Cargando…
Neutrino Mass Textures from Oscillations with Maximal Mixing
We study the implications of neutrino oscillations with maximal mixing for the neutrino Dirac and Majorana matrices in the see-saw mechanism for three non degenerate neutrino masses. We find the form of the Dirac matrix for a structure-less Majorana matrix and, conversely, the structure of the Major...
Autores principales: | , |
---|---|
Lenguaje: | eng |
Publicado: |
1998
|
Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/S0370-2693(98)01007-7 http://cds.cern.ch/record/359736 |
_version_ | 1780892632146247680 |
---|---|
author | Altarelli, Guido Feruglio, Ferruccio |
author_facet | Altarelli, Guido Feruglio, Ferruccio |
author_sort | Altarelli, Guido |
collection | CERN |
description | We study the implications of neutrino oscillations with maximal mixing for the neutrino Dirac and Majorana matrices in the see-saw mechanism for three non degenerate neutrino masses. We find the form of the Dirac matrix for a structure-less Majorana matrix and, conversely, the structure of the Majorana matrix if the Dirac matrix is according to our naive intuition. We give some examples of Majorana matrices that, in a 3 X 3 context, lead to maximal mixing without too much fine tuning and cross talk with the Dirac input. |
id | cern-359736 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1998 |
record_format | invenio |
spelling | cern-3597362023-03-14T18:49:59Zdoi:10.1016/S0370-2693(98)01007-7http://cds.cern.ch/record/359736engAltarelli, GuidoFeruglio, FerruccioNeutrino Mass Textures from Oscillations with Maximal MixingParticle Physics - PhenomenologyWe study the implications of neutrino oscillations with maximal mixing for the neutrino Dirac and Majorana matrices in the see-saw mechanism for three non degenerate neutrino masses. We find the form of the Dirac matrix for a structure-less Majorana matrix and, conversely, the structure of the Majorana matrix if the Dirac matrix is according to our naive intuition. We give some examples of Majorana matrices that, in a 3 X 3 context, lead to maximal mixing without too much fine tuning and cross talk with the Dirac input.We study the implications of neutrino oscillations with maximal mixing for the neutrino Dirac and Majorana matrices in the see-saw mechanism for three non degenerate neutrino masses. We find the form of the Dirac matrix for a structure-less Majorana matrix and, conversely, the structure of the Majorana matrix if the Dirac matrix is according to our naive intuition. We give some examples of Majorana matrices that, in a 3 X 3 context, lead to maximal mixing without too much fine tuning and cross talk with the Dirac input.We study the implications of neutrino oscillations with maximal mixing for the neutrino Dirac and Majorana matrices in the see-saw mechanism for three non degenerate neutrino masses. We find the form of the Dirac matrix for a structure-less Majorana matrix and, conversely, the structure of the Majorana matrix if the Dirac matrix is according to our naive intuition. We give some examples of Majorana matrices that, in a 3 X 3 context, lead to maximal mixing without too much fine tuning and cross talk with the Dirac input.We study the implications of neutrino oscillations with maximal mixing for the neutrino Dirac and Majorana matrices in the see-saw mechanism for three non degenerate neutrino masses. We find the form of the Dirac matrix for a structure-less Majorana matrix and, conversely, the structure of the Majorana matrix if the Dirac matrix is according to our naive intuition. We give some examples of Majorana matrices that, in a 3 X 3 context, lead to maximal mixing without too much fine tuning and cross talk with the Dirac input.We study the implications of neutrino oscillations with maximal mixing for the neutrino Dirac and Majorana matrices in the see-saw mechanism for three non degenerate neutrino masses. We find the form of the Dirac matrix for a structure-less Majorana matrix and, conversely, the structure of the Majorana matrix if the Dirac matrix is according to our naive intuition. We give some examples of Majorana matrices that, in a 3×3 context, lead to maximal mixing without too much fine tuning and cross talk with the Dirac input.hep-ph/9807353CERN-TH-98-226DFPD-98-TH-34CERN-TH-98-226DFPD-98-TH-34oai:cds.cern.ch:3597361998-07-14 |
spellingShingle | Particle Physics - Phenomenology Altarelli, Guido Feruglio, Ferruccio Neutrino Mass Textures from Oscillations with Maximal Mixing |
title | Neutrino Mass Textures from Oscillations with Maximal Mixing |
title_full | Neutrino Mass Textures from Oscillations with Maximal Mixing |
title_fullStr | Neutrino Mass Textures from Oscillations with Maximal Mixing |
title_full_unstemmed | Neutrino Mass Textures from Oscillations with Maximal Mixing |
title_short | Neutrino Mass Textures from Oscillations with Maximal Mixing |
title_sort | neutrino mass textures from oscillations with maximal mixing |
topic | Particle Physics - Phenomenology |
url | https://dx.doi.org/10.1016/S0370-2693(98)01007-7 http://cds.cern.ch/record/359736 |
work_keys_str_mv | AT altarelliguido neutrinomasstexturesfromoscillationswithmaximalmixing AT feruglioferruccio neutrinomasstexturesfromoscillationswithmaximalmixing |