Neutrino phenomenology via Type-(I+II) seesaw in the $U(1)_{L_e-L_\mu}$ model
We show how, L_e-L_\mu L e − L μ gauged symmetry is used as the Standard Model (SM) extension with the type (I+II) seesaw mechanism for neutrino mass generation. The particle content of this model involves three extra right handed neutrinos, one scalar triplet and one singlet with the SM spectrum. W...
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Published in | SciPost physics proceedings no. 16; p. 023 |
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Main Authors | , , , , |
Format | Journal Article |
Language | English |
Published |
SciPost
15.07.2025
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Online Access | Get full text |
ISSN | 2666-4003 2666-4003 |
DOI | 10.21468/SciPostPhysProc.16.023 |
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Abstract | We show how, L_e-L_\mu L e − L μ gauged symmetry is used as the Standard Model (SM) extension with the type (I+II) seesaw mechanism for neutrino mass generation. The particle content of this model involves three extra right handed neutrinos, one scalar triplet and one singlet with the SM spectrum. We discuss about lepton flavour violating decays \mu → e\gamma μ → e γ , \tau \to \mu \bar \mu\mu τ → μ μ ‾ μ and anomalous magnetic moment of muon. |
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AbstractList | We show how, $L_e-L_\mu$ gauged symmetry is used as the Standard Model (SM) extension with the type (I+II) seesaw mechanism for neutrino mass generation. The particle content of this model involves three extra right handed neutrinos, one scalar triplet and one singlet with the SM spectrum. We discuss about lepton flavour violating decays $\mu → e\gamma$, $\tau \to \mu \bar \mu\mu$ and anomalous magnetic moment of muon. We show how, L_e-L_\mu L e − L μ gauged symmetry is used as the Standard Model (SM) extension with the type (I+II) seesaw mechanism for neutrino mass generation. The particle content of this model involves three extra right handed neutrinos, one scalar triplet and one singlet with the SM spectrum. We discuss about lepton flavour violating decays \mu → e\gamma μ → e γ , \tau \to \mu \bar \mu\mu τ → μ μ ‾ μ and anomalous magnetic moment of muon. |
ArticleNumber | 023 |
Author | Panda, Papia SINGIRALA, SHIVARAMAKRISHNA Mohanta, Rukmani Kumar Behera, Mitesh Mishra, Priya |
Author_xml | – sequence: 1 givenname: Priya orcidid: 0000-0003-1914-9959 surname: Mishra fullname: Mishra, Priya – sequence: 2 givenname: Mitesh surname: Kumar Behera fullname: Kumar Behera, Mitesh – sequence: 3 givenname: Papia orcidid: 0000-0001-9142-7090 surname: Panda fullname: Panda, Papia – sequence: 4 givenname: SHIVARAMAKRISHNA orcidid: 0000-0002-8444-7875 surname: SINGIRALA fullname: SINGIRALA, SHIVARAMAKRISHNA – sequence: 5 givenname: Rukmani surname: Mohanta fullname: Mohanta, Rukmani |
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Cites_doi | 10.1103/PhysRevD.103.072002 10.1109/19.769558 10.1007/JHEP12(2012)123 10.1007/JHEP03(2010)044 10.1103/PhysRevD.77.075010 10.1007/JHEP09(2011)083 10.21468/SciPostPhysProc.16.023 |
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Snippet | We show how, L_e-L_\mu L e − L μ gauged symmetry is used as the Standard Model (SM) extension with the type (I+II) seesaw mechanism for neutrino mass... We show how, $L_e-L_\mu$ gauged symmetry is used as the Standard Model (SM) extension with the type (I+II) seesaw mechanism for neutrino mass generation. The... |
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