Nonmesonic weak decay of Λ hypernuclei: The ΛN - ΣN coupling
- Autores
- Bauer, Eduardo; Garbarino, G.; Rodríguez Peña, Carlos Andrés
- Año de publicación
- 2017
- Idioma
- inglés
- Tipo de recurso
- artículo
- Estado
- versión publicada
- Descripción
- The nonmesonic weak decay of Λ hypernuclei is studied within a microscopic diagrammatic approach which is extended to include the ΛN - ΣN strong interaction coupling. We adopt a nuclear matter formalism which, through the local density approximation, allows us to model finite hypernuclei. One-meson-exchange potentials are used for the weak and strong four-baryon interactions. The rates for the neutron- and proton-induced weak decays, ΛN → nN and ΛN → ΣN → nN (N = n or p; Σ = Σ⁻, Σ⁰, and Σ⁺), are predicted for Λ¹²C, Λ²⁸Si, Λ⁵⁶Fe, and Λ²⁰⁸Pb. The ΛN - ΣN coupling turns out to provide a contribution of about 23% (5%) to the total neutron-induced rate (proton-induced rate). Again as an effect of the hyperon coupling, the total one-nucleon-induced rate increases by about 9%, while the Γn/Γp ratio increases by about 17%. The saturation property of the nonmesonic rates with increasing hypernuclear mass number is clearly obtained and explained. The above percentage modifications remain almost unaltered through the hypernuclear mass number. All the non-negligible changes introduced by the ΛN - ΣN coupling lead to a definite improvement of our predictions once compared with the available KEK and FINUDA data.
Facultad de Ciencias Astronómicas y Geofísicas
Facultad de Ciencias Exactas
Instituto de Física La Plata - Materia
-
Astronomía
Ciencias Exactas
Física
Physics
hypernuclei
microscopic diagrammatic approach
nuclear matter
meson
nonmesonic weak decay - Nivel de accesibilidad
- acceso abierto
- Condiciones de uso
- http://creativecommons.org/licenses/by-nc-sa/4.0/
- Repositorio
- Institución
- Universidad Nacional de La Plata
- OAI Identificador
- oai:sedici.unlp.edu.ar:10915/126543
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Nonmesonic weak decay of Λ hypernuclei: The ΛN - ΣN couplingBauer, EduardoGarbarino, G.Rodríguez Peña, Carlos AndrésAstronomíaCiencias ExactasFísicaPhysicshypernucleimicroscopic diagrammatic approachnuclear mattermesonnonmesonic weak decayThe nonmesonic weak decay of Λ hypernuclei is studied within a microscopic diagrammatic approach which is extended to include the ΛN - ΣN strong interaction coupling. We adopt a nuclear matter formalism which, through the local density approximation, allows us to model finite hypernuclei. One-meson-exchange potentials are used for the weak and strong four-baryon interactions. The rates for the neutron- and proton-induced weak decays, ΛN → nN and ΛN → ΣN → nN (N = n or p; Σ = Σ⁻, Σ⁰, and Σ⁺), are predicted for <sub>Λ</sub>¹²C, <sub>Λ</sub>²⁸Si, <sub>Λ</sub>⁵⁶Fe, and <sub>Λ</sub>²⁰⁸Pb. The ΛN - ΣN coupling turns out to provide a contribution of about 23% (5%) to the total neutron-induced rate (proton-induced rate). Again as an effect of the hyperon coupling, the total one-nucleon-induced rate increases by about 9%, while the Γ<sub>n</sub>/Γ<sub>p</sub> ratio increases by about 17%. The saturation property of the nonmesonic rates with increasing hypernuclear mass number is clearly obtained and explained. The above percentage modifications remain almost unaltered through the hypernuclear mass number. All the non-negligible changes introduced by the ΛN - ΣN coupling lead to a definite improvement of our predictions once compared with the available KEK and FINUDA data.Facultad de Ciencias Astronómicas y GeofísicasFacultad de Ciencias ExactasInstituto de Física La Plata2017-10info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionArticulohttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdfhttp://sedici.unlp.edu.ar/handle/10915/126543enginfo:eu-repo/semantics/altIdentifier/issn/2469-9985info:eu-repo/semantics/altIdentifier/issn/2469-9993info:eu-repo/semantics/altIdentifier/arxiv/1701.03957info:eu-repo/semantics/altIdentifier/doi/10.1103/physrevc.96.044303info:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-sa/4.0/Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International (CC BY-NC-SA 4.0)reponame:SEDICI (UNLP)instname:Universidad Nacional de La Platainstacron:UNLP2025-09-03T11:02:19Zoai:sedici.unlp.edu.ar:10915/126543Institucionalhttp://sedici.unlp.edu.ar/Universidad públicaNo correspondehttp://sedici.unlp.edu.ar/oai/snrdalira@sedici.unlp.edu.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:13292025-09-03 11:02:19.956SEDICI (UNLP) - Universidad Nacional de La Platafalse |
dc.title.none.fl_str_mv |
Nonmesonic weak decay of Λ hypernuclei: The ΛN - ΣN coupling |
title |
Nonmesonic weak decay of Λ hypernuclei: The ΛN - ΣN coupling |
spellingShingle |
