A [SU(6)]4xZ_4 flavor model without mirror fermions

ABSTRACT: We introduce a three family extension of the Pati-Salam model which is anomaly free and contains in a single irreducible representation the known quarks and leptons without mirror fermions. Assuming that the breaking of the symmetry admits the implementation of the survival hypothesis, we...

Full description

Autores:
Ponce Gutiérrez, William Antonio
Zepeda, Arnulfo
Tipo de recurso:
Article of investigation
Fecha de publicación:
1994
Institución:
Universidad de Antioquia
Repositorio:
Repositorio UdeA
Idioma:
eng
OAI Identifier:
oai:bibliotecadigital.udea.edu.co:10495/43387
Acceso en línea:
https://hdl.handle.net/10495/43387
Palabra clave:
Simetría interrumpida (física)
Broken symmetry (Physics)
Grupo de renormalización
Renormalization group
Quarks
Leptones (física nuclear)
Leptons (nuclear physics)
Campos de calibración (física)
Gauge fields (physics)
Teoría de los grupos
Groups, Theory of
Fermiones
Fermions
Espectrometría de masas
Mass spectrometry
http://id.loc.gov/authorities/subjects/sh85017032
http://id.loc.gov/authorities/subjects/sh85112866
Rights
openAccess
License
http://creativecommons.org/licenses/by-nc-nd/2.5/co/
id UDEA2_6ddff3bb81f91eec8653b1ccbfc7c962
oai_identifier_str oai:bibliotecadigital.udea.edu.co:10495/43387
network_acronym_str UDEA2
network_name_str Repositorio UdeA
repository_id_str
dc.title.spa.fl_str_mv A [SU(6)]4xZ_4 flavor model without mirror fermions
title A [SU(6)]4xZ_4 flavor model without mirror fermions
spellingShingle A [SU(6)]4xZ_4 flavor model without mirror fermions
Simetría interrumpida (física)
Broken symmetry (Physics)
Grupo de renormalización
Renormalization group
Quarks
Leptones (física nuclear)
Leptons (nuclear physics)
Campos de calibración (física)
Gauge fields (physics)
Teoría de los grupos
Groups, Theory of
Fermiones
Fermions
Espectrometría de masas
Mass spectrometry
http://id.loc.gov/authorities/subjects/sh85017032
http://id.loc.gov/authorities/subjects/sh85112866
title_short A [SU(6)]4xZ_4 flavor model without mirror fermions
title_full A [SU(6)]4xZ_4 flavor model without mirror fermions
title_fullStr A [SU(6)]4xZ_4 flavor model without mirror fermions
title_full_unstemmed A [SU(6)]4xZ_4 flavor model without mirror fermions
title_sort A [SU(6)]4xZ_4 flavor model without mirror fermions
dc.creator.fl_str_mv Ponce Gutiérrez, William Antonio
Zepeda, Arnulfo
dc.contributor.author.none.fl_str_mv Ponce Gutiérrez, William Antonio
Zepeda, Arnulfo
dc.contributor.researchgroup.spa.fl_str_mv Grupo de Fenomenología de Interacciones Fundamentales
dc.subject.lcsh.none.fl_str_mv Simetría interrumpida (física)
Broken symmetry (Physics)
Grupo de renormalización
Renormalization group
topic Simetría interrumpida (física)
Broken symmetry (Physics)
Grupo de renormalización
Renormalization group
Quarks
Leptones (física nuclear)
Leptons (nuclear physics)
Campos de calibración (física)
Gauge fields (physics)
Teoría de los grupos
Groups, Theory of
Fermiones
Fermions
Espectrometría de masas
Mass spectrometry
http://id.loc.gov/authorities/subjects/sh85017032
http://id.loc.gov/authorities/subjects/sh85112866
dc.subject.lemb.none.fl_str_mv Quarks
Leptones (física nuclear)
Leptons (nuclear physics)
Campos de calibración (física)
Gauge fields (physics)
Teoría de los grupos
Groups, Theory of
Fermiones
Fermions
Espectrometría de masas
Mass spectrometry
dc.subject.lcshuri.none.fl_str_mv http://id.loc.gov/authorities/subjects/sh85017032
http://id.loc.gov/authorities/subjects/sh85112866
description ABSTRACT: We introduce a three family extension of the Pati-Salam model which is anomaly free and contains in a single irreducible representation the known quarks and leptons without mirror fermions. Assuming that the breaking of the symmetry admits the implementation of the survival hypothesis, we calculate the mass scales using the renormalization group equation. Finally we show that the proton remains perturbatively stable.
