Publications Repository - Helmholtz-Zentrum Dresden-Rossendorf

Any safety assessment of waste disposal concepts requires comprehensive and consistent thermodynamic data for the respective reactive transport modelling. This includes sorption, ion exchange or surface precipitation as major retardation processes. The current lack of respective quality-assured databases for these interface phenomena (invalid reaction formulation, missing consistency, restricted application ranges, and contradictory data) severely hampers a reliable modelling.
This work aims on a re-evaluation of already published sorption raw data based on spectroscopically verified surface complexes and their formation reactions. This shall help to transform the free-for-use digitized sorption data collection RES³T (http://www.hzdr.de/res3t) into a true thermodynamic reference database be used for complex real systems such as rocks or soils following the “Component Additivity” approach. Coupled to this is an extension of RES³T allowing also for the storage of sorption raw data sets. Eventually, a full integration with the thermodynamic reference database THEREDA (http://www.thereda.de) is envisaged to provide a comprehensive database for a holistic geochemical modeling.
Sorption speciation calculations of radionuclides on various mineral surfaces will be presented, showing the actual consequences of inconsistent sorption data that can be found in literature, as well as the possibilities using a validated surface speciation. The latter is mainly based on a combination of ATR FT-IR, TRLFS, and EXAFS which allows to create chemically realistic surface complexing models. In combination with the site-density data (including ones from crystallographic measurements), surface complexation models are deduced that describe the sorption of radionuclides accurately and with less surface species then assumed in a vast number of literature references published in the past. Due to the correct description of the realistic surface chemistry and the internal consistency, these models are more robust to other chemical and environmental conditions (pH, pe, composition of the aqueous phase).
As examples, the sorption of uranium(VI) onto various mineral phases (Al-, Fe- and Si-phases), ubiquitous in nature will be presented.

We examine kinematic dynamo action driven by an axisymmetric large scale flow that is superimposed with an azimuthally propagating non-axisymmetric perturbation with a frequency ω. Although we apply a rather simple large scale velocity field, our simulations exhibit a complex behavior with oscillating and azimuthally drifting eigenmodes as well as stationary regimes. Within these non-oscillating regimes we find parametric resonances characterized by a considerable enhancement of dynamo action and by a locking of the phase of the magnetic field to the pattern of the perturbation. We find an approximate fulfillment of the relationship between the resonant frequency ω_res of the disturbed system and the eigenfrequency ω₀ of the undisturbed system given by ω_res = 2 ω₀ which is known from paradigmatic rotating mechanical systems and our prior study [Giesecke et al., Phys. Rev. E, 86, 066303 (2012)]. We find further -- broader -- regimes with weaker enhancement of the growth rates but without phase locking. However, this amplification regime arises only in case of a basic (i.e. unperturbed) state consisting of several different eigenmodes with rather close growth rates. Qualitatively, these observations can be explained in terms of a simple low dimensional model for the magnetic field amplitude that is derived using Floquet theory.

Herein we present a molecular doping of a high mobility diketopyrrolopyrrole–dithienylthieno[3,2-b]thiophene donor–acceptor copolymer poly[3,6-(dithiophene-2-yl)-2,5-di(6-dodecyloctadecyl)pyrrolo[3,4-c]pyrrole-1,4-dione-alt-thieno[3,2-b]thiophene], PDPP(6-DO)2TT, with the electron-deficient compound hexafluorotetracyanonaphthoquinodimethane (F6TCNNQ). Despite a slightly negative HOMO(donor)–LUMO(acceptor) offset of −0.12 eV which may suggest a reduced driving force for the charge transfer (CT), a partial charge CT was experimentally observed in PDPP(6-DO)2TT:F6TCNNQ by absorption, vibrational, and electron paramagnetic resonance spectroscopies and predicted by density functional theory calculations. Despite the modest CT, PDPP(6-DO)2TT:F6TCNNQ films possess unexpectedly high conductivities up to 2 S/cm (comparable with the conductivities of the benchmark doped polymer system P3HT:F4TCNQ having a large positive offset). The observation of the high conductivity in doped PDPP(6-DO)2TT films can be explained by a high hole mobility in PDPP(6-DO)2TT blends which compensates a lowered (relatively to P3HT:F4TCNQ) concentration of free charge carriers. We also show that F6TCNNQ-doped P3HT, the system which has not been reported so far to the best of our knowledge, exhibits a conductivity up to 7 S/cm, which exceeds the conductivity of the benchmark P3HT:F4TCNQ system.

Developing highly active and durable oxygen reduction reaction (ORR) catalysts is crucial to reduce the cost of polymer electrolyte fuel cells (PEFCs). To meet those requirements, unsupported Pt-Cu alloy nanochains (aerogels) were synthesized by a simple co-reduction route in aqueous solution and their structure was characterized by X-ray absorption spectroscopy and scanning transmission electron microscopy coupled with energy-dispersive X-ray spectroscopy. These catalysts exceeded the ORR activity of commercial Pt/C catalysts by more than 100% in rotating disk electrode (RDE) experiments and met the corresponding US DOE target for automotive PEFC implementation, thereby qualifying as very promising materials. The behavior of Pt-Cu aerogels under PEFC operation conditions was mimicked by acid washing experiments which showed that the Cu content in the alloy phase and ORR activity decrease through this step. Comparing composition, structure and ORR activity for various specimens, the Cu content in the alloy phase was identified as the main descriptor of ORR activity. An almost linear correlation was found between those two parameters and complemented by supporting data from the literature.

In the present work point defects in ZnO crystals were characterized by positron lifetime spectroscopy combined with back-diffusion measurement of slow positrons. Defects in ZnO crystals grown by various techniques were compared. Hydrothermally grown ZnO crystals contain defects characterized by lifetime of ≈181 ps. These defects were attributed to Zn vacancies associated with hydrogen. ZnO crystals prepared by other techniques (Bridgman, pressurized melt growth, and seeded chemical vapour transport) exhibit shorter lifetime of ≈165 ps. Positron back-diffusion studies revealed that hydrothermally grown ZnO crystals contain higher density of defects than the crystals grown by other techniques. The lowest concentration of defects was detected in the crystal grown by seeded chemical vapor transport.

Purpose/Objective: Radiochemotherapy (RCT) for patients with head and neck squamous cell carcinoma (HNSCC) frequently causes xerostomia and dysphagia, which may be alleviated by treatment adaption, e.g., modulation of dose distribution to the salivary glands. Current clinical models, which are based on dosimetric parameters, mostly achieve moderate prediction accuracy. Therefore, we aimed to improve the prediction of xerostomia and dysphagia by using additional imaging biomarkers based on computed tomography (CT) scans.

Material/Methods: In this study 46 patients with UICC stage III/IV advanced head and neck squamous cell carcinoma (HNSCC) were considered (NCT00180180, [1]). All patients received primary RCT and underwent a pre-treatment CT scan without intravenous contrast agent. Patient-reported xerostomia and dysphagia were evaluated at baseline, every week during RCT, four weeks after treatment and three monthly thereafter. 5040 imaging features were extracted from the parotid and submandibular glands. Feature reproducibility tests based on the RIDER re-test data set [2] were performed leading to 1513 imaging features in total. The most informative features were selected by a univariate logistic regression analysis. The developed radiomic signature was used to train and validate multivariate logistic regression and random forest models using repeated 5-fold cross validation. The predication accuracy was assessed by the area under the curve (AUC).

Results: The logistic regression and the random forest model achieved similar performance in predicting xerostomia (AUC=0.71). The developed signature consisted of one dosimetric parameter and one imaging feature. For the prediction of dysphagia both models achieved only a moderate prediction accuracy (AUC=0.55).

Conclusions: For prediction of xerostomia, a signature was developed and showed a good performance. For dysphagia only moderately performing models could be obtained in this cohort. Based on our results, subgroups of patients at a high risk of xerostomia may be identified and offered treatment adaption. However, further investigations are currently ongoing, i.e., externally validating the developed signature, which is an important step in developing clinically relevant prediction models.

Magnetization of a Ho₂Fe₁₄Si₃ single crystal was measured in a steady magnetic field of up to 9 T and in pulsed fields of up to 60 T applied along the principal axes. Ho₂Fe₁₄Si₃ is a ferrimagnet below T_C = 480 K, has a spontaneous magnetic moment of about 8 µ_B/f.u. (at T = 4.2 K) and exhibits a large easy-plane magnetic anisotropy. There is also a certain anisotropy within the basal plane, the b axis [120] being the easy-magnetization direction. In fields applied along the a and b axes field-induced first-order phase transitions are observed at 29 T and at 22 T, respectively. Along the easy axis b we observe also an S-shaped anomaly at about 47 T, which does not correspond to a phase transition. A simple model predicts that the two observed first-order transitions are the only ones taking place in Ho₂Fe₁₄Si₃; the magnetization should subsequently grow continuously and arrive at saturation at ~100 T. This is in stark contrast to the behavior of the parent compound Ho₂Fe₁₇, where as many as three sequential first-order transitions are expected for H‖b. The reason for the disparity is that the basal-plane anisotropy constant K_Ho is at least one order of magnitude smaller in Ho₂Fe₁₄Si₃ than it is in Ho₂Fe₁₇.

We present first data on charged kaons and phi mesons in Au+Au collisions at a kinetic beam energy of 1.23A GeV. As observed already at slightly higher beam energies, we find significantly different slopes for the K+ and K- transverse-mass spectra, and no significant increase of the the K-/K+ multiplicity ratio with increasing centrality of the collision. The {\phi}/K- multiplicity ratio is found to be surprisingly high with a value of 0.52 ± 0.16 and shows no dependence on the centrality, either. The different slopes of the K+ and K- spectra can be explained by feed-down from phi mesons, which substantially softens the spectra of K- mesons.

Purpose or Objective
With the increase of proton therapy facilities worldwide featuring Pencil Beam Scanning (PBS) as their only treatment modality, PBS is on the way of becoming the standard for proton therapy. However, for some indications in the thoracic region PBS is not widely used due to uncertainties in the planned dose, which can be caused by combined effects of setup errors, range uncertainty, interplay effect, breathing irregularity, anatomical variations, delivery machine uncertainties, etc. By performing pre-treatment plan robustness evaluation that includes these effects, it is evident that actual delivered fractional dose at any instance is highly uncertain to predict. 4D dose accumulation is able to control some of the uncertainties that are affecting pretreatment evaluation of the plan quality. Therefore, the purpose of this proof-of-concept study is to investigate the
feasibility of monitoring and assessing the quality of delivered treatment fractions throughout the treatment course.

Material and Methods
4D dose accumulation is performed by utilizing (1) delivery machine log files (IBA, Belgium), (2) breathing pattern records (ANZAI, Japan) and (3) planning 4DCT scans or repeated 4D control CT scans (Siemens, Germany). Dose computation is performed in the RayStation (RaySearch, Sweden) treatment planning system (TPS). For every spot that is delivered during a particular fraction, the spot energy, position, dose (as charge) and absolute time of delivery is retrieved from the machine
log file using a dedicated script. Patient’s breathing pattern is analyzed and inhale peaks are determined. Subsequently, all breathing cycles are divided in 10 phases and each phase is associated with absolute time. PBS spots are split in 10 groups according to their corresponding phase and written to 10 treatment sub-plans (DICOM), where every sub-plan corresponds to a particular phase of the 4DCT. Using scripting capabilities of the TPS, sub-plans are imported for dose computation. Eventually dose warping to the reference phase is performed to estimate the delivered fractional dose. Data sets used for the proof-of-concept were not collected during the same treatment fraction.

Results
By using the described method the timeline of a PBS delivery can be correlated with patient’s breathing pattern as shown in Figure 1. Computation of log based sub-plans on 4DCT results in an accumulated fractional 4D dose distribution as shown in Figure 2. Based on the exemplary case, the method allows to assess the conformity between planned and delivered doses (i.e.,
CTV V95 has dropped to 96.7% from nominal 100%).

Conclusion
The availability of a real-time 4D dose accumulation based treatment assessment tool allows to assess the quality of the delivered dose during progress of the treatment course and to take appropriate actions, as for example, plan adaptation, in cases of significant deviations. It is foreseen to extend this study for a full treatment course of a broader population of patients.

Purpose
The dose distribution and range of proton beams are exceedingly prone to uncertainties and anatomical changes, demanding for an in-vivo range verification. A promising approach is prompt γ-ray imaging (PGI), which was recently implemented clinically in Dresden using a so-called PGI slit camera [1,2] in double scattering (DS). However, the detectability of local range shifts, affecting only part of the lateral field in DS, is limited. The spot-wise dose deposition in pencil beam scanning (PBS) promises a finer spatial resolution of range shifts. The purpose of this study is to comprehensively investigate the sensitivity to detect range shifts in DS and PBS using a head phantom in a clinical setup.

Materials and Methods
For a realistic brain tumor treatment, treatment plans in DS and PBS (2 beams, 60 GyE,
2 GyE/fx), were created. One beam (1 GyE) was applied to a CIRS head phantom and monitored with the PGI slit camera. To investigate the influence of the spot dose, the same beam with 5 GyE was also delivered and measured. Global and local (5 cm in diameter) range shifts were introduced and the PGI profiles (prompt-γ counts over depth) with and without shifts were compared. Sum profiles containing prompt-γ counts over the entire fraction were used for the comparison of DS and PBS. Moreover, PGI profiles measured in PBS were analyzed spot-wise and will also be compared with simulated profiles for absolute range determination.
 
Results
A good agreement between introduced and measured global shifts was found in the sum profile evaluation for both modalities, PBS and DS (Table 1). Relative differences were below 2, 7 and 12 % for the 10, 7 and 4 mm shifts, respectively. Local shifts are not detectable using sum profiles. For the applied local shifts, a spot-wise comparison of PGI profiles in PBS allows the detection and localization of global and local shifts (Figure 1). For interpretation, neighboured spots should be clustered, as shifts detected for single spots are less reliable due to low statistics. Higher doses (5 vs. 1 GyE) allow the detection of smaller shifts as shown in Figure 1 for the 4 mm local shift.

Conclusion
The systematic sensitivity study revealed the capability of the PGI slit camera to detect range shifts under clinical conditions. In both treatment modalities, global range shifts can be detected. Additionally, in PBS a spot-wise comparison allows also the determination of interfractional local range shifts. Moreover, a still ongoing evaluation of PBS measured and simulated spot-wise profiles for absolute range verification will be presented.

Counter-Current Flow Limitation (CCFL) is of importance for PWR safety analyses in several accident scenarios connected with loss of coolant events. To investigate the characteristics of this phenomenon and to establish a database suitable for CFD-model development and validation a 1:3 scaled flat model of a German Konvoi reactor hot leg including a part of the steam generator inlet chamber was built up. The test section was operated in the TOPFLOW pressure chamber to allow optical observation of steam-water flows at pressure levels up to 50 bars. The test series comprises air-water tests at 1 and 2 bar as well as steam-water tests at 10, 25 and 50 bar. The gas was injected from the tank simulating the reactor vessel while the water enters into the steam generator (SG) separator tank. A steel sheet divides the SG separator tank in two parts. The first one serves as completion of the SG inlet chamber from the water side and the second is necessary to keep the level in the first part constant, using the steel sheet as level drain. This allows to investigate CCFL under steady state conditions. During the experiments the flow structure was observed along the hot leg model using a high-speed camera and web-cams. In addition pressure was measured at several positions along the horizontal part and the water levels in the reactor simulator and steam generator simulator tanks were determined. From the measurements flooding curves basing on the Wallis parameters for gas and liquid were obtained. The results show a slight shift of the curves in dependency on pressure. In addition a slight decrease of the slope was found with increasing pressure. Additional investigations on the frequencies of liquid slugs were done.

