Abstract
We study the modular invariance in magnetized torus models. Modular invariant flavor model is a recently proposed hypothesis for solving the flavor puzzle, where the flavor symmetry originates from modular invariance. In this framework coupling constants such as Yukawa couplings are also transformed under the flavor symmetry. We show that the low-energy effective theory of magnetized torus models is invariant under a specific subgroup of the modular group. Since Yukawa couplings as well as chiral zero modes transform under the modular group, the above modular subgroup (referred to as modular flavor symmetry) provides a new type of modular invariant flavor models with $D_4 \times \mathbb{Z}_2$, $(\mathbb{Z}_4 \times \mathbb{Z}_2) \rtimes \mathbb{Z}_2$, and $(\mathbb{Z}_8 \times \mathbb{Z}_2) \rtimes \mathbb{Z}_2$. We also find that conventional discrete flavor symmetries which arise in magnetized torus model are non-commutative with the modular flavor symmetry. Combining both two symmetries we obtain a larger flavor symmetry, where the conventional flavor symmetry is a normal subgroup of the whole group.
Highlights
The origin of the flavor structure of the quarks and leptons is a long-standing problem
We find that conventional discrete flavor symmetries which arise in magnetized torus model are noncommutative with the modular flavor symmetry
We have investigated the modular symmetry of the magnetized torus
Summary
The origin of the flavor structure of the quarks and leptons is a long-standing problem. These results have been used to investigate the property of the modular transformation for each component [42,43,44,45,46], and it is found that the Yukawa couplings as well as the chiral zero modes form a representation of the modular group It still remains unclear whether the full effective action including the Yukawa term is modular invariant. The generators of the Yukawa invariant modular subgroup form a new type of flavor symmetry referred to as modular flavor symmetry, such as Z2, D4 × Z2, ðZ4 × Z2Þ ⋊ Z2, and ðZ8 × Z2Þ ⋊ Z2 depending on the value of magnetic fluxes.
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