiments on homogeneous dynamo action is delineated. It is worked out what sort of insight can be expected from experiments, and what not. Special focus is laid on the principle and the main results of the Riga dynamo experiment which is shown to represent a genuine hydromagnetic dynamo with a non-trivial saturation mechanism that relies mainly on the fluidity of the electrically conducting medium.

Strongly decreasing atmospheric emissions and acidic depositions during the 1990s have caused a chemical reversal from acidification in several drinking-water reservoirs of the Ore Mountains, SE Germany. Responses of phytoplankton, zooplankton, and fish stock were studied in five reservoirs and in enclosure scale where a water body of 1,200 m3 was experimentally neutralized by application of a new buffering substance. Three months after this treatment, the dominating chrysophytes and dinoflagellates were substituted by diatoms and cryptomonades. The colonization by acidic-sensitive species of green algae, cryptomonades, rotifers, and Cladocera (e.g. Bosmina longirostris) is explained by the occurrence of dormant stages or by survival of individuals in very low abundances. In conformity with the enclosure experiment, three reservoirs showed significantly (p<0.01) falling trends of chlorophyll a and phytoplankton biovolume, mainly due to the decline of dinoflagellates. Picoplankton and diatoms slightly increased in two reservoirs. The zooplankton biocoenosis was dominated by rotifers and small cladocera, the genus Daphnia was still lacking. Two reservoirs were re-colonized by zooplanktivorous fish populations of either perch (Perca fluviatilis) or sunbleak (Leucaspius delineatus). The latter exhibited extremely high fluctuating abundance and biomass and even suffered from a population crash. This natural mortality was caused by limited food supply. Hence, severe top-down control may delay the recovery of bigger zooplankton species like daphnids. Fishery management comprising the introduction of predatory fishes could help to control zooplanktivorous fish populations and to prevent their mass mortality.

Radioactive isotopes are uniquely applicable to observe reactions or circuits of reactions at the molecular level without disturbing the system being studied. The advent of molecular imaging modalities, particularly positron emission tomography (PET), is a major breakthrough for the visualisation and quantitative assessment of cellular and molecular processes occurring in living tissues. The recent development of animal PET scanners that offers 2-mm resolution and is tailored to laboratory rodents, has made a further great impact on in vivo biochemistry. With these live-imaging modalities at hand, radiotracer-based technologies allow to look directly at biochemical distribution and interaction processes. Tremendous progress made in radiotracer chemistry, primarily in carbon-11 and fluorine-18 radiochemistry, and in the design of imaging devices strengthens the usefulness of radiotracers in nuclear medicine and drug research and development and opens exciting opportunities for new applications, e.g. in food science.

Due to recent progress in crystal growth and unique optical and electrical properties ZnO becomes a prospective material for use in optoelectronic devices. ZnO thin films have been prepared at unheated glass substrates by reactive DC magnetron sputtering. The oxygen fraction in Ar + O2 gas mixture was varied from 0 to approximately 83%. The films have been characterized by spectroscopic ellipsometry (SE), atomic force microscopy (AFM) and X-ray diffraction (XRD). The dielectric function of ZnO layers was parameterized using Drude-Lorentz oscillator. As shown by SE, the dielectric functions of the films prepared at low oxygen fraction are characteristic for cermet materials (mixture of oxide and metal particles). XRD confirms the presence of both ZnO and metallic Zn phases in these films. The layers produced at high oxygen fractions (above 60%) are insulating and their dielectric functions can be reasonably described by Lorentz oscillator alone. Importantly, that the latter films are polycrystalline with pronounced (002) type texture even at a thickness of only 50 nm. The XRD results point to a high mechanical stress in these films that can be related to the bombardment by negative oxygen ions during the film growth.
ZnO films prepared at medium oxygen fraction of 48% were annealed in vacuum at about 340 °C for 1.5 hour with in situ control of optical properties by SE and resistivity by two point probe measurement. The influence of the structural ordering during annealing on the refractive index is higher than the free electron density variation. An enhancement of the film resistivity at the final annealing stage (last 40 min) with concomitant decrease of the free electron concentration could be an indication of the acceptor-like defect formation.

Intersubband optical transitions at short wavelengths in strain-compensated In0.70Ga0.30As—AlAs double quantum wells are investigated by means of mid-infrared absorption. Trade-offs between achieving a high transition energy and a large oscillator strength of the two highest-energy intersubband transitions using our strain-compensation approach are analyzed as a function of the widths of the two wells. Two design strategies leading to relatively strong intersubband optical transitions at 800 meV, 1.55 µm, are described and the corresponding structures grown using gas-source molecular-beam epitaxy on (001)InP are investigated. The strongest intersubband transitions obtained experimentally are generally between 300 and 600 meV, 2–4 µm. Significant oscillator strength, however, also extends out to 800 meV, 1.55 µm.

Thema: Entwicklung und Testung einer neuen Klasse hybrider keramischen Funktionswerkstoffe (Biocere), die als schwermetallbindende Filtermaterialien oder als Immobilisierungsmatrix für lebende Zellen in der Umwelt- und Biotechnologie genutzt werden können.

The paper report about spatial dynamics studies of the Molten Salt Reactors (MSR). MSR is one of the concepts considered within the 'Generation IV International Forum'. The graphite-moderated channel type MSR based on the previous Oak Ridge National Laboratory (ORNL) research is considered.
The physical models and numerical solution procedures used in the dynamics code DYN3D-MSR are described. The most relevant peculiarities in MSR dynamics are the delayed neutrons precursors drift with the flowing fuel and the direct release of fission energy into the fuel-coolant salt. The code is based on the in-house developed code DYN3D for Light Water Reactor, which solves two-group neutron diffusion equations by the help of a nodal expansion method. The same method for prompt neutron kinetics is used in DYN3D-MSR, but the appropriate models for the delayed neutrons and for the thermal-hydraulic have been integrated.
The code has been validated against experimental data gained from the Molten Salt Reactor Experiment (MSRE), performed in the ORNL. After successful validation, the code DYN3D-MSR was applied to the analysis of several hypothetical transients typical for liquid fuel systems. Particularly, a prompt reactivity insertion modeling a control rod ejection accident was analyzed. By performing these analyses, the DYN3D-MSR code has been shown to be an effective tool for MSR dynamics studies.

