cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.79668.v1/t3
title: "Table 3" of "Observation of top quark production in proton-nucleus collisions"

description: Invariant mass distributions of the W candidate, $m_{jj'}$, in the $\geq$2 b category after all selections. The error bars indicate the statistical uncertainties.
description: Reconstructed invariant mass distributions of the hadronic W (jj') boson
and top quark (jj'b) candidates in each b jet category. The kinematic variables
describe the $\ell$+jets decay channel, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$). The measured cross sections are given per decay channel
and for their combination.

The fiducial region is defined as:
- $\equiv$1lepton, $p_T$&gt;30GeV&&|$\eta$|&lt;2.1
- exluding 1.444&lt;|$\eta$|&lt;1.566 region only in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;20GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;15GeV&&|$\eta$|&lt;2.4 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$4jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.5
- min($\Delta R(jet,\ell)$) &gt; 0.3
- ambiguities in pairing the jj' are resolved by choosing the combination that results in the smaller value of the $\Delta R(j,j')$, where $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$
- ambiguities in pairing the jj'b are resolved by choosing the combination that results in the smaller value of the $|m_{jj'b}-m_{\ell\nu b}|$

The acceptance is measured in the $\mu$+jets channel as:
0.060$\pm$0.002(tot)

The acceptance is measured in the $\rm{e}$+jets channel as:
0.056$\pm$0.002(tot)

The efficiency is measured in the $\mu$+jets channel as:
0.91$\pm$0.04(tot)

The efficiency is measured in the $\rm{e}$+jets channel as:
0.63$\pm$0.03(tot)
DOI: 10.17182/hepdata.79668.v1/t4
title: "Table 4" of "Observation of top quark production in proton-nucleus collisions"

description: Invariant mass distributions of the $t\to jj^{'}b$ candidates, $m_{top}$, in the 0 b category after all selections. The error bars indicate the statistical uncertainties.
description: Reconstructed invariant mass distributions of the hadronic W (jj') boson
and top quark (jj'b) candidates in each b jet category. The kinematic variables
describe the $\ell$+jets decay channel, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$). The measured cross sections are given per decay channel
and for their combination.

The fiducial region is defined as:
- $\equiv$1lepton, $p_T$&gt;30GeV&&|$\eta$|&lt;2.1
- exluding 1.444&lt;|$\eta$|&lt;1.566 region only in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;20GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;15GeV&&|$\eta$|&lt;2.4 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$4jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.5
- min($\Delta R(jet,\ell)$) &gt; 0.3
- ambiguities in pairing the jj' are resolved by choosing the combination that results in the smaller value of the $\Delta R(j,j')$, where $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$
- ambiguities in pairing the jj'b are resolved by choosing the combination that results in the smaller value of the $|m_{jj'b}-m_{\ell\nu b}|$

The acceptance is measured in the $\mu$+jets channel as:
0.060$\pm$0.002(tot)

The acceptance is measured in the $\rm{e}$+jets channel as:
0.056$\pm$0.002(tot)

The efficiency is measured in the $\mu$+jets channel as:
0.91$\pm$0.04(tot)

The efficiency is measured in the $\rm{e}$+jets channel as:
0.63$\pm$0.03(tot)
DOI: 10.17182/hepdata.79668.v1/t5
title: "Table 5" of "Observation of top quark production in proton-nucleus collisions"

description: Invariant mass distributions of the $t\to jj^{'}b$ candidates, $m_{top}$, in the 1 b category after all selections. The error bars indicate the statistical uncertainties.
description: Reconstructed invariant mass distributions of the hadronic W (jj') boson
and top quark (jj'b) candidates in each b jet category. The kinematic variables
describe the $\ell$+jets decay channel, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$). The measured cross sections are given per decay channel
and for their combination.

The fiducial region is defined as:
- $\equiv$1lepton, $p_T$&gt;30GeV&&|$\eta$|&lt;2.1
- exluding 1.444&lt;|$\eta$|&lt;1.566 region only in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;20GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;15GeV&&|$\eta$|&lt;2.4 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$4jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.5
- min($\Delta R(jet,\ell)$) &gt; 0.3
- ambiguities in pairing the jj' are resolved by choosing the combination that results in the smaller value of the $\Delta R(j,j')$, where $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$
- ambiguities in pairing the jj'b are resolved by choosing the combination that results in the smaller value of the $|m_{jj'b}-m_{\ell\nu b}|$

The acceptance is measured in the $\mu$+jets channel as:
0.060$\pm$0.002(tot)

The acceptance is measured in the $\rm{e}$+jets channel as:
0.056$\pm$0.002(tot)

