cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.83203.v1/t2
title: "Figure 9: upper limit on tan(beta) in modified MSSM m_h(mod-)" of "Search for charged Higgs bosons decaying into top and bottom quarks at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Expected and observed upper limits on $\tan\beta$ as a function of $m_{H^{+}}$ in the $m_h^{\mathrm{mod-}}$ scenario of the MSSM. Limits are shown for $\tan\beta$ values in the range of 0.5-60, where predictions are available from both scenarios. The bands surrounding the expected limits show the 68% and 95% confidence intervals. The limits are based on the combination of the $\ell+$jets and $\ell\ell$ final states. The production cross-section of $t\bar{t}H$ and $tH$, as well as the branching ratios of the $H$, are fixed to their SM values at each point in the plane. Uncertainties on the predicted $H^{+}$ cross-sections or branching ratios are not considered.
description: CERN-LHC. A search for charged Higgs bosons heavier than the top quark and decaying via $H^\pm\to tb$ is presented. The dataset analysed corresponds to 36.1 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=13$ TeV and was recorded with the ATLAS detector at the LHC in 2015 and 2016. The production of a charged Higgs boson in association with a top quark and a bottom quark, $pp \to tbH^\pm$, is explored in the mass range from $m_{H^\pm}=200$ to $2000$ GeV using multi-jet final states with one or two electrons or muons. Events are categorised according to the multiplicity of jets and how likely these are to have originated from hadronisation of a bottom quark. Multivariate techniques are used to discriminate between signal and background events. No significant excess above the background-only hypothesis is observed and exclusion limits are derived for the production cross-section times branching ratio of a charged Higgs boson as a function of its mass, which range from 2.9 pb at $m_{H^\pm} = 200$ GeV to 0.070 pb at $m_{H^\pm} = 2000$ GeV. The results are interpreted in two benchmark scenarios of the Minimal Supersymmetric Standard Model.
DOI: 10.17182/hepdata.83203.v1/t3
title: "Figure 9: lower limit on tan(beta) in modified MSSM m_h(mod-)" of "Search for charged Higgs bosons decaying into top and bottom quarks at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Expected and observed lower limits on $\tan\beta$ as a function of $m_{H^{+}}$ in the $m_h^{\mathrm{mod-}}$ scenario of the MSSM. Limits are shown for $\tan\beta$ values in the range of 0.5-60, where predictions are available from both scenarios. The bands surrounding the expected limits show the 68% and 95% confidence intervals. The limits are based on the combination of the $\ell+$jets and $\ell\ell$ final states. The production cross-section of $t\bar{t}H$ and $tH$, as well as the branching ratios of the $H$, are fixed to their SM values at each point in the plane. Uncertainties on the predicted $H^{+}$ cross-sections or branching ratios are not considered.
description: CERN-LHC. A search for charged Higgs bosons heavier than the top quark and decaying via $H^\pm\to tb$ is presented. The dataset analysed corresponds to 36.1 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=13$ TeV and was recorded with the ATLAS detector at the LHC in 2015 and 2016. The production of a charged Higgs boson in association with a top quark and a bottom quark, $pp \to tbH^\pm$, is explored in the mass range from $m_{H^\pm}=200$ to $2000$ GeV using multi-jet final states with one or two electrons or muons. Events are categorised according to the multiplicity of jets and how likely these are to have originated from hadronisation of a bottom quark. Multivariate techniques are used to discriminate between signal and background events. No significant excess above the background-only hypothesis is observed and exclusion limits are derived for the production cross-section times branching ratio of a charged Higgs boson as a function of its mass, which range from 2.9 pb at $m_{H^\pm} = 200$ GeV to 0.070 pb at $m_{H^\pm} = 2000$ GeV. The results are interpreted in two benchmark scenarios of the Minimal Supersymmetric Standard Model.
DOI: 10.17182/hepdata.83203.v1/t4
title: "Figure 9: upper limit on tan(beta) in hMSSM" of "Search for charged Higgs bosons decaying into top and bottom quarks at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Expected and observed upper limits on $\tan\beta$ as a function of $m_{H^{+}}$ in the hMSSM scenario of the MSSM. Limits are shown for $\tan\beta$ values in the range of 0.5-60, where predictions are available from both scenarios. The bands surrounding the expected limits show the 68% and 95% confidence intervals. The limits are based on the combination of the $\ell+$jets and $\ell\ell$ final states. The production cross-section of $t\bar{t}H$ and $tH$, as well as the branching ratios of the $H$, are fixed to their SM values at each point in the plane. Uncertainties on the predicted $H^{+}$ cross-sections or branching ratios are not considered.
description: CERN-LHC. A search for charged Higgs bosons heavier than the top quark and decaying via $H^\pm\to tb$ is presented. The dataset analysed corresponds to 36.1 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=13$ TeV and was recorded with the ATLAS detector at the LHC in 2015 and 2016. The production of a charged Higgs boson in association with a top quark and a bottom quark, $pp \to tbH^\pm$, is explored in the mass range from $m_{H^\pm}=200$ to $2000$ GeV using multi-jet final states with one or two electrons or muons. Events are categorised according to the multiplicity of jets and how likely these are to have originated from hadronisation of a bottom quark. Multivariate techniques are used to discriminate between signal and background events. No significant excess above the background-only hypothesis is observed and exclusion limits are derived for the production cross-section times branching ratio of a charged Higgs boson as a function of its mass, which range from 2.9 pb at $m_{H^\pm} = 200$ GeV to 0.070 pb at $m_{H^\pm} = 2000$ GeV. The results are interpreted in two benchmark scenarios of the Minimal Supersymmetric Standard Model.
DOI: 10.17182/hepdata.83203.v1/t5
title: "Figure 9: lower limit on tan(beta) in hMSSM" of "Search for charged Higgs bosons decaying into top and bottom quarks at $\sqrt{s}$ = 13 TeV with the ATLAS detector"

