Structure of Cr51

Some comments are made on calculations with the generalized semimicroscopic model and a deformed configuration mixing shell model in the light of results obtained with a cluster-phonon model. Although the models yield a fairly good description of experimental data, a manifest discrepancy exists with...

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Publicado: 1983
Acceso en línea:https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_05562813_v28_n4_p1843_Heras
http://hdl.handle.net/20.500.12110/paper_05562813_v28_n4_p1843_Heras
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Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA) de Universidad de Buenos Aires
id paper:paper_05562813_v28_n4_p1843_Heras
record_format dspace
spelling paper:paper_05562813_v28_n4_p1843_Heras2023-06-08T15:41:28Z Structure of Cr51 Some comments are made on calculations with the generalized semimicroscopic model and a deformed configuration mixing shell model in the light of results obtained with a cluster-phonon model. Although the models yield a fairly good description of experimental data, a manifest discrepancy exists with these on the B(E2; 312→g.s.) values predicted by the generalized semimicroscopic and cluster-phonon models. There is also a difference in expected values for the nuclear deformation. NUCLEAR STRUCTURE Cr51; calculated levels, J, π, B(E2), B(M1), q, μ, S, b, τ. Cluster-phonon model; particle-hole excitations. © 1983 The American Physical Society. 1983 https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_05562813_v28_n4_p1843_Heras http://hdl.handle.net/20.500.12110/paper_05562813_v28_n4_p1843_Heras
institution Universidad de Buenos Aires
institution_str I-28
repository_str R-134
collection Biblioteca Digital - Facultad de Ciencias Exactas y Naturales (UBA)
description Some comments are made on calculations with the generalized semimicroscopic model and a deformed configuration mixing shell model in the light of results obtained with a cluster-phonon model. Although the models yield a fairly good description of experimental data, a manifest discrepancy exists with these on the B(E2; 312→g.s.) values predicted by the generalized semimicroscopic and cluster-phonon models. There is also a difference in expected values for the nuclear deformation. NUCLEAR STRUCTURE Cr51; calculated levels, J, π, B(E2), B(M1), q, μ, S, b, τ. Cluster-phonon model; particle-hole excitations. © 1983 The American Physical Society.
title Structure of Cr51
spellingShingle Structure of Cr51
title_short Structure of Cr51
title_full Structure of Cr51
title_fullStr Structure of Cr51
title_full_unstemmed Structure of Cr51
title_sort structure of cr51
publishDate 1983
url https://bibliotecadigital.exactas.uba.ar/collection/paper/document/paper_05562813_v28_n4_p1843_Heras
http://hdl.handle.net/20.500.12110/paper_05562813_v28_n4_p1843_Heras
_version_ 1768543471973433344

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