Abstract
Abstract The sequential fission of target-like nuclei after deep inelastic collisions of 58 Ni on 208 Pb and 90 Zr on 208 Pb is treated in the framework of a classical model. The transfer of mass during the deep inelastic part of the reaction and the mass asymmetry in the secondary fission process are dynamically described by coordinates which are defined by the mass ratios of the fragments. It is found that the coupling of the excitation energy to the fission degree of freedom is important in order to understand the experimental features of the sequential fission.
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