cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.104860.v1/t96
title: "Cutflow: 5" of "Search for R-parity violating supersymmetry in a final state containing leptons and many jets with the ATLAS experiment using $\sqrt{s} = 13$ TeV proton-proton collision data"

description: Cut flow for the electroweakino production model, considering only the production of $\tilde{\chi}^{\pm}_1 \tilde{\chi}^0_1$, with $m(\tilde{\chi}^{\pm}_1,\tilde{\chi}^0_1)= 250$ GeV. The column labelled $\mathrm{N}_{\mathrm{raw}}$ shows the number of generated events, while $\mathrm{N}_{\mathrm{events}}$ shows the expected number of events with a luminosity of 139fb$^{−1}$. The last column shows the cut flow efficiency with respect to all weighted events. The events are skimmed by requiring at least one electron or muon that satisfies very loose identification criteria, where the lepton satisfies $p_{\mathrm{T}} &gt; 25$ GeV. The efficiency of this cut is considered in the quoted efficiency of the lepton trigger requirement. Selections with negligible inefficiencies on the given sample, such as data quality requirements, are not displayed. In the $2\ell^{\mathrm{sc}}$ category no events are expected, as only one lepton is expected to be produced in the decay.Selections that have not been evaluated in the analysis or are not applicable are denoted with a dash (--).
description: CERN-LHC.

A search for R-parity violating supersymmetry in final states characterised by high jet multiplicity, at least one isolated light lepton and either zero or at least three $b$-tagged jets is presented. The search uses 139 fb$^{-1}$ of $\sqrt{s} = 13$ TeV proton-proton collision data collected by the ATLAS experiment during Run 2 of the Large Hadron Collider. The results are interpreted in the context of R-parity-violating supersymmetry models that feature gluino production, top-squark production, or electroweakino production. The dominant sources of background are estimated using a data-driven model, based on observables at medium jet multiplicity, to predict the $b$-tagged jet multiplicity distribution at the higher jet multiplicities used in the search. Machine learning techniques are used to reach sensitivity to electroweakino production, extending the data-driven background estimation to the shape of the machine learning discriminant. No significant excess over the Standard Model expectation is observed and exclusion limits at the 95% confidence-level are extracted, reaching as high as 2.4 TeV in gluino mass, 1.35 TeV in top-squark mass, and 320 (365) GeV in higgsino (wino) mass.
DOI: 10.17182/hepdata.104860.v1/t97
title: "Cutflow: 6" of "Search for R-parity violating supersymmetry in a final state containing leptons and many jets with the ATLAS experiment using $\sqrt{s} = 13$ TeV proton-proton collision data"

description: Cut flow for the electroweakino production model, considering only the production of $\tilde{\chi}^0_1 \tilde{\chi}^0_2$, with $m(\tilde{\chi}^0_1,\tilde{\chi}^0_2)= 250$ GeV. The column labelled $\mathrm{N}_{\mathrm{raw}}$ shows the number of generated events, while $\mathrm{N}_{\mathrm{events}}$ shows the expected number of events with a luminosity of 139fb$^{−1}$. The last column shows the cut flow efficiency with respect to all weighted events. The events are skimmed by requiring at least one electron or muon that satisfies very loose identification criteria, where the lepton satisfies $p_{\mathrm{T}} &gt; 25$ GeV. The efficiency of this cut is considered in the quoted efficiency of the lepton trigger requirement. Selections with negligible inefficiencies on the given sample, such as data quality requirements, are not displayed. Selections that have not been evaluated in the analysis or are not applicable are denoted with a dash (--).
description: CERN-LHC.

