Modular S4S_4 and A4A_4 Symmetries and Their Fixed Points: New Predictive Examples of Lepton Mixing

preprint2026arXivOpen access

Abstract

In the modular symmetry approach to neutrino models, the flavour symmetry emerges as a finite subgroup ΓNΓ_N of the modular symmetry, broken by the vacuum expectation value (VEV) of a modulus field ττ. If the VEV of the modulus ττ takes some special value, a residual subgroup of ΓNΓ_N would be preserved. We derive the fixed points τS=iτ_S=i, τST=(−1+i3)/2τ_{ST}=(-1+i\sqrt{3})/2, τTS=(1+i3)/2τ_{TS}=(1+i\sqrt{3})/2, τT=i∞τ_T=i\infty in the fundamental domain which are invariant under the modular transformations indicated. We then generalise these fixed points to τf=γτSτ_f=γτ_S, γτSTγτ_{ST}, γτTSγτ_{TS} and γτTγτ_{T} in the upper half complex plane, and show that it is sufficient to consider γ∈ΓNγ\inΓ_{N}. Focussing on level N=4N=4, corresponding to the flavour group S4S_4, we consider all the resulting triplet modular forms at these fixed points up to weight 6. We then apply the results to lepton mixing, with different residual subgroups in the charged lepton sector and each of the right-handed neutrinos sectors. In the minimal case of two right-handed neutrinos, we find three phenomenologically viable cases in which the light neutrino mass matrix only depends on three free parameters, and the lepton mixing takes the trimaximal TM1 pattern for two examples. One of these cases corresponds to a new Littlest Modular Seesaw based on CSD(n)(n) with n=1+6≈3.45n=1+\sqrt{6}\approx 3.45, intermediate between CSD(3)(3) and CSD(4)(4). Finally, we generalize the results to examples with three right-handed neutrinos, also considering the level N=3N=3 case, corresponding to A4A_4 flavour symmetry.

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