Probing maximal zero textures with broken cyclic symmetry in inverse seesaw

Within the framework of inverse seesaw mechanism we investigate neutrino mass matrices invariant under cyclic symmetry (Z3) with maximal zero texture (6 zero textures). We explore two different approaches to obtain the cyclic symmetry invariant form of the constituent matrices. In the first one we c...

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Main Authors: Rome Samanta, Ambar Ghosal
Format: Article
Language:English
Published: Elsevier 2016-10-01
Series:Nuclear Physics B
Online Access:http://www.sciencedirect.com/science/article/pii/S0550321316302668
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spelling doaj-c5b95635345544b7ba1714313b253c282020-11-24T23:02:37ZengElsevierNuclear Physics B0550-32131873-15622016-10-01911C84686210.1016/j.nuclphysb.2016.08.036Probing maximal zero textures with broken cyclic symmetry in inverse seesawRome SamantaAmbar GhosalWithin the framework of inverse seesaw mechanism we investigate neutrino mass matrices invariant under cyclic symmetry (Z3) with maximal zero texture (6 zero textures). We explore two different approaches to obtain the cyclic symmetry invariant form of the constituent matrices. In the first one we consider explicit cyclic symmetry in the neutrino sector of the Lagrangian which dictates the emerged effective neutrino mass matrix (mν) to be symmetry invariant and hence leads to a degeneracy in masses. We then consider explicit breaking of the symmetry through a dimensionless parameter ϵ′ to remove the degeneracy. It is seen that the method doesn't support the current neutrino oscillation global fit data even after considering the correction from cyclic symmetry invariant charged lepton mass matrix (ml) unless the breaking parameter is too large. In the second method, we assume the same forms of the neutrino mass matrices, however, symmetry is broken in the charged lepton sector. All the structures of the mass matrices are now dictated by an effective residual symmetry of some larger symmetry group in the Lagrangian. For illustration, we exemplify a toy model based on softly broken A4 symmetry group which leads to one of the combinations of ml, mD, MRS and μ to generate effective mν. All the emerged mass matrices predict a constraint range of the CP violating phases and atmospheric mixing angle along with an inverted hierarchical structure of the neutrino masses. Further, significant predictions on ββ0ν decay parameter |m11| and the sum of the three light neutrino masses (Σimi) are also obtained.http://www.sciencedirect.com/science/article/pii/S0550321316302668
collection DOAJ
language English
format Article
sources DOAJ
author Rome Samanta
Ambar Ghosal
spellingShingle Rome Samanta
Ambar Ghosal
Probing maximal zero textures with broken cyclic symmetry in inverse seesaw
Nuclear Physics B
author_facet Rome Samanta
Ambar Ghosal
author_sort Rome Samanta
title Probing maximal zero textures with broken cyclic symmetry in inverse seesaw
title_short Probing maximal zero textures with broken cyclic symmetry in inverse seesaw
title_full Probing maximal zero textures with broken cyclic symmetry in inverse seesaw
title_fullStr Probing maximal zero textures with broken cyclic symmetry in inverse seesaw
title_full_unstemmed Probing maximal zero textures with broken cyclic symmetry in inverse seesaw
title_sort probing maximal zero textures with broken cyclic symmetry in inverse seesaw
publisher Elsevier
series Nuclear Physics B
issn 0550-3213
1873-1562
publishDate 2016-10-01
description Within the framework of inverse seesaw mechanism we investigate neutrino mass matrices invariant under cyclic symmetry (Z3) with maximal zero texture (6 zero textures). We explore two different approaches to obtain the cyclic symmetry invariant form of the constituent matrices. In the first one we consider explicit cyclic symmetry in the neutrino sector of the Lagrangian which dictates the emerged effective neutrino mass matrix (mν) to be symmetry invariant and hence leads to a degeneracy in masses. We then consider explicit breaking of the symmetry through a dimensionless parameter ϵ′ to remove the degeneracy. It is seen that the method doesn't support the current neutrino oscillation global fit data even after considering the correction from cyclic symmetry invariant charged lepton mass matrix (ml) unless the breaking parameter is too large. In the second method, we assume the same forms of the neutrino mass matrices, however, symmetry is broken in the charged lepton sector. All the structures of the mass matrices are now dictated by an effective residual symmetry of some larger symmetry group in the Lagrangian. For illustration, we exemplify a toy model based on softly broken A4 symmetry group which leads to one of the combinations of ml, mD, MRS and μ to generate effective mν. All the emerged mass matrices predict a constraint range of the CP violating phases and atmospheric mixing angle along with an inverted hierarchical structure of the neutrino masses. Further, significant predictions on ββ0ν decay parameter |m11| and the sum of the three light neutrino masses (Σimi) are also obtained.
url http://www.sciencedirect.com/science/article/pii/S0550321316302668
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