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Bimodal fission of Hs*

Authors :
Francis Hanappe
G. N. Knyazheva
E. M. Kozulin
I. M. Itkis
E. Vardaci
K. V. Novikov
M. G. Itkis
T. Loktev
Giorgio Giardina, Avazbek K Nasirov and Giuseppe Mandaglio
Itkis, I. M
Itkis, M. G
Knyazheva, G. N
Kozulin, E. M
Loktev, T. A
Novikov, K. V
Hanappe, F
Vardaci, Emanuele
Source :
Journal of physics. Conference series, 515 (1
Publication Year :
2014
Publisher :
IOP Publishing, 2014.

Abstract

Mass and energy distributions of fission fragments obtained in the reactions 22Ne + 249Cf, 26Mg + 248Cm, and 22Ne + 238U have been measured. A special attention will be paid on the properties of mass-energy distribution of fission fragments obtained in the reaction 26Mg + 248Cm at an excitation energy of 35 MeV. At this energy shell effects should become more effective in fission, the TKE distribution of symmetric fragments obtained in the reaction 26Mg + 248Cm differs strongly from a Gaussian shape. Besides a low-energy component, a high-energy component, not foreseen in the LDM, arises. This is attributed to the fact that both fission fragments are close to the spherical neutron shell N 82. It means that for the compound nucleus 274Hs*, formed in the reaction 26Mg + 248Cm, the phenomenon of bimodal fission was observed for the first time. For the compound nucleus 260No* formed in the reaction 22Ne + 238U at the initial excitation energy of 41 MeV the bimodal fission as well as superasymmetric fission were observed. © Published under licence by IOP Publishing Ltd.<br />SCOPUS: cp.j<br />info:eu-repo/semantics/published

Details

Language :
English
Database :
OpenAIRE
Journal :
Journal of physics. Conference series, 515 (1
Accession number :
edsair.doi.dedup.....e5d894640e94c2832aab970439d1c620