Publications Repository - Helmholtz-Zentrum Dresden-Rossendorf

I review the status of nuclear astrophysics in Germany, with a focus on recent experimental progress

I review recent nuclear astrophysics work at HZDR Dresden, both related to the LUNA underground accelerator in Italy and independently from it.

This talk gives an overview of the results obtained by Institute of Resource Ecology of the HZDR in the German-French Project EcoMetals

The integration of high-mobility III-V compound semiconductors emerges as a promising route for Si device technologies to overcome the limits of further down-scaling. In this paper, a non-conventional approach of the combination of ion beam implantation with short-time flash lamp annealing is employed to fabricate InxGa1-xAs nanocrystals and to study their crystallization process in thin Si layers. The implantation fluence ratio of Ga and In ions has been varied to tailor the final nanocrystal composition. Raman spectroscopy and X-ray diffraction analyses verify the formation of ternary III-V nanocrystals within the Si layer. Transmission electron microscopy reveals single-crystalline precipitates with a low number of defects. A liquid epitaxy mechanism is used to describe the formation process of III-V nanocrystals after melting of the implanted thin Si layer by flash lamp annealing. The fabricated InxGa1-xAs nanocrystals are mainly Ga-rich with respect to the implanted Ga/In ratio.

In this presentation the present electron sources and the relevant issues will be discussed. For the electron positron colliders and accelerator based light sources, the electron gun and injector design, are arguably the most critical part. There are a variety of electron source designs: DC guns, normal-conducting RF guns, superconducting RF gun and hybrid guns. All variants have their own ad-vantages and difficulties. We will overview the typical sources around the world, and compare their advantages and main challenges. The polarization production will also be discussed.

We present an overview of iterative reconstruction schemes for Small Angle X-Ray Scattering (SAXS) and also Positron Emission Tomography (PET) that we implemented. Aspects of such algorithms and details about their implementation that we think will be crucial for making visible the electron dynamics in laser-driven plasma experiments are highlighted.

Gold Ore Processing: Project Development and Operations, Second Edition, brings together all the technical aspects relevant to modern gold ore processing, offering a practical perspective that is vital to the successful and responsible development, operation, and closure of any gold ore processing operation. This completely updated edition features coverage of established, newly implemented, and emerging technologies; updated case studies; and additional topics, including automated mineralogy and geometallurgy, cyanide code compliance, recovery of gold from e-waste, handling of gaseous emissions, mercury and arsenic, emerging non-cyanide leaching systems, hydro re-mining, water management, solid–liquid separation, and treatment of challenging ores such as double refractory carbonaceous sulfides. Outlining best practices in gold processing from a variety of perspectives, Gold Ore Processing: Project Development and Operations is a must-have reference for anyone working in the gold industry, including metallurgists, geologists, chemists, mining engineers, and many others.

In the context of integrated computational materials engineering (ICME) recycling covers processes at the end of the lifetime (EoL) of mechanical, electronic, or other components of machines and devices. Depending on the state in which they exist as EoL material they can either be used directly for new material production. This chapter provides a short overview of materials that are being recycled today and the methods applied. It focuses on computational methods applied in the field of recycling, the foremost being methods of computational thermochemistry since mutual solubilities, phase transformations, and reactions as well as heat balances play the most important part in recycling just as they do in standard production. The chapter discusses materials-centric recycling, product-centric recycling, physical separation methods and chemical separation methods. It shows various aspects and phenomena that affect the final recovery of all elements from a product, including the residence time of materials in the market, and subsequent metallurgical processing.

Spin waves, the eigen-excitations of ferromagnets, are promising candidates for spin transport in lateral devices. Fe60Al40 films in the B2 phase is paramagnetic. Starting from a FeAl film in the paramagnetic state the incident ions randomize the site occupancies and, thereby, transform it to the chemically disordered, ferromagnetic A2 phase. The aim is to investigate spin wave propagation in this ferromagnetic material in free standing structure as well as in structure within a paramagnetic matrix. By using Helium-Ion microscopy it is possible to create well defined disordered FeAl conduits with resolution down to nm range. Two di↵erent ferromagnetic stripes were implanted in a microstructure paramagnetic FeAl. A free-standing 2 μm width stripe. And a stripe of the same width with was additionally embedded in the paramagnetic FeAl. For the excitation of spin waves we processed a microwave antenna on top of these stripes. To observe Spin wave behavior Billouin light scattering microscopy was applied. We show that the spin wave behaviour is influenced by the surrounding paramagnetic material due to a di↵erent internal field distribution. In addition the normalized transversal mode widths of spin waves in the embedded systems are wider than in the free standing stripes.

Pathological alterations in cell functions are frequently accompanied by metabolic reprogramming including modifications in amino acid metabolism. Amino acid detection is thus integral to the diagnosis of many hereditary metabolic diseases. The development of malignant diseases as metabolic disorders comes along with a complex dysregulation of genetic and epigenetic factors affecting metabolic enzymes. Cancer cells might transiently or permanently become auxotrophic for non-essential or semi-essential amino acids such as asparagine or arginine. Also, transformed cells are often more susceptible to local shortage of essential amino acids such as methionine than normal tissues. This offers new points of attacking unique metabolic features in cancer cells. To better understand these processes, highly sensitive methods for amino acid detection and quantification are required. Our review summarizes the main methodologies for amino acid detection with a particular focus on applications in biomedicine and cancer, provides a historical overview of the methodological pre-requisites in amino acid analytics. We compare classical and modern approaches such as the combination of gas chromatography and liquid chromatography with mass spectrometry (GC-MS/LC-MS). The latter is increasingly applied in clinical routine. We therefore illustrate an LC-MS workflow for analyzing arginine and methionine as well as their precursors and analogs in biological material. Pitfalls during protocol development are discussed, but LC-MS emerges as a reliable and sensitive tool for the detection of amino acids in biological matrices. Quantification is challenging, but of particular interest in cancer research as targeting arginine and methionine turnover in cancer cells represent novel treatment strategies.

Color processing is a central component of mammalian vision. Gender-related differences of color processing revealed by non-invasive functional transcranial Doppler ultrasound suggested right hemisphere pattern for Blue/Yellow chromatic opponency by men, and a left hemisphere pattern by women. The present study measured the blood-flow related accumulation of [18F]fluorodeoxyglucose ([18F]FDG) in mouse brain using small animal positron emission tomography and magnetic resonance imaging (PET/MRI) with statistical parametric mapping during light stimulation with Blue and Yellow filters compared to darkness condition.
PET revealed a reverse pattern compared to previous human studies: Male mice presented with left visual cortex dominance for blueON-channels through the right eye, while female mice presented with right visual cortex dominance for blueON-channel through the left eye. We applied statistical parametric mapping (SPM) to examine gender differences in activated architectonic areas within the orbital and medial prefrontal cortex and their cortico-cortical connections and sub-cortical networks that lead to the striatum, medial thalamus and other brain areas. The connectivity evoked by Blue stimulation spread through a wide range of brain structures implicated in viscerosensory and visceromotor systems in the left intra-hemispheric regions in male mice, but in the right-to-left inter-hemispheric regions in female mice. Spatial and chromatic opponency was maintained using a yellowON-OFF push-pull interaction in male mice, but a blueON-ON push-forward interaction in female mice. Color functional ocular dominance plasticity was noted in the right eye in male mice but in the left eye in female mice. This animal model could be used in the study of color processing mechanisms and gender complementarity in normal and pathological brain conditions.

Bubble columns (BC) are frequently used in chemical, petroleum and biochemical industries due to their simple construction, ease of temperature control and good heat and mass transfer characteristics. Their hydrodynamics depend on the prevailing flow patterns (regimes) which in turn depend mainly on the superficial gas velocity Ug, the gas distributor design and column diameter. At low Ug values the bubbly flow (homogeneous) regime prevails, which is characterized with relatively small and uniform bubbles and a gentle agitation of the gas-liquid dispersion. The bubble size distribution (BSD) is very narrow and it is only influenced by the gas distributor. A relatively uniform gas holdup profile and a rather flat liquid velocity profile are observed. When the gas distributor is not effective, a gas maldistribution instead of the bubbly flow is observed. The transition regime is characterized by large eddies and a widened BSD due to bubble coalescence. It has been found that the occurrence and the persistence of the transition regime depend largely on the quality of the aeration. The transition from the homogeneous to the heterogeneous (churn-turbulent flow) regime is a gradual process.
In the churn-turbulent flow regime large bubbles start to form whose wakes cause gross circulation patterns. This flow regime is characterized by a wide BSD, vigorous mixing and by the existence of a radial gas holdup profile, which causes liquid circulation, as well. Both bubble coalescence and break-up occur. The gas sparger has little effect on the hydrodynamics.
In particular, the circulation zones give rise to the assumption that regime transitions in different regions occur at different operating conditions. Thus, the primary objective of this work is to compare the main transition velocities Utrans in both the core and annulus of two different BCs based on the modified Shannon entropy (SE). The ratio of the minimum-to-maximum SE in a time-dependent signal can be used successfully for position-dependent flow regime identification in BCs.
The modified SE algorithm has been applied to gas holdup time series data obtained by means of a conductivity wire-mesh sensor (fs=2000 Hz, sensor’s axial position: 1.3 m). Two different BCs operated with an air-deionized water (clear liquid height: 2.0 m) system were used. Both facilities were equipped with perforated plate distributors having the same opening diameter (Ø 4.0×10-3 m). The gas sparger in the small BC (0.15 m in ID) consisted of 14 holes, while the one in the large BC (0.4 m in ID) consisted of 101 holes. In both cases the open area was 1 %.
The SE quantifies the degree of uncertainty involved in predicting the output of a probabilistic event. In the case of fully predictable outcome of an event, the SE will be zero. The definition of the probability in the SE algorithm (Zhong et al., 2009) was modified. Then, the total number of points (60,000) in the signal was divided into six segments (each consisting of 10,000 points) and the modified SE in each of them was calculated. It was found that the ratio of the minimum-to-maximum (SEmin/SEmax) modified SE in every time series at various Ug values can be used for the flow regime identification.
It was found that the dimensionless SEmin/SEmax ratio in the annulus (r/R=0.88) of the small BC (0.15 m in ID) was characterized with two local minima, which corresponded to the two main Utrans values (0.045 and 0.089 m/s). These two boundaries delineated the ranges of the three main hydrodynamic regimes: gas maldistribution (Ug≤0.045 m/s), transition (0.0450.089 m/s). The existence of the gas maldistribution regime in both BCs has been visualized by Nedeltchev et al. (2015).
The SEmin/SEmax in the core (r/R=0) of the small BC (0.15 m in ID) was also capable of identifying the two main Utrans values. At Ug=0.034 m/s the onset of the transition flow regime was identified, whereas at Ug=0.089 m/s the second minimum in the SE ratio distinguished the formation of the churn-turbulent flow regime. The same Utrans values for the whole cross-section of the small BC have been reported by Nedeltchev et al. (2015). It is noteworthy that the minima in the core are much deeper and very well pronounced.
The results in Figure 2 exhibit further that the gas maldistribution ends at lower Ug value in the core of the small BC. The second Utrans value is independent of the radial position. A similar comparison between the Utrans values in both zones of the large BC will be presented. The effect of the radial position on the Utrans values will be studied since it will give an information about the BSD.

Due to the complex hydrodynamics of bubble columns, there are no reliable methods for identification of both main transition velocities. In addition, it is not clear which type of signal is most suitable for flow regime identification. In this work, both the information entropies (IE) and reconstruction entropies (RE) have been extracted for the first time from tomographic raw images obtained by means of ultrafast X-ray tomography. The time series have been recorded with a sampling frequency of 1000 Hz in a bubble column (0.1 m in ID) operated with an air-deionized water system under ambient conditions. The main transition velocities Utrans in two semi-rings from the cross-section of the bubble column have been identified based on both the IE and RE values calculated from 5 signal reconstructions. In each semi-ring the RE algorithm has been applied to two different cases for signal’s processing. In the centrally located smaller semi-ring the two main Utrans values were successfully identified at 0.04 and 0.1 m/s. In the surrounding larger semi-ring the onsets of the transition and heterogeneous regimes occurred at 0.03 and 0.09 m/s. The results imply that following the above-described approaches the main transition velocities can be extracted from any part of the column’s cross-section.
In summary, this work demonstrates that the ultrafast X-ray tomography data can be used for flow regime identification in a bubble column provided that the hidden information in the time series is quantified by both the IE and RE algorithms.

The project DRESDYN (DREsden Sodium facility for DYNamo and thermohydraulic studies) conducted at Helmholtz-Zentrum Dresden-Rossendorf (HZDR) provides a new platform for a variety of liquid sodium experiments devoted to problems of geo- and astrophyscal magnetohydrodynamics.
Most ambitious experiment will be a precession driven dynamo experiment which consists of a large cylindrical cavity lled with liquid sodium that will simultaneously rotate around two axis.
The experiment is motivated by the idea of a precession-driven ow as a complementary energy source for the geodynamo or the ancient lunar dynamo. My presentation addresses corresponding numerical examinations aimed at an optimization of the precession driven ow with regard to improve the dynamo process in the planned experiment.

The bubble column hydrodynamics are complex and the macroscopic flow structure is different in the column core and annulus due to both the bubble coalescence and breakup phenomena as well as the gross liquid circulation. In this work, for the first time the local Kolmogorov entropy (KE) minima at different superficial gas velocities Ug were identified. It was found that there is an agreement between the local KE minima (occurring around r/R=0.63) and the inversion point (dimensionless radius=0.7) for the axial liquid velocity reported by both Chen et al. (1994) and Wu and Al-Dahhan (2001).
The KE radial profiles were also used to confirm the chaotic similarities between the flow patterns in the bubble bed at three different Ug values (0.089, 0.134 and 0.146 m/s) belonging to the heterogeneous regime. This implies that the flow patterns and the degrees of turbulence at these Ug values are also identical. The same similarity was also found between the KE profiles at Ug = 0.056 and 0.067 m/s, which belong to the transition flow regime. These results imply that the flow patterns in the bubble bed repeat (especially at different Ug values falling into the same flow regime).
Based on the KE profiles as a function of Ug , the effect of the dimensionless radial position on the various transition velocities was studied. It was found that the end of the gas maldistribution regime is shifted to slightly higher Ug value in the column core and annulus. In most of the cases, the onset of the churn-turbulent regime occurs at Ug = 0.101 m/s.