description: Expected and observed lower limits on $\tan\beta$ as a function of $m_{H^{+}}$ in the hMSSM scenario of the MSSM. Limits are shown for $\tan\beta$ values in the range of 0.5-60, where predictions are available from both scenarios. The bands surrounding the expected limits show the 68% and 95% confidence intervals. The limits are based on the combination of the $\ell+$jets and $\ell\ell$ final states. The production cross-section of $t\bar{t}H$ and $tH$, as well as the branching ratios of the $H$, are fixed to their SM values at each point in the plane. Uncertainties on the predicted $H^{+}$ cross-sections or branching ratios are not considered.
description: CERN-LHC. A search for charged Higgs bosons heavier than the top quark and decaying via $H^\pm\to tb$ is presented. The dataset analysed corresponds to 36.1 fb$^{-1}$ of $pp$ collisions at $\sqrt{s}=13$ TeV and was recorded with the ATLAS detector at the LHC in 2015 and 2016. The production of a charged Higgs boson in association with a top quark and a bottom quark, $pp \to tbH^\pm$, is explored in the mass range from $m_{H^\pm}=200$ to $2000$ GeV using multi-jet final states with one or two electrons or muons. Events are categorised according to the multiplicity of jets and how likely these are to have originated from hadronisation of a bottom quark. Multivariate techniques are used to discriminate between signal and background events. No significant excess above the background-only hypothesis is observed and exclusion limits are derived for the production cross-section times branching ratio of a charged Higgs boson as a function of its mass, which range from 2.9 pb at $m_{H^\pm} = 200$ GeV to 0.070 pb at $m_{H^\pm} = 2000$ GeV. The results are interpreted in two benchmark scenarios of the Minimal Supersymmetric Standard Model.
DOI: 10.17182/hepdata.83355.v1/t1
title: "Table 1" of "Search for charged Higgs bosons decaying via $H^{\pm} \to \tau^{\pm}\nu_{\tau}$ in the $\tau$+jets and $\tau$+lepton final states with 36 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 13$ TeV with the ATLAS experiment"