Ni-Ti thin films as-sputtered are amorphous if the substrate is not intentionally heated during deposition. Therefore, these films have to be heat-treated to induce crystallization in order to exhibit the shape memory effect. Several films have been prepared by dc magnetron sputtering and then studied concerning the influence of the type of substrate (single crystal Si, polycrystalline Si) on the crystallization kinetics and the final structure. The structural development of the films during crystallization (at a constant temperature of 430°C) has been studied by X-ray diffraction in grazing incidence geometry (GID) off-plane at a synchrotron radiation beamline. These experiments allow to establish a correlation between the deposition conditions and the kinetics of crystallization. For films deposited at an electrode distance of 70 mm on a Si(100) substrate, a longer crystallization time is needed compared with films obtained at 40 mm, for otherwise fixed deposition parameters. The analysis of the nucleation kinetics by using the Kolmogorov-Johson-Mehl-Avrami equation lead to exponents between 2.6 and 3. The presence of an intermediate layer of poly-Si drastically enhances the crystallization process. Additionally, ex-situ annealing of identical samples at 500°C during 1 hour and complementary characterization of the structure and morphology of the films by Cross-sectional Transmission Electron Microscopy (XTEM) and Selected Area Electron Diffraction (SAED) were performed. The temperature dependence of the electrical resistivity was measured, identifying the phase transformation temperature ranges. An increase of the overall resistivity with the precipitation of Ni4Ti3 has been detected. Results obtained by X-ray reflectometry (XRR) and GID suggest that during crystallization excess nickel is driven into an amorphous region ahead of the crystal/amorphous interface, thus leading to a higher concentration of Ni at the surface and further precipitation of Ni4Ti3. t the shape memory effect. Several films have been prepared by dc magnetron sputtering and then studied concerning the influence of the type of substrate (single crystal Si, polycrystalline Si) on the crystallization kinetics and the final structure. The structural development of the films during crystallization (at a constant temperature of 430°C) has been studied by X-ray diffraction in grazing incidence geometry (GID) off-plane at a synchrotron radiation beamline. These experiments allow to establish a correlation between the deposition conditions and the kinetics of crystallization. For films deposited at an electrode distance of 70 mm on a Si(100) substrate, a longer crystallization time is needed compared with films obtained at 40 mm, for otherwise fixed deposition parameters. The analysis of the nucleation kinetics by using the Kolmogorov-Johson-Mehl-Avrami equation lead to exponents between 2.6 and 3. The presence of an intermediate layer of poly-Si drastically enhances the crystallization process. Additionally, ex-situ annealing of identical samples at 500°C during 1 hour and complementary characterization of the structure and morphology of the films by Cross-sectional Transmission Electron Microscopy (XTEM) and Selected Area Electron Diffraction (SAED) were performed. The temperature dependence of the electrical resistivity was measured, identifying the phase transformation temperature ranges. An increase of the overall resistivity with the precipitation of Ni4Ti3 has been detected. Results obtained by X-ray reflectometry (XRR) and GID suggest that during crystallization excess nickel is driven into an amorphous region ahead of the crystal/amorphous interface, thus leading to a higher concentration of Ni at the surface and further precipitation of Ni4Ti3.

The electrical properties of heavily Al doped single and nanocrystalline 4H-SiC layers on semi-insulating 4H-SiC substrate, prepared by multi-energy, high-fluence Al implantation and subsequent furnace annealing, are investigated by sheet resistance and Hall effect measurements. Ion beam induced crystallization is used to prepare the nanocrystalline SiC layers. The doping levels are chosen around the solid solubility limit of 2x1020 cm-3 in the range from 5x1019 to 1.5x1021 cm-3. The comparison of the results shows that heavily Al doped single crystalline SiC layers have superior conduction properties. The lowest resistivities measured at room temperature are 0.07 Ohm-cm and 0.8 Ohm-cm for the single crystalline and nanocrystalline samples, respectively. Recent results on enhanced Al acceptor activation in nanocrystalline SiC cannot be confirmed. There is an upper limit for the hole concentration in the nanocrystalline samples independent of the Al supersaturation level in the as-implanted state due to outdiffusion of Al in excess to the solid solubility limit during annealing. In contrast to the nanocrystalline SiC layers the as-implanted Al profile in single crystalline material remains stable after annealing even for concentrations above the solid solubility limit. Therefore, in single crystalline material efficient impurity band conduction due to strongly interacting acceptors can be achieved in the range of supersaturation. For lower doping levels impurity band conduction is more effective in nanocrystalline SiC.

Since high-k insulators appear more and more to be preferable to SiO2 in semiconductor technology, Ge is again becoming of increasing interest, since its carrier mobility is higher than that of Si. Atomistic simulations are a powerful tool to investigate atomic-level physics and to get a better understanding of the processes during the technological steps in integrated electronic device manufacturing.
In the present work different interatomic potentials for Ge are evaluated with respect to their accuracy in describing the structure and energetics as well as the migration of point defects. A number of parameterizations of the Stillinger-Weber (SW) potential and one Tersoff type potential were tested.
The formation energies for different configurations of the interstitial are calculated. Also the formation energy of the vacancy and the bond defect are estimated. It can be shown that the extended 110-dumbbell configuration is the interstitial with the lowest formation energy for most SW parameter sets. In the Tersoff case the tetrahedral interstitial shows the lowest formation energy. For the SW-type potentials the vacancy shows a strong inward-distortion, whereas for the Tersoff potential it shows a slight outwards-distortion.
In recent ab-initio calculations the 110 dumbbell has been found to be the most stable interstitial structure. This is in qualitative agreement with the results for most SW parameter sets, although these calculations predict the extended dumbbell configuration as the interstitial with the lowest formation energy. For the SW parameter sets of W. Yu (model B) and Nordlund, the formation energy of this dumbbell is also in qualitative agreement with the ab-initio result. The formation energy of the vacancy obtained with these SW parameter sets is nearly equal to the ab-initio result. The observed inwards relaxation of the atoms around the vacancy is also found by ab-initio calculations. However, the details of the lattice distortion near the vacancy and the interstitial differ from those predicted by ab-initio calculations.
For the reasons mentioned above, the SW parameter sets of Nordlund et al. and W. Yu et al. are selected for migration investigations. In both cases the vacancy mobility strongly dominates interstitial mobility. Some investigations are also performed with the Tersoff potential, where the vacancy shows a very low mobility.
The results are used to estimate the self-diffusion coefficient. With the SW approach it is shown that self-diffusion in Ge is mediated by vacancies. This stands in good agreement with experimental data. However, the calculated migration energy (2.2 eV) is less than the measured value (3.09 eV). With the Tersoff potential an interstitial dominated mechanism is found. Therefore the Tersoff potential cannot be considered useful for a study of point defect and self-diffusion in Ge.

