Abstract

Measurements of the isotope distribution of fission fragments, often denoted as the primary fission yield (pre-neutron yield) or independent fission yield (post-neutron yield) are still challenging at low excitation energies, so that it is important to investigate it within a theory. Such quantities are vital for applications as well. In this study, fragment distributions from the fission of U isotopes at low excitation energies are studied using a dynamical model. The potential energy surface is derived from the two center shell model including the shell and pairing corrections. In order to calculate the charge distribution of fission fragments, we introduce a new parameter η Z as the charge asymmetry, in addition to three parameters describing a nuclear shape, z as the distance between two centers of mass, δ as fragment deformation, and η A as the mass asymmetry. Using this model, we calculated the isotopic distribution of 236 U for the n-induced process 235 U + n → 236 U at low excitation energies. As a result, we found that the current model can well reproduce isotopic fission-fragment distribution which can be compared favorably with major libraries.

Highlights

  • We extend our model in order to treat the charge mode that allows the isotope yield calculation

  • We show various properties of obtained fission-fragments using the Langevin model with the charge fluctuation for 236U at E∗ = 20MeV which corresponds to n+235U at En = 14MeV

  • The current mass distribution reproduces the peak positions and width of the experimental data as well as the result only with the mass mode. It means that the current modification keeps the gross feature of the fissioning system

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Summary

Introduction

We extend our model in order to treat the charge mode that allows the isotope yield calculation. Difference between the current work and other recent works relating to the fission properties based on the Langevin model [2, 3], is the way of the charge mode. We consider the charge mode simultaneously with other degrees of freedom within unified computational scheme solving a system of coupled equations. Another important feature of the present model is that the microscopic shell effects are essential part of our model that is very important for the considered energy region

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