cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.91237.v4/t1
title: "Table 1" of "Search for the $HH \rightarrow b \bar{b} b \bar{b}$ process via vector-boson fusion production using proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Acceptance x efficiency versus $\kappa_{2V}$ for non-resonant signal of $HH$.
description: CERN-ATLAS. Searches for HH-&gt;bbbb process via vector boson fusion production using proton-proton collisions at sqrt(s)=13 TeV with the ATLAS detector
DOI: 10.17182/hepdata.91237.v4/t2
title: "Table 2" of "Search for the $HH \rightarrow b \bar{b} b \bar{b}$ process via vector-boson fusion production using proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Acceptance x efficiency versus resonance mass for both narrow and broad resonance $X$ to $HH$.
description: CERN-ATLAS. Searches for HH-&gt;bbbb process via vector boson fusion production using proton-proton collisions at sqrt(s)=13 TeV with the ATLAS detector
DOI: 10.17182/hepdata.91237.v4/t3
title: "Table 3" of "Search for the $HH \rightarrow b \bar{b} b \bar{b}$ process via vector-boson fusion production using proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Post-fit mass distribution of the $HH$ candidates in the signal region. The expected background is shown after the profile-likelihood fit to data with the background-only hypothesis; the narrow-width resonant signal at 800 GeV and the non-resonant signal at $\kappa_{2V}$ = 3 are overlaid, both normalised to the corresponding observed upper limits on the cross-section.
description: CERN-ATLAS. Searches for HH-&gt;bbbb process via vector boson fusion production using proton-proton collisions at sqrt(s)=13 TeV with the ATLAS detector
DOI: 10.17182/hepdata.91237.v4/t4
title: "Table 4" of "Search for the $HH \rightarrow b \bar{b} b \bar{b}$ process via vector-boson fusion production using proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Observed and expected limits at 95% CL on the cross-section of narrow resonance $X$ to $HH$ as a function of the mass $m_{X}$.
description: CERN-ATLAS. Searches for HH-&gt;bbbb process via vector boson fusion production using proton-proton collisions at sqrt(s)=13 TeV with the ATLAS detector
DOI: 10.17182/hepdata.91237.v4/t5
title: "Table 5" of "Search for the $HH \rightarrow b \bar{b} b \bar{b}$ process via vector-boson fusion production using proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Observed and expected limits at 95% CL on the cross-section of broad resonance $X$ to $HH$ as a function of the mass $m_{X}$.
description: CERN-ATLAS. Searches for HH-&gt;bbbb process via vector boson fusion production using proton-proton collisions at sqrt(s)=13 TeV with the ATLAS detector
DOI: 10.17182/hepdata.91237.v4/t6
title: "Table 6" of "Search for the $HH \rightarrow b \bar{b} b \bar{b}$ process via vector-boson fusion production using proton-proton collisions at $\sqrt{s} = 13$ TeV with the ATLAS detector"

description: Observed and expected limits at 95% CL on the cross-sections of non-resonant $HH$ production via VBF as a function of the di-vector-boson-di-Higgs-boson coupling modifier $\kappa_{2V}$. The theory prediction of the cross-section as a function of $\kappa_{2V}$ is also shown. The minimum theory cross-section is 1.37 fb at $\kappa_{2V}=1.17$.
description: CERN-ATLAS. Searches for HH-&gt;bbbb process via vector boson fusion production using proton-proton collisions at sqrt(s)=13 TeV with the ATLAS detector
DOI: 10.17182/hepdata.91238.v1/t1
title: "Table 1" of "Coherent J/$\psi$ photoproduction at forward rapidity in ultra-peripheral Pb-Pb collisions at $\sqrt{s_{\rm{NN}}}=5.02$ TeV"

description: Differential cross section as a function of rapidity for coherent J/PSI photoproduction in ultra-peripheral Pb-Pb collisions.
description: No data abstract available.
DOI: 10.17182/hepdata.91239.v1/t1
title: "Jets in pp 5.02 TeV" of "Measurement of charged jet cross section in $pp$ collisions at ${\sqrt{s}=5.02}$ TeV"

