Constraints on $H^\pm$ parameter space in 2HDM at $\sqrt{s}=$ 8 TeV and $\sqrt{s}=$ 13 TeV

Ijaz Ahmed; Murad Badshah; Nadia Kausar

doi:10.1007/s10773-020-04572-4

paper

Constraints on $H^{\pm}$ parameter space in 2HDM at $s =$ 8 TeV and $s =$ 13 TeV

arXiv:2004.08418 · doi:10.1007/s10773-020-04572-4

Abstract

This paper reflects the heavy Higgs scenario where the mass of charged Higgs is equal to or greater than 200 GeV. The CMS observed and expected values of upper limits on the product $σ_{H}^{\pm} B R (H^{\pm} \to t b^{\mp})$ , assuming $H^{\pm} \to t b^{\mp} = 1$ , both at 8 TeV (at integrated luminosity of 19.7 $f b^{- 1}$ ) and 13 TeV (at integrated luminosity of 35.9 $f b^{- 1}$ ) c.m energies are used. By comparing these expected and observed upper limits with computational values , we find out the expected and observed exclusion regions of charged Higgs parameter space ( $m_{H}^{\pm} - t an β$ space ) in 2HDM both at $s =$ 8 and $s =$ 13 TeV. We compare the expected and observed exclusion regions and observe that exclusion regions made by observed upper limits are always greater than the exclusion made by expected upper limits both at 8 and 13 TeV c.m energies. Only in the mass range from 200 GeV to 220 GeV the expected exclusion region is greater than the observed one only at $s =$ 13 TeV. We also equate the exclusion regions at these two different center of mass energies and find that the expected exclusion region and observed exclusion region at $s =$ 13 TeV are always greater than the expected exclusion region and observed exclusion region at $S =$ 8 TeV respectively.

arXiv comment11 pages,19 figures,12 tables

Constraints on H± parameter space in 2HDM at s​= 8 TeV and s​= 13 TeV

Abstract

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Constraints on $H^{\pm}$ parameter space in 2HDM at $s =$ 8 TeV and $s =$ 13 TeV