Detailed experimental data obtained at the TOPFLOW facility for steam-water vertical pipe flow were used to test the complex interaction of local bubble distributions, bubble size distributions and local heat and mass transfer. Steam is injected into sub-cooled water and condenses during the upwards flow. The model considers a large number of bubble classes (50). This allows the investigation of the influence of the bubble size distribution. The results of the simulations show a good agreement with the experimental data. The condensation process is clearly slower, if large bubbles are injected (4 mm holes). Also bubble break-up has a strong influence on the condensation process because of the change of the interfacial area. Some unsureness arises from the unknown interfacial area for large bubbles and possible uncertainties of the heat transfer coefficient.

Experimental data obtained at the TOPFLOW facility for steam-water vertical pipe flow were used to test the complex interaction of local bubble distributions, bubble size distributions and local heat and mass transfer. Steam is injected into sub-cooled water and condenses during the upwards flow. The model considers a large number of bubble classes (50). This allows the investigation of the influence of the bubble size distribution. The results of the simulations show a good agreement with the experimental data. The condensation process clearly depends on the initial bubble size. Also bubble break-up has a strong influence on the condensation process because of the change of the interfacial area.

Electric potential difference probes (PDP) are mostly applied on laboratory scale to measure local velocities in electrically conducting media. Their principle of operation is based on Ohms law. In the absence of electric currents, and provided a proper orthogonal arrangement, the voltage drop measured between the two electrodes is proportional to the fluids velocity. The measuring magnetic field may be applied globally or by a small permanent magnet at the very tip of the Sensor (VIVES--probe). A typical probe as described in the original work has an electrode spacing of 5 mm while using relatively large CoSm magnets. Because the electrodes are usually mounted on the side of the magnet where the field is weaker, the authors were limited to measure velocities down to 1 cm/s at U =1 mV. They specified a sensitivity of 1 mm/s.

Along with progress in analog electronics, results have recently been published by (GELFGAT) who reported on an increased sensitivity of almost an order of magnitude even for a smaller probe. As stated by the the authors, all measurements were conducted at least five times comprising 200 readings, each. From this averaging it becomes obvious that turbulence measurements have not been possible. The subject of this investigation was the flow driven by a rotating magnetic field (RMF), which may be characterised by the aspect ratio and the magnetic Taylor number.

In the present paper, it is described how the applicable range of PDPs regarding sensitivity can be increased further by about two orders of magnitude. An extremely low-noise preamplifier served as a basis of a multistage measuring chain consisting of another two amplifiers and steep
Butterworth filters. For the differential signal processing required for such small voltages as a few nanovolt it was vital to provide a proper common mode rejection throughout the whole instrumental chain. Since acquisition of velocity fluctuations does not allow any averaging or even the use of integrating amplifiers, potential sources of statistical errors had to be avoided. In particular, the electromagnetic noise was countered by a sophisticated wiring scheme. Systematic errors such as thermoelectric currents are detrimental to the measurement of very small mean velocities. Meticulously avoiding both temperature differences and gradients of Seebeck coefficients, it was possible to reduce thermoelectrical voltages below the velocity signal level.

RMF-driven flows comprise a secondary recirculation in the meridional plane. According to theory, the change-over from a Stokes regime to a laminar boundary one of the primary swirl takes place at a Taylor number of approx. 1000, accompanied by a change of the linear scaling (velocity versus Taylor number) to a power 2/3 characteristic. A sensitivity of 0.01 mm/s permitted to safely determine mean velocities for Taylor numbers commencing with 31.

Besides sensitivity and accuracy, measurements of turbulent velocity fluctuations put a severe
restriction on the size of the sensor in order to resolve all scales of potentially significant vortices. The high sensitivity described above was achieved substantially by state of the art analog instrumentation while the dimensions of the probe were quite small. Having an induction
of 75 mT at the tips of the electrodes, their spacing of 1 mm delivered a signal of 180 nV per cm/s, only. Nevertheless, the performance of the measuring chain allowed for the acquisition of
velocity fluctuations even in the transitional regime slightly above the critical Taylor number. The wavenumber spectra calculated via Taylors hypothesis were well resolved up to the end of the inertial range and showed a steep decrease with an exponent less than 4.

We consider the growth of single crystals by the floating-zone method using a radio frequency (RF) heating magnetic field. The quality of the grown crystals, especially of complicated intermetallic compounds, strongly depends on the growth conditions, particularly on the shape of the solidification front. To obtain single crystals of high physical and chemical precision, a convex to the melt growth interface is desirable. The shape of the solid-liquid interface can strongly be influenced by the convective heat transport in the melt. The major mechanism driving the melt flow is the electromagnetic force due to the RF-heating. This force drives a melt flow directed radially inwards at mid-height of the floating zone. Favourable growth conditions, however, would require the flow to be directed away from the solidification front at the axis of symmetry and, respectively, to be directed against it at the free surface of the floating zone. This flow can be generated by an electromagnetic force directed along the free surface towards the solidification front.
We developed the solution of a two-phase stirrer which allows a flexible control of the melt motion. This stirrer basically consists in an additional coil superimposed to the primary induction coil. The additional coil is not connected to any power supply, but it is part of a secondary circuit with adjustable capacitor and resistance. The current in the secondary coil is solely induced by the primary coil. In that way, an electromagnetic pump is created. Its intensity and resulting flow direction can easily be adjusted to the process needs. The flexible system parameter are the location and distance of the secondary coil with respect to the primary one, and the capacitor and resistance of the secondary circuit.
We present numerical and experimental results for the melt flow and temperature fields resulting from the influence of such a two-phase stirrer. Ni-based single crystals as well as various intermetallic compounds have been grown, and the obtained results are discussed in relation to the provided flow control.