The efficiency is measured in the $\mu$+jets channel as:
0.91$\pm$0.04(tot)

The efficiency is measured in the $\rm{e}$+jets channel as:
0.63$\pm$0.03(tot)
DOI: 10.17182/hepdata.79668.v1/t6
title: "Table 6" of "Observation of top quark production in proton-nucleus collisions"

description: Invariant mass distributions of the $t\to jj^{'}b$ candidates, $m_{top}$, in the $\geq$2 b category after all selections. The error bars indicate the statistical uncertainties.
description: Reconstructed invariant mass distributions of the hadronic W (jj') boson
and top quark (jj'b) candidates in each b jet category. The kinematic variables
describe the $\ell$+jets decay channel, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$). The measured cross sections are given per decay channel
and for their combination.

The fiducial region is defined as:
- $\equiv$1lepton, $p_T$&gt;30GeV&&|$\eta$|&lt;2.1
- exluding 1.444&lt;|$\eta$|&lt;1.566 region only in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;20GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;15GeV&&|$\eta$|&lt;2.4 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$4jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.5
- min($\Delta R(jet,\ell)$) &gt; 0.3
- ambiguities in pairing the jj' are resolved by choosing the combination that results in the smaller value of the $\Delta R(j,j')$, where $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$
- ambiguities in pairing the jj'b are resolved by choosing the combination that results in the smaller value of the $|m_{jj'b}-m_{\ell\nu b}|$

The acceptance is measured in the $\mu$+jets channel as:
0.060$\pm$0.002(tot)

The acceptance is measured in the $\rm{e}$+jets channel as:
0.056$\pm$0.002(tot)

The efficiency is measured in the $\mu$+jets channel as:
0.91$\pm$0.04(tot)

The efficiency is measured in the $\rm{e}$+jets channel as:
0.63$\pm$0.03(tot)
DOI: 10.17182/hepdata.79668.v1/t7
title: "Table 7" of "Observation of top quark production in proton-nucleus collisions"

description: The measured cross section in the $\mu$+jets, $\rm{e}$+jets and $\ell$+jets channels. The first uncertainty is the statistical, the second is the systematic.
description: Reconstructed invariant mass distributions of the hadronic W (jj') boson
and top quark (jj'b) candidates in each b jet category. The kinematic variables
describe the $\ell$+jets decay channel, where $\ell$ can be either a muon ($\mu$)
or electron ($\rm{e}$). The measured cross sections are given per decay channel
and for their combination.

The fiducial region is defined as:
- $\equiv$1lepton, $p_T$&gt;30GeV&&|$\eta$|&lt;2.1
- exluding 1.444&lt;|$\eta$|&lt;1.566 region only in the $\rm{e}$+jets channel
- no additional lepton with $p_T$&gt;20GeV&&|$\eta$|&lt;2.5 and $p_T$&gt;15GeV&&|$\eta$|&lt;2.4 in the $\mu$+jets and $\rm{e}$+jets channel, respectively
- $\geq$4jets(anti-kt,R=0.4), $p_T$&gt;25GeV&&|$\eta$|&lt;2.5
- min($\Delta R(jet,\ell)$) &gt; 0.3
- ambiguities in pairing the jj' are resolved by choosing the combination that results in the smaller value of the $\Delta R(j,j')$, where $\Delta R=\sqrt{ (\Delta \eta)^{2} + (\Delta \phi)^{2}}$
- ambiguities in pairing the jj'b are resolved by choosing the combination that results in the smaller value of the $|m_{jj'b}-m_{\ell\nu b}|$

The acceptance is measured in the $\mu$+jets channel as:
0.060$\pm$0.002(tot)

The acceptance is measured in the $\rm{e}$+jets channel as:
0.056$\pm$0.002(tot)

The efficiency is measured in the $\mu$+jets channel as:
0.91$\pm$0.04(tot)