Steady state counter-current flow limitation (CCFL) experiments were conducted in a 1:3 scaled flat model of the hot leg and part of the steam generator inlet chamber of a German Konvoi pressurized water reactor. The experiments include air-water tests at 1 and 2 bar as well as steam-water tests at 10, 25 and 50 bar. Flooding characteristics are obtained in dependency on the dimensionless gas and liquid flow rates (Wallis-parameter). They should a slight, but clear dependency on pressure – with increasing pressure more liquid can flow in counter-current to the gas in case of partial CCFL. Also the dimensionless gas flow rate for zero penetration slightly increases with pressure. Beside the flooding characteristics also slug frequencies were analyses basing on pressure measurements along the horizontal part of the test section. Finally, comprehensive video material was obtained which is suited for extracting quantitative data on the local flow structure. This can contribute to the further CFD-code development and validation.

We implement and benchmark parallel I/O methods for the fully-manycore driven particle-in-cell code PIConGPU. Identifying throughput and overall I/O size as a major challenge for applications on today's and future HPC systems, we present a scaling law characterizing performance bottlenecks in state-of-the-art approaches for data reduction. Consequently, we propose, implement and verify multi-threaded data-transformations for the I/O library ADIOS as a feasible way to trade underutilized host-side compute potential on heterogeneous systems for reduced I/O latency.

With own practical examples e.g. linking the product design of LED lamps and screens, mobile phones to metallurgy Markus Reuter will illustrate the opportunities and limitations of reaching a CE. The keynote will show simulation based design for recycling tools, developed by the author and colleague through his many years of industry and academia experience.

A new cyclotron is currently being commissioned at the Center of Radiopharmaceutical Cancer Research of the HZDR. The energy range of up to 28 MeV protons for the 18O(p,n)18F reaction required a recalculation of the neutron source terms needed in the shielding calculations, since the manufacturer supplied data was based on a 24 MeV proton beam. The radiation transport programs MCNP6 and FLUKA were used to calculate the neutron fluence emerging from the 18O-enriched water target during operation. Both Monte Carlo programs agree within 20 % on the neutron yield per incident proton for 24 and 28 MeV proton beams, while at 24 MeV, the manufacturer supplied data is considerably lower than the simulation results. To validate the radiation fields obtained in the simulations, an experimental program has been started using activation samples which are placed close to the water target of the cyclotron which is currently used to produce 18F. After irradiation, the samples are analyzed, and the resulting activation is compared to Monte Carlo calculations of the expected sample activation.

Mitteldeutscher Kreislaufwirtschaftstag
Der „Mitteldeutsche Kreislaufwirtschaftstag“ wird erstmals Elemente des Sächsischen Kreislaufwirtschaftstages und des Mitteldeutschen Entsorgungsforums zu einem neuen Fachforum vereinen. Während der eintägigen Veranstaltung wird der Status Quo der Branche in acht Vorträgen beleuchtet. Einige der Schwerpunkte sind aktuelle Entwicklungen in der europäischen und deutschen Kreislaufwirtschaftspolitik, Perspektiven für die private Entsorgungswirtschaft, Systeminnovationen, praktische Fragen zur effektiven Verwertung biogener oder mineralischer Abfälle sowie Best-Practice-Beispiele für ein abfallwirtschaftliches Behördenengineering. Zu den Referenten gehören Dr. Helge Wendenburg vom Bundesministerium für Umwelt, Naturschutz, Bau und Reaktorsicherheit, Peter Kurth vom BDE Bundesverband der Deutschen Entsorgungs-, Wasser- und Rohstoffwirtschaft, Prof. Markus Reuter vom Helmholtz-Institut für Ressourcentechnologie in Freiberg, Michael Heide von der Bundesgütegemeinschaft Recycling-Baustoffe und Dr. Hubert Seier von der DSC GmbH.

Leaching experiments of uranium(VI) doped calcium-silicate-hydrate (CSH) phases with various calcium to silicon ratios were carried out in NaCl, NaCl/Na2SO4, NaCl/NaHCO3 and NaHCO3 containing solutions to study the time-dependent release of Ca, Si and U. Potential changes of the U(VI)-CSH binding induced by leaching were monitored with time-resolved laser-induced fluorescence spectroscopy (TRLFS), infrared spectroscopy (IR), thermogravimetric analysis (TGA), differential scanning calorimetry (DSC) and powder X-ray diffraction (PXRD).

Abstract
Background & Aims: Recent studies have suggested that the enteric nervous system can modulate gut immunity. Ecto-nucleoside triphosphate diphosphohydrolases (E-NTPDases) of the CD39 family regulate purinergic signaling by sequential phosphohydrolysis of extracellular ATP, a pro-inflammatory signaling molecule. Herein, we test the hypothesis that E-NTPDases modulate neuro-immune crosstalk in gut inflammation.
Methods: We determined expression patterns of NTPDase-2 and NTPDase-3 in murine and human colon. Experimental colitis was induced by dextran sodium sulfate (DSS) in mice deficient in NTPDase-2 or NTPDase-3. We compared plasma ADPase activity from Crohn’s patients to healthy controls, and correlated levels of ADPase activity with Crohn’s disease activity.
Results: NTPDase-2 and 3 were mainly expressed in cells of the enteric nervous system in both murine and human colon. When compared to wild type, DSS-induced colitis was exacerbated in NTPDase-2 null mice, as measured by both clinical disease activity and histology, while NTPDase-3 null mice merely developed more severe anemia. Colonic macrophages isolated from NTPDase-2 null mice displayed a more pro-inflammatory phenotype compared to wild type. Crohn’s patients had decreased plasma ADPase activity when compared to healthy controls. The enzyme activity sensitive to an inhibitor against NTPDase-2 and NTPDase-3 showed the most striking difference and was inversely correlated with Crohn’s disease activity.
Conclusions: NTPDase-2 and 3 are ecto-enzymes expressed in the enteric nervous system in both murine and human colon, and are protective against gut inflammation in experimental colitis and exhibit alterations in human Crohn’s disease. These observations suggest that purinergic signaling modulated by non-CD39 NTPDases governs neuro-immune interactions that are relevant in Crohn’s disease.

Low and intermediate level waste contain cellulosic material in considerable amounts. In a repository nuclear waste is often surrounded by cementitious backfill material. If water ingresses a hyperalkaline environment will be established. Since cellulose will be relatively fast degraded under alkaline conditions, there is a high risk that small organic, water soluble molecules will be formed. These molecules can act as complexing agents for radionuclides and thereby affecting their sorption behavior and solubility adversely. Therefore the focus of current investigations is on the interaction of uranium (VI) with Isosaccharinic acid (ISA) as main degradation product of cellulose first in the acidic pH range. The progress and results of these studies within the MIND project (work package 1) will be presented.

The chromitite seams of the Lower Group (LG) and Middle Group (MG) of the Bushveld Complex in South Africa contain elevated Pt and Pd concentrations. So far, only limited work has been done on the distribution of platinum-group elements (PGE) and platinum-group minerals (PGM) in these ores. In particular, the knowledge about the effects of weathering of PGM and the redistribution of PGE in these ores are rare. Previous studies showed that the main PGM are PGE-sulfides (cooperite-braggite, malanite, laurite), followed by PGE-sulfarsenides, sperrylite and Pt-Fe alloys. During weathering PGM are largely destroyed and only relict PGM are observed. Platinum-group minerals are weathered along small cracks and neo-formation of PGM may take place. Additionally, the mineralogical siting of Ru within chromitites is studied here. It was shown by LA-ICP-MS work that chromite can host some 100s-ppb of Ru.

Herein, new ligands for the vesicular acetylcholine transporter (VAChT), based on a benzovesamicol scaffold, are presented. VAChT is acknowledged as a marker for cholinergic neurons and a positron emission tomography tracer for VAChT could serve as a tool for quantitative analysis of cholinergic neuronal density. With an easily accessible triflate precursor, aminocarbonylations were utilized to evaluate the chemical space around the C5 position on the tetrahydronaphthol ring. Synthesized ligands were evaluated for their affinity and selectivity for VAChT. Small, preferably aromatic, N-substituents proved to be more potent than larger substituents. Of the fifteen compounds synthesized, benzyl derivatives (±)-7i and (±)-7l had the highest affinities for VAChT. Compound (±)-7i was chosen to investigate the importance of stereochemistry for binding to VAChT and selectivity toward the σ₁ and σ₂ receptors. Enantiomeric resolution gave (+)-7i and (-)-7i, and the eutomer showed seven times better affinity. Although racemate (±)-7i was initially promising, the affinity of (-)-7i for VAChT was not better than 56.7nM which precludes further preclinical evaluation. However, the nanomolar binding together with the ready synthesis of [¹¹C]-(±)-7i shows that (-)-7i can serve as a scaffold for future optimizations to provide improved ¹¹C-labelled VAChT PET tracers.

Objectives:

Internal carotid-artery stenosis (ICAS) is a major public health issue, as it accounts for approximately 20% of all strokes1. However, related complex hemodynamic impairments are not well understood2. We therefore propose a multimodal MRI-protocol. The major aims were to evaluate its reliability and investigate physiological changes.
Methods:
In the ongoing clinical study, 52 subjects (29 healthy controls: 70.3±4.7y, 13 males; 23 patients with asymptomatic unilateral ICAS, NASCET>70%: 70.5±6.8y, 15 males) underwent MRI on a Philips 3T-Ingenia. We propose a combination of three different MR-based methods, accounting for cerebrovascular reactivity (CVR) by breathhold-fMRI (voxelsize 3x3x3mm3, 38 slices, TE/TR=30ms/1200ms, acq.time=5:48min), CBF by pCASL (3D-readout, voxelsize 2.7x2.8x6mm3, 16 slices, TE/TR=7.4ms/4403ms, label duration=1800ms, PLD=2000ms, acq.time 5:43min) and relative oxygen extraction fraction (rOEF) by a multi-parametric quantitative-BOLD approach3 (voxelsize 2x2x3mm3, 30 slices). For each participant, individual masks of watershed areas were defined for both hemispheres in grey-matter and mean values of all three modalities were compared.
Results:
In healthy participants, our results show no significant lateralization of all three modalities on a group level. For ICAS-patients, regionally reduced CVR (p=0.003) as well as hypoperfusion (p< 0.001) were found ipsilateral to the stenosis (figure). In accordance with the literature, we did not find ICAS-induced changes in oxygen extraction on a group level (p=0.310).4 Even though focal rOEF increases could be suspected in single patients.
Conclusions:
The presented preliminary results thus imply successful application of our multimodal-MRI approach and are highly promising with respect to gaining a deeper insight into ICAS-related physiological changes. Further investigations of the relations between the parameters are currently in progress.

Various centres of the German Helmholtz Association (HGF) started in 2012 to develop a modular data acquisition (DAQ) platform, covering the entire range from detector readout to data transfer into parallel computing environments. This platform integrates generic hardware components like the multi-purpose HGF-Advanced Mezzanine Card or a smart scientific camera framework, adding user value with Linux drivers and board support packages. Technically the scope comprises the DAQ-chain from FPGA-modules to computing servers, notably frontend-electronics-interfaces, microcontrollers and GPUs with their software plus high-performance data transmission links. The core idea is a generic and component-based approach, enabling the implementation of specific experiment requirements with low effort. This so called DTS-platform will support standards like MTCA.4 in hard- and software to ensure compatibility with commercial components. Its capability to deploy on other crate standards or FPGA-boards with PCI express or Ethernet interfaces remains an essential feature. Competences of the participating centres are coordinated in order to provide a solid technological basis for both research topics in the Helmholtz Programme "Matter and Technology", "Detector Technology and Systems" and "Accelerator Research and Development". The DTS-platform aims at reducing costs and development time and will ensure access to latest technologies for the collaboration. Due to its flexible approach, it has the potential to be applied in other scientific programs.

Fully Depleted Silicon on Insulator transistors (FDSOI) are a promising approach for further scaling. The device features a fully depleted body which is isolated by an insulator box. This introduces better electrostatics, lower leakage current and thus better channel control. The device performance is heavily influenced by the orientation, confinement and strain in the ultra-thin body. In this work the electronic structure of ultra-thin silicon layers is investigated using Density Functional Theory (DFT). The simulation parameters for the model system were calibrated to reproduce the experimental band gap of bulk silicon. This ensures that the model describes the electronic structure of ultra-thin silicon layers accurately. Our study demonstrates the impact of confinement, orientation and strain on material dependent transport properties and their influence on the device performance. For this purpose our results will be used as an input for device simulations using Synopsys Sentaurus TCAD.
We find that the band gap of the silicon layer increases with decreasing slab thickness which is a clear indication of quantum confinement. From the simulation, the band gap for the {100} confinement is found to be higher than {110} and {111} scenarios. Band gap is one of the factors which influence the intrinsic carrier in the semiconductor and thereby the transport. Another important factor for the transport is lattice strain. Strain is a useful method for modulating band structures. One good example is the transformation of direct band gap in {100} confined silicon slab to indirect band gap with 2 % biaxial compression. In our presentation we will discuss the influence of the effective mass as well. Furthermore, the strain dependence of the electronic structure and its impact on device properties is analyzed systematically.

Reconfigurable transistors (RFETs) can be switched between electron and hole current by changing the polarity of the gate potential. This allows a much higher functionality and hence, logic operations can be realized with fewer transistors. The device performance of such a transistor is strongly dominated by the contact physics.
In this work, the electron transport across the NiSi 2 -Si interface is studied using the NEGF formalism and density functional theory, which allows us to consider the atomic structure of the interface. A new model is then presented which relates the electron transport through the interface to the transfer characteristic of an RFET. The model is compared to experimental data, which shows very good agreement, especially with respect to the ratio between electron and hole current (left figure).
Based on the model, different structure variations at the interface and their consequences on the device performance are discussed. It is demonstrated that best symmetry between electron and hole current is achieved for the <110> crystal orientation, which is much worse for <100> orientation (right figure). This makes the <110> orientation advantageous for RFETs. Also the influence of strain generated parallel to the interface plane is investigated (right figure). It is shown that strain can be used to tune the symmetry in case of <110> crystal orientation even further. This is entirely different for the <100> crystal orientation, where the highest electron currents are observed for all strain states. In this state, the electron currents are about three orders of magnitude higher than the hole currents. A detailed discussion of these differences based on work function and band structure analysis will be given in our contribution.

The electron transport across metal-semiconductor interfaces is crucial for the functionality of reconfigurable field-effect transistors, which can be switched between electron and hole current. Devices were already fabricated experimentally, however, a profound understanding of the underlaying mechanism is not yet available.
This study focuses on the NiSi2-Si interface, which is studied using the NEGF formalism. Based on the calculated transmission spectra, the transfer characteristic of a reconfigurable transistor is obtained using a simplified approach. Even though this model strongly simplifies the electrostatic environment in a transistor, very good agreement with experimental devices is demonstrated. The impact of strain on the device characteristic is studied as well. It is shown that the magnitude of electron and hole current can be altered successfully. They can also be tuned to be symmetric, which fits to experimental observations. Finally, new insight into the device functionality is gained based on our calculations of the work functions and effective masses of the isolated NiSi 2 and Si.

The development of effective and ecofriendly processes for the recovery of critical elements poses a challenge for scientists all over the world. A novel approach is the generation of highly specific peptides that bind with high affinity to individual elements of interest. The peptides are selected by phage surface display (PSD) technology. In this study PSD technology has been applied in two different approaches. The focus of the first approach was the identification of peptides that bind specifically to special particles of interest that are part of electronic scrap aiming towards the development of new recycling processes. In the second approach metal ion binding peptides were isolated via PSD to use them for the targeted removal and enrichment of these elements from complex leaching solutions or from industrial waters. To address the economic production of peptides, the development of a new expression system is also part of this study.