description: Fig. 3: Fully corrected charged jet differential cross sections in pp collisions at $\\sqrt{s}$ = 5.02 TeV. Statistical uncertainties are displayed as vertical error bars. The total systematic uncertainties are shown as shaded bands around the data points. Data are scaled to enhance visibility.
description: No data abstract available.
DOI: 10.17182/hepdata.91239.v1/t2
title: "Cross section ratio with radius" of "Measurement of charged jet cross section in $pp$ collisions at ${\sqrt{s}=5.02}$ TeV"

description: Fig. 6: Charged jet cross section ratios for $\\sigma$(R = 0.2)/$\\sigma$(R = 0.4) (Red) and $\\sigma$(R = 0.2)/$\\sigma$(R = 0.6). The systematic uncertainty of the cross section ratio is indicated by a shaded band drawn around data points.
description: No data abstract available.
DOI: 10.17182/hepdata.91239.v1/t3
title: "Jets with UE subtraction in pp 5.02 TeV" of "Measurement of charged jet cross section in $pp$ collisions at ${\sqrt{s}=5.02}$ TeV"

description: Charged jet differential cross sections with UE subtraction in pp collisions at $\sqrt{s}$ = 5.02 TeV. Statistical uncertainties are displayed as vertical error bars. The total systematic uncertainties are shown as shaded bands around the data points. Data are scaled to enhance visibility.
description: No data abstract available.
DOI: 10.17182/hepdata.91239.v1/t4
title: "Jets with leading $p_{T}$ 5 GeV/$c$ in pp 5.02 TeV" of "Measurement of charged jet cross section in $pp$ collisions at ${\sqrt{s}=5.02}$ TeV"

description: Charged jet differential cross sections without UE subtraction in pp collisions at $\sqrt{s}$ = 5.02 TeV with the leading track bias. All jets must contain at least one track with $p_{T}$ &gt; 5 GeV/$c$. Statistical uncertainties are displayed as vertical error bars. The total systematic uncertainties are shown as shaded bands around the data points. Data are scaled to enhance visibility
description: No data abstract available.
DOI: 10.17182/hepdata.91241.v1/t1
title: "Figure 2(a)" of "Search for flavour-changing neutral currents in processes with one top quark and a photon using 81 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS experiment"

description: Post-fit distributions of a background-only fit to the signal region (SR) and the control regions (CRs) of the NN output in the SR. In addition, the expected signal is overlaid for an effective coupling strength corresponding to the observed limit multiplied by a factor of ten.
description: CERN-LHC, ATLAS. A search for flavour-changing neutral current events via the coupling of a top quark, a photon, and an up or charm quark is presented using 81$fb^{−1}$ of proton-proton collision data taken at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC. Events with a photon, an electron or muon, a $b$-tagged jet, and missing transverse momentum are selected. A neural network based on kinematic variables differentiates between events from signal and background processes. The data are consistent with the background-only hypothesis, and limits are set on the strength of the $tq\gamma$ coupling in an effective field theory. These are also interpreted as 95 % CL upper limits on the cross section for FCNC $t\gamma$ production via a left-handed (right-handed) $tu\gamma$ coupling of 36 fb (78 fb) and on the branching ratio for $t \rightarrow \gamma u$ of $2.8 \times 10^{−5}$ ($6.1 \times 10^{−5}$). In addition, they are interpreted as 95 % CL upper limits on the cross section for FCNC $t\gamma$ production via a left-handed (right-handed) $tc\gamma$ coupling of 40 fb (33 fb) and on the branching ratio for $t \rightarrow \gamma c$ of $22 \times 10^{−5}$ ($18 \times 10^{−5}$).
DOI: 10.17182/hepdata.91241.v1/t2
title: "Table 1" of "Search for flavour-changing neutral currents in processes with one top quark and a photon using 81 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS experiment"

description: Observed (expected) 95 % CL limits on the effective coupling strengths for different vertices and couplings, the production cross section, and the branching ratio. For the former, the energy scale is assumed to be $\Lambda$ = 1 TeV.
description: CERN-LHC, ATLAS. A search for flavour-changing neutral current events via the coupling of a top quark, a photon, and an up or charm quark is presented using 81$fb^{−1}$ of proton-proton collision data taken at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC. Events with a photon, an electron or muon, a $b$-tagged jet, and missing transverse momentum are selected. A neural network based on kinematic variables differentiates between events from signal and background processes. The data are consistent with the background-only hypothesis, and limits are set on the strength of the $tq\gamma$ coupling in an effective field theory. These are also interpreted as 95 % CL upper limits on the cross section for FCNC $t\gamma$ production via a left-handed (right-handed) $tu\gamma$ coupling of 36 fb (78 fb) and on the branching ratio for $t \rightarrow \gamma u$ of $2.8 \times 10^{−5}$ ($6.1 \times 10^{−5}$). In addition, they are interpreted as 95 % CL upper limits on the cross section for FCNC $t\gamma$ production via a left-handed (right-handed) $tc\gamma$ coupling of 40 fb (33 fb) and on the branching ratio for $t \rightarrow \gamma c$ of $22 \times 10^{−5}$ ($18 \times 10^{−5}$).
DOI: 10.17182/hepdata.91241.v1/t3
title: "Auxiliary Figure 2(a)" of "Search for flavour-changing neutral currents in processes with one top quark and a photon using 81 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS experiment"

