TY - JOUR
T1 - Neutrino mass in a gauged Lμ − Lτ model
AU - Chen, Chuan Hung
AU - Nomura, Takaaki
N1 - Funding Information:
This work was partially supported by the Ministry of Science and Technology of Taiwan , under grant MOST-103-2112-M-006-004-MY3 (CHC).
Publisher Copyright:
© 2019 The Authors
PY - 2019/3
Y1 - 2019/3
N2 - We study the origin of neutrino mass through lepton-number violation and spontaneous U(1)Lμ−Lτ symmetry breaking. To accomplish the purpose, we include one Higgs triplet, two singlet scalars, and two vector-like doublet leptons in the U(1)Lμ−Lτ gauge extension of the standard model. To completely determine the free parameters, we employ the Frampton–Glashow–Marfatia (FGM) two-zero texture neutrino mass matrix as a theoretical input. It is found that when some particular Yukawa couplings vanish, an FGM pattern can be achieved in the model. Besides the explanation of neutrino data, we find that the absolute value of neutrino mass mj can be obtained in the model, and their sum can satisfy the upper bound of the cosmological measurement with ∑j|mj|<0.12 eV. The effective Majorana neutrino mass for neutrinoless double-beta decay is below the current upper limit and is obtained as 〈mββ〉=(0.34,2.3)×10−2 eV. In addition, the doubly charged Higgs H±± decaying to μ±τ± final states can be induced from a dimension-6 operator and is not suppressed, and its branching ratio is compatible with the H±±→W±W± decay when the vacuum expectation value of Higgs triplet is O(0.01) GeV.
AB - We study the origin of neutrino mass through lepton-number violation and spontaneous U(1)Lμ−Lτ symmetry breaking. To accomplish the purpose, we include one Higgs triplet, two singlet scalars, and two vector-like doublet leptons in the U(1)Lμ−Lτ gauge extension of the standard model. To completely determine the free parameters, we employ the Frampton–Glashow–Marfatia (FGM) two-zero texture neutrino mass matrix as a theoretical input. It is found that when some particular Yukawa couplings vanish, an FGM pattern can be achieved in the model. Besides the explanation of neutrino data, we find that the absolute value of neutrino mass mj can be obtained in the model, and their sum can satisfy the upper bound of the cosmological measurement with ∑j|mj|<0.12 eV. The effective Majorana neutrino mass for neutrinoless double-beta decay is below the current upper limit and is obtained as 〈mββ〉=(0.34,2.3)×10−2 eV. In addition, the doubly charged Higgs H±± decaying to μ±τ± final states can be induced from a dimension-6 operator and is not suppressed, and its branching ratio is compatible with the H±±→W±W± decay when the vacuum expectation value of Higgs triplet is O(0.01) GeV.
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U2 - 10.1016/j.nuclphysb.2019.01.016
DO - 10.1016/j.nuclphysb.2019.01.016
M3 - Article
AN - SCOPUS:85061209024
SN - 0550-3213
VL - 940
SP - 292
EP - 311
JO - Nuclear Physics B
JF - Nuclear Physics B
ER -