Objectives
Molecular imaging by means of PET supports both the molecular profiling of tumors and the validation of corresponding targeted therapies in cancer treatment. The intracellular pathways triggered by nicotinic acetylcholine receptors (nAChR) mediate carcinogenic effects related to tobacco-derived compounds as well as autocrine and paracrine stimulation. In particular the α7 nAChR is of significance for the pathogenesis of cancers and may have potential for novel therapeutic concepts. Accordingly, we investigated with the in-house developed α7 nAChR-specific radioligand [18F]NS10743 the expression of α7 nAChR in the heterotopic U87-MG xenograft mouse model of glioblastoma.
Methods
Subcutaneous U87-MG tumor xenografts were generated in female NMRI nu/nu mice. [18F]NS10743 was obtained by automated radiosynthesis [1]. All animals were scanned in a nanoScan® PET/MRI system for 60 min post injection of [18F]NS10743 under control (n=5) and blocking (n=4) conditions (2 mg/kg NS6740 i.p. 15 min before the radioligand) on two consecutive days. Volumes of interest (VOI) were identified from the co-registered MR images (brain, tumor, and muscle) or from the first frame of the PET images (vena cava). Data analysis was based on the calculation of standardized uptake values (SUVs) and the shape of the time-activity curves (TACs). Intratumoral heterogeneity has been addressed by an additional VOI using a 75%-SUVmax isocontour in the control scans. Perfusion was assessed by Hoechst 33342, and autoradiography, fluorescence microscopy, and immunohistochemistry studies were performed ex vivo.
Results
Within 3-4 weeks after implantation of U87-MG cells, the longest axis of the tumor xenograft reached 5-10 mm. Dynamic PET scans, performed after i.v. administration of 6-12 MBq [18F]NS10743 (7-65 GBq/µmol at time of injection), revealed moderate uptake in the tumor with SUVmax of 0.91±0.16 at 40 min p.i. and tumor-to-muscle ratios of 0.93±0.08 at 60 min p.i. The individual tumor TACs are consistent regarding shape with relatively slow increase in the uptake of activity. NS6740 pre-blocking significantly reduced the activity uptake in the tumor (SUVmax=0.65±0.10; p<0.05).
Conclusions
Dynamic PET with [18F]NS10743 was able to detect α7 nAChR in the subcutaneous U87-MG mouse xenograft model of glioblastoma. The suitability of this approach for detection of α7 nAChR-expressing tumors in the brain remains to be investigated.
References
[1] R. Teodoro et al., Appl Radiat Isot, 2014, 95c,76-84

Grain boundaries in 2D materials can have marked influence on the material properties. The effects can be not only detrimental, but also beneficial in transition metal dichalcogenides (TMDs), so that controlling the density and type of the boundaries in these systems should be important for engineering their properties. However, this is often possibly only during the growth stage. Molybdenum and tungsten dichalcogenides feature a particular set of 60° mirror twin boundaries, which are reported to occur upon merging of the growing flakes, to appear during growth to accommodate for the nonstoichiometry of the sample, or to be produced a posteriori by electron irradiation or thermal annealing. Furthermore, different preparation conditions lead to different atomic structure of the boundary, which consequently exhibit different electronic properties. This has obviously garnered interest for the ability to control grain boundary types and densities. In this progress report, the recent experimental and theoretical work related to the characterization of mirror twin boundaries is reviewed. A consistent set of formation energies for the mirror twin boundaries is provided, which then allows a coherent picture on the formation mechanisms under different conditions to be drawn. Finally, the electronic structure of these boundaries is analyzed and their potential applications are discussed.

We have investigated the structure of atomic defects within monolayer NbSe2 encapsulated in graphene by combining atomic resolution transmission electron microscope imaging, density functional theory (DFT) calculations, and strain mapping using geometric phase analysis. We demonstrate the presence of stable Nb and Se monovacancies in monolayer material and reveal that Se monovacancies are the most frequently observed defects, consistent with DFT calculations of their formation energy. We reveal that adventitious impurities of C, N, and O can substitute into the NbSe2 lattice stabilizing Se divacancies. We further observe evidence of Pt substitution into both Se and Nb vacancy sites. This knowledge of the character and relative frequency of different atomic defects provides the potential to better understand and control the unusual electronic and magnetic properties of this exciting two-dimensional material.

Multi-dentate ligands are instrumental to extraction and separations chemistry associated with nuclear fuel reprocessing. Specifically, the TALSPEAK (Trivalent Actinide Lanthanide Separation by Phosphorus reagent Extraction from Aqueous Komplexations) process utilises DTPA to facilitate the separation of minor actinides, MA3+ (Am3+ and Cm3+), from Ln3+ and Y3+, allowing the MA3+ to be reprocessed further by transmutation. The TALSPEAK process involves the preferential extraction of the major component (Ln3+) into the organic phase using HDEHP, while the DTPA-derived ligands remain in the aqueous phase coordinating MA3+ which favour soft donor interactions. The process requires the use of lactic acid as a buffer to maintain pH 3.6 in order to prevent the precipitation of DTPA complexes at low pH, commonly experienced during the processing cycle. Amino acid conjugates derived from EDTA and DTPA present ideal candidates as self-buffering DTPA/EDTA ligands, therefore removing the need for lactic acid in the TALSPEAK process. The ligands (right) produce an internal buffer pH 1.5-2.5 at μM to mM concentrations. The synthesis, coordination chemistry, photophysical properties and separation behaviour of these new ligands and stability towards ionising radiation is presented.

Two-dimensional (2D) transition metal dichalcogenides (TMDs), like MoS2, have unique electronic and optical properties, which can further be tuned using ion bombardment and post-synthesis ion-beam mediated methods combined with exposure of the irradiated sample to precursor gases. The optimization of these techniques requires a complete understanding of the response of 2D TMDs to ion irradiation, which is affected by the reduced dimensionality of the system. By combining analytical potential molecular dynamics with first-principles calculations, we study the production of defects in free-standing MoS2 sheets under noble gas ion irradiation for a wide range of ion energies when nuclear stopping dominates, and assess the probabilities for different defects to appear. We show that depending on the incident angle, ion type and energy, sulfur atoms can be sputtered away predominantly from the top or bottom layers, creating unique opportunities for engineering mixed MoSX compounds where X are chemical elements from group V or VII. We study the electronic structure of such systems, demonstrate that they can be metals, and finally discuss how metal/semiconductor/metal junctions, which exhibit negative differential resistance, can be designed using focused ion beams combined with the exposure of the system to fluorine.

Recent pharmacologic data revealed the implication of α3β4 nicotinic acetylcholine receptors (nAChRs) in nicotine and drug addiction. To image α3β4 nAChRs in vivo, we aimed to establish the synthesis of a [¹⁸F]-labelled analog of the highly affine and selective α3β4 ligand (S)-3-(4-(4-fluorophenyl)-1H-1,2,3-triazol-1-yl)quinuclidine ((S)-T1). (S)-[¹⁸F]T1 was synthesized from ethynyl-4-[¹⁸F]fluorobenzene ([¹⁸F]5) and (S)-azidoquinuclidine by click reaction.
After a synthesis time of 130 min (S)-[¹⁸F]T1 was obtained with a radiochemical yield (non-decay corrected) of 4.3 ± 1.3%, a radiochemical purity of > 99% and a molar activity of > 158 GBq/µmol. The brain uptake and the brain-to-blood ratio of (S)-[¹⁸F]T1 in mice at 30 min post injection were 2.02 (SUV) and 6.1, respectively.
According to an ex-vivo analysis, the tracer remained intact (> 99%) in brain. Only one major radiometabolite was detected in plasma and urine samples. In-vitro autoradiography on pig brain slices revealed binding of (S)-[¹⁸F]T1 to brain regions associated with the expression of α3β4 nAChRs, which could be reduced by the α3β4 nAChR selective drug AT-1001. These findings make (S)-[¹⁸F]T1 a potential tool for the non-invasive imaging of α3β4 nAChRs in the brain by PET.

During short pulse high power laser solid matter interactions, a significant fraction of laser pulse energy is absorbed to generate an intense beam of fast electrons with relativistic kinetic energies near the critical density surface. The transport of the intense fast beam into the solid target is of fundamental importance to many complex dynamics such as plasma oscillation, heating, ionization, instability, electric field and magnetic field generation, photon emission and so on. In the talk, we will present the ultrafast plasma dynamics for ion heating in buried layer targets[1], bulk electron heating [2], collisional ionization [2,3], transport instability and quasistatic magnetic generation from PIC simulations.
In order to connect the complex plasma dynamics seen in PIC simulations with experiments, we will discuss the role of insitu synthetic diagnostics that mimic experimental diagnostics. As one key example we propose to use XRay Free Electron Lasers for probing the density modulations in the bulk target by small angle Xray scattering which allows for femtosecond and nanometer resolution of transient plasma processes. We will also discuss the feasibility to probe selfgenerated MegaGauss magnetic fields associated with the transport instability of the laser accelerated hot electrons using Faraday rotation method. With these techniques, probing fundamental plasma properties will allow for direct comparison to simulations, challenging state of the art theoretical modeling of collisions, ionizations and so on.
[1] L. G. Huang, M. Bussmann, T. Kluge, A. L. Lei, W. Yu, and T. E. Cowan, Phys. Plasmas 20, 093109 (2013).
[2] L. G. Huang, T. Kluge, and T. E. Cowan, Phys. Plasmas 23, 063112 (2016).
[3] T. Kluge, M. Bussmann, H.K.Chung, C. Gutt, L. G. Huang, M. Zacharias, U. Schramm, and T. E. Cowan, Phys.Plasmas 23, 033103 (2016).

Because of their remarkable stability towards a wide variety of transition metals1, the bidentate N-donor ligands 2,2’-bipyridine (bipy) and 1,10-phenanthroline (phen) have attracted considerable attention in the field of coordination chemistry over the last decades. The coordination chemistry of uranium (U) with these N-donor ligands has been also explored primarily for its hexavalent state (U(VI) as UO22+), whilst much less attention has been paid for the lower oxidation states, such as tetravalent (U(IV)). Here we present a systematic study on the coordination chemistry of U(IV) and -(VI) with bipy and phen under different chemical conditions, such as different solvents and changing the metal / ligand ratio.
We succeeded to obtain a series of U(IV) complexes with the U:ligand ratio of 1:1 and 1:2, all showing the eight-fold coordination geometry of the uranium centre. In addition to the ligand, chloro and methanolato ligands are also coordinating to the metal centre for charge compensation. Interestingly, the complexation between U(IV) and the ligand does occur even in protic solvents, in which the ligand is expected to be protonated. We also obtained another series of U(VI) complexes with both bipy and phen, underlining the versatile coordination chemistry of uranyl (UO22+). That is, the coordination between uranyl and the ligand depends strongly on the pH of the solvent used. For instance, as shown in the right of Fig. 1, dinuclear uranyl arrangements with hydroxo-brinding are dominated in the media with higher pH. As illustrated in Fig. 1, bipy and phen are forming isostructural complexes both with U(IV) and- (VI). The electronic structure of the complexes is further studied by quantum chemical calculations.

Because of their unique electronic properties originating from 5f-orbitals, the coordination chemistry of actinides (An) is still an attractive research field in terms not only of nuclear engineering but also of basic chemistry. In particular, the early An show profound complex chemistry due to a wide variety of possible oxidation states ranging from +II to +VII, which is in contrast to the dominant trivalent state for their chemical analog of lanthanides. The aim of our research activities is to gain knowledge about the interaction of An with a variety of hard- and soft-donor ligands, eventually providing a comprehensive understanding of the electronic nature of actinide compounds. To this end, the focus of this study lies on the characterization of Th(IV) and U(IV) complexes with the imine ligand salen and its derivative (Figure 1). The ligands possess both O- (i.e. hard) and N-donor (soft) groups in the structure, which could be also considered as a simplified model of naturally relevant organic O-/N-donor ligands.

Results and Discussion
A series of single crystals of the U(IV)-salen complexes were obtained as a function of M:L ratio and pH by liquid-liquid diffusion methods. SC-XRD measurements on the obtained crystals revealed the new crystal structures, all showing the eight-fold coordination of the U centre with a trigonal dodecahedral geometry with the ligands on the primary coordination sphere of U.
UV-visible absorption measurements of U(IV)-salen solution as a function of M:L ratio indicate the existence of two independent solution species in the system, assigning as the U(IV)-salen complexes with the M:L ratios of 1:1 and 1:2. 1H-NMR spectra of the dissolved complex [UIV(Le)2] and the pure ligand in solution were recorded. All expected multiplets of the complex can be clearly identified and confirm complexation. The spectra also showed a significant high-field shift due to proximity of the paramagnetic uranium(IV) centre, indicating that the metal is positioned at the centre of the coordination polyhedron formed by the two ligand molecules.

Understanding the interactions between radionuclides and mineral phases underpins site environmental clean-up and waste management in the nuclear industry. The transport and fate of radionuclides in many subsurface environmental systems are controlled by adsorption, redox and mineral incorporation processes. Interactions of iron (oxyhydr)oxides with uranium have been extensively studied due to both the abundance of uranium as an environmental contaminant and the ubiquity of iron (oxyhydr)oxides in engineered and natural environments. Despite this, detailed mechanistic information regarding the incorporation of uranium into Fe(II) bearing magnetite and green rust is sparse. Here, we present a co-precipitation study where U(VI) was reacted with environmentally relevant iron(II/III) (oxyhydr)oxide mineral phases. Based on diffraction, microscopic and spectroscopic evidence, we propose the reduction of U(VI) via a one electron transfer to U(V) and stabilisation of the U(V) by incorporation during co-precipitation with iron (oxyhydr)oxides. U(V) was stable in both magnetite and green rust structures and incorporated via substitution for octahedrally coordinated Fe in a uranate-like coordination environment. As the Fe(II)/Fe(III) ratio increased, a proportion of U(IV) was also precipitated as surface associated UO2. These novel observations have significant implications for the behaviour of uranium within engineered and natural environments.

The fundamental oscillation mode of magnetic vortices in thin-film elements has recently been proposed for designing spin-torque-driven nano-oscillators [1]. Commercial applications require tuning of the output frequency by external parameters, such as applied fields or spin-polarized currents. However, the tunability of vortex-based devices is limited, since the gyrotropic frequency is specific to the individual sample design. Indeed, the fundamental frequency is known to be determined by the saturation magnetisation, M_s , as well as the geometrical confinement of the magnetisation e.g. the diameter and height of a magnetic disk [2, 3]. Micromagnetic simulations [4] have shown that if regions with different saturation magnetisation can be induced in a magnetic disk, multiple precession frequencies can be generated. Ion implantation is a promising method to fabricate such devices [5].
To study the formation of magnetic vortices with respect to size and thickness, disks with different radii- 0.5 µm to 4 µm and thicknesses- 25 nm and 30 nm were prepared using electron beam lithography followed by electron beam evaporation. Moreover, to allow for electrical measurements, the single disks were contacted by gold leads to study the interaction of spin polarized current on the magnetic vortex. The presence of vortex is verified by magneto optic Kerr effect (MOKE), X-ray magnetic circular dichroism (XMCD) and magnetotransport measurements.
The magnetic field dependence can be tuned by the disk size as shown by XMCD (Figure 1 (a)). Higher magnetic stability due to larger annihilation fields can be achieved by smaller disk diameters whereas larger field sensitivity is present in larger disks (Figure 1 (b)).
Magnetotransport measurements on electrically contacted disks (Figure 2 (a)) show the presence of anisotropic magnetoresistance (AMR) in different disks with varying thickness (Figure 2 (b)). Additionally, to the shown static DC measurements, AC measurements are accessible by a lock-in technique and the resonance frequencies measured for 3 µm and 4 µm radii disks with 25 nm permalloy are 40.9 MHz and 29.5 MHz respectively. In order to alter the saturation magnetisation within defined volumes and to achieve two different oscillation frequencies, a concentric region is irradiated within the actual disk (Figure 2 (c)). After ion irradiation, modified magnetic vortex dynamics are investigated by ac-magnetotransport measurements and the results are supported by micromagnetic simulations.
Acknowledgements:
This work is supported by the Helmholtz Young Investigator Initiative Grant No. VH-N6-1048. Support of the Nanofabrication Facilities of Rossendorf at the Ion Beam Centre is gratefully acknowledged (Dr. Artur Erbe, Bernd Scheumann).