description: Post-fit distributions of a background-only fit to the SR and the CRs of the NN output in the SR for the $tu\gamma$ right-handed coupling. In addition, the expected signal is overlaid for an effective coupling strength corresponding to the observed limit multiplied by a factor of ten.
description: CERN-LHC, ATLAS. A search for flavour-changing neutral current events via the coupling of a top quark, a photon, and an up or charm quark is presented using 81$fb^{−1}$ of proton-proton collision data taken at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC. Events with a photon, an electron or muon, a $b$-tagged jet, and missing transverse momentum are selected. A neural network based on kinematic variables differentiates between events from signal and background processes. The data are consistent with the background-only hypothesis, and limits are set on the strength of the $tq\gamma$ coupling in an effective field theory. These are also interpreted as 95 % CL upper limits on the cross section for FCNC $t\gamma$ production via a left-handed (right-handed) $tu\gamma$ coupling of 36 fb (78 fb) and on the branching ratio for $t \rightarrow \gamma u$ of $2.8 \times 10^{−5}$ ($6.1 \times 10^{−5}$). In addition, they are interpreted as 95 % CL upper limits on the cross section for FCNC $t\gamma$ production via a left-handed (right-handed) $tc\gamma$ coupling of 40 fb (33 fb) and on the branching ratio for $t \rightarrow \gamma c$ of $22 \times 10^{−5}$ ($18 \times 10^{−5}$).
DOI: 10.17182/hepdata.91241.v1/t4
title: "Auxiliary Figure 2(b)" of "Search for flavour-changing neutral currents in processes with one top quark and a photon using 81 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS experiment"

description: Post-fit distributions of a background-only fit to the SR and the CRs of the NN output in the SR for the $tc\gamma$ left-handed coupling. In addition, the expected signal is overlaid for an effective coupling strength corresponding to the observed limit multiplied by a factor of ten.
description: CERN-LHC, ATLAS. A search for flavour-changing neutral current events via the coupling of a top quark, a photon, and an up or charm quark is presented using 81$fb^{−1}$ of proton-proton collision data taken at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC. Events with a photon, an electron or muon, a $b$-tagged jet, and missing transverse momentum are selected. A neural network based on kinematic variables differentiates between events from signal and background processes. The data are consistent with the background-only hypothesis, and limits are set on the strength of the $tq\gamma$ coupling in an effective field theory. These are also interpreted as 95 % CL upper limits on the cross section for FCNC $t\gamma$ production via a left-handed (right-handed) $tu\gamma$ coupling of 36 fb (78 fb) and on the branching ratio for $t \rightarrow \gamma u$ of $2.8 \times 10^{−5}$ ($6.1 \times 10^{−5}$). In addition, they are interpreted as 95 % CL upper limits on the cross section for FCNC $t\gamma$ production via a left-handed (right-handed) $tc\gamma$ coupling of 40 fb (33 fb) and on the branching ratio for $t \rightarrow \gamma c$ of $22 \times 10^{−5}$ ($18 \times 10^{−5}$).
DOI: 10.17182/hepdata.91241.v1/t5
title: "Auxiliary Figure 2(c)" of "Search for flavour-changing neutral currents in processes with one top quark and a photon using 81 fb$^{-1}$ of $pp$ collisions at $\sqrt{s} = 13$ TeV with the ATLAS experiment"

