Abstract

Abstract Performing a fit to all publicly available data, we analyze the extent to which the latest results from the LHC and Tevatron constrain the couplings of the Higgs boson like state at ~ 125 GeV. To this end we assume that only Standard Model (SM) particles appear in the Higgs decays, but tree-level Higgs couplings to the up-quarks, down-quarks and vector bosons, relative to the SM are free parameters. We also assume that the leptonic couplings relative to the SM are the same as for the down-quark, and a custodial symmetry for the V = W, Z couplings. In the simplest approach, the effective Higgs couplings to gluons and photons are computed in terms of the previous parameters. This approach is also applied to Two-Higgs-Doublet Models of Type I and Type II. However, we also explore the possibility that the net Higgs to gg and γγ couplings have extra loop contributions coming from Beyond-the-Standard Model physics. We find that the SM p- value ~ 0.5 is more than 2σ away from fits in which: a) there is some non-SM contribution to the γγ coupling of the Higgs; or b) the sign of the top quark coupling to the Higgs is opposite that of the W coupling. In both these cases p-values ~ 0.9 can be achieved. Since option b) is difficult to realize in realistic models, it would seem that new physics contributions to the effective couplings of the Higgs are preferred.

Highlights

  • JHEP02(2013)053 the Higgs sector is as simple as envisioned in the SM

  • We explore the possibility that the net Higgs to gg and γγ couplings have extra loop contributions coming from Beyond-the-Standard Model physics

  • For a first test of the SM nature of the observed Higgs boson, we take CU = CD = CV = 1 but we allow for additional new physics contributions to the γγ and gg couplings, parameterized by ∆Cg and ∆Cγ, coming from loops involving non-SM particles or from anomalies

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Summary

Introduction

JHEP02(2013)053 the Higgs sector is as simple as envisioned in the SM. In particular it is crucial to determine the Higgs couplings to gauge bosons and to fermions as defined by the Lagrangian. This approach, when we allow in the most general case for the CU , CD, CV , Cγ and Cg couplings to be fully independent, encompasses a very broad range of models, including in particular those in which the Higgs sector consists of any number of doublets + singlets, the only proviso being the absence of decays of the observed ∼ 125 GeV state to non-SM final states.

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