Abstract

While current ATLAS and CMS measurements exclude a light charged Higgs ($m_{H^\pm}<160$ GeV) for most of the parameter region in the context of the MSSM scenarios, these bounds are significantly weakened in the Type II 2HDM once the exotic decay channel into a lighter neutral Higgs, $H^\pm \to AW/HW$, is open. In this study, we examine the possibility of a light charged Higgs produced in top decay via single top or top pair production, with the subsequent decay $H^\pm \rightarrow AW/HW$, which can reach a sizable branching fraction at low $\tan\beta$ once it is kinematically permitted. With a detailed collider analysis, we obtain exclusion and discovery bounds for the 14 TeV LHC assuming the existence of a 70 GeV neutral scalar. Assuming ${\rm BR}(H^\pm \rightarrow AW/HW)=100\%$ and ${\rm BR}(A/H \rightarrow \tau\tau)=8.6\%$, the 95% exclusion limits on ${\rm BR}(t \rightarrow H^+ b)$ are about 0.2% and 0.03% for single top and top pair production respectively, with an integrated luminosity of 300 ${\rm fb}^{-1}$. The discovery reaches are about 3 times higher. In the context of the Type II 2HDM, discovery is possible at both large $\tan\beta > 17$ for 155 GeV $< m_{H^\pm} <$ 165 GeV, and small $\tan\beta < 6$ over the entire mass range. Exclusion is possible in the entire $\tan\beta$ versus $m_{H^\pm}$ plane except for charged Higgs masses close to the top threshold. The exotic decay channel $H^\pm \to AW/HW$ is therefore complementary to the conventional $H^\pm \rightarrow \tau\nu$ channel.

Highlights

  • While current ATLAS and CMS measurements exclude a light charged Higgs for most of the parameter region in the context of the MSSM scenarios, these bounds are significantly weakened in the Type II 2HDM once the exotic decay channel into a lighter neutral Higgs, H± → AW/HW, is open

  • We examine the possibility of a light charged Higgs produced in top decay via single top or top pair production, which is the most prominent production channel for a light charged Higgs at the LHC

  • For the benchmark point BP1 with H± → AW ±, the exclusion reach based on top pair production covers the entire parameter space, while discovery is possible for small tan β < 6 and large tan β > 18, independent of sin(β−α)

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Summary

Theoretical motivation

In the generic 2HDM, there are no mass relations between the charged scalars, the scalar and pseudoscalar states Both the decays H± → h0W and H± → AW can be accessible or even dominant in certain regions of the parameter space. In the left panel of figure 2, we show the contours of the branching fraction BR(H± → AW ) in the mH± − tan β plane assuming mA = 70 GeV, h0 being the SM-like Higgs and mH0 decoupled. This branching fraction dominates for values of tan β less than 10 to 30 for charged Higgs masses in the range between 155 GeV and 170 GeV. The authors of [47, 48] have shown that decays of H± → AiW/HiW can be significant in certain regions of parameter space

Current limits
25 Type II 2HDM with mA 70 GeV
Collider analysis
Limits
Implication for the type II 2HDM
Findings
Conclusion
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