Abstract

The fragment angular distribution from the multichance fission of excited nuclei with a double humped fission barrier is considered. It is shown that the fragment angular distribution is determined by contributions related to both the saddle points. The relative weights of these contributions are calculated in the framework of the diffusion model. The possibility of determining the nuclear dissipation is discussed. A comparison of the experimental data with the calculations leads to a value of the reduced dissipation coefficient for the Pu isotopes produced in the reaction at = 37 and 43 MeV.

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