Abstract

Leptonic CP violating phase δ CP in the light neutrino sector and leptogenesis via present matter-antimatter asymmetry of the Universe entails each other. Probing CP violation in light neutrino oscillation is one of the challenging tasks today. The reactor mixing angle θ 13 measured in reactor experiments, LBL, and DUNE with high precision in neutrino experiments indicates towards the vast dimensions of scope to detect δ CP . The correlation between leptonic Dirac CPV phase δ CP , reactor mixing angle θ 13 , lightest neutrino mass m 1 , and matter-antimatter asymmetry of the Universe within the framework of μ − τ symmetry breaking assuming the type I seesaw dominance is extensively studied here. Here, a SO(10) GUT model with flavor μ − τ symmetry is considered. In this work, the idea is to link baryogenesis through leptogenesis and the hint of CP violation in the neutrino oscillation data to a breaking of the mu-tau symmetry. Small tiny breaking of the μ − τ symmetry allows a large Dirac CP violating phase in neutrino oscillation which in turn is characterized by awareness of measured value of θ 13 and to provide a hint towards a better understanding of the experimentally observed near-maximal value of ν μ − ν τ mixing angle θ 23 ≃ π / 4 . Precise breaking of the μ − τ symmetry is achieved by adding a 120-plet Higgs to the 10 + 1 2 ¯ 6 -dimensional representation of Higgs. The estimated three-dimensional density parameter space of the lightest neutrino mass m 1 , δ CP , and reactor mixing angle θ 13 is constrained here for the requirement of producing the observed value of baryon asymmetry of the Universe through the mechanism of leptogenesis. Carrying out numerical analysis, the allowed parameter space of m 1 , δ CP , and θ 13 is found out which can produce the observed baryon to photon density ratio of the Universe.

Highlights

  • In 1950, Bruno Pontecorvo for the first time emphasized the idea of neutrino oscillations which resembled K0 − K 0 oscillations

  • We have used user-defined Dirac Neutrino Yukawa couplings [11] for the Yukawa interactions associated with the broken μ − τ symmetry model for the generation of nonzero reactor mixing angle θ13 and leptonic CP phase δCP in type I seesaw mechanism in the light of leptogenesis; there can be a transformation of the lepton asymmetry into a baryon asymmetry by nonperturbative B + L violating processes as discussed in [6]

  • The μ − τ symmetry upon spontaneously broken down through the 120 plets leads to nonzero reactor angle θ13, which in turn induces leptonic dirac CPV phase in the UPMNS matrix

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Summary

Introduction

In 1950, Bruno Pontecorvo for the first time emphasized the idea of neutrino oscillations which resembled K0 − K 0 oscillations.

Results
Conclusion
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