Fundamental fermion masses from deformed SUq(2) triplets
Autor(a) principal: | |
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Data de Publicação: | 1997 |
Outros Autores: | |
Tipo de documento: | Artigo |
Idioma: | eng |
Título da fonte: | Repositório Institucional da UNESP |
Texto Completo: | http://hdl.handle.net/11449/224332 |
Resumo: | A spectrum-generating q-algebra, within the framework of SUq(2), as firstly suggested by Iachello, is studied in order to describe the mass spectrum of three generations of quarks and leptons. The SUq(2) quantum group is a q-deformed extension of SU(2), where q = ea (with α real) is the deformation parameter. In this work, the essential use of inequivalent representations of SUq(2) is introduced. The inequivalent representations are labelled by (j, v0), where j = 0, 1/2, 1, ... and v0 is a positive real number. A formula for the fermion masses Mm(j, v0), with -j ≤ m ≤ j is derived. As an example, a possible scheme which corresponds to two triplets (j = 1) associated to up and down quarks is presented here in some detail. They are associated to different values of the deformation parameter, indicating a dependence of the charge Q on the parameter α. The masses of the charged leptons are treated in a similar way. The current results show that some mass relations for quarks and leptons found in the literature can be considered as approximations of the equations obtained in the j = 1 representations. The breaking of SUq(2) necessary to describe the Cabibbo-Kobayashi-Maskawa (CKM) flavor mixing is briefly discussed. |
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Fundamental fermion masses from deformed SUq(2) tripletsA spectrum-generating q-algebra, within the framework of SUq(2), as firstly suggested by Iachello, is studied in order to describe the mass spectrum of three generations of quarks and leptons. The SUq(2) quantum group is a q-deformed extension of SU(2), where q = ea (with α real) is the deformation parameter. In this work, the essential use of inequivalent representations of SUq(2) is introduced. The inequivalent representations are labelled by (j, v0), where j = 0, 1/2, 1, ... and v0 is a positive real number. A formula for the fermion masses Mm(j, v0), with -j ≤ m ≤ j is derived. As an example, a possible scheme which corresponds to two triplets (j = 1) associated to up and down quarks is presented here in some detail. They are associated to different values of the deformation parameter, indicating a dependence of the charge Q on the parameter α. The masses of the charged leptons are treated in a similar way. The current results show that some mass relations for quarks and leptons found in the literature can be considered as approximations of the equations obtained in the j = 1 representations. The breaking of SUq(2) necessary to describe the Cabibbo-Kobayashi-Maskawa (CKM) flavor mixing is briefly discussed.Inst. de Fis. Teórica Universidade Estadual Paulista, Rua Pamplona 145, 01405-900 São Paulo, SPInst. de Fis. Teórica Universidade Estadual Paulista, Rua Pamplona 145, 01405-900 São Paulo, SPUniversidade Estadual Paulista (UNESP)Palladino, B. E. [UNESP]Ferreira, P. Leal [UNESP]2022-04-28T19:55:58Z2022-04-28T19:55:58Z1997-03-01info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/article303-314Nuovo Cimento della Societa Italiana di Fisica A, v. 110, n. 3, p. 303-314, 1997.0369-3546http://hdl.handle.net/11449/2243322-s2.0-0040600464Scopusreponame:Repositório Institucional da UNESPinstname:Universidade Estadual Paulista (UNESP)instacron:UNESPengNuovo Cimento della Societa Italiana di Fisica Ainfo:eu-repo/semantics/openAccess2022-04-28T19:55:58Zoai:repositorio.unesp.br:11449/224332Repositório InstitucionalPUBhttp://repositorio.unesp.br/oai/requestopendoar:29462024-08-05T17:01:44.430164Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP)false |
