Three Flavor Quasi-Dirac Neutrino Mixing, Oscillations and Neutrinoless Double Beta Decay

The extension of the Standard model by three right-handed neutrino fields exhibit appealing symmetry between left-handed and right-handed sectors, which is only violated by interactions. It can accommodate three flavor quasi-Dirac neutrino mixing scheme, which allows processes with violation of both...

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Main Authors: Amina Khatun, Adam Smetana, Fedor Šimkovic
Format: Article
Language:English
Published: MDPI AG 2020-08-01
Series:Symmetry
Subjects:
Online Access:https://www.mdpi.com/2073-8994/12/8/1310
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spelling doaj-c23dfab7e5e043efb795a3d6b18153ae2020-11-25T02:59:35ZengMDPI AGSymmetry2073-89942020-08-01121310131010.3390/sym12081310Three Flavor Quasi-Dirac Neutrino Mixing, Oscillations and Neutrinoless Double Beta DecayAmina Khatun0Adam Smetana1Fedor Šimkovic2Department of nuclear Physics and Biophysics, Comenius University, Mlynská dolina F1, SK842 48 Bratislava, SlovakiaInstitute of Experimental and Applied Physics, Czech Technical University in Prague, 166 36 Prague, Czech RepublicDepartment of nuclear Physics and Biophysics, Comenius University, Mlynská dolina F1, SK842 48 Bratislava, SlovakiaThe extension of the Standard model by three right-handed neutrino fields exhibit appealing symmetry between left-handed and right-handed sectors, which is only violated by interactions. It can accommodate three flavor quasi-Dirac neutrino mixing scheme, which allows processes with violation of both lepton flavor and total lepton number symmetries. We propose a <inline-formula><math display="inline"><semantics><mrow><mn>6</mn><mo>×</mo><mn>6</mn></mrow></semantics></math></inline-formula> unitary matrix for parameterizing the mixing among three flavors of quasi-Dirac neutrino. This mixing matrix is constructed by two <inline-formula><math display="inline"><semantics><mrow><mn>3</mn><mo>×</mo><mn>3</mn></mrow></semantics></math></inline-formula> unitary matrices that diagonalizes the Dirac mass term in the Lagrangian. By only assuming the Standard Model <inline-formula><math display="inline"><semantics><mrow><mi>V</mi><mo>−</mo><mi>A</mi></mrow></semantics></math></inline-formula> weak interaction, it is found that probabilities of neutrino oscillations among active flavor states and effective masses measured by single beta decay, by neutrinoless double-beta decay and by cosmology only depend on single <inline-formula><math display="inline"><semantics><mrow><mn>3</mn><mo>×</mo><mn>3</mn></mrow></semantics></math></inline-formula> unitary matrix relevant to mixing of active neutrino flavors. Further, by considering <inline-formula><math display="inline"><semantics><mrow><mn>1</mn><mi>σ</mi></mrow></semantics></math></inline-formula> and <inline-formula><math display="inline"><semantics><mrow><mn>3</mn><mi>σ</mi></mrow></semantics></math></inline-formula> uncertainties in the measured oscillation probability of electron antineutrino from reactor, derivation of the constraint on the Majorana neutrino mass component is demonstrated. The consequence for effective Majorana neutrino mass governing the neutrinoless double-beta decay is discussed.https://www.mdpi.com/2073-8994/12/8/1310quasi-Diracneutrino oscillationMajorana neutrino massneutrinoless double beta decay
collection DOAJ
language English
format Article
sources DOAJ
author Amina Khatun
Adam Smetana
Fedor Šimkovic
spellingShingle Amina Khatun
Adam Smetana
Fedor Šimkovic
Three Flavor Quasi-Dirac Neutrino Mixing, Oscillations and Neutrinoless Double Beta Decay
Symmetry
quasi-Dirac
neutrino oscillation
Majorana neutrino mass
neutrinoless double beta decay
author_facet Amina Khatun
Adam Smetana
Fedor Šimkovic
author_sort Amina Khatun
title Three Flavor Quasi-Dirac Neutrino Mixing, Oscillations and Neutrinoless Double Beta Decay
title_short Three Flavor Quasi-Dirac Neutrino Mixing, Oscillations and Neutrinoless Double Beta Decay
title_full Three Flavor Quasi-Dirac Neutrino Mixing, Oscillations and Neutrinoless Double Beta Decay
title_fullStr Three Flavor Quasi-Dirac Neutrino Mixing, Oscillations and Neutrinoless Double Beta Decay
title_full_unstemmed Three Flavor Quasi-Dirac Neutrino Mixing, Oscillations and Neutrinoless Double Beta Decay
title_sort three flavor quasi-dirac neutrino mixing, oscillations and neutrinoless double beta decay
publisher MDPI AG
series Symmetry
issn 2073-8994
publishDate 2020-08-01
description The extension of the Standard model by three right-handed neutrino fields exhibit appealing symmetry between left-handed and right-handed sectors, which is only violated by interactions. It can accommodate three flavor quasi-Dirac neutrino mixing scheme, which allows processes with violation of both lepton flavor and total lepton number symmetries. We propose a <inline-formula><math display="inline"><semantics><mrow><mn>6</mn><mo>×</mo><mn>6</mn></mrow></semantics></math></inline-formula> unitary matrix for parameterizing the mixing among three flavors of quasi-Dirac neutrino. This mixing matrix is constructed by two <inline-formula><math display="inline"><semantics><mrow><mn>3</mn><mo>×</mo><mn>3</mn></mrow></semantics></math></inline-formula> unitary matrices that diagonalizes the Dirac mass term in the Lagrangian. By only assuming the Standard Model <inline-formula><math display="inline"><semantics><mrow><mi>V</mi><mo>−</mo><mi>A</mi></mrow></semantics></math></inline-formula> weak interaction, it is found that probabilities of neutrino oscillations among active flavor states and effective masses measured by single beta decay, by neutrinoless double-beta decay and by cosmology only depend on single <inline-formula><math display="inline"><semantics><mrow><mn>3</mn><mo>×</mo><mn>3</mn></mrow></semantics></math></inline-formula> unitary matrix relevant to mixing of active neutrino flavors. Further, by considering <inline-formula><math display="inline"><semantics><mrow><mn>1</mn><mi>σ</mi></mrow></semantics></math></inline-formula> and <inline-formula><math display="inline"><semantics><mrow><mn>3</mn><mi>σ</mi></mrow></semantics></math></inline-formula> uncertainties in the measured oscillation probability of electron antineutrino from reactor, derivation of the constraint on the Majorana neutrino mass component is demonstrated. The consequence for effective Majorana neutrino mass governing the neutrinoless double-beta decay is discussed.
topic quasi-Dirac
neutrino oscillation
Majorana neutrino mass
neutrinoless double beta decay
url https://www.mdpi.com/2073-8994/12/8/1310
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