A search for R-parity violating supersymmetry in final states characterised by high jet multiplicity, at least one isolated light lepton and either zero or at least three $b$-tagged jets is presented. The search uses 139 fb$^{-1}$ of $\sqrt{s} = 13$ TeV proton-proton collision data collected by the ATLAS experiment during Run 2 of the Large Hadron Collider. The results are interpreted in the context of R-parity-violating supersymmetry models that feature gluino production, top-squark production, or electroweakino production. The dominant sources of background are estimated using a data-driven model, based on observables at medium jet multiplicity, to predict the $b$-tagged jet multiplicity distribution at the higher jet multiplicities used in the search. Machine learning techniques are used to reach sensitivity to electroweakino production, extending the data-driven background estimation to the shape of the machine learning discriminant. No significant excess over the Standard Model expectation is observed and exclusion limits at the 95% confidence-level are extracted, reaching as high as 2.4 TeV in gluino mass, 1.35 TeV in top-squark mass, and 320 (365) GeV in higgsino (wino) mass.
DOI: 10.17182/hepdata.104861.v1/t1
title: "Table 1" of "Search for lepton-flavor violating decays of the Higgs boson in the $\mu\tau$ and e$\tau$ final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed (expected) 95% CL upper limits on $B(H\to\mu\tau)$ for each individual category and combined
description: No data abstract available.
DOI: 10.17182/hepdata.104861.v1/t2
title: "Table 2" of "Search for lepton-flavor violating decays of the Higgs boson in the $\mu\tau$ and e$\tau$ final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Observed (expected) 95% CL upper limits on $B(H\to e\tau)$ for each individual category and combined
description: No data abstract available.
DOI: 10.17182/hepdata.104861.v1/t3
title: "Table 3" of "Search for lepton-flavor violating decays of the Higgs boson in the $\mu\tau$ and e$\tau$ final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: Summary of observed and expected upper limits at 95% CL, best fit branching fractions and corresponding constraints on Yukawa couplings for the $H\to\mu\tau$ and $H\to e\tau$ channels
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t3
title: "Table 3" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $p_{T}$-distributions of kaons ($K^{+}+K^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t1
title: "Table 1" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $p_{T}$-distributions of pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t2
title: "Table 2" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $p_{T}$-distributions of pions ($\pi^{+}+\pi^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t4
title: "Table 4" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $p_{T}$-distributions of kaons ($K^{+}+K^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t5
title: "Table 5" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $p_{T}$-distributions of protons ($p+pbar$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t6
title: "Table 6" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $p_{T}$-distributions of protons ($p+pbar$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t7
title: "Table 7" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $p_{T}$-distributions of kaons ($K^{+}+K^{-}$)/pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104861.v1/t4
title: "Table 4" of "Search for lepton-flavor violating decays of the Higgs boson in the $\mu\tau$ and e$\tau$ final states in proton-proton collisions at $\sqrt{s}$ = 13 TeV"

description: 95% CL observed upper limits on the Yukawa couplings
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t10
title: "Table 10" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $p_{T}$-distributions of protons ($p+pbar$)/pions ($\pi^{+}+\pi^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t11
title: "Table 11" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Integrated yield ratios of kaons ($K^{+}+K^{-}$) to pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t12
title: "Table 12" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Integrated yield ratios of kaons ($K^{+}+K^{-}$) to pions ($\pi^{+}+\pi^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t8
title: "Table 8" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $p_{T}$-distributions of kaons ($K^{+}+K^{-}$)/pions ($\pi^{+}+\pi^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t9
title: "Table 9" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $p_{T}$-distributions of protons ($p+pbar$)/pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t13
title: "Table 13" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Integrated yield ratios of protons ($p+pbar$) to pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t14
title: "Table 14" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: Integrated yield ratios of protons ($p+pbar$) to pions ($\pi^{+}+\pi^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t15
title: "Table 15" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $p_{T}$-dependent nuclear modification factor of pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t16
title: "Table 16" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $p_{T}$-dependent nuclear modification factor of kaons ($K^{+}+K^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104923.v1/t17
title: "Table 17" of "Production of charged pions, kaons and (anti-)protons in Pb-Pb and inelastic pp collisions at $\sqrt{s_{\rm{NN}}}$ = 5.02 TeV"

description: $p_{T}$-dependent nuclear modification factor of protons ($p+pbar$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.
description: No data abstract available.
DOI: 10.17182/hepdata.104924.v1/t1
title: "Table 5 (binned)" of "Measurement of prompt open-charm production cross sections in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The differential cross sections of prompt D^{*+} plus D^{*-}, D0 + bar{D0}, and D+ + D-production in pT bins with |eta| &lt; 2.1;the first uncertainty is statistical, the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.104925.v1/t1
title: "ph1_pt" of "Measurement of the production cross section of pairs of isolated photons in $pp$ collisions at 13 TeV with the ATLAS detector"

