Abstract

In this work we propose an extension to the Standard Model in which we consider a type-III two-Higgs-doublet model (2HDM) plus massive neutrinos and the horizontal flavor symmetry ${S}_{3}$ ($\ensuremath{\nu}2\mathrm{HDM}\ensuremath{\bigotimes}{S}_{3}$). In the above framework and with the explicit breaking of flavor symmetry ${S}_{3}$, the Yukawa matrices in the flavor-adapted basis are represented by means of a matrix with two texture zeros. Also, the active neutrinos are considered as Majorana particles and their masses are generated through the type-I seesaw mechanism. The unitary matrices that diagonalize the mass matrices, as well as the flavor-mixing matrices, are expressed in terms of fermion mass ratios. Consequently, in the mass basis the entries of the Yukawa matrices naturally acquire the form of the so-called Cheng-Sher ansatz. For the leptonic sector of $\ensuremath{\nu}2\mathrm{HDM}\ensuremath{\bigotimes}{S}_{3}$, we compare, through a ${\ensuremath{\chi}}^{2}$ likelihood test, the theoretical expressions of the flavor-mixing angles with the masses and flavor-mixing leptons current experimental data. The results obtained in this ${\ensuremath{\chi}}^{2}$ analysis are in very good agreement with the current experimental data. We also obtain allowed value ranges for the ``Dirac-like'' phase factor, as well as for the two Majorana phase factors. Furthermore, we study the phenomenological implications of these numerical values of the $CP$-violation phases on the neutrinoless double-beta decay, and for long baseline neutrino oscillation experiments such as T2K, $\mathrm{NO}\ensuremath{\nu}\mathrm{A}$, and DUNE.

Highlights

  • According to the most recent neutrino physics literature [1,2], there are still several unresolved issues, including whether the neutrinos are Dirac or Majorana fermions, the absolute neutrino mass scale, and the possible sources of charge-parity (CP) violation (CPV) in leptons

  • We have studied the theory of neutrino masses, mixings, and CPV as the realization of an S3 flavor symmetry in the framework of the type-III two-Higgs-doublet model

  • The explicit sequential breaking of flavor symmetry according to the chain Sj3L ⊗ Sj3R ⊃ Sd3iag ⊃ Sd2iag allowed us to represent the Yukawa matrices in the flavor basis with a Hermitian matrix with two texture zeros

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Summary

INTRODUCTION

According to the most recent neutrino physics literature [1,2], there are still several unresolved issues, including whether the neutrinos are Dirac or Majorana fermions, the absolute neutrino mass scale, and the possible sources of charge-parity (CP) violation (CPV) in leptons. In this work we will study the flavor dynamics through Yukawa matrices in the specific scenario of 2HDM-III plus massive neutrinos and a horizontal flavor symmetry S3 (ν2HDM ⊗ S3) In this context, under the action of the S3 flavor symmetry group the right-handed neutrinos as well as the two Higgs fields transform as singlets, while the active neutrinos are considered as Majorana particles and their masses are generated through the type-I seesaw mechanism. II we present the Yukawa Lagrangian in the ν2HDM ⊗ S3, and the form of the Dirac and Majorana fermion mass matrices in terms of its eigenvalues In this way, we derive explicit and analytical expressions for the leptonic flavor-mixing angles and Higgs-fermion couplings. Ð7Þ where vk are the vacuum expectation values of the two Higgs bosons Φk, with k 1⁄4 1, 2

Mass matrices from the S3 flavor symmetry
The mass and mixing matrices as functions of fermion masses
The mixing angle and CP violation phases
NUMERICAL ANALYSIS
The likelihood test χ 2
PHENOMENOLOGICAL IMPLICATIONS
Neutrinoless double-beta decay
CP violation in neutrino oscillations in matter
CONCLUSIONS

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