Bubble columns (used for absorption, oxidation, chlorination, hydrogenation, waste water treatment, etc.), operate in different hydrodynamic regimes (homogeneous, transition and heterogeneous). It is essential to identify the boundaries between these flow regimes since most of the correlations for prediction of the main design parameters (gas holdup, interfacial area, mass transfer coefficients, etc.) are valid only within a certain flow regime. In the past three decades different methods of data analysis (statistical, spectral, fractal, chaotic, wavelet, etc.) have been developed for flow regime identification. However, they can identify successfully only the first transition velocity (from homogeneous to transition regime). The bubble column hydrodynamics are very complex and usually more than two regime transitions occur. They could be detected by means of some new and more powerful method of data analysis. In this work, we introduce a new dimensionless parameter based on the division of the X-ray tomography data into many state vectors. Some routines from nonlinear chaos analysis (Schouten et al., 1994) are used.
The bubble column had an inner diameter of 0.1 m and was equipped with a perforated plate distributor (55 holes, ø 0.5×10-3 m). The gas-liquid system consisted of air and deionized water. The clear liquid height Ho was set at 0.66 m. Superficial gas velocities Ug ranging from 0.01 up to 0.10 m/s were employed. The data used for the new method were recorded by means of ultrafast X-ray tomography (scan level=0.5 m). The time series consisted of 29,000 points and were sampled with a frequency of 1000 Hz.
Every reconstructed image was divided into the same semi-rings. In this work the pixel values in a specific semi-ring (inner radius=10×10-3 m ; outer radius=15×10-3 m) were used for further analysis. The data were divided into state vectors consisting of 50 elements and then the distance between pre-selected vector pairs was estimated. For this purpose, the maximum norm (Schouten et al., 1994) was used, i.e. the vector distance was equal to the maximum absolute difference between two elements from the vector pair. The number of vector pairs with distance smaller than some pre-selected criterion (three times the average absolute deviation (AAD)) was used as a basis for the new method for flow regime identification in a bubble column.
It was found that the ratio of the number of vector pairs (with a distance smaller than 3AAD) found in the second part of the signal divided by the one in the first part of the signal can be used for identifying three transition velocities Utrans. They correspond to three well-pronounced local minima. At Ug=0.02 m/s the gas maldistribution regime transforms itself into homogeneous (bubbly) regime. This flow regime is stable up to Ug=0.04 m/s. Beyond this critical gas velocity begins the transition flow regime. The onset of the heterogeneous (churn-turbulent) regime occurs at Ug=0.06 m/s.
When the reconstruction entropies (RE) (Nedeltchev, 2015) are extracted from the vector pairs (meeting the criterion about the vector distance) in both the first and second parts of the signal and the ratio between them is calculated, the same three Utrans values are identified. It was illustrated that the three local minima occur at Ug=0.02, 0.04 and 0.06 m/s, respectively.
In the full-length contribution, based on the above-mentioned new approach, the transition velocities Utrans in many different parts from the column’s cross-section will be identified. A comparison between the transition velocities in the column core and annulus will also be shown.

The application of bubble columns to industrial processes, such as Fischer-Tropsch synthesis and liquid-phase methanol synthesis, often involves a large amount of heat generation. That is why, heat exchangers are installed to remove the generated heat. However, the bubble dynamics in bubble columns with dense internals is still not well understood.
In this work, for the first time a flow regime identification in a bubble column with internals (dense vertical heat exchanger tubes) was performed. The bubble column had an inner diameter of 0.1 m and was equipped with a perforated plate distributor (55 holes, ø 0.5×10-3 m). The gas-liquid system consisted of air and deionized water. The clear liquid height Ho was set at 1.1 m. Superficial gas velocities Ug ranging from 0.01 up to 0.15 m/s were employed. The bubble column was equipped with 37 heat exchanger tubes having a square pitch with a diameter of 8×10-3 m and a clearance of 3×10-3 m. Gas holdup fluctuations were recorded by means of a conductivity wire-mesh sensor installed at an axial position of 0.715 m. The time series (60,000 points, sampling frequency (fs)=2000 Hz) were further treated based on the non-linear chaos theory (Schouten et al., 1994; Nedeltchev et al., 2014).
For comparison, the two main transition velocities Utrans in the empty bubble column (Ho=0.66 m) counterpart were also identified. The information entropies were extracted from X-ray data (29,000 points, fs=1000 Hz) recorded by the ultrafast tomographic facility. It was shown that in a bubble column with internals two main transition velocities Utrans can be identified by means of the Kolmogorov entropy (KE) profile. The flow regime boundaries are identifiable on the basis of the sudden change in the decreasing KE rate. It is interesting to note that well-pronounced local KE minima (Nedeltchev et al., 2014), known from empty bubble columns, are not observed in a bubble column with internals.
At Ug=0.05 m/s the bubbly flow (homogeneous) regime transforms itself into the transition regime. The rate of the KE decrease in both flow regimes is different. At Ug=0.11 m/s the heterogeneous regime (mixture of churn-turbulent and slug flow regimes) is formed. It is characterized with constant KE values. The existence of the slug flow regime in the column core is explainable with the relatively small diameter of the column at which, according to Wilkinson et al. (1992), the effect of the column wall is still present.
In an empty bubble column, two well-pronounced local minima of the information entropy values denote the two main Utrans values. The first transition velocity occurs earlier at Ug=0.04 m/s as compared to the column with internals, which means that the presence of internals stabilizes the bubbly flow regime. The second transition velocity (the onset of the heterogeneous flow regime) is unaffected by the internals.
In the full-length contribution, the time-dependent nature of the main transition velocities as well as the effect of the axial height on the Utrans values in bubble columns with and without internals will also be discussed in a comparable manner. A comparison between the transition velocities in the column core and annulus will also be shown.

Bubble columns are characterized by an effective phase contact, high heat and mass transfer coefficients, low maintenance and operating costs due to the absence of moving parts and low column pressure drop. Due to their numerous advantages bubble columns are used extensively in many applications (oxidation, chlorination, waste water treatment, etc.). Therefore, it is essential to have detailed knowledge about the hydrodynamic behavior of these gas-liquid contactors. The identification of the boundaries of the main hydrodynamic regimes is important for improvement of the design, operation and control of bubble columns. The main objective of our work is to apply a new identification method (based on the modified Shannon entropy) to x-ray tomography data for accurate determination of the boundaries of the main hydrodynamic regimes (homogeneous, transition and heterogeneous).
The time series (extracted from reconstructed raw images) were measured by means of ultrafast x-ray tomography (sampling frequency=1000 Hz) in a bubble column (0.1 m in ID) and they were subsequently treated by the modified Shannon entropy algorithm developed by Nedeltchev et al. (2016). The raw time series give very good information about the x-ray attenuation and they are measure for the density distribution and the fraction of gas phase in different regions from the column’s cross-section. The column was equipped with a perforated plate distributor (55 holes, Ø 0.5×10-3 m) and operated with an air-deionized water system at ambient conditions. The tomographic scans were performed at an axial height of 0.5 m.
The data were organized in groups of 100 points and their sums were calculated. These sums were needed for the calculation of the probabilities of appearance of a particular value in the time series and the local Shannon entropies. It was found that the maximum sum can be used as a flow regime identifier. It was shown that two well-pronounced minima can be distinguished in the maximum sum values extracted at different superficial gas velocities Ug in the central part of the column’s cross-section. The first local minimum occurs at Ug=0.03 m/s and identifies the end of the homogeneous regime. The onset of the heterogeneous regime occurs at Ug=0.07 m/s. It was illustrated that the information entropy extracted from the data in the entire cross-section is capable of identifying the two main transition velocities at 0.025 m/s and 0.085 m/s. So, it was concluded that the heterogeneous regime starts somewhat earlier in the center of the cross-section. The homogeneous regime in the center and the entire cross-section ends at practically the same Ug value (0.025-0.03 m/s). It is noteworthy that for air-water system the theoretical prediction (0.029 m/s) by the correlation of Reilly et al. (1994) is very close to our experimental results.
Such a comparison has been performed at 20 different segments of the column’s cross section. The approach enables the preparation of a radial profile of the transition velocities. Flow regime identification results based on the maximum sums, information amounts and Shannon entropies are compared and discussed.

Objectives: In an ongoing clinical study (–)-(S)-[18F]fluspidine (1, 2) is being investigated for imaging of sigma-1 receptors in patients with major depression by PET. Beside estimation of the fraction of unchanged radiotracer in plasma and urine, radiometabolites formed should be detected and their structures elucidated.
Methods: (–)-(S)-[18F]Fluspidine or unlabelled reference were incubated with human liver microsomes (HLM) in presence of NADPH and/or activated glucuronic acid (UDPGA) at 37°C. Metabolites were detected by radio-HPLC or LC-MS and characterized by aid of reference compounds or structural elucidation using different MS methods (EPI, MS3). Plasma (10, 20, 30 min p.i) and urine (90 min p.i.) samples of human subjects receiving 268 (245-290) MBq (–)-(S)-[18F]fluspidine i.v. were investigated and compared to results from HLM incubations.
Results: By incubation with HLM mainly 3 hydroxylation products and one debenzylation product were formed. The product hydroxylated at the alkyl side chain was glucuronidated subsequently. Plasma samples (10, 20, 30 min p.i.) obtained from human showed 97.7%, 93.8%, and 88.6% (SD=2.6-7.9, n=6-8) of unchanged tracer. In urine (90 min p.i.) the fraction of tracer was 0–7.8% (average of 2.3%, n=10) and up to 3 main radiometabolites were detected (Figure 1). The one with the highest intensity, also found in plasma, matched the glucuronide formed in vitro. Debenzylation of the parent tracer was detected with a small proportion.
Conclusions: The results demonstrate an appropriate metabolic stability of (–)-(S)-[18F]fluspidine for the application as PET ligand. The structure of the major radiometabolite found in plasma and urine could be assigned by means of in vitro studies. Routes of metabolism are currently investigated in more detail. 302
References:
[1] German Clinical Trial Register, DRKS-ID: DRKS00008321
[2] Fischer et al. Eur. J. Nucl. Med. Mol. Imaging 2011, 38, 540–551

In our contribution we give a brief overview of two widely discussed quantum processes: electron-positron pairs production off a probe photon propagating through a polarized short-pulsed electromagnetic (e.m.) (e.g.\ laser) wave field or generalized Breit-Wheeler process and a single a photon emission off an electron interacting with the laser pules, so-called non-linear Compton scattering. We show that at small and moderate laser field intensities the shape and duration of the pulse are very important for the probability of considered processes. However, at high intensities the multi-photon interactions of the fermions with laser field are decisive and completely determined all aspects of subthreshold electron-positron pairs and photon production

Context. Material processed by the CNO cycle in stellar interiors is enriched in 17O. When mixing processes from the stellar surface reach these layers, as occurs when stars become red giants and undergo the first dredge up, the abundance of 17O increases. Such an occurrence explains the drop of the 16O/17O observed in RGB stars with mass larger than 1.5 M_\solar. As a consequence, the interstellar medium is continuously polluted by the wind of evolved stars enriched in 17O . Aims. Recently, the Laboratory for Underground Nuclear Astrophysics (LUNA) collaboration released an improved rate of the 17O(p,alpha)14N reaction. In this paper we discuss the impact that the revised rate has on the 16O/17O ratio at the stellar surface and on 17O stellar yields. Methods. We computed stellar models of initial mass between 1 and 20 M_\solar and compared the results obtained by adopting the revised rate of the 17O(p,alpha)14N to those obtained using previous rates. Results. The post-first dredge up 16O/17O ratios are about 20% larger than previously obtained. Negligible variations are found in the case of the second and the third dredge up. In spite of the larger 17O(p,alpha)14N rate, we confirm previous claims that an extra-mixing process on the red giant branch, commonly invoked to explain the low carbon isotopic ratio observed in bright low-mass giant stars, marginally affects the 16O/17O ratio. Possible effects on AGB extra-mixing episodes are also discussed. As a whole, a substantial reduction of 17O stellar yields is found. In particular, the net yield of stars with mass ranging between 2 and 20 M_\solar is 15 to 40% smaller than previously estimated. Conclusions. The revision of the 17O(p,alpha)14N rate has a major impact on the interpretation of the 16O/17O observed in evolved giants, in stardust grains and on the 17O stellar yields.

The portable consumer electronics necessitates functional elements to be lightweight, flexible, and wearable [1-4]. The unique possibility to adjust the shape of the devices offered by this alternative formulation of the electronics provides vast advantages over the conventional rigid devices particularly in medicine and consumer electronics. There is already a remarkable number of available flexible devices starting from interconnects, sensing elements towards complex platforms consisting of communication and diagnostic components.
We developed shapeable magnetoelectronics [5] – namely, flexible [6-8], printable [9,10], stretchable [11,12] and even imperceptible [13] magnetosensitive large area elements, which were completely missing in the family of flexible electronics, e.g. for smart skin applications. On the other hand, we realized self-assembled compact tubular microchannels based on strain engineering [14] with integrated passive sensory elements [15-17] and communication antenna devices [18] for on-chip and bio-medical applications, e.g. smart implants [19,20].
Combining these two research directions carried out at different length scales into a single truly interdisciplinary topic opens up the novel field of smart biomimetics [20]. In this respect, we demonstrated mechanically and electrically active compact biomimetic microelectronics, which can serve as a base for realization of novel regenerative neuronal cuff implants with unmatched functionalities. The biomimetic microelectronics can mechanically adapt to and impact the environment possessing the possibility to assess, adopt and communicate the environmental changes and even stimulate the environment electrically.
In my talk, these recent developments will be covered.

