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The flavor structures on magnetized orbifold models and 4D modular symmetric models

2024/03/26 by Shota Kikuchi, Kikuchi, Shota
Psychology · #FOS: Physical sciences #High Energy Physics - Phenomenology (hep-ph) #High Energy Physics - Theory (hep-th) #Phonetics and Phonology Research

paper · pdf · doi:10.48550/arxiv.2403.17280

openalex publication_date 2024/03/26 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/28

Abstract

We study quark and lepton flavor structures on magnetized T2/ℤ2 twisted orbifold model. There are 6,460 number of flavor models but most of them cannot lead to realistic flavor observables because of the difficulties on realizing mass hierarchies and small (large) mixing angles of quarks (leptons). We find that certain zero point patterns of zero-modes of fermions and Higgs fields give the flavor models being able to avoid these difficulties. We classify such flavor models and show numerical example. Next we study four-dimensional (4D) modular symmetric quark flavor models without fine-tuning. Mass matrices become hierarchical as close to the modular symmetric points depending on its residual charges. Actually the residual ZN symmetries with N≥ 6 can originate the large quark mass hierarchies. Also the products of residual symmetries such as Z3× Z3× Z3 have such possibility. We study the quark flavor model with Γ6 symmetry and A4× A4× A4 symmetry. We assume the vicinity of the cusp τ=i∞ where residual Z6 and Z3× Z3× Z3 symmetry remain. Consequently we find the models realizing the order of the quark mass ratios and the absolute values of the Cabibbo-Kobayashi-Maskawa (CKM) matrix elements without fine-tuning. Finally we construct the Siegel modular forms. Zero-modes on T6 at z=0 are the Siegel modular forms of weight 1/2 for the subgroup of Sp(6,ℤ). They have several moduli parameters and therefore have the possibility realizing the flavor structures including the CP phases. We study the Siegel modular forms transformed by \widetildeΔ(96) and show numerical example. We find one of moduli parameters ω1 works on the large mass hierarchies and ω2 works on the CP violation successfully in our model.

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