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Axion and Right-handed Neutrino in the Minimal SUSY SO(10) Model

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arxiv hep-ph/0412373 v3 pith:Z6RUYMHF submitted 2004-12-24 hep-ph astro-ph

classification hep-phastro-ph
keywords axiondeltamodelright-handedsubsetbreakingequivlambda
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

The connection between the axion and right-handed neutrinos is explored in the framework of the minimal SUSY SO(10) model. The former is related to the Peccei-Quinn (PQ) solution to the strong CP problem and the latter is to the light Majorana neutrinos through the see-saw mechanism. In this model, a relative phase between $({\bf 10,1,3}) (\equiv {\bf \bar{\Delta}}_R) \subset {\bf \bar{126}}$ and $({\bf \bar{10},1,3}) (\equiv {\bf \Delta}_R) \subset {\bf 126}$ multiplets of ${\rm SU}(4) \times {\rm SU}(2)_L \times {\rm SU}(2)_R \subset {\rm SO}(10)$ becomes a physical degree of freedom identified with the axion. Then, the PQ symmetry breaking scale ($\Lambda_{\rm PQ}$) and the $B-L$ symmetry breaking scale ($\Lambda_{\rm B-L}$) coincide through the VEV of ${\bf \bar{\Delta}}_R$. The scalar partner of the lightest right-handed neutrino is regarded as the inflaton, which gives a consistent density fluctuation for the CMB.

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  1. Five dimensional $SU(5) \times U(1)_{\rm PQ}$ grand unification

    hep-ph 2024-12 conditional novelty 5.0 of 10

    The authors propose a 5D SU(5) x U(1)_PQ orbifold model in which SU(5) breaking and a high-quality QCD axion from the fifth component of the U(1) field arise from the same boundary conditions, with intermediate-scale ...

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