Initialising ...
Initialising ...
Initialising ...
Initialising ...
Initialising ...
Initialising ...
Initialising ...
Goto, Jun; Sugawara, Masahiko*; Oshima, Masumi; Toh, Yosuke; Kimura, Atsushi; Osa, Akihiko; Koizumi, Mitsuo; Mizumoto, Motoharu; Osaki, Toshiro*; Igashira, Masayuki*; et al.
AIP Conference Proceedings 769, p.788 - 791, 2005/05
no abstracts in English
Kai, Tetsuya; Kobayashi, Katsuhei*; Yamamoto, Shuji*; Cho, H.*; Fujita, Yoshiaki*; Kimura, Itsuro*; Okawachi, Yasushi*; Wakabayashi, Toshio*
Annals of Nuclear Energy, 28(8), p.723 - 739, 2001/05
Times Cited Count:7 Percentile:48.68(Nuclear Science & Technology)no abstracts in English
Furutaka, Kazuyoshi
JNC TN8400 2000-028, 70 Pages, 2000/10
This report describes the study done by the author as a postdoctoral research associate at Japan Nuclear Cycle Development Institute. This report is divided into two parts: improvements in accuracy in determination of thermal neutron capture cross sections, and improvements in accuracy of photo-nuclear absorption cross section measurements using the HHS. (1)In the measurements of thermal neutron capture cross sections using an activation method, accuracies of the final results attained are limited by (1) accuracy of -ray peak detection efficiencies, and (2) accuracies of -ray emission probabilities. In this study; to determine thermal neutron capture cross sections more accurately, the following researches have been done using a newly developed three-dimensional coincidence measurement system: (1)accurate determination of -ray standard sources using a - coincidence method, for precise calibration of -ray peak detection efficiency, and (2) development of a - coincidence measurement system using a plastic scintillation detector as a -ray detector, for the determination of -ray emission probabilities of short-lived nuclides, and measurement of -ray emission probabilities of Tc nuclide using the coincidence system. (2)To transform radioactive nuclides with small thermal neutron capture cross sections, use of photonuclear absorption reaction has been suggested. In order to transform these nuclides efficiently using the reaction, one has to know detailed behavior of the photo-absorption cross sections. In this study, a Monte-Carlo simulation code has been used to create a standard set of -ray response functions of the high-resolution high-energy spectrometer (HHS), to enable reliable analyses of the data obtained by the spectrometer.
*
JNC TJ9400 2000-009, 63 Pages, 2000/02
The present status of nuclear data for technetium (Tc)-99, which is a well-known fission product (FP), has been reviewed and investigated. And making use of the Kyoto university Lead Slowing-down Spectrometer (KULS), the cross section of the Tc (n, ) Tc reaction has been measured in the energy range from thermal to keV neutron energy with an Ar-gas proportinal counter. The neutron flux/spectrum has been monitored with a BF proportional counter, and the relative measurement has been normalized to the well-known standard capture cross section value for the Tc (n, ) Tc reaction at 0.0253 eV. Self-shielding corrections, especially near the resonance peaks, were made by the calculations with the MCNP code. Although the experimental data measured by Chou et al with a lead slowing-down spectrometer are higher in general, the energy dependency is similar to the present measurement. The evaluated data in ENDF/B-VI and JENDL-3.2 are higher near the resonances at 5.6 and 20 eV and above several 100 eV. A lead slowing-down spectrometer was installed coupled to a 46 MeV electron linac at the Research Reactor Institute, Kyoto university (KURRI). Characteristics of the Kyoto University Lead Slowing-down Spectrometer (KULS) were measured and (1)the relation between neutron slowing-down time t(s) and energy E(keV) (E=190/t in Bi hole and E=156/t in Pb hole) and (2)the energy resolution (40% in Bi and Pb holes) were experimentally investigated. (3)The neutron energy spectrum in the KULS was also measured by the neutron TOF method. The results obtained by the MCNP code were in general agreement with these experimental ones.
