Pati–Salam unification from noncommutative geometry and the TeV-scale WR boson

We analyze the running at one-loop of the gauge couplings in the spectral PatiSalam model that was derived in the framework of noncommutative geometry. There are a few different scenarios for the scalar particle content which are determined by the precise form of the Dirac operator for the finite noncommutative space. We consider these different scenarios and establish for all of them unification of the Pati-Salam gauge couplings. The boundary conditions are set by the usual RG flow for the Standard Model couplings at an intermediate mass scale at which the Pati-Salam symmetry is broken.

Section: Jhep11(2015)011supporting

confidence: 73%

Grand unification in the spectral Pati-Salam model

Chamseddine

Connes

Suijlekom

2015

“…-Make the first-order condition more flexible, as investigated in [17,18], with phenomenological consequences in [33] (see also [34]). …”

Section: Jhep03(2018)089mentioning

confidence: 99%

Lorentz signature and twisted spectral triples

Devastato

Farnsworth

Lizzi

et al. 2018

“…1 Realization of a few TeV intermediate scale within the framework of grand unification is also discussed in refs. [65][66][67].…”

Section: The Modelmentioning

confidence: 99%

The ATLAS diboson resonance in non-supersymmetric SO(10)

Evans

Olive

Zheng

2016

SO(10) grand unification accommodates intermediate gauge symmetries with which gauge coupling unification can be realized without supersymmetry. In this paper, we discuss the possibility that a new massive gauge boson associated with an intermediate gauge symmetry explains the excess observed in the diboson resonance search recently reported by the ATLAS experiment. The model we find has two intermediate symmetries,where the latter gauge group is broken at the TeV scale. This model achieves gauge coupling unification with a unification scale sufficiently high to avoid proton decay. In addition, this model provides a good dark matter candidates, whose stability is guaranteed by a Z 2 symmetry present after the spontaneous breaking of the intermediate gauge symmetries. We also discuss prospects for testing these models in the forthcoming LHC experiments and dark matter detection experiments.