Dispersion of the energy distribution as a function of fission-fragment masses
Descripción del Articulo
Once again, the width of the total kinetic energy distribution for thermal neutron induced fission of U-235 and Pu-239 was measured as a function of the fragment mass-ratio. Data were obtained by means of the "double energy method" with an experimental lay-out specifically designed to elim...
| Autor: | |
|---|---|
| Formato: | artículo |
| Fecha de Publicación: | 1985 |
| Institución: | Instituto Peruano de Energía Nuclear |
| Repositorio: | IPEN-Institucional |
| Lenguaje: | inglés |
| OAI Identifier: | oai:repositorio.ipen.gob.pe:20.500.13054/75 |
| Enlace del recurso: | https://hdl.handle.net/20.500.13054/75 |
| Nivel de acceso: | acceso abierto |
| Materia: | Dispersiones Fragmentos de fisión Distribución de la energía Uranio 235 Plutonio 239 Fisión Método de Monte Carlo |
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Montoya, ModestoMontoya, Modesto2014-04-15T16:11:42Z2014-04-15T16:11:42Z1985-02Montoya Modesto. Dispersion of the energy distribution as a function of fission-fragment masses. Revista Informe Nuclear. 1985; 2(2):33-43.https://hdl.handle.net/20.500.13054/75Once again, the width of the total kinetic energy distribution for thermal neutron induced fission of U-235 and Pu-239 was measured as a function of the fragment mass-ratio. Data were obtained by means of the "double energy method" with an experimental lay-out specifically designed to eliminate possible error sources. An appropriate Monte-Carlo procedure was used to correct the raw data for all dispersion effects induced by prompt neutron emission. These "corrected" data clearly demonstrate that most, of the sharp variation in the observed width, σ EK (μ) previously interpreted as having some real physical origin, are in fact generated by the "uncorrected" raw data as such. Similarly treated data, obtained with the Lohengrin mass-spectrometer, are also discussed.Asociación de Profesionales Nucleares del IPENapplication/pdfengLimaPEinfo:eu-repo/semantics/openAccessInstituto Peruano de Energía NuclearRepositorio Institucional del Instituto Peruano de Energía Nuclearreponame:IPEN-Institucionalinstname:Instituto Peruano de Energía Nuclearinstacron:IPENDispersionesFragmentos de fisiónDistribución de la energíaUranio 235Plutonio 239FisiónMétodo de Monte CarloDispersion of the energy distribution as a function of fission-fragment massesDispersión de la distribución de energía en función de la masa de los fragmentos de fisióninfo:eu-repo/semantics/articleORIGINALInforme Nuclear - 2(2) (1985) p 33-43.pdfInforme Nuclear - 2(2) (1985) p 33-43.pdfapplication/pdf347361https://repositorio.ipen.gob.pe/bitstream/20.500.13054/75/1/Informe%20Nuclear%20-%202%282%29%20%281985%29%20p%2033-43.pdf18af2f81597d838d4475ceb05d37dff6MD51LICENSElicense.txtlicense.txttext/plain; charset=utf-8104https://repositorio.ipen.gob.pe/bitstream/20.500.13054/75/2/license.txt9e6c7c779786f52766c8501bd95e714cMD52TEXTInforme Nuclear - 2(2) (1985) p 33-43.pdf.txtInforme Nuclear - 2(2) (1985) p 33-43.pdf.txtExtracted texttext/plain12https://repositorio.ipen.gob.pe/bitstream/20.500.13054/75/3/Informe%20Nuclear%20-%202%282%29%20%281985%29%20p%2033-43.pdf.txt36c6f0b2061da514c400c0bc2749b5cfMD53THUMBNAILInforme Nuclear - 2(2) (1985) p 33-43.pdf.jpgInforme Nuclear - 2(2) (1985) p 33-43.pdf.jpgGenerated Thumbnailimage/jpeg23593https://repositorio.ipen.gob.pe/bitstream/20.500.13054/75/4/Informe%20Nuclear%20-%202%282%29%20%281985%29%20p%2033-43.pdf.jpg7b5c67d9bf3adf9b8cbb6c0700ba2ca7MD5420.500.13054/75oai:repositorio.ipen.gob.pe:20.500.13054/752022-02-07 18:03:39.958Repositorio Institucional del Instituto Peruano de Energía Nuclearrepositorio@ipen.gob.peU2UgRGlzdHJpYnV5ZSBiYWpvIHVuYSBMaWNlbmNpYSBDcmVhdGl2ZSBDb21tb25zIEF0cmlidWNpw7NuLU5vQ29tZXJjaWFsLVNpbkRlcml2YXIgNC4wIEludGVybmFjaW9uYWwuDQo= |
| dc.title.es_PE.fl_str_mv |
Dispersion of the energy distribution as a function of fission-fragment masses |
| dc.title.alternative.es_PE.fl_str_mv |
Dispersión de la distribución de energía en función de la masa de los fragmentos de fisión |
| title |
Dispersion of the energy distribution as a function of fission-fragment masses |
