Neutron emission effects on fragment mass and kinetic energy distribution from fission of Pu-239 induced by thermal neutrons

Descripción del Articulo

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...

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Detalles Bibliográficos
Autores: Montoya, Modesto, Rojas, Justo, Lobato, Iván
Formato: artículo
Fecha de Publicación:2010
Institución:Instituto Peruano de Energía Nuclear
Repositorio:IPEN-Institucional
Lenguaje:inglés
OAI Identifier:oai:repositorio.ipen.gob.pe:20.500.13054/660
Enlace del recurso:https://hdl.handle.net/20.500.13054/660
Nivel de acceso:acceso abierto
Materia:Emisión de neutrones
Plutonio 239
Fragmentación nuclear
Energía cinética
Neutrones térmicos
Método de Monte Carlo
Descripción
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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