description: Observed and expected 95% CL exclusion limits on $\sigma(pp\to tbH^+)\times \mathrm{\cal{B}}(H^+\to\tau\nu)$ as a function of the charged Higgs boson mass in 36.1 fb$^{-1}$ of $pp$ collision data at $\sqrt{s} = 13$ TeV, after combination of the $\tau_{\rm had-vis}$+jets and $\tau_{\rm had-vis}$+lepton final states.
description: CERN-LHC. This data presents the result of a search for charged Higgs bosons decaying via $H^{\pm}\to\tau^{\pm}\nu_{\tau}$ in 36 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 13$ TeV recorded with the ATLAS experiment. No evidence of a charged Higgs boson is found. For the mass range of $m_{H^{\pm}}$ = 90-2000 GeV, upper limits at the 95% confidence level are set on the production cross-section of the charged Higgs boson times the branching fraction $\mathrm{\cal{B}}(H^{\pm} \to \tau^{\pm}\nu_{\tau})$ in a range of 4.2-0.0025 pb. In the mass range 90-160 GeV, assuming the Standard Model cross-section for $t\bar{t}$ production, this corresponds to upper limits between 0.25% and 0.031% for the branching fraction $\mathrm{\cal{B}}(t\to bH^{\pm}) \times \mathrm{\cal{B}}(H^{\pm} \to \tau^{\pm}\nu_{\tau})$.

The $\tau$+jets channel fiducial region is defined as:
- At least one hadronic tau decay ($\tau_{\rm had-vis}$)
- Choose $\tau_{\rm had-vis}$ with highest $p_{\rm T}$ satisfying Medium ID cut
- $p_{\rm T}$($\tau_{\rm had-vis}$) &gt; 40 GeV, |$\eta$($\tau_{\rm had-vis}$)| &lt; 1.37 or 1.52 &lt; |$\eta$($\tau_{\rm had-vis}$)| &lt; 2.3
- No electrons or muons
- At least three jets with $p_{\rm T}$ &gt; 25 GeV, of which at least one is $b$-tagged
- $E_{\rm T}^{\rm miss}$ &gt; 150 GeV
- $m_{\rm T}$($\tau_{\rm had-vis}$, $E_{\rm T}^{\rm miss}$) &gt; 50 GeV

The $\tau$+lepton channel fiducial region is defined as:
- At least one hadronic tau decay ($\tau_{\rm had-vis}$)
- Choose $\tau_{\rm had-vis}$ with highest $p_{\rm T}$ satisfying Medium ID cut
- $p_{\rm T}$($\tau_{\rm had-vis}$) &gt; 30 GeV, |$\eta$($\tau_{\rm had-vis}$)| &lt; 1.37 or 1.52 &lt; |$\eta$($\tau_{\rm had-vis}$)| &lt; 2.3
- Exactly one light lepton (electron or muon) satisfying Tight ID cut
- $p_{\rm T}$(e) &gt; 30 GeV, |$\eta$(e)| &lt; 1.37 or 1.52 &lt; |$\eta$(e)| &lt; 2.47
- $p_{\rm T}$($\mu$) &gt; 30 GeV, |$\eta$($\mu$)| &lt; 2.5
- At least one is $b$-tagged with $p_{\rm T}$ &gt; 25 GeV
- $E_{\rm T}^{\rm miss}$ &gt; 50 GeV
DOI: 10.17182/hepdata.83355.v1/t2
title: "Table 2" of "Search for charged Higgs bosons decaying via $H^{\pm} \to \tau^{\pm}\nu_{\tau}$ in the $\tau$+jets and $\tau$+lepton final states with 36 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 13$ TeV with the ATLAS experiment"

description: Observed and expected 95% CL exclusion limits on $\mathrm{\cal{B}}(t\to bH^+)\times\mathrm{\cal{B}}(H^+\to\tau\nu)$ as a function of the charged Higgs boson mass in 36.1 fb$^{-1}$ of $pp$ collision data at $\sqrt{s} = 13$ TeV, after combination of the $\tau_{\rm had-vis}$+jets and $\tau_{\rm had-vis}$+lepton final states.
description: CERN-LHC. This data presents the result of a search for charged Higgs bosons decaying via $H^{\pm}\to\tau^{\pm}\nu_{\tau}$ in 36 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 13$ TeV recorded with the ATLAS experiment. No evidence of a charged Higgs boson is found. For the mass range of $m_{H^{\pm}}$ = 90-2000 GeV, upper limits at the 95% confidence level are set on the production cross-section of the charged Higgs boson times the branching fraction $\mathrm{\cal{B}}(H^{\pm} \to \tau^{\pm}\nu_{\tau})$ in a range of 4.2-0.0025 pb. In the mass range 90-160 GeV, assuming the Standard Model cross-section for $t\bar{t}$ production, this corresponds to upper limits between 0.25% and 0.031% for the branching fraction $\mathrm{\cal{B}}(t\to bH^{\pm}) \times \mathrm{\cal{B}}(H^{\pm} \to \tau^{\pm}\nu_{\tau})$.

