Neutrino masses in SU(5) X U(1)F with adjoint flavons

ABSTRACT: We present a SU(5) x U(1)F supersymmetric model for neutrino masses and mixings that implements the seesaw mechanism by means of the heavy SU(2) singlets and triplets states contained in three adjoints of SU(5). We discuss how Abelian U(1)F symmetries can naturally yield non-hierarchical l...

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Autores:
Nardi, Enrico
Restrepo Quintero, Diego Alejandro
Velásquez López, Mauricio de Jesús
Tipo de recurso:
Article of investigation
Fecha de publicación:
2012
Institución:
Universidad de Antioquia
Repositorio:
Repositorio UdeA
Idioma:
eng
OAI Identifier:
oai:bibliotecadigital.udea.edu.co:10495/8628
Acceso en línea:
http://hdl.handle.net/10495/8628
Palabra clave:
Neutrinos
Flavones
Masa (Física)
Mass (physics)
Rights
openAccess
License
Atribución-NoComercial-SinDerivadas 2.5 Colombia
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dc.title.spa.fl_str_mv Neutrino masses in SU(5) X U(1)F with adjoint flavons
title Neutrino masses in SU(5) X U(1)F with adjoint flavons
spellingShingle Neutrino masses in SU(5) X U(1)F with adjoint flavons
Neutrinos
Flavones
Masa (Física)
Mass (physics)
title_short Neutrino masses in SU(5) X U(1)F with adjoint flavons
title_full Neutrino masses in SU(5) X U(1)F with adjoint flavons
title_fullStr Neutrino masses in SU(5) X U(1)F with adjoint flavons
title_full_unstemmed Neutrino masses in SU(5) X U(1)F with adjoint flavons
title_sort Neutrino masses in SU(5) X U(1)F with adjoint flavons
dc.creator.fl_str_mv Nardi, Enrico
Restrepo Quintero, Diego Alejandro
Velásquez López, Mauricio de Jesús
dc.contributor.author.none.fl_str_mv Nardi, Enrico
Restrepo Quintero, Diego Alejandro
Velásquez López, Mauricio de Jesús
dc.subject.none.fl_str_mv Neutrinos
Flavones
Masa (Física)
Mass (physics)
topic Neutrinos
Flavones
Masa (Física)
Mass (physics)
description ABSTRACT: We present a SU(5) x U(1)F supersymmetric model for neutrino masses and mixings that implements the seesaw mechanism by means of the heavy SU(2) singlets and triplets states contained in three adjoints of SU(5). We discuss how Abelian U(1)F symmetries can naturally yield non-hierarchical light neutrinos even when the heavy states are strongly hierarchical, and how it can also ensure that R{parity arises as an exact accidental symmetry. By assigning two flavons that break U(1)F to the adjoint representation of SU(5) and assuming universality for all the fundamental couplings, the coe cients of the e ective Yukawa and Majorana mass operators become calculable in terms of group theoretical quantities. There is a single free parameter in the model, however, at leading order the structure of the light neutrinos mass matrix is determined in a parameter independent way.
