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...

Full description

Bibliographic Details
Main Authors: Weijian Wang, Ruihong Wang, Zhi-Long Han, Jin-Zhong Han
Format: Article
Language:English
Published: SpringerOpen 2017-12-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-017-5446-9
id doaj-cf57169f232e440393be629391807efc
record_format Article
spelling 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
work_keys_str_mv AT weijianwang theblblscotogenicmodelsfordiracneutrinomasses
AT ruihongwang theblblscotogenicmodelsfordiracneutrinomasses
AT zhilonghan theblblscotogenicmodelsfordiracneutrinomasses
AT jinzhonghan theblblscotogenicmodelsfordiracneutrinomasses
AT weijianwang blblscotogenicmodelsfordiracneutrinomasses
AT ruihongwang blblscotogenicmodelsfordiracneutrinomasses
AT zhilonghan blblscotogenicmodelsfordiracneutrinomasses
AT jinzhonghan blblscotogenicmodelsfordiracneutrinomasses
_version_ 1725970925114884096