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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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Lenguaje: | eng |
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2002
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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. |
id | cern-547822 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2002 |
record_format | invenio |
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 |