Abstract

We study the lepton flavor models, whose flavor symmetries are finite subgroups of the modular group such as $S_3$ and $A_4$. In our models, couplings are also nontrivial representations of these groups and modular functions of the modulus. We study the possibilities that these models realize realistic values of neutrino masses and lepton mixing angles.

Highlights

  • One of the unsolved but important mysteries in particle physics is the mystery about the flavor structure of the quarks and leptons, such as the generation number, mass hierarchy, and mixing angles

  • Many models have been proposed imposing non-Abelain discrete flavor symmetries, e.g., S3, A4, S4 and other various finite groups. (See for review [1,2,3,4].) In particular, the lepton sector has been intensively studied, because at least two of three lepton mixing angles are large compared with the quark mixing angles, and their experimental results have been improved precisely

  • In Appendix, we briefly review modular functions and show modular functions corresponding to the A4 triplet and the S3 doublet

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Summary

INTRODUCTION

One of the unsolved but important mysteries in particle physics is the mystery about the flavor structure of the quarks and leptons, such as the generation number, mass hierarchy, and mixing angles. Such a mystery would provide us with hints to explore physics beyond the standard model. Modular transformations act nontrivially on string modes and interchange massless modes such as quarks and leptons to each other In this sense, modular symmetry is a non-Abelain discrete flavor symmetry. In Appendix, we briefly review modular functions and show modular functions corresponding to the A4 triplet and the S3 doublet

MODULAR TRANSFORMATION AND ITS SUBGROUP SYMMETRIES
Experimental values
General setup of our models
A4 MODEL
Λ ðHuHuLLYðτÞÞ1: ð27Þ
Normal ordering in A4 model
S3 MODEL
Normal ordering in S3 models
Model 1
Model 2
CONCLUSION
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