cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.93071.v2/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.v2/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.v2/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.v2/t40
title: "Table 40" 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 350 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: 10.15468/dl.hp83qc
title: Occurrence Download

description: A dataset containing 110260 species occurrences available in GBIF matching the query:
{
 "and" : [
 {
 "and" : [
 "HasGeospatialIssue is false",
 "HasCoordinate is true",
 "OccurrenceStatus is Present",
 {
 "not" : {
 "BasisOfRecord" : [
 "is one of (Fossil, Living Specimen)"
 ]
 }
 }
 ]
 },
 "TaxonKey is one of (Duperreya sericea, Spergularia aberrans, Limonium teuchirae, Limonium soboliferum, Limonium squarrosum, Limonium migjornense, Limonium mazarae, Limonium formenterae, Limonium florentinum, Limonium lausianum, Plantago nivea, Monsonia glauca, Lactuca inermis, Plantago loeflingii, Pulicaria grandidentata, Pulicaria lhotei, Pulicaria filaginoides, Psoralea rhizotoma, Scleria bulbifera, Psoralea vanberkeliae, Limonium aegaeum, Limonium dolihiense, Isoetes boryana, Lactuca tenerrima, Psoralea sericea, Clutia africana, Genoplesium rhyoliticum, Garrya flavescens, Doryanthes palmeri, Eriospermum aequilibre, Anacampseros albidiflora, Anacampseros nebrownii, Anacampseros ruschii, Nototriche pulvinata, Physospermum verticillatum, Gleichenia dicarpa, Spergularia sezer-zenginii, Limonium cavanillesii, Plantago maris-mortui, Aeschynomene indica, Gypsophila pilulifera, Drosanthemopsis kwaganapensis, Limonium diomedeum, Triteleia versicolor, Eriospermum ramosum, Duvalia pubescens, Rumex altissimus, Rumex arifolius, Staavia pinifolia, Limonium thaenicum, Limonium teretifolium, Limonium pseudebusitanum, Limonium tacapense, Limonium silvestrei, Limonium melitense, Plantago afra, Calliandra humilis, Psoralea ivumba, Lactuca reviersii, Glyptopleura setulosa, Tolpis proustii, Tolpis calderae, Aeschynomene scabra, Pulicaria clausonis, Rumex utahensis, Vaccinium deliciosum, Lactuca dregeana, Habenaria brevilabiata, Lactuca quercina, Limonium athinense, Limonium ikaricum, Limonium minoicum, Plantago cretica, Perityle cuneata, Clutia daphnoides, Genoplesium turfosum, Eriospermum calcareum, Eriospermum cernuum, Eriospermum ciliatum, Eriospermum descendens, Xerochrysum wilsonii, Limonium calanchicola, Plantago alpina, Gypsophila pulvinaris, Limonium liberianum, Limonium stenophyllum, Hesperevax sparsiflora, Limonium himariense, Chaptalia runcinata, Brownleea galpinii, Wurmbea inframediana, Eriospermum villosum, Oreocarya flavoculata, Rumex impurus, Staavia brownii, Limonium pseudodictyocladum, Limonium sventenii, Limonium sucronicum, Limonium gallurense, Limonium furnarii)",
 "Year is greater than or equal to 1950"
 ]
}

 The dataset includes 110260 records from 876 constituent datasets; see https://api.gbif.org/v1/occurrence/download/0015764-251025141854904/datasets/export for details.
 
Data from some individual datasets included in this download may be licensed under less restrictive terms.
DOI: 10.17182/hepdata.93071.v2/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.v2/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.v2/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"
DOI: 10.17182/hepdata.93071.v2/t44
title: "Table 44" 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 700 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"