description: Differential cross section as a function of $p_{T,\gamma_{1}}$. The table contains the values measured in data and theory predictions from SHERPA, DIPHOX and NNLOJET.
description: Measurement of inclusive production cross section of pairs of isolated prompt photons with the ATLAS Detector at centre-of-mass energy 13 TeV.The transverse momentum of the photons is required to be greater than 40(30) GeV for the (sub)leading photon. The photons are required to be seperated by more than $\Delta R &gt; 0.4$. The photons are required to be isolated with $E_\mathrm{T}^\mathrm{iso}&lt;0.09\cdot p_{\mathrm{T},\gamma}$. The isolation energy $E_\mathrm{T}^\mathrm{iso}$ is defined as the scalar sum of the transverse momenta of particles in a cone of $\Delta R &lt; 0.2$ around the photon and is corrected for the transverse momentum density of jets in the event.For each differential cross section measurement 100 data bootstrap replicas are provided in the resources which should be used to estimate the statistical uncertainty and the correlations between different observables. For convenience the statitistical uncertainties are also contained in the main tables.The systematic uncertainties can be considered fully correlated and seperate up-and down-variations are provided. Sometimes the up-and down-variations have the same sign. The uncertainties need to be symmetrized before calculating chi2 values.
DOI: 10.17182/hepdata.104925.v1/t2
title: "ph2_pt" of "Measurement of the production cross section of pairs of isolated photons in $pp$ collisions at 13 TeV with the ATLAS detector"

description: Differential cross section as a function of $p_{T,\gamma_{2}}$. The table contains the values measured in data and theory predictions from SHERPA, DIPHOX and NNLOJET.
description: Measurement of inclusive production cross section of pairs of isolated prompt photons with the ATLAS Detector at centre-of-mass energy 13 TeV.The transverse momentum of the photons is required to be greater than 40(30) GeV for the (sub)leading photon. The photons are required to be seperated by more than $\Delta R &gt; 0.4$. The photons are required to be isolated with $E_\mathrm{T}^\mathrm{iso}&lt;0.09\cdot p_{\mathrm{T},\gamma}$. The isolation energy $E_\mathrm{T}^\mathrm{iso}$ is defined as the scalar sum of the transverse momenta of particles in a cone of $\Delta R &lt; 0.2$ around the photon and is corrected for the transverse momentum density of jets in the event.For each differential cross section measurement 100 data bootstrap replicas are provided in the resources which should be used to estimate the statistical uncertainty and the correlations between different observables. For convenience the statitistical uncertainties are also contained in the main tables.The systematic uncertainties can be considered fully correlated and seperate up-and down-variations are provided. Sometimes the up-and down-variations have the same sign. The uncertainties need to be symmetrized before calculating chi2 values.
DOI: 10.17182/hepdata.104925.v1/t3
title: "yy_xs" of "Measurement of the production cross section of pairs of isolated photons in $pp$ collisions at 13 TeV with the ATLAS detector"

description: Integrated fiducial cross section measured in data and from different predictions.
description: Measurement of inclusive production cross section of pairs of isolated prompt photons with the ATLAS Detector at centre-of-mass energy 13 TeV.The transverse momentum of the photons is required to be greater than 40(30) GeV for the (sub)leading photon. The photons are required to be seperated by more than $\Delta R &gt; 0.4$. The photons are required to be isolated with $E_\mathrm{T}^\mathrm{iso}&lt;0.09\cdot p_{\mathrm{T},\gamma}$. The isolation energy $E_\mathrm{T}^\mathrm{iso}$ is defined as the scalar sum of the transverse momenta of particles in a cone of $\Delta R &lt; 0.2$ around the photon and is corrected for the transverse momentum density of jets in the event.For each differential cross section measurement 100 data bootstrap replicas are provided in the resources which should be used to estimate the statistical uncertainty and the correlations between different observables. For convenience the statitistical uncertainties are also contained in the main tables.The systematic uncertainties can be considered fully correlated and seperate up-and down-variations are provided. Sometimes the up-and down-variations have the same sign. The uncertainties need to be symmetrized before calculating chi2 values.
DOI: 10.17182/hepdata.104925.v1/t4
title: "yy_m" of "Measurement of the production cross section of pairs of isolated photons in $pp$ collisions at 13 TeV with the ATLAS detector"

