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Program - Brookhaven National Laboratory

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LF 5 5:00 PM<br />

A New Signal Processing Technique for Neutron Capture Cross Section Measurement<br />

Based on Pulse Width Analysis<br />

T. Katabuchi, M. Mizumoto, K. Terada, T. Matsuhashi, M. Igashira<br />

Tokyo Institute of Technology<br />

K. Hirose, A. Kimura, S. Nakamura, Y. Toh, K. Y. Hara, F. Kitatani, K. Furutaka, M. Koizumi, M.<br />

Oshima, H. Harada<br />

Japan Atomic Energy Agency<br />

J. Hori<br />

Kyoto University<br />

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

Hokkaido University<br />

We have been developing an NaI(Tl) spectrometer for neutron capture cross section measurement at the<br />

Materials and Life Science Experimental Facility (MLF) of the Japan Proton Accelerator Research Complex<br />

(J-PARC). The NaI(Tl) spectrometer was installed at the beam line of the Accurate Neutron Nucleus<br />

Reaction Measurement Instrument (ANNRI) in the MLF. The purpose of the NaI(Tl) spectrometer is (1)<br />

to provide reliable nuclear data by combining with measurement using a Ge spectrometer installed upstream<br />

of the ANNRI beam line and (2) to extend the achievable high energy limit of measurement beyond the<br />

Ge spectrometer measurement, using faster signal response of an NaI(Tl) detector than a Ge detector.<br />

To achieve the second goal, electronics and data acquisition system with a small dead time are required.<br />

Thus, we developed a new fast signal processing technique for neutron capture cross section measurement<br />

based on pulse width analysis. In the technique, pulse width of anode negative signals from photomultiplier<br />

tubes of the NaI(Tl) spectrometer were determined from time under a threshold level measured with a<br />

fast time digitizer (FAST ComTech MCS6). Then, the pulse width of each signal was converted to the<br />

pulse height from width-height calibration measurement using standard gamma-ray sources, and discrete<br />

gamma-rays from the neutron capture reactions, 28 Si(n,γ) 29 Si and 14 N(n,γ) 15 N. To test this pulse width<br />

method, we carried out cross section measurement of the 197 Au(n,γ) 198 Au and 99 Tc(n,γ) 100 Tc reactions.<br />

The pulse-height weighting technique was applied to derive the neutron capture cross sections. In this<br />

presentation, we present the whole scheme of the signal processing and data analysis, and compare the<br />

obtained cross sections with the evaluated nuclear data.<br />

LF 6 5:15 PM<br />

Neutron Flux Characterization of the Cold Beam PGAA-NIPS Facility at the Budapest<br />

Research Reactor<br />

Tamas Belgya, Zoltan Kis, Laszlo Szentmiklosi<br />

Centre for Energy Research IKI, HAS, Budapest, Hungary<br />

A reliable flux characterization is essential for facilities using neutron beams. The NIPS station at the<br />

Budapest Research Reactor (BRR) has recently been equipped with neutron-tomographic equipment. In<br />

addition to this, the beam could be characterized using a large surface wire chamber (on loan) applying<br />

time-of-flight method. The energy distribution was measured at 3 horizontal positions with this latter<br />

in pinhole geometry, while the spatial inhomogeneity was measured with our new neutron-tomographic<br />

equipment. The PGAA-NIPS facility at the BRR is heavily involved in the determination of nuclear data<br />

for reactor and other applications [1]. The cold neutron beam makes it possible to avoid problems arising<br />

187

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