cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.93071.v4/t14
title: "Table 14" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: The expected 95% CL upper limits on $\tan\beta$ as a function of $m_{A}$ in the hMSSM scenario. The lowest value of $\tan\beta$ considered by the hMSSM scenario is 0.8 and the highest value of mass is 2 TeV. The points in the region which is called "Not applicable" in the paper figure are kept in the HEPData table. Linear connection is applied in the range of signal mass points from 400 to 1000 GeV in the paper figure. The range of $\tan\beta$ shown in the paper figure and the HEPData is from 1 to 60. No theoretical uncertainty is considered when computing these limits.
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.v4/t9
title: "Table 9" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: The expected 95% CL upper limits with plus one sigma on $\tan\beta$ as a function of $m_{A}$ in the $M_{h}^{125}$ scenario. The lowest value of $\tan\beta$ considered for the $M_{h}^{125}$ scenario is 0.5. The points in the region which is called "Not applicable" in the paper figure are kept in the HEPData table. Linear connection is applied in the range of signal mass points from 400 to 1000 GeV in the paper figure. The range of $\tan\beta$ shown in the paper figure and the HEPData is from 1 to 60. No theoretical uncertainty is considered when computing these limits.
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.v4/t15
title: "Table 15" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: The expected 95% CL upper limits with plus one sigma on $\tan\beta$ as a function of $m_{A}$ in the hMSSM scenario. The lowest value of $\tan\beta$ considered by the hMSSM scenario is 0.8 and the highest value of mass is 2 TeV. The points in the region which is called "Not applicable" in the paper figure are kept in the HEPData table. Linear connection is applied in the range of signal mass points from 400 to 1000 GeV in the paper figure. The range of $\tan\beta$ shown in the paper figure and the HEPData is from 1 to 60. No theoretical uncertainty is considered when computing these limits.
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.v4/t16
title: "Table 16" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: The expected 95% CL upper limits with minus one sigma on $\tan\beta$ as a function of $m_{A}$ in the hMSSM scenario. The lowest value of $\tan\beta$ considered by the hMSSM scenario is 0.8 and the highest value of mass is 2 TeV. The points in the region which is called "Not applicable" in the paper figure are kept in the HEPData table. Linear connection is applied in the range of signal mass points from 400 to 1000 GeV in the paper figure. The range of $\tan\beta$ shown in the paper figure and the HEPData is from 1 to 60. No theoretical uncertainty is considered when computing these limits.
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.v4/t17
title: "Table 17" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: The expected 95% CL upper limits with plus two sigma on $\tan\beta$ as a function of $m_{A}$ in the hMSSM scenario. The lowest value of $\tan\beta$ considered by the hMSSM scenario is 0.8 and the highest value of mass is 2 TeV. The points in the region which is called "Not applicable" in the paper figure are kept in the HEPData table. Linear connection is applied in the range of signal mass points from 400 to 1000 GeV in the paper figure. The range of $\tan\beta$ shown in the paper figure and the HEPData is from 1 to 60. No theoretical uncertainty is considered when computing these limits.
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.v4/t18
title: "Table 18" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: The expected 95% CL upper limits with minus two sigma on $\tan\beta$ as a function of $m_{A}$ in the hMSSM scenario. The lowest value of $\tan\beta$ considered by the hMSSM scenario is 0.8 and the highest value of mass is 2 TeV. The points in the region which is called "Not applicable" in the paper figure are kept in the HEPData table. Linear connection is applied in the range of signal mass points from 400 to 1000 GeV in the paper figure. The range of $\tan\beta$ shown in the paper figure and the HEPData is from 1 to 60. No theoretical uncertainty is considered when computing these limits.
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: 10.15468/dl.dyskzk
title: Occurrence Download

description: A dataset containing 2426 species occurrences available in GBIF matching the query:
{
 "TaxonKey" : [
 "is Loddigesia mirabilis"
 ]
}

 The dataset includes 2426 records from 24 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015778-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.93013.v1/t24
title: "Ds+/D+ ratio vs DN/DETA(NCH), PT(D) 4 TO 6, Figure 14" of "Measurement of prompt D$^0$, D$^+$, D$^{*+}$, and D$^+_s$ production in p$-$Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$"

description: Ratio of prompt Ds+ over D+ production cross section as a function of the charged particle pseudorapidity density in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.
description: No data abstract available.
DOI: 10.17182/hepdata.93071.v4/t19
title: "Table 19" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Acceptance times efficiency for a scalar boson produced by gluon-gluon fusion as a function of the scalar boson mass.
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.v4/t20
title: "Table 20" of "Search for heavy Higgs bosons decaying into two tau leptons with the ATLAS detector using $pp$ collisions at $\sqrt{s}=13$ TeV"

description: Acceptance times efficiency for a scalar boson produced by b-associated production as a function of the scalar boson mass.
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.v4/t21
title: "Table 21" 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 95% CL upper limits on the scalar boson production cross section times ditau branching fraction as a function of the scalar boson mass and the fraction of the b-associated production. The limits are calculated from a statistical combination of the 1l1tau_h and 2tau_h channels.
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.v4/t22
title: "Table 22" 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 95% CL upper limits on the scalar boson production cross section times ditau branching fraction as a function of the scalar boson mass and the fraction of the b-associated production. The limits are calculated from a statistical combination of the 1l1tau_h and 2tau_h channels.
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"