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Program - Brookhaven National Laboratory

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nuclei are short. We will describe a series of new measurements that were performed at the Lead Slowing-<br />

Down Spectrometer (LSDS) facility at Los Alamos <strong>National</strong> <strong>Laboratory</strong> (LANL), directed to measure the<br />

neutron-induced fission cross section of 237 U. The target was prepared by irradiation of an isotopically enriched<br />

sample of 236 U in the High Flux Isotope Reactor (HFIR) at Oak Ridge <strong>National</strong> <strong>Laboratory</strong> (ORNL),<br />

followed by a chemical separation and electro-deposition of the 237 U sample. A dedicated compensated<br />

ionization chamber was designed at the Nuclear and Radiochemistry Group (C-NR), LANL, consisting of<br />

two identical chambers for the simultaneous measurements of 235 U(n,f) and 237 U(n,f) rates. The samples<br />

of 235 U and 237 U were electroplated on opposite sides of the same Ti plate, at C-NR, LANL, and HFIR,<br />

ORNL, respectively. The four-day long measurement was carried out at the LSDS facility where a cube of<br />

high purity lead, 1.2 m on the side was driven by a high intensity pulsed neutron source in its center produced<br />

by 800 MeV protons on a tungsten target. The neutrons were moderated by scattering interactions<br />

with the lead resulting in a time-neutron energy correlation. The compensated ionization chamber was<br />

installed in one of the channels of LSDS and neutron-induced reaction rates were measured as a function<br />

of the neutron slowing-down time in the LSDS. Signals from the ionization chamber were recorded using<br />

waveform digitizers and saved for off-line analysis. Progress on the cross section data analysis will be presented.<br />

This work benefited from the LANSCE accelerator facility and was performed under the auspices<br />

of the U.S. Department of Energy under contract DE-AC52-06NA25396.<br />

BA 4 11:40 AM<br />

Cross Section Measurement of 237 Np(n, γ) at J-PARC/MLF/ANNRI<br />

K. Hirose, K. Furutaka, K.Y. Hara, H. Harada, A. Kimura, T. Kin, F. Kitatani, M. Koizumi, S.<br />

Nakamura, M. Ohshima, Y. Toh<br />

Japan Atomic Energ Agency<br />

M. Igashira, T. Katabuchi, M. Mizumoto<br />

Research <strong>Laboratory</strong> for Nuclear Reactors, Tokyo Institute of Technology, Japan<br />

T. Kamiyama, K. Kino, Y. Kiyanagi<br />

Graduate School of Engineering, Hokkaido University, Japan<br />

J. Hori<br />

Research Reactor Institute, Kyoto University, Japan<br />

The cross section of the 237 Np(n, γ) reaction has been measured in an energy range from 10 meV to 1 keV<br />

at the Japan Proton Accelerator Research Complex (J-PARC). The NaI(Tl) spectrometer installed in the<br />

accurate neutron-nucleus reaction measurement instrument (ANNRI) was used for the measurement. The<br />

relative cross section was obtained using the neutron spectrum measured by the 10 B(n, α1) reaction. The<br />

absolute value of the cross section was deduced by normalizing the relative cross section to the evaluated<br />

value in JENDL-4.0 at the first resonance. In this presentation, the obtained results for the cross section,<br />

the Westcott factor and the resonance analysis are reported. This work was supported by JSPS KAKENHI<br />

Grant Number 22226016.<br />

Session BC Nuclear Reaction Models<br />

Monday March 4, 2013<br />

Room: Empire East at 10:30 AM<br />

BC 1 10:30 AM<br />

29

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