Recently various drag reduction techniques were studied numerically and experimentally in many papers. Among others there is the subtopic of magnetohydrodynamic (MHD) drag reduction where the Lorentz force is used for the purpose of drag reduction in an electrically conducting fluid. In many recently published papers permanent magnets and high electric current densities are used in order to achieve reasonable Lorentz forces. This choice, however, immediately leads to a low efficiency.
We consider a plane channel as the flow configuration. Here, the fully developed turbulent channel flow is homogeneous in the streamwise and spanwise directions, thus, periodic boundary conditions can be applied in these directions. This simplifies the numerical solution of the problem significantly. We present the results of direct numerical simulations of turbulent channel flow drag reduction using electromagnetic forces. The Lorentz force is created by the interaction of a permanent magnetic field and an electric current from electrodes placed on the bottom wall surface. Two various electromagnetic field cases are considered. In the first case an oscillating electric current and a permanent magnetic field create a spanwise oscillating Lorentz force, whereas in the second case a stationary electric current and a permanent magnetic field create a steady streamwise force.
The reason of the low MHD drag reduction efficiency by a spanwise oscillating Lorentz force, as obtained up to now in literature, is explained. The main result of our work is that using a load factor k ~ 1 leads to a significant efficiency improvement for all considered cases. The efficiency increases when the load factor is close to its optimum value. We show that the time oscillating spanwise Lorentz force reduces the skin-friction drag. The full drag is also reduced, the efficiency is increased by 100 times but is still much less than 1. In this case, the skin-friction drag may be strongly reduced at a very small load factor k < 1, but not the full drag.
The application of the streamwise Lorentz force leads to a much more effective drag reduction if we consider the drag as a full force applied to the body. The skin-friction drag increases but the full drag may be reduced to the zero value with a good efficiency.

The Traveling Magnetic Field (TMF) is a versatile tool to control the flow in an electrically conducting fluid. It introduces a mainly axial Lorentz force into the fluid which leads to meridional flow patterns. Applying the TMF to the Vertical Gradient Freeze (VGF) growth of semiconductor single crystals, the heat and mass transport in the melt can be tailored for growth under optimised flow conditions to improve crystal properties and/or growth yield.
In this paper we present experimental and numerical results on the TMF driven flow in an isothermal model fluid as well as in a VGF melt. The field is created by an equally spaced set-up of six coils of 36 windings each. Induction and frequency can be varied between 0-5 mT and 50-400 Hz, respectively.
Model experiments were carried out at about 20°C with the traveling field applied to InGaSn melts in cylindrical, non-conducting vessels of different diameters. Axial velocity profiles were measured by means of the Ultrasonic Doppler Velocimetry (UDV) method. The basic flow was investigated as a function of the aspect ratio and of the non-dimensional forcing and screening parameters with the focus on the transition from laminar to time-dependent convection. For comparison, numerical calculations were performed using advanced, highly accurate spectral methods as well as commercial codes.
For the growth experiments a VGF furnace was equipped with the TMF set-up. The maximum temperature of the furnace is about 1300°C and crystals with a diameter up to three inches can be grown. Ga doped germanium single crystals were grown under the influence of the field and without field. The TMF impact on the thermal field in the melt was studied on the basis of natural or artificially induced dopant striations which characterise the solid-liquid interface and, thus, the local temperature field. The transition to instationary melt flow which is indicated by the appearance of regular striation patterns in the crystal, was investigated by increasing the TMF forcing parameter intentionally during growth. Numerical results came from a quasi-2D simulation of the melt flow using the commercial code CrysVun++. A global, thermal model of the VGF furnace has been developed for this purpose.

Atomistic computer simulations show that the metastable defect structure formed immediately after ion bombardment of silicon does not only consist of isolated mono-vacancies and mono-interstitials but also of more complex defects. Amongst them a small percentage of very mobile di-interstitials is found. The structure and energetics of these defects as well as their migration are investigated in more detail, and the results are compared with literature data. Mobile and immobile di-interstitial configurations are found. The migration mechanism shows a pronounced dependence on the temperature. The di-interstitial diffusivity and the self-diffusion coefficient per defect are calculated. The di-interstitial migrates much faster than the mono-interstitial.
The high mobility of the di-interstitials and the fact that they can be already formed during the ion bombardment may have implications for the current understanding of many experimental results obtained in the last decade, in particular for the explanation of the implantation-induced migration of interstitial-like defects at room temperature.

As an effort to improve the corrosion behavior of the mild steel under work conditions, we attempted to produce a high chromium content layer on its surface by applying the recoil implantation process. After polishing, SAE 1020 construction steel samples were covered with chromium and then bombarded with ions. As recoil bombarding atom, we used nitrogen, a light mass specimen. Recoil atoms were applied either by ion beam (IB) accelerator or by plasma immersion ion implantation (PIII) method. Samples treated by the PIII process showed better results, presenting a thicker layer of high Cr content, as measured by Auger electron spectroscopy (AES).

We investigate different kinds of electro-vortex flows generated in a shallow layer of liquid metal. The metal flow is driven by an externally applied electrical current which interacts with its own magnetic field. Due to symmetry this interaction alone causes not yet a flow as the Lorentz force is purely irrotational. If, however, ferromagnetic C-cores or yokes are applied, the magnetic field distribution is modified and a flow driving action results. An electro-vortex flow occurs with several eddies in this MHD-layer. In the stable case, for some range of electrical current values, these eddies are held in permanent position. The unstable case is characterized by an oscillation of the eddies, which are moving in the plane of the layer. One of the reasons to perform this study is related with the occurrence of similar unstable processes in some devices used for metallurgical purposes including the flat MHD-layer considered here. We have investigated this flow by experimental and numerical methods.
We applied the ultrasound Doppler velocimetry which allows us to measure velocity profiles in non-transparent media. The oxide particles of this alloy were acting as good tracers for ultrasound measurements and allowed us to obtain the time-dependences of the velocity profiles. At higher electrical currents, the profiles showed large-scale low-frequency oscillations. Various types of flows are distinguished depending on the location of the ferromagnetic C-core.
The mathematical model of the processes was based on the MHD-equations, which have been modified using a thin-layer approximation. The numerical calculations support the results obtained in experiments, and showed the behavior of the velocity field with the moving of the eddies.

The production of K+ and of K- mesons in heavy-ion collisions at beam energies of 1 to 2 A GeV has systematically been investigated with the kaon spectrometer KaoS. The ratio of the K+ production excitation function for Au+Au and for C+C reactions increases with decreasing beam energy, which is expected for a soft nuclear equation-of-state. A comprehensive study of the K+ and of the K- emission as a function of the size of the collision system, of the collision centrality, of the kaon energy, and of the polar emission angle has been performed. The K-/K+ ratio is found to be nearly constant as a function of the collision centrality and can be explained by the dominance of strangeness exchange. On the other hand, the spectral slopes and the polar emission patterns are different for K- and for K+. Furthermore the azimuthal distribution of the particle emission has been investigated. K+ mesons and pions are emitted preferentially perpendicular to the reaction plane as well in Au+Au as in Ni+Ni collisions. In contrast for K- mesons in Ni+Ni reactions an in-plane flow was observed for the first time at these incident energies.

