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LHC-scale left-right symmetry and unification

2013/11/19 by Carolina Arbeláez, Martin Hirsch, M. Hirsch +2 · 1 citation
Mathematics · Physics and Astronomy · #Computer science #Gauge (firearms) #Gauge symmetry #Gauge theory #Geometry #Grand Unified Theory #High-Energy Particle Collisions Research #Large Hadron Collider #Mathematics #Neutrino Physics Research #Particle physics #Particle physics theoretical and experimental studies #Physics #Physics beyond the Standard Model #Programming language #Proton decay #Quark #Scale (ratio) #Standard Model (mathematical formulation) #Supersymmetry #Symmetry (geometry) #Symmetry breaking #Theoretical physics #Top quark #Unification #hep-ph

paper · pdf · doi:10.1103/physrevd.89.035002

published as Phys. Rev. D 89, 035002 (2014)

arxiv created 2013/11/19 · openalex publication_date 2014/02/07 · arxiv updated 2014/02/12 · openalex created_date 2025/10/10 · openalex updated_date 2026/08/05

Abstract

We construct a comprehensive list of nonsupersymmetric standard model extensions with a low-scale left-right (LR)-symmetric intermediate stage that may be obtained as simple low-energy effective theories within a class of renormalizable SO(10) grand unified theories. Unlike the traditional ``minimal'' LR models many of our example settings support a perfect gauge coupling unification even if the LR scale is in the LHC domain at a price of only (a few copies of) one or two types of extra fields pulled down to the TeV-scale ballpark. We discuss the main aspects of a potentially realistic model building conforming the basic constraints from the quark and lepton sector flavor structure, proton decay limits, etc. We pay special attention to the theoretical uncertainties related to the limited information about the underlying unified framework in the bottom-up approach, in particular, to their role in the possible extraction of the LR-breaking scale. We observe a general tendency for the models without new colored states in the TeV domain to be on the verge of incompatibility with the proton stability constraints.

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