### Abstract

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 m_{j} can be obtained in the model, and their sum can satisfy the upper bound of the cosmological measurement with ∑_{j}|m_{j}|<0.12 eV. The effective Majorana neutrino mass for neutrinoless double-beta decay is below the current upper limit and is obtained as 〈m_{ββ}〉=(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.

Original language | English |
---|---|

Pages (from-to) | 292-311 |

Number of pages | 20 |

Journal | Nuclear Physics B |

Volume | 940 |

DOIs | |

Publication status | Published - 2019 Mar 1 |

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### All Science Journal Classification (ASJC) codes

- Nuclear and High Energy Physics

### Cite this

_{μ}− L

_{τ}model.

*Nuclear Physics B*,

*940*, 292-311. https://doi.org/10.1016/j.nuclphysb.2019.01.016

}

_{μ}− L

_{τ}model',

*Nuclear Physics B*, vol. 940, pp. 292-311. https://doi.org/10.1016/j.nuclphysb.2019.01.016

**Neutrino mass in a gauged L _{μ} − L_{τ} model.** / Chen, Chuan-Hung; Nomura, Takaaki.

Research output: Contribution to journal › Article

TY - JOUR

T1 - Neutrino mass in a gauged Lμ − Lτ model

AU - Chen, Chuan-Hung

AU - Nomura, Takaaki

PY - 2019/3/1

Y1 - 2019/3/1

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.

UR - http://www.scopus.com/inward/record.url?scp=85061209024&partnerID=8YFLogxK

UR - http://www.scopus.com/inward/citedby.url?scp=85061209024&partnerID=8YFLogxK

U2 - 10.1016/j.nuclphysb.2019.01.016

DO - 10.1016/j.nuclphysb.2019.01.016

M3 - Article

AN - SCOPUS:85061209024

VL - 940

SP - 292

EP - 311

JO - Nuclear Physics B

JF - Nuclear Physics B

SN - 0550-3213

ER -

_{μ}− L

_{τ}model. Nuclear Physics B. 2019 Mar 1;940:292-311. https://doi.org/10.1016/j.nuclphysb.2019.01.016