cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.93071.v3/t34
title: "Table 34" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Observed two dimensional likelihood scan of the gluon-gluon fusion cross section times branching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the scalar boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively. The value of $2\Delta(\mathrm{NLL})$ for 1500 GeV signal mass point is shown in the HEPData table.
description: CERN-LHC. A search for additional heavy neutral Higgs bosons is performed using a data sample corresponding to an integrated luminosity of 139 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.93071.v3/t35
title: "Table 35" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Observed two dimensional likelihood scan of the gluon-gluon fusion cross section times branching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the scalar boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively. The value of $2\Delta(\mathrm{NLL})$ for 2000 GeV signal mass point is shown in the HEPData table.
description: CERN-LHC. A search for additional heavy neutral Higgs bosons is performed using a data sample corresponding to an integrated luminosity of 139 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.93071.v3/t36
title: "Table 36" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Observed two dimensional likelihood scan of the gluon-gluon fusion cross section times branching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the scalar boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively. The value of $2\Delta(\mathrm{NLL})$ for 2500 GeV signal mass point is shown in the HEPData table.
description: CERN-LHC. A search for additional heavy neutral Higgs bosons is performed using a data sample corresponding to an integrated luminosity of 139 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.93071.v3/t37
title: "Table 37" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Expected two dimensional likelihood scan of the gluon-gluon fusion cross section times branching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the scalar boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively. The value of $2\Delta(\mathrm{NLL})$ for 200 GeV signal mass point is shown in the HEPData table.
description: CERN-LHC. A search for additional heavy neutral Higgs bosons is performed using a data sample corresponding to an integrated luminosity of 139 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.93071.v3/t38
title: "Table 38" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Expected two dimensional likelihood scan of the gluon-gluon fusion cross section times branching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the scalar boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively. The value of $2\Delta(\mathrm{NLL})$ for 250 GeV signal mass point is shown in the HEPData table.
description: CERN-LHC. A search for additional heavy neutral Higgs bosons is performed using a data sample corresponding to an integrated luminosity of 139 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.93071.v3/t39
title: "Table 39" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Expected two dimensional likelihood scan of the gluon-gluon fusion cross section times branching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the scalar boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively. The value of $2\Delta(\mathrm{NLL})$ for 300 GeV signal mass point is shown in the HEPData table.
description: CERN-LHC. A search for additional heavy neutral Higgs bosons is performed using a data sample corresponding to an integrated luminosity of 139 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.93071.v3/t41
title: "Table 41" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Expected two dimensional likelihood scan of the gluon-gluon fusion cross section times branching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the scalar boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively. The value of $2\Delta(\mathrm{NLL})$ for 400 GeV signal mass point is shown in the HEPData table.
description: CERN-LHC. A search for additional heavy neutral Higgs bosons is performed using a data sample corresponding to an integrated luminosity of 139 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.93071.v3/t42
title: "Table 42" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Expected two dimensional likelihood scan of the gluon-gluon fusion cross section times branching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the scalar boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively. The value of $2\Delta(\mathrm{NLL})$ for 500 GeV signal mass point is shown in the HEPData table.
description: CERN-LHC. A search for additional heavy neutral Higgs bosons is performed using a data sample corresponding to an integrated luminosity of 139 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"
DOI: 10.17182/hepdata.93071.v3/t43
title: "Table 43" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Expected two dimensional likelihood scan of the gluon-gluon fusion cross section times branching fraction, $\sigma(gg\phi)\times B(\phi\to\tau\tau)$, vs the b-associated production times branching fraction, $\sigma(bb\phi)\times B(\phi\to\tau\tau)$ for the scalar boson mass ($m_\phi$) indicated in the table. For each mass, 10000 points are scanned. At each point $\Delta(\mathrm{NLL})$ is calculated, defined as the negative-log-likelihood (NLL) of the conditional fit with $\sigma(gg\phi)$ and $\sigma(bb\phi)$ fixed to their values at the point and with the minimum NLL value at any point subtracted. The best-fit point and the preferred 68% and 95% boundaries are found at $2\Delta(\mathrm{NLL})$ values of 0.0, 2.30 and 5.90, respectively. The value of $2\Delta(\mathrm{NLL})$ for 600 GeV signal mass point is shown in the HEPData table.
description: CERN-LHC. A search for additional heavy neutral Higgs bosons is performed using a data sample corresponding to an integrated luminosity of 139 fb$^{-1}$ from proton-proton collisions at $\sqrt{s}$ = 13 TeV recorded by the ATLAS detector at the LHC.

The 1l1tau_h channel fiducial region is defined as:
- 1e+&gt;=1tau_h or 1mu+&gt;=1tau_h
- ptLepton &gt; 30 GeV
- |etaMuon| &lt; 2.4, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- ptTauVis &gt; 25 GeV
- |etaTauVis| &lt; 2.3 (excluding 1.37 &lt; |etaTauVis| &lt; 1.52)
- No events with more than 1 electron (ptEle &gt; 15 GeV) or muon (ptMuon &gt; 7 GeV, |etaMuon|&lt;2.5)
- If multiple tau_h exist, the leading visible pt one is chosen
- l and tau_h opposite electric charge
- |DeltaPhi(l,tau_h)| &gt; 2.4 rad
- mT(l,MET) &lt; 40 GeV
- veto 80 &lt; m(l,tau_h) &lt; 110 in 1e1tau_h channel

The 2tau_h channel fiducial region is defined as:
- &gt;=2tau_h
- ptTauVis &gt; 65 GeV (at least one with ptTauVis &gt; 130 GeV, note that technically, this upper threshold was 85 GeV for ~10% of the data)
- No events with an electron or muon, ptLepton &gt; 7 (15) GeV for muons (electrons), |etaMuon| &lt; 2.5, |etaEle| &lt; 2.47 (excluding 1.37 &lt; |etaEle| &lt; 1.52)
- If more than two tau_h exist, the two leading visible pt ones are chosen
- The two tau_h have opposite electric charge
- |DeltaPhi(tau1_h,tau2_h)| &gt; 2.7 rad

For Higgs interpretations events entering the fiducial region of each channel are categorised as: 
- "b-tag: if they contain a b-quark initiated jet (ptJet &gt; 20 GeV, |etaJet|&lt;2.5)"
- "b-veto: otherwise"