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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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Autor principal: Vives, Oscar
Lenguaje:eng
Publicado: 2005
Materias:
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
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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