description: Post-fit distributions of a background-only fit to the SR and the CRs of the NN output in the SR for the $tc\gamma$ right-handed coupling. In addition, the expected signal is overlaid for an effective coupling strength corresponding to the observed limit multiplied by a factor of ten.
description: CERN-LHC, ATLAS. A search for flavour-changing neutral current events via the coupling of a top quark, a photon, and an up or charm quark is presented using 81$fb^{−1}$ of proton-proton collision data taken at a centre-of-mass energy of 13 TeV with the ATLAS detector at the LHC. Events with a photon, an electron or muon, a $b$-tagged jet, and missing transverse momentum are selected. A neural network based on kinematic variables differentiates between events from signal and background processes. The data are consistent with the background-only hypothesis, and limits are set on the strength of the $tq\gamma$ coupling in an effective field theory. These are also interpreted as 95 % CL upper limits on the cross section for FCNC $t\gamma$ production via a left-handed (right-handed) $tu\gamma$ coupling of 36 fb (78 fb) and on the branching ratio for $t \rightarrow \gamma u$ of $2.8 \times 10^{−5}$ ($6.1 \times 10^{−5}$). In addition, they are interpreted as 95 % CL upper limits on the cross section for FCNC $t\gamma$ production via a left-handed (right-handed) $tc\gamma$ coupling of 40 fb (33 fb) and on the branching ratio for $t \rightarrow \gamma c$ of $22 \times 10^{−5}$ ($18 \times 10^{−5}$).
DOI: 10.17182/hepdata.91242.v1/t1
title: "Table 1" of "Measurement of the $t\bar{t}$ production cross-section and lepton differential distributions in $e\mu $ dilepton events from $pp$ collisions at $\sqrt{s}=13\,\text {TeV}$ with the ATLAS detector"

description: Absolute differential cross-section in the fiducial region as a function of lepton pT. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb). The last bin includes overflow beyond the upper bin boundary. The corresponding correlation matrices are given in Tables 23 and 24.
description: CERN-LHC. Measurements of the absolute and fiducial differential cross-sections for single leptons and the dilepton system in ttbar production at sqrt(s)=13 TeV, decaying to the e-mu bbbar nnubar final state.
The fiducial region is defined as: - opposite sign electron and muon - each lepton with pT&gt;20 GeV and |eta|&lt;2.5 - no requirements on jets or missing transverse energy (neutrinos)
Results are provided including the contribution of leptonic tau decays, or corrected for the estimated tau contribution, corresponding to direct t-&gt;W-&gt;e/mu only
DOI: 10.17182/hepdata.91242.v1/t2
title: "Table 2" of "Measurement of the $t\bar{t}$ production cross-section and lepton differential distributions in $e\mu $ dilepton events from $pp$ collisions at $\sqrt{s}=13\,\text {TeV}$ with the ATLAS detector"

description: Normalised differential cross-section in the fiducial region as a function of lepton pT. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb). The last bin includes overflow beyond the upper bin boundary. The corresponding correlation matrices are given in Tables 25 and 26.
description: CERN-LHC. Measurements of the absolute and fiducial differential cross-sections for single leptons and the dilepton system in ttbar production at sqrt(s)=13 TeV, decaying to the e-mu bbbar nnubar final state.
The fiducial region is defined as: - opposite sign electron and muon - each lepton with pT&gt;20 GeV and |eta|&lt;2.5 - no requirements on jets or missing transverse energy (neutrinos)
Results are provided including the contribution of leptonic tau decays, or corrected for the estimated tau contribution, corresponding to direct t-&gt;W-&gt;e/mu only
DOI: 10.17182/hepdata.91242.v1/t3
title: "Table 3" of "Measurement of the $t\bar{t}$ production cross-section and lepton differential distributions in $e\mu $ dilepton events from $pp$ collisions at $\sqrt{s}=13\,\text {TeV}$ with the ATLAS detector"

description: Absolute differential cross-section in the fiducial region as a function of lepton |eta|. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb). The corresponding correlation matrices are given in Tables 27 and 28.
description: CERN-LHC. Measurements of the absolute and fiducial differential cross-sections for single leptons and the dilepton system in ttbar production at sqrt(s)=13 TeV, decaying to the e-mu bbbar nnubar final state.
The fiducial region is defined as: - opposite sign electron and muon - each lepton with pT&gt;20 GeV and |eta|&lt;2.5 - no requirements on jets or missing transverse energy (neutrinos)
Results are provided including the contribution of leptonic tau decays, or corrected for the estimated tau contribution, corresponding to direct t-&gt;W-&gt;e/mu only
DOI: 10.17182/hepdata.91242.v1/t4
title: "Table 4" of "Measurement of the $t\bar{t}$ production cross-section and lepton differential distributions in $e\mu $ dilepton events from $pp$ collisions at $\sqrt{s}=13\,\text {TeV}$ with the ATLAS detector"