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[2] J. A. Rogers et al., Nature 477, 45 (2011).
[3] S. Bauer et al., Adv. Mater. 26, 149 (2014).
[4] M. Kaltenbrunner et al., Nature 499, 458 (2013).
[5] D. Makarov et al., Appl. Phys. Rev. 3, 011101 (2016).
[6] G. Lin, D. Makarov et al., Lab Chip 14, 4050 (2014).
[7] M. Melzer, D. Makarov et al., Adv. Mater. 27, 1274 (2015).
[8] N. Münzenrieder, D. Makarov et al., Adv. Electron. Mater. (2016), 10.1002/aelm.201600188.
[9] D. Karnaushenko, D. Makarov et al., Adv. Mater. 27, 880 (2015).
[10] D. Karnaushenko, D. Makarov et al., Adv. Mater. 24, 4518 (2012).
[11] M. Melzer, D. Makarov et al., Adv. Mater. 27, 1333 (2015).
[12] M. Melzer, D. Makarov et al., Nano Lett. 11, 2522 (2011).
[13] M. Melzer, D. Makarov et al., Nat. Commun. 6, 6080 (2015).
[14] O. G. Schmidt et al., Nature 410, 168 (2001).
[15] I. Mönch, D. Makarov et al., ACS Nano 5, 7436 (2011).
[16] C. Müller, D. Makarov et al., Appl. Phys. Lett. 100, 022409 (2012).
[17] E. J. Smith, D. Makarov et al., Lab Chip 12, 1917 (2012).
[18] D. D. Karnaushenko, D. Makarov et al., NPG Asia Materials 7, e188 (2015).
[19] D. Karnaushenko, D. Makarov et al., Adv. Mater. 27, 6582 (2015).
[20] D. Karnaushenko, D. Makarov et al., Adv. Mater. 27, 6797 (2015).

The twisted magnetization textures in chiral magnets are inherently frustrated, similarly to the mesophases in chiral liquid-crystals. The twisted basic texture can become dramatically altered by the penetration of secondary twists over larger lengths and the formation of defects. Hence, a well-ordered and smooth texture like a simple spiral may be twisted or defected. In chiral liquid-crystal systems, the frustration results in the formation of defects like the disclination networks of blue phases or twisted-grain-boundary phases. Such states can easily be shaped and transformed under the influence of competing anisotropies, e.g., by applied fields in the bulk and by anchoring the molecules of a liquid crystal at surfaces.
We investigated surfaces of FeGe single crystals with the cubic B20 structure using various magnetic imaging techniques and found a ferromagnetic order above the magnetic ordering transition in the bulk. This ferromagnetic order is seen by magnetic optical Kerr effect (MOKE) microscopy as a simple ferromagnetic domain structure of an Ising-like magnet at room-temperature. Scanning electron microcopy with polarization analysis (SEMPA) and X-ray photoemission electron microscopy (XPEEM) allowed us to follow the evolution of a fine-structure in this ferromagnetic surface upon lowering the temperature, when the bulk of the FeGe crystal orders into the spiral ground-state.
We discover a static defect-ordered state with a network of line-defects emerges near the surface under the influence of a particular surface-magnetic ordering transition. These defects of the helical magnetic order are topologically necessary lines where the magnetic order becomes singular or passes through zero at elevated temperatures. This ferromagnetic skin has a strong uniaxial anisotropy and frustrates the helimagnetic texture by anchoring it to the surface. In the spiral below the Neel temperature at 279 K, conical modulations in the ferromagnetic surface layer are observed that prove the formation of a network of dislocations because the propagation direction of the surface-modulation deviates from the propagation direction in the bulk. Near magnetic ordering temperature a coexistence of bubble-like circular domains and stripes is observed in the surface layer. This illustrates the appearance of complex three-dimensional textures with defects, double-twists and spiral-like kinks near the surface and related to the particular surface-magnetic ordering. Hence, at the first-order transition between the precursor state and spiral order in zero magnetic field of FeGe, a co-existence of helical and skyrmionic textures is revealed. Ab initio calculations have been used to motivate the existence of enhanced spin-moments at the surfaces of FeGe and an increased effect of spin-orbit coupling. This explains the experimental observations of a surface-magnetic ordering in FeGe, which acts like a strongly uniaxial ferromagnetic film with an Ising-like character on the underlying spiral bulk state.
Similar experiments using MOKE and XPEEM on the isostructural compound FeSi give evidence of a fragile magnetic ordering at the surface of this anomalous paramagnetic semiconductor, too. This may mean that the FeSi surfaces may behave like strongly anisotropic ultrathin magnetic films, while no magnetic long-range ordering takes place in the bulk.

While conventionally magnetic films and structures are fabricated on flat surfaces, the topology of curved surfaces has only recently started to be explored and leads to new fundamental physics as well as applied device ideas [1]. In particular, novel effects occur when the magnetization is modulated by curvature providing a new degree of freedom that leads to new magnetization configurations (see for instance [2,3]) and is predicted to have major implications on the spin dynamics due to topological constraints for instance in circular tubes and rolls [4].
Advances in this novel field solely rely on the understanding of the fundamentals behind the modifications of magnetic responses of 3D-curved magnetic thin films. The lack of an inversion symmetry and the emergence of a curvature induced effective anisotropy and Dzyaloshinskii-Moriya interaction are characteristic of curved surfaces [5-7], leading to curvature-driven magnetochiral effects [8-10] and topologically induced magnetization patterning [7, 11], including unlimited domain wall velocities in hollow tubes [4], chirality symmetry breaking [7-10] and Cherenkov-like effects for magnons [12]. In addition to these rich physics, the application potential of 3D-shaped objects is currently being explored as magnetic field sensorics for magnetofluidic applications [13], spin-wave filters [14], magneto-encephalography devices [15] and high-speed racetrack memory devices [4]. To this end, the initially fundamental topic of the magnetism in curved geometries strongly benefited from the input of the application-oriented community, which among others explores the shapeability aspect of the curved magnetic thin films. These activities resulted in the development of the family of shapeable magnetoelectronics [16], which already includes flexible [17], printable [18], stretchable [19] and even imperceptible [20] magnetic field sensorics.
These recent developments starting from the theoretical predictions to the fabrication and characterization of 3D-curved magnetic thin films and their application potential are in the focus of this talk.
References
[1] R. Streubel, DM et al., J. Phys. D: Appl. Phys. vol. 49, pp. 363001, 2016.
[4] M. Yan et al., Phys. Rev. Lett. vol. 104, pp. 057201, 2010.
[5] Y. Gaididei et al., Phys. Rev. Lett. vol. 112, pp. 257203, 2014.
[6] O. V. Pylypovskyi, DM et al., Phys. Rev. Lett. vol. 114, pp. 197204, 2015.
[7] O. V. Pylypovskyi, DM et al., Sci. Rep. vol. 6, pp. 23316, 2016.
[8] R. Hertel, SPIN vol. 03, pp. 1340009, 2013.
[9] M. Yan et al., Appl. Phys. Lett. vol. 100, pp. 252401, 2012.
[10] J. A. Otalora et al., Appl. Phys. Lett. vol. 100, pp. 072407, 2012.
[11] V. P. Kravchuk, DM et al., Phys. Rev. B vol. 85, pp. 144433, 2012.
[12] M. Yan et al., Phys. Rev. B vol. 88, pp. 220412, 2013.
[13] I. Mönch, DM et al., ACS Nano vol. 5, pp. 7436, 2011.
[14] F. Balhorn et al., Phys. Rev. Lett. vol. 104, pp. 037205, 2010.
[15] D. Karnaushenko, DM et al., Adv. Mater. vol. 27, pp. 6582, 2015.
[16] D. Makarov et al., Appl. Phys. Rev. vol. 3, pp. 011101, 2016.
[17] M. Melzer, DM et al., Adv. Mater. vol. 27, pp. 1274, 2015.
[18] D. Karnaushenko, DM et al., Adv. Mater. vol. 27, pp. 880, 2015.
[19] M. Melzer, DM et al., Nano Lett. vol. 11, pp. 2522, 2011.
[20] M. Melzer, DM et al., Nature Commun. vol. 6, pp. 6080, 2015.

Cosmogenic nuclides in meteorites can provide information on cosmic ray exposure (CRE) histories. In space, meteoroids are irradiated by galactic cosmic ray particles, inducing the production of cosmogenic nuclides (¹⁰Be, ²⁶Al, ³⁶Cl, ⁴¹Ca, ⁵³Mn, ⁶⁰Fe). Meteorites are routinely measured for ¹⁰Be, ²⁶Al, and ³⁶Cl. However the database for ⁵³Mn and ⁶⁰Fe is scarce due to the low availability of high-MV accelerators and the debate over the half-lives of ⁵³Mn and ⁶⁰Fe. We Report new ⁵³Mn and ⁶⁰Fe data for iron meteorites measured at Canberra (⁵³Mn, ⁶⁰Fe) and Munich (⁶⁰Fe). Among these radionuclides, ⁵³Mn has the longest half-life, thus is least influenced by terrestrial ages. The advantage of ⁵³Mn and ⁶⁰Fe isotopes is that only two (Fe, Ni) and one (Fe) target element(s), respectively, dominate production, overcoming the problem of inhomogeneous S and P distribution. Our new ⁶⁰Fe data almost doubles that present in the literature. We measured ⁵³Mn in seven subsamples of the iron meteorite Twannberg. The new ⁵³Mn and ⁶⁰Fe data, with ¹⁰Be, ²⁶Al, ³⁶Cl, ⁴¹Ca and the noble gases, will better constrain the CRE histories of meteorites and will also serve as benchmarks to validate and improve Monte-Carlo model calculations.

Spin-transfer-torque induced switching is investigated in 200 nm diameter circularly shaped, perpendicular magnetized nanopillars. A synthetic antiferromagnet, consisting of two Co/Ni multilayers coupled anti-ferromagnetically across a Ru layer, is used as a reference layer to minimize the dipolar field on the free layer. The free layer is a single 4x[Co/Ni] multilayer. The use of Pt and Pd was avoided to lower the spin-orbit scattering in magnetic layers and intrinsic damping in the free layer, and therefore, reduce the critical current required for spin-transfer-torque switching. The intrinsic Gilbert damping of a continuous 4[Co/Ni] multilayer film was measured by ferromagnetic resonance to be alpha = 0.022, which is significantly lower than in Pt or Pd based magnetic multilayers. In zero magnetic field the critical current required to switch the free layer from the parallel to antiparallel alignment is 5.2 mA, and from antiparallel to parallel alignment is 4.9 mA. Given the volume of the free layer, V_FL = 1.011022 m3, the switching efficiency, I_c=(V_FL/µ0H_c), is 5.281020 A/Tm^3, twice as efficient as any previously reported device with a similar structure

Our multi-method MS study (AMS, noble gas MS, LA-(MC)-ICP-MS) aims to constrain the evolution of the western Namibian drainages since the last ca. 40 Ma. Therefore, fluvial sediments of several rivers and their precursors were sampled. In order to obtain precise Surface exposure ages of the various terrace levels, the routinely used cosmogenic nuclides ¹⁰Be, ²¹Ne, ²⁶Al (quartz), and ³⁶Cl (calcite) were applied either on surface samples or on depth-profiles consisting of 3 to 5 samples each. U-Pb small scale isochrone (SSI) ages of calcareous matrices were also used for terrace dating. Sedimentary provenances were revealed by detrital zircon (ZrSiO₄) geochronology using U-Th-Pb and Lu-Hf isotope systematics. They indicate varying detrital zircon patterns through time. Our approach facilitates the recognition of changes in the fluvial sediment provenance at certain points in time. Such combined studies have a huge potential for revealing the palaeohydrological history, and to estimate amplitudes and processing Speeds of past events or changing sizes of catchment areas, which is of particular interest for modelling the palaeoclimate and palaeogeography.

During the sump recirculation phase after loss-of-coolant accidents (LOCA) in pressurized water reactors (PWR), coolant spilling out of the leak in the primary cooling circuit is collected in the reactor sump and recirculated to the reactor core by residual-heat removal pumps. The long-term contact of the boric acid containing coolant with hot-dip galvanized containment internals (e.g. grating treads, supporting grids of sump strainers) may cause corrosion of the corresponding materials influencing the cooling water chemistry.
Generic investigations regarding such zinc corrosion processes, changes of the coolant chemistry and possible resulting in-core effects are subject of joint research projects of the Helmholtz-Zentrum Dresden-Rossendorf (HZDR), TU Dresden (TUD) and Zittau/Görlitz University of Applied Sciences (HSZG). Lab-scale experiments at HZDR and TUD were focused on elucidation of physico-chemical corrosion and precipitation processes as well as resulting clogging effects [1-2].
Recent results of generic experiments in a lab-scale corrosion test facility led to further information regarding the main parameters determining the zinc corrosion rates and the whole corrosion process in such scenarios.
Main influences on the zinc corrosion rates were identified as the impact of the coolant jet onto the corroding surface and the particular flow conditions around submerged zinc surfaces.
In contrast, variations of the coolant temperature in the range between 25 °C and 70 °C as well as small changes in the boric acid concentration have no significant influence on the corrosion rates during the first stage of the corrosion process.
Further lab-scale experiments at realistic time-dependent LOCA parameters like calculated temperature courses in the sump and inside the reactor core are planned to evaluate, if zinc corrosion processes with subsequent zinc borate precipitations could lead to considerable clogging effects inside the reactor core.
The results obtained at lab-scale were complemented by corresponding experiments in semi-technical test facilities of the project partner HSZG.

[1] Seeliger, A.; Alt, S.; Kästner, W.; Renger, S.; Kryk, H., Harm, U. : Zinc corrosion after loss-of-coolant accidents in pressurized water reactors - thermo- and fluid-dynamic effects. Nuclear Engineering and Design, 2016, 305, 489-502
[2] Hoffmann, W.; Kryk, H.; Seeliger, A.; Kästner, W.; Alt, S. & Renger, S.: Zinc corrosion after loss-of-coolant accidents in pressurized water reactors - physicochemical effects. Nuclear Engineering and Design, 2014, 280, 570-578

This diploma thesis extends the open source particle-in-cell code PIConGPU by two new physics modules which incorporate effects of radiation emission and back reaction of highly relativistic electrons in strong electromagnetic background fields into the simulation. The first module involves the treatment of nonlinear Thomson- and Compton-scattering using the synchrotron approximation. It allows for the generation of X-ray and gamma photons in the classical regime as well as in the QED regime including self consistent radiation back reaction. Through simulations of collisions between laser pulses and electron bunches the impact of QED effects on experimental spectra is investigated. The second module covers the scattering of electrons on atomic nuclei including electron deflection and generation of Bremsstrahlung-photons. In a numerical case study it is shown that the analysis of Bremstrahlung can be used as experimental diagnostic for electron dynamics in overdense plasmas.