publishDate 1994
dc.date.issued.none.fl_str_mv 1994
dc.date.accessioned.none.fl_str_mv 2024-11-11T21:00:49Z
dc.date.available.none.fl_str_mv 2024-11-11T21:00:49Z
dc.type.spa.fl_str_mv Artículo de investigación
dc.type.coar.spa.fl_str_mv http://purl.org/coar/resource_type/c_2df8fbb1
dc.type.redcol.spa.fl_str_mv https://purl.org/redcol/resource_type/ART
dc.type.coarversion.spa.fl_str_mv http://purl.org/coar/version/c_970fb48d4fbd8a85
dc.type.driver.spa.fl_str_mv info:eu-repo/semantics/article
dc.type.version.spa.fl_str_mv info:eu-repo/semantics/publishedVersion
format http://purl.org/coar/resource_type/c_2df8fbb1
status_str publishedVersion
dc.identifier.issn.none.fl_str_mv 0143-0807
dc.identifier.uri.none.fl_str_mv https://hdl.handle.net/10495/43387
dc.identifier.doi.none.fl_str_mv 10.1007/BF01411026
dc.identifier.eissn.none.fl_str_mv 1361-6404
identifier_str_mv 0143-0807
10.1007/BF01411026
1361-6404
url https://hdl.handle.net/10495/43387
dc.language.iso.spa.fl_str_mv eng
language eng
dc.relation.ispartofjournalabbrev.spa.fl_str_mv Eur. J. Phys.
dc.relation.citationendpage.spa.fl_str_mv 13
dc.relation.citationstartpage.spa.fl_str_mv 1
dc.relation.citationvolume.spa.fl_str_mv 63
dc.relation.ispartofjournal.spa.fl_str_mv European Journal of Physics
dc.rights.uri.*.fl_str_mv http://creativecommons.org/licenses/by-nc-nd/2.5/co/
dc.rights.uri.spa.fl_str_mv https://creativecommons.org/licenses/by-nc-nd/4.0/
dc.rights.accessrights.spa.fl_str_mv info:eu-repo/semantics/openAccess
dc.rights.coar.spa.fl_str_mv http://purl.org/coar/access_right/c_abf2
rights_invalid_str_mv http://creativecommons.org/licenses/by-nc-nd/2.5/co/
https://creativecommons.org/licenses/by-nc-nd/4.0/
http://purl.org/coar/access_right/c_abf2
eu_rights_str_mv openAccess
dc.format.extent.spa.fl_str_mv 13 páginas
dc.format.mimetype.spa.fl_str_mv application/pdf
dc.publisher.spa.fl_str_mv IOP Publishing
European Physical Society
dc.publisher.place.spa.fl_str_mv Londres, Inglaterra
institution Universidad de Antioquia
bitstream.url.fl_str_mv https://bibliotecadigital.udea.edu.co/bitstreams/a323c9d1-70d4-42ed-8b5d-e5f0952cb626/download
https://bibliotecadigital.udea.edu.co/bitstreams/f1e0936c-760a-4a63-82a8-424b34a6bbd6/download
https://bibliotecadigital.udea.edu.co/bitstreams/bdc8b42d-95b3-4c43-b3cf-8044f93a2a30/download
https://bibliotecadigital.udea.edu.co/bitstreams/e6ae0f83-2a0d-4a44-af69-3cf018d2f1a9/download
https://bibliotecadigital.udea.edu.co/bitstreams/3884fed2-4b3b-4545-a545-fd85ecc756db/download
bitstream.checksum.fl_str_mv 839f1fb695e4e37ad26ca3dc0b756598
b88b088d9957e670ce3b3fbe2eedbc13
8a4605be74aa9ea9d79846c1fba20a33
be0a21b6b07095a4a54b20cf367ed12d
2596abb2862726f323a064d3818bc81a
bitstream.checksumAlgorithm.fl_str_mv MD5
MD5
MD5
MD5
MD5
repository.name.fl_str_mv Repositorio Institucional de la Universidad de Antioquia
repository.mail.fl_str_mv aplicacionbibliotecadigitalbiblioteca@udea.edu.co
_version_ 1851052122765787136
