Collective vibrations and the nature of the intrinsic field

Autores
Hernández, E. S.; Plastino, Ángel Ricardo
Año de publicación
1974
Idioma
inglés
Tipo de recurso
artículo
Estado
versión publicada
Descripción
During the last years a considerable progress has been made concerning the description of nuclear properties by recourse to self-consistent methods. Of these, the HartreeFock-Bogolubov approach promises to be specially apt to describe many details of the nuclear structure (1). One can envisage that the quasi-particle random-phase approximation (QRPA), if used in conjuction with a self-consistent quasi-particle (q.p.) basis), will provide us with an extremely potent tool to deal with the microscopic aspects of collective vibrational states. Now, this kind of states manifest themselves in their most patent form in the so-called deformed heavy nuclei, i.e. transuranic and rareearth ones. Of course, due to the high single-particle (s.p.) level density found in this regions of the periodic table, one easily realizes that even the first stage of the description referred to above, i.e. the HFB one, consitutes a very serious numerical problem. However, some intents have already been made in this direction (see, for example, ref. (2)) and, with the rapid progress that the development of processing data systems is showing, it canot be doubted that steps towards the already mentioned goal will be undertaken in the near future.It must be borne in mind, however, that evaluating the matrix elements of the residual interactions between q.p. will surely prove to be a tremendous task, since one needs millions of them. The purpose of the present letter is to point out that this later job, i.e. the computation of the residual matrix elements (r.m.e.), may be unnecessary. We intend to show here that the information to be gained from the knowledge of this r.m.e. is not needed in order to describe the most important details concerning the microscopic structure of vibrational states in deformed heavy nuclei.
Facultad de Ciencias Exactas
Materia
Física
Residual matrix elements
Intrinsic Field
Nivel de accesibilidad
acceso abierto
Condiciones de uso
http://creativecommons.org/licenses/by-nc-sa/4.0/
Repositorio
SEDICI (UNLP)
Institución
Universidad Nacional de La Plata
OAI Identificador
oai:sedici.unlp.edu.ar:10915/134965

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spelling Collective vibrations and the nature of the intrinsic fieldHernández, E. S.Plastino, Ángel RicardoFísicaResidual matrix elementsIntrinsic FieldDuring the last years a considerable progress has been made concerning the description of nuclear properties by recourse to self-consistent methods. Of these, the HartreeFock-Bogolubov approach promises to be specially apt to describe many details of the nuclear structure (1). One can envisage that the quasi-particle random-phase approximation (QRPA), if used in conjuction with a self-consistent quasi-particle (q.p.) basis), will provide us with an extremely potent tool to deal with the microscopic aspects of collective vibrational states. Now, this kind of states manifest themselves in their most patent form in the so-called deformed heavy nuclei, i.e. transuranic and rareearth ones. Of course, due to the high single-particle (s.p.) level density found in this regions of the periodic table, one easily realizes that even the first stage of the description referred to above, i.e. the HFB one, consitutes a very serious numerical problem. However, some intents have already been made in this direction (see, for example, ref. (2)) and, with the rapid progress that the development of processing data systems is showing, it canot be doubted that steps towards the already mentioned goal will be undertaken in the near future.It must be borne in mind, however, that evaluating the matrix elements of the residual interactions between q.p. will surely prove to be a tremendous task, since one needs millions of them. The purpose of the present letter is to point out that this later job, i.e. the computation of the residual matrix elements (r.m.e.), may be unnecessary. We intend to show here that the information to be gained from the knowledge of this r.m.e. is not needed in order to describe the most important details concerning the microscopic structure of vibrational states in deformed heavy nuclei.Facultad de Ciencias Exactas1974info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionArticulohttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdf75-79http://sedici.unlp.edu.ar/handle/10915/134965enginfo:eu-repo/semantics/altIdentifier/issn/1827-613Xinfo:eu-repo/semantics/altIdentifier/issn/0375-930Xinfo:eu-repo/semantics/altIdentifier/doi/10.1007/bf02752732info: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:UNLP2025-09-29T11:32:37Zoai:sedici.unlp.edu.ar:10915/134965Institucionalhttp://sedici.unlp.edu.ar/Universidad públicaNo correspondehttp://sedici.unlp.edu.ar/oai/snrdalira@sedici.unlp.edu.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:13292025-09-29 11:32:37.968SEDICI (UNLP) - Universidad Nacional de La Platafalse
dc.title.none.fl_str_mv Collective vibrations and the nature of the intrinsic field
title Collective vibrations and the nature of the intrinsic field
spellingShingle Collective vibrations and the nature of the intrinsic field
Hernández, E. S.