The $\tau$+jets channel fiducial region is defined as:
- At least one hadronic tau decay ($\tau_{\rm had-vis}$)
- Choose $\tau_{\rm had-vis}$ with highest $p_{\rm T}$ satisfying Medium ID cut
- $p_{\rm T}$($\tau_{\rm had-vis}$) &gt; 40 GeV, |$\eta$($\tau_{\rm had-vis}$)| &lt; 1.37 or 1.52 &lt; |$\eta$($\tau_{\rm had-vis}$)| &lt; 2.3
- No electrons or muons
- At least three jets with $p_{\rm T}$ &gt; 25 GeV, of which at least one is $b$-tagged
- $E_{\rm T}^{\rm miss}$ &gt; 150 GeV
- $m_{\rm T}$($\tau_{\rm had-vis}$, $E_{\rm T}^{\rm miss}$) &gt; 50 GeV

The $\tau$+lepton channel fiducial region is defined as:
- At least one hadronic tau decay ($\tau_{\rm had-vis}$)
- Choose $\tau_{\rm had-vis}$ with highest $p_{\rm T}$ satisfying Medium ID cut
- $p_{\rm T}$($\tau_{\rm had-vis}$) &gt; 30 GeV, |$\eta$($\tau_{\rm had-vis}$)| &lt; 1.37 or 1.52 &lt; |$\eta$($\tau_{\rm had-vis}$)| &lt; 2.3
- Exactly one light lepton (electron or muon) satisfying Tight ID cut
- $p_{\rm T}$(e) &gt; 30 GeV, |$\eta$(e)| &lt; 1.37 or 1.52 &lt; |$\eta$(e)| &lt; 2.47
- $p_{\rm T}$($\mu$) &gt; 30 GeV, |$\eta$($\mu$)| &lt; 2.5
- At least one is $b$-tagged with $p_{\rm T}$ &gt; 25 GeV
- $E_{\rm T}^{\rm miss}$ &gt; 50 GeV
DOI: 10.17182/hepdata.83355.v1/t3
title: "Table 3" of "Search for charged Higgs bosons decaying via $H^{\pm} \to \tau^{\pm}\nu_{\tau}$ in the $\tau$+jets and $\tau$+lepton final states with 36 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 13$ TeV with the ATLAS experiment"

description: Observed 95% CL exclusion contour in the tan$\beta$ - $m_H$ plane shown in the context of the hMSSM, for the regions in which theoretical predictions are available (0.5$\leq\text{tan}\beta\leq60$).
description: CERN-LHC. This data presents the result of a search for charged Higgs bosons decaying via $H^{\pm}\to\tau^{\pm}\nu_{\tau}$ in 36 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 13$ TeV recorded with the ATLAS experiment. No evidence of a charged Higgs boson is found. For the mass range of $m_{H^{\pm}}$ = 90-2000 GeV, upper limits at the 95% confidence level are set on the production cross-section of the charged Higgs boson times the branching fraction $\mathrm{\cal{B}}(H^{\pm} \to \tau^{\pm}\nu_{\tau})$ in a range of 4.2-0.0025 pb. In the mass range 90-160 GeV, assuming the Standard Model cross-section for $t\bar{t}$ production, this corresponds to upper limits between 0.25% and 0.031% for the branching fraction $\mathrm{\cal{B}}(t\to bH^{\pm}) \times \mathrm{\cal{B}}(H^{\pm} \to \tau^{\pm}\nu_{\tau})$.

