Covert symmetries in the neutrino mass matrix
Abstract The flavour neutrino puzzle is often addressed by considering neutrino mass matrices m with a certain number of vanishing entries (m ij = 0 for some values of the indices), since a reduction in the number of free parameters increases the predictive power. Symmetries that can enforce texture...
Main Authors: | , , , |
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Format: | Article |
Language: | English |
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SpringerOpen
2020-02-01
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Series: | Journal of High Energy Physics |
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Online Access: | https://doi.org/10.1007/JHEP02(2020)066 |
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author | Fredrik Björkeroth Luca Di Luzio Federico Mescia Enrico Nardi |
author_facet | Fredrik Björkeroth Luca Di Luzio Federico Mescia Enrico Nardi |
author_sort | Fredrik Björkeroth |
collection | DOAJ |
description | Abstract The flavour neutrino puzzle is often addressed by considering neutrino mass matrices m with a certain number of vanishing entries (m ij = 0 for some values of the indices), since a reduction in the number of free parameters increases the predictive power. Symmetries that can enforce textures zero can also enforce a more general type of conditions f(m ij ) = 0 with f some function of the matrix elements m ij . In this case m can have all entries non-vanishing with no reduction in its predictive power. We classify all generation-dependent U(1) symmetries which, in the presence of two leptonic Higgs doublets, can reduce the number of independent high-energy parameters of type-I seesaw to the minimum number compatible with non-vanishing neutrino mixings and CP violation. These symmetries are broken above the scale where the effective operator is generated and can thus remain covert, in the sense that no explicit evidence of the symmetry can be read off the neutrino mass matrix, and different symmetries can give rise to the same low-energy structure. We find that only two cases are viable: one yields a structure with two zero-textures already considered in the literature, the other has no zero-textures and has never been considered before. It predicts normal ordering, a lightest neutrino mass ∼ 10 meV, a Dirac phase δ ∼ 3 π 2 $$ \frac{3\pi }{2} $$ and definite values for the Majorana phases. |
first_indexed | 2024-12-16T15:04:03Z |
format | Article |
id | doaj.art-b4ece6966baa490b963c553add02aaa2 |
institution | Directory Open Access Journal |
issn | 1029-8479 |
language | English |
last_indexed | 2024-12-16T15:04:03Z |
publishDate | 2020-02-01 |
publisher | SpringerOpen |
record_format | Article |
series | Journal of High Energy Physics |
spelling | doaj.art-b4ece6966baa490b963c553add02aaa22022-12-21T22:27:12ZengSpringerOpenJournal of High Energy Physics1029-84792020-02-012020212510.1007/JHEP02(2020)066Covert symmetries in the neutrino mass matrixFredrik Björkeroth0Luca Di Luzio1Federico Mescia2Enrico Nardi3INFN, Laboratori Nazionali di FrascatiDeutsches Elektronen-Synchrotron DESYDepartament de Física Quàntica i Astrofísica, Institut de Ciències del Cosmos (ICCUB), Universitat de BarcelonaINFN, Laboratori Nazionali di FrascatiAbstract The flavour neutrino puzzle is often addressed by considering neutrino mass matrices m with a certain number of vanishing entries (m ij = 0 for some values of the indices), since a reduction in the number of free parameters increases the predictive power. Symmetries that can enforce textures zero can also enforce a more general type of conditions f(m ij ) = 0 with f some function of the matrix elements m ij . In this case m can have all entries non-vanishing with no reduction in its predictive power. We classify all generation-dependent U(1) symmetries which, in the presence of two leptonic Higgs doublets, can reduce the number of independent high-energy parameters of type-I seesaw to the minimum number compatible with non-vanishing neutrino mixings and CP violation. These symmetries are broken above the scale where the effective operator is generated and can thus remain covert, in the sense that no explicit evidence of the symmetry can be read off the neutrino mass matrix, and different symmetries can give rise to the same low-energy structure. We find that only two cases are viable: one yields a structure with two zero-textures already considered in the literature, the other has no zero-textures and has never been considered before. It predicts normal ordering, a lightest neutrino mass ∼ 10 meV, a Dirac phase δ ∼ 3 π 2 $$ \frac{3\pi }{2} $$ and definite values for the Majorana phases.https://doi.org/10.1007/JHEP02(2020)066Global SymmetriesNeutrino PhysicsBeyond Standard Model |
spellingShingle | Fredrik Björkeroth Luca Di Luzio Federico Mescia Enrico Nardi Covert symmetries in the neutrino mass matrix Journal of High Energy Physics Global Symmetries Neutrino Physics Beyond Standard Model |
title | Covert symmetries in the neutrino mass matrix |
title_full | Covert symmetries in the neutrino mass matrix |
title_fullStr | Covert symmetries in the neutrino mass matrix |
title_full_unstemmed | Covert symmetries in the neutrino mass matrix |
title_short | Covert symmetries in the neutrino mass matrix |
title_sort | covert symmetries in the neutrino mass matrix |
topic | Global Symmetries Neutrino Physics Beyond Standard Model |
url | https://doi.org/10.1007/JHEP02(2020)066 |
work_keys_str_mv | AT fredrikbjorkeroth covertsymmetriesintheneutrinomassmatrix AT lucadiluzio covertsymmetriesintheneutrinomassmatrix AT federicomescia covertsymmetriesintheneutrinomassmatrix AT enriconardi covertsymmetriesintheneutrinomassmatrix |