Nonmesonic hyperon weak decay spectra in <sup>12</sup><sub>Λ</sub>C

We study the nonmesonic weak decay (NMWD) ΛN → nN of the <sup>12</sup><sub>Λ</sub>C hypernucleus induced by the nucleon N = n,p with transition rate ΓN. The nuclear process is described by the interplay of two models; one describing the NMWD of hyperon Λ in the nuclear envir...

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Autores principales: Gonzalez, I., Deppman, A., Duarte, S., Krmpotic, Francisco, Hussein, M. S., Barbero, César Alberto
Formato: Objeto de conferencia
Lenguaje:Inglés
Publicado: 2010
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Acceso en línea:http://sedici.unlp.edu.ar/handle/10915/84346
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id I19-R120-10915-84346
record_format dspace
institution Universidad Nacional de La Plata
institution_str I-19
repository_str R-120
collection SEDICI (UNLP)
language Inglés
topic Ciencias Exactas
Física
Nonmesonic weak decay
Partículas Elementales
spellingShingle Ciencias Exactas
Física
Nonmesonic weak decay
Partículas Elementales
Gonzalez, I.
Deppman, A.
Duarte, S.
Krmpotic, Francisco
Hussein, M. S.
Barbero, César Alberto
Nonmesonic hyperon weak decay spectra in <sup>12</sup><sub>Λ</sub>C
topic_facet Ciencias Exactas
Física
Nonmesonic weak decay
Partículas Elementales
description We study the nonmesonic weak decay (NMWD) ΛN → nN of the <sup>12</sup><sub>Λ</sub>C hypernucleus induced by the nucleon N = n,p with transition rate ΓN. The nuclear process is described by the interplay of two models; one describing the NMWD of hyperon Λ in the nuclear environment, and the other taking into account the Final State Interaction (FSI) of the two outgoing nucleons with the residual nucleus. The first one is done in the framework of the Independent-Particle Shell-Model (IPSM), with the decay dynamics represented by the exchange of π+η+K+ρ+ω+ K*mesons with usual parametrization. For the second one is used a time dependent multicollisional intranuclear cascade schema (implemented in the CRISP code - Collaboration Rio-São Paulo). The results obtained for inclusive and exclusive kinetic energy spectra, and the angular correlation are compared with recent data from KEK and FINUDA experiments. The calculated ratio (Γ n /Γ p ) FSI , between the numbers of emitted back-to-back nn and np pairs, is in good agreement with the experimental data.
format Objeto de conferencia
Objeto de conferencia
author Gonzalez, I.
Deppman, A.
Duarte, S.
Krmpotic, Francisco
Hussein, M. S.
Barbero, César Alberto
author_facet Gonzalez, I.
Deppman, A.
Duarte, S.
Krmpotic, Francisco
Hussein, M. S.
Barbero, César Alberto
author_sort Gonzalez, I.
title Nonmesonic hyperon weak decay spectra in <sup>12</sup><sub>Λ</sub>C
title_short Nonmesonic hyperon weak decay spectra in <sup>12</sup><sub>Λ</sub>C
title_full Nonmesonic hyperon weak decay spectra in <sup>12</sup><sub>Λ</sub>C
title_fullStr Nonmesonic hyperon weak decay spectra in <sup>12</sup><sub>Λ</sub>C
title_full_unstemmed Nonmesonic hyperon weak decay spectra in <sup>12</sup><sub>Λ</sub>C
title_sort nonmesonic hyperon weak decay spectra in <sup>12</sup><sub>λ</sub>c
publishDate 2010
url http://sedici.unlp.edu.ar/handle/10915/84346
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