The $\tau$+jets channel fiducial region is defined as:
- At least one hadronic tau decay ($\tau_{\rm had-vis}$)
- Choose $\tau_{\rm had-vis}$ with highest $p_{\rm T}$ satisfying Medium ID cut
- $p_{\rm T}$($\tau_{\rm had-vis}$) &gt; 40 GeV, |$\eta$($\tau_{\rm had-vis}$)| &lt; 1.37 or 1.52 &lt; |$\eta$($\tau_{\rm had-vis}$)| &lt; 2.3
- No electrons or muons
- At least three jets with $p_{\rm T}$ &gt; 25 GeV, of which at least one is $b$-tagged
- $E_{\rm T}^{\rm miss}$ &gt; 150 GeV
- $m_{\rm T}$($\tau_{\rm had-vis}$, $E_{\rm T}^{\rm miss}$) &gt; 50 GeV

The $\tau$+lepton channel fiducial region is defined as:
- At least one hadronic tau decay ($\tau_{\rm had-vis}$)
- Choose $\tau_{\rm had-vis}$ with highest $p_{\rm T}$ satisfying Medium ID cut
- $p_{\rm T}$($\tau_{\rm had-vis}$) &gt; 30 GeV, |$\eta$($\tau_{\rm had-vis}$)| &lt; 1.37 or 1.52 &lt; |$\eta$($\tau_{\rm had-vis}$)| &lt; 2.3
- Exactly one light lepton (electron or muon) satisfying Tight ID cut
- $p_{\rm T}$(e) &gt; 30 GeV, |$\eta$(e)| &lt; 1.37 or 1.52 &lt; |$\eta$(e)| &lt; 2.47
- $p_{\rm T}$($\mu$) &gt; 30 GeV, |$\eta$($\mu$)| &lt; 2.5
- At least one is $b$-tagged with $p_{\rm T}$ &gt; 25 GeV
- $E_{\rm T}^{\rm miss}$ &gt; 50 GeV
DOI: 10.17182/hepdata.83355.v1/t4
title: "Table 4" of "Search for charged Higgs bosons decaying via $H^{\pm} \to \tau^{\pm}\nu_{\tau}$ in the $\tau$+jets and $\tau$+lepton final states with 36 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 13$ TeV with the ATLAS experiment"

description: Expected 95% CL exclusion contour in the tan$\beta$ - $m_H$ plane shown in the context of the hMSSM, for the regions in which theoretical predictions are available (0.5$\leq\text{tan}\beta\leq60$).
description: CERN-LHC. This data presents the result of a search for charged Higgs bosons decaying via $H^{\pm}\to\tau^{\pm}\nu_{\tau}$ in 36 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 13$ TeV recorded with the ATLAS experiment. No evidence of a charged Higgs boson is found. For the mass range of $m_{H^{\pm}}$ = 90-2000 GeV, upper limits at the 95% confidence level are set on the production cross-section of the charged Higgs boson times the branching fraction $\mathrm{\cal{B}}(H^{\pm} \to \tau^{\pm}\nu_{\tau})$ in a range of 4.2-0.0025 pb. In the mass range 90-160 GeV, assuming the Standard Model cross-section for $t\bar{t}$ production, this corresponds to upper limits between 0.25% and 0.031% for the branching fraction $\mathrm{\cal{B}}(t\to bH^{\pm}) \times \mathrm{\cal{B}}(H^{\pm} \to \tau^{\pm}\nu_{\tau})$.

The $\tau$+jets channel fiducial region is defined as:
- At least one hadronic tau decay ($\tau_{\rm had-vis}$)
- Choose $\tau_{\rm had-vis}$ with highest $p_{\rm T}$ satisfying Medium ID cut
- $p_{\rm T}$($\tau_{\rm had-vis}$) &gt; 40 GeV, |$\eta$($\tau_{\rm had-vis}$)| &lt; 1.37 or 1.52 &lt; |$\eta$($\tau_{\rm had-vis}$)| &lt; 2.3
- No electrons or muons
- At least three jets with $p_{\rm T}$ &gt; 25 GeV, of which at least one is $b$-tagged
- $E_{\rm T}^{\rm miss}$ &gt; 150 GeV
- $m_{\rm T}$($\tau_{\rm had-vis}$, $E_{\rm T}^{\rm miss}$) &gt; 50 GeV