The magnetic “vortex” is a potential candidate for future spintronic devices, like frequency sensors [S. Kasai, et al. PRL 97, 107204 (2006)] [R. Moriya, et al. Nat. Phys. 4:368 (2008)], spin torque oscillators [V. S. Pribiag, et al. Nat. Phys. 3:498 (2007)], and tunable magnonic crystals [J. Shibata, et al. PRB 67, 224404 (2003)]. The fundamental frequency is determined by the saturation magnetisation, as well as the geometrical confinement of the magnetisation i.e. the diameter and height of a magnetic disk. In this study, Permalloy disks (with diameters ranging from 1µm to 8µm) are patterned and contacted to study the interaction of spin polarized current on the magnetic vortex. The presence of vortex is verified by magneto optic Kerr effect, X-ray photoemission electron microscopy and magnetotransport measurements. The resonance frequency is measured using a lock-in technique based on the anisotropic magnetoresistance effect. Modification of the resonance frequency by ion irradiation will be presented.

Magnetic tunnel junctions have been commonly used in spintronics applications, such as magnetic random access memory (M-RAM), spin transfer torque RAM (STT-RAM) and hard disc drive (HDD) because of high storage capacity. A spin polarized current flowing through a ferromagnetic layer can exert spin-transfer-torque (STT) on the local magnetization. When we apply thermal gradient across the junction we can induce what is called thermal spin transfer torque (T-STT). In this study, the microresonator FMR technique is used in order to analyze how the ferromagnetic resonance signal corresponding to the free layer of an in-plane MgO-based tunnel junction device is modified in the presence of a temperature gradients across the barrier. Details of resonator fabrication and preliminary measurements are presented. This work is supported by DFG-SPP1538.

In contrast to the dominant trivalent state for the lanthanides (Ln(III)), a wide variety of oxidation states (from +II to +VII) of actinides (An) makes their chemistry intricate but attractive. Especially the early An of thorium (Th), uranium (U), neptunium (Np) and plutonium (Pu) form highly charged cations with the oxidation state four (An4+), which are of particularly interest for the coordination chemistry due to their strong interaction with organic ligands. The focus of our investigations lies in the comprehensive characterization of tetravalent An (An(IV)) complexes with soft ligand donor atoms, such as nitrogen. The present study focuses particularly on the interaction of An(IV) with benzamidinate ligands, which could be considered as a simplified model of naturally occurring N-donor organic compounds.
Recently, the lanthanide complexes with the chiral benzamidine, (S,S)-N,N-Bis-(1-phenylethyl)-benzamidine ((S)-HPEBA), have been successfully synthesized by the group of Prof. Roesky1,2. The present study is inspired by these precedent studies to synthesize a new series of benzamidine compounds with An(IV).

Ferrimagnet HoFe₆Al₆ (tetragonal ThMn₁₂-type crystal structure) has a compensation point for the Ho and Fe magnetic sublattices at a temperature close to absolute zero. The experimental study was carried out in fields up to 60 T. H-T phase diagrams and a full magnetization process along the principal crystallographic directions of a single-crystalline sample are obtained theoretically by using a model of a f-d ferrimagnet with two anisotropic sublattices, coupled by weak exchange interaction. The two first-order phase transitions, found experimentally along the [110] and [100] axes, were explained theoretically. The transition along the [110] direction occurs between noncollinear and collinear phases, it starts at the compensation point and ends at a tricritical point around 60 T. The transition along the [100] direction goes also from the point of compensation to the point of the liquid-vapor type at 40 T. This transition was shown to occur between two distinct noncollinear phases. The crucial role of the strong rare-earth anisotropy for the positions of the obtained critical points was revealed.

Combined strain and magnetization measurements on the Heusler shape-memory alloys Ni₄₅Co₅Mn₃₈Sb₁₂ and Ni₄₄Co₆Mn₃₈Sb₁₂ give evidence for strong magneto-structural coupling. The sample length changes up to 1% at the martensitic transformation, between a ferromagnetic, austenitic phase at high temperatures and a weakly magnetic, low-symmetry martensitic phase at lower temperatures. Under moderate uniaxial stress, the change in the sample length increases to and saturates at about 3%, pointing to stabilization of a single martensitic variant. A reverse martensitic transformation can also be induced by applying magnetic field: we find that within the temperature range of thermal hysteresis of the martensitic transformation, applying a field can induce a metastable expansion of the sample, while at slightly lower temperatures, the field response is reversible. These findings provide key information for future use of Ni(Co)-Mn-Sb-based Heusler compounds in, e.g., actuators and mechanical switches.

We report on the investigation of dielectron production in tagged quasi-free neutron-proton collisions by using a deuteron beam of kinetic energy 1.25 GeV/u inpinging on a liquid hydrogen target. Our measurements with HADES confirm a significant excess of e+e− pairs above the π0 mass in the exclusive channel dp→npe+e−(pspect) as compared to the exclusive channel ppe+e− measured in proton-proton collisions at the same energy. That excess points to different bremsstrahlung production mechanisms. Two models were evaluated for the role of the charged pion exchange between nucleons and double-Δ excitation combined with intermediate ρ-meson production. Differential cross sections as a function of the e+e− invariant mass and of the angles of the virtual photon, proton and electrons provide valuable constraints and encourage further investigations on both experimental and theoretical side.

Since the Fukushima accident the spent fuel pool has gained some special focus in nuclear safety research, since it is potentially endangered by a longer persisting station black-out or a loss of the coolant due to a leakage in the pool liner. Behind this background the German national joint project SINABEL (SIcherheit NAsslager BrennElement Lagerbecken) has been launched, which targets an experimental investigation and an improved modelling of the thermal hydraulics in fuel element mock-up in the spent fuel pool under accident scenario conditions. The goal is to develop validated simulation tools for the prediction of temperature courses and the support of the emergency management.
Experimental investigations within the project are performed in a mock-up of a 10 x 10 boiling water reactor fuel element. Surface temperatures of the electrical heated rods are measured by means of 134 thermocouples at different locations. Another parameter of interest is the steam flow velocity in the sub-channels. For this purpose no commercial measurement technique is applicable due to limited accessibility and high temperatures. For this reasons a special thermal anemometry grid sensor has been developed. It consists of a grid of thermal resistors in the bundle cross-section with one resistor in each sub-channel. Via the resistors fluid temperature as well as flow velocity can be obtained. Applied measurement techniques are resistance thermometry and thermal anemometry respectively. The measurements are obtained simultaneously by sampling the data with a special multiplexed excitation scheme. Our contribution gives a brief description of the thermal anemometry grid sensor along with first results from studies on a potential natural circulation in the completely dried state.

Low-frequency neutronic noise with a bandwidth of up to ten percent of the reactor power has been observed in Konvoi-type PWRs in Germany in the last years. Several attempts were made to identify the reasons for increased magnitudes of the neutronic fluctuations in comparison with pre-Konvoi reactors, and various hypotheses have been created to explain this effect.
In this paper, results of noise simulations performed with use of the reactor dynamics code DYN3D are presented. Both fluctuations of the coolant inlet temperature and mass flow rate were considered. Besides of un-correlated fluctuations, correlated temperature fluctuations were simulated. The correlations between fluctuations in the individual fuel assemblies were obtained based on an experimentally validated coolant mixing model. However, the features of the neutronic noise found in the simulations do not correspond to the measurements.
Obviously, more complex mechanisms than only temperature and/or mass flow fluctuations have to be considered. Simulated fluctuations of the local moderator density, independently from thermal hydraulics, indicate that potentially deformations or vibrations of the fuel rod lattice leading to variations of the local moderator content might be responsible for the observed neutronic noise. Advanced models coupling neutronics, thermal hydraulics, turbulence and mechanical modelling have to be developed.

Some features of the field induced phase transition accompanied by the vacuum creation of an electron-positron plasma (EPP) in strong time-dependent electric fields have been discussed in the work [1] in the domain of the tunneling mechanism (ω ≪ m, where ω is the characteristic frequency of the external field and m is the electron mass). In the present contribution the features of this process will be considered in the few photon domain where ω ~ m. We observe a narrowing of the transient domain of the quickly oscillations and, mainly, a considerable growth of the effectiveness of the EPP production. Under these circumstances, we see an increase of the effectiveness of the EPP creation in the particular case of a bifrequent excitation, where both mechanisms (tunneling and few photon) act simultaneously [2, 3].

Integrated small animal X-ray imaging and irradiation devices have facilitated image-guided pre-clinical radiooncological experiments. Here, a proton-based radiography method is proposed for in-line small animal treatment planning and positioning verification at an experimental proton beamline.
A double-scattered 125 MeV proton beam (10 x 10 cm² field size) and a flat-panel, scintillation-based dose detector (Lynx, IBA Dosimetry) were used to obtain planar scans of deceased mice positioned in a closed multi-modality bed. Two modes of image acquisition were used: absorption and scattering. In absorption mode, slabs of plastic with a water equivalent path length (WEPL) of 7.08 g/cm² were placed between object and Lynx detector. In scattering mode, all plastic slabs were removed. Digital, pixel-wise image processing was applied to combine the information. A WEPL calibration curve was obtained using plastic slices of known WEPL as objects. For verification, planar X-ray images of the same objects were acquired.
The proposed radiography technique allowed for detection of contours (e.g., mouse body, bed and background) and reliable automated (rigid) registration of proton radiography images to planar X-ray scans. Planar 2D radiological thickness maps of mice were obtained. Specific structures could be visualized with a spatial resolution of less than 1 mm, especially regions with high local density differences including lung, hind leg, jaws and skull.
The method appears suitable to position small animals for precise irradiation of subcutaneous (hind leg) and orthotopic (lung, brain) tumor models. Currently extended image analysis may enhance visualization of the animal’s internal structure to facilitate in-line treatment planning.

Multiple year-round (2006-2015) records of the bulk and size-segregated composition of aerosol were obtained at the inland site of Concordia located in East Antarctica. The well-marked maximum of non-sea-salt sulfate (nssSO₄) in January (84 ± 25 ng m^-3 against 4.4 ± 2.3 ng m^-3 in July) is consistent with observations made at the coast (280 ± 78 ng m^-3 in January against 16 ± 9 ng m^-3 in July at Dumont d’Urville, for instance). In contrast, the well-marked maximum of MSA at the coast in January (60 ± 23 ng m^-3 at Dumont d’Urville) is not observed at Concordia (4.6 ± 2.4 ng m^-3 in January). Instead, the MSA level at Concordia peaks in October (5.6 ± 1.9 ng m^-3) and March (13.2 ± 6.1 ng m^-3).
As a result, a surprisingly low MSA to nssSO₄ ratio (RMSA) is observed at Concordia in midsummer (0.05 ± 0.02 in January against 0.25 ± 0.09 in March). We find that the low value of RMSA in mid-summer at Concordia is mainly driven by a drop of MSA levels that takes place in submicron aerosol (0.3 μm diameter). The drop of MSA coincides with periods of high photochemical activity as indicated by high ozone levels, strongly suggesting the occurrence of an efficient chemical destruction of MSA over the Antarctic plateau in mid-summer. The relationship between MSA and nssSO₄ levels is examined separately for each season and indicates that concentration of non-biogenic sulfate over the Antarctic plateau does not exceed 1 ng m^-3 in fall and winter and remains below 5 ng m^-3 in spring. This weak non-biogenic sulfate level is discussed in the light of radionuclides (²¹⁰Pb, ¹⁰Be, and ⁷Be) also measured on bulk aerosol samples collected at Concordia. The findings highlight the complexity in using MSA in deep ice cores extracted from inland Antarctica as a proxy of past DMS emissions from the southern ocean.

For the safety case for high-level radioactive waste repositories, redox phenomena play an important role for radionuclide retention. In the near field, the corrosion of steel canisters will release large amounts of ferrous iron and in addition produce H2 with a strong influence on the “in situ” redox potential (Eh). This combination of high {FeII} and low (Eh) in the interstitial waters of the engineered barrier system (bentonite, consisting predominantly of the phyllosilicate montmorillonite) is expected to have a strong impact on the retention of redox sensitive radionuclides like Tc, Se and the early actinides U, Np, and Pu, all of high relevance for safety of radioactive waste repositories.
In the present work we investigated by X-ray absorption spectroscopy (XAS) the influence of FeII on the retention of the redox sensitive NpV by montmorillonite. Since natural montmorillonite always contains structural Fe, we made use of a synthetic iron-free montmorillonite (IFM) [1] to discriminate the influence of sorbed FeII from that of structural iron. For FeII loadings below 40 mmol·kg-1, sorbed Fe had no effect, with Np showing the typical sorption behaviour of the pentavalent aquo-ion by forming comparatively weak inner-sphere sorption complexes at the edge sites of montmorillonite. For FeIIsorb above 40 mmol·kg-1, however, we observed an increasing reduction of NpV to NpIV, with a complete reduction for FeIIsorb  80 mmol·kg-1. In spite of the low solubility of NpO2, we did not observe precipitation of this phase, but formation of mononuclear innersphere sorption complexes (Fig. 1-A). The influence of structural FeII was investigated using citrate-dithionite–bicarbonate (CDB) reduced SWy montmorillonite (i.e. structural FeIII fully reduced to FeII). XAS showed that Np is present only as NpIV on the clay surface (Fig. 1-B).
Our study demonstrates that both structural and adsorbed FeII on montmorillonite lead to a surface mediated reduction of NpV, thereby increasing the retention by more than two orders of magnitude.

Technetium–99 is a β–emitting fission product which needs to be analysed for the safety assessment of repositories for radioactive waste disposal due to its significant inventory in spent nuclear fuel and its long half-life (t½ ~211.000 a). Although several oxidation states of Tc are reported in the literature, Tc(VII) and Tc(IV) are the prevailing redox states in the absence of any complexing ligand under non-reducing and reducing conditions, respectively. Tc(VII) is the most stable oxidation state of Tc in suboxic/oxidising environments. It is found as the highly mobile TcO4– anion over the entire pH range and shows very high solubility and weak sorption properties. Under reducing conditions, Tc(IV) forms sparingly soluble hydrous oxides TcO2∙xH2O(s) and is usually sorbed strongly onto mineral surfaces. Because of the large differences in the aquatic chemistry of Tc(VII) and Tc(IV), an accurate knowledge of Tc redox chemistry is necessary for an appropriate assessment of Tc retention/mobilization processes.
In the present work, the mechanisms for the reduction and uptake of Tc by magnetite (Fe3O4) and mackinawite (FeS) are investigated using X-ray absorption spectroscopy, in combination with thermodynamic calculations of the Tc/Fe systems and accurate characterization of the solution properties (pHm, pe, [Tc]). Batch sorption experiments were performed under strictly anoxic conditions using freshly prepared magnetite and mackinawite in 0.1 M NaCl solutions with varying initial Tc(VII) concentrations (2·10–5 and 2·10–4 M) and Tc loadings (400–900 ppm). EXAFS data evaluation shows that the mechanisms of Tc(IV) retention by magnetite and mackinawite are strongly dependent on the loading, [Tc]0 and pHm. The results provide key inputs for the understanding of the mechanisms driving the reduction and retention of Tc by magnetite and mackinawite under repository-relevant conditions, whilst highlighting the need of coupling classical wet-chemistry techniques, thermodynamic calculations and advanced spectroscopic methods when investigating complex processes or systems such as redox and mineral interfaces.

Peatlands play an important role in arsenic sequestration. In such carbon-rich and sulfidic environments the dominant species is generally assumed to be arsenite for which recent X-ray absorption spectroscopy (XAS)-based studies showed that it can strongly bind to natural organic matter (NOM) via reduced sulfur bridges [1]. However, in sulfidic solutions, arsenite can also react with sulfide or elemental sulfur to form thioarsenates. Thioarsenates are often overlooked due to a lack of suitable analytical methods [2] and their mobility in organic-rich systems is unknown. Porewater analysis of an arsenic-rich, minerotrophic peatland (Gola di Lago, Switzerland) showed that thioarsenates actually accounted for up to 70 % of total porewater arsenic, with monothioarsenate (MTA) being the dominant species. To investigate the extent, kinetics, and mechanisms of MTA binding to NOM, MTA was incubated with sulfurized peat at pH 4.5, 7.0, and 8.5. While MTA was stable for 41 days at pH 8.5, it was completely transformed to arsenite at pH 4.5, following acid-catalyzed and sulfide-dependent redox transformation kinetics. Total arsenic sorption was lowest at pH 8.5 and highest at pH 4.5 (7 and 32 μmol As/mol C, respectively). XAS revealed that in this sulfidic system, arsenic was bound to NOM as previously reported via reduced sulfur bridges as arsenite and additionally via oxygen as arsenite at low to neutral pH or as arsenate and low amounts of arsenite via oxygen at high pH. MTA did not bind to sulfurized NOM at all. The results demonstrate that the mobility of arsenic in sulfidic, organic-rich systems strongly depends on the pH, the sulfide-to-arsenic and the sulfide-to-carbon ratios which govern thioarsenate formation in solution, their transformation to arsenite and finally its sorption kinetics.
[1] Langner et al. (2012) Nat. Geosci. 5, 66-73. [2] Planer-Friedrich et al. (2015) Environ. Sci. Technol. 49, 6554-6563.