The prenyl group is known as an important structural building block in natural and medicinal products. The isotopic substitution of one of the two methyl groups with a [11C]methyl group would provide an access to a large number of interesting 11C-labelled compounds. Here we report a strategy for the synthesis of 11C-labelled prenyl group-containing derivatives starting from methyl-substituted alkynes (1) via a novel 11C-C bond forming reaction. A commonly employed strategy to form a,a’-disubstituted alkenes comprises the formation of alkenylzirconocenes by the syn-insertion of a C-C triple bond into the Zr-H bond of Schwartz reagent [Cp2Zr(H)Cl] followed by metal-mediated C-C bond formation with electrophiles under retention of the configuration of the C-C douple bond [1,2].
In principle the formation of alkenylzirconocenes by syn-addition of Schwartz reagent onto disubstituted alkynes (1) leads to a mixture of regioisomers 2 and 2’. However, treatment of an excess of Schwartz reagent favors the formation of the sterically less hindered isomer 2. Transmetalation with transition metal complexes M(PPh3)4 and conversion with [11C]MeI leads to compound 4.

The fluoroethyl ester-containing phenyltropane derivative MCL-322 was shown to display high affinity to the dopamine transporter (DAT) (Ki = 2.3 nM). The binding affinities (Ki values) for the serotonin transporter and norepinephrine transporter were determined to be 5.1 nM and 280 nM, respectively [1]. The high binding affinities and selectivities of MCL-322 make the corresponding 18F-labelled compound an attractive PET radioligand for imaging DAT in brain tissue. Here, we report on the radiosynthesis of [18F]MCL-322 and its radiopharmacological characterization involving biodistribution, autoradiography and small animal PET studies.

An increasing number of PET centers is using 6-[18F]fluoro-L-DOPA ([18F]FDOPA) to study presynaptic dopamine metabolism in vivo.
Currently the electrophilic radiofluoro-destannylation reaction of N-Boc-3,4-di(Boc-O)-6-trimethylstannyl-L-phenylalanine ethyl ester with [18F]F2 has emerged as the preparation method of choice for the reliable and reproducible radiosynthesis of [18F]FDOPA (1-5).
Up to now the radiofluorination step of the trimethyltin precursor is carried out in trichlorofluoromethan (CFCl3, Freon 11) as the solvent. De Vries et al. (4) have reported Freon 11 as the superior solvent to provide the highest radiochemical yields for the radiofluorination step. The authors also have investigated the possibility to substitute Freon 11 with other solvents. They observed considerable losses of radioactivity (61-71%) during the evaporation step of the solvents (e.g. chloroform and acetonitrile). They discussed this finding with the formation of volatile radiofluorine compounds originating from the reaction of [18F]F2 gas with the solvents.
For Freon 11 is hardly available in Europe for environmental protection reasons, we investigated the possibility of substituting Freon 11 with chloroform. In contrast to (4) we use 5 M HCl for protecting group hydrolysis. The acid is added directly after the radiofluorination step and the solvent was evaporated at 130°C. First results with chloroform also show increased losses of radioactivity in comparison to Freon 11. However, we found that the rate of radioactivity loss depends on the quality of the chloroform used. The radioactivity losses using chloroform stabilised with ethanol were in the range of 25%, whereas the amylene stabilised chloroform gave losses of 40%. In contrast, using deuterated chloroform (CDCl3) for NMR analysis purposes stabilised with silver no significant losses of radioactivity were observed in comparison with Freon 11. We conclude that no competitive radiofluorination of the solvent chloroform, neither CHCl3 nor CDCl3, with [18F]F2 occures. Instead of that the observed radioactivity losses can be explained by the radiofluorination of stabilisers present in CHCl3.The non-decay-corrected total yield for [18F]FDOPA preparation using Freon 11 as the solvent is 17% (n = 26). Using CDCl3 (silver stabilised) instead of CFCl3 the average non-decay-corrected total yield is slightly higher, being 20% (n = 17).
The use of CDCl3 has further advantages:

• easy handling (boiling point = 61°C) and unlimited availability,
• better environmental protection properties,
• the radiofluoro-destannylation reaction can be carried out at temperatures above freezing-point

AIMS: Corticosteroids are implicated in neuropsychiatric disorders such as severe depression and anxiety. This work investigates the usefulness of nonsteroidal glucocorticoid receptor (GR) ligand [11C]AL-438 as PET ligand for imaging of brain GRs.
METHODS: [11C]AL-438 was synthesised by methylation of the corresponding O-desmethyl labelling precursor with [11C]MeI. Radiopharmacological characterisation of [11C]AL-438 was performed in Wistar rats using biodistribution studies, ex vivo autoradiography and small animal PET studies.
RESULTS: [11C]MeI was trapped in a DMF solution containing the O-desmethyl labelling precursor and NaOH as the base. The methylation reaction was accomplished within 5 min at 100°C. The total synthesis time including HPLC-purification was 40-45 min. [11C]AL-438 was obtained in radiochemical yields of 30-40% (decay-corrected) at a specific radioactivity of 15 to 20 GBq/µmol at the end of the synthesis. The radiochemical purity of [11C]AL-438 exceeded 98%.
Biodistribution studies in rats demonstrated a brain uptake of 1.6 ± 0.4% ID/g after 5 min p.i., which decreased to 0.6 ± 0.1% ID/g after 60 min. Brain to blood ratios at 5 min and 60 min p.i. were 3.0 and 1.0, respectively. The pituitary and adrenals as major GR-containing peripheral organs showed uptake of 2.4 ± 0.5% ID/g and 7.5 ± 1.5% ID/g after 5 min and of 1.8 ± 1.0% ID/g and 3.8 ± 0.6% ID/g after 60 min, respectively. The uptake in the pituitary and adrenals could not be reduced significantly by pretreatment with 10 mg/kg of corticosterone.
Ex vivo autoradiographic studies of [11C]AL-438 on rat brain 5 min after i.v. administration showed specific accumulation of radioactivity in regions rich of GR, such as hypothalamus and various nuclei of thalamus. CONCLUSION: The biodistribution and the brain autoradiographic data of [11C]AL-438 correlated with the expected pattern of GRs in rodents.

