Muon g − 2 and non-thermal leptogenesis in U 1 L μ − L τ $$ \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ model

Abstract The gauged U 1 L μ − L τ $$ \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ symmetry is the simplest possibility to explain the observed muon g − 2, while being consistent with the neutrino oscillations through the seesaw mechanism. In this paper, we investigate if leptogenesis can work at the sa...

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Main Authors: Shintaro Eijima, Masahiro Ibe, Kai Murai
Format: Article
Language:English
Published: SpringerOpen 2023-05-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP05(2023)010
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author Shintaro Eijima
Masahiro Ibe
Kai Murai
author_facet Shintaro Eijima
Masahiro Ibe
Kai Murai
author_sort Shintaro Eijima
collection DOAJ
description Abstract The gauged U 1 L μ − L τ $$ \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ symmetry is the simplest possibility to explain the observed muon g − 2, while being consistent with the neutrino oscillations through the seesaw mechanism. In this paper, we investigate if leptogenesis can work at the same time. At first glance, leptogenesis seems challenging because the right-handed neutrino masses are related to the U 1 L μ − L τ $$ \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ breaking scale of 10 – 100 GeV as required from the muon g − 2. Contrary to this expectation, we find that non-thermal leptogenesis with the right-handed neutrino masses of O $$ \mathcal{O} $$ (107) GeV is possible. The successful scenario results in strict predictions on the neutrino oscillation parameters, which will be tested in future experiments.
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spelling doaj.art-3b17e06d6f564ba1b5df2fa2aecd6a0b2023-08-27T11:04:30ZengSpringerOpenJournal of High Energy Physics1029-84792023-05-012023514310.1007/JHEP05(2023)010Muon g − 2 and non-thermal leptogenesis in U 1 L μ − L τ $$ \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ modelShintaro Eijima0Masahiro Ibe1Kai Murai2ICRR, University of TokyoICRR, University of TokyoICRR, University of TokyoAbstract The gauged U 1 L μ − L τ $$ \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ symmetry is the simplest possibility to explain the observed muon g − 2, while being consistent with the neutrino oscillations through the seesaw mechanism. In this paper, we investigate if leptogenesis can work at the same time. At first glance, leptogenesis seems challenging because the right-handed neutrino masses are related to the U 1 L μ − L τ $$ \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ breaking scale of 10 – 100 GeV as required from the muon g − 2. Contrary to this expectation, we find that non-thermal leptogenesis with the right-handed neutrino masses of O $$ \mathcal{O} $$ (107) GeV is possible. The successful scenario results in strict predictions on the neutrino oscillation parameters, which will be tested in future experiments.https://doi.org/10.1007/JHEP05(2023)010Baryo- and LeptogenesisNeutrino MixingNew Gauge InteractionsSterile or Heavy Neutrinos
spellingShingle Shintaro Eijima
Masahiro Ibe
Kai Murai
Muon g − 2 and non-thermal leptogenesis in U 1 L μ − L τ $$ \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ model
Journal of High Energy Physics
Baryo- and Leptogenesis
Neutrino Mixing
New Gauge Interactions
Sterile or Heavy Neutrinos
title Muon g − 2 and non-thermal leptogenesis in U 1 L μ − L τ $$ \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ model
title_full Muon g − 2 and non-thermal leptogenesis in U 1 L μ − L τ $$ \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ model
title_fullStr Muon g − 2 and non-thermal leptogenesis in U 1 L μ − L τ $$ \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ model
title_full_unstemmed Muon g − 2 and non-thermal leptogenesis in U 1 L μ − L τ $$ \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ model
title_short Muon g − 2 and non-thermal leptogenesis in U 1 L μ − L τ $$ \textrm{U}{(1)}_{L_{\mu }-{L}_{\tau }} $$ model
title_sort muon g 2 and non thermal leptogenesis in u 1 l μ l τ textrm u 1 l mu l tau model
topic Baryo- and Leptogenesis
Neutrino Mixing
New Gauge Interactions
Sterile or Heavy Neutrinos
url https://doi.org/10.1007/JHEP05(2023)010
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