Nonmesonic weak decay of Λ hypernuclei: The ΛN - ΣN coupling Bauer, Eduardo Astronomía Ciencias Exactas Física Physics hypernuclei microscopic diagrammatic approach nuclear matter meson nonmesonic weak decay |
title_short |
Nonmesonic weak decay of Λ hypernuclei: The ΛN - ΣN coupling |
title_full |
Nonmesonic weak decay of Λ hypernuclei: The ΛN - ΣN coupling |
title_fullStr |
Nonmesonic weak decay of Λ hypernuclei: The ΛN - ΣN coupling |
title_full_unstemmed |
Nonmesonic weak decay of Λ hypernuclei: The ΛN - ΣN coupling |
title_sort |
Nonmesonic weak decay of Λ hypernuclei: The ΛN - ΣN coupling |
dc.creator.none.fl_str_mv |
Bauer, Eduardo Garbarino, G. Rodríguez Peña, Carlos Andrés |
author |
Bauer, Eduardo |
author_facet |
Bauer, Eduardo Garbarino, G. Rodríguez Peña, Carlos Andrés |
author_role |
author |
author2 |
Garbarino, G. Rodríguez Peña, Carlos Andrés |
author2_role |
author author |
dc.subject.none.fl_str_mv |
Astronomía Ciencias Exactas Física Physics hypernuclei microscopic diagrammatic approach nuclear matter meson nonmesonic weak decay |
topic |
Astronomía Ciencias Exactas Física Physics hypernuclei microscopic diagrammatic approach nuclear matter meson nonmesonic weak decay |
dc.description.none.fl_txt_mv |
The nonmesonic weak decay of Λ hypernuclei is studied within a microscopic diagrammatic approach which is extended to include the ΛN - ΣN strong interaction coupling. We adopt a nuclear matter formalism which, through the local density approximation, allows us to model finite hypernuclei. One-meson-exchange potentials are used for the weak and strong four-baryon interactions. The rates for the neutron- and proton-induced weak decays, ΛN → nN and ΛN → ΣN → nN (N = n or p; Σ = Σ⁻, Σ⁰, and Σ⁺), are predicted for <sub>Λ</sub>¹²C, <sub>Λ</sub>²⁸Si, <sub>Λ</sub>⁵⁶Fe, and <sub>Λ</sub>²⁰⁸Pb. The ΛN - ΣN coupling turns out to provide a contribution of about 23% (5%) to the total neutron-induced rate (proton-induced rate). Again as an effect of the hyperon coupling, the total one-nucleon-induced rate increases by about 9%, while the Γ<sub>n</sub>/Γ<sub>p</sub> ratio increases by about 17%. The saturation property of the nonmesonic rates with increasing hypernuclear mass number is clearly obtained and explained. The above percentage modifications remain almost unaltered through the hypernuclear mass number. All the non-negligible changes introduced by the ΛN - ΣN coupling lead to a definite improvement of our predictions once compared with the available KEK and FINUDA data. Facultad de Ciencias Astronómicas y Geofísicas Facultad de Ciencias Exactas Instituto de Física La Plata |
description |
The nonmesonic weak decay of Λ hypernuclei is studied within a microscopic diagrammatic approach which is extended to include the ΛN - ΣN strong interaction coupling. We adopt a nuclear matter formalism which, through the local density approximation, allows us to model finite hypernuclei. One-meson-exchange potentials are used for the weak and strong four-baryon interactions. The rates for the neutron- and proton-induced weak decays, ΛN → nN and ΛN → ΣN → nN (N = n or p; Σ = Σ⁻, Σ⁰, and Σ⁺), are predicted for <sub>Λ</sub>¹²C, <sub>Λ</sub>²⁸Si, <sub>Λ</sub>⁵⁶Fe, and <sub>Λ</sub>²⁰⁸Pb. The ΛN - ΣN coupling turns out to provide a contribution of about 23% (5%) to the total neutron-induced rate (proton-induced rate). Again as an effect of the hyperon coupling, the total one-nucleon-induced rate increases by about 9%, while the Γ<sub>n</sub>/Γ<sub>p</sub> ratio increases by about 17%. The saturation property of the nonmesonic rates with increasing hypernuclear mass number is clearly obtained and explained. The above percentage modifications remain almost unaltered through the hypernuclear mass number. All the non-negligible changes introduced by the ΛN - ΣN coupling lead to a definite improvement of our predictions once compared with the available KEK and FINUDA data. |
publishDate |
2017 |
dc.date.none.fl_str_mv |
2017-10 |
dc.type.none.fl_str_mv |
info:eu-repo/semantics/article info:eu-repo/semantics/publishedVersion Articulo http://purl.org/coar/resource_type/c_6501 info:ar-repo/semantics/articulo |
format |
article |
status_str |
publishedVersion |
dc.identifier.none.fl_str_mv |
http://sedici.unlp.edu.ar/handle/10915/126543 |
url |
http://sedici.unlp.edu.ar/handle/10915/126543 |
dc.language.none.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
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dc.rights.none.fl_str_mv |
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openAccess |
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http://creativecommons.org/licenses/by-nc-sa/4.0/ Creative Commons Attribution-NonCommercial-ShareAlike 4.0 International (CC BY-NC-SA 4.0) |
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