The defect structure of Ge-implanted and annealed silicon was investigated. Based on the observation of both, interstitial- and vacancy-type defects, a stacked structure of layers of vacancy and interstitial clusters was detected. These defects form a substructure within the basic dual structure consisting of a vacancy-dominated and an interstitial-dominated region. The appearance of cavities (vacancy clusters) in the interstitial-dominated region indicates significant vacancy–vacancy clustering beside the vacancy–interstitial recombination. Clustering of vacancies and interstitials prevents the vacancy–interstitial recombination. The observed defect structure is in contrast to the widely accepted +1 model which predicts the complete recombination of ion-generated vacancies and interstitials. The limits of the +1 model are discussed.

Postulating an unlikely core melt down accident for a light water reactor (LWR), the possible failure mode of the reactor pressure vessel (RPV) and its failure time have to be investigated for a determination of the load conditions for subsequent containment analyses. Worldwide several experiments have been performed in this field accompanied with material properties evaluation, theoretical, and numerical work.
At the Institute of Safety Research of the FZR a finite element model (FEM) has been devel-oped simulating the thermal processes and the viscoplastic behaviour of the vessel wall. An advanced model for creep and material damage has been established and has been validated using experimental data. The thermal and the mechanical calculations are sequentially and recursively coupled. The model is capable of evaluating fracture time and fracture position of a vessel with an internally heated melt pool.
The model was applied to pre- and post test calculations for the FOREVER test series repre-senting the lower head RPV of a pressurized water reactor (PWR) in the geometrical scale of 1:10. These experiments were performed at the Royal Institute of Technology in Stockholm. In this paper the differences between the results of a simple coupled and a recursive coupled FE-simulation are highlighted. Due to the thermal expansion at the beginning and the accu-mulating creep strain later on the shape of the melt pool and of the vessel wall are changing. Despite of the fact that these relative small geometrical changes take place relatively slowly over time, the effect on the temperature field is rather significant concerning the mechanical material behavior and the resulting failure time. Assuming the same loading conditions, the change in the predicted failure time between the simple and the recursive coupled model is in the order of magnitude of the total failure time of the simple model. The comparison with results from the FOREVER-experiments shows that the recursive coupled model is closer to reality than the one-way coupled model.

La polución de aguas por metales pesados es un serio problema ambiental, siendo las principales fuentes de esta contaminación las aguas procedentes de industrias metalúrgicas y mineras. A diferencia de otros contaminantes, una característica preocupante de los metales pesados es la tendencia a persistir indefinidamente en el ambiente, circulando a través de la cadena trófica y acumulándose eventualmente en los organismos superiores.

La búsqueda de soluciones a este tipo de problemas ha hecho que en las dos últimas décadas se haya incrementado notablemente la investigación en relación al potencial biotecnológico de los microorganismos para su eliminación, teniendo en cuenta la capacidad de la biomasa microbiana para concentrarlos y removerlos. Para el tratamiento de aguas dulces se ha ensayado biomasa procedente de bacterias, hongos y algas. No obstante, para el de aguas marinas, si bien hay abundante bibliografía sobre la utilización de algas, apenas hay referencias sobre la utilización de bacterias, por lo que ha parecido de interés realizar una investigación sobre la capacidad de bioadsorción de metales pesados por una cepa bacteriana marina.

Esta comunicación presenta los resultados preliminares obtenidos trabajando con una bacteria aislada de aguas someras del Mar de Alborán, denominada MAH1. Esta cepa bacteriana que crece bien en medios de cultivo comunes y produce abundante cantidad de EPS, presenta la capacidad de desarrollarse en un rango de temperaturas de 2 a 47ºC y a concentraciones de NaCl de 0,6 a 20%. Los ensayos realizados con ella han tenido una doble finalidad: probar, en condiciones estándar, la capacidad de bioadsorción de cromo, plomo, lantano, cobalto, níquel y manganeso y determinar, mediante obresvación con microcopio electronico de transmisión, la localización celular de los metales bioadsorbidos. Los ensayos de bioadsorción se han realizado con biomasa húmeda obtenida en fase exponencial de crecimiento y con soluciones de los metales a concentración 0,5 mM en agua mili- Q y pH 4,5. Los resultados obtenidos indican una buena adsorcion para el cromo y para el plomo (0,91 y 0,78 mmol/gr de biomasa seca, respectivamente), y menor para el resto de los metales ensayados (lantano 0,08 mmol/gr; cobalto 0,1 mmol/gr; manganeso 0,063 mmol/gr y níquel 0,14 mmol/gr). La localización celular de los metales bioadsorbidos ha sido: Pb y Cr, en la pared celular, La en el EPS y los restantes, intracelularmente.

Estos resultados indican que se trata de una bacteria que puede ser buen candidato para desarrollar sistemas de tratamiento de aguas marinas contaminadas por metales pesados, más aún si se tiene en cuenta que son preliminares y que no se han optimizado las condiciones para la bioadsorción de cada metal.

Unusual, S-layer-like gene carrying, mobile elements were localized on the chromosomes of the uranium mining waste pile isolate Bacillus sphaericus JG-A12 and of the closely related strain Bacillus sphaericus NCTC 9602 in the vicinity of the functional S-layer genes. Each of the two almost identical elements designated ISBsph1 (strain 9602) and ISBsph2 (strain JG-A12) possess four ORFs which encode a putative integrase /recombinase, a putative XRE-family like protein containing a DNA binding helix turn helix motif, and a S-layer-like gene copy. Interestingly, the S-layer-like gene copies of the two IS elements are analogous to the coding parts of the previously described plasmid-located, identical between each other, and siltent S-layer genes of the two strains. In the case of the strain JG-A12, however, the ISBsph2 borne s-layer-like gene is truncated.
Comparative analyses of the functional, of the plasmid-located, and of the IS-element-specific S-layer genes of the above mentioned two strains between each other and with the S-layer genes of the other Bacillus sphaericus strains studied up to date revealed that all functional S-layer genes possess mosaic structure and share regions with very high identitiy which are surrounded by regions possessing very low or almost no identity.
Our results strongly suggest that the functional S-layer protein genes in Bacillus sphaericus have evolved via horizontal transfer of genetic information followed by rearrangements which were mediated by mobile elements.
The primary structure of the functional S-layer of the uranium mining waste isolage JG-A12 and in particular its higher capability in comparison to the other S-layers to bind uranium and other metals indicate that the environmental stress factors played an important role in the evolution of its gene.

