Flavor symmetries from modular subgroups in magnetized compactifications

A bstract We study the flavor structures of zero-modes, which are originated from the modular symmetry on $$ {T}_1^2\times {T}_2^2 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>T</mml:mi> <mml:mn>1</mml:mn> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo>×</mml:mo> <mml:msubsup> <mml:mi>T</mml:mi> <mml:mn>2</mml:mn> <mml:mn>2</mml:mn> </mml:msubsup> </mml:math> and its orbifold with magnetic fluxes. We introduce the constraint on the moduli parameters by τ 2 = Nτ 1 , where τ i denotes the complex structure moduli on $$ {T}_i^2 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>T</mml:mi> <mml:mi>i</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> </mml:math> . Such a constraint can be derived from the moduli stabilization. The modular symmetry of $$ {T}_1^2\times {T}_2^2 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>T</mml:mi> <mml:mn>1</mml:mn> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo>×</mml:mo> <mml:msubsup> <mml:mi>T</mml:mi> <mml:mn>2</mml:mn> <mml:mn>2</mml:mn> </mml:msubsup> </mml:math> is $$ \textrm{SL}{\left(2,\mathbb{Z}\right)}_{\tau_1}\times \textrm{SL}{\left(2,\mathbb{Z}\right)}_{\tau_2}\subset \textrm{Sp}\left(4,\mathbb{Z}\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>SL</mml:mi> <mml:msub> <mml:mfenced> <mml:mn>2</mml:mn> <mml:mi>ℤ</mml:mi> </mml:mfenced> <mml:msub> <mml:mi>τ</mml:mi> <mml:mn>1</mml:mn> </mml:msub> </mml:msub> <mml:mo>×</mml:mo> <mml:mi>SL</mml:mi> <mml:msub> <mml:mfenced> <mml:mn>2</mml:mn> <mml:mi>ℤ</mml:mi> </mml:mfenced> <mml:msub> <mml:mi>τ</mml:mi> <mml:mn>2</mml:mn> </mml:msub> </mml:msub> <mml:mo>⊂</mml:mo> <mml:mi>Sp</mml:mi> <mml:mfenced> <mml:mn>4</mml:mn> <mml:mi>ℤ</mml:mi> </mml:mfenced> </mml:math> and it is broken to Γ 0 ( N ) × Γ 0 ( N ) by the moduli constraint. The wave functions represent their covering groups. We obtain various flavor groups in these models.

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Publication Details

Journal
Journal of High Energy Physics
Published
2024-12-17
DOI
https://doi.org/10.1007/jhep12(2024)128
Citations
2
Primary Topic
Neutrino Physics Research
Type
article
Field-Weighted Citation Impact
1.32

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article

Flavor symmetries from modular subgroups in magnetized compactifications

Hajime Otsuka, Kaito Nasu, Shohei Takada, Tatsuo Kobayashi et al.
2 citations
Journal of High Energy Physics
Neutrino Physics Research
1.32
article

Flavor symmetries from modular subgroups in magnetized compactifications

Hajime Otsuka, Kaito Nasu, Shohei Takada, Tatsuo Kobayashi, Ryusei Nishida
article en
2 citations

Abstract

A bstract We study the flavor structures of zero-modes, which are originated from the modular symmetry on $$ {T}_1^2\times {T}_2^2 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>T</mml:mi> <mml:mn>1</mml:mn> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo>×</mml:mo> <mml:msubsup> <mml:mi>T</mml:mi> <mml:mn>2</mml:mn> <mml:mn>2</mml:mn> </mml:msubsup> </mml:math> and its orbifold with magnetic fluxes. We introduce the constraint on the moduli parameters by τ 2 = Nτ 1 , where τ i denotes the complex structure moduli on $$ {T}_i^2 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>T</mml:mi> <mml:mi>i</mml:mi> <mml:mn>2</mml:mn> </mml:msubsup> </mml:math> . Such a constraint can be derived from the moduli stabilization. The modular symmetry of $$ {T}_1^2\times {T}_2^2 $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msubsup> <mml:mi>T</mml:mi> <mml:mn>1</mml:mn> <mml:mn>2</mml:mn> </mml:msubsup> <mml:mo>×</mml:mo> <mml:msubsup> <mml:mi>T</mml:mi> <mml:mn>2</mml:mn> <mml:mn>2</mml:mn> </mml:msubsup> </mml:math> is $$ \textrm{SL}{\left(2,\mathbb{Z}\right)}_{\tau_1}\times \textrm{SL}{\left(2,\mathbb{Z}\right)}_{\tau_2}\subset \textrm{Sp}\left(4,\mathbb{Z}\right) $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mi>SL</mml:mi> <mml:msub> <mml:mfenced> <mml:mn>2</mml:mn> <mml:mi>ℤ</mml:mi> </mml:mfenced> <mml:msub> <mml:mi>τ</mml:mi> <mml:mn>1</mml:mn> </mml:msub> </mml:msub> <mml:mo>×</mml:mo> <mml:mi>SL</mml:mi> <mml:msub> <mml:mfenced> <mml:mn>2</mml:mn> <mml:mi>ℤ</mml:mi> </mml:mfenced> <mml:msub> <mml:mi>τ</mml:mi> <mml:mn>2</mml:mn> </mml:msub> </mml:msub> <mml:mo>⊂</mml:mo> <mml:mi>Sp</mml:mi> <mml:mfenced> <mml:mn>4</mml:mn> <mml:mi>ℤ</mml:mi> </mml:mfenced> </mml:math> and it is broken to Γ 0 ( N ) × Γ 0 ( N ) by the moduli constraint. The wave functions represent their covering groups. We obtain various flavor groups in these models.

Journal of High Energy PhysicsVol. 2024(12)
Kyushu University (JP), Hokkaido University (JP)
Japan Society for the Promotion of Science
Openalex Percentile: Top 10%
Neutrino Physics Research
1.32
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