The interaction of radio(-contaminants) at water-mineral interfaces is a key process in retarding their migration in the environment. Therefore, elucidation of the processes involved, and the development of sorption models accounting for these processes, is crucial for a reliable risk assessment. This task can realistically only be tackled, if for a given multimineralic soil or rock the most relevant minerals can be identified. Only for these, the sorption processes need to be determined and modelled, and the sorption by the soil/rock entity is then predictable by summing up the sorption of these few minerals according to their fraction in the soil or rock.
Here we show that this procedure can already be hampered at the level of a presumably pure mineral. Sorption experiments conducted with purified illite du Puy showed under certain conditions (pH, concentration, dissolved carbonate) an unexpected enhancement of the retention of UVI and EuIII. EXAFS and TRLF spectroscopies revealed that this effect is due to the interaction with phosphate groups not expected at the illite surface. Only after a severe acid treatment of the illite, sorption and surface complexation approached that expected for pure illite. The release of Ca and P during the severe acid treatment suggest dissolution of an apatite-type accessory mineral. The mineral itself is difficult to identify with common analytical methods such as XRD or TEM due to i.e. low concentration and/or amorphous nature of the accessory phase, low electron density of its constituent elements. Our results demonstrate that accessory phases might substantially contribute to the sorption of a bulk mineral phase.

SIMS (Secondary Ion Mass Spectrometry) is a routinely used analytical technique for geochemical and mineralogical applications. Nevertheless, quantification is still the major challenge of this method. Due to the fact, that each analysed matrix needs its own matrix-matched reference material (RM), the list of available reference materials is short compared to the needs of the analysts. A current evaluation of the GeoReM database [1] shows a strong focus on using the well-known NIST SRM 610-617 glasses for trace element analysis and several zircons for isotope analysis.

One approach for the production of suitable RMs is the use of ion implantation to introduce a known amount of an isotope into a matrix-matched material. This approach is widely-used for SIMS applications in materials science, but rarely used for geochemical problems. Bumett et al. (2014) [2] demonstrated the principal appropriateness of this method and ways to calibrate nominal implant fluence. We choose the more elaborate way of implanting a box profile to allow a homogeneous distribution of the respective isotope in all three dimensions.

The mineralogical and chemical “simple” SiO₂ system entails many interesting scientific challenges like the Ti-in-quartz geothermometer [3, 4]. We implanted ⁴⁷Ti respectively ⁴⁸Ti into synthetic ultra-high purity silica glass. Several box profiles with concentrations between 10 and 1000 ppm and a maximum depth of homogeneous ^47/48Ti distribution between 200 and 500 nm were produced at the Ion Beam Center in Dresden-Rossendorf. The single implantation steps with different ion-energies and -doses were simulated with the SRIM (Stopping and Range of Ions in Matter) software [5] and optimized to the necessary concentrations, implantation-depths and limits of the implanter. After the implantations, the surface-roughness of the implanted glasses was measured using atomic force microscopy (AFM). The roughness is still in the range necessary for SIMS measurements.

We characterized several implanted test-samples with different concentrations and maximum implantation-depths by means of SIMS and other analytical techniques. It has been shown, that Ti is dissolved in the glass structure. The homogeneity of the Ti-concentration is within ± 5% uncertainty in all 3 dimensions.

[1] http://georem.mpch-mainz.gwdg.de
[2] Bumett, D.S., et al. (2014). Ion Implants as Matrix-Appropriate Calibrators for Geochemical Ion Probe Analyses. Geostandards and Geoanalytical Research, 39(3), 265-276.
[3] Wark, D. A., Watson E. B. (2006). TitaniQ: a titanium-in-quartz geothermometer. Contributions to Mineralogy and Petrology, 152(6), 743-754.
[4] Thomas, J. B., Watson E. B., et al. (2010). TitaniQ under pressure: the effect of pressure and temperature on the solubility of Ti in quartz. Contributions to Mineralogy and Petrology, 160(5), 743–759.
[5] Ziegler J. F. (2004). SRIM-2003. Nuclear Instruments and Methods in Physics Research Section B, 219-220, 1027-1036.

Current endeavor experimentally studies the initial bubble size distribution from the stainless steel diffusers and needle spargers with very fine orifice diameters range from 30 to 200 µm. To evaluate the performance of these spargers, the results where compared with four industrial rubber membranes in terms of Sauter mean diameter, pressure drop and frequency of bubble formation. Outcomes of current study showed that, the stainless steel perforated plates impose their superiority over the flexible membranes, by generating 50% smaller bubbles, and 70% higher bubble generation frequency at 60% less pressure drop. Moreover, the perforated stainless steel plates are able to produce bubble sizes in the same class as needles at 40% of the pressure drop caused by needle spargers and average of 60% higher bubble generation frequency.

In this talk I will present our recent experimental investigations on carrier dynamics in graphene studied via nonlinear laser spectroscopy, on time-resolved photoluminescence dynamics of single InAs/GaAs quantum dots under pulsed inter-sublevel excitation, and on sub-diffraction limited terahertz imaging by a GaAs-based superlens studied by scattering near-field optical microscopy. The experiments have been carried out using the mid-infrared/terahertz free-electron laser facility FELBE in Dresden, Germany.

The TALSPEAK process [1] was developed at Oak Ridge National Laboratory in the 1960’s to separate trivalent actinide ions, An(III), from the chemically similar lanthanide ions, Ln(III), by solvent extraction. The idea was to use an extracting agent unselective for An(III) over Ln(III) and add a complexing agent to the aqueous phase to infer selectivity [2]. Despite the simplicity of this concept, TALSPEAK is actually a rather complex system, with numerous equilibria involved. The original TALSPEAK system consisted of HDEHP (bis-2-ethylhexyl phosphoric acid) as the extracting agent, DTPA (diethylenetriamine pentaacetic acid) as the An(III)-selective complexing agent and lactic acid as buffering agent. Constantly improving TALSPEAK by substituting the components of the original system, ALSEP [3] and Advanced TALSPEAK [4, 5] have been developed.
We have pursued a concept which differs in two aspects, (a) using amino acids (AA) as buffering agent [6] and (b) linking them to the complexing agent. This way, only a single molecule is added to the aqueous phase and the system is expected to behave more simply. Several DTPA-AA conjugates were synthesised, DTPA-Arg, DTPA-His, DTPA-Ser and DTPA-Ala. These were tested in solvent extraction experiments. Organic phase was 0.2 mol/L HDEHP in kerosene, aqueous phases were solutions containing 50 mmol/L DTPA-AA conjugate, Am(III) and Ln(III) (Y; La–Lu). pH was adjusted by adding HNO3 or NaOH.
The lowest pH at which separation was achieved (i.e., Am(III) distribution ratio < 1 and all Ln(III) distribution ratios > 1) was in the range of 1.1–1.5. Separation factors for Eu(III) over Am(III) were ≈ 100 and the minimum separation factors between Am(III) and the least extracted Ln(III), being Nd(III) in all cases, were 30–40.
The coordination chemistry was studied by luminescence and NMR. Photophysical studies of the Eu(III)-DTPA-AA complexes demonstrated characteristic Eu(III) emission, with associated lifetime decay profiles confirming 1:1 coordination. 1H NMR studies were performed with Am(III), confirming successful complexation.
In conclusion, an improved TALSPEAK system is reported which compares favourably to known TALSPEAK systems.
1. Weaver, B.; Kappelmann, F. A., USAEC report ORNL-3559, Oak Ridge National Laboratory, USA: 1964.
2. Nilsson, M.; Nash, K. L., Solvent Extr. Ion Exch. 2007, 25 (6), 665–701.
3. Gelis, A. V.; Lumetta, G. J., Ind. Eng. Chem. Res. 2014, 53 (4), 1624–1631.
4. Braley, J. C.; Grimes, T. S.; Nash, K. L., Ind. Eng. Chem. Res. 2010, 51 (2), 629–638.
5. Lumetta, G. J.; Casella, A. J.; Rapko, B. M.; Levitskaia, T. G.; Pence, N. K.; Carter, J. C.; Niver, C. M.; Smoot, M. R., Solvent Extr. Ion Exch. 2015, 33 (3), 211–223.
6. Grimes, T. S.; Tillotson, R. D.; Martin, L. R., Solvent Extr. Ion Exch. 2014, 32 (4), 378–390.

THz spectroscopy of solids with a free electron laser

Purpose: X-ray based position verification of the target volume in image-guided radiation therapy (IGRT) of patients with pancreatic ductal adenocarcinoma (PDAC) is currently performed on rigid fiducial markers that are implanted under endoscopic ultrasonography. A new biodegradable liquid fiducial marker has recently been introduced. To assess its potential use for magnetic resonance imaging (MRI) guided radiotherapy of PDAC, the MRI visibility and artefacts of this marker were quantified and compared against rigid gold markers.

Material and Methods: Different spherical volumes (10 µL, 25 µL, 50 µL and 100 µL) of BioXmark® (Nanovi Radiotherapy A/S) as well as four differently oriented Gold Anchor™ (Naslund Medical AB; Ø 0.28 mm, 1 cm and 2 cm length) and three VisiCoil™ (IBA Dosimetry; Ø 0.35 mm, 5 mm and 10 mm length) were implanted in a spherical gel phantom mimicking the proton spin relaxation properties of healthy pancreatic tissue at 3 Tesla. MR relaxometry was performed to quantify the size and magnitude of the decrease in T¬2* relaxation time and relative proton density ρ(H) as a measure of visibility, and to quantify the size and magnitude of the increase in magnetic field inhomogeneity ΔB_0 as a measure of signal artefacts. The phantom was scanned in a 3.0 T Philips Ingenuity TF PET/MR scanner with an 8-channel head coil. For T2*- and ΔB_0-mapping a spoiled 3D multi-echo gradient echo sequence (GRE) was performed. ρ(H)-mapping was based on the signal intensity at TE = 0 ms relative to ultrapure water extrapolated from the T2-decay curve deduced from a spin echo sequence with different echo times. The signal was corrected for its T1 decay and B1- field inhomogeneity, for which an inversion-recovery spin echo sequence with multiple inversion times and a gradient echo sequence with different repetition times was utilized respectively.

Results: The rigid markers showed a direct linear relationship between size of visibility and artefact. BioXmark® showed a tendency towards larger size of visibility at smaller artefacts. BioXmark® markers up to 100 µL created volumes of visibility comparable to the size of visibility of VisiCoil™ and Gold Anchor™ markers. The magnitude of visibility was the highest for BioXmark® from 25µL – 100µL showing no correlation with the magnitude of artefact. The rigid markers show a non-linear correlation between magnitude of visibility and artefact where Gold Anchor™ induce the strongest artefacts.

Conclusion: BioXmark® causes signal voids on MRI due to its low proton density without strongly affecting the magnetic field in the surrounding tissue. The latter was found to be the main effect leading to the visibility of the rigid markers especially in GRE sequences. Hence, especially when a low level of image distortion is required, MRI characteristics of the BioXmark® surpass those of rigid gold markers currently being used for IGRT of PDAC.

For preclinical cancer research, dedicated small animal imaging and irradiation devices are increasingly gaining importance to examine experimental tumors and normal tissue models. We designed a special small animal bed, which is intended to be used for multimodal imaging (e.g. MRI, CT, PET) and image-guided treatment with different radiation types (e.g. photons, protons). The multimodality small animal bed was constructed with CAD software and produced with a 3D printer using the fused deposition modeling procedure. The bed is made of thin acrylonitrile butadiene styrene (ABS), which is fully compatible with magnetic fields, barely influence radiation and is chemically resistant against most frequently used disinfectants. To facilitate proper positioning and alignment of the animal, the bed contains a tooth bar and ear pins for cranial fixation as well as a detachable distal foot holder for the hind leg. For inhalation anesthesia, a respective mask is integrated. To avoid hypothermia, the bed is supplied with a controllable stream of HEPA-filtered warm air. Furthermore, the respiration of the animal can be monitored during the experiment using a respiratory cushion. Suitability of the prototype was tested for photon and proton irradiation as well as CT imaging and proton radiography. In conclusion, the designed multimodality bed enables standardized positioning of small animals and provides integrated solutions for their anesthesia, warming and monitoring. Ist use for multimodal monitoring and image-guided irradiation of experimental tumors will simplify the workflow and image analyses for preclinical radiooncological investigations.

The Hämmerlein skarn deposit, located in the western Erzgebirge (Germany), consists of a cassiterite-dominated Sn mineralization associated with minor Zn-Cu-In sulphide mineralization. In this contribution, we describe the nature of the sulphide-associated In mineralization based on underground mapping, mineralogical methods (microscopy, SEM-based MLA studies and EPMA X-ray element maps) and mineral chemistry data (quantitative EPMA data).
In-bearing sphalerite and roquesite [CuInS2] are closely associated with paragenetically late In-bearing chalcopyrite (average 0.15 wt% In). Sphalerite contains up to 20 wt% In as well as elevated Cu contents. The highest In concentrations occur exclusively at rims and along cracks of sphalerite grains. The appearance resembles diffusion profiles, suggesting that In enrichment is due to an hydrothermal overprint that postdates the formation of sphalerite. Detailed textural observations show that the diffusion fronts in sphalerite grains are thicker where they are in contact to anhedral masses of hematite and magnetite that are regarded as product of decomposition of of In-bearing chalcopyrite. Hematite and magnetite have In concentrations below the detection limit (EPMA). Indium and Cu, released by the decomposition of In-bearing chalcopyrite, were incorporated into sphalerite along grain boundaries and cracks.. EPMA element distribution maps indicate that the In enrichment in sphalerite is related to the coupled substitution of Cu+ + In3+ ↔ 2 Zn2+ [1].

[1] Johan (1988) Mineralogy and Petrology 39, 211–229.

Mineral Systems Analysis aims to provide a holistic understanding of geological processes required to form and preserve ore deposits at all scales [1]. Detailed knowledge of the ore-forming process alone does thus not suffice. Instead, comprehensive knowledge is required, taking into consideration all drivers of a given mineral system, including geodynamic setting and crustal architecture, crustal fertility (metal source), metal transport mechanism, processes of local concentration (trap) as well as postdepositonal alteration and preservation. Robust conceptual models are the result of Mineral Systems Analysis; these models are used to efficiently identify exploration targets or target regions [2].
Mineral Systems Analysis has generally not been applied to the Variscan Orogen, despite its exceptional endowment in mineral deposits. This is attributable to a severe lack of modern geoscientific data for most of the known mineral deposits many of which have ceased production decades ago. As a direct consequence, our understanding of the mineral system of the Variscan Orogen is rather tentative. We illustrate the state of knowledge on selected examples and illustrate how the use of state-of-the-art geochemical data, combined with current regional geotectonic understanding, vastly improve our understanding – and enable us to carry out Mineral Systems Analysis. This, in turn, will provide a suitable foundation for future exploration targeting.