Interactions of U(VI) with the indigenous bacterial and archael communities of the uranium mining waste pile Johanngeorgestadt in Germany were studied. For this several portions of one sample with a natural content of 40 mg U/kg were supplemented with 60 mg U/kg and 260 mg U/kg in form of uranyl nitrate. Part of the most contaminated portion was additionally incubated under anaerobic conditions. Bothe, selective sequential extraction (SSE) and X-ray absorption spectroscopic analyses, indicated that added U(VI) was bound as uranyl by inner-sphere sorption complexes. No reduction of U(VI) to U(IV) was observed even by the anaerobic treatment.
Analyses of the constructed 16S rRNA gene clone libraries of the untreated and of the U(VI)-supplemented samples revealed changes in the bacterial and in the archaeal parts of the natural microbial community. In the untreated sample the bacterial community was predominated by Alphaproteobacteria and Holophaga/Acidobacterium members. The number of the latter was strongly reduced by increasing the uranium content up to 100 mg U/kg. Instead, a large number of sequences were found representing Gamma-Pseudomonas spp., Arthrobacter ssp. (Actinobacteria) as well as Geobacter spp. (Deltaproteobacteria). The most contaminated portion containing approximately 300 mg U/kg was predominated by represenatives of Cytophaga/Flavobacterium/Bacteroides group. The anaerobic treatment of this sample induced also proliferation of Alpha- and Gammaproteobacteria in it.
The archaeal populations in the original waste sample were rather diverse, whereas the supplemented with U samples wee strongly predominated by a few particular Grenarchaeota species.
Our results indicate that the addition of U(VI) to a low contaminated uranium mining waste sample induces significant shifting in the indigenous microbial populations in dependence on the amount of U(VI) and the redox conditions.

It could be shown that dendritic compounds show the same complex stoichiometry in non-water and water soluble forms. The stability constants in both solution sytems are comparable. As a consequence this demonstrates the possible use of such compounds in for complexation of metal ions aquatic systems.
As the fluorescence decay times change with the concentration of the added metal ion two effects have to be discussed: Dynamic fluorescence quenching, excited state reactions of the ligand. In case of dynamic fluorescence quenching a linear relationship between the concentration of the quencher and the ratio of the fluorescence decay time without and with quencher should be observed.

Summary

During the past decade many studies on speciation of actinides in natural and artificial environments have been done. High demands on the sensitivity in speciation of actinides lead to the development of advanced detection methods. This is connected with intensive use of laser systems as excitation source. Laser can provide any wavelength from the near UV to the NIR (Near Infrared) wavelength range. The development of tunable solid-state lasers overcame some disadvantages of dye laser systems. The application of low temperatures for samples measured with fluorescence spectroscopic methods brought effort in the detection of carbonate species. The availability of modern femtosecond laser systems in combination with ICCD (Intensified Charge Coupled Device) cameras gave the possibility to exploit the fluorescence properties of aromatic organic compounds for the study of their interaction with actinides, especially non-fluorescent metal ions.
The fluorescence of some tetravalent actinides as Pa(IV) and U(IV) in aquatic systems was described firstly. The speciation of actinides in arsenate and several carbonate systems was investigated. The interaction with ligands from life sciences as ATP (adenosine triphosphate) and sugar phosphates became more and more important. Also studies of the speciation of actinides in plants and microorganism cannot be neglected.
In the solid state the speciation of uranium(VI) in several natural and synthetic minerals has been studied as well as the behaviour of depleted uranium in the environment. The interaction of actinides with rock materials and minerals as well as their uptake is also of common interest in actinide chemistry. Especially the sorption and inclusion of Cm into several minerals lead to an improvement in knowledge of minor components in solids.
It is not possible to give a complete overview on the literature about the laser-induced spectroscopy of actinides. The restricted length of this contribution allows only a relatively small and personally influenced selection.

Carbon (C) and carbon nitride (CNx) films were grown on Si(100) substrates by direct ion beam sputtering (IBS) of a carbon target at different substrate temperatures (RT-450°C) and Ar/N2 sputtering gas mixtures. Additionally, the effect of concurrent nitrogen ion assistance during the growth of CNx films by IBS was also investigated. The samples were analyzed by elastic recoil detection analysis (ERDA) and x-ray near edge absorption spectroscopy (XANES). ERDA results showed that significant nitrogen amount (up to 20 at. %) was incorporated in the films, without any other nitrogen source but the N2-containing sputtering gas. The nitrogen concentration is proportional to the N2 content in the sputtering beam and no saturation limit is reached under the present working conditions. The film areal density derived from ERDA revealed a decrease in the amount of deposited material at increasing the growth temperature, with a correlation between the C and N losses. XANES results indicate that N atoms are efficiently incorporated into the carbon network and can be found in different bonding environments, such as pyridine-like, nitrile-like, graphite-like, and embedded N2 molecules. The contribution of molecular and pyridine-like nitrogen decreases when the temperature increases while the contribution of the nitrile-like nitrogen increases. The concurrent nitrogen ion assistance resulted in the significant increase of the nitrogen content in the film but it induced a further reduction of the deposited material. Additionally, the assisting ions inhibited the formation of the nitrile-like configurations while promoting nitrogen environments in graphite-like positions. The nitrogen incorporation and release mechanisms are discussed in terms of film growth precursors, ion bombardment effects and chemical sputtering.

We determined structural parameters for the near-neighbor surrounding of plutonium(III) in complexes with humic and fulvic acids at pH 1 and for the purpose of comparison also for the plutonium(III) aquo ion by means of X-ray absorption fine structure (XAFS) spectroscopy. It could be shown that in the complexes with humic substances as well as in the Pu3+ aquo ion sample the trivalent oxidation state of plutonium was stable within the time of the experiment. In the humate and fulvate complexes, the plutonium(III) is surrounded by about 8 oxygen atoms with an average Pu-O distance of 2.48 ± 0.02 Å. The structural parameters determined for plutonium(III) humate and fulvate complexes were compared to structural parameters of plutonium(III) and plutonium(IV) aquo ions given in the literature.

Azimuthal distributions of pi+, K+ and K- mesons have been measured in Au+Au reactions at 1.5 AGeV and Ni+Ni reactions at 1.93 AGeV. In semi-central collisions at midrapidity, pi+ and K+ mesons are emitted preferentially perpendicular to the reaction plane in both collision systems. In contrast for K- mesons in Ni+Ni reactions an in-plane elliptic flow was observed for the first time at these incident energies.