The efficiency is measured in the $\rm{e}$+jets channel as:
0.63$\pm$0.03(tot)
DOI: 10.17182/hepdata.79779.v1/t1
title: "Limit model : HVTWW" of "Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector"

description: Limit
description: No data abstract available.
DOI: 10.17182/hepdata.79779.v1/t2
title: "Limit model : HVTWZ" of "Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector"

description: Limit
description: No data abstract available.
DOI: 10.17182/hepdata.79779.v1/t3
title: "Limit model : RSGWW-SmReW" of "Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector"

description: Limit
description: No data abstract available.
DOI: 10.17182/hepdata.79779.v1/t4
title: "Limit model : RSGWW" of "Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector"

description: Limit
description: No data abstract available.
DOI: 10.17182/hepdata.79779.v1/t5
title: "Limit model : VBF-HVTWW" of "Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector"

description: Limit
description: No data abstract available.
DOI: 10.17182/hepdata.79779.v1/t6
title: "Limit model : VBF-HVTWZ" of "Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector"

description: Limit
description: No data abstract available.
DOI: 10.17182/hepdata.79779.v1/t7
title: "Limit model : VBFWWNWA" of "Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector"

description: Limit
description: No data abstract available.
DOI: 10.17182/hepdata.79779.v1/t8
title: "Limit model : ggHWWNWA" of "Search for $WW/WZ$ resonance production in $\ell \nu qq$ final states in $pp$ collisions at $\sqrt{s} =$ 13 TeV with the ATLAS detector"

description: Limit
description: No data abstract available.
DOI: 10.17182/hepdata.79797.v1/t1
title: "Table 1" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Upper limits on Zprime to Z h production cross section x branching fraction in pb
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t2
title: "Table 2" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Upper limits on Wprime to W h production cross section x branching fraction in pb
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t10
title: "Table 10" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Acceptance * Reconstruction efficiency for pp-&gt; A (gluon fusion)
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t3
title: "Table 3" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Upper limits for the scaling factor of the production cross section for V’ times its branching fraction to Wh/Zh in Model A.
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t4
title: "Table 4" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Upper limits on A to Z h production cross section x branching fraction in pb (gluon fusion production)
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t5
title: "Table 5" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Upper limits on A to Z h production cross section x branching fraction in pb ( production with associated b-quarks)
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t6
title: "Table 6" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Acceptance * Reconstruction efficiency for pp-&gt; Zprime
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t7
title: "Table 7" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Acceptance * Reconstruction efficiency for pp-&gt; Zprime
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t8
title: "Table 8" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Acceptance * Reconstruction efficiency for pp-&gt; Wprime
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t9
title: "Table 9" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Acceptance * Reconstruction efficiency for pp-&gt; A (gluon fusion)
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t11
title: "Table 11" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Acceptance * Reconstruction efficiency for pp-&gt; A (b-quark associated)
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t12
title: "Table 12" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Acceptance * Reconstruction efficiency for pp-&gt; A (b-quark associated)
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t13
title: "Table 13" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Upper limits at the 95% CL on the product of the production cross-section for pp-&gt;A and the branching fractions for A-&gt;Zh and h-&gt;bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 10%.
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t14
title: "Table 14" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Upper limits at the 95% CL on the product of the production cross-section for pp-&gt;A and the branching fractions for A-&gt;Zh and h-&gt;bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 20%.
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t15
title: "Table 15" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Upper limits at the 95% CL on the product of the production cross-section for pp-&gt;A and the branching fractions for A-&gt;Zh and h-&gt;bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 30%.
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t16
title: "Table 16" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Upper limits at the 95% CL on the product of the production cross-section for pp-&gt;A and the branching fractions for A-&gt;Zh and h-&gt;bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 40%.
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t17
title: "Table 17" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Upper limits at the 95% CL on the product of the production cross-section for pp-&gt;A and the branching fractions for A-&gt;Zh and h-&gt;bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 50%.
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t18
title: "Table 18" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Upper limits at the 95% CL on the product of the production cross-section for pp-&gt;A and the branching fractions for A-&gt;Zh and h-&gt;bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 60%.
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t19
title: "Table 19" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Upper limits at the 95% CL on the product of the production cross-section for pp-&gt;A and the branching fractions for A-&gt;Zh and h-&gt;bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 70%.
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector
DOI: 10.17182/hepdata.79797.v1/t20
title: "Table 20" of "Search for heavy resonances decaying into a $W$ or $Z$ boson and a Higgs boson in final states with leptons and $b$-jets in 36 fb$^{-1}$ of $\sqrt s = 13$ TeV $pp$ collisions with the ATLAS detector"

description: Upper limits at the 95% CL on the product of the production cross-section for pp-&gt;A and the branching fractions for A-&gt;Zh and h-&gt;bb evaluated by combining the 0-lepton and 2-lepton channels. The signal is smeared by a Breit-Wigner function with A boson width of 0% , assuming a combination of the gluon--gluon fusion and b-quark associated production modes with a bbA fraction of 80%.
description: CERN-ATLAS. Search for heavy resonances decaying into a W or Z boson and a Higgs boson in final states with leptons and b-jets in 36 1/fb of 13 TeV pp collisions with the ATLAS detector