Abstract

Using the stochastic Langevin model, we calculate the evolution of postsaddle giant dipole resonance (GDR) $\ensuremath{\gamma}$-ray multiplicity (${M}_{\ensuremath{\gamma}}$) as a function of the postsaddle friction strength ($\ensuremath{\beta}$) with excitation energy for ${}^{240}$Cf, ${}^{224}$Th, and ${}^{200}$Pb systems. It is found that with raising the excitation energy the sensitivity of the postsaddle $\ensuremath{\gamma}$ emission to friction is substantially increased. We further find that ${M}_{\ensuremath{\gamma}}$ shows a greater sensitivity to $\ensuremath{\beta}$ with increasing size of the fissioning nucleus. The results suggest that on the experimental side, populating those fissioning systems with a large size and a high energy favors better determination of the postsaddle friction strength by measuring the GDR $\ensuremath{\gamma}$ multiplicity emitted in the fission process.

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