Abstract

The even weight modular forms of level $N$ can be arranged into the common irreducible representations of the inhomogeneous finite modular group $\Gamma_N$ and the homogeneous finite modular group $\Gamma'_N$ which is the double covering of $\Gamma_N$, and the odd weight modular forms of level $N$ transform in the new representations of $\Gamma'_N$. We find that the above structure of modular forms can naturally generate texture zeros of the fermion mass matrices if we properly assign the representations and weights of the matter fields under the modular group. We perform a comprehensive analysis for the $\Gamma'_3\cong T'$ modular symmetry. The three generations of left-handed quarks are assumed to transform as a doublet and a singlet of $T'$, we find six possible texture zeros structures of quark mass matrix up to row and column permutations. We present five benchmark quark models which can produce very good fit to the experimental data. These quark models are further extended to include lepton sector, the resulting models can give a unified description of both quark and lepton masses and flavor mixing simultaneously although they contain less number of free parameters than the observables.

Highlights

  • The standard model (SM) of particle physics has been extensively tested

  • The even-weight modular forms of level N can be arranged into the common irreducible representations of the inhomogeneous finite modular group ΓN and the homogeneous finite modular group Γ0N which is the double covering of ΓN, and the odd-weight modular forms of level N transform in the new representations of Γ0N

  • We show that the above structure of modular forms can naturally produce texture zeros of the fermion mass matrices if we properly assign the representations and weights of the matter fields under the modular group

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Summary

INTRODUCTION

The standard model (SM) of particle physics has been extensively tested. neither significant evidence of departures from the SM nor convincing hints for the presence of new physics have been found. Several models of lepton masses and mixing have been constructed based on the finite modular groups Γ2 ≅ S3 [31,32,33,34], Γ3 ≅ A4 [11,31,32,35,36,37,38,39,40,41,42,43,44,45,46,47,48,49,50,51], Γ4 ≅ S4 [48,52,53,54,55,56,57,58], and Γ5 ≅ A5 [57,59,60] This new approach has been extended to modular forms of general integer weight which can be arranged into irreducible representations of the homogeneous finite modular group Γ0N [61]. Γ0N, and ρrðγÞ is the representation matrix of the element γ in the irreducible representation r

Modular forms of level 3
CCA pffiffi
General structure of S
General structures of C and R
Possible structures of the quark mass matrix
QUARK MASS MATRICES FOR SINGLET ASSIGNMENTS OF THE RIGHT-HANDED QUARKS
General structures of R0a and C0a
PHENOMENOLOGICALLY VIABLE MODELS FOR QUARK MASSES AND CKM MIXING
Numerical results
QUARK-LEPTON UNIFICATION
Lepton sector
NONMINIMAL KÄHLER POTENTIAL
VIII. CONCLUSION AND SUMMARY
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