Física
Residual matrix elements
Intrinsic Field
title_short Collective vibrations and the nature of the intrinsic field
title_full Collective vibrations and the nature of the intrinsic field
title_fullStr Collective vibrations and the nature of the intrinsic field
title_full_unstemmed Collective vibrations and the nature of the intrinsic field
title_sort Collective vibrations and the nature of the intrinsic field
dc.creator.none.fl_str_mv Hernández, E. S.
Plastino, Ángel Ricardo
author Hernández, E. S.
author_facet Hernández, E. S.
Plastino, Ángel Ricardo
author_role author
author2 Plastino, Ángel Ricardo
author2_role author
dc.subject.none.fl_str_mv Física
Residual matrix elements
Intrinsic Field
topic Física
Residual matrix elements
Intrinsic Field
dc.description.none.fl_txt_mv During the last years a considerable progress has been made concerning the description of nuclear properties by recourse to self-consistent methods. Of these, the HartreeFock-Bogolubov approach promises to be specially apt to describe many details of the nuclear structure (1). One can envisage that the quasi-particle random-phase approximation (QRPA), if used in conjuction with a self-consistent quasi-particle (q.p.) basis), will provide us with an extremely potent tool to deal with the microscopic aspects of collective vibrational states. Now, this kind of states manifest themselves in their most patent form in the so-called deformed heavy nuclei, i.e. transuranic and rareearth ones. Of course, due to the high single-particle (s.p.) level density found in this regions of the periodic table, one easily realizes that even the first stage of the description referred to above, i.e. the HFB one, consitutes a very serious numerical problem. However, some intents have already been made in this direction (see, for example, ref. (2)) and, with the rapid progress that the development of processing data systems is showing, it canot be doubted that steps towards the already mentioned goal will be undertaken in the near future.It must be borne in mind, however, that evaluating the matrix elements of the residual interactions between q.p. will surely prove to be a tremendous task, since one needs millions of them. The purpose of the present letter is to point out that this later job, i.e. the computation of the residual matrix elements (r.m.e.), may be unnecessary. We intend to show here that the information to be gained from the knowledge of this r.m.e. is not needed in order to describe the most important details concerning the microscopic structure of vibrational states in deformed heavy nuclei.
Facultad de Ciencias Exactas
description During the last years a considerable progress has been made concerning the description of nuclear properties by recourse to self-consistent methods. Of these, the HartreeFock-Bogolubov approach promises to be specially apt to describe many details of the nuclear structure (1). One can envisage that the quasi-particle random-phase approximation (QRPA), if used in conjuction with a self-consistent quasi-particle (q.p.) basis), will provide us with an extremely potent tool to deal with the microscopic aspects of collective vibrational states. Now, this kind of states manifest themselves in their most patent form in the so-called deformed heavy nuclei, i.e. transuranic and rareearth ones. Of course, due to the high single-particle (s.p.) level density found in this regions of the periodic table, one easily realizes that even the first stage of the description referred to above, i.e. the HFB one, consitutes a very serious numerical problem. However, some intents have already been made in this direction (see, for example, ref. (2)) and, with the rapid progress that the development of processing data systems is showing, it canot be doubted that steps towards the already mentioned goal will be undertaken in the near future.It must be borne in mind, however, that evaluating the matrix elements of the residual interactions between q.p. will surely prove to be a tremendous task, since one needs millions of them. The purpose of the present letter is to point out that this later job, i.e. the computation of the residual matrix elements (r.m.e.), may be unnecessary. We intend to show here that the information to be gained from the knowledge of this r.m.e. is not needed in order to describe the most important details concerning the microscopic structure of vibrational states in deformed heavy nuclei.
publishDate 1974
dc.date.none.fl_str_mv 1974
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