Abstract.
The symmetric SL-mode and asymmetric lumped (S1 + S2)-mode fission cross-sections of 235U(n,F) and 233U(n,F) reactions are calculated up to \(E_{\rm {n}} = 200\) MeV within a statistical model. For each U nuclide, emerging in \((\rm {n},x\rm {nf})\) reactions a separate triaxial outer fission barrier is assumed for the SL-mode. To reproduce the measured branching ratio of symmetric and asymmetric fission events for the 238U(n,F) reaction, more fissions coming from neutron-deficient nuclei were assumed. The damping of the triaxial collective modes contribution to the level density at the SL-mode outer saddle was essential for the branching ratio description. These assumptions allow to reproduce observed fission cross-sections of 235U(n,F) and 233U(n,F) reactions. The calculated branching ratio sensitivity to the target nuclide fissility is investigated.
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Communicated by A. Molinari
Received: 26 August 2003, Revised: 31 January 2004, Published online: 17 August 2004
PACS:
24.10.Pa Thermal and statistical models - 25.85.Ec Neutron-induced fission - 24.75. + i General properties of fission
V.M. Maslov: maslov@bas-net.by
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Maslov, V.M. Uranium symmetric/asymmetric neutron-induced fission up to 200 MeV. Eur. Phys. J. A 21, 281–286 (2004). https://doi.org/10.1140/epja/i2003-10210-4
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DOI: https://doi.org/10.1140/epja/i2003-10210-4