Limits on the charged Higgs parameters in the two Higgs doublet model using CMS $$\sqrt{s}=13$$ s=13 TeV results

Abstract The latest CMS results on the upper limits on $$\sigma _{H^\pm }$$ σH± BR($$H^\pm \rightarrow \tau ^\pm \nu )$$ H±→τ±ν) and $$\sigma _{H^\pm }$$ σH± BR($$H^+ \rightarrow t{\bar{b}}$$ H+→tb¯ ) for $$\sqrt{s}=13$$ s=13 TeV at an integrated luminosity of 35.9 $$\hbox {fb}^{-1}$$ fb-1 are used...

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Main Author: Prasenjit Sanyal
Format: Article
Language:English
Published: SpringerOpen 2019-11-01
Series:European Physical Journal C: Particles and Fields
Online Access:http://link.springer.com/article/10.1140/epjc/s10052-019-7431-y
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spelling doaj-5d452aa8558143e4b7cc671aa16c28222020-11-25T04:02:17ZengSpringerOpenEuropean Physical Journal C: Particles and Fields1434-60441434-60522019-11-0179111910.1140/epjc/s10052-019-7431-yLimits on the charged Higgs parameters in the two Higgs doublet model using CMS $$\sqrt{s}=13$$ s=13 TeV resultsPrasenjit Sanyal0Department of Physics, Indian Institute of Technology KanpurAbstract The latest CMS results on the upper limits on $$\sigma _{H^\pm }$$ σH± BR($$H^\pm \rightarrow \tau ^\pm \nu )$$ H±→τ±ν) and $$\sigma _{H^\pm }$$ σH± BR($$H^+ \rightarrow t{\bar{b}}$$ H+→tb¯ ) for $$\sqrt{s}=13$$ s=13 TeV at an integrated luminosity of 35.9 $$\hbox {fb}^{-1}$$ fb-1 are used to impose constraints on the charged Higgs $$H^\pm $$ H± parameters within the Two Higgs Doublet Model (2HDM). The 2HDM is the simplest extension of the Standard Model (SM) under the same gauge symmetry to contain charged Higgs and is relatively little constrained compared to the Minimal Supersymmetric Standard Model (MSSM). The latest results lead to much more stringent constraints on the charged Higgs parameter space than for the earlier 8 TeV results. The CMS collaboration also studied the exotic bosonic decays $$H^\pm \rightarrow W^\pm A$$ H±→W±A and $$A \rightarrow \mu ^+ \mu ^-$$ A→μ+μ- for the first time and put upper limits on the BR($$t\rightarrow H^+ b$$ t→H+b ) for the light charged Higgs boson. These constraints lead to the exclusion of parameter space which is not excluded by the $$\tau \nu $$ τν channel. For comparison the exclusion regions from flavor physics constraints are also discussed.http://link.springer.com/article/10.1140/epjc/s10052-019-7431-y
collection DOAJ
language English
format Article
sources DOAJ
author Prasenjit Sanyal
spellingShingle Prasenjit Sanyal
Limits on the charged Higgs parameters in the two Higgs doublet model using CMS $$\sqrt{s}=13$$ s=13 TeV results
European Physical Journal C: Particles and Fields
author_facet Prasenjit Sanyal
author_sort Prasenjit Sanyal
title Limits on the charged Higgs parameters in the two Higgs doublet model using CMS $$\sqrt{s}=13$$ s=13 TeV results
title_short Limits on the charged Higgs parameters in the two Higgs doublet model using CMS $$\sqrt{s}=13$$ s=13 TeV results
title_full Limits on the charged Higgs parameters in the two Higgs doublet model using CMS $$\sqrt{s}=13$$ s=13 TeV results
title_fullStr Limits on the charged Higgs parameters in the two Higgs doublet model using CMS $$\sqrt{s}=13$$ s=13 TeV results
title_full_unstemmed Limits on the charged Higgs parameters in the two Higgs doublet model using CMS $$\sqrt{s}=13$$ s=13 TeV results
title_sort limits on the charged higgs parameters in the two higgs doublet model using cms $$\sqrt{s}=13$$ s=13 tev results
publisher SpringerOpen
series European Physical Journal C: Particles and Fields
issn 1434-6044
1434-6052
publishDate 2019-11-01
description Abstract The latest CMS results on the upper limits on $$\sigma _{H^\pm }$$ σH± BR($$H^\pm \rightarrow \tau ^\pm \nu )$$ H±→τ±ν) and $$\sigma _{H^\pm }$$ σH± BR($$H^+ \rightarrow t{\bar{b}}$$ H+→tb¯ ) for $$\sqrt{s}=13$$ s=13 TeV at an integrated luminosity of 35.9 $$\hbox {fb}^{-1}$$ fb-1 are used to impose constraints on the charged Higgs $$H^\pm $$ H± parameters within the Two Higgs Doublet Model (2HDM). The 2HDM is the simplest extension of the Standard Model (SM) under the same gauge symmetry to contain charged Higgs and is relatively little constrained compared to the Minimal Supersymmetric Standard Model (MSSM). The latest results lead to much more stringent constraints on the charged Higgs parameter space than for the earlier 8 TeV results. The CMS collaboration also studied the exotic bosonic decays $$H^\pm \rightarrow W^\pm A$$ H±→W±A and $$A \rightarrow \mu ^+ \mu ^-$$ A→μ+μ- for the first time and put upper limits on the BR($$t\rightarrow H^+ b$$ t→H+b ) for the light charged Higgs boson. These constraints lead to the exclusion of parameter space which is not excluded by the $$\tau \nu $$ τν channel. For comparison the exclusion regions from flavor physics constraints are also discussed.
url http://link.springer.com/article/10.1140/epjc/s10052-019-7431-y
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