Kentaro Hirose
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Kentaro Hirose has a total of 46 co-authors. Here are the top co-authors by number of shared publications:
H. Makii
Advanced Science Research Center, Japan Atomic Energy Agency (JAEA), 2-4 Shirakata Shirane, Tokai, Ibaraki 319-1195 Japan
2 shared publications- Hideo Harada
Nuclear Science and Engineering Center, Japan Atomic Energy Agency, Ibaraki, Japan
2 shared publications I. Nishinaka
Advanced Science Research Center, Japan Atomic Energy Agency (JAEA), 2-4 Shirakata Shirane, Tokai, Ibaraki 319-1195 Japan
2 shared publicationsK. Nishio
Advanced Science Research Center, Japan Atomic Energy Agency (JAEA), 2-4 Shirakata Shirane, Tokai, Ibaraki 319-1195 Japan
2 shared publicationsN. Tamura
Graduate School of Science and Technology, Niigata University, Niigata 950-2181, Japan
2 shared publicationsS. Chiba
Laboratory for Advanced Nuclear Energy, Institute for Innovative Research, Tokyo Institute of Technology, 2-12-1-N1-19, Ookayama, Meguro-ku, Tokyo 152-8550 Japan
2 shared publications
Latest Publications
- 27 November 2017
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 119 (22) , 222501
Role of Multichance Fission in the Description of Fission-Fragment Mass Distributions at High Energies
Fission-fragment mass distributions were measured for , , and populated in the excitation-energy range from 10 to 60 MeV by multinucleon transfer channels in the reaction at the Japan Atomic Energy Agency tandem facility. Among them, the data for and were observed for the first time. It was found that the mass distributions for all the studied nuclides maintain a double-humped shape up to the highest measured energy in contrast to expectations of predominantly symmetric fission due to the washing out of nuclear shell effects. From a comparison with the dynamical calculation based on the fluctuation-dissipation model, this behavior of the mass distributions was unambiguously attributed to the effect of multichance fission.- 27 November 2017
- Published by American Physical Society (APS) in Physical Review Letters
- Vol. 119 (22) , 222501
Role of Multichance Fission in the Description of Fission-Fragment Mass Distributions at High Energies
Fission-fragment mass distributions were measured for , , and populated in the excitation-energy range from 10 to 60 MeV by multinucleon transfer channels in the reaction at the Japan Atomic Energy Agency tandem facility. Among them, the data for and were observed for the first time. It was found that the mass distributions for all the studied nuclides maintain a double-humped shape up to the highest measured energy in contrast to expectations of predominantly symmetric fission due to the washing out of nuclear shell effects. From a comparison with the dynamical calculation based on the fluctuation-dissipation model, this behavior of the mass distributions was unambiguously attributed to the effect of multichance fission.- 15 December 2016
- Published by Elsevier in Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
- Vol. 856, 133-138
Simultaneous measurement of neutron-induced fission and capture cross sections for 241Am at neutron energies below fission threshold
- 15 December 2016
- Published by Elsevier in Nuclear Instruments and Methods in Physics Research Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
- Vol. 856, 133-138
Simultaneous measurement of neutron-induced fission and capture cross sections for 241Am at neutron energies below fission threshold
- Open Access
- 28 January 2013
- Published by Taylor & Francis in Journal of Nuclear Science and Technology
- Vol. 50 (2) , 188-200
Cross-section measurement of237Np (n,????) from 10 meV to 1 keV at Japan Proton Accelerator Research Complex
The cross-section of the 237Np reaction has been measured in the energy range from 10 meV to 1 keV using the ANNRI-NaI(Tl) spectrometer at the Japan Proton Accelerator Research Complex (J-PARC). The cross-section was obtained relative to that of the 10B reaction. The absolute value of the cross-section was deduced by normalizing the relative cross-section to the evaluated value of JENDL-4.0 at the first resonance. The thermal cross-section was obtained to be ( ) b. The Maxwellian-averaged cross-section for meV was derived as ( ) b by referring the cross-section below 10 meV from JENDL-4.0. These results lead to the Westcott's g-factor of .
- 28 January 2013
- Published by Taylor & Francis in Journal of Nuclear Science and Technology
- Vol. 50 (2) , 188-200
Open AccessCross-section measurement of237Np (n,????) from 10 meV to 1 keV at Japan Proton Accelerator Research Complex
The cross-section of the 237Np reaction has been measured in the energy range from 10 meV to 1 keV using the ANNRI-NaI(Tl) spectrometer at the Japan Proton Accelerator Research Complex (J-PARC). The cross-section was obtained relative to that of the 10B reaction. The absolute value of the cross-section was deduced by normalizing the relative cross-section to the evaluated value of JENDL-4.0 at the first resonance. The thermal cross-section was obtained to be ( ) b. The Maxwellian-averaged cross-section for meV was derived as ( ) b by referring the cross-section below 10 meV from JENDL-4.0. These results lead to the Westcott's g-factor of .