description: Normalised differential cross-section in the fiducial region as a function of lepton |eta|. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb). The corresponding correlation matrices are given in Tables 29 and 30.
description: CERN-LHC. Measurements of the absolute and fiducial differential cross-sections for single leptons and the dilepton system in ttbar production at sqrt(s)=13 TeV, decaying to the e-mu bbbar nnubar final state.
The fiducial region is defined as: - opposite sign electron and muon - each lepton with pT&gt;20 GeV and |eta|&lt;2.5 - no requirements on jets or missing transverse energy (neutrinos)
Results are provided including the contribution of leptonic tau decays, or corrected for the estimated tau contribution, corresponding to direct t-&gt;W-&gt;e/mu only
DOI: 10.17182/hepdata.91242.v1/t5
title: "Table 5" of "Measurement of the $t\bar{t}$ production cross-section and lepton differential distributions in $e\mu $ dilepton events from $pp$ collisions at $\sqrt{s}=13\,\text {TeV}$ with the ATLAS detector"

description: Absolute differential cross-section in the fiducial region as a function of dilepton pT. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb). The last bin includes overflow beyond the upper bin boundary. The corresponding correlation matrices are given in Tables 31 and 32.
description: CERN-LHC. Measurements of the absolute and fiducial differential cross-sections for single leptons and the dilepton system in ttbar production at sqrt(s)=13 TeV, decaying to the e-mu bbbar nnubar final state.
The fiducial region is defined as: - opposite sign electron and muon - each lepton with pT&gt;20 GeV and |eta|&lt;2.5 - no requirements on jets or missing transverse energy (neutrinos)
Results are provided including the contribution of leptonic tau decays, or corrected for the estimated tau contribution, corresponding to direct t-&gt;W-&gt;e/mu only
DOI: 10.17182/hepdata.91242.v1/t6
title: "Table 6" of "Measurement of the $t\bar{t}$ production cross-section and lepton differential distributions in $e\mu $ dilepton events from $pp$ collisions at $\sqrt{s}=13\,\text {TeV}$ with the ATLAS detector"

description: Normalised differential cross-section in the fiducial region as a function of dilepton pT. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb). The last bin includes overflow beyond the upper bin boundary. The corresponding correlation matrices are given in Tables 33 and 34.
description: CERN-LHC. Measurements of the absolute and fiducial differential cross-sections for single leptons and the dilepton system in ttbar production at sqrt(s)=13 TeV, decaying to the e-mu bbbar nnubar final state.
The fiducial region is defined as: - opposite sign electron and muon - each lepton with pT&gt;20 GeV and |eta|&lt;2.5 - no requirements on jets or missing transverse energy (neutrinos)
Results are provided including the contribution of leptonic tau decays, or corrected for the estimated tau contribution, corresponding to direct t-&gt;W-&gt;e/mu only
DOI: 10.17182/hepdata.91242.v1/t10
title: "Table 10" of "Measurement of the $t\bar{t}$ production cross-section and lepton differential distributions in $e\mu $ dilepton events from $pp$ collisions at $\sqrt{s}=13\,\text {TeV}$ with the ATLAS detector"

description: Normalised differential cross-section in the fiducial region as a function of dilepton |rapidity|. The first column gives the cross-section including contributions from leptonic tau decays, the second without. Systematic uncertainties are given for ttbar modelling (ttmod), lepton calibration (lept), jet and b-tagging calibration (jet), backgrounds (bkg) and integrated luminosity and beam energy (leb). The corresponding correlation matrices are given in Tables 41 and 42.
description: CERN-LHC. Measurements of the absolute and fiducial differential cross-sections for single leptons and the dilepton system in ttbar production at sqrt(s)=13 TeV, decaying to the e-mu bbbar nnubar final state.
The fiducial region is defined as: - opposite sign electron and muon - each lepton with pT&gt;20 GeV and |eta|&lt;2.5 - no requirements on jets or missing transverse energy (neutrinos)
Results are provided including the contribution of leptonic tau decays, or corrected for the estimated tau contribution, corresponding to direct t-&gt;W-&gt;e/mu only