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Hg region; Derivative analysis approachKattikat Melcom, D. T.*; Tsekhanovich, I.*; Guezet, F.*; Andreyev, A.*; Nishio, Katsuhisa
Physical Review C, 114(1), p.014627_1 - 014627_8, 2026/07
Times Cited Count:0 Percentile:0.00(Physics, Nuclear)Takagi, Shinya*; Harada, Sota*; Aritomo, Yoshihiro*; Hirose, Kentaro; Nishio, Katsuhisa
Physical Review C, 112(4), p.044607_1 - 044607_9, 2025/10
Times Cited Count:0 Percentile:0.00(Physics, Nuclear)Iwamoto, Hiroki; Meigo, Shinichiro
Journal of Nuclear Science and Technology, 56(2), p.160 - 171, 2019/02
Times Cited Count:4 Percentile:28.59(Nuclear Science & Technology)We present a new model to describe the fission probability of the high-energy fission model, as deduced from the intranuclear cascade calculation with the Intra-Nuclear Cascade model of Li
ge (INCL) version 4.6 and Prokofiev's phenomenological systematics of the proton-induced fission cross sections. This model is implemented in the de-excitation model of the Generalized Evaporation Model (GEM), and applied to Monte Carlo spallation reaction simulation using the Particle and Heavy Ion Transport code System (PHITS). Comparing with experimental data for subactinide nuclei shows that this model can provide a unified prediction of the proton-, neutron-, and deuteron-induced fission cross sections with markedly improved accuracy. The calculated fission fragments tend to shift to higher mass numbers. To account for the isotopic distributions of fission fragments within the framework of a coupled INCL/GEM, modification of INCL is required, especially for description of the highly-excited states of residual nuclei.
Kishida, Norio*; Murata, Toru*; Asami, Tetsuo*; Kosako, Kazuaki*; Maki, Koichi*; Harada, Hideo*; Lee, Y.*; Chang, J.*; Chiba, Satoshi; Fukahori, Tokio
AIP Conference Proceedings 769, p.199 - 202, 2005/05
Nuclear data for photonuclear reactions are required in the field of shielding design of high-energy electron accelerators and high-energy
-ray therapy. The JENDL Photonuclear Data File was prepared by a working group on nuclear data evaluations for photonuclear reactions in Japanese Nuclear Data Committee. From a survey of many literatures, it is difficult to construct the photonuclear data file by using only measured data, since there are not sufficient experimental data. We were therefore evaluating with theoretical calculations based on statistical nuclear reaction models. The photonuclear cross sections that are to be contained in the file are as follows: photoabsorption cross sections, yield cross sections and DDX for neutrons, protons, deuterons, tritons,
He-particles and alpha-particles, and isotope production cross sections. For the actinide nuclides, photofission cross sections are also included. The maximum energy of incident photons is 140 MeV and stored are the photonuclear data for 68 nuclides from
H to
Np.
Np,
Am,
Am and
Am irradiated by neutrons and protons at energies up to 250 MeVKonobeyev, A. Y.; Fukahori, Tokio; Iwamoto, Osamu
JAERI-Research 2002-032, 36 Pages, 2002/12
The evaluation of nuclear data has been performed for
Np,
Am,
Am and
. Neutron data were obtained at the energies from 20 to 250 MeV and combined with JENDL-3.3 data at 20 MeV. Evaluation of the proton data has been done from 1 to 250 MeV. The coupled channel optical model was used to obtain angular distributions for elastic and inelastic scattering and transmission coefficients. Pre-equilibrium exciton model and Hauser-Feshbach statistical model were used to describe neutron and charged particles emission from the excited nuclei. These evaluation is the first work for producing the full set of evaluated file up to 250 MeV for
Np and americium isotopes.
Pu,
Pu,
Pu,
Pu and
Pu irradiated by neutrons and protons at the energies up to 250 MeVKonobeyev, A. Y.; Fukahori, Tokio; Iwamoto, Osamu
JAERI-Research 2002-029, 48 Pages, 2002/12
The evaluation of nuclear data for plutonium isotopes with atomic mass number from 238 to 242 has been performed. Neutron data were obtained at the energies from 20 to 250 MeV and combined with JENDL-3.3 data at 20 MeV. Evaluation of the proton data has been done from 1 to 250 MeV. The coupled channel optical model was used to obtain angular distributions for elastic and inelastic scattering and transmission coefficients. Pre-equilibrium exciton model and Hauser-Feshbach statistical model were used to describe neutron and charged particles emission from the excited nuclei. These evaluation is the first work for producing the full set of evaluated file up to 250 MeV for plutonium isotopes.