The oldest known granular iron formation (GIF) occurs in the ca. 2.96¬–2.92 Ga Mozaan Group of the Pongola Supergroup of southern Africa. The GIF comprises stacked beds interbedded with deeper water facies iron formation. The chert granules are marked by irregular rims composed of magnetite and calcite and can be defined as oncoids. Initial geochemical studies showed that the calcite is isotopically light, suggesting an organic carbon source for CO2, and that the Fe isotope characteristics of shallower water GIF are decoupled from those in the deeper water iron formation. Due to the complexity of the oncoidal rim morphologies, traditional petrography is complicated by the bias inherent to 2D intersections of the samples. However, the different mineral densities allow successful µXCT application revealing that rim morphologies are fairly homogenous consisting of multiple, multi-directional, micro-scale chert, magnetite and calcite domes surrounding the granule cores. The chert cores of the granules and domes suggest continuous chert precipitation in a wave-reworked environment. A surprising result was that calcite was not limited to the granule rims, and that some granules contain abundant calcite in their cores, indicating that calcite formation is not linked to that of magnetite. Ferric iron can therefore not be the organic carbon oxidant. 3D reconstruction of granules and samples shows that the GIF contains multiple upward fining beds, with granules decreasing in size, followed by granule and rim fragments, terminating in an Fe-rich clay layer. Granule rims can also be seen to have been broken off. These characteristics support deposition from storm surge currents.

The necessity to reprocess spent nuclear fuel has arisen from increasing volumes of highly active and long-lived radionuclides associated with nuclear fission alongside increasing environmental impact concerns. In particular, one major challenge is the separation of the long-lived trivalent minor actinides (here, AmIII and CmIII) from the trivalent lanthanides in order to allow the future transmutation of the actinides into shorter lived radionuclides for the purpose of reducing the long-term radiotoxicity of the waste and the volume build up in storage. There are currently a number of different processes under development world-wide, all of which rely on the coordination chemistry and selective extraction of the minor actinides from the trivalent lanthanides using solvent partitioning. Of these, The TALSPEAK process (Trivalent Actinide Lanthanide Separation by Phosphorus reagent Extraction from Aqueous Komplexations) has showed great promise in separating the trivalent lanthanides from the minor actinides. The process uses DTPA (diethylenetriamine pentaacetic acid) as the chelating holdback reagent, HDEHP (bis-2-ethylhexyl phosphoric acid) as the extracting ligand and lactic acid as the buffer to prevent precipitation of DTPA that occurs at below pH 3.6. However, despite the considerable separation factors obtainable, and the fact the process exhibits promising radiolysis resistance, the process operates at sub optimal pH values. To overcome these limitations, we have developed a family of DTPA-amino acid conjugates that operate under TALSPEAK-like conditions over a much lower pH range of 1.5-2.5. Additionally, these ligands show comparable selectivity to the TALSPEAK process and are also relatively resistant to radiolysis. We will discuss the coordination chemistry of these ligands with the lanthanides and minor actinides using a combination of luminescence and NMR spectroscopies.

Liquid Metal Batteries (LMBs) are a promising electrical energy storage technology, built as a stable density stratification of two liquid metals separated by a molten salt. Their operation has been proved only for small prototypes, in order to transfer it to the industrial scale full knowledge of the different phenomena occurring in LMBs is required. In this work, done at Helmholtz-Zentrum Dresden-Rossendorf, we focus our attention on the thermal phenomena that appear inside Li||Bi LMBs . The system is first analyzed in the framework of the electrochemistry, a simple voltage model is developed and the heat generation terms are estimated. The geometrical and operating parameters are fully defined from multi-physics considerations. Then LMBs are studied with the continuum mechanics approach and all possible thermal phenomena are discussed. In the hypothesis of pure heat conduction, the first assessment of the effects of the reversible heat generation was done. Moreover the multiphase solver multiphaseInterFOAM is extended in order to take into account the thermal convection inside the cell. The results of our solver are compared to the one of a pseudo-spectral code. Finally some simulation results of thermal convection in LMBs are proposed.

One important natural process retarding the transport of contaminants is sorption onto mineral surfaces. A respective process understanding and realistic geochemical modelling of sorption is thus of high relevance in safety assessments of radioactive waste repositories. Further application areas are groundwater protection, environmental remediation or e.g. disposal of chemotoxic hazardous waste. Most often conventional concepts with constant distribution coefficients (Kd-values) are applied in reactive transport simulations, with the advantage to be simple and computationally fast, but not reflecting changes in geochemical conditions. Here, the smart Kd concept (www.smartkd-concept.de), a mechanistic approach mainly based on surface complexation models, is applied in geochemical modelling and has been further developed to calculate more realistic distribution coefficients for a wide range of important environmental parameters, e.g. pH, ionic strenght, competing cations and complexing ligands [1, 2] using PHREEQC, UCODE and RepoSUN/SimLab [3, 4, 5]. The philosophy behind this approach is to compute a-priori multidimensional smart Kd matrices which are available for subsequent transport simulations. We could demonstrate that constant Kd-values (e.g. for U(VI) [6], see Fig. 1) used so far are too crude an assumption but they rather range over several orders of magnitude. For considering worst case scenarios much smaller Kd-values have to be use than in conventional concepts. Similar results will be presented for Am and Np.

The reliable simulation of all relevant phenomena occurring during accidents in nuclear power plants (NPP) is an ongoing challenge for the development of computer codes. New generation reactor designs are using more and more passive type systems within their safety systems to cope with accidents. System codes such as the code system AC2 consisting of the modules ATHLET, ATHLET/CD and COCOSYS used in licensing procedures and for safety analyses have to be further developed and validated to be able to simulate such passive systems behaviour.
One aim of the German project EASY is the enhancement and validation of AC2 towards its use for reliable analysis of the behaviour of passive safety systems in nuclear power plants (NPP).
In this paper the work related on the extended coupling between the modules ATHLET and COCOSYS and first results showing the extended capability of the new design of coupling will be presented.
For that the coupling of both codes had to be extended to allow the simulation of the interaction between passive components linked to the primary system with interaction to the containment behaviour. The new coupling concept, using a full interlinked data network and an advanced data transfer between both modules, has in addition an user interface to implement additional modules into ATHLET code. Here new technologies are used to couple both codes improving the modular structure and maintainability.

Advanced reactor concepts such as Generation III, III+ and also SMR provide passive safety systems to cope with design basis accidents like loss of coolant accident or loss of main heat sink. In order to be able to assess the controllability of such DBA with passive systems only, computer codes are needed which are able to simulate the behaviour of these passive systems and which are well validated. In the German EASY project the coupled code system AC2 –mainly composed of the system code ATHLET-(CD) and the containment code COCOSYS –is currently being enhanced and validated for such applications on the basis of the KERENA reactor concept of AREVA.
Beyond the implementation of a suitable and effective coupling of the two codes ATHLET and COCOSYS, code development is done for modelling the behaviour of a passive flooding valve and enhancing the ATHLET 3D-model for large water pools.
Validation of the codes is done in two ways: Firstly, single effect tests, performed at the INKA facility in Karlstein, are used to validate the codes for the passive components used in the KERENA design. Secondly, the coupled code system is validated by simulating several integral tests which will be performed at the INKA facility during EASY. These integral tests represent design basis accidents such as SB-LOCA, LB-LOCA and SBO.
Finally, an uncertainty and sensitivity analyses of two integral tests will be performed since the behaviour of passive safety systems is affected strongly by the respective boundary conditions of the system.

The purpose of this study was to identify patients who likely benefit most from proton therapy (PT), based on the potential reduction of normal tissue complication probability (NTCP) compared to photon therapy. The NTCP models required for this comparison were developed using clinical data on acute side effects of prostate cancer and brain tumour patients having received PT.
In this study, 113 patients with primary brain tumours and 30 patients with adenocarcinoma of the prostate who had received PT were included. For the brain tumour patients, the radiation-induced acute side effects alopecia, erythema, pain and fatigue were considered. For prostate cancer patients, several gastrointestinal and genitourinary side effects were investigated. The occurrence of these side effects was correlated with different dose-volume parameters of associated organs at risk (OARs), such as skin and brain or rectum and bladder. The respective NTCPs were modelled by logistic regression. For every patient a volumetric modulated arc therapy (VMAT) photon treatment plan was retrospectively created. Differences in dosimetric parameters and NTCP between PT and VMAT plans were evaluated.
Significant correlations were found between acute side effects and dose to OARs. For example, occurrence of alopecia grade 2 and erythema grade ≥2 depended on dose-volume parameters in the high dose region of the skin (p<0.001). Proton plans showed significantly reduced low to intermediate dose volumes in all investigated OARs compared to VMAT plans (p<0.001). In the more relevant high dose volumes smaller differences between proton and photon treatment were found.
We found significant correlations between the occurrence of acute side effects and dose-volume parameters of associated OARs for patients with primary brain tumours or prostate cancer receiving PT. After inclusion of late side effects and validation in an external dataset, these NTCP models may be used to identify patients likely to benefit most from PT.

Patients with advanced lung cancer have a low overall survival despite treatment. Radiotherapy treatment is often lim-ited by the toxicity in the surrounding healthy tissue of the lung, oesophagus, spinal cord and heart. The prospective randomized clincial trial PRONTOX (NCT02731001) aims on the analyses of toxicities in patients treated for advanced lung cancer with either photon therapy or proton therapy. Only patients with tumor motion <10 mm are included. Photon and proton treatment plans are created based on time-resolved computed tomography (4D CT) imaging. Both plans are independently evaluated by experienced physicians for their applicability. If both treatments are deemed acceptable in terms of dosimetric parameters, randomization is executed. The dosimetric analysis includes the evaluation of the individual tumour motion and the uncertainties in range (3.5 %) and set-up (±3 mm) for the proton therapy treatment. End of March 2017, three patients were included, of which 2 had already finished their treatment getting double-scattered proton therapy. For the three patients, tumour motion was negligible and had only small effects on the dose distribution. The additional uncertainty analyses revealed the robustness of the generated proton therapy plans against the individual motion (maximum motion amplitude < 2 mm) as well as range and set-up uncertainties. During the treatment, respiratory surrogate signals were recorded for evaluation of breathing variabilities. In addition, control 4D CT were acquired once a week during treatment according to the trial protocol. Based on this imaging, changes in the patient anatomy and tumour motion were assessed. For the two patients who already completed treatment, the effect of anatomical changes and tumour motion changes on the fractional and accumulated dose distribution was small. No intervention e.g. a treatment plan adaptation was required in any case. Follow-up showed no recurrence and no side effects for these two patients so far.

Robust optimization in proton therapy considers uncertainties in patient setup and particle range during the optimization process. However, anatomical changes that may occur during the treatment course are neglected. The aim of this study was to quantify the influence of anatomical changes on the dose distributions for head and neck cancer (HNC) patients scheduled for bilateral neck irradiation.

Datasets from eight bilateral HNC patients, consisting of a planning computed tomography (CT) and weekly control CTs, were used. Intensity-modulated proton therapy plans were calculated with minimax robust optimization, account-ing 3 mm and 3.5% for setup and range uncertainty, respectively. The dose to the low- and high-risk clinical target vol-umes (CTV) consisted of 57 and 70 Gy(RBE), respectively, in 33 fractions. Organs at risk, e.g. spinal cord, brainstem, parotid glands, larynx, pharyngeal constrictor and esophageal inlet muscle, were considered for plan optimization and analysis. The cumulative dose during 33 fractions was checked weekly taking the anatomy of the control CTs into ac-count, and compared with the nominal plan.

Nominal plans fulfilled the clinical specifications of D98 ≥ 95% of the prescribed dose to the CTVs (range: 95.8-98.8% for low-risk CTV and 96.2-98.9% for high-risk CTV). During the treatment course, anatomical changes lead to reduced D98 values in five patients, with minimum of 87.3% in the low-risk CTV and 91.3% in the high-risk CTV. Maximum doses to spinal cord and brainstem remained below 45 Gy and 54 Gy, respectively. Mean doses to the contralateral pa-rotid gland remained below 26 Gy, except in one patient (maximum mean dose = 27.2 Gy).

For some patients, robust optimization prior to treatment initiation is insufficient to account for anatomical changes occurring during the treatment course. The results for a total cohort of 17 patients, including robustness analysis and plan adaptation strategies will be presented.

The use of stem cells to support tissue repair is facilitated by loading of the therapeutic cells with magnetic nanoparticles (MNPs) enabling magnetic tracking and targeting. Current methods for magnetizing cells use artificial MNPs and have disadvantages of variable uptake, cellular cytotoxicity and loss of nanoparticles on cell division. Here we demonstrate a transgenic approach to magnetize human mesenchymal stem cells (MSCs). MSCs are genetically modified by transfection with the mms6 gene derived from Magnetospirillum magneticum AMB-1, a magnetotactic bacterium that synthesises single-magnetic domain crystals which are incorporated into magnetosomes. Following transfection of MSCs with the mms6 gene there is bio-assimilated synthesis of intracytoplasmic magnetic nanoparticles which can be imaged by MR and which have no deleterious effects on cell proliferation, migration or differentiation. The assimilation of magnetic nanoparticle synthesis into mammalian cells creates a real and compelling, cytocompatible, alternative to exogenous administration of MNPs.

1. Introduction
The TALSPEAK process [1] was developed at Oak Ridge National Laboratory in the 1960’s to separate trivalent actinide ions, An(III), from chemically similar lanthanide ions, Ln(III) by solvent extraction. The idea was using an extracting agent unselective for An(III) over Ln(III) and adding a complexing agent to the aqueous phase to infer selectivity [2]. Despite the simplicity of this concept, TALSPEAK is actually a rather complex system, with numerous equilibria involved. The original TALSPEAK system consisted of HDEHP (bis-2-ethylhexyl phosphoric acid) as the extracting agent, DTPA (diethylenetriamine pentaacetic acid) as the An(III)-selective complexing agent and lactic acid as buffering agent. Constantly improving TALSPEAK by substituting the components of the original system, ALSEP [3] and Advanced TALSPEAK [4, 5] have been developed.
We have pursued a concept which differs in two aspects, (a) using amino acids (AA) as buffering agent and (b) linking them to the complexing agent. This way, only a single molecule is added to the aqueous phase and the system is expected to behave more simply.
2. Results and Discussion
Several DTPA-AA conjugates were synthesised, DTPA-Arg, DTPA-His, DTPA-Ser and DTPA-Ala. These were tested in solvent extraction experiments. Organic phase was 0.2 mol/L HDEHP in kerosene, aqueous phases were solutions containing 50 mmol/L DTPA-AA conjugate, Am(III) and Ln(III) (Y; La–Lu). pH was adjusted by adding HNO3 or NaOH.
The lowest pH at which separation was achieved (i.e., Am(III) distribution ratio < 1 and all Ln(III) distribution ratios > 1) was in the range of 1.1–1.5. Separation factors for Eu(III) over Am(III) were ≈ 100 and the minimum separation factors between Am(III) and the least extracted Ln(III), being Nd(III) in all cases, were 30–40.
The coordination chemistry was studied by luminescence and NMR. Photophysical studies of the Eu(III)-DTPA-AA complexes demonstrated characteristic Eu(III) emission, with associated lifetime decay profiles confirming 1:1 coordination. 1H NMR studies were performed with Am(III), confirming successful complexation.
In conclusion, an improved TALSPEAK system is reported which compares favourably to known TALSPEAK systems.

Key words: TALSPEAK, amino acids, actinides(III), lanthanides(III)

1. Weaver, B.; Kappelmann, F. A., USAEC report ORNL-3559, Oak Ridge National Laboratory, USA: 1964.
2. Nilsson, M.; Nash, K. L., Solvent Extr. Ion Exch. 2007, 25 (6), 665–701.
3. Gelis, A. V.; Lumetta, G. J., Ind. Eng. Chem. Res. 2014, 53 (4), 1624–1631.
4. Braley, J. C.; Grimes, T. S.; Nash, K. L., Ind. Eng. Chem. Res. 2010, 51 (2), 629–638.
5. Lumetta, G. J.; Casella, A. J.; Rapko, B. M.; Levitskaia, T. G.; Pence, N. K.; Carter, J. C.; Niver, C. M.; Smoot, M. R., Solvent Extr. Ion Exch. 2015, 33 (3), 211–223.