| spellingShingle |
Dispersion of the energy distribution as a function of fission-fragment masses Montoya, Modesto Dispersiones Fragmentos de fisión Distribución de la energía Uranio 235 Plutonio 239 Fisión Método de Monte Carlo |
| title_short |
Dispersion of the energy distribution as a function of fission-fragment masses |
| title_full |
Dispersion of the energy distribution as a function of fission-fragment masses |
| title_fullStr |
Dispersion of the energy distribution as a function of fission-fragment masses |
| title_full_unstemmed |
Dispersion of the energy distribution as a function of fission-fragment masses |
| title_sort |
Dispersion of the energy distribution as a function of fission-fragment masses |
| dc.creator.none.fl_str_mv |
Montoya, Modesto |
| author |
Montoya, Modesto |
| author_facet |
Montoya, Modesto |
| author_role |
author |
| dc.contributor.author.fl_str_mv |
Montoya, Modesto |
| dc.subject.es_PE.fl_str_mv |
Dispersiones Fragmentos de fisión Distribución de la energía Uranio 235 Plutonio 239 Fisión Método de Monte Carlo |
| topic |
Dispersiones Fragmentos de fisión Distribución de la energía Uranio 235 Plutonio 239 Fisión Método de Monte Carlo |
| description |
Once again, the width of the total kinetic energy distribution for thermal neutron induced fission of U-235 and Pu-239 was measured as a function of the fragment mass-ratio. Data were obtained by means of the "double energy method" with an experimental lay-out specifically designed to eliminate possible error sources. An appropriate Monte-Carlo procedure was used to correct the raw data for all dispersion effects induced by prompt neutron emission. These "corrected" data clearly demonstrate that most, of the sharp variation in the observed width, σ EK (μ) previously interpreted as having some real physical origin, are in fact generated by the "uncorrected" raw data as such. Similarly treated data, obtained with the Lohengrin mass-spectrometer, are also discussed. |
| publishDate |
1985 |
| dc.date.accessioned.none.fl_str_mv |
2014-04-15T16:11:42Z |
| dc.date.available.none.fl_str_mv |
2014-04-15T16:11:42Z |
| dc.date.issued.fl_str_mv |
1985-02 |
| dc.type.es_PE.fl_str_mv |
info:eu-repo/semantics/article |
| format |
article |
| dc.identifier.citation.es_PE.fl_str_mv |
Montoya Modesto. Dispersion of the energy distribution as a function of fission-fragment masses. Revista Informe Nuclear. 1985; 2(2):33-43. |
| dc.identifier.uri.none.fl_str_mv |
https://hdl.handle.net/20.500.13054/75 |
| identifier_str_mv |
Montoya Modesto. Dispersion of the energy distribution as a function of fission-fragment masses. Revista Informe Nuclear. 1985; 2(2):33-43. |
| url |
https://hdl.handle.net/20.500.13054/75 |
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eng |
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eng |
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info:eu-repo/semantics/openAccess |
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openAccess |
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application/pdf |
| dc.publisher.es_PE.fl_str_mv |
Lima |
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PE |
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Instituto Peruano de Energía Nuclear Repositorio Institucional del Instituto Peruano de Energía Nuclear |
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IPEN |
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Nota importante:
La información contenida en este registro es de entera responsabilidad de la institución que gestiona el repositorio institucional donde esta contenido este documento o set de datos. El CONCYTEC no se hace responsable por los contenidos (publicaciones y/o datos) accesibles a través del Repositorio Nacional Digital de Ciencia, Tecnología e Innovación de Acceso Abierto (ALICIA).
La información contenida en este registro es de entera responsabilidad de la institución que gestiona el repositorio institucional donde esta contenido este documento o set de datos. El CONCYTEC no se hace responsable por los contenidos (publicaciones y/o datos) accesibles a través del Repositorio Nacional Digital de Ciencia, Tecnología e Innovación de Acceso Abierto (ALICIA).