Das Radionuklid ⁴⁴Ti (T_1/2 = 58,9 a) wird vor allem während Supernovaexplosionen gebildet und spielt eine wichtige Rolle für deren theoretische Modelle und die Nukleosynthese schwerer Elemente. In Supernovaüberresten kann ⁴⁴Ti mittels &gamma-Astronomie nachgewiesen werden, allerdings befinden sich die Beobachtungen nicht im Einklang mit den theoretischen Modellen. Problematisch dabei ist, dass der Wirkungsquerschnitt der Reaktion ⁴⁰Ca(&alpha,&gamma)⁴⁴Ti bisher nur unzureichend bekannt ist [1].
Während bislang nur ⁴⁴Ti-AMS-Messungen an großen Beschleunigern (ab 10 MV Terminalspannung) durchgeführt wurden [2], sollte es prinzipiell auch möglich sein, an 6-MV-Anlagen dieses Radionuklid zuverlässig zu messen. Wir präsentieren erste Tests an der AMS-Anlage DREAMS des HZDR, die zeigen, dass mithilfe einer Degrader-Folie eine zuverlässige Abtrennung des stabilen Isobars ⁴⁴Ca und Messung des Radionuklids ⁴⁴Ti auch bei Beschleunigungsspannungen von 6 MV möglich ist.
Diese ersten Tests dienen dazu, die Machbarkeit von AMS-basierten Messungen des Wirkungsquerschnitts der Reaktion ⁴⁰Ca(&alpha,&gamma)⁴⁴Ti an DREAMS auszuloten.
Das Projekt wurde unterstützt vom DAAD.

Ref.: [1] Schmidt et al., Phys. Rev. C 88, 025803 (2013)
[2] Nassar et al., Phys. Rev. Let. 96, 041102 (2006)

In the work presented in this paper, the shape and absorption rate of an individual elongated Taylor bubble of CO2 through contaminated water was measured in millimeter-size channel. The influence of concentration of surfactant on dissolution rate of an individual elongated Taylor bubble of carbon dioxide in water was investigated using high resolution X-ray radiography technique in vertical channels. The bubbles were held stationary in the down-flowing liquid and the liquid-side mass transfer coefficient was determined from microfocus X-ray images.
The experiments cover a range of initial bubble equivalent diameter (deq: sphere-volume equivalent bubble diameter) varying from 6 to 10 mm. The pipe is a glass pipe with 6 mm inside diameter (D). The bubble is unceasingly monitored by holding the bubble stationary using downward flow of liquid. The X-ray method was chosen since it is not dependent on the refractive index; therefore it is the most accurate method in comparison with other conventional optical techniques. This technique was qualified to disclose the three-dimensional shape of Taylor bubbles in capillary and enabled the acquisition of a series of high-resolution radiographic images of nearly stationary Taylor bubbles (Haghnegahdar et al., 2015). The processed images which give volume (and also the interfacial area) of the bubble with high accuracy as a function of time, are used to evaluate the liquid side mass transfer coefficient between bubble and liquid using the mass conservation equation. The liquid phase is milli-pore water contaminated by conventional surfactants and the gas phase is CO2.
The results confirmed the accumulation of surfactants on the tail of the bubbles. Furthermore, applying different concentrations of surfactant reveals that in our case, where surface coverage ratio of surfactant on the bubbles is high, increase of contamination does not have a noticeable influence on the mass transfer coefficient of bubbles.

In the work presented in this paper, the shape and absorption rate of an individual elongated Taylor bubble of CO2 through contaminated water was measured in millimeter-size channel. The influence of presence of trace amount of surfactant on dissolution rate of an individual elongated Taylor bubble of carbon dioxide in water was investigated using high resolution X-ray radiography technique in vertical channels. The bubbles were held stationary in the down-flowing liquid and the liquid-side mass transfer coefficient was determined from microfocus X-ray images.
The experiments cover a range of initial bubble equivalent diameter (deq: sphere-volume equivalent bubble diameter) varying from 6 to 10 mm. The pipe is a glass pipe with 6 mm inside diameter (D). The bubble is unceasingly monitored by holding the bubble stationary using downward flow of liquid. The X-ray method was chosen since it is not dependent on the refractive index; therefore it is the most accurate method in comparison with other conventional optical techniques. This technique was qualified to disclose the three-dimensional shape of Taylor bubbles in capillary and enabled the acquisition of a series of high-resolution radiographic images of nearly stationary Taylor bubbles (Haghnegahdar et al., 2015). The processed images which give volume (and also the interfacial area) of the bubble with high accuracy as a function of time, are used to evaluate the liquid side mass transfer coefficient between bubble and liquid using the mass conservation equation. The liquid phase is milli-pore water contaminated by conventional surfactants and the gas phase is CO2.
The results confirmed the accumulation of surfactants on the tail of the bubbles. Furtheremore, it was shown that the presence of surfactants not only decrease the rate of mass transfer, but also change the bubble shape and liquid film thickness around the bubble.

For milli- and micro-reactors the bubble shape and relative velocity between two phases are mainly governed by the cross-sectional shape of the channel. For channels with circular cross section (pipes) enormous attention has been paid in the last decades and many studies on hydrodynamics and mass transfer to be found in literature. However other channel cross sections such as square channels were a subject of only a few studies [1]. Concerning the role and importance of square channels in various existing and potential industrial applications such as micro-electromechanical systems, monolith froth reactors, there exist still some gaps particularly in related aspects of transport phenomena in these channels and there needs to be further experimental work to provide detailed heat and mass transfer data for model validation.
In the work presented in this paper, the dissolution rate of a single Taylor bubble of carbon dioxide in water was investigated using high resolution X-ray radiography and tomography technique in vertical channels. The liquid side mass transfer coefficient was calculated by measuring the changes in the size of the bubble at constant pressure. The experiments cover a large range of initial Taylor bubble length varying from 4 to 26 mm. The pipe is a glass pipe with 6 mm inside diameter and square cross section. The bubbles were held stationary using the technique of Schulze and Schluender [2]. The method which is used to measure the variation of the bubble size is X-ray tomography. The X-ray method was chosen since it is not dependent on the refractive index; therefore it is the most accurate method in comparison with other conventional optical techniques. Furthermore this technique allows tomography for square channels, while full 3D shape determination by optical techniques is difficult in square channels. The processed images which give volume (and also the interfacial area) of the bubble as a function of time, are used to evaluate the liquid side mass transfer coefficient between bubble and liquid using the mass conservation equation.
The results for the long term dissolution of single CO2 bubbles show that the dissolution curves for bubbles with different initial size follow the same trend and have relatively constant slope. In addition, it is shown that the measured mass transfer coefficient increases as the equivalent diameter of the bubble (diameter of the sphere having the same volume) decreases. The trend for the change of liquid-side mass transfer coefficient as a function of bubble size is in accordance with the data predictivd by the penetration theory.

In the current years increasing efforts have been done to develop sustainable processes with smaller ecological footprint, which is. to decrease the industrial pollution and the environmental impact.
One serious pollutant that results from the textile industry etc. is the increasing usage of dyes. The treatment of dye-polluted water is still challenging since today's methods, such as absorption and membrane filtration, have their limitations.
The application of biocatalysts represents a sustainable solution as it results in nontoxic products at comparable eco-friendly treatment costs. In particular, oxidation enzymes, such as laccase, which can oxidize dye are in the scope. However, direct application of laccase enzyme is not favorable because it requires processes to recover the enzyme, while enzymes, immobilized on a carrier can be re-used as long as the activity is sufficiently high.
Loofa is a natural-grown material of the cucumber family, which provides attractive morphological properties. Moreover, loofa carrier can be decomposed after the process without additional treatment and is inexpensive.
In the contribution, the developed laccase immobilization methodology and the optimization of the immobilization using the Response Surface Methodology (RMS) will be discussed. Furthermore, the capability to degrade dye-polluted water will be evaluated and a novel bioreactor for the water treatment will be suggested

The computation power of supercomputers grows faster than the bandwidth of their storage and network. Especially applications using hardware accelerators like Nvidia GPUs cannot save enough data to be analyzed in a later step. There is a high risk of loosing important scientific information. We introduce the in situ template library ISAAC which enables arbitrary applications like scientific simulations to live visualize their data without the need of deep copy operations or data transformation using the very same compute node and hardware accelerator the data is already residing on. Arbitrary meta data can be added to the renderings and user defined steering commands can be asynchronously sent back to the running application. Using an aggregating server, ISAAC streams the interactive visualization video and enables user to access their applications from everywhere.

The quark meson (linear sigma) model with linearized fluctuations displays at a critical end point the onset of a curve of first-order phase transitions (FOPTs) located at non-zero chemical potentials and temperatures below a certain cross-over temperature. The model qualifies well for an illustrative example to study the impact of the emerging FOPT, e.g. on photon emissivities. Such a case study unravels the tight interlocking of the phase structure with the emission rates, here calculated according to lowest-order tree level processes by kinetic theory expressions. It is the strong dependence of the rates on the effective masses of the involved degrees of freedom which distinctively vary over the phase diagram thus shaping the emissivity accordingly. At the same time, thermodynamic properties of the medium are linked decisively to these effective masses, i.e. a consistent evaluation of thermodynamics, governing for instance adiabatic expansion paths, and emission rates is maintained within such an approach.

In the current years increasing efforts have been done to develop sustainable processes with smaller ecological footprint, which is. to decrease the industrial pollution and the environmental impact.
One serious pollutant that results from the textile industry etc. is the increasing usage of dyes. The treatment of dye-polluted water is still challenging since today's methods, such as absorption and membrane filtration, have their limitations.
The application of biocatalysts represents a sustainable solution as it results in nontoxic products at comparable eco-friendly treatment costs. In particular, oxidation enzymes, such as laccase, which can oxidize dye are in the scope. However, direct application of laccase enzyme is not favorable because it requires processes to recover the enzyme, while enzymes, immobilized on the carrier can be re-used as long as the activity is sufficiently high.
Loofa is a natural-grown material of the cucumber family, which provides attractive morphological properties. Moreover, loofa carrier can be decomposed after the process without additional treatment and is inexpensive.
In the contribution, the developed laccase immobilization methodology and the optimization of the immobilization using the Response Surface Methodology (RMS) will be discussed. Furthermore, the capability to degrade dye-polluted water will be evaluated and a novel bioreactor for the water treatment will be suggested

The former uranium mine Königstein (Germany) is currently in the process of a controlled flooding for remediation purposes. However, the flooding water still contains high concentrations of uranium and other heavy metals. For that reason the water has to be cleaned up by a conventional waste water treatment. The aim of this study was to investigate the interactions between anaerobic microorganisms and uranium for possible bioremediation approaches due to the fact, that microorganisms could be used as an alternative for the intensive and expensive waste water treatment.
Flooding water from the former uranium mine was directly sampled and gas-flushed with N2. 10 mM glycerol was added as carbon source. The approaches were incubated for six weeks at 30 °C. Samples were taken three times a week for measuring of the redox potential. Every week samples were taken to investigate the redox state of uranium by XANES (X-ray absorption near edge structure) measurements. During the incubation time the redox potential decreased from 660 mV to 300 mV. By Iterative Target-Factor Analysis (ITFA) it was determined that 100 % of uranium(VI) was reduced to uranium(IV) within six weeks of incubation. In addition, investigations of the supernatant with UV-vis resulted in the same findings. The results show that naturally occurring anaerobic microorganisms within the flooding water of the former uranium mine Königstein are able to reduce the soluble uranium(VI) into the less soluble uranium(IV). In conclusion, anaerobic microorganisms within the flooding water could be used as an alternative for bioremediation approaches.

The active transport of ions across biological membranes requires their hydration shell to interact with the interior of membrane proteins. However, the influence of the external lipid phase on internal dielectric dynamics is hard to access by experiment. Using the octahelical transmembrane architecture of the copper-transporting P1B-type ATPase from Legionella pneumophila as a model structure, we have established the site-specific labeling of internal cysteines with a polarity-sensitive fluorophore. This enabled dipolar relaxation studies in a solubilized form of the protein and in its lipid-embedded state in nanodiscs. Time-dependent fluorescence shifts revealed the site-specific hydration and dipole mobility around the conserved ion-binding motif. The spatial distribution of both features is shaped significantly and independently of each other by membrane lateral pressure.

The lecture introduces and discusses principles of multiphase flow measurement. In detail it addresses fundamental issues of multiphase fluid dynamics, measureable parameters, hardware and software aspects of measurement techniques, as well as its relation to multiphase flow modelling and CFD code development.

In magnonics, spin waves are conceived of as electron-charge-free information carriers. Their wave behavior has established them as the key elements to achieve low power consumption, fast operative rates, and good packaging in magnon-based computational technologies. Hence, knowing alternative ways that reveal certain properties of their undulatory motion is an important task. Here, we show using micromagnetic simulations and analytical calculations that spin-wave propagation in ferromagnetic nanotubes is fundamentally different than in thin films. The dispersion relation is asymmetric regarding the sign of the wave vector. It is a purely curvature-induced effect and its fundamental origin is identified to be the classical dipole-dipole interaction. The analytical expression of the dispersion relation has the same mathematical form as in thin films with the Dzyalonshiinsky-Moriya interaction. Therefore, this curvatureinduced effect can be seen as a “dipole-induced Dzyalonshiinsky-Moriya-like” effect.

