Axion in the minimal SO(10) GUT

A bstract The QCD axion is investigated within the minimal supersymmetric SO(10) grand unified theory, where the Yukawa sector involves Higgs multiplets 10 and $$ \overline{\textbf{126}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mn>126</mml:mn> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> . The relative phase between the VEVs of ( 10 , 1 , 3 ) ⊂ $$ \overline{\textbf{126}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mn>126</mml:mn> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> and ( $$ \overline{\textbf{10}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mn>10</mml:mn> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> , 1 , 3 ) ⊂ 126 under SU(4) C × SU(2) L × SU(2) R is identified with the axion. The axion is dominantly the relative phase between ∆ R and $$ {\overline{\Delta }}_R $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mover> <mml:mtext>∆</mml:mtext> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>R</mml:mi> </mml:msub> </mml:math> , with a small 10 -Higgs component due to the VEV hierarchy. The Peccei-Quinn and B − L symmetry breaking scales coincide through $$ \left|\left\langle {\Delta}_R\right\rangle \right|=\left|\left\langle {\overline{\Delta}}_R\right\rangle \right| $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mfenced> <mml:mfenced> <mml:msub> <mml:mi>Δ</mml:mi> <mml:mi>R</mml:mi> </mml:msub> </mml:mfenced> </mml:mfenced> <mml:mo>=</mml:mo> <mml:mfenced> <mml:mfenced> <mml:msub> <mml:mover> <mml:mi>Δ</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>R</mml:mi> </mml:msub> </mml:mfenced> </mml:mfenced> </mml:math> . The scalar partner of the lightest right-handed neutrino plays the role of the inflaton, realizing hybrid inflation consistent with the observed CMB density fluctuations. After inflation, both fields acquire VEVs, and the domain-wall problem is resolved through the Lazarides-Shafi mechanism, which naturally restricts the model to three generations.

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Journal
Journal of High Energy Physics
Published
2026-03-13
DOI
https://doi.org/10.1007/jhep03(2026)128
Primary Topic
Black Holes and Theoretical Physics
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article
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article

Axion in the minimal SO(10) GUT

Takeshi Fukuyama
Journal of High Energy Physics
Black Holes and Theoretical Physics
article

Axion in the minimal SO(10) GUT

Takeshi Fukuyama
article en

Abstract

A bstract The QCD axion is investigated within the minimal supersymmetric SO(10) grand unified theory, where the Yukawa sector involves Higgs multiplets 10 and $$ \overline{\textbf{126}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mn>126</mml:mn> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> . The relative phase between the VEVs of ( 10 , 1 , 3 ) ⊂ $$ \overline{\textbf{126}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mn>126</mml:mn> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> and ( $$ \overline{\textbf{10}} $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mover> <mml:mn>10</mml:mn> <mml:mo>¯</mml:mo> </mml:mover> </mml:math> , 1 , 3 ) ⊂ 126 under SU(4) C × SU(2) L × SU(2) R is identified with the axion. The axion is dominantly the relative phase between ∆ R and $$ {\overline{\Delta }}_R $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:msub> <mml:mover> <mml:mtext>∆</mml:mtext> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>R</mml:mi> </mml:msub> </mml:math> , with a small 10 -Higgs component due to the VEV hierarchy. The Peccei-Quinn and B − L symmetry breaking scales coincide through $$ \left|\left\langle {\Delta}_R\right\rangle \right|=\left|\left\langle {\overline{\Delta}}_R\right\rangle \right| $$ <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"> <mml:mfenced> <mml:mfenced> <mml:msub> <mml:mi>Δ</mml:mi> <mml:mi>R</mml:mi> </mml:msub> </mml:mfenced> </mml:mfenced> <mml:mo>=</mml:mo> <mml:mfenced> <mml:mfenced> <mml:msub> <mml:mover> <mml:mi>Δ</mml:mi> <mml:mo>¯</mml:mo> </mml:mover> <mml:mi>R</mml:mi> </mml:msub> </mml:mfenced> </mml:mfenced> </mml:math> . The scalar partner of the lightest right-handed neutrino plays the role of the inflaton, realizing hybrid inflation consistent with the observed CMB density fluctuations. After inflation, both fields acquire VEVs, and the domain-wall problem is resolved through the Lazarides-Shafi mechanism, which naturally restricts the model to three generations.

Journal of High Energy PhysicsVol. 2026(3)
The University of Osaka (JP)
Openalex Percentile: Top 23%
Black Holes and Theoretical Physics
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