Neutrino masses and gauged U(1) ℓ lepton number

Abstract We investigate the tree-level neutrino mass generation in the gauged U(1) ℓ lepton model recently proposed by us [1]. With the addition of one Standard Model(SM) singlet, ϕ 1(Y = 0, ℓ = 1), and one SM triplet scalar, T (Y = −1, ℓ = 0), realistic lepton masses can be accommodated. The result...

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Main Authors: We-Fu Chang, John N. Ng
Format: Article
Language:English
Published: SpringerOpen 2018-10-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP10(2018)015
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author We-Fu Chang
John N. Ng
author_facet We-Fu Chang
John N. Ng
author_sort We-Fu Chang
collection DOAJ
description Abstract We investigate the tree-level neutrino mass generation in the gauged U(1) ℓ lepton model recently proposed by us [1]. With the addition of one Standard Model(SM) singlet, ϕ 1(Y = 0, ℓ = 1), and one SM triplet scalar, T (Y = −1, ℓ = 0), realistic lepton masses can be accommodated. The resulting magnitude of neutrino mass is given by ∼ v t 3 /v L 2 , where v t and v L are the vacuum expectation values of T and ϕ 1, respectively, and it is automatically of the inverse see-saw type. Since v L is the lepton number violation scale we take it to be high, i.e. O ≳ (TeV). Moreover, the induced lepton flavor violating processes and the phenomenology of the peculiar triplet are studied. An interesting bound, 0.1 ≲ v t ≲ 24.1 GeV, is obtained when taking into account the neutrino mass generation, Br(μ → eγ), and the limits from oblique parameters, ΔS and ΔT. Collider phenomenology of the SM triplets is also discussed.
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spelling doaj.art-f641ba1f8380428ea847a6a40f41da602022-12-22T01:54:50ZengSpringerOpenJournal of High Energy Physics1029-84792018-10-0120181012910.1007/JHEP10(2018)015Neutrino masses and gauged U(1) ℓ lepton numberWe-Fu Chang0John N. Ng1Department of Physics, National Tsing Hua UniversityTRIUMF Theory GroupAbstract We investigate the tree-level neutrino mass generation in the gauged U(1) ℓ lepton model recently proposed by us [1]. With the addition of one Standard Model(SM) singlet, ϕ 1(Y = 0, ℓ = 1), and one SM triplet scalar, T (Y = −1, ℓ = 0), realistic lepton masses can be accommodated. The resulting magnitude of neutrino mass is given by ∼ v t 3 /v L 2 , where v t and v L are the vacuum expectation values of T and ϕ 1, respectively, and it is automatically of the inverse see-saw type. Since v L is the lepton number violation scale we take it to be high, i.e. O ≳ (TeV). Moreover, the induced lepton flavor violating processes and the phenomenology of the peculiar triplet are studied. An interesting bound, 0.1 ≲ v t ≲ 24.1 GeV, is obtained when taking into account the neutrino mass generation, Br(μ → eγ), and the limits from oblique parameters, ΔS and ΔT. Collider phenomenology of the SM triplets is also discussed.http://link.springer.com/article/10.1007/JHEP10(2018)015Anomalies in Field and String TheoriesBeyond Standard ModelGauge SymmetryNeutrino Physics
spellingShingle We-Fu Chang
John N. Ng
Neutrino masses and gauged U(1) ℓ lepton number
Journal of High Energy Physics
Anomalies in Field and String Theories
Beyond Standard Model
Gauge Symmetry
Neutrino Physics
title Neutrino masses and gauged U(1) ℓ lepton number
title_full Neutrino masses and gauged U(1) ℓ lepton number
title_fullStr Neutrino masses and gauged U(1) ℓ lepton number
title_full_unstemmed Neutrino masses and gauged U(1) ℓ lepton number
title_short Neutrino masses and gauged U(1) ℓ lepton number
title_sort neutrino masses and gauged u 1 l lepton number
topic Anomalies in Field and String Theories
Beyond Standard Model
Gauge Symmetry
Neutrino Physics
url http://link.springer.com/article/10.1007/JHEP10(2018)015
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