Since autumn 2011, the DREsden AMS-facility (DREAMS), is performing routine AMS at the 6MV tandem accelerator of the ion beam centre (IBC) at the Helmholtz-Zentrum Dresden-Rossendorf [1,2]. In routine operation are measurements of ¹⁰Be, ²⁶Al, ³⁶Cl, ⁴¹Ca, and ¹²⁹I for a wide range of applications. Most of the samples are prepared at our own chemistry labs – or in close cooperation with the users – to allow best performance for diverse tasks [3]. Our performance to measure these routine isotopes improved considerably over the last years [2]. This successful approach needs a careful selection of measurement parameters like a propper measurement order, a specific tuning using low-level (traceable) standards and individual setting of detector parameters for each beam time. One example for an additional improvement is the low-background value of ²⁶Al/²⁷Al = 6 × 10⁻¹⁶ reached in blanks from commercial carriers. For ⁴¹Ca measurements we get 30% more transmission, while having ten times less background from ⁴¹K. Further promising developments include the upgrade to nonroutine
AMS-nuclides like ⁴⁴Ti [4] and to actinides [5].
Ref.: [1] S. Akhmadaliev et al., NIMB 294 (2013) 5.
[2] G. Rugel et al., NIMB 370 (2016) 94.
[3] S. Merchel, this conference.
[4] A. Scharf, this conference.
[5] Nasrin B. Khojasteh, this conference.

Field ionization plays an important role in modeling the interaction of high-power, ultra-short lasers pulses with matter. Many field ionization models exist that have predictive capability at non-relativistic laser intensities and for laser pulse durations that much longer than the atomic time scales. Most existing models take a quasi-static approach to the laser field on atomic dimensions and time scales. Yet, with pulses as short as a few ~10 to ~100 as and intensities of 10 21 W/cm 2 the feasibility of these approximations becomes questionable. Still the exploration of plasma effects in relativistic laser matter interaction requires to test the boundaries of validity for these models. This thesis will take a step to point out the difficulties to be considered when existing ionization models are applied to such extreme cases.

It is vital to treat field ionization adequately and validate the different existing models critically in order to obtain trustworthy results from plasma simulations. This poster presents numerical methods for modelling field ionization in laser-plasma interactions. Based on results obtained in earlier Monte-Carlo simulations on CPU and later application to the fully-relativistic particle-in-cell code PIConGPU it is pointed out that different ionization models and the details of modelling field ionization can have a major influence on plasma dynamics.

In recent years magnonics has become one of the prime topics in magnetics research. The prospect of possible technological applications has played a major part in this development. The reliable generation of spin waves with short wavelengths is an ongoing challenge in this eld, as it is di cult by means of a patterned stripline antenna. Here we report on the imaging of spiral shaped short wavelength spin waves emitted by a magnetic vortex core in a permalloy disc. We take advantage of the magnetic perturbation generated by the small moving core, 10-20nm in diameter, to generate spin waves of sub-100nm wavelength. Imaging of these waves has been done using Time-Resolved Scanning Transmission X-Ray Microscopy at the MAXYMUS endstation of the BESSY II synchrotron facility. The experimentally derived dispersion relations match with analytical expressions for hybridized modes between Damon-Eshbach and exchange dominated magnons in in nite ferromagnetic lms. This holds as well for our micromagnetic simulations in these vortex structures.

Thermal processing in the ms range comprises modern, non-equilibrium annealing techniques which allow various material modifications at the surface without affecting the bulk. Flash lamp annealing (FLA) is one of the most diverse methods of short time annealing with applications ranging from the classical field of semiconductor doping to the treatment of polymers and flexible substrates. The presentation focuses on the FLA of transparent conducting oxides.

The lesson 6 of the "Short Course on Multiphase Flow Modelling" deals with the simulation of a rectangular bubble colum and of a spray. Modeling advices and datasets are given.

The magneto-elastic (ME) coupling has recently become of inter- est thanks to its numerous applications, e.g. in the fabrication of magneto-electric multiferroics. This effect has been recently studied quasi-statically on micro- and nanostructured magnetostrictive materials strained using piezoelectric substrates. However, due to limitations in the RF properties of piezoelectric materials, the influence of the ME coupling on the magneto-dynamical processes has not yet been investigated in depth. Here, thanks to a newly-developed approach that allows the in-situ straining of magnetostrictive materials whilst preserving good RF properties of the substrate, we present a first study of the influence of the ME coupling on the gyration dynamics of magnetic vortices in microstructured magnetostrictive elements using time-resolved x-ray magnetic microscopy. In particular, we observe that the application of a strain to the magnetostrictive material leads to a reduction of the gyration eigenfrequency, and to a modification of the orbit of the vortex core, both of which can be controlled by changing the magnitude of the applied strain.

A variety of measurement techniques already exist to characterize multiphase flows in large scale as well as in mini scale systems. But when looking at smaller dimensions than millimeters and higher flow velocities the amount of available techniques diminishes drastically. Another problem is the capability of existing solutions to be applicable for online measurements even in non-transparent systems. On this account the current work presents a measurement technique based on optical fibers which is comparable to other commonly applied techniques, but additionally works in a running chemical reaction process. The current work deals with the validation of the double fiber system and a detailed comparison to several widely accepted conventional and modern measurement techniques. These are high speed camera, gravimetric analysis and ultrafast X-ray tomography. The experimental work has been performed in a cold flow loop operating setup with a gas-liquid flow. The final aim has been to characterize the multiphase flow in a mini channel system of a monolith. The investigated monoliths have a cell density of 39 cpsi and 400 cpsi and are made of Cordierite, an opaque ceramic material. By using the developed optical fiber system and the mentioned reference techniques parameters like bubble velocity, flow regime, hold-up or phase distribution have been assessed to compare the common techniques with the newly developed fiber system. The presented fiber optic measurement technique allows reliable, reproducible measurements of local phase characteristics. The mounting space of maximum 250 μm realizes a high local resolution even at small scales. In comparison to other techniques high level of agreement has been proven.

In laser-generated plasmas the free electron density is a crucial parameter for plasma dynamics. Therefore, to model its spatial and temporal evolution the adequate treatment of ionization is vital. This poster presents the work in progress on numerical field ionization methods implemented in the world's fastest 3D3V electromagnetic particle-in-cell code PIConGPU. Thus, computing a value for the systematic error via repeating simulations with varying ionization schemes is in reach. With high performance computing we can give a range of validity for predictions of pump-probe experiments with high power lasers and X-ray free electron lasers.

Outline of data acquisition requirements of in-beam dosimetry using Positron Emission Tomography and presentation of the developed GPU code "raptr".

In laser-generated plasmas the free electron density is a crucial parameter for plasma dynamics. Therefore, to model its spatial and temporal evolution the adequate treatment of ionization is vital. This poster presents the work in progress on numerical field ionization methods implemented in the world's fastest 3D3V electromagnetic particle-in-cell code PIConGPU. Thus, computing a value for the systematic error via repeating simulations with varying ionization schemes is in reach. With high performance computing we can give a range of validity for predictions of pump-probe experiments with high power lasers and X-ray free electron lasers.

A generalized approach developed for the simulation of two-phase flow problems with multi-scale interfacial structures is applied for the simulation of a plunging jet. The GEneralized TwO Phase flow (GENTOP) modeling approach considers different scales in term of interfacial structure. The explicit statistical simulation of the interface between continuous gas and fluid is combined with the Euler/Euler simulation of dispersed gas. For the dispersed gas the Multiple Size Group (MUSIG) approach simulates different bubble sizes. The mass transfer between the bubble sizes is considered by bubble breakup and coalescence models. The gas entrainment during the plunging jet is described by the transition between continuous gas and dispersed gas. Therefor a special sub grid model is applied.
This set of models is applied for the simulation of plunging jet experiments performed by Chanson et al. (2004). In the tests different geometric scales of plunging jet were investigated and here analyzed. The paper shows the capabilities of this approach and identifies weak points which need further development.

The lecture gives an introduction to high-resolution gamma-ray computed tomography and its application for quantitative measurements and visualization of two-phase flow in industrial and scientific applications. Exemplarily, recent results from investigations on an industrial centrifugal pump under several gas entrainment conditions will be presented.

In the framework of the European project NURESAFE, the reactor dynamics code DYN3D, developed at HZDR, was coupled with the CFD solver Trio_U, developed at CEA France, in order to replace DYN3D’s one-dimensional hydraulic part with a full three-dimensional description of the coolant flow in the reactor core at higher spatial resolution. The present document gives an introduction into the coupling method and shows results of its application to the simulation of an MSLB accident of a PWR.

Advanced 3D computational tools are increasingly used to simulate complex phenomena occurring during scenario involving operational transients and accidents in nuclear power plants. Among these scenarios, one can mention the asymmetric coolant mixing under natural circulation flow regimes. This issue motivated some detailed experimental investigations carried out within the OECD/NEA PKL projects. The aim of these investigations was, besides the assessment of the mixing phenomenon in the reactor pressure vessel, to provide experimental data for computer code validations. In the current study, the ROCOM/PKL-3 T2.3 experimental test is assessed using on one hand thermal-hydraulic system codes with 3D capabilities, and on the other hand a CFD computational tool. The results emphasize the capabilities and the differences between the considered computational tools as well as their suitability for such purposes.

Analysis and control of industrial processes is inseparably interlinked with appropriate process measurement techniques. Among such distributed sensing, imaging and tomography are emerging technologies, which gain more and more attention, as they have the capability to measure field quantities. Research and application in the field of process tomography is continuously intense and recently many innovative concepts and ideas have been born and demonstrated. Exchange of knowledge within the process tomography community and transfer of knowledge to research and industry are supported by the International Society for Industrial Process Tomography on the basis of regular expert meetings. This special issue is a compilation of the 21 most important contributions from the 7th International Symposium on Industrial Process Tomography ISPT7, held in Dresden, Germany, Sept. 1-4, 2015. It covers a broad range of process tomography technologies but also a broad range of technology readiness levels from very fundamental aspects, such as raw data processing or new methods of analysis of tomographic images, new modalities, such as microwave tomography, up to important industrial applications, such as cyclone separators, bubble column reactors and waste water abatement.

Since 2009 the DREAMS (DREsden Accelerator Mass Spectrometry) facility offers users to do their own sample preparation for AMS targets. A large number of samples from interdisciplinary research Topics such as astronomy, climate, cosmochemistry and geology could be transformed into BeO, Al₂O₃, AgCl and CaF₂ showing reasonable to excellent performance [Rugel et al., this DPG.]. However, besides our constant approach to become a little better every day, sometimes very new challenges can arise due to the low availability of the sample material, low radionuclide concentration or a possible contamination of the sample with disturbing elements and nuclides. Two examples:

Ice samples are always in our focus. As we were facing Problems with ¹⁰Be contamination in "dirty" ground ice, we measured ³⁶Cl and ^natCl by isotope dilution in permafrost ice wedge samples as heavy as 1.6 kg. The chemical yield of AgCl was only 20-35% (and is a function of total ^natCl), which might be improved by preconcentration steps.
For the determination of in-situ or atmospheric ²⁶Al in marine and terrestrial sediments [e.g. Gärtner et al., this DPG.], we had sometimes unaccountable low chemical yields, which seems to be partially due to
redissolving aluminium hydroxide in the last washings.
Thanks to A. Gärtner, P. Ludwig, D. Rodrigues and several students for providing/processing samples.

Der Vortrag stellt das vom BMWi geförderte gleichnamige Vorhaben vor. In diesem werden nichtinvasive Prüf- und Überwachunsgmethoden zur Erkennung von Veränderungen des Inventars von Transport- und Lagerbehältern (Typ CASTOR) auf ihre Machbarkeit untersucht. Hintergund ist die in Deutschland absehbare verlängerte Zwischenlagerung abgebrannter Brennelemente in Trockenlägern an den heutigen Kernkraftwerksstandorten. Für Zwischenlagerungszeiträume von mehreren Jahrzehnten ist heue keine verlässliche Aussage über etwaige Zustandsveränderungen an den Brennelementen möglich. Daher kommt nichtinvasiven Monitoringverfahren für den Behälterinhalt ein große Bedeutung zu. Untersucht werden Verfahren auf Basis von Gamma-, Neutronen- und Myonenstrahlung, akustische und schwingungsspektroskopische Verfahren sowie Thermographieverfahren.

The invited lecture discussed and demonstrates the application of tomographic imaging in multiphase flow measurement. Thereby the discussion is guided along prototypical application examples in the fields of oil and gas production, chemical engineering and nuclear engineering. Emphasize is given to open quesions and future needs to improve applicability and significance of tomographic imaging techniques in fundmental and engineering research.

Das Phänomen der Tropfenkondensation, sowie der damit verbundene hohe Wärmeübertragungskoeffizient, haben ein großes Potential für die Optimierung industrieller Kondensationsprozesse. Ein wesentlicher Parameter der Kondensationsoberfläche bei der Tropfenkondensation ist der Kontaktwinkel eines Flüssigkeitstropfens auf einer Oberfläche. Insbesondere bei Arbeitsmedien mit geringen Oberflächenspannungen, sind niedrige Oberflächenenergien notwendig, um Tropfenkondensation zu realisieren. Selbst-aggregierende Monoschichten (SAM) auf der Basis von Phosphonsäure stellen eine Möglichkeit zur Herstellung von hydrophoben Oberflächen dar, welche auch bei Instandhaltung nachträglich aufgebracht oder erneuert werden können. Der Einfluss derartiger Beschichtungen auf das Verhalten von Kondensationssystemen wird untersucht.
Ein hoher Kontaktwinkel kennzeichnet die hydrophobe Eigenschaft einer Oberfläche, welche mit Hilfe von SAM durch ein auf Phosphonsäure basierendes nass¬chemisches Verfahren erzeugt wurde. Durch eine Kombination von künstlich eingestellter Rauigkeit und SAM-Beschichtung ist es möglich Kontaktwinkel in einem weiten Spektrum gezielt einzustellen. Dies eröffnet die Möglichkeit, individuell auf den Kondensationsprozess und Dampfgehalt angepasste Funktionsflächen zu fertigen.
Besonders hohe Kontaktwinkel wurden auf Proben mit hoher Rauigkeit und bei SAM mit langen Kohlenstoffketten gemessen. Aufgrund des nasschemischen Beschichtungsverfahrens können beliebige Geometrien, wie beispielsweise innen-berippte Rohre und Hohlstrukturen, behandelt werden. Dies ermöglicht die gezielte Beeinflussung der Wärmeübertragungseigenschaften und des Kondensat-Ablaufes in einer Struktur. In einem integralen Versuchsstand wird der Einsatz dieser neuartigen Wärmeübertragerflächen mit hoher Auflösung untersucht.

