Abstract

We study and compare various $Z'$ models arising from $SO(10)$, focussing in particular on the Abelian subgroup $U(1)_{R} \times U(1)_{B-L}$, broken at the TeV scale to Standard Model hypercharge $U(1)_{Y}$. The gauge group $U(1)_{R} \times U(1)_{B-L}$, which is equivalent to the $U(1)_{Y}\times U(1)_{\chi}$ in a different basis, is well motivated from $SO(10)$ breaking and allows neutrino mass via the linear seesaw mechanism. Assuming supersymmetry, we consider single step gauge unification to predict the gauge couplings, then consider the detection and characterisation prospects of the resulting $Z'$ at the LHC by studying its possible decay modes into di-leptons as well as into Higgs bosons. The main new result here is to analyse in detail the expected leptonic forward-backward asymmetry at the high luminosity LHC and show that it may be used to discriminate the $U(1)_{R} \times U(1)_{B-L}$ model from the usual $B-L$ model based on $U(1)_{Y}\times U(1)_{B-L}$.

Highlights

  • SOð10Þ grand unified theories (GUTs) are very attractive since they predict right-handed neutrinos and make neutrino mass inevitable

  • We review the Large Hadron Collider (LHC) results specific to the BLR model in Drell-Yan (DY) processes as well as in final states including Higgs bosons

  • Notice that Z0 decays into non-MSSM-like Higgs states can be heavily suppressed in comparison, in virtue of the fact that the additional CP-odd state not giving mass to the Z0 can be made arbitrarily heavy, a setup which we assume here, so that we refrain from accounting for these decay patterns

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Summary

INTRODUCTION

SOð10Þ grand unified theories (GUTs) are very attractive since they predict right-handed neutrinos and make neutrino mass inevitable. We shall not consider the high-energy SOð10Þ breaking here, so the starting point of the considered model is to assume that, below the GUT scale, we have the gauge group as on the right-hand side of Eq (3), namely, SUð3ÞC × SUð2ÞL × Uð1ÞR × Uð1ÞB−L ð4Þ. Note that in this basis the hypercharge gauge group Uð1ÞY of the SM is not explicitly present, instead it is “unified”.

Z0 COUPLINGS TO FERMIONS
Z0 COUPLINGS TO HIGGS BOSONS
RENORMALIZATION GROUP EQUATIONS
Preliminaries
Drell-Yan
Higgs final states
CONCLUSION
FvL mD ε1
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