Abstract

We analyse the interplay of generalised CP transformations and the non-Abelian discrete group T ′ and use the semi-direct product G f = T ′ ⋊H CP, as family symmetry acting in the lepton sector. The family symmetry is shown to be spontaneously broken in a geometrical manner. In the resulting flavour model, naturally small Majorana neutrino masses for the light active neutrinos are obtained through the type I see-saw mechanism. The known masses of the charged leptons, lepton mixing angles and the two neutrino mass squared differences are reproduced by the model with a good accuracy. The model allows for two neutrino mass spectra with normal ordering (NO) and one with inverted ordering (IO). For each of the three spectra the absolute scale of neutrino masses is predicted with relatively small uncertainty. The value of the Dirac CP violation (CPV) phase δ in the lepton mixing matrix is predicted to be δ = π/2 or 3π/2. Thus, the CP violating effects in neutrino oscillations are predicted to be maximal (given the values of the neutrino mixing angles) and experimentally observable. We present also predictions for the sum of the neutrino masses, for the Majorana CPV phases and for the effective Majorana mass in neutrinoless double beta decay. The predictions of the model can be tested in a variety of ongoing and future planned neutrino experiments.

Highlights

  • We analyse the interplay of generalised CP transformations and the nonAbelian discrete group T and use the semi-direct product Gf = T HCP, as family symmetry acting in the lepton sector

  • After some general remarks about the connection between the T and CP symmetries in section 2, we present in section 3 a fully consistent and explicit model of lepton flavour with a T family symmetry and geometrical CP violation

  • We give the values of the Dirac phase δ for two values of sin2 θ23 from its 3σ allowed range, sin2 θ23 = 0.50 and 0.60, and for the best fit values of sin2 θ12 and sin2 θ13: sin2 θ23 = 0.50 : cos δ = − 0.123, δ = 97.09◦ or 262.91◦ ; sin2 θ23 = 0.60 : cos δ = − 0.176, δ = 100.12◦ or 259.88◦. These results show that | sin δ|, which determines the magnitude of the CP violation effects in neutrino oscillations, exhibits very weak dependence on the value of sin2 θ23: for any value of sin2 θ23 from the interval 0.39 ≤ sin2 θ23 ≤ 0.60 we get | sin δ| ≥ 0.98

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Summary

T Symmetry and Generalised CP Transformations

We would like to clarify the role of a generalised CP transformation combined with the non-Abelian discrete symmetry group T. Let Gf = T HCP be the symmetry group acting in the lepton sector such that both T and HCP act on the lepton flavour space. Motivated by this study we will present a model where Gf is broken such that all lepton mixing angles and physical CP phases of the PMNS mixing matrix can be predicted in terms of two mixing angles and two phases. The breaking of Gf will be achieved through non zero vacuum expectation values (vevs) of some scalar fields, the so-called flavons

The consistency conditions
Transformation properties under generalised CP
Conditions to violate physical CP
The model
The flavon sector
The matter sector
The charged lepton sector
The neutrino sector
Comments about the θr
Geometrical CP violation and residual symmetries
Absolute neutrino mass scale
The mixing angles and Dirac CPV phase
The Majorana CPV phases
The neutrinoless double beta decay effective Majorana mass
Limiting cases
Summary and conclusions
A Technicalities about T
B Messenger sector
Full Text
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