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A Unified Description of Quark and Lepton Mass Matrices in a Universal Seesaw Model

In the democratic universal seesaw model, the mass matrices are given by \bar{f}_L m_L F_R + \bar{F}_L m_R f_R + \bar{F}_L M_F F_R (f: quarks and leptons; F: hypothetical heavy fermions), m_L and m_R are universal for up- and down-fermions, and M_F has a structure ({\bf 1}+ b_f X) (b_f is a flavour-...

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Detalles Bibliográficos
Autores principales: Koide, Y, Fusaoka, H
Lenguaje:eng
Publicado: 2002
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevD.66.113004
http://cds.cern.ch/record/581107
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author Koide, Y
Fusaoka, H
author_facet Koide, Y
Fusaoka, H
author_sort Koide, Y
collection CERN
description In the democratic universal seesaw model, the mass matrices are given by \bar{f}_L m_L F_R + \bar{F}_L m_R f_R + \bar{F}_L M_F F_R (f: quarks and leptons; F: hypothetical heavy fermions), m_L and m_R are universal for up- and down-fermions, and M_F has a structure ({\bf 1}+ b_f X) (b_f is a flavour-dependent parameter, and X is a democratic matrix). The model can successfully explain the quark masses and CKM mixing parameters in terms of the charged lepton masses by adjusting only one parameter, b_f. However, so far, the model has not been able to give the observed bimaximal mixing for the neutrino sector. In the present paper, we consider that M_F in the quark sectors are still "fully" democratic, while M_F in the lepton sectors are partially democratic. Then, the revised model can reasonably give a nearly bimaximal mixing without spoiling the previous success in the quark sectors.
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spelling cern-5811072019-09-30T06:29:59Zdoi:10.1103/PhysRevD.66.113004http://cds.cern.ch/record/581107engKoide, YFusaoka, HA Unified Description of Quark and Lepton Mass Matrices in a Universal Seesaw ModelParticle Physics - PhenomenologyIn the democratic universal seesaw model, the mass matrices are given by \bar{f}_L m_L F_R + \bar{F}_L m_R f_R + \bar{F}_L M_F F_R (f: quarks and leptons; F: hypothetical heavy fermions), m_L and m_R are universal for up- and down-fermions, and M_F has a structure ({\bf 1}+ b_f X) (b_f is a flavour-dependent parameter, and X is a democratic matrix). The model can successfully explain the quark masses and CKM mixing parameters in terms of the charged lepton masses by adjusting only one parameter, b_f. However, so far, the model has not been able to give the observed bimaximal mixing for the neutrino sector. In the present paper, we consider that M_F in the quark sectors are still "fully" democratic, while M_F in the lepton sectors are partially democratic. Then, the revised model can reasonably give a nearly bimaximal mixing without spoiling the previous success in the quark sectors.hep-ph/0209148AMU-2002-09CERN-TH-2002-236US-2002-09oai:cds.cern.ch:5811072002-09-13
spellingShingle Particle Physics - Phenomenology
Koide, Y
Fusaoka, H
A Unified Description of Quark and Lepton Mass Matrices in a Universal Seesaw Model
title A Unified Description of Quark and Lepton Mass Matrices in a Universal Seesaw Model
title_full A Unified Description of Quark and Lepton Mass Matrices in a Universal Seesaw Model
title_fullStr A Unified Description of Quark and Lepton Mass Matrices in a Universal Seesaw Model
title_full_unstemmed A Unified Description of Quark and Lepton Mass Matrices in a Universal Seesaw Model
title_short A Unified Description of Quark and Lepton Mass Matrices in a Universal Seesaw Model
title_sort unified description of quark and lepton mass matrices in a universal seesaw model
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1103/PhysRevD.66.113004
http://cds.cern.ch/record/581107
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