QRAP: A numerical code for projected (Q)uasiparticle (RA)ndom (P)hase approximation

Autores
Samana, Arturo Rodolfo; Krmpotić, Francisco; Bertulani, C. A.
Año de publicación
2010
Idioma
inglés
Tipo de recurso
artículo
Estado
versión publicada
Descripción
A computer code for quasiparticle random phase approximation – QRPA and projected quasiparticle random phase approximation – PQRPA models of nuclear structure is explained in details. The residual interaction is approximated by a simple δ -force. An important application of the code consists in evaluating nuclear matrix elements involved in neutrino–nucleus reactions. As an example, cross sections for 56 Fe and 12 C are calculated and the code output is explained. The application to other nuclei and the description of other nuclear and weak decay processes are also discussed.
Program summary Title of program: QRAP ( Q uasiparticle RA ndom P hase approximation) Computers: The code has been created on a PC, but also runs on UNIX or LINUX machines Operating systems: WINDOWS or UNIX Program language used: Fortran-77 Memory required to execute with typical data: 16 Mbytes of RAM memory and 2 MB of hard disk space No. of lines in distributed program, including test data, etc.: ∼ 8000 No. of bytes in distributed program, including test data, etc.: ∼ 256 kB Distribution format: tar.gz Nature of physical problem: The program calculates neutrino– and antineutrino–nucleus cross sections as a function of the incident neutrino energy, and muon capture rates, using the QRPA or PQRPA as nuclear structure models. Method of solution: The QRPA, or PQRPA, equations are solved in a self-consistent way for even–even nuclei. The nuclear matrix elements for the neutrino–nucleus interaction are treated as the beta inverse reaction of odd–odd nuclei as function of the transfer momentum. Typical running time: ≈ 5 min on a 3 GHz processor for Data set 1.
Instituto de Física La Plata
Materia
Física
QRPA
QRPA Projected
Semileptonic processes
Nivel de accesibilidad
acceso abierto
Condiciones de uso
http://creativecommons.org/licenses/by/4.0/
Repositorio
SEDICI (UNLP)
Institución
Universidad Nacional de La Plata
OAI Identificador
oai:sedici.unlp.edu.ar:10915/130594

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oai_identifier_str oai:sedici.unlp.edu.ar:10915/130594
network_acronym_str SEDICI
repository_id_str 1329
network_name_str SEDICI (UNLP)
spelling QRAP: A numerical code for projected (Q)uasiparticle (RA)ndom (P)hase approximationSamana, Arturo RodolfoKrmpotić, FranciscoBertulani, C. A.FísicaQRPAQRPA ProjectedSemileptonic processesA computer code for quasiparticle random phase approximation – QRPA and projected quasiparticle random phase approximation – PQRPA models of nuclear structure is explained in details. The residual interaction is approximated by a simple δ -force. An important application of the code consists in evaluating nuclear matrix elements involved in neutrino–nucleus reactions. As an example, cross sections for 56 Fe and 12 C are calculated and the code output is explained. The application to other nuclei and the description of other nuclear and weak decay processes are also discussed.Program summary Title of program: QRAP ( Q uasiparticle RA ndom P hase approximation) Computers: The code has been created on a PC, but also runs on UNIX or LINUX machines Operating systems: WINDOWS or UNIX Program language used: Fortran-77 Memory required to execute with typical data: 16 Mbytes of RAM memory and 2 MB of hard disk space No. of lines in distributed program, including test data, etc.: ∼ 8000 No. of bytes in distributed program, including test data, etc.: ∼ 256 kB Distribution format: tar.gz Nature of physical problem: The program calculates neutrino– and antineutrino–nucleus cross sections as a function of the incident neutrino energy, and muon capture rates, using the QRPA or PQRPA as nuclear structure models. Method of solution: The QRPA, or PQRPA, equations are solved in a self-consistent way for even–even nuclei. The nuclear matrix elements for the neutrino–nucleus interaction are treated as the beta inverse reaction of odd–odd nuclei as function of the transfer momentum. Typical running time: ≈ 5 min on a 3 GHz processor for Data set 1.Instituto de Física La Plata2010info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionArticulohttp://purl.org/coar/resource_type/c_6501info:ar-repo/semantics/articuloapplication/pdf1123-1135http://sedici.unlp.edu.ar/handle/10915/130594enginfo:eu-repo/semantics/altIdentifier/issn/0010-4655info:eu-repo/semantics/altIdentifier/arxiv/0906.4301info:eu-repo/semantics/altIdentifier/doi/10.1016/j.cpc.2010.02.003info:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by/4.0/Creative Commons Attribution 4.0 International (CC BY 4.0)reponame:SEDICI (UNLP)instname:Universidad Nacional de La Platainstacron:UNLP2025-10-22T17:12:11Zoai:sedici.unlp.edu.ar:10915/130594Institucionalhttp://sedici.unlp.edu.ar/Universidad públicaNo correspondehttp://sedici.unlp.edu.ar/oai/snrdalira@sedici.unlp.edu.arArgentinaNo correspondeNo correspondeNo correspondeopendoar:13292025-10-22 17:12:11.901SEDICI (UNLP) - Universidad Nacional de La Platafalse
dc.title.none.fl_str_mv QRAP: A numerical code for projected (Q)uasiparticle (RA)ndom (P)hase approximation
title QRAP: A numerical code for projected (Q)uasiparticle (RA)ndom (P)hase approximation
spellingShingle QRAP: A numerical code for projected (Q)uasiparticle (RA)ndom (P)hase approximation
Samana, Arturo Rodolfo
Física
QRPA
QRPA Projected
Semileptonic processes
title_short QRAP: A numerical code for projected (Q)uasiparticle (RA)ndom (P)hase approximation
title_full QRAP: A numerical code for projected (Q)uasiparticle (RA)ndom (P)hase approximation
title_fullStr QRAP: A numerical code for projected (Q)uasiparticle (RA)ndom (P)hase approximation
title_full_unstemmed QRAP: A numerical code for projected (Q)uasiparticle (RA)ndom (P)hase approximation
title_sort QRAP: A numerical code for projected (Q)uasiparticle (RA)ndom (P)hase approximation
dc.creator.none.fl_str_mv Samana, Arturo Rodolfo
Krmpotić, Francisco
Bertulani, C. A.