For remediation of uranium contaminated environments from activities such as uranium mining and uranium processing, microorganisms could be important due to their ability to immobilize radionuclides and heavy metals. To improve bioremediation strategies based on a better understanding of binding mechanisms on the molecular level, we applied uranium interaction experiments with Acidovorax facilis, an aerobic, Gram-negative Betaproteobacteria, which is commonly found in soils. Experiments were performed in batch cultures under aerobic conditions at 25 °C using nutrient broth. The cells were grown to an optical density (OD600) of around 1.5. For sorption experiments UO2(NO3)2 was added to the culture to achieve an initial uranium concentration of 0.05 and 0.1 M, respectively, at a neutral pH range. Energy-filtered transmission electron microscopy (EF-TEM) coupled with electron energy-loss spectroscopy (EELS) and time-resolved laser fluorescence spectroscopy (TRLFS) were applied. The results provide spectroscopically and microscopically evidence of uranium sorbed at the outer membrane of Acidovorax f. cells by showing high electron density and uranium ionization intensity peaks. In addition, uranium was detected in the small polyphosphate granules of the cells, indicating the formation of a uranyl-phosphate complex as a result of an intracellular bioaccumulation process. The results support the TRLFS measurements, concluding that uranium is bound on carboxylic functionality groups, e.g., peptidoglycan (R−COO−UO2) and either on phosphoryl groups, e.g., uranyl-lipopolysaccharide-complexes R-O-PO3-UO2 and [R-O-PO3]2-UO22- of the outer membrane [1].
[1] Barkleit, A. et al. (2008). Dalton Transaction 2879-2886.

III-nitride heterostructures in the form of multilayered quantum wells (MQWs) or quantum dots (QDs) and interacting Ge QDs (“quantum molecules”) are promising candidates for high-speed intersubband (ISB) optical devices relying on the quantum confinement of electrons. Microstructural parameters (interatomic distances, coordination numbers, and Debye–Waller factors) were determined by means of EXAFS spectroscopy based on the Synchrotron Radiation, and the relationship between the variations in these parameters and the morphology of superlattices and symmetric assembles of QDs were established. The EXAFS technique has been used to study the local structure of thin hexagonal GaN/AlN MQWs grown by ammonia MBE at different temperatures. It is shown that the heterointerface intermixing leads to a decrease in the Ga-Al interatomic distance and the Ga–Ga coordination number in MQWs. The degree of intermixing in the boundary layers rises from 30% to 40% with increase of the growth temperature from 795 to 895◦ C. It was found that in the first phase of quantum molecules growth Ge atoms concentration is 25%. With further growth (deposition of the base layers) Ge concentration increases up to 35–45%, depending on the temperature (from 610 to 550◦C) of deposition

Selenium is an important element for technology and dietary supplements but it is toxic at slightly higher concentration. Thus, its removal from the wastewaters is important. Microbial reduction of selenium oxyanions in thermophilic bioreactor (55 oC) removed higher selenium when compared to the control mesophilic bioreactor (30 oC). This study demonstrated that the better performance of the thermophilic bioreactor was due to the better settling properties of biogenic elemental selenium nanorods (BioSe-Nanorods) produced in thermophilic conditions compared to biogenic elemental selenium nanospheres (BioSe-Nanospheres) produced in mesophilic conditions. The BioSe-Nanorods were less colloidally stable than the extracellular polymeric substances (EPS) capped BioSe-Nanospheres as demonstrated by the former's lesser negative zeta potential values when exposed to elevated concentrations of NaCl and CaCl2 as well as better settling in different lake waters. The lower colloidal stability was due to a lesser negative surface charge density of BioSe-Nanorods compared to BioSe-Nanospheres. This study also argued that the EPS were the corona of BioSe-Nanorods as well. Further, this study observed that the formation of BioSe-Nanorods proceeds via BioSe-Nanospheres. This study demonstrates the importance of the shape of nanoparticles in determining their bioremediation effectiveness and the fate in the environment.

Under irradiation NiSiPCr clusters are formed in high-Cr ferritic martensitic steels as well as in FeCr model alloys. In the literature little is known about the origin and contribution to the hardening of these clusters. In this work we performed density functional theory (DFT) calculations to study the stability of small substitutional NiCr-vacancy clusters and interstitial configurations in bcc Fe. Based on DFT data and experimental considerations a ternary potential for the ferritic FeNiCr system was developed. The potential was applied to study the thermodynamic stability of NiCr clusters by means of Metropolis Monte Carlo (MMC) simulations. The results of our simulations show that Cr and Ni precipitate as separate fractions and suggest only a limited synergetic effect between Ni and Cr. Therefore our results suggest that the NiCrSiP clusters observed in experiments must be the result of other mechanisms than the synergy of Cr and Ni at thermal equilibrium.

Using intense, spectrally narrow terahertz pulses from the free-electron laser facility FELBE in Dresden, Germany, we have investigated exciton population dynamics in III-V QWs and single quantum dots. To this end, carriers are optically injected by picosecond near-infrared pulses to populate the lowest excitonic level. Using narrowband terahertz pulses, excitons are resonantly excited into higher levels. Time-dependent photoluminescence measurements based on a streak camera system and on time-correlated photon counting, respectively, then allow us to study the transient population of dipole-allowed higher exciton levels and to access the relaxation dynamics.

This talk reviews recent spectroscopic studies on semiconductor nanostructures using the THz free-electron laser FELBE. Its intense, quasi-continuous, nearly transform-limited ps pulses provide unique research opportunities to advance THz science.

Liquid metal batteries (LMBs) are discussed today as a cheap grid scale energy storage, as required for the deployment of fluctuating renewable energies. LMBs incorporate stratified three-layer fluid systems consisting of two liquid metal electrodes separated by a thin molten salt electrolyte. Due to the high electrical conductivities of the liquid metals, LMBs are highly susceptible for becoming unstable by MHD interactions of magnetic fields induced by internal and external currents. Besides the Tayler instability and the electrovortex instability, the so-called sloshing instability, also known as the metal pad roll instability in aluminum reduction cells, was identified as a key instability mechanism capable to cause short-circuits. Dimensionless stability parameters derived from inviscid two-layer systems can predict the onsets for sloshing and short-circuits with some success for a limited parameter range, but the two-layer description is far from perfect. To quantify the two-layer limitations, a three-layer dispersion relation was derived and deviations from the two-layer system were discussed. On this basis it is planned to extract three-layer stability criteria additionally including viscous damping to predict instability onsets in direct dependence of the geometrical parameters and material properties of LMBs. Further to this, three-layer experiments are under development aiming to measure the interaction and stability of interfacial waves using Doppler Ultrasound Velocimetry (DOP) and Magnetic Field Tomography (MFT) for checking the validity of different stability criteria.

We have investigated the electronic structure of Sr2IrO4 using core level resonant inelastic x-ray scattering. The experimental spectra can be well reproduced using ab initio density functional theory based multiplet ligand field theory calculations, thereby validating these calculations. We found that the low-energy, effective Ir t2g orbitals are practically degenerate in energy. We uncovered that covalency in Sr2IrO4, and generally in iridates, is very large with substantial oxygen ligand hole character in the Ir t2g Wannier orbitals. This has far reaching consequences, not only are onsite crystal-field energies determined by the long range crystal-structure, more significantly, magnetic exchange interactions will have long range distance dependent anisotropies in the spin direction. These findings set constraints and show pathways for the design of d5 materials that can host compass like magnetic interactions.

Substantial experimental and theoretical efforts worldwide are devoted to explore the phase diagram of strongly interacting matter. At LHC and top RHIC energies, QCD matter is studied at very high temperatures and nearly vanishing net-baryon densities. There is evidence that a Quark-Gluon-Plasma (QGP) was created at experiments at RHIC and LHC. The transition from the QGP back to the hadron gas is found to be a smooth cross over. For larger net-baryon densities and lower temperatures, it is expected that the QCD phase diagram exhibits a rich structure, such as a first-order phase transition between hadronic and partonic matter which terminates in a critical point, or exotic phases like quarkyonic matter. The discovery of these landmarks would be a breakthrough in our understanding of the strong interaction and is therefore in the focus of various high-energy heavy-ion research programs. The Compressed Baryonic Matter (CBM) experiment at FAIR will play a unique role in the exploration of the QCD phase diagram in the region of high net-baryon densities, because it is designed to run at unprecedented interaction rates. High-rate operation is the key prerequisite for high-precision measurements of multi-differential observables and of rare diagnostic probes which are sensitive to the dense phase of the nuclear fireball. The goal of the CBM experiment at SIS100 (sqrt(s_NN) = 2.7 - 4.9 GeV) is to discover fundamental properties of QCD matter: the phase structure at large baryon-chemical potentials (mu_B > 500 MeV), effects of chiral symmetry, and the equation-of-state at high density as it is expected to occur in the core of neutron stars. In this article, we review the motivation for and the physics programme of CBM, including activities before the start of data taking in 2022, in the context of the worldwide efforts to explore high-density QCD matter.

Mit Beschluss des Bundestages vom 30. Juni 2011 wird Deutschland bis 2022 seine Kernkraftwerke schrittweise stilllegen. Mit der Energiewende soll bis 2050 ein Großteil der benötigten Energie aus regenerativen Trägern bereitgestellt werden. Bis dahin ist es ein langer und schwieriger Weg, auf welchem noch zahlreiche technologische Probleme gelöst werden müssen.
Im Gegensatz zur Bundesrepublik setzen viele Länder (z. B.: China) weiterhin auf die Kernenergie. Ein Grund dafür: neuartige Reaktorkonzepte (Gen IV) machen diese sicherer und effizienter, vor allem stellen sie Lösungen zur Beseitigung des nuklearen Abfalls vor.
Dieser Vortrag beschäftigt sich mit ausgewählten Aspekten der Energiewende, erläutert die physikalischen Prozesse die zur Erzeugung oder Vernichtung des hochradioaktiven Kernabfalls führen und gibt einen Überblick über zukünftige Reaktortechnologien und Transmutationsanlagen.

In this talk I will present recent experimental investigations on carrier dynamics in graphene studied via pump-probe 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.

We explore the transient response of single self-assembled InAs/GaAs quantum dots (QD) to narrow-band terahertz (THz) pulses produced by the free-electron laser FELBE at HZDR. The THz excitation is tuned to the electron inter-sublevel s-to-p transition. For the QDs under study, this transition occurs in the range 13-20 meV because of in-situ intermixing. The THz pulse is applied at a time delay of about 0.7 ns after interband excitation. The dynamics of electron excitation and relaxation between QD sublevels is revealed by time-resolved micro-photoluminescence (PL) measurements performed on individual QDs.

A single-color pump-probe system has been commissioned at the Novosibirsk free electron laser facility. Monochromatic laser radiation with a bandwidth of about 1% can be tuned within the spectral ranges of 90 - 240 and 30 - 90 μm. The laser emits radiation as a continuous stream of 100-ps pulses with a repetition rate of 5.6 MHz. The average radiation power can reach 100 W. The temperature of samples located in a helium cryostat can be varied from 2 up to 325 K. The results of pump-probe measurements of non-equilibrium dynamics of hot electrons in a germanium crystal will be presented.

A single-color pump-probe system has been commissioned at the Novosibirsk free electron laser. The laser emits a tunable monochromatic terahertz radiation. To prove the proper system operation, we investigated the time-resolved absorption of a sample of n-type germanium doped with antimony, which was previously investigated at the FELBE facility, in the temperature range from 5 to 50 K. The measured relaxation time amounted to about 1.7 ns, which agreed with the results obtained at FELBE. The results of pump-probe measurements of non-equilibrium dynamics of hot electrons in a germanium crystal at cryogenic temperatures are presented for wavelengths of 105, 146 and 150 μm.

Proton beams provide superior dose-conformity in radiation therapy. However, the large sizes and costs limit the widespread use of proton therapy (PT). The recent progress in proton acceleration via high-power laser systems has made it a compelling alternative to conventional accelerators, as it could potentially reduce the overall size and cost of the PT facilities. However, the laser-accelerated beams exhibit different characteristics than conventionally accelerated beams, i.e. very intense proton bunches with large divergences and broad-energy spectra. For the application of laser-driven beams in PT, new solutions for beam transport, such as beam capture, integrated energy selection, beam shaping and delivery system are required due to due to the specific beam parameters. The generation of these beams are limited by the low repetition rate of high-power lasers and this limitation would require alternative solutions for tumour irradiation which can efficiently utilize the available high proton fluence and broad-energy spectra per proton bunch to keep treatment times short. This demands new dose delivery system and irradiation field formation schemes. In this paper, we present a multi-functional light-weight and compact proton gantry design based on ironless pulsed high-field magnets for laser-driven sources. This achromatic design includes an improved beam capturing and energy selection system, with a novel beam shaping and dose delivery system, so-called ELPIS. ELPIS system utilizes magnetic fields, instead of physical scatterers, for broadening the spot-size of broadenergetic beams while capable of simultaneously scanning them in lateral directions. To investigate the clinical feasibility of this gantry design, we conducted a treatment planning study with a 3D treatment planning system augmented for the pulsed beams with optimizable broad-energetic widths and selectable beam spot sizes. High quality treatment plans could be achieved with such unconventional beam parameters, deliverable via the presented gantry and ELPIS dose delivery system. The conventional PT gantries are huge and require large space for the gantry to rotate the beam around the patient, which could be reduced up to 4 times with the presented pulse powered gantry system. With the development of next generation high-power laser systems, with petawatt laser power, necessary to reach proton energies required for therapy application, it could be possible to reduce the footprint of the PT facilities, without compromising on clinical standards.

The present investigation aims to study the optical response of anisotropic Ag nanoparticle arrays deposited on rippled silicon substrates by performing a qualitative comparison between experimental and theoretical results. Spectroscopic ellipsometry was used along with numerical calculations using finite-difference time-domain (FDTD) method and rigorous coupled wave analysis (RCWA) to reveal trends in the optical and geometrical properties of the nanoparticle array. Ellipsometric data show two resonances, in the orthogonal x and y directions, that originate from localized plasmon resonances as demonstrated by the calculated near-fields from FDTD calculations. The far-field calculations by RCWA point to decoupled resonances in x direction and possible coupling effects in y direction, corresponding to the short and long axis of the anisotropic nanoparticles, respectively.