Solid organic matter is an important constituent not only in coal, but also in black shale-hosted ore deposits. The reliable recognition and quantification of organic carbon – as well as its microfabric relation to associated inorganic minerals - plays a crucial role in characterization by scanning electron microscopy-based image analysis. However, the use of conventional epoxy resin in the preparation of grain mounts does not allow for recognition of solid organic carbon compounds. In this study we illustrate that the use of iodized epoxy resin readily overcomes this bottleneck. Best results are obtained with an addition of 15 wt% iodoform to the epoxy resin. With process samples of black shale-hosted polymetallic Kupferschiefer-type ore as a case study it is shown that recognition and quantification of solid organic carbon is easily achieved and that tangible parameters such as particle and grain sizes, association and liberation for ore and gangue minerals can be determined in the presence of solid organic matter. Due to the inherent uncertainty of the exact chemical composition of the kerogen contained in Kupferschiefer it was not possible to attain exact comparability between chemical Corg assays and assays calculated from MLA data. However, the results are still found to closely agree with one another. The strength of iodized resin lies in its ability to distinguish organic matter with high hydration ratios in addition to the easy integration in sample preparation. It could therefore be an attractive supplement in the analyses of other raw materials containing complex organic-matter.

Spintronic devices are often patterned from continuous films into micro- or nanostructures. Fabrication of those nano-devices is self-limited and depends on the lateral resolution of the chosen fabrication method. Ion irradiation offers an alternative route to introduce smaller magnetic patterns limited by the size of the ion beam. Irradiation of oxide materials can cause chemical reduction and lead to the local formation of metallic species. By using the oxide family of ferromagnets (e.g., Fe, Ni and Co), reduction leads to the formation of ferromagnetic and conducting volumes limited by the size of the ion irradiated area that are embedded into a non-magnetic and insulating matrix. On the other hand, the physical mechanism behind ion irradiation-induced oxide reduction could not be explained. Therefore, our studies focus on ion (H, He, Ne, O) irradiated cobalt-oxide (CoO or Co3O4) systems in order to explain the physics behind the process. Also, the knowledge is being exploited to tune exchange-bias direction, prepare nano contacts for synchronized spin torque oscillators, and to form topographically stabilized magnetic skyrmions.

We present an approach for reconstructing real space information from small angle x-ray scattering images that utilizes reduced models to describe the scattering distribution. This implies a massive reduction of the reconstruction space dimensionality. First reconstruction results for experimental data are shown.

BaZrO3 (BZO) is a potential candidate material for electrode in solid oxide fuel cells (SOFL) because of its excellent reported proton conductivity [1, 2]. It is suggested that presence of intrinsic point defects such as O vacancies act as sinks for O atoms produced upon hydrogenation of water molecule and promote proton conductivity. For this, the formation energy of O atom should be lower and its migration should be suppressed [3]. Since these materials are used at high temperature, it is very important to consider effects of phonons on the defect chemistry [4, 5, 6]. In this work, first, we identify thermodynamically favorable conditions for the formation of BZO by free energy calculations of bulk phases using Density Functional Theory. Next, we study the free energy of formation of both neutral and charged O vacancies of stable BZO phase and discuss significance of these results for experimental growth conditions. Initial results show that phonon contributions to free formation energy of charged vacancy is significantly high compared to neutral vacancy due to large lattice distortion and negative formation entropy for charged vacancy. Studies also show that acceptor doping both at A and B site lowers the formation energy of O vacancy in the vicinity of dopant atoms resulting in increase of proton conductivity [7, 8]. In order to understand the mechanism of this enhancement, we study the free energy of formation of O clusters in reducing conductions for acceptor doping at A and B sites.

References

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[2] K. D. Kreuer, ed. T. Ishihara, Springer, 2009, pp. 261–271.
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The dynamic and static structure factors contain a wealth of information about the state and properties of a physical system. The structure of a system relates directly to its equation of state, collective modes, stopping power and relaxation processes.
Since x-ray and particle scattering are extremely important experimental tools to diagnose warm dense matter, theoretical predictions of the structure have become one of the best modes of comparison between theory and experiment in the warm dense matter regime.
We give an overview of state of the art theoretical methods to calculate the structure of warm dense matter in equilibrium and non-equilibrium. Results are given for such states as created in recent experiments. Limits of the current theories and possible future developments are discussed.

Warm dense matter states in the transition region from high pressure solids to high temperature plasmas are found in terrestrial planets, giant planets, and exoplanets. Such states are created in the laboratory during interaction of lasers or shock waves with matter. The intention is usually to obtain direct experimental access to equilibrium or nonequilibrium warm dense matter states or it might be an intermediate state on the way to fusion plasmas states or laser-plasma acceleration experiments.
Studying warm dense matter, one faces several challenges. The first is the determination of a full set of basic parameter like density, charge state, temperature, or the momentum distribution function that fixes the state of matter in the phase space. Only then is it meaningful to investigate important quantities like the equation of state, phase transitions, structure, collective excitations, relaxation processes, or the stopping power.
Here, we present recent developments and results in warm dense matter physics. The close interplay between theory and experiment via x-ray scattering and first principle simulations is highlighted. The dynamic structure factor containing a wealth of information serves as the connection between measurements and calculations. Results are given for a number of elements like aluminium, carbon, or iron, and materials like plastic.

Powerful femtosecond pump lasers and femtosecond x-ray probe beams created by free electron lasers make it possible to create and diagnose strongly correlated states of matter in which the electron and ion Wigner distribution functions are of a strongly non-equilibrium type.
We therefore present a quantum theory for the dynamic structure factors in just such non-equilibrium, correlated, two-component systems.
To make our theory applicable for x-ray scattering as in equilibrium, a generalized Chihara decomposition for the total electron structure factor in non-equilibrium is derived. Examples are given and the influence of correlations and exchange on the structure and the x-ray scattering spectrum are discussed for a model non-equilibrium distribution, as often encountered during laser heating of materials, as well as for two-temperature systems.

We present simulation results on laser ion acceleration using hydrogen ribbon targets irradiated by ultra-intense, ultra-short laser pulses. These targets promise to produce pure proton beams applicable for cancer therapy at high repetition rates. We address critical issues concerning the acceleration process that potentially hinders the application of these beams in a clinical scenario.

For achieving proton energies suitable for the treatment of deep seated tumors it is important to increase the laser intensity. At high laser intensities, plasma instabilities both at the target surfaces and target bulk can create electron filaments which result in non-uniform proton beams, detrimental for delivering uniform dose distributions.

By varying the laser contrast it is possible to change the preplasma scale length to influence the formation of instabilities. Other means of controlling proton beams are either changing target geometry (e.g. going from planar ribbon targets to spherical droplet targets) or the polarization. We present results of 2D3V particle-in-cell simulations at realistic densities that show the influence on the plasma dynamics and final beam properties and discuss their relevance regarding applications of solid hydrogen targets for laser-driven proton tumor therapy.

Oxygen vacancy (OV) controlled hydrophobicity of self-assembled TiO₂ nanorods (NRs) on chemically etched Si pyramids is investigated by irradiating with 50 keV Ar-ions at room temperature. Apparent contact angle (CA) is found to increase from 122° to 141° up to a fluence of 1 × 10¹⁵ ions/cm², followed by a gradual reduction to 130° at 1 × 10¹⁷ ions/cm². However, the drop in apparent CA is found to be associated with the decrease in fractional surface area via transformation of NRs to an amorphous layer above 1 × 10¹⁵ ions/cm², though it is still higher than that of as-grown one. Detailed X-ray photoelectron spectroscopy and electron paramagnetic resonance measurements suggest that the control of hydrophobic behavior is related to the suppression of surface free energy via migration of OVs into the voids in TiO_x layers.

Coordination polymers are organic-inorganic complexes built up from the association of metallic centers with O- or N-donor ligands. In the particular case of actinides (An), previous literature mainly has reported the synthesis of solid networks bearing U(VI) or Th(IV). Trans-uranium elements have been much less studied due to their high radiotoxicity and limited amount of the material source. Among the possible oxidation states of An, the tetravalent state has been investigated most actively and large polynuclear oxo-clusters have been isolated for U1,2 or Pu3. In contrast, there are very few data concerning Np(IV) compounds. In 2012, Takao et al.4 reported the formation of Np(IV) hexanuclear cluster in an aqueous solution. The knowledge of the formation of such polynuclear An(IV) species could be of significant importance for the fate of An in contaminated soils containing O-donor ligands, such as humic acids or organic pollutants.
In this work, we studied the crystallization of Np(IV) with various aromatic polycarboxylate ligands in different solvents and analyzed their crystal structures. In water, an infinite chain of Np2O2(H2O)2(1,2-bdc)2 were isolated in the presence of phthalate.5 This compound crystallizes as orange aggregates, whereas the analogue compound with uranium is obtained as green crystals. With mellitic acid the oxidation of Np(IV) to Np(V) was observed and led to large green plates, involving layers of {NpO7H2O0-2} units linked to each other via trans-dioxo neptunyl bonds.
The use of other solvents allowed the crystallization of large polynuclear discrete Np(IV) clusters. For example, using DMF, the hexanuclear unit of [Np6O4(OH)4] has been obtained with different dicarboxylic ligands and is the basic building unit to form an open-framework structure (Figure 1, left). The corresponding structures revealed the isolation of the hexanuclear cluster An6O8 with Np(IV), the first example of hexanuclear Np(IV) complex characterized in the solid state. These clusters are linked by the ligand creating tetrahedral and octahedral voids in the structure. The formation of larger neptunium-based polyoxo clusters will be also presented.

Purpose Sustainability differentiation has become an important issue for companies throughout the value chain. There is thus a need for detailed and credible analyses, which show the current status and point out where improvements can be done and how. The study describes how a comprehensive product-centric eco-efficiency indicator framework can be used to evaluate, benchmark, and communicate the sustainability of a copper production value chain. The indicator framework, together with the suggested data collection and simulation methods, aims at evaluating the whole system, while still enabling a focus on scopes of different width. The status of the environment, current production technologies, locationspecific and process-specific issues all play a role in achieving sustainable development.
Methods Copper cathode production from copper ore was chosen to exemplify the developed framework. Data sets from a simulation tool were used when available and LCI databases and LCA software were utilized for the remaining steps. The value chain is analyzed and the benchmark for each indicator built according to the new Gaia Refiner indicator framework. This method enables analysis of specific production steps with a higher degree of accuracy.
Results and discussion The case study shows how some important environmental sustainability issues in copper production can be analyzed and benchmarked within a product group. Benchmark data is collected and used in the analysis for the selected system scope. Data availability is still an issue and the example shows which areas require more information in this context so that products and value chains can be benchmarked in the future on a more consistent basis. The energy mix, chemical use, and land use contribute to potential environmental sustainability risks within the product benchmarking group, while emissions control shows competitive environmental sustainability advantages for the case study.
Conclusions The methodology is shown to work well in highlighting the sustainability advantages and risks of value chains in copper production with the selected system scope in a visualmanner through the Sustainability Indicator "Flower" The importance of a baseline is clear.
The effect of the metal ore grade on the results shows that the scalability of the analysis system is very important. Scaling the system scope up will show the differences in varying value chains and scaling the system scope down will show efficiency differences between more similar value chains, thus visualizing where innovation has the biggest impact.

The long-lived radionuclides ¹⁰Be (t_1/2=1.4 Myr) and ²⁶Al (t_1/2=0.7 Myr) are widely used for dating applications, e.g. determination of surface exposure durations of terrestrial quartz or meteorites to cosmic rays. Stratigraphic chronologies of marine reservoirs such as sediments, deep-sea crusts and nodules are often obtained via ¹⁰Be /⁹Be ratios, while ²⁶Al/²⁷Al ratios are only scarcely used.

The deep-ocean floor is shielded from cosmic rays by several km of water, preventing direct cosmogenic production. In marine reservoirs, inputs of ¹⁰Be and ²⁶Al occur due to their production in the atmosphere, in which ¹⁰Be is however ~500 times more abundant than ²⁶Al. The freshly produced radionuclides settle onto the open ocean floor within ~100 (²⁶Al) and ~1000 (¹⁰Be) years. An additional source may be the production via the ²³Na(alpha,n)²⁶Al reaction induced by alpha-particles originating from decay of U and Th.

We analyzed 85 samples from four deep-sea sediment cores from the Indian Ocean and 21 from two manganese nodules from the Atlantic Ocean. The isotope ratios of ²⁶Al/²⁷Al and ¹⁰Be/⁹Be were measured by AMS at the VERA facility (University of Vienna, Austria) and at the DREAMS facility (HZDR, Dresden, Germany). Due to the low ²⁶Al/²⁷Al ratios, i.e. ~10^-14 vs. ¹⁰Be/⁹Be: ~10^-11, the measurement of ²⁶Al is much more time consuming. However, as stable ²⁷Al is naturally enough abundant in sediments (in contrast to stable ⁹Be), the work without addition of a carrier and stable isotope measurements reduces potential error sources.

Our results indicate that ¹⁰Be/⁹Be and ²⁶Al/²⁷Al are both valuable tools for dating deep-sea sediments up to 3-5 Myr. Beyond these limits in-situ production of ²⁶Al becomes significant. The nodule in-situ production of ²⁶Al is clearly dominating the atmospheric production.

Each year, about 30,000 tons of extraterrestrial solid material falls onto the Earth's surface. A non-negligible fraction of these materials are micrometeorites (MMs); small (1 µm up to 1 mm), mostly spherical, particles that predominantly originate from the asteroid belt between Mars and Jupiter.

As soon as MMs are released in space, they are affected by the radiation pressure of the Sun causing them to spiral inwards. While travelling towards the Sun, the particles are irradiated by solar and galactic cosmic rays, producing cosmogenic nuclides such as ¹⁰Be (t_1/2=1.4 Myr) and ²⁶Al (t_1/2=0.7 Myr).

In urban areas MMs are accumulating on the rooftops of buildings [1]. They can be easily collected from roofs of high buildings, where anthropogenic influences like pollution (e.g. from traffic) are reduced.

We have taken samples using a simple magnet from the rooftops of three physics buildings of the northern and southern hemisphere: the physics building of the Berlin Institute of Technology (~45 m above street level, Berlin, Germany), the accelerator buildings of the ANU in Canberra (44 m, Australia), and the accelerator building at HZDR, Dresden, Germany (24 m).

The magnetic fraction is investigated non-destructively by SEM-EDX to allow for enrichment of potential magnetic MM particles (~50–200 μm). Proof of extraterrestrial origin will be achieved by the determination of minor elements such as Ni from the interior of the spherules after cutting. We will then perform a radiochemical separation from individual samples and measure ¹⁰Be and ²⁶Al by AMS at the DREAMS facility (HZDR [2]).

The experimental concentrations of those radionuclides will be compared with theoretical production rates [3] to deduce exposure ages and the potential origin of the samples.

[1] Genge et al., Geol., doi:10.1130/G38352.1 (2016)
[2] Rugel et al., NIMB, 370, 94 (2016)
[3] Trappitsch & Leya, Meteorit. Planet. Sci., 48, 195 (2013)

Selenium is toxic and thus its fate in the environment has to be ascertained. The bio-transformation of Se oxyanions by microorganisms will affect its (bio)availability in the environment. The microorganisms are known to reduce Se oxyanions to biological Se(0) nanoparticles (BioSe-Nanospheres) or biological Se(0) nanorods (BioSe-Nanorods) under mesophilic (30 °C) and thermophilic (55 °C) conditions, respectively. Though both types exhibit a coating of extracellular polymeric substances, their colloidal properties differs, leading to a different mobility in environmental waters. [1] Consequently, understanding the underlying mechanisms of the formation of amorphous BioSe-Nanospheres and trigonal BioSe-Nanorods is essential to understand the fate of selenium in the environment.
This study identified BioSe-Nanospheres produced by various microorganisms behaving differently when exposed to thermophilic conditions (55 °C). The bacteria strain E.coli K12 and the anaerobic granular sludge from a full scale Upflow Anaerobic Sludge Bioreactor were used to produce BioSe-Nanospheres at 30 °C. After purification (to separate the particles from the cells) the BioSe-Nanospheres were heated for 7 days at 55 °C with shaking. The Raman and Scanning Electron Microsocpy data evidenced a transformation of the anaerobic granular sludge Se(0) particles to trigonal BioSe-Nanorods upon heating, while the BioSe-Nanospheres of the bacteria strain E.coli K12 remained spherical and amorphous.
The CD-Spectrosopy data revealed that the proteins coating the anaerobic granular sludge BioSe-Nanospheres gets unstable during a heating time of 23 hours, suggesting a denaturating process. Such a behavior was not observed for particles produced via E. coli. Unravelling the differences in particles coating and selenium allotropy which results in changes of mobility and toxicity will further increase the knowledge on the environmental fate of selenium.
[1] Jain, R. et al., Environ. Sci.: Nano, 2017.

