Nonmesonic weak decay spectra of 4/ʌ He

To comprehend the recent Brookhaven National Laboratory experiment E788 on He Λ 4, we have outlined a simple theoretical framework, based on the independent-particle shell model, for the one-nucleon-induced nonmesonic weak decay spectra. Basically, the shapes of all the spectra are tailored by the k...

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Autores principales: Bauer, Eduardo, Galeao, A. P., Hussein, M. S., Krmpotić, Francisco, Parker, Joseph D.
Formato: Articulo
Lenguaje:Inglés
Publicado: 2009
Materias:
Acceso en línea:http://sedici.unlp.edu.ar/handle/10915/129532
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id I19-R120-10915-129532
record_format dspace
institution Universidad Nacional de La Plata
institution_str I-19
repository_str R-120
collection SEDICI (UNLP)
language Inglés
topic Física
Nonmesonic decay
One-nucleon spectra
Two-nucleon spectra
One-meson-exchange model
s-Shell hypernuclei
Independent-particle shell model
spellingShingle Física
Nonmesonic decay
One-nucleon spectra
Two-nucleon spectra
One-meson-exchange model
s-Shell hypernuclei
Independent-particle shell model
Bauer, Eduardo
Galeao, A. P.
Hussein, M. S.
Krmpotić, Francisco
Parker, Joseph D.
Nonmesonic weak decay spectra of 4/ʌ He
topic_facet Física
Nonmesonic decay
One-nucleon spectra
Two-nucleon spectra
One-meson-exchange model
s-Shell hypernuclei
Independent-particle shell model
description To comprehend the recent Brookhaven National Laboratory experiment E788 on He Λ 4, we have outlined a simple theoretical framework, based on the independent-particle shell model, for the one-nucleon-induced nonmesonic weak decay spectra. Basically, the shapes of all the spectra are tailored by the kinematics of the corresponding phase space, depending very weakly on the dynamics, which is gauged here by the one-meson-exchange potential. In spite of the straightforwardness of the approach a good agreement with data is achieved. This might be an indication that the final-state-interactions and the two-nucleon induced processes are not very important in the decay of this hypernucleus. We have also found that the π + K exchange potential with soft vertex-form-factor cutoffs (Λ π ≈ 0.7 GeV, Λ K ≈ 0.9 GeV ), is able to account simultaneously for the available experimental data related to Γ p and Γ n for H Λ 4, He Λ 4, and He Λ 5.
format Articulo
Articulo
author Bauer, Eduardo
Galeao, A. P.
Hussein, M. S.
Krmpotić, Francisco
Parker, Joseph D.
author_facet Bauer, Eduardo
Galeao, A. P.
Hussein, M. S.
Krmpotić, Francisco
Parker, Joseph D.
author_sort Bauer, Eduardo
title Nonmesonic weak decay spectra of 4/ʌ He
title_short Nonmesonic weak decay spectra of 4/ʌ He
title_full Nonmesonic weak decay spectra of 4/ʌ He
title_fullStr Nonmesonic weak decay spectra of 4/ʌ He
title_full_unstemmed Nonmesonic weak decay spectra of 4/ʌ He
title_sort nonmesonic weak decay spectra of 4/ʌ he
publishDate 2009
url http://sedici.unlp.edu.ar/handle/10915/129532
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AT husseinms nonmesonicweakdecayspectraof4ʌhe
AT krmpoticfrancisco nonmesonicweakdecayspectraof4ʌhe
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