500 keV nitrogen implantations at different tilt angles (0o, 0.5o, 1.2o, 1.6o, 4o) with respect to the c-axis of 6H-SiC were carried out. Radiation damage distributions have been investigated by Backscattering Spectrometry combined with channeling technique (BS/C) using 3550 keV 4He+ ion beam. A comparative simultaneous evaluation of the damage depth distributions in the Si and C sublattices of 6H-SiC led to a correction factor of 0.8 in the electronic stopping power of 4He+ ions along <0001> channel. Full-cascade Crystal-TRIM simulations with the same set of damage accumulation model parameters could reconstruct the measured shapes and heights of damage distributions for all implantation tilt angles. Secondary defect generation effects in addition to the primary point defect accumulation were assumed in the analysis.

This study evaluates chemical trends of seven acidified reservoirs and 22 tributaries in the Erzgebirge from 1993 to 2003. About 85% of these waters showed significantly (p < 0.05) declining concentrations of protons (−69%), nitrate (−41%), sulfate (−27%), and reactive aluminum (−50% on average). This reversal is attributed to the intense reduction of industrial SO2 and NOx emissions from formerly high levels, which declined by 99% and 82% in the German–Czech border region between 1993 and 1999. The deposition rates of protons and sulfur decreased by 70–90%. Since 1993, the dry deposition of total inorganic nitrogen diminished to a minor degree, but the wet deposition remained unchanged. The surface waters reflect a substantial decrease in Al exchange processes, a release of sulfur previously stored in soils, and an uptake of nitrate by forest vegetation. The latter effect may be supported by soil protection liming which contributed to the chemical reversal in almost 20% of the study waters.

The IR, green, and UV electroluminescence from rare-earth (Er, Tb, and Gd) implanted SiO2 MOS devices is studied, exhibiting quantum efficiencies comparable to III-V light emitting diodes.

Different methods of defect engineering are applied in this study for ion beam synthesis of a buried layer of SiC and SiO2 in Si. The initial state of phase formation is investigated by implantation of relatively low ion fluences. He-induced cavities and Si ion implantation generated excess vacancies are intentionally introduced in the Si substrate in order to act as trapping centers for C and O atoms and to accommodate volume expansion due to SiC and SiO2 phase formation. Especially the simultaneous dual implantation is shown to be an effective method to achieve better results from ion beam synthesis at implantation temperatures above 400oC. For SiC synthesis it is the only successful way to introduce vacancy defects. The “in situ” generation of vacancies during implantation increases the amount of SiC nanoclusters and improves crystal quality of Si in the case of SiO2 synthesis. Also the pre-deposition of He-induced cavities is clearly advantageous for the formation of a narrow SiO2 layer. Moreover, in-diffusion of O by surface oxidation can substitute a certain fraction of the O ion fluence necessary to obtain a buried homogeneous SiO2 layer.
The results show that defect engineering for SiC and SiO2 synthesis is working. However, the implementation of a single action is not sufficient to achieve a significant improvement of ion beam synthesis. Only an optimized combination of the different versions of defect engineering can bring about pronounced better results.

Die „Nanopartikel-Zell-Chirurgie“ unter Ausnutzung der Partikelstrahlung von Radionukliden trägt ein großes Potential für die adjuvante Krebstherapie in sich, sofern es gelingt, das entsprechende Radiotherapeutikum im Tumor selektiv zu deponieren und dort eine letale Strahlendosis unter weitgehender Schonung gesunden Gewebes zu erreichen, so dass die Zelle in ihrer Gesamtheit untergeht. In diesem Zusammenhang gewinnen magnetische Kern/Hüll-Nanoteilchen an Bedeutung. Durch zielgerichtete Modifizierung können auf der Oberfläche von magnetischen Ferrit-Nanoteilchen spezielle Haftgruppen zur stabilen Fixierung von Radionukliden angebracht werden. Diese radioaktiv markierten Nanoteilchen können dann durch geeignete Magnetfelder an Tumoren fixiert werden. Bedeutendes Zukunftspotential ist außerdem im zusätzlichen, selektiven Targeting der radioaktiv markierten, magnetischen Nanoteilchen durch Einführung von zielsuchenden Strukturen - wie Antikörper oder spezifische Peptide - in die Hülle der Nanopartikel gegeben.
Für erste Untersuchungen zur radioaktiven Markierung wurden Magnetit-Teilchen mit einem mittleren Kerndurchmesser von 10 nm ausgewählt, die eine DMSA-Hüllschicht tragen. DMSA bildet mit Technetium(V) und Rhenium(V) sehr stabile Komplexe, die eine quadratisch-pyramidale Koordinationsgeometrie aufweisen (s. Abb. 1).
Die Markierung von DMSA mit den therapeutisch relevanten Radionukliden ¹⁸⁶Re und ¹⁸⁸Re liefert die entsprechenden radioaktiven Komplexe in hoher Ausbeute, wobei in der Regel bei Temperaturen von 100°C gearbeitet wird. Für die eingesetzten DMSA-umhüllten magnetischen Nanoteilchen konnten bei Raumtemperatur Markierungs-ausbeuten bis zu 70% für das Generatornuklid ¹⁸⁸Re erzielt werden, wobei das Radionuklid mindestens 24 h stabil an diesen Teilchen gebunden bleibt.

An easy and gentle method for the preparation of ¹⁸⁸Re(V) complexes with bidentate and tetradentate ligands is described starting from the precursor complex ¹⁸⁸Re(III)-EDTA. That complex is prepared at room temperature in acidic solution and reacts by a combined re-oxidation/ligand exchange reaction with appropriate ligands like DMSA or ECD (DMSA = dimercapto succinic acid, ECD = L,L-ethylene dicysteine diethyl ester) or en and cyclam (en = ethylene diamine, cyclam = 1,4,8,11-tetraazacyclotetradecane) to the ¹⁸⁸Re(V)-oxo- and dioxocomplexes, respectively. The chelates were unambiguously identified by chromatographic comparison with spectroscopically characterised samples or known ^99mTc-kit reconstitutions. The reaction succeeds under mild conditions (room temperature, short time, neutral or weak basic solutions) with high yields and has potential for labelling of sensitive biomolecules with ¹⁸⁸Re.

Abstract is not available.