Akimune, Hidetoshi; Daito, Izuru*; Fujita, Yoshitaka*; Fujiwara, Mamoru; Harakeh, M. N.*; Jnecke, J.*; Yosoi, Masaru*
Physical Review C, 61(1), p.011304_1 - 011304_4, 2000/01
Times Cited Count:22 Percentile:73.05(Physics, Nuclear)no abstracts in English
Nakajima, Kazuhisa; Nakanishi, Hiroshi*; Ogata, Atsushi*; Harano, Hideki*; Ueda, Toru*; Uesaka, Mitsuru*; Watanabe, Takahiro*; Yoshii, Koji*; Dewa, Hidenori; Hosokai, Tomonao; et al.
Proceedings of 6th European Particle Accelerator Conference (EPAC98) (CD-ROM), p.809 - 811, 1998/01
no abstracts in English
Yamagishi, Hideshi; Ara, Katsuyuki
JAERI-Research 97-063, 17 Pages, 1997/09
no abstracts in English
*
PNC TJ9604 97-001, 108 Pages, 1997/03
A lead slowing-down spectrometer was installed coupled to the 46 MeV electron linac at Research Reactor Institute, Kyoto university (KURRI). Characteristics of the Kyoto University Lead Slowing-down Spectrometer (KULS) were measured for (1)the relation between neutron slowing-down time t(s) and energy E (keV) (E=190/t in Bi hole and E=156/ in Pb hole), (2)energy resolutlon (40 % in Bi and Pb holes), and (3)neutron energy spectrum by the neutron TOF method. The results obtained by the MCNP code were in general agreement with these experimental ones. The KULS has been applied to the fission cross section measurements of Am-241, Am-243 and Am-242m relative to that of U-235 from 0.1 eV to 10 keV, making use of the back-to-back type double fission chambers. For Am-241, Dabbs and ENDF/B-VI data are in good agreement with the present measurement. The JEND L-3.2 data are smaller by a factor of 2 between 10 and 200 eV. The ENDF/B-VI data for Am-243 are lower between 15 and 60 eV, and the JENDL-3.2 are lower in general above 100 eV. It has been found that the preliminary result for the Am-242m(n,f) reaction is close to the ENDF/B-VI and the JENDL-3.2 data. Thermal neutron cross sections for Am-241 and Am-243 have also been measured in a standard Maxwellian distribution spectrum field. Finally, aiming at the measurement of capture cross section for MA nuclides, the experimental investigation for Np-237 sample (2 mg) has been performed with the KULS. Due to the comparable background counts to the foreground ones, the capture events from the sample have scarecely been detected with an Ar-gas proportional counter.
Morishima, Hiroshige*; Koga, Taeko*
PNC TJ1630 96-001, 27 Pages, 1996/03
no abstracts in English
PNC TJ1630 95-001, 29 Pages, 1995/03
None
Ikeda, Yujiro; Kasugai, Yoshimi*; Uno, Yoshitomo; Konno, Chikara; Maekawa, Hiroshi
Proc., Int. Conf. on Nuclear Data for Science and Technology,Vol. 2, 0, p.1078 - 1080, 1994/00
no abstracts in English
Kasugai, Atsushi; Sakamoto, Keishi; Maebara, Sunao; Tsuneoka, Masaki; Nagashima, Takashi
JAERI-M 93-101, 30 Pages, 1993/05
no abstracts in English
Uwamino, Yoshitomo*; Okubo, Toru*; Shibata, Seiichi*; Shibata, Tokushi*
PNC TJ2602 87-003, 32 Pages, 1988/03
None
Nuclear Instruments and Methods in Physics Research A, 253, p.43 - 46, 1986/00
Times Cited Count:0 Percentile:0.02(Instruments & Instrumentation)no abstracts in English
; N.R.Johnson*; F.K.McGowan*; C.Baktash*; I.Y.Lee*; Y.Schutz*; R.V.Ribas*; J.C.Wells*
Physical Review C, 33(6), p.1988 - 1998, 1986/00
Times Cited Count:45 Percentile:88.78(Physics, Nuclear)no abstracts in English
IEEE Transactions on Nuclear Science, NS-31(1), p.757 - 760, 1984/00
no abstracts in English
*;
Nuclear Instruments and Methods, 159(1), p.139 - 143, 1979/00
no abstracts in English