Nishitani, Takeo; Iguchi, Tetsuo*; Ebisawa, Katsuyuki*; Yamauchi, Michinori*; Walker, C.*; Kasai, Satoshi
JAERI-Tech 2002-062, 39 Pages, 2002/07
no abstracts in English
Yamauchi, Michinori*; Nishitani, Takeo; Ochiai, Kentaro; Morimoto, Yuichi*; Hori, Junichi; Ebisawa, Katsuyuki*; Kasai, Satoshi
JAERI-Tech 2002-032, 41 Pages, 2002/03
A micro-fission chamber and a dummy chamber without uranium were fabricated and the performance was tested. They are designed to be installed inside the vacuum vessel of compact ITER (ITER-FEAT) for neutron monitoring. Vacuum leak rate of the chamber, resistances between central conductor and outer sheath, and mechanical strength up to 50G acceleration were confirmed to meet design criteria. Gamma-ray sensitivity was measured with
Co gamma-ray irradiation facility at JAERI Takasaki. The output signals for gamma-rays in Campbelling mode were estimated to be less than 0.1% those by neutrons at the location behind the blanket module in ITER-FEAT. Detector response for 14 MeV neutrons was investigated with the FNS facility. Excellent linearity between count rates and neutron fluxes was confirmed. According to the test for the change of surrounding materials, the sensitivity was enhanced by slow-downed neutrons, which agreed with the calculation result by MCNP-4C code. As a result, it was concluded that the developed micro-fission chamber is applicable for ITER-FEAT.
Sawa, Kazuhiro; Ueta, Shohei; Sumita, Junya; Verfondern, K.*
Journal of Nuclear Science and Technology, 38(6), p.411 - 419, 2001/06
Times Cited Count:18 Percentile:74.90(Nuclear Science & Technology)no abstracts in English
Ando, Yoshihira*; Nishihara, Kenji; Takano, Hideki
Journal of Nuclear Science and Technology, 37(10), p.924 - 933, 2000/10
no abstracts in English
Sawa, Kazuhiro; Sumita, Junya; Watanabe, Takashi*
JAERI-Data/Code 99-034, 115 Pages, 1999/06
no abstracts in English
UV.M.Maslov*; Y.V.Porodzinskij*; Hasegawa, Akira; Shibata, Keiichi
JAERI-Research 98-040, 64 Pages, 1998/08
no abstracts in English
Sawa, Kazuhiro; Minato, Kazuo; Fukuda, Kosaku
JAERI-Research 96-063, 34 Pages, 1996/11
no abstracts in English
V.M.Maslov*;
JAERI-Research 96-030, 68 Pages, 1996/06
no abstracts in English
latticesNakajima, Ken;
Nuclear Technology, 113, p.375 - 379, 1996/03
Times Cited Count:5 Percentile:44.01(Nuclear Science & Technology)no abstracts in English
U fission cross sectionV.M.Maslov*;
Nuclear Science and Engineering, 124(3), p.492 - 497, 1996/00
Times Cited Count:7 Percentile:53.42(Nuclear Science & Technology)no abstracts in English
Fukahori, Tokio; Chiba, Satoshi; Takada, Hiroshi; Nakahara, Yasuaki; Watanabe, Yukinobu*
Nihon Genshiryoku Gakkai-Shi, 37(4), p.264 - 273, 1995/00
Times Cited Count:0 Percentile:0.00(Nuclear Science & Technology)no abstracts in English
U captures to
U fission in low-enriched UO
tight latticesNakajima, Ken; ; Yamamoto, Toshihiro; ; Suzaki, Takenori
Journal of Nuclear Science and Technology, 31(11), p.1160 - 1170, 1994/11
Times Cited Count:8 Percentile:59.14(Nuclear Science & Technology)no abstracts in English
Ogawa, Toshihide; ; Hoshino, Katsumichi; Odajima, Kazuo; Maeda, Hikosuke
JAERI-M 94-021, 45 Pages, 1994/02
no abstracts in English
F +
Ta reaction at high angular momentumQ.Bujia*; Ikezoe, Hiroshi; Sugiyama, Yasuharu; Tomita, Yoshiaki; Ideno, K.; H.J.Kim*
JAERI-M 91-188, 8 Pages, 1991/11
no abstracts in English