The $\tau$+lepton channel fiducial region is defined as:
- At least one hadronic tau decay ($\tau_{\rm had-vis}$)
- Choose $\tau_{\rm had-vis}$ with highest $p_{\rm T}$ satisfying Medium ID cut
- $p_{\rm T}$($\tau_{\rm had-vis}$) &gt; 30 GeV, |$\eta$($\tau_{\rm had-vis}$)| &lt; 1.37 or 1.52 &lt; |$\eta$($\tau_{\rm had-vis}$)| &lt; 2.3
- Exactly one light lepton (electron or muon) satisfying Tight ID cut
- $p_{\rm T}$(e) &gt; 30 GeV, |$\eta$(e)| &lt; 1.37 or 1.52 &lt; |$\eta$(e)| &lt; 2.47
- $p_{\rm T}$($\mu$) &gt; 30 GeV, |$\eta$($\mu$)| &lt; 2.5
- At least one is $b$-tagged with $p_{\rm T}$ &gt; 25 GeV
- $E_{\rm T}^{\rm miss}$ &gt; 50 GeV
DOI: 10.17182/hepdata.83355.v1/t5
title: "Table 5" of "Search for charged Higgs bosons decaying via $H^{\pm} \to \tau^{\pm}\nu_{\tau}$ in the $\tau$+jets and $\tau$+lepton final states with 36 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 13$ TeV with the ATLAS experiment"

description: Observed a95% CL exclusion contour in the tan$\beta$ - $m_H$ plane shown in the context of the $m_{H}^{mod-}$ scenario, for the regions in which theoretical predictions are available (0.5$\leq\text{tan}\beta\leq60$).
description: CERN-LHC. This data presents the result of a search for charged Higgs bosons decaying via $H^{\pm}\to\tau^{\pm}\nu_{\tau}$ in 36 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 13$ TeV recorded with the ATLAS experiment. No evidence of a charged Higgs boson is found. For the mass range of $m_{H^{\pm}}$ = 90-2000 GeV, upper limits at the 95% confidence level are set on the production cross-section of the charged Higgs boson times the branching fraction $\mathrm{\cal{B}}(H^{\pm} \to \tau^{\pm}\nu_{\tau})$ in a range of 4.2-0.0025 pb. In the mass range 90-160 GeV, assuming the Standard Model cross-section for $t\bar{t}$ production, this corresponds to upper limits between 0.25% and 0.031% for the branching fraction $\mathrm{\cal{B}}(t\to bH^{\pm}) \times \mathrm{\cal{B}}(H^{\pm} \to \tau^{\pm}\nu_{\tau})$.

The $\tau$+jets channel fiducial region is defined as:
- At least one hadronic tau decay ($\tau_{\rm had-vis}$)
- Choose $\tau_{\rm had-vis}$ with highest $p_{\rm T}$ satisfying Medium ID cut
- $p_{\rm T}$($\tau_{\rm had-vis}$) &gt; 40 GeV, |$\eta$($\tau_{\rm had-vis}$)| &lt; 1.37 or 1.52 &lt; |$\eta$($\tau_{\rm had-vis}$)| &lt; 2.3
- No electrons or muons
- At least three jets with $p_{\rm T}$ &gt; 25 GeV, of which at least one is $b$-tagged
- $E_{\rm T}^{\rm miss}$ &gt; 150 GeV
- $m_{\rm T}$($\tau_{\rm had-vis}$, $E_{\rm T}^{\rm miss}$) &gt; 50 GeV