Safety assessment studies of future nuclear waste repositories carried out in many countries predict selenium-79 to be a critical radionuclide due to its presence in the anionic form resulting in weak retardation by most common rock minerals. This assumption, however, ignores its potential uptake by AFm phases, positively charged anion exchangers which are present in significant quantities in the cementitious materials used in artificial barriers. Here we report for the first time wet chemistry and spectroscopic data on the interaction of the most reduced selenium anion species, i.e. HSe-, with two AFm phases commonly found in cement, monocarbonate (AFm-CO3) and hemicarbonate (AFm-OHCO3). Batch sorption experiments show that Se(-II) is retained much more strongly (Rd = 100±50 L kg-1) by the hemicarbonate than by the monocarbonate (Rd = 4±2 L kg-1). The cause of this different sorption behavior was elucidated by extended X-ray absorption fine-structure (EXAFS) spectroscopy, showing that Se(-II) is mainly intercalated in the larger and hence more accessible interlayer of the hemicarbonate (d-spacing = 0.82 nm), whereas most Se(-II) is sorbed by the anion exchange sites on the outer surfaces of the AFm platelets in the case of monocarbonate, where the interlayer space is less accessible due to the smaller d-spacing of 0.75 nm. EXAFS spectra of oxidation experiments further show that Se(-II) in the interlayers is better protected from oxidation than Se(-II) sorbed to the outer surfaces. The quantitative sorption data along with the molecular-scale processes obtained from this study provide crucial insight into the Se mobility in the cementitious near-field of a radioactive waste repository under reducing conditions.

Aim: Amino acid transporters (AATs) are proteins that supply cells with amino acids (AAs). Cancer cells, compared to normal ones, often present a rapid growth and a high proliferation rate, supported by increased expression and/or activity of AATs. Radiolabeled AAs that intensively accumulate in tumour cells can provide high contrast SPECT or PET imaging of primary lesions and distant metastases. One of the most upregulated AAT in cancers is the LAT1 system which transports large neutral AAs as branched and aromatic ones. Therefore, a lot of radiolabelled tyrosine analogues have been developed (i.e. O-2-[18F]fluoroethyl-L-tyrosine, [18F]DOPA, [123I]ITIC(OH)). While radioiodinated derivatives of some of these electron-rich arenes are easily available, fluoroaryl analogues are particularly complicated to access by classical nucleophilic substitution with [18F]F-. Based on the ITIC(OH) scaffold, we developed a new synthetic pathway to easily produce radioiodinated or radiofluorinated tyrosine analogues.
Material and methods: A convergent synthetic pathway (Fig. 1) was designed to produce the radioiodinated tracers, reference fluorinated derivatives, and radiofluorinated compounds from common organotin intermediates. The latter were synthesized from iodinated analogues and labelled with [125I]iodide using electrophilic demetallation reaction or converted into iodonium salts for 18F-labelling. The reference fluorinated derivatives were obtained by treatment of the organotin compounds by F-TEDA-PF6. The enantiomeric excess of all produced compounds was assessed by chiral analytic HPLC analyses. For comparison, the corresponding derivatives from the series D were also synthesized.
Results: Our synthetic approach allowed the successful production of non-radioactive iodinated or fluorinated derivatives with high ee (>99%) and with a controlled position of halogenation. While, corresponding radioiodinated structures were easily synthesized using classical electrophilic substitution from organotin intermediates, the access to iodonium salt precursors and radiofluorinated derivatives warranted a lot of investigations to achieve acceptable (radio)chemical yields. Chiral analytical HPLC analyses revealed that no racemisation occurred during radiolabelling with [125I]iodide or [18F]fluoride.
Conclusion: We developed an efficient method to access to radioiodinated or radiofluorinated cyclic tyrosine analogues via organotin and iodonium salt intermediates. This strategy could be extended to a broad range of electron-rich aromatic derivatives.

Fig. 1. Convergent synthetic approach to access to radioiodinated and radiofluorinated cyclic tyrosine analogues via organotin intermediates

Amorphous indium zinc oxide (IZO) thin films are accessible by solution-deposition of mixtures of molecular single-source precursors with dimethyl 2-hydroxyimino- and 2-nitromalonato ligands (dmm-NOH and Hdmm-NO2, respectively). Thermal combustion of the precursor molecules In3O3(dmm-NO2)3.(toluene) and [Zn4O(dmm-NO)6] leads to a highly exothermic decomposition reaction yielding amorphous indium zinc oxide (IZO) even at a temperature of 150 °C. The main aim of the present investigation is to correlate the electronic performance in such solution processed field-effect transistors (FET) with the presence of surface groups and bulk defects depending on the processing temperatures of the resulting IZO films (250 to 400 °C). In depth electronic characterization using X-Ray- and Photoelectron Emission Spectroscopy (XPS and UPS) reveals major electronic changes during thin film formation in the temperature range between 275 and 300 °C. These findings are confirmed by Positron Annihilation Spectroscopy (PAS) which allows the monitoring of defects in a picometer range in the resulting functional IZO thin films. Resulting transistor mobilities (m) of the semiconducting IZO films are in the range of those of amorphous silicon even at a processing temperature of 250 °C and increase up to 6 and 9.5 cm2 (V s)-1 at 350 and 400 °C with on/off ratios of 105 up to 107, respectively.

A novel hybrid material Bi(III)@MIL-101 (Bi(III) = Bi-containing oxoclusters, MIL-101 = chromium(III) oxoterephthalate) has been obtained by the intra-pore hydrolysis of guest bismuth(III) chloride in ammonia solution. The compound was fully characterized by chemical analysis, PXRD, nitrogen sorption and TEM techniques. According to characterization techniques all Bi species are only inside matrix and elemental analysis reveals ca. 1 Bi atom per mesocage. The chemical structure of Bi(III)-containing clusters inside MIL-101 matrix has been suggested according to EXAFS study. The catalytic activity of Bi(III)@MIL-101 has been tested in photodegradation of methyl red (MR). An introduction of Bi(III)-species inside MIL-101 has significantly increased the photocatalytic performance in comparison with layered BiOCl which has been obtained in the same synthetic conditions without MIL-101.

Pyrite (FeS2) is a typical container of Pt in ores of magmatic and hydrothermal origin and in some carbonrich ores of sedimentary-diagenetic origin. Knowledge of the state of Pt disseminated in the matrix of pyrite, including local atomic environment (type of atoms in the nearest and distant coordination shells, coordination numbers, interatomic distances) and oxidation state, is necessary for physical-chemical modeling of platinum group element mineralization and for the improvement of Pt ore extraction and processing technologies. Here we report results of an investigation of local atomic structure of synthetic Pt-bearing pyrites by means of X-ray absorption spectroscopy (XAS). Synthesis experiments, performed at 580° and 590°C in a Pt-saturated system by means of salt-flux method, yielded crystals of pyrite with concentrations of Pt up to 4 wt %. Scanning electron microscopy (SEM) and electron probe microanalysis (EPMA) showed that the distribution of Pt within the pyrite grains is of zonal character, but within the distinct zones Pt is distributed homogeneously. Negative correlation between the concentrations of Pt and Fe was observed in the synthesized pyrite grains. The slope of the correlation line corresponds to the formation of the solid solution in the Pt-Fe-S system and/or to the formation of PtS2. The XAS experiments revealed the existence of two forms of Pt in pyrite. The main form is the solid solution Pt(IV), which isomorphically substitutes for Fe. The Pt-S distance in pyrite is ~0.1 Å longer than that of Fe-S in pure pyrite. The distortion of the pyrite crystal structure disappears at R >2.5 Å. The second Ptrich form was identified by means of high-resolution transmission electron microscopy (HRTEM) as nanosized inclusions of PtS2. Heating experiments with in situ registration of X-ray absorption spectra resulted in partial decomposition (dissolution) of PtS2 nanosized inclusions with the formation of the solid solution (Fe1–xPtx)S2. Therefore, the PtS2 nanosized particles can be considered as a quench product. Our data demonstrate that both Pt solid solution and PtS2 nanosized inclusions (at high Pt content) can exist in natural Pt-bearing pyrites.

We report on the significant role of the synthetic route and importance of solvent for synthesis of organic-inorganic lead iodide materials. Through one route, intercalation of dimethylformamide in the crystal structure was observed leading to one dimensional (1D) [NH3(CH2)4NH3]Pb2I6 structure of the product. This product was compared with the two dimensional (2D) [NH3(CH2)4NH3]PbI4 recovered from aqueous solvent based synthesis with the same precursors. UV-visible absorption spectroscopy showed a red-shift of 0.1 eV for the band gap of the 1D network in relation to the 2D system. This shift primarily originates from a shift in the valence band edge as determined from photoelectron- and X-ray spectroscopy results. These findings also suggest iodide 5p orbital as the principle component in the density of states in the valence band edge. Single crystal data shows change in the local coordination around iodide, while in both materials, lead atoms are surrounded by iodide atoms in octahedral units. The conductivity of the one dimensional material ([NH3(CH2)4NH3]Pb2I6) was 50% of the two dimensional material ([NH3(CH2)4NH3]PbI4). The fabricated solar cells reflect these changes in the chemical and electronic structure of both materials, although the total light conversion efficiency of solar cells based on both products were similar.

The Ribbon Growth on Substrate (RGS) technology is a promising technology that allows the controlled, high crystallization rate production of silicon wafers and advanced metal-silicide alloys. In order to optimize this process, insights from modelling the
liquid metal flow are very desirable. The RGS process is dominated by a time-dependent, three-dimensional free-surface flow of the processed melt under the influence of electromagnetic forces. Thereby, main flow structures and possible instabilities strongly depend
on the melt shape. We have developed a new numerical multiphysics-software within the OpenFOAM (extensions) framework, which allows us to efficiently simulate hydrodynamic and electrodynamic effects and their interaction.

The bubble shape is fundamental for every aspect of modelling bubbly flows. The interface is usually highly deformable so that the bubble shape is in general dependent on the surrounding flow field. Since recent work on this topic addressed almost entirely single-bubbles rising in quiescent flow, the extent of such flow field dependencies is rather unknown. This study examines the effect on the bubble shape when flow properties, i.e. the gas flow rate, sparger setup, and column geometry, are changed by evaluating six different bubble column experiments. The results of this integral approach reveal that the bubble shape of small bubbles is distinctly influenced whereas the shape of large bubbles is unchanged. Averaged over all flow rates, we find that the size-dependent bubble shapes are quite similar for all six experiments.
Further studies focusing on single local effects like the shear rate or wake effects are highly desirable to obtain a deeper understanding of the underlying processes; for this purpose, the given results can help to assess the most important effect and in which extend it should be studied.

It is more and more possible to design bubbly flow reactors with methods of the computational fluid dynamics (CFD). Measurements that can be used for model validation, however, are often missing, especially for complex setups like airlift reactors. Such measurements include locally resolved information about the dispersed and continuous phase, particularly the information about the flow field and interface structures are important. In the present work Reynolds stresses, liquid velocity and gas void fraction profiles as well as bubble size distributions are provided at several positions in the riser and the downcomer in a rectangular airlift reactor for this purpose. In addition, the hydrodynamics inside this airlift reactor are described in detail by the measured values.

We present Raman, terahertz transmission, and transport measurements on (BiIn)2Se3 films to study the evolution of phonon modes and resistivity with an increasing indium content across the metal-insulator phase transition. The frequencies of two Raman-active modes E2g and A21g as well as an infrared-active mode Eu increase with an increasing indium content due to the smaller atomic weight of indium compared to bismuth. Terahertz data are fitted by a Drude Lorentz model. Drude scattering rates increase from 47 to 75 cm -1 with an increasing indium content from 0% to 16% due to stronger impurity scattering. The carrier concentration drops significantly for x=24%. The temperature dependence of the resistivity switches from metallic at x=16% to insulating at x =24%, indicating a metal-insulator transition in between.

The lateral lift force has an important influence on the gas distribution in bubbly flows. For this reason reliable closure models reflecting this force are required for CFD-simulations of bubbly flows. In Direct Numerical Simulations as well in experimental investigation it was shown that the lift force strongly depends on the bubble size and even changes its sign depending on the bubble size. Tomiyama et al. (2002) obtained a correlation from experiments with single bubbles in a linear laminar shear flow for high Morton number systems, which is frequently used in CFD-simulations. In this work the lift force is determined experimentally in low Morton number systems with a turbulent background flow. Single bubbles move through a linear shear field generated in a flat column by asymmetric aerating. An averaged bubble trajectory is obtained from a long-term averaged gas volume fraction field along which the force balance including buoyancy, drag, virtual mass and lift is solved to determine the lift force coefficient. The additional parameters required, as relative velocity are obtained from the experiments. The dependency of the lift force coefficient on the horizontal bubble diameter is in good agreement with the data obtained by Tomiyama et al., however the Wellek correlation for the aspect ratio seems to be not valid for the pure system considered.

An understanding of the fluid dynamics and the transport phenomena in bubble columns (in the homogeneous and heterogeneous flow regimes) is of fundamental importance to support the design and scale-up methods. In this respect, multiphase Computational Fluid-Dynamics (CFD) simulations in the Eulerian multi-fluid framework are particularly useful to study the fluid dynamics in large-scale reactors; in particular, this study concerns the modeling of the fluid dynamics in bubble columns within the boundaries of the homogeneous flow regime. Reliable predictions of the homogeneous flow regime with this approach are, however, limited up to now. One important drawback is that usually the needed closure models for the interphase forces, turbulence and coalescence and break-up are selected case-by-case, which hinder improvement of the predictive value. A set of closure relations has been collected at the Helmholtz-Zentrum Dresden-Rossendorf that represents the best available knowledge and may serve as a baseline model for further investigations. In this paper, the validation of this set of closure relations has been extended to the pseudo-homogeneous flow regime—characterized by a wide spectrum of bubble sizes and typically associated with the large sparger openings used in industrial applications—in large-scale bubble columns, thus establishing a first step towards the simulation of industrial-scale reactors. To this end, the benchmark considered is a comprehensive dataset obtained for a large-scale bubble column, which has been built accordingly with the well-known scale up criteria (large-diameter, high aspect ratio and large sparger openings). The numerical approach has been tested in its fixed-poly-dispersed formulation (considering the two- and four-classes approaches to represent the dispersed phase) and considering the coalescence and break-up closures. The results suggest that the correct simulation of the fluid dynamics in the bubble column requires the definition of coalescence and break-up closures. The results have been critically analyzed and the reasons for the discrepancies between the numerical results and the experimental data have been identified and may serve as basis for future studies.

