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Family symmetries in F-theory GUTs

We discuss F-theory SU(5) GUTs in which some or all of the quark and lepton families are assigned to different curves and family symmetry enforces a leading order rank one structure of the Yukawa matrices. We consider two possibilities for the suppression of baryon and lepton number violation. The f...

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Detalles Bibliográficos
Autores principales: King, S F, Leontaris, G K, Ross, G G
Formato: info:eu-repo/semantics/article
Lenguaje:eng
Publicado: Nucl. Phys. B 2010
Materias:
Acceso en línea:https://dx.doi.org/10.1016/j.nuclphysb.2010.05.014
http://cds.cern.ch/record/1264268
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author King, S F
Leontaris, G K
Ross, G G
author_facet King, S F
Leontaris, G K
Ross, G G
author_sort King, S F
collection CERN
description We discuss F-theory SU(5) GUTs in which some or all of the quark and lepton families are assigned to different curves and family symmetry enforces a leading order rank one structure of the Yukawa matrices. We consider two possibilities for the suppression of baryon and lepton number violation. The first is based on Flipped SU(5) with gauge group SU(5)\times U(1)_\chi \times SU(4)_{\perp} in which U(1)_{\chi} plays the role of a generalised matter parity. We present an example which, after imposing a Z_2 monodromy, has a U(1)_{\perp}^2 family symmetry. Even in the absence of flux, spontaneous breaking of the family symmetry leads to viable quark, charged lepton and neutrino masses and mixing. The second possibility has an R-parity associated with the symmetry of the underlying compactification manifold and the flux. We construct an example of a model with viable masses and mixing angles based on the gauge group SU(5)\times SU(5)_{\perp} with a U(1)_{\perp}^3 family symmetry after imposing a Z_2 monodromy.
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spelling cern-12642682019-09-30T06:29:59Z doi:10.1016/j.nuclphysb.2010.05.014 http://cds.cern.ch/record/1264268 eng King, S F Leontaris, G K Ross, G G Family symmetries in F-theory GUTs Particle Physics - Phenomenology We discuss F-theory SU(5) GUTs in which some or all of the quark and lepton families are assigned to different curves and family symmetry enforces a leading order rank one structure of the Yukawa matrices. We consider two possibilities for the suppression of baryon and lepton number violation. The first is based on Flipped SU(5) with gauge group SU(5)\times U(1)_\chi \times SU(4)_{\perp} in which U(1)_{\chi} plays the role of a generalised matter parity. We present an example which, after imposing a Z_2 monodromy, has a U(1)_{\perp}^2 family symmetry. Even in the absence of flux, spontaneous breaking of the family symmetry leads to viable quark, charged lepton and neutrino masses and mixing. The second possibility has an R-parity associated with the symmetry of the underlying compactification manifold and the flux. We construct an example of a model with viable masses and mixing angles based on the gauge group SU(5)\times SU(5)_{\perp} with a U(1)_{\perp}^3 family symmetry after imposing a Z_2 monodromy. info:eu-repo/grantAgreement/EC/FP7/237920 info:eu-repo/semantics/openAccess Education Level info:eu-repo/semantics/article http://cds.cern.ch/record/1264268 Nucl. Phys. B Nucl. Phys. B, (2010) pp. 119-135 2010-05-07
spellingShingle Particle Physics - Phenomenology
King, S F
Leontaris, G K
Ross, G G
Family symmetries in F-theory GUTs
title Family symmetries in F-theory GUTs
title_full Family symmetries in F-theory GUTs
title_fullStr Family symmetries in F-theory GUTs
title_full_unstemmed Family symmetries in F-theory GUTs
title_short Family symmetries in F-theory GUTs
title_sort family symmetries in f-theory guts
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1016/j.nuclphysb.2010.05.014
http://cds.cern.ch/record/1264268
http://cds.cern.ch/record/1264268
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