Broken scaling neutrino mass matrix and leptogenesis based on A4 modular invariance

Abstract In this work, we have proposed a modular A 4 symmetric model of neutrino mass which, simultaneously, explains observed baryon asymmetry of the Universe (BAU). In minimal extension of the standard model (SM) with two right-handed neutrinos we work in a supersymmetric framework. At Type-I see...

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Main Authors: Monal Kashav, Surender Verma
Format: Article
Language:English
Published: SpringerOpen 2021-09-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP09(2021)100
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spelling doaj-36d9d001115442cebc1fa6e0f1c46a9b2021-09-26T11:53:51ZengSpringerOpenJournal of High Energy Physics1029-84792021-09-012021912310.1007/JHEP09(2021)100Broken scaling neutrino mass matrix and leptogenesis based on A4 modular invarianceMonal Kashav0Surender Verma1Department of Physics and Astronomical Science, Central University of Himachal PradeshDepartment of Physics and Astronomical Science, Central University of Himachal PradeshAbstract In this work, we have proposed a modular A 4 symmetric model of neutrino mass which, simultaneously, explains observed baryon asymmetry of the Universe (BAU). In minimal extension of the standard model (SM) with two right-handed neutrinos we work in a supersymmetric framework. At Type-I seesaw level, the model predicts scaling in the neutrino mass matrix. In order to have correct low energy phenomenology, we propose two possible scenarios of scale-breaking in the neutrino mass matrix emanating from Type-I seesaw. Scenario-1 is based on the dimension-5 Weinberg operator whereas scenario-2 implements Type-II seesaw via scalar triplet Higgs superfields (∆, ∆ ¯ $$ \overline{\Delta } $$ ). Interestingly, the breaking patterns in both, otherwise dynamically different scenarios, are similar which can be attributed to the same charge assignments of superfields (∆, ∆ ¯ $$ \overline{\Delta } $$ ) and the Higgs superfield H u under modular A 4 symmetry. The breaking is found to be proportional to the Yukawa coupling of modular weight 10 ( Y 1 , 1 ′ 10 $$ {Y}_{1,1\prime}^{10} $$ ). We, further, investigates the predictions of the model under scenario-2 (Type-I+II) for neutrino mass, mixings and matter-antimatter asymmetry of the Universe. The model predicts normal hierarchical neutrino masses and provide a robust range (0.05 − 0.08)eV for sum of neutrino masses (Σm i ). Lepton number violating 0νββ decay amplitude (M ee ) is obtained to lie in the range (0.04 − 0.06)eV. Future 0νββ decay experiments such as NEXT and nEXO shall pose crucial test for the model. Both CP conserving and CP violating solutions are allowed in the model. Interesting correlations are obtained, specially, between Yukawa couplings of modular weight 2 and complex modulus τ. Contrary to Y 2 2 $$ {Y}_2^2 $$ and Y 3 2 $$ {Y}_3^2 $$ , the Yukawa coupling Y 1 2 $$ {Y}_1^2 $$ is found to be insensitive to τ and thus to CP violation because complex modulus τ is the only source of CP violation in the model. We, also, investigate the prediction of the model for BAU. The model exhibit consistent explanation of BAU for right-handed Majorana neutrino mass scale in the range ((1 − 5) × 1013) GeV.https://doi.org/10.1007/JHEP09(2021)100Discrete SymmetriesNeutrino PhysicsGauge Symmetry
collection DOAJ
language English
format Article
sources DOAJ
author Monal Kashav
Surender Verma
spellingShingle Monal Kashav
Surender Verma
Broken scaling neutrino mass matrix and leptogenesis based on A4 modular invariance
Journal of High Energy Physics
Discrete Symmetries
Neutrino Physics
Gauge Symmetry
author_facet Monal Kashav
Surender Verma
author_sort Monal Kashav
title Broken scaling neutrino mass matrix and leptogenesis based on A4 modular invariance
title_short Broken scaling neutrino mass matrix and leptogenesis based on A4 modular invariance
title_full Broken scaling neutrino mass matrix and leptogenesis based on A4 modular invariance
title_fullStr Broken scaling neutrino mass matrix and leptogenesis based on A4 modular invariance
title_full_unstemmed Broken scaling neutrino mass matrix and leptogenesis based on A4 modular invariance
title_sort broken scaling neutrino mass matrix and leptogenesis based on a4 modular invariance
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2021-09-01
description Abstract In this work, we have proposed a modular A 4 symmetric model of neutrino mass which, simultaneously, explains observed baryon asymmetry of the Universe (BAU). In minimal extension of the standard model (SM) with two right-handed neutrinos we work in a supersymmetric framework. At Type-I seesaw level, the model predicts scaling in the neutrino mass matrix. In order to have correct low energy phenomenology, we propose two possible scenarios of scale-breaking in the neutrino mass matrix emanating from Type-I seesaw. Scenario-1 is based on the dimension-5 Weinberg operator whereas scenario-2 implements Type-II seesaw via scalar triplet Higgs superfields (∆, ∆ ¯ $$ \overline{\Delta } $$ ). Interestingly, the breaking patterns in both, otherwise dynamically different scenarios, are similar which can be attributed to the same charge assignments of superfields (∆, ∆ ¯ $$ \overline{\Delta } $$ ) and the Higgs superfield H u under modular A 4 symmetry. The breaking is found to be proportional to the Yukawa coupling of modular weight 10 ( Y 1 , 1 ′ 10 $$ {Y}_{1,1\prime}^{10} $$ ). We, further, investigates the predictions of the model under scenario-2 (Type-I+II) for neutrino mass, mixings and matter-antimatter asymmetry of the Universe. The model predicts normal hierarchical neutrino masses and provide a robust range (0.05 − 0.08)eV for sum of neutrino masses (Σm i ). Lepton number violating 0νββ decay amplitude (M ee ) is obtained to lie in the range (0.04 − 0.06)eV. Future 0νββ decay experiments such as NEXT and nEXO shall pose crucial test for the model. Both CP conserving and CP violating solutions are allowed in the model. Interesting correlations are obtained, specially, between Yukawa couplings of modular weight 2 and complex modulus τ. Contrary to Y 2 2 $$ {Y}_2^2 $$ and Y 3 2 $$ {Y}_3^2 $$ , the Yukawa coupling Y 1 2 $$ {Y}_1^2 $$ is found to be insensitive to τ and thus to CP violation because complex modulus τ is the only source of CP violation in the model. We, also, investigate the prediction of the model for BAU. The model exhibit consistent explanation of BAU for right-handed Majorana neutrino mass scale in the range ((1 − 5) × 1013) GeV.
topic Discrete Symmetries
Neutrino Physics
Gauge Symmetry
url https://doi.org/10.1007/JHEP09(2021)100
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