Abstract
With the current measurements performed by CMS and ATLAS experiments, the light charged Higgs scenario ($m_{H^{\pm}}$ $<$ 160 GeV), is excluded for most of the parameter space in the context of MSSM. However, there is still possibility to look for heavy charged Higgs boson particularly in the $s$-channel single top production process where the charged Higgs may appear as a heavy resonance state and decay to $t\bar{b}$. The production process under consideration in this paper is $pp \ra H^{\pm} \ra t\bar{b}~+~h.c.$, where the top quark decays to $W^{+}b$ and $W^{+}$ boson subsequently decays to two light jets. It is shown that despite the presence of large QCD and electroweak background events, the charged Higgs signal can be extracted and observed at a large area of MSSM parameter space ($m_{H^{\pm}}$,tan$\beta$) at LHC. The observability of charged Higgs is potentially demonstrated with 5$\sigma$ contours and $95\%$ confidence level exclusion curves at different integrated LHC luminosities assuming a nominal center of mass energy of $\sqrt{s}$ = 14 TeV.
Highlights
Attempts towards extending the SM scalar sector resulted in the Two Higgs Doublet Model (2HDM) [4,5,6,7], the Minimal Supersymmetric Standard Model (MSSM) [8,9,10] and Next to Minimal Sypersymmetric Standard Model (NMSSM) [11,12].The discovery of another scalar boson, neutral or charged, would serve as unambiguous evidence for the new physics beyond the SM
The couplings of the charged Higgs boson to up-type quarks are proportional to cotβ while the charged Higgs boson couplings to the down-type quarks and charged leptons are proportional to tanβ, where tanβ is defined as the ratio of the vacuum expectation values of the two Higgs boson doublet fields
The aim of this paper is to study the s−channel single top in the chain pp → H ± → tb → bbW → bbj1 j2 at LHC using new techniques and generators focusing on the charged Higgs mass in the available area of the parameter space which has not yet been excluded by LHC data, i.e., 200 < m H± < 400 GeV
Summary
Attempts towards extending the SM scalar sector resulted in the Two Higgs Doublet Model (2HDM) [4,5,6,7], the Minimal Supersymmetric Standard Model (MSSM) [8,9,10] and Next to Minimal Sypersymmetric Standard Model (NMSSM) [11,12]. The MSSM used as a benchmark in this paper is a special case of Type-II 2HDM This model leads to five physical Higgs bosons: light and heavy CP-even Higgs bosons, h and H, a CP-odd Higgs boson, A, and two charged Higgs bosons, H ±. If the mass of charged Higgs m H± is smaller than the mass difference between top and bottom quarks, m H± < mt − mb, the dominant production mechanism for the charged Higgs is via top quark decay: t → bH ±. In [21,22], the s-channel single top has been considered as a source of charged Higgs production and decay to tbwhere the W boson from the top quark decay, undergoes a hadronic decay to a pair of light jets. This benchmark point provides the largest parameter space in the mh direction and conservative exclusion limits for tanβ
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