The $$B-L$$ B - L scotogenic models for Dirac neutrino masses
Abstract We construct the one-loop and two-loop scotogenic models for Dirac neutrino mass generation in the context of $$U(1)_{B-L}$$ U ( 1 ) B - L extensions of standard model. It is indicated that the total number of intermediate fermion singlets is uniquely fixed by the anomaly free condition and...
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doaj-cf57169f232e440393be629391807efc2020-11-24T21:28:22ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522017-12-01771211010.1140/epjc/s10052-017-5446-9The $$B-L$$ B - L scotogenic models for Dirac neutrino massesWeijian Wang0Ruihong Wang1Zhi-Long Han2Jin-Zhong Han3Department of Physics, North China Electric Power UniversityCollege of Information Science and Technology, Hebei Agricultural UniversitySchool of Physics and Technology, University of JinanSchool of Physics and Telecommunications Engineering, Zhoukou Normal UniversityAbstract We construct the one-loop and two-loop scotogenic models for Dirac neutrino mass generation in the context of $$U(1)_{B-L}$$ U ( 1 ) B - L extensions of standard model. It is indicated that the total number of intermediate fermion singlets is uniquely fixed by the anomaly free condition and the new particles may have exotic $$B-L$$ B - L charges so that the direct SM Yukawa mass term $$\bar{\nu }_L\nu _R\overline{\phi ^0}$$ ν ¯ L ν R ϕ 0 ¯ and the Majorana mass term $$(m_N/2)\overline{\nu _R^C}\nu _R$$ ( m N / 2 ) ν R C ¯ ν R are naturally forbidden. After the spontaneous breaking of the $$U(1)_{B-L}$$ U ( 1 ) B - L symmetry, the discrete $$Z_{2}$$ Z 2 or $$Z_{3}$$ Z 3 symmetry appears as the residual symmetry and gives rise to the stability of intermediate fields as DM candidates. Phenomenological aspects of lepton flavor violation, DM, leptogenesis and LHC signatures are discussed.http://link.springer.com/article/10.1140/epjc/s10052-017-5446-9 |
collection |
DOAJ |
language |
English |
format |
Article |
sources |
DOAJ |
author |
Weijian Wang Ruihong Wang Zhi-Long Han Jin-Zhong Han |
spellingShingle |
Weijian Wang Ruihong Wang Zhi-Long Han Jin-Zhong Han The $$B-L$$ B - L scotogenic models for Dirac neutrino masses European Physical Journal C: Particles and Fields |
author_facet |
Weijian Wang Ruihong Wang Zhi-Long Han Jin-Zhong Han |
author_sort |
Weijian Wang |
title |
The $$B-L$$ B - L scotogenic models for Dirac neutrino masses |
title_short |
The $$B-L$$ B - L scotogenic models for Dirac neutrino masses |
title_full |
The $$B-L$$ B - L scotogenic models for Dirac neutrino masses |
title_fullStr |
The $$B-L$$ B - L scotogenic models for Dirac neutrino masses |
title_full_unstemmed |
The $$B-L$$ B - L scotogenic models for Dirac neutrino masses |
title_sort |
$$b-l$$ b - l scotogenic models for dirac neutrino masses |
publisher |
SpringerOpen |
series |
European Physical Journal C: Particles and Fields |
issn |
1434-6044 1434-6052 |
publishDate |
2017-12-01 |
description |
Abstract We construct the one-loop and two-loop scotogenic models for Dirac neutrino mass generation in the context of $$U(1)_{B-L}$$ U ( 1 ) B - L extensions of standard model. It is indicated that the total number of intermediate fermion singlets is uniquely fixed by the anomaly free condition and the new particles may have exotic $$B-L$$ B - L charges so that the direct SM Yukawa mass term $$\bar{\nu }_L\nu _R\overline{\phi ^0}$$ ν ¯ L ν R ϕ 0 ¯ and the Majorana mass term $$(m_N/2)\overline{\nu _R^C}\nu _R$$ ( m N / 2 ) ν R C ¯ ν R are naturally forbidden. After the spontaneous breaking of the $$U(1)_{B-L}$$ U ( 1 ) B - L symmetry, the discrete $$Z_{2}$$ Z 2 or $$Z_{3}$$ Z 3 symmetry appears as the residual symmetry and gives rise to the stability of intermediate fields as DM candidates. Phenomenological aspects of lepton flavor violation, DM, leptogenesis and LHC signatures are discussed. |
url |
http://link.springer.com/article/10.1140/epjc/s10052-017-5446-9 |
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