Neutron emission effects on fragment mass and kinetic energy distribution from fission of Pu-239 induced by thermal neutrons
The average of fragment kinetic energy (<E*>) and the multiplicity of prompt neutrons (v) as a function of fragment mass (m*), as well as the fragment mass yield (Y (m*)) from thermal neutron induced fission of Pu-239, have been measured by Tsuchiya et al. In that work the mass and kinetic ener...
| Autores: | , , |
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| Tipo de recurso: | artículo |
| Fecha de publicación: | 2010 |
| País: | Perú |
| Institución: | Instituto Peruano de Energía Nuclear |
| Repositorio: | IPEN-Institucional |
| Idioma: | inglés |
| OAI Identifier: | oai:repositorio.ipen.gob.pe:20.500.13054/660 |
| Acceso en línea: | https://hdl.handle.net/20.500.13054/660 |
| Access Level: | acceso abierto |
| Palabra clave: | Emisión de neutrones Plutonio 239 Fragmentación nuclear Energía cinética Neutrones térmicos Método de Monte Carlo |
| Sumario: | The average of fragment kinetic energy (<E*>) and the multiplicity of prompt neutrons (v) as a function of fragment mass (m*), as well as the fragment mass yield (Y (m*)) from thermal neutron induced fission of Pu-239, have been measured by Tsuchiya et al. In that work the mass and kinetic energy are calculated from the measured kinetic energy of one fragment and the diference of time of flight of the two complementary fragments. However they do not present their results about the standard deviation σE* (m*). In this work we have made a numerical simulation of that experiment, assuming an initial distribution of the primary fragment kinetic energy (E(A)) with a constant value of the standard deviation as function of fragment mass (σE (A)). As a result of that simulation we obtain the dependence σE* (m*) which presents an enhancement between m* = 92 and m* = 110, and a peak at m* = 121. |
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