@article{oai:repo.qst.go.jp:00048697,
 author = {Hirose, K. and Nishio, K. and Tanaka, S. and Leguillon, R. and Makii, H. and Nishinaka, Ichiro and Orlandi, R. and Tsukada, K. and Smallcombe, J. and J., Vermeulen M. and Chiba, S. and Aritomo, Y. and Ohtsuki, T. and Nakano, K. and Araki, S. and Watanabe, Y. and Tatsuzawa, R. and Takai, N. and Yamura, N. and Goto, S. and Tsekhanovich, I. and N., Andreyev A. and 西中 一朗},
 issue = {22},
 journal = {Physical Review Letters},
 month = {Dec},
 note = {Fission-fragment mass distributions were measured for 237–240U, 239–242Np, and 241–244Pu populated in the excitation-energy range from 10 to 60 MeV by multinucleon transfer channels in the reaction 18O+238U at the Japan Atomic Energy Agency tandem facility. Among them, the data for 240U and 240,241,242Np 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.},
 pages = {222501-1--222501-6},
 title = {Role of multichance fission in the description of fission-fragment mass distributions at high energies},
 volume = {119},
 year = {2017}
}