2021
DOI: 10.1103/physrevd.104.035035
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Semisimple extensions of the Standard Model gauge algebra

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Cited by 19 publications
(35 citation statements)
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“…Here G vert breaks to the SM gauge symmetry, while G horiz breaks ultimately to nothing, giving rise to heavy gauge bosons that mediate very weak flavour-changing forces. Curiously, if we want to fit all 48 Weyl fermions of the SM+3ν R into a single irrep R of a unified gauge group G that acts faithfully on matter, assuming G is connected and semi-simple, then the only options are G " Spinp10q tSU p2q or SOp3qu with R " p16, 3q [4]. 2 Both these are horizontal extensions of the Spinp10q GUT.…”
Section: Introductionmentioning
confidence: 99%
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“…Here G vert breaks to the SM gauge symmetry, while G horiz breaks ultimately to nothing, giving rise to heavy gauge bosons that mediate very weak flavour-changing forces. Curiously, if we want to fit all 48 Weyl fermions of the SM+3ν R into a single irrep R of a unified gauge group G that acts faithfully on matter, assuming G is connected and semi-simple, then the only options are G " Spinp10q tSU p2q or SOp3qu with R " p16, 3q [4]. 2 Both these are horizontal extensions of the Spinp10q GUT.…”
Section: Introductionmentioning
confidence: 99%
“…Recently, Ref. [4] classified all semi-simple Lie algebras g in which the SM+3ν R gauge algebra can be embedded without needing extra fermions. This list of algebras enumerates all possible ways in which flavour could be intertwined with the SM gauge interactions, albeit subject to the (not insignificant) assumption that there are no extra fermions beyond those of the SM+3ν R .…”
Section: Introductionmentioning
confidence: 99%
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