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Symmetries, Large Leptonic Mixing and a Fourth Generation

We show that large leptonic mixing occurs most naturally in the framework of the Sandard Model just by adding a fourth generation. One can then construct a small $Z_4$ discrete symmetry, instead of the large $S_{4L}\times S_{4R}$, which requires that the neutrino as well as the charged lepton mass m...

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Autor principal: Silva-Marcos, Joaquim I.
Lenguaje:eng
Publicado: 2002
Materias:
Acceso en línea:https://dx.doi.org/10.1088/1126-6708/2002/12/036
http://cds.cern.ch/record/547822
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author Silva-Marcos, Joaquim I.
author_facet Silva-Marcos, Joaquim I.
author_sort Silva-Marcos, Joaquim I.
collection CERN
description We show that large leptonic mixing occurs most naturally in the framework of the Sandard Model just by adding a fourth generation. One can then construct a small $Z_4$ discrete symmetry, instead of the large $S_{4L}\times S_{4R}$, which requires that the neutrino as well as the charged lepton mass matrices be proportional to a $4\times 4$ democratic mass matrix, where all entries are equal to unity. Without considering the see-saw mechanism, or other more elaborate extensions of the SM, and contrary to the case with only 3 generations, large leptonic mixing is obtained when the symmetry is broken.
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institution Organización Europea para la Investigación Nuclear
language eng
publishDate 2002
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spelling cern-5478222023-10-04T08:15:57Zdoi:10.1088/1126-6708/2002/12/036http://cds.cern.ch/record/547822engSilva-Marcos, Joaquim I.Symmetries, Large Leptonic Mixing and a Fourth GenerationParticle Physics - PhenomenologyWe show that large leptonic mixing occurs most naturally in the framework of the Sandard Model just by adding a fourth generation. One can then construct a small $Z_4$ discrete symmetry, instead of the large $S_{4L}\times S_{4R}$, which requires that the neutrino as well as the charged lepton mass matrices be proportional to a $4\times 4$ democratic mass matrix, where all entries are equal to unity. Without considering the see-saw mechanism, or other more elaborate extensions of the SM, and contrary to the case with only 3 generations, large leptonic mixing is obtained when the symmetry is broken.We show that large leptonic mixing occurs most naturally in the framework of the Sandard Model just by adding a fourth generation. One can then construct a small $Z_4$ discrete symmetry, instead of the large $S_{4L}\times S_{4R}$, which requires that the neutrino as well as the charged lepton mass matrices be proportional to a $4\times 4$ democratic mass matrix, where all entries are equal to unity. Without considering the see-saw mechanism, or other more elaborate extensions of the SM, and contrary to the case with only 3 generations, large leptonic mixing is obtained when the symmetry is broken.hep-ph/0204217CERN-TH-2002-072oai:cds.cern.ch:5478222002-04-18
spellingShingle Particle Physics - Phenomenology
Silva-Marcos, Joaquim I.
Symmetries, Large Leptonic Mixing and a Fourth Generation
title Symmetries, Large Leptonic Mixing and a Fourth Generation
title_full Symmetries, Large Leptonic Mixing and a Fourth Generation
title_fullStr Symmetries, Large Leptonic Mixing and a Fourth Generation
title_full_unstemmed Symmetries, Large Leptonic Mixing and a Fourth Generation
title_short Symmetries, Large Leptonic Mixing and a Fourth Generation
title_sort symmetries, large leptonic mixing and a fourth generation
topic Particle Physics - Phenomenology
url https://dx.doi.org/10.1088/1126-6708/2002/12/036
http://cds.cern.ch/record/547822
work_keys_str_mv AT silvamarcosjoaquimi symmetrieslargeleptonicmixingandafourthgeneration