publishDate 2012
dc.date.issued.none.fl_str_mv 2012
dc.date.accessioned.none.fl_str_mv 2017-10-24T13:30:46Z
dc.date.available.none.fl_str_mv 2017-10-24T13:30:46Z
dc.type.spa.fl_str_mv info:eu-repo/semantics/article
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dc.identifier.citation.spa.fl_str_mv Nardi, E., Restrepo Quintero, D. A., & Velásquez López, M. de J. (2012). Neutrino masses in SU(5) X U(1)F with adjoint flavons. European Physical Journal C. 72(1941), 1-9. DOI:10.1140/epjc/s10052-012-1941-1
dc.identifier.issn.none.fl_str_mv 1434-6052
dc.identifier.uri.none.fl_str_mv http://hdl.handle.net/10495/8628
dc.identifier.doi.none.fl_str_mv 14346044
10.1140/epjc/s1005201219411
identifier_str_mv Nardi, E., Restrepo Quintero, D. A., & Velásquez López, M. de J. (2012). Neutrino masses in SU(5) X U(1)F with adjoint flavons. European Physical Journal C. 72(1941), 1-9. DOI:10.1140/epjc/s10052-012-1941-1
1434-6052
14346044
10.1140/epjc/s1005201219411
url http://hdl.handle.net/10495/8628
dc.language.iso.spa.fl_str_mv eng
language eng
dc.relation.ispartofjournalabbrev.spa.fl_str_mv EUR. Phys. J. C,
dc.rights.*.fl_str_mv Atribución-NoComercial-SinDerivadas 2.5 Colombia
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dc.publisher.spa.fl_str_mv Springer Verlag
dc.publisher.group.spa.fl_str_mv Grupo de Fenomenologia de Interacciones Fundamentales
dc.publisher.place.spa.fl_str_mv Alemania
institution Universidad de Antioquia
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spelling Nardi, EnricoRestrepo Quintero, Diego AlejandroVelásquez López, Mauricio de Jesús2017-10-24T13:30:46Z2017-10-24T13:30:46Z2012Nardi, E., Restrepo Quintero, D. A., & Velásquez López, M. de J. (2012). Neutrino masses in SU(5) X U(1)F with adjoint flavons. European Physical Journal C. 72(1941), 1-9. DOI:10.1140/epjc/s10052-012-1941-11434-6052http://hdl.handle.net/10495/86281434604410.1140/epjc/s1005201219411ABSTRACT: We present a SU(5) x U(1)F supersymmetric model for neutrino masses and mixings that implements the seesaw mechanism by means of the heavy SU(2) singlets and triplets states contained in three adjoints of SU(5). We discuss how Abelian U(1)F symmetries can naturally yield non-hierarchical light neutrinos even when the heavy states are strongly hierarchical, and how it can also ensure that R{parity arises as an exact accidental symmetry. By assigning two flavons that break U(1)F to the adjoint representation of SU(5) and assuming universality for all the fundamental couplings, the coe cients of the e ective Yukawa and Majorana mass operators become calculable in terms of group theoretical quantities. There is a single free parameter in the model, however, at leading order the structure of the light neutrinos mass matrix is determined in a parameter independent way.application/pdfengSpringer VerlagGrupo de Fenomenologia de Interacciones FundamentalesAlemaniainfo:eu-repo/semantics/articlehttp://purl.org/coar/resource_type/c_2df8fbb1https://purl.org/redcol/resource_type/ARTArtículo de investigaciónhttp://purl.org/coar/version/c_970fb48d4fbd8a85http://purl.org/coar/version/c_71e4c1898caa6e32Atribución-NoComercial-SinDerivadas 2.5 Colombiainfo:eu-repo/semantics/openAccesshttp://creativecommons.org/licenses/by-nc-nd/2.5/co/http://purl.org/coar/access_right/c_abf2https://creativecommons.org/licenses/by-nc-nd/4.0/NeutrinosFlavonesMasa (Física)Mass (physics)Neutrino masses in SU(5) X U(1)F with adjoint flavonsEUR. Phys. J. C,European Physical Journal C19721941ORIGINALRestrepoDiego_2011_NeutrinoMassesAdjoint.pdfRestrepoDiego_2011_NeutrinoMassesAdjoint.pdfArtículo de investigaciónapplication/pdf395623http://bibliotecadigital.udea.edu.co/bitstream/10495/8628/1/RestrepoDiego_2011_NeutrinoMassesAdjoint.pdfa4309872ca1c33ca6c69cd22b3631941MD51CC-LICENSElicense_urllicense_urltext/plain; charset=utf-849http://bibliotecadigital.udea.edu.co/bitstream/10495/8628/2/license_url4afdbb8c545fd630ea7db775da747b2fMD52license_textlicense_texttext/html; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/8628/3/license_textd41d8cd98f00b204e9800998ecf8427eMD53license_rdflicense_rdfapplication/rdf+xml; charset=utf-80http://bibliotecadigital.udea.edu.co/bitstream/10495/8628/4/license_rdfd41d8cd98f00b204e9800998ecf8427eMD54LICENSElicense.txtlicense.txttext/plain; charset=utf-81748http://bibliotecadigital.udea.edu.co/bitstream/10495/8628/5/license.txt8a4605be74aa9ea9d79846c1fba20a33MD5510495/8628oai:bibliotecadigital.udea.edu.co:10495/86282021-05-16 11:45:58.585Repositorio Institucional Universidad de Antioquiaandres.perez@udea.edu.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