Four coordination polymers bearing uranium or neptunium have been hydrothermally synthesized at 130°C, from a tetravalent actinide chloride (AnCl4) source in association with phthalic (noted 1,2-H2bdc hereafter) or mellitic (noted H6mel hereafter) acid in aqueous mediua. With the phthalate ligand, two analogous assemblies ([An2O2(H2O)2(1,2-bdc)2]·H2O ; An = U4+ (1) or Np4+ (2)) have been isolated and are built up from the connection of square anti-prismatic polyhedra (AnO8) linked to each other via μ3-oxo groups (edge-sharing mode) in order to construct infinite zig-zag ribbons. The phthalate molecules connect adjacent chains to each other to generate a 2D network. Water molecules are bonded to the actinide center or found intercalated between the layers. With the mellitate ligand, two distinct structures have been identified. The uranium-based compound (U2(OH)2(H2O)2(mel) (3)) exhibits a 3D structure composed of dinuclear units of UO8 polyhedra (square anti-prism) linked via common edge (μ2-hydroxo). The 3D framework consists of the connection of the mellitate linker with the dinuclear brick with its six carboxylate arms. The structure of the neptunium mellitate ([(NpO2)10(H2O)14(Hmel)2]·12H2O (4)) reveals the oxidation of the initial Np(IV) toward Np(V) in our synthetic hydrothermal conditions, and this generates typical neptunyl entities with pentagonal bipyramidal environment (NpO7 unit). The resulting network is a layered assembly, composed of sheets of NpO7 linked in a square net, with cation-cation interactions between neptunyl bond (Np=O) and Np-O bonds from the pentagonal plane. The cohesion of the 3D structure is ensured by the mellitate molecules acting as bridging linkers between the NpO7 sub-network. For the mellitate, only four carboxylate groups are engaged with the connection of the NpO7-based layer.

Abstract
18F-FDG PET imaging is routinely used to assess recruitment of BAT thermogenesis which requires mitochondrial uncoupling protein 1 (UCP1). It remains unsettled whether 18F-FDG uptake by BAT is altered in the absence of UCP1-mediated heat production.
METHODS: UCP1 knockout (UCP1 KO) and wild-type (WT) mice received single intraperitoneal injections of the selective β3 adrenergic receptor agonist CL 316, 243 (1mg/kg) and underwent metabolic cage, infrared thermal imaging and static 18F-FDG PET/MRI experiments. Bioenergetics of isolated brown adipocytes were examined by extracellular flux analysis.
RESULTS: In response to CL 316, 243 treatment, oxygen consumption and BAT thermogenesis were diminished in UCP1 KO mice; however the stimulation of 18F-FDG uptake by BAT was fully retained. Brown adipocytes derived from UCP1 KO mice exhibited defective induction of uncoupled respiration when glycolytic flux appeared normal.
CONCLUSION: Increased glucose metabolism in BAT can occur independently of UCP1-mediated thermogenesis.

Sorption of trivalent actinides and lanthanides onto the surface of geological materials relevant for nuclear waste disposal is a topic that has been widely studied in recent years. However, the sorption properties of metals are often investigated by studying the sorption behaviour of a single metal at a time, thus, these experiments do not account for potential effects of sorption competition in the presence of multiple dissolved elements or compounds. Bradbury and Baeyens (2005) performed extensive investigations of the sorption competition between various metal cations on the clay mineral montmorillonite. By investigating the competition of metals with similar and dissimilar chemical behaviour (e.g. tendency to hydrolysis and valence state), the authors concluded that metal cations with dissimilar chemical properties do not affect the uptake of one another by the clay mineral, whereas metals with similar chemistries do. Thus, if the data obtained in single metal sorption experiments are used in the safety assessment of nuclear disposal, careful considerations of the chemical environment in the near- or far-field of nuclear waste repository is needed to avoid the possible overestimation of radionuclide sorption.
In this study, we have combined batch sorption and spectroscopic experiments that were performed with Eu(III), Cm(III) and Am(III) in in the absence and presence of Y(III) as competing cation. The objective was to investigate how the sorption behaviour of trivalent actinides and lanthanides is affected by the presence of another trivalent metal. Following the findings of Bradbury and Baeyens (2005) our hypothesis is that the addition of higher concentrations of trivalent Y(III) together with a chemically similar trivalent metal, Eu(III), Cm(III) or Am(III), would affect the sorption behaviour of that metal.
Batch sorption experiments were performed with Eu(III) at different pH (pH-edges) and concentrations (isotherms). The competing metal Y(III) was added before Eu(III) to the mineral suspension in concentrations ranging from 1×10-6 M to 1×10-4 M. In the Eu(III) pH-edge experiments, the sorption of 1×10-5 M Eu(III) was investigated on 0.5 g/l corundum at varying pH, with and without Y(III). In the Eu(III) isotherm experiments, the initial Eu(III) concentration was varied between 1×10-9 M – 1×10-4 M and Y(III) was used in the competing isotherm samples at a constant pH of 7. Batch experiments showed that the addition of Y(III) did decrease the sorption of Eu(III) (Figure 1) on a macroscopic scale. However, as the main emphasis of this study was the possible changes happening at the molecular level as a results of sorption competition, spectroscopic methods were also employed. Time-resolved laser fluorescence spectroscopy (TRLFS) enables the investigations of Cm(III) sorption speciation directly on the mineral surface. We investigated the changes in the speciation of 1×10-7 M Cm(III) in 0.5 g/l corundum suspensions at varying pH under non-competing and competing conditions using 1×10-4 M Y(III). The results indicate changes in the Cm(III) sorption species distribution, thus, confirming our findings in the batch sorption experiments showing that 1×10-4 M Y(III) suppresses Cm sorption complex formation on the mineral surface depending on the solution pH (Figure 2). Cm(III) luminescence spectra of only Cm(III) and of Cm(III) together with Y(III), show that the fraction of aqueous Cm species is substantially greater with high concentrations of Y(III) present. Only when the pH is increased above 7, the first Cm sorption species appears, resulting in a shift of the observed emission peak maximum. X-ray absorption spectroscopy (XAS) was applied to identify the formed trivalent actinide sorption complexes. We investigated the sorption of 6×10-6 M or 2×10-5 M Am(III) on the corundum surface at pH 8.5 in the absence and presence of 2×10-5 or 2×10-4 M Y(III). The treatment of the XAS-data is still ongoing and results will be discussed more closely in the conference presentation.

If radionuclides are released in the environment their mobility and behavior is influenced by interactions with abiotic and biotic matter. As fungi are ubiquitous in nature they have to be taken into consideration in particular. For example, fungi can bind radionuclides in different ways, with the result that the radionuclides are immobilized and preventing further migration through the soil. The aim of this study was to investigate the binding of uranium and europium, the latter as surrogate for trivalent actinides, by fungi Schizophyllum commune and Leucoagaricus naucinus.
First batch experiments showed the binding of U(VI) and Eu(III) by fungi depends on the initial conditions. Both fungi showed increasing sorption capacities with higher initial metal concentrations and lower initial biomass. In contrast, the fungi showed different metal binding behavior in dependence on pH. Scanning transmission electron microscopy in combination with high angle annular dark-field analysis (HAADF-STEM) revealed location of U(VI) on the surface and inside of cells of Schizophyllum commune.
Furthermore the U(VI)-binding of the fungi was investigate with time-resolved laser-induced fluorescence spectroscopy (TRLFS) depending on metal concentration. The results showed the speciation of U(VI) is changed in the initial solution during binding process. In addition, it was demonstrated that mainly phosphate groups are responsible for the binding on the surface of the biomass.

The neutron source terms for a proton beam hitting an O-18 enriched water target were calculated with MCNP6 and FLUKA. First comparisons of simulation and experiments for activation studies at the IBA CYCLONE 18/9 cyclotron.

We investigate the impact of the new LUNA rate for the nuclear reaction 22Ne(p,γ)23Na on the chemical ejecta of intermediate-mass stars, with particular focus on the thermally- pulsing asymptotic giant branch (TP-AGB) stars that experience hot-bottom burning. To this aim we use the PARSEC and COLIBRI codes to compute the complete evolution, from the pre- main sequence up to the termination of the TP-AGB phase, for a few sets of stellar models with initial masses in the range 3.0 M⊙ − 6.0 M⊙ and three values of metallicity, Zi = 0.0005, Zi = 0.006, and Zi = 0.014. We compare the results of the Ne-Na nucleosynthesis obtained with the new LUNA rate and others available in the literature. We find that the improvement in the astrophysical S-factor obtained with LUNA has remarkably reduced the corresponding nuclear uncertainties in the 22Ne and 23Na AGB yields, which drop from factors of ≃ 10 to just a few for the lowest metallicity models. The uncertainties that still affect the 22Ne and 23Na AGB ejecta are mainly dominated by evolutionary aspects (efficiency of mass-loss, dredge-up events, convection). With the new LUNA data AGB stars with hot-bottom burning produce amounts of 23Na that are in between those predicted with NACRE and Iliadis et al. rates. Finally, we discuss how the LUNA results impact on the hypothesis that invokes primordial massive AGB and super-AGB stars as the main agents of the observed O-Na anticorrelation in Galactic globular clusters. In this context, we derive quantitative constraints on the efficiencies that should characterize other key physical processes (mass loss, third dredge-up, sodium destruction) in order to simultaneously reproduce both the Na-rich, O-poor extreme of the anticorrelation and the observational constraints on the CNO abundance. While best-fitting AGB models can be actually singled out, yet they cannot be taken as a theoretical piece in full support to the AGB hypothesis, as various issues still remain.

Vortrag zum Kick-off Meeting des FENABIUM Verbundprojekts (BMBF) mit der TU Dresden und Universität Leipzig.
Die Ergebnisse zeigen die Synthese und Charakterisierung vierwertiger Actinidkomplexe mit Amidinen und Schiffschen Basen unter Schutzgasbedingungen, die in der Gruppe "Chemie der f-Elemente" des Instituts für Ressourcenökologie durchgeführt wurden.

The storage of highly radioactive waste is a challenging task for many scientists. For a deep geological deposition of the waste a multi-barrier concept is favoured, which combines a technical barrier (canister including the highly radioactive waste), a geotechnical barrier (e.g. Bentonite) and the geological barrier (host rock). Due to their properties, namely a high swelling capacity and a low hydraulic conductivity, Bentonites fulfil in this system a sealing and buffering function. Depending on the mineral composition Bentonites contain many suitable electron-donors and –acceptors, enabling potential microbial life. For the potential repository of nuclear waste the microbial mediated transformation of Bentonite could influence its properties as a barrier material. To elucidate the microbial potential within selected Bentonites, microcosms were set up containing a certain amount of Bentonite (20 g) and 40 ml anaerobic synthetic Opalinus-clay-pore water solution under an N2/CO2-gas-atmosphere. Substrates like acetate and lactate were supplemented to stimulate potential microbial activity. Microcosms were incubated in the dark, without shaking at 30°C. Within an indefinite time scale samples were taken at different time-points of incubation and were analysed regarding geochemical parameters like pH, O2-concentration, redox potential, iron-concentration and sulphate-concentration as well as biological parameters like the consumption and formation of metabolites. First results show that bentonites represent a source for microbial life, demonstrated by the consumption of lactate and the formation of pyruvate. Furthermore, microbial iron-reduction was determined. The results reveal the importance of the selection of the best suitable Bentonite in order to avoid transformation by indigenous microbes.

The temperature dependence of the upper critical field (H_c2) in a (Li_1−xFe_x)OHFe_1−ySe single crystal (T_c ≈ 40 K) has been determined by means of magnetotransport measurements down to 1.4 K both for inter-plane (H‖c, H^‖c _c2) and in-plane (H‖ab, H^‖ab _c2) field directions in static magnetic fields up to 14 T and pulsed magnetic fields up to 70 T. H^‖c _c2 exhibits a quasilinear increase with decreasing temperature below the superconducting transition and can be described well by an effective two-band model with unbalanced diffusivity, while H^‖ab _c2 shows a flattening below 35 K and follows the Werthamer–Helfand–Hohenberg (WHH) model incorporating orbital pair-breaking and spin-paramagnetic effects, yielding zero-temperature critical fields of H^‖c _c2(0) ≈ 67 T and H^‖ab _c2(0) ≈ 98 T. The anisotropy of the upper critical fields, γ(T)= H^‖ab _c2/ H^‖c _c2 monotonically decreases with decreasing temperature from about 7 near T_c to 1.5 at 0 K. This reduced anisotropy, observed in most Fe-based superconductors, is caused by the Pauli limitation of H^‖ab _c2.

We consider the conversion of an electric field into photons as a secondary probe of the dynamical Schwinger process. In spatially homogeneous electric fields, quantum fluctuations of electron-positron (e+e−) pairs are lifted on the mass shell leaving asymptotically a small finite pair density. The e+e− dynamics in turn couples to the quantized photon field and drives its on-shell mode occupation. The spectral properties of the emerging asymptotic photons accompanying the Schwinger process are calculated in lowest-order perturbation theory. Soft photons in the optical range are produced amass in the sub critical region, thus providing a promising discovery avenue, e.g.\ for laser parameters of the Extreme Light Initiative (ELI-NP) to be put in operation soon.

The soft-wall model, emerging as bottom-up holographic scenario anchored in the AdS/CFT correspondence, displays the disappearance of normalisable modes referring to vector mesons at a temperature $T_{\dis}$ depending on the chemical potential μ, $T_{\dis}(\mu)$. We explore options for making $T_{\dis}(\mu)$ consistent with the freeze-out curve Tf.o.(μ) from relativistic heavy-ion collisions and the cross-over curve Tc(μ) from QCD at small values of μ.