Abstract

Abstract We study a renormalizable supersymmetric (SUSY) $SO(10)$ grand unified theory model where the Yukawa couplings of single ${\bf 10}$, single ${\bf \overline{126}}$, and single ${\bf 120}$ fields ($Y_{10}$, $Y_{126}$, and $Y_{120}$) account for the quark and lepton Yukawa couplings and the neutrino mass. We pursue the possibility that $Y_{10}$, $Y_{126}$, and $Y_{120}$ reproduce the correct quark and lepton masses, Cabibbo–Kobayashi–Maskawa and Pontecorvo–Maki–Nakagawa–Sakata (PMNS) matrices and neutrino mass differences, and at the same time suppress dimension-5 proton decays (proton decays via colored Higgsino exchange) through their texture, so that the soft SUSY-breaking scale can be reduced as much as possible without conflicting the current experimental bound on proton decays. We perform a numerical search for such a texture, and investigate implications of that texture on unknown neutrino parameters, the Dirac CP phase of the PMNS matrix, the lightest neutrino mass, and the $(1,1)$-component of the neutrino mass matrix in the charged lepton basis. Here we concentrate on the case when the active neutrino mass is generated mostly by the Type-2 seesaw mechanism, in which case we can obtain predictions for the neutrino parameters from the condition that dimension-5 proton decays be suppressed as much as possible.

Highlights

  • The SO(10) grand unified theory (GUT) [1, 2] is a well-motivated scenario beyond the Standard Model (SM), since it unifies the SM gauge groups into an anomaly-free group, it unifies the SM matter fields and the right-handed neutrino of each generation into one 16 representation, and it accommodates the seesaw mechanism for the tiny neutrino mass [3, 4, 5, 6, 7]

  • The present paper focuses on the case when the active neutrino mass is dominated by the Type-2 seesaw contribution coming from the tiny vacuum expectation value (VEV) of 126 field, whereas the Type-1 seesaw contribution resulting from integrating out right-handed neutrinos is assumed subdominant

  • We search for the texture of the Yukawa couplings Y10, Y126, Y120 discussed in Section 3, i.e., the texture which reproduces the correct quark and lepton Yukawa couplings and neutrino mass matrix according to Eqs. (3)-(5),(7) and in which the components of Yukawa couplings (Y10)uRdR, (Y126)uRdR, (Y10)uRsR, (Y126)uRsR, (Y10)uLdL, (Y126)uLdL, (Y10)uLuL, (Y126)uLuL, (Y10)uLsL, (Y126)uLsL are reduced

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Summary

Introduction

The SO(10) grand unified theory (GUT) [1, 2] is a well-motivated scenario beyond the Standard Model (SM), since it unifies the SM gauge groups into an anomaly-free group, it unifies the SM matter fields and the right-handed neutrino of each generation into one 16 representation, and it accommodates the seesaw mechanism for the tiny neutrino mass [3, 4, 5, 6, 7]. We perform a numerical search for such a texture in the model that includes single 10, single 126 and single 120 fields, by the following steps We spot those components of the Yukawa matrices Y10, Y126, Y120 (proportional to Y10, Y126, Y120) which can be reduced to suppress dimension-5 proton decays without conflicting the requirement that they reproduce the correct quark and lepton Yukawa couplings and neutrino mass matrix. We numerically fit the experimental data on the quark and lepton masses, CKM and PMNS mixing matrices and neutrino mass differences in terms of Y10, Y126, Y120, and we minimize the components of Y10, Y126, Y120 spotted above In this way, we numerically discover a texture of the fundamental Yukawa couplings that suppresses dimension-5 proton decays and reproduces the correct fermion data. Gives rise to dimension-5 operators inducing a proton decay

A R are proportional to
Components of the Yukawa matrices that can be reduced
Procedures
Results
Summary
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