Abstract

In the framework of the representation theory of finite groups, it was recently shown that a fully constrained complex-symmetric mass matrix can be conveniently mapped into a sextet of $\Sigma(72\times3)$. In this paper, we introduce an additional flavor group $X_{24}$ in the model so that the vacuum alignment of the $\Sigma(72\times3)$ sextet is determined not only by the symmetries of $\Sigma(72\times3)$ but also by that of $X_{24}$. We define several flavons which transform as multiplets under $\Sigma(72\times3)$ as well as $X_{24}$. The vacuum alignment of each of these flavons is obtained as a simultaneous invariant eigenstate of specific elements of the groups $\Sigma(72\times3)$ and $X_{24}$; i.e.,~the vacuum alignment is fully determined by its residual symmetries. These flavons couple together uniquely resulting in the fully constrained sextet of $\Sigma(72\times3)$. Through this work we propose a general formalism in which the flavor symmetry group ($G_f$) is obtained as the direct product, $G_f=G_r \times G_x$. Fermions transform nontrivially only under $G_r$ while they remain invariant under $G_x$. Flavons, on the other hand, transform nontrivially under both $G_r$ and $G_x$. The vacuum alignment of each flavon multiplet transforming irreducibly under $G_r \times G_x$ is uniquely identified by its corresponding residual symmetry (a subgroup of $G_r \times G_x$). Several such flavons couple together to form an effective multiple of $G_r$ which remains invariant under $G_x$. This effective multiplet couples to the fermions.

Highlights

  • More than two decades [1] of experiments in neutrino oscillations have provided us with measurements of the neutrino mixing angles θ12, θ23, θ13 as well as the masssquared differences, Δm221, Δm231 [2,3]

  • We argue that the orientations of the neutrino basis states as well as the flavon vacuum expectation value (VEV) should be uniquely specifiable in terms of the residual symmetries that form subgroups of the discrete flavor group

  • We showed that a fully constrained Majorana mass matrix can be constructed using a sextet of Σð72 × 3Þ

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Summary

INTRODUCTION

More than two decades [1] of experiments in neutrino oscillations have provided us with measurements of the neutrino mixing angles θ12, θ23, θ13 as well as the masssquared differences, Δm221, Δm231 [2,3]. CP violation in neutrino sector, nature of neutrinos (Majorana or Dirac), and existence of sterile neutrinos are some of them Parameters such as the light neutrino mass and the complex phases in the mixing matrix need to be measured. Many of these questions are expected to be resolved by future experiments in the coming decades [4,5,6,7,8,9,10]. Which leads to TφM with φ 1⁄4 Æπ=16, was proposed [27] shortly after the discovery of nonzero θ13 by the Daya Bay experiment These matrices are fully constrained in the sense that they do not contain free parameters. In the Majorana mass term, two of these conjugate triplets couple to produce a conjugate sextet, pffiffi pffiffi

SijkνRj
CA: ξ3
VACUUM ALIGNMENT IN FLAVOR SPACE
THE DISCRETE GROUP X24
THE MODEL
THE FLAVON VACUUM ALIGNMENTS
THE NEW FRAMEWORK
SUMMARY
Example 1
Example 2
Full Text
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