Constraints on $H^\pm$ parameter space in 2HDM at $\sqrt{s}=$ 8 TeV and $\sqrt{s}=$ 13 TeV
international Journal of Theoretical Physics Volume 59 Issue 7, September 2020 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 $\sigma_H^\pm BR(H^\pm \rightarrow tb^\...
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Zusammenfassung: | international Journal of Theoretical Physics Volume 59 Issue 7,
September 2020 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 $\sigma_H^\pm BR(H^\pm \rightarrow tb^\mp)$,
assuming $H^\pm \rightarrow tb^\mp=1$, both at 8 TeV (at integrated luminosity
of 19.7 $fb^{-1}$ ) and 13 TeV (at integrated luminosity of 35.9 $fb^{-1}$ )
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 - tan\beta $ space ) in
2HDM both at $\sqrt{s}=$8 and $\sqrt{s}=$ 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 $\sqrt{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 $\sqrt{s}=$13 TeV are always greater than the
expected exclusion region and observed exclusion region at $\sqrt{S}=$8 TeV
respectively. |
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DOI: | 10.48550/arxiv.2004.08418 |