The $\tau$+lepton channel fiducial region is defined as:
- At least one hadronic tau decay ($\tau_{\rm had-vis}$)
- Choose $\tau_{\rm had-vis}$ with highest $p_{\rm T}$ satisfying Medium ID cut
- $p_{\rm T}$($\tau_{\rm had-vis}$) &gt; 30 GeV, |$\eta$($\tau_{\rm had-vis}$)| &lt; 1.37 or 1.52 &lt; |$\eta$($\tau_{\rm had-vis}$)| &lt; 2.3
- Exactly one light lepton (electron or muon) satisfying Tight ID cut
- $p_{\rm T}$(e) &gt; 30 GeV, |$\eta$(e)| &lt; 1.37 or 1.52 &lt; |$\eta$(e)| &lt; 2.47
- $p_{\rm T}$($\mu$) &gt; 30 GeV, |$\eta$($\mu$)| &lt; 2.5
- At least one is $b$-tagged with $p_{\rm T}$ &gt; 25 GeV
- $E_{\rm T}^{\rm miss}$ &gt; 50 GeV
DOI: 10.17182/hepdata.83355.v1/t6
title: "Table 6" of "Search for charged Higgs bosons decaying via $H^{\pm} \to \tau^{\pm}\nu_{\tau}$ in the $\tau$+jets and $\tau$+lepton final states with 36 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 13$ TeV with the ATLAS experiment"

description: Expected 95% CL exclusion contour in the tan$\beta$ - $m_H$ plane shown in the context of the $m_{H}^{mod-}$ scenario, for the regions in which theoretical predictions are available (0.5$\leq\text{tan}\beta\leq60$).
description: CERN-LHC. This data presents the result of a search for charged Higgs bosons decaying via $H^{\pm}\to\tau^{\pm}\nu_{\tau}$ in 36 fb$^{-1}$ of $pp$ collision data recorded at $\sqrt{s} = 13$ TeV recorded with the ATLAS experiment. No evidence of a charged Higgs boson is found. For the mass range of $m_{H^{\pm}}$ = 90-2000 GeV, upper limits at the 95% confidence level are set on the production cross-section of the charged Higgs boson times the branching fraction $\mathrm{\cal{B}}(H^{\pm} \to \tau^{\pm}\nu_{\tau})$ in a range of 4.2-0.0025 pb. In the mass range 90-160 GeV, assuming the Standard Model cross-section for $t\bar{t}$ production, this corresponds to upper limits between 0.25% and 0.031% for the branching fraction $\mathrm{\cal{B}}(t\to bH^{\pm}) \times \mathrm{\cal{B}}(H^{\pm} \to \tau^{\pm}\nu_{\tau})$.

The $\tau$+jets channel fiducial region is defined as:
- At least one hadronic tau decay ($\tau_{\rm had-vis}$)
- Choose $\tau_{\rm had-vis}$ with highest $p_{\rm T}$ satisfying Medium ID cut
- $p_{\rm T}$($\tau_{\rm had-vis}$) &gt; 40 GeV, |$\eta$($\tau_{\rm had-vis}$)| &lt; 1.37 or 1.52 &lt; |$\eta$($\tau_{\rm had-vis}$)| &lt; 2.3
- No electrons or muons
- At least three jets with $p_{\rm T}$ &gt; 25 GeV, of which at least one is $b$-tagged
- $E_{\rm T}^{\rm miss}$ &gt; 150 GeV
- $m_{\rm T}$($\tau_{\rm had-vis}$, $E_{\rm T}^{\rm miss}$) &gt; 50 GeV

The $\tau$+lepton channel fiducial region is defined as:
- At least one hadronic tau decay ($\tau_{\rm had-vis}$)
- Choose $\tau_{\rm had-vis}$ with highest $p_{\rm T}$ satisfying Medium ID cut
- $p_{\rm T}$($\tau_{\rm had-vis}$) &gt; 30 GeV, |$\eta$($\tau_{\rm had-vis}$)| &lt; 1.37 or 1.52 &lt; |$\eta$($\tau_{\rm had-vis}$)| &lt; 2.3
- Exactly one light lepton (electron or muon) satisfying Tight ID cut
- $p_{\rm T}$(e) &gt; 30 GeV, |$\eta$(e)| &lt; 1.37 or 1.52 &lt; |$\eta$(e)| &lt; 2.47
- $p_{\rm T}$($\mu$) &gt; 30 GeV, |$\eta$($\mu$)| &lt; 2.5
- At least one is $b$-tagged with $p_{\rm T}$ &gt; 25 GeV
- $E_{\rm T}^{\rm miss}$ &gt; 50 GeV