Abstract

The possibility of a light charged Higgs boson $H^\pm$ that decays predominantly to quarks ($cs$ and/or $cb$) and with a mass in the range 80 GeV $\le m_{H^\pm} \le 90$ GeV is studied in the context of Three-Higgs-Doublet Models (3HDMs). At present the Large Hadron Collider (LHC) has little sensitivity to this scenario, and currently the best constraints are from LEP2 and Tevatron searches. The branching ratio of $H^\pm\to cb$ can be dominant in two of the five types of 3HDM, and we determine the parameter space where this occurs. The decay $H^\pm\to cb$ has recently been searched for at the LHC for the first time, and with increased integrated luminosity one would expect sensitivity to the region 80 GeV $\le m_{H^\pm} \le 90$ GeV due to the smaller backgrounds with respect to $H^\pm\to cs$ decays.

Highlights

  • In 2012, the ATLAS and CMS Collaborations of the Large Hadron Collider (LHC) announced the discovery of a new particle with a mass of around 125 GeV [1,2]

  • In the 2HDM (Type III), in which fermions receive their masses from both vacuum expectation values (VEVs), the Yukawa couplings of HÆ depend on more parameters than in the Aligned 2HDM and a large BRðHÆ → cbÞ can be obtained [33]

  • We only consider mHÆ < mt, and results will be presented for the cases of mHÆ 1⁄4 85 GeV and mHÆ 1⁄4 130 GeV

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Summary

INTRODUCTION

In 2012, the ATLAS and CMS Collaborations of the Large Hadron Collider (LHC) announced the discovery of a new particle with a mass of around 125 GeV [1,2]. It is possible that it is the first scalar to be discovered from a nonminimal Higgs sector, which contains additional scalar isospin doublets or higher representations such as scalar isospin triplets. In such a scenario, future measurements of. As pointed out in previous works [6,7,8,9,10], in a 3HDM there is a phenomenologically attractive possibility of an HÆ being light (mHÆ < mt) and having a large BR for the decay channel HÆ → cb, a scenario which would not be expected in a. The constraints on the fermionic couplings are summarized, and explicit formulae for the BRs of the decay of HÆ to fermions are given

Fermionic couplings of HÆ in the 3HDM
The Branching Ratios of HÆ
Tevatron searches
LHC searches
RESULTS
CONCLUSIONS
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