description: Differential cross section as a function of $m_{\gamma\gamma}$. The table contains the values measured in data and theory predictions from SHERPA, DIPHOX and NNLOJET.
description: Measurement of inclusive production cross section of pairs of isolated prompt photons with the ATLAS Detector at centre-of-mass energy 13 TeV.The transverse momentum of the photons is required to be greater than 40(30) GeV for the (sub)leading photon. The photons are required to be seperated by more than $\Delta R &gt; 0.4$. The photons are required to be isolated with $E_\mathrm{T}^\mathrm{iso}&lt;0.09\cdot p_{\mathrm{T},\gamma}$. The isolation energy $E_\mathrm{T}^\mathrm{iso}$ is defined as the scalar sum of the transverse momenta of particles in a cone of $\Delta R &lt; 0.2$ around the photon and is corrected for the transverse momentum density of jets in the event.For each differential cross section measurement 100 data bootstrap replicas are provided in the resources which should be used to estimate the statistical uncertainty and the correlations between different observables. For convenience the statitistical uncertainties are also contained in the main tables.The systematic uncertainties can be considered fully correlated and seperate up-and down-variations are provided. Sometimes the up-and down-variations have the same sign. The uncertainties need to be symmetrized before calculating chi2 values.
DOI: 10.17182/hepdata.104925.v1/t6
title: "yy_pTt" of "Measurement of the production cross section of pairs of isolated photons in $pp$ collisions at 13 TeV with the ATLAS detector"

description: Differential cross section as a function of $a_{T,\gamma\gamma}$. The table contains the values measured in data and theory predictions from SHERPA, DIPHOX and NNLOJET.
description: Measurement of inclusive production cross section of pairs of isolated prompt photons with the ATLAS Detector at centre-of-mass energy 13 TeV.The transverse momentum of the photons is required to be greater than 40(30) GeV for the (sub)leading photon. The photons are required to be seperated by more than $\Delta R &gt; 0.4$. The photons are required to be isolated with $E_\mathrm{T}^\mathrm{iso}&lt;0.09\cdot p_{\mathrm{T},\gamma}$. The isolation energy $E_\mathrm{T}^\mathrm{iso}$ is defined as the scalar sum of the transverse momenta of particles in a cone of $\Delta R &lt; 0.2$ around the photon and is corrected for the transverse momentum density of jets in the event.For each differential cross section measurement 100 data bootstrap replicas are provided in the resources which should be used to estimate the statistical uncertainty and the correlations between different observables. For convenience the statitistical uncertainties are also contained in the main tables.The systematic uncertainties can be considered fully correlated and seperate up-and down-variations are provided. Sometimes the up-and down-variations have the same sign. The uncertainties need to be symmetrized before calculating chi2 values.
DOI: 10.17182/hepdata.104924.v1/t2
title: "Table 6 (binned)" of "Measurement of prompt open-charm production cross sections in proton-proton collisions at $\sqrt{s} = $ 13 TeV"

description: The differential cross sections of prompt D^{*+} plus D^{*-}, D0 + bar{D0}, and D+ + D-production in |eta| bins with 4 &lt; pT &lt; 100 GeV;the first uncertainty is statistical, the second is systematic.
description: No data abstract available.
DOI: 10.17182/hepdata.104925.v1/t5
title: "yy_pT" of "Measurement of the production cross section of pairs of isolated photons in $pp$ collisions at 13 TeV with the ATLAS detector"

description: Differential cross section as a function of $p_{T,\gamma\gamma}$. The table contains the values measured in data and theory predictions from SHERPA, DIPHOX and NNLOJET.
description: Measurement of inclusive production cross section of pairs of isolated prompt photons with the ATLAS Detector at centre-of-mass energy 13 TeV.The transverse momentum of the photons is required to be greater than 40(30) GeV for the (sub)leading photon. The photons are required to be seperated by more than $\Delta R &gt; 0.4$. The photons are required to be isolated with $E_\mathrm{T}^\mathrm{iso}&lt;0.09\cdot p_{\mathrm{T},\gamma}$. The isolation energy $E_\mathrm{T}^\mathrm{iso}$ is defined as the scalar sum of the transverse momenta of particles in a cone of $\Delta R &lt; 0.2$ around the photon and is corrected for the transverse momentum density of jets in the event.For each differential cross section measurement 100 data bootstrap replicas are provided in the resources which should be used to estimate the statistical uncertainty and the correlations between different observables. For convenience the statitistical uncertainties are also contained in the main tables.The systematic uncertainties can be considered fully correlated and seperate up-and down-variations are provided. Sometimes the up-and down-variations have the same sign. The uncertainties need to be symmetrized before calculating chi2 values.