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Understanding the differences in neutrino and charged-fermion flavour structures
We present a new mechanism to explain naturally and through a common flavour symmetry the mildly hierarchical neutrino masses with large mixings and the hierarchical Yukawa matrices with small mixing angles. Although this mechanism is not linked to a particular flavour symmetry, it is particularly s...
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Lenguaje: | eng |
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2005
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Acceso en línea: | http://cds.cern.ch/record/832107 |
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author | Vives, Oscar |
author_facet | Vives, Oscar |
author_sort | Vives, Oscar |
collection | CERN |
description | We present a new mechanism to explain naturally and through a common flavour symmetry the mildly hierarchical neutrino masses with large mixings and the hierarchical Yukawa matrices with small mixing angles. Although this mechanism is not linked to a particular flavour symmetry, it is particularly simple in the framework of a SU(3) flavour symmetry. In this model, we obtain exactly maximal atmospheric mixing, large although not maximal solar mixing and a normal neutrino hierarchy. All neutrino parameters are basically fixed. For instance, we predict that the angle $\theta_{13}$ comes entirely from the charged lepton sector and, using the difference of the solar angle from maximality, we can fix the mass of lightest neutrino. |
id | cern-832107 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 2005 |
record_format | invenio |
spelling | cern-8321072023-03-14T17:17:32Zhttp://cds.cern.ch/record/832107engVives, OscarUnderstanding the differences in neutrino and charged-fermion flavour structuresParticle Physics - PhenomenologyWe present a new mechanism to explain naturally and through a common flavour symmetry the mildly hierarchical neutrino masses with large mixings and the hierarchical Yukawa matrices with small mixing angles. Although this mechanism is not linked to a particular flavour symmetry, it is particularly simple in the framework of a SU(3) flavour symmetry. In this model, we obtain exactly maximal atmospheric mixing, large although not maximal solar mixing and a normal neutrino hierarchy. All neutrino parameters are basically fixed. For instance, we predict that the angle $\theta_{13}$ comes entirely from the charged lepton sector and, using the difference of the solar angle from maximality, we can fix the mass of lightest neutrino.We present a new mechanism to explain naturally and through a common flavour symmetry the mildly hierarchical neutrino masses with large mixings and the hierarchical Yukawa matrices with small mixing angles. Although this mechanism is not linked to a particular flavour symmertry, it is particularly simple in the framework of a SU(3) flavour symmetry. In this model, we obtain exactly maximal atmospheric mixing, large although not maximal solar mixing and a normal neutrino hierarchy. All neutrino parameters are basically fixed. For instance, we predict that the angle $\theta_{13}$ comes entirely from the charged lepton sector and, using the difference of the solar angle from maximality, we can fix the mass of lightest neutrino.hep-ph/0504079CERN-PH-TH-2005-059CERN-PH-TH-2005-059oai:cds.cern.ch:8321072005-04-11 |
spellingShingle | Particle Physics - Phenomenology Vives, Oscar Understanding the differences in neutrino and charged-fermion flavour structures |
title | Understanding the differences in neutrino and charged-fermion flavour structures |
title_full | Understanding the differences in neutrino and charged-fermion flavour structures |
title_fullStr | Understanding the differences in neutrino and charged-fermion flavour structures |
title_full_unstemmed | Understanding the differences in neutrino and charged-fermion flavour structures |
title_short | Understanding the differences in neutrino and charged-fermion flavour structures |
title_sort | understanding the differences in neutrino and charged-fermion flavour structures |
topic | Particle Physics - Phenomenology |
url | http://cds.cern.ch/record/832107 |
work_keys_str_mv | AT vivesoscar understandingthedifferencesinneutrinoandchargedfermionflavourstructures |