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
Summary
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
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