author Samana, Arturo Rodolfo
author_facet Samana, Arturo Rodolfo
Krmpotić, Francisco
Bertulani, C. A.
author_role author
author2 Krmpotić, Francisco
Bertulani, C. A.
author2_role author
author
dc.subject.none.fl_str_mv Física
QRPA
QRPA Projected
Semileptonic processes
topic Física
QRPA
QRPA Projected
Semileptonic processes
dc.description.none.fl_txt_mv A computer code for quasiparticle random phase approximation – QRPA and projected quasiparticle random phase approximation – PQRPA models of nuclear structure is explained in details. The residual interaction is approximated by a simple δ -force. An important application of the code consists in evaluating nuclear matrix elements involved in neutrino–nucleus reactions. As an example, cross sections for 56 Fe and 12 C are calculated and the code output is explained. The application to other nuclei and the description of other nuclear and weak decay processes are also discussed.
Program summary Title of program: QRAP ( Q uasiparticle RA ndom P hase approximation) Computers: The code has been created on a PC, but also runs on UNIX or LINUX machines Operating systems: WINDOWS or UNIX Program language used: Fortran-77 Memory required to execute with typical data: 16 Mbytes of RAM memory and 2 MB of hard disk space No. of lines in distributed program, including test data, etc.: ∼ 8000 No. of bytes in distributed program, including test data, etc.: ∼ 256 kB Distribution format: tar.gz Nature of physical problem: The program calculates neutrino– and antineutrino–nucleus cross sections as a function of the incident neutrino energy, and muon capture rates, using the QRPA or PQRPA as nuclear structure models. Method of solution: The QRPA, or PQRPA, equations are solved in a self-consistent way for even–even nuclei. The nuclear matrix elements for the neutrino–nucleus interaction are treated as the beta inverse reaction of odd–odd nuclei as function of the transfer momentum. Typical running time: ≈ 5 min on a 3 GHz processor for Data set 1.
Instituto de Física La Plata
description A computer code for quasiparticle random phase approximation – QRPA and projected quasiparticle random phase approximation – PQRPA models of nuclear structure is explained in details. The residual interaction is approximated by a simple δ -force. An important application of the code consists in evaluating nuclear matrix elements involved in neutrino–nucleus reactions. As an example, cross sections for 56 Fe and 12 C are calculated and the code output is explained. The application to other nuclei and the description of other nuclear and weak decay processes are also discussed.
publishDate 2010
dc.date.none.fl_str_mv 2010
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/10915/130594
url http://sedici.unlp.edu.ar/handle/10915/130594
dc.language.none.fl_str_mv eng
language eng
dc.relation.none.fl_str_mv info:eu-repo/semantics/altIdentifier/issn/0010-4655
info:eu-repo/semantics/altIdentifier/arxiv/0906.4301
info:eu-repo/semantics/altIdentifier/doi/10.1016/j.cpc.2010.02.003
dc.rights.none.fl_str_mv info:eu-repo/semantics/openAccess
http://creativecommons.org/licenses/by/4.0/
Creative Commons Attribution 4.0 International (CC BY 4.0)
eu_rights_str_mv openAccess
rights_invalid_str_mv http://creativecommons.org/licenses/by/4.0/
Creative Commons Attribution 4.0 International (CC BY 4.0)
dc.format.none.fl_str_mv application/pdf
1123-1135
dc.source.none.fl_str_mv reponame:SEDICI (UNLP)
instname:Universidad Nacional de La Plata
instacron:UNLP
reponame_str SEDICI (UNLP)
collection SEDICI (UNLP)
instname_str Universidad Nacional de La Plata
instacron_str UNLP
institution UNLP
repository.name.fl_str_mv SEDICI (UNLP) - Universidad Nacional de La Plata
repository.mail.fl_str_mv alira@sedici.unlp.edu.ar
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