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Predictions of the Higgs mass and the weak mixing angle in the 6D gauge-Higgs unification

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arxiv 1509.04818 v4 pith:UO4M2UKY submitted 2015-09-16 hep-ph hep-th

classification hep-phhep-th
keywords higgsmassweakanglegaugegauge-higgsmixingpredicted
verification ladder T0 review T1 audit T2 compute T3 formal
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abstract

In the gauge-Higgs unification with multiple extra spaces, the Higgs self-coupling is of the order of $g^2$ and Higgs is predicted to be light, being consistent with the LHC results. When the gauge group is simple, the weak mixing angle is also predictable. We address a question whether there exists a model of gauge-Higgs unification in 6-dimensional space-time, which successfully predicts the mass ratios of the Higgs boson and weak gauge bosons. First, by use of a useful formula we give a general argument on the condition to get a realistic prediction of the weak mixing angle $sin^{2}theta_{W} = 1/4$, and find that triplet and sextet representations of the minimal SU(3) gauge group lead to the realistic prediction. Concerning the Higgs mass, we notice that in the models with one Higgs doublet, the predicted Higgs mass is always the same: $M_H = 2 M_W$. However, by extending our discussion to the models with two Higgs doublets, the situation changes: we obtain an interesting prediction $M_{H} leq 2M_{W}$ at the leading order of the perturbation. Thus it is possible to recover the observed Higgs mass, 125 GeV, for a suitable choice of the parameter. The situation is in clear contrast to the case of the minimal supersymmetric standard model, where $M_{H} leq M_{Z}$ at the classical level and the predicted Higgs mass cannot recover the observed value.

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Cited by 2 Pith papers

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  1. Models with rank-reducing discrete boundary conditions on $T^2/{\mathbb Z}_4$

    hep-ph 2025-02 conditional novelty 6.0 of 10

    An SU(6) gauge-Higgs unification model on T^2/Z4 with rank-reducing boundary conditions yields two Higgs doublets from the gauge field, quark unification in a 15, and a vacuum with small electroweak breaking via the H...

  2. Gauge symmetry breaking with $S^2$ extra dimensions

    hep-ph 2025-05 conditional novelty 5.0 of 10

    On S2, a cos θ background gauge field breaks the gauge group to its centralizer; the KK mass spectrum is (j(j+1) - kα^2)/R^2 for charged modes.

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