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Fission-mode calculations for 239U,a revision of the multi-modal random neck-rupture model
Institution:1. Institute Laue-Langevin, F-38042 Grenoble Cédex 9, France;2. JRC - Institute for Reference Material and Measurements (IRMM), Retieseweg, B-2440 Geel, Belgium;1. Culham Centre for Fusion Energy, Science Centre, Abingdon, Oxon, OX14 3DB, UK;2. ENEA, Department of Fusion and Technology for Nuclear Safety and Security, E. Fermi 45, 00044 Frascati, Rome, Italy;1. Department of Physics, Faculty of Science, Fayoum University, Egypt;2. Department of Physics, Taibah University, Almadinah Almunawwarah, Saudi Arabia;3. Department of Physics, Cairo University, Giza 12613, Egypt;1. Institute for Nuclear Research, 03028 Kyiv, Ukraine;2. Cyclotron Institute, Texas A&M University, College Station, TX 77843, USA
Abstract:In the course of an experimental study of the fragment characteristics after neutron-induced fission of 238U with incident neutron energies between 1.2 and 5.8 MeV fission-mode calculations in the frame of the multi-modal random neck-rupture model have been performed. During these calculations some technical parts of the model have been revised. The identification of fission modes is now based on unequivocal and reproducible criteria. The Rayleigh criterion has consequently been applied to determine each possible scission configuration. The most remarkable new results are that all physically relevant fission modes branch off in the second potential minimum exhibiting different outer barriers, and that the total kinetic energy distribution of the fission fragments is a direct consequence of the Rayleigh criterion. The fragment characteristics as the mean mass, the mean total kinetic energy and the corresponding width obtained from the fission-mode calculations compare reasonably well with the experimental findings.For the first time the weighted fission cross sections through each particular fission mode have been analyzed simultaneously using a Hill-Wheeler type expression for the transmission through a double-humped fission barrier. The results support the picture of individual outer barriers with slightly different penetrabilities and a slightly lower inner barrier.
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