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Program - Brookhaven National Laboratory

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PR 64<br />

Nuclear Data Measurements at VERA for Fusion, ADS and Environmental Applications<br />

A. Wallner, VERA <strong>Laboratory</strong>, Faculty of Physics, University of Vienna, Währinger Strasse 17, A-1090<br />

Vienna, Austria and Department of Nuclear Physics, Australian <strong>National</strong> University, Canberra, ACT<br />

0200, Australia. K. Buczak, O. Forstner, R. Golser, W. Kutschera, C. Lederer, A. Priller, P. Steier,<br />

VERA <strong>Laboratory</strong>, Faculty of Physics, University of Vienna, Währinger Strasse 17, A-1090 Vienna,<br />

Austria. A. Klix, Karlsruhe Institute of Technology (KIT), Campus Nord, Institut für Kernphysik,<br />

Karlsruhe, Germany and. A. Krasa, A. Plompen, European Commission, Joint Research Centre,<br />

Institute for Reference Materials and Measurements, Geel, Belgium. D. Schumann, Paul Scherrer<br />

Institute, 5232 Villigen PSI, Switzerland. V. Semkova, NAPC Nuclear Data Section, International<br />

Atomic Energy Agency, A-1400 Vienna, Austria.<br />

Accurate cross sections are the backbones for calculating the production of long-lived radionuclides, which<br />

are of interest in a variety of fields. We summarize some recent cross-section measurements using Accelerator<br />

Mass Spectrometry (AMS) for counting long-lived radionuclides. Data presented here relate to<br />

nuclear fusion and advanced reactor concepts but also to the production of cosmogenic radionuclides for<br />

environmental and geological applications. Lack of information exists for a list of nuclides as pointed<br />

out by nuclear data requests. AMS represents an ultra-sensitive technique for measuring a limited, but<br />

steadily increasing number of longer-lived radionuclides. This method implies a two-step procedure with<br />

sample activation and subsequent AMS measurement. Cross section measurements via neutron activations<br />

in the fast neutron energy range were performed in cooperation with TU Dresden (TUD), utilizing their<br />

neutron generator, i.e. producing 14-MeV neutrons via the (d,t) reaction; and higher energy neutrons were<br />

produced via the Van de Graaff facility at IRMM, Geel, with neutron energies between 13 and 22 MeV.<br />

After activation the AMS measurements were performed at the VERA laboratory. An overview of recent<br />

measurements with reference to the respective application is given and the method is exemplified for some<br />

specific neutron-induced reactions leading to longer-lived nuclides: we will present new precise data for<br />

58 Ni(n,α) and 56 Fe(n,2n), both leading to 55 Fe. A systematic study of 14 C production from 14 N(n,p) and<br />

nat O will be shown. We also continued our studies of 26 Al production in a fusion environment. Finally, new<br />

results obtained for (n,3n) reactions on 70 Ge, 204 Pb and actinides will be compared to model calculations.<br />

PR 65<br />

Processing with LLNL’s New Evaluated Nuclear Data Structure GND and Infrastructure<br />

Fudge<br />

B. R. Beck, G. W. Hedstrom, C. M. Mattoon, Lawrence Livermore <strong>National</strong> <strong>Laboratory</strong>.<br />

Lawrence Livermore <strong>National</strong> <strong>Laboratory</strong> (LLNL) has made an initial effort towards defining a new structure<br />

for storing evaluated nuclear reaction data called Generalized Nuclear Data (GND). In addition to<br />

the structure, LLNL has developed an infrastructure called Fudge that allows one to modify, visualize<br />

and process (e.g., convert to a form suitable for deterministic transport) data stored in the GND structure.<br />

Additionally, the Fudge infrastructure can convert an ENDF formatted evaluated nuclear data file<br />

to and from GND. By converting an ENDF file to GND and processing we can now compare Fudge’s<br />

processing results to other ENDF processing codes such as NJOY. In this presentation we will describe the<br />

Fudge processing codes, demonstrate how to obtain Fudge and use it to process an ENDF file as well as<br />

show comparisons between the results of Fudge and NJOY processing. This work has been supported by<br />

Department of Energy contract No. DE-AC52-07NA27344 (Lawrence Livermore <strong>National</strong> <strong>Laboratory</strong>).<br />

295

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