dc.title.none.fl_str_mv |
Fundamental fermion masses from deformed SUq(2) triplets |
title |
Fundamental fermion masses from deformed SUq(2) triplets |
spellingShingle |
Fundamental fermion masses from deformed SUq(2) triplets Palladino, B. E. [UNESP] |
title_short |
Fundamental fermion masses from deformed SUq(2) triplets |
title_full |
Fundamental fermion masses from deformed SUq(2) triplets |
title_fullStr |
Fundamental fermion masses from deformed SUq(2) triplets |
title_full_unstemmed |
Fundamental fermion masses from deformed SUq(2) triplets |
title_sort |
Fundamental fermion masses from deformed SUq(2) triplets |
author |
Palladino, B. E. [UNESP] |
author_facet |
Palladino, B. E. [UNESP] Ferreira, P. Leal [UNESP] |
author_role |
author |
author2 |
Ferreira, P. Leal [UNESP] |
author2_role |
author |
dc.contributor.none.fl_str_mv |
Universidade Estadual Paulista (UNESP) |
dc.contributor.author.fl_str_mv |
Palladino, B. E. [UNESP] Ferreira, P. Leal [UNESP] |
description |
A spectrum-generating q-algebra, within the framework of SUq(2), as firstly suggested by Iachello, is studied in order to describe the mass spectrum of three generations of quarks and leptons. The SUq(2) quantum group is a q-deformed extension of SU(2), where q = ea (with α real) is the deformation parameter. In this work, the essential use of inequivalent representations of SUq(2) is introduced. The inequivalent representations are labelled by (j, v0), where j = 0, 1/2, 1, ... and v0 is a positive real number. A formula for the fermion masses Mm(j, v0), with -j ≤ m ≤ j is derived. As an example, a possible scheme which corresponds to two triplets (j = 1) associated to up and down quarks is presented here in some detail. They are associated to different values of the deformation parameter, indicating a dependence of the charge Q on the parameter α. The masses of the charged leptons are treated in a similar way. The current results show that some mass relations for quarks and leptons found in the literature can be considered as approximations of the equations obtained in the j = 1 representations. The breaking of SUq(2) necessary to describe the Cabibbo-Kobayashi-Maskawa (CKM) flavor mixing is briefly discussed. |
publishDate |
1997 |
dc.date.none.fl_str_mv |
1997-03-01 2022-04-28T19:55:58Z 2022-04-28T19:55:58Z |
dc.type.status.fl_str_mv |
info:eu-repo/semantics/publishedVersion |
dc.type.driver.fl_str_mv |
info:eu-repo/semantics/article |
format |
article |
status_str |
publishedVersion |
dc.identifier.uri.fl_str_mv |
Nuovo Cimento della Societa Italiana di Fisica A, v. 110, n. 3, p. 303-314, 1997. 0369-3546 http://hdl.handle.net/11449/224332 2-s2.0-0040600464 |
identifier_str_mv |
Nuovo Cimento della Societa Italiana di Fisica A, v. 110, n. 3, p. 303-314, 1997. 0369-3546 2-s2.0-0040600464 |
url |
http://hdl.handle.net/11449/224332 |
dc.language.iso.fl_str_mv |
eng |
language |
eng |
dc.relation.none.fl_str_mv |
Nuovo Cimento della Societa Italiana di Fisica A |
dc.rights.driver.fl_str_mv |
info:eu-repo/semantics/openAccess |
eu_rights_str_mv |
openAccess |
dc.format.none.fl_str_mv |
303-314 |
dc.source.none.fl_str_mv |
Scopus reponame:Repositório Institucional da UNESP instname:Universidade Estadual Paulista (UNESP) instacron:UNESP |
instname_str |
Universidade Estadual Paulista (UNESP) |
instacron_str |
UNESP |
institution |
UNESP |
reponame_str |
Repositório Institucional da UNESP |
collection |
Repositório Institucional da UNESP |
repository.name.fl_str_mv |
Repositório Institucional da UNESP - Universidade Estadual Paulista (UNESP) |
repository.mail.fl_str_mv |
|
_version_ |
1808128741860179968 |