The visualization of Eph receptors, which are overexpressed in various tumor entities, using selective small molecule Eph inhibitors by means of PET is a promising approach for tumor imaging. Indazolylpyrimidineamines represent a class of compounds, which are known to have high affinity especially for the EphB4 receptor. Radiofluorination of these compounds could provide a highly specific imaging agent and was investigated using a classical nucleophilic introduction of [18F]fluoride as well as a less common nucleophilic ring opening reaction of azetidinium salts. In the past, radiofluorinations using azetidinium precursors were demonstrated to result in high radiochemical yields in short periods of time. For this purpose, an azetidinium precursor based on the indazolylpyrimidineamine lead compound was developed and radiofluorination was successfully accomplished. The respective [18F]radiotracer was quickly prepared with high radiochemical purity >97% and in a radiochemical yield of 34%.

Due to their wide-spread application of Rare Earth Elements (REE) in high technological products, their separation from one another is mandatory. The optimization of physico-chemical conditions for the design of any effective extraction and recycling processes relies on accurate, consolidated, internationally recognized and reliable thermodynamic data, which are so far not available for REE.

This study aims at providing such a critically-assessed and internally consistent data base for europium. An evaluation of all available primary literature sources for Eu(III) complexation constants (log β) and solubility products (log Ksp) with inorganic ligands (OH−, Cl−, NO3−, SO42−, PO43−, and CO32−), evidenced several critical issues i) inconsistencies between different sources, ii) lack of accurate activity coefficient treatment in case of the formation of weak complexes, and iii) absence of independent spectroscopic validation of the stoichiometry of the proposed complexes.

Thus, several actions have been undertaken:

a) recalculation of the log β of weak complexes (Cl−, NO3−) by using an hypothetical reference state (at trace ligand concentration) [1].
b) in case of PO43− complexation, Time-resolved Laser-induced Fluorescence Spectroscopy was used to monitor the speciation evolution of Eu at micromolar concentrations and to identify the prevailing species as well as their stoichiometries. The respective complexation constants were derived from the spectroscopic data sets.
c) the conditional log β and log Ksp were extrapolated to standard conditions (I = 0 M, T = 298.15 K) using the Specific Ion Interaction Theory.

[1] Spahiu, K. et al. (1998) Radiochim. Acta 82, 413-419.

The fundamental formation of the three phase contact in flotation is an intensively and controversially discussed phenomenon and the contact angle method is usually employed to characterise the wettability of solid surfaces. A more recent technique to explore the hydrophobicity of solid particulate phases is inverse gas chromatography (iGC) which is used to quantify the wettability of solid surfaces through thermodynamic parameters. In this article, the recently introduced net free energy of interaction between particles and bubbles immersed in water ΔGpwb is derived from the surface free energy analysis and its correlation to the flotability of solid phases is evaluated. At the same time, a more detailed analysis on the action of flotation reagents is presented performing iGC measurements under dry and flotation experiments under aqueous conditions. In general, flotation reagents have to satisfy required features to adsorb selectively, render the solid surface wetting property sufficiently, and comply current regulations concerning the preservation of the environment. Consequently, many conventional reagents are increasingly subjected to restrictions. One potential alternative candidate is nanocellulose due to the versatile chemical composition and functionality. The synthesis of cellulose nanocrystals (CNCs) includes different mechanical and chemical modification routes to lower the crystal sizes and integrate specific functional groups and organic components into the cellulose structure. This study is concentrated on the investigation of aminated CNCs for the flotation of quartz in comparison to conventional reagents. The employment of CNCs as a renewable and sustainable alternative to conventional chemicals is challenging due to the more complex structure of cellulose crystals and leads to new perspectives regarding the action of flotation reagents at the interface of a mineral under dry and wet environments.

Frustrated magnets provide a promising avenue for realizing exotic quantum states of matter, such as spin liquids and spin ice or complex spin molecules. Under an external magnetic field, frustrated magnets can exhibit fractional magnetization plateaus related to definite spin patterns stabilized by field-induced lattice distortions. Magnetization and ultrasound experiments in MnCr₂S₄ up to 60 T reveal two fascinating features: an extremely robust magnetization plateau with an unusual spin structure and two intermediate phases, indicating possible realizations of supersolid phases. The magnetization plateau characterizes fully polarized chromium moments, without any contributions from manganese spins. At 40 T, the middle of the plateau, a regime evolves, where sound waves propagate almost without dissipation. The external magnetic field exactly compensates the Cr–Mn exchange field and decouples Mn and Cr sublattices. In analogy to predictions of quantum lattice-gas models, the changes of the spin order of the manganese ions at the phase boundaries of the magnetization plateau are interpreted as transitions to supersolid phases.

After 6 years of ³⁶Cl routine operation, more than 6000 unknown samples have been measured at the 5 MV French AMS national facility ASTER (CEREGE, Aix en Provence). This paper presents the long term behavior of ASTER through the analysis of the measurements of the most used chlorine standards and reference materials, KNSTD1600, SM-Cl-12 and SM-Cl-13 over a 46 months’ time period.
Comparison of measured chlorine concentrations (both ³⁵Cl and ³⁶Cl ) from ice samples on two AMS facilities operating at 5MV (ASTER) and 6MV (DREAMS, Helmholtz-Zentrum Dresden-Rossendorf ) and normalizing to two different reference materials agree within uncertainties making both reference materials (SM-Cl-12 and KNSTD1600) suitable for ³⁶Cl measurement at ASTER.

he Sakatti Cu-Ni-PGE deposit is situated in northern Finland and was discovered by Anglo American Exploration in 2009 (Halkoaho 2014). It is said to be one of the most significant discoveries in Finland for more than a generation (Maier et al. 2015). The mineralization comprises massive, disseminated and vein sulphides. A stockwork is formed by the sulphide veins, which contains exceptionally high grades of Cu, platinum-group elements (PGE) and Au in the shallow eastern part of the deposit. In contrast to the massive and disseminated sulphide mineralization, the mineralogy, mineral paragenesis and petrography of the stockwork zone is relatively poorly uninvestigated, and this study aimed at increasing knowledge of it.
Traditional light microscopy and automated scanning electron microscope (SEM)- based image analyses using a mineral liberation analyser (MLA) on 20 samples from 11 drill holes revealed a classic magmatic sulphide assemblage of chalcopyrite ± pyrrhotite, pentlandite and pyrite. Additionally, 1,133 platinum-group mineral (PGM) particles belonging almost exclusively to the moncheite (PtTe2) – merenskyite (PdTe2) – melonite (NiTe2) solid solution series were discovered (Fig. 1 a, b). Notably, almost two-thirds of the PGE-bearing phases consist of melonite. Some of the PGM particles contain inclusions of electrum (AgAu2) and muthmannite (AgAuTe2), which possess an average of 0.25 wt% Au. For the first time at Sakatti, one particle of irarsite (IrAsS) was encountered. The PGM display a trimodal particle area distribution, which is a result of an increasing mineralogical complexity of the particles relative to their sizes. Most of the PGM are hosted in inclusions (76%) (mainly in chalcopyrite), whereas minor amounts are located at grain boundaries (19%) and in cracks (5%).
An enrichment of PPGE relative to IPGE was recognized in the sulphide veins, which is in line with data on the massive and disseminated sulphide mineralization at Sakatti (Ahvenjärvi 2015). However, the di erence between maximum and minimum enrichments is more pronounced for the sulphide veins.
Element ratios calculated from geochemical data obtained by ICP-MS/OE analyses and displayed in various plots (e.g. Cu/Ir vs. Ni/Pd, Rh vs. Rh/Cu (Fig. 2)) indicate that the Cu-rich sulphide veins represent the magmatic crystallization products of a highly fractionated Cu-rich sulphide liquid enriched in Pt, Pd, Au, Ag, As, Bi, Pb, Se, Te and Zn, which separated from monosulphide solid solution (mss). Intermediate solid solution (iss) solidi ed from the Cu-rich sulphide liquid, exsolving chalcopyrite at <550 °C. Simultaneously, small volumes of intercumulus residual melt mainly contained the precious metals Bi and Te due to their incompatibility in iss. Solitary and composite PGM, as well as Au minerals crystallized rst from the residual melt (<600 °C), followed by a succession of various Bi, Ag and Pb tellurides (~540 °C), and nally sphalerite (ZnS) and galena (PbS). However, melonite crystallized in two stages: as large, solitary grains directly exsolved from Ni-bearing iss (~600 °C) shortly after the formation of moncheite and merenskyite from the residual melt, and during subsolidus exsolution (<600 °C) with precipitation on the surfaces of earlier formed PGM. Finally, slight remobilization of the PGM occurred at temperatures <300 °C, veri ed by minor amounts of Cl-bearing minerals and ragged particle shapes. Surprisingly, the geochemical data (Fig. 2), petrography and genetic concept of the sulphide veins at Sakatti proved to be very similar to the Cu-rich footwall veins at the McCreedy East deposit in Sudbury (Canada) (Naldrett et al. 1999, Dare et al. 2014).

Given the physical properties and the sensitivity to morphological variations of proton therapy, it could greatly benefit from integration with magnetic resonance (MR) imaging. Such integration raises several challenges, as both systems mutually interact with each other. The problem of magnetic field induced dose distortions has been predicted by Monte Carlo (MC) simulation in previous studies, but no experimental validation has been performed yet. We present and compare simulated and measured dose distributions in a realistic magnet setup.

2D dose distributions of proton pencils beams (80-180MeV) traversing the field of a 1T NdFeB permanent magnet while depositing energy in a PMMA slab phantom were simulated using the Geant4 toolkit and measured using EBT3 radiochromic films. The Geant4 model was validated against depth-dose measurements performed with a multi-layer ionisation chamber. The magnetic vector field was calculated using finite-element modelling and validated experimentally using a Hall probe. Deflected beam trajectories and depth-dose curves were extracted from the 2D dose distributions and compared. Demagnetization and radioactivation of the magnet material were simulated and monitored during measurement.

The range predicted by the MC model agreed with the Giraffe measurements within 0.5mm, and calculated and measured magnetic field data agreed within 2%. The lateral beam deflection was clearly visible on EBT3 films and ranged from 1mm to 10mm for 80MeV and 180MeV, respectively. Simulated and measured range and deflection agreed within 1mm for all studied energies. Demagnetization and radioactivation effects were negligible.

For the first time, MC simulations of magnetically deflected proton beams inside tissue-equivalent material have been experimentally validated with dose measurements. The results indicate that the magnetic field induced proton beam deflection is both measurable and accurately predictable. This demonstrates the feasibility of accurate dose calculation as well as measurement within the framework of MR-integrated proton therapy.

We present recent simulation studies of laser wake eld acceleration that match experiments performed at HZDR which produce quasi mono-energetic electron bunches of several hundred picocoulombs charge. The talk focuses on the dynamics of this new acceleration scheme and required code improvements to study it using the 3D3V particle-in-cell code PIConGPU. We discuss in detail the influence of various ionization mechanisms and laser implementations on the plasma dynamics. Furthermore, we present computation constrains and implementation challenges that these new methods entail. On top of discussing the acceleration scheme, we predict experimental observables using PIConGPU’s in-situ synthetic radiation diagnostics. It allows predicting spectra from infrared to x-rays and provides the capability to determine the temporal and spatial origin of the radiation. These radiation simulations give valuable spectral signatures that allow conclusions on the micrometer femtosecond electron dynamics occurring in experiments. As an example of such a signature, simu- lated betatron spectra will be compared to experimentally measured spectra in order to determine the spatial extent of the electron bunch.

In the present study the stabilizing effect of the actinide analogue ion Eu3+ on zirconia in dependency of the molar fraction and the influence of the trivalent stabilizer cation radius on zirconia solids in a series of Ln3+ (Ln3+ = La, Sm, Gd, Tb, Lu) co-doped with Eu3+ is investigated using a combination of x-ray powder diffraction (PXRD) and time-resolved laser fluorescence spectroscopy (TRLFS). PXRD is employed to gain an insight into the zirconia crystal structure in the presence of Eu3+ and/or Ln3+ and to identify the various zirconia phases (m, t, and c).
For the material with 2% Eu3+ mainly the monoclinic structure is to be seen in the PXRD pattern. A sample with 8% Eu3+ can be assigned to the tetragonal structure while at an incorporation percentage of 22% Eu3+ the cubic phase is predominant. The broadness of the TRLFS emission peaks of the sample with 2% Eu3+ speaks for a poorly ordered solid or Eu3+ incorporation on a very distorted host cation site. The 7F1 as well as the 7F2 band show a strong band splitting which correlates to low crystal symmetry. The band splitting of both samples with higher europium content is reduced because of a higher symmetry as could be seen in the XRD pattern. To prove the transferability of the lanthanide to actinides selected samples will be prepared and studied using Cm3+ as dopant.
The effect of different stabilizers on the nucleation process has been studied using a combination of the crystal truncation diffraction (CTR) and the resonant anomalous x-ray scattering techniques (RAXR) using synchrotron radiation at the European synchrotron radiation facility (ESRF) in Grenoble.
The results of these ongoing investigations will be presented in detail at the conference.

Mn oxide minerals are ubiquitous in soils and sediments and participate in a variety of chemical reactions that affect groundwater and bulk soil composition. Even at tracer concentrations they play a decisive role in regulating the mobility of contaminants due to their high sorption and redox capacity and scavenging capability [1]. Due to its long half-life and its toxicity, Np-237 is considered as a major contaminant of the ecosystem in the long-term safety assessment of nuclear waste repositories. The pentavalent state is environmentally most relevant [2].
In this work, Np(V) sorption on amorphous birnessite (Bs) is investigated using a combination of ATR FT-IR and EXAFS spectroscopy on a molecular level with thermodyanamic modelling of batch sorption studies.
For the first time, in-situ Np(V) sorption is comparatively studied on the oxyhydroxides of Fe and Mn by ATR FT-IR spectroscopy under a variety of environmentally relevant sorption conditions, e.g. micromolar Np concentrations, low acidic to neutral pH, moderate ionic strength [3]. From the results, the formation of single inner-sphere complexes can be derived. In addition, time resolved spectra provide kinetic information on the surface reactions. Complementary EXAFS measurements evidence mononuclear bidentate edge-sharing Np(V) complexes on the Bs surface.

A new class of multimetallic hierarchical aerogels composed entirely of interconnected Ni-Pd_xPt_y nano-building-blocks with in situ engineered morphologies and compositions is demonstrated. The underlying mechanism of the galvanic shape-engineering is elucidated in terms of nanowelding of intermediate nanoparticles. The hierarchical aerogels integrate two levels of porous structures, leading to improved electrocatalysis performance.

A comprehensive database on upward two-phase flows in vertical pipes was obtained using the wire-mesh sensor technologies for gas-liquid flows in vertical pipes. The investigations were done for different pipe diameter as well as for flows with and without phase transfer. Wire-mesh sensors provide detailed information on the structure of the gas-liquid interphase. Basic characteristics of gas-liquid flows can be observed in such experiments and are discussed in this chapter. The quantitative results obtained in the measurements as radial volume fraction profiles, radial gas velocity profiles, bubble size distributions, distributions of interfacial area density, and others are valuable data for the development and validation of Computational fluid dynamics (CFD) codes for multiphase flows.