spelling Ponce Gutiérrez, William AntonioZepeda, ArnulfoGrupo de Fenomenología de Interacciones Fundamentales2024-11-11T21:00:49Z2024-11-11T21:00:49Z19940143-0807https://hdl.handle.net/10495/4338710.1007/BF014110261361-6404ABSTRACT: We introduce a three family extension of the Pati-Salam model which is anomaly free and contains in a single irreducible representation the known quarks and leptons without mirror fermions. Assuming that the breaking of the symmetry admits the implementation of the survival hypothesis, we calculate the mass scales using the renormalization group equation. Finally we show that the proton remains perturbatively stable.Banco de la República ColombiaConsejo Nacional de Humanidades, Ciencias y TecnologíasCOL000842313 páginasapplication/pdfengIOP PublishingEuropean Physical SocietyLondres, Inglaterrahttp://creativecommons.org/licenses/by-nc-nd/2.5/co/https://creativecommons.org/licenses/by-nc-nd/4.0/info:eu-repo/semantics/openAccesshttp://purl.org/coar/access_right/c_abf2Simetría interrumpida (física)Broken symmetry (Physics)Grupo de renormalizaciónRenormalization groupQuarksLeptones (física nuclear)Leptons (nuclear physics)Campos de calibración (física)Gauge fields (physics)Teoría de los gruposGroups, Theory ofFermionesFermionsEspectrometría de masasMass spectrometryhttp://id.loc.gov/authorities/subjects/sh85017032http://id.loc.gov/authorities/subjects/sh85112866A [SU(6)]4xZ_4 flavor model without mirror fermionsArtículo de investigaciónhttp://purl.org/coar/resource_type/c_2df8fbb1https://purl.org/redcol/resource_type/ARThttp://purl.org/coar/version/c_970fb48d4fbd8a85info:eu-repo/semantics/articleinfo:eu-repo/semantics/publishedVersionEur. J. Phys.13163European Journal of PhysicsRoR:01shra089RoR:059ex5q34PublicationORIGINALPonceWilliam_1994_FlavorModel.pdfPonceWilliam_1994_FlavorModel.pdfArtículo de investigaciónapplication/pdf120592https://bibliotecadigital.udea.edu.co/bitstreams/a323c9d1-70d4-42ed-8b5d-e5f0952cb626/download839f1fb695e4e37ad26ca3dc0b756598MD51trueAnonymousREADCC-LICENSElicense_rdflicense_rdfapplication/rdf+xml; charset=utf-8823https://bibliotecadigital.udea.edu.co/bitstreams/f1e0936c-760a-4a63-82a8-424b34a6bbd6/downloadb88b088d9957e670ce3b3fbe2eedbc13MD52falseAnonymousREADLICENSElicense.txtlicense.txttext/plain; charset=utf-81748https://bibliotecadigital.udea.edu.co/bitstreams/bdc8b42d-95b3-4c43-b3cf-8044f93a2a30/download8a4605be74aa9ea9d79846c1fba20a33MD53falseAnonymousREADTEXTPonceWilliam_1994_FlavorModel.pdf.txtPonceWilliam_1994_FlavorModel.pdf.txtExtracted texttext/plain25566https://bibliotecadigital.udea.edu.co/bitstreams/e6ae0f83-2a0d-4a44-af69-3cf018d2f1a9/downloadbe0a21b6b07095a4a54b20cf367ed12dMD58falseAnonymousREADTHUMBNAILPonceWilliam_1994_FlavorModel.pdf.jpgPonceWilliam_1994_FlavorModel.pdf.jpgGenerated Thumbnailimage/jpeg7100https://bibliotecadigital.udea.edu.co/bitstreams/3884fed2-4b3b-4545-a545-fd85ecc756db/download2596abb2862726f323a064d3818bc81aMD59falseAnonymousREAD10495/43387oai:bibliotecadigital.udea.edu.co:10495/433872025-03-26 17:18:46.003http://creativecommons.org/licenses/by-nc-nd/2.5/co/open.accesshttps://bibliotecadigital.udea.edu.coRepositorio Institucional de la Universidad de Antioquiaaplicacionbibliotecadigitalbiblioteca@udea.edu.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