cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.132904.v1/t14
title: "Table 14" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of results for jet RAA as a function of pT and in bins of rg for 0-10% centrality interval. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.132904.v1/t15
title: "Table 15" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of results for jet RAA as a function of rg and in bins of pT for 50-80% centrality interval. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.132904.v1/t16
title: "Table 16" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of results for jet RAA as a function of rg and in bins of pT for 30-50% centrality interval. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.132904.v1/t17
title: "Table 17" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of results for jet RAA as a function of rg and in bins of pT for 10-30% centrality interval. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.130943.v1/t1
title: "Table 1" of "Strong constraints on jet quenching in centrality-dependent $p$+Pb collisions at 5.02 TeV from ATLAS"

description: The per-jet charged particle yield in pPb and pp collisions for hadrons near a $p_{T}^{\textrm{jet}} &gt; 30~\textrm{GeV}$ jet ($\Delta\phi_{\textrm{ch,jet}} &lt; \pi/8$).
description: No data abstract available.
DOI: 10.17182/hepdata.130943.v1/t2
title: "Table 2" of "Strong constraints on jet quenching in centrality-dependent $p$+Pb collisions at 5.02 TeV from ATLAS"

description: The per-jet charged particle yield in pPb and pp collisions for hadrons opposite to a $p_{T}^{\textrm{jet}} &gt; 30~\textrm{GeV}$ jet ($\Delta\phi_{\textrm{ch,jet}} &gt; 7\pi/8$).
description: No data abstract available.
DOI: 10.17182/hepdata.130943.v1/t3
title: "Table 3" of "Strong constraints on jet quenching in centrality-dependent $p$+Pb collisions at 5.02 TeV from ATLAS"

description: The per-jet charged particle yield in pPb and pp collisions for hadrons near a $p_{T}^{\textrm{jet}} &gt; 60~\textrm{GeV}$ jet ($\Delta\phi_{\textrm{ch,jet}} &lt; \pi/8$).
description: No data abstract available.
DOI: 10.17182/hepdata.130943.v1/t4
title: "Table 4" of "Strong constraints on jet quenching in centrality-dependent $p$+Pb collisions at 5.02 TeV from ATLAS"

description: The per-jet charged particle yield in pPb and pp collisions for hadrons opposite to a $p_{T}^{\textrm{jet}} &gt; 60~\textrm{GeV}$ jet ($\Delta\phi_{\textrm{ch,jet}} &gt; 7\pi/8$).
description: No data abstract available.
DOI: 10.17182/hepdata.130943.v1/t5
title: "Table 5" of "Strong constraints on jet quenching in centrality-dependent $p$+Pb collisions at 5.02 TeV from ATLAS"

description: The ratio of per-jet charged particle yields in pPb and pp collisions, $I_{pPb}$, for hadrons near a $p_{T}^{\textrm{jet}} &gt; 30~\textrm{GeV}$ jet ($\Delta\phi_{\textrm{ch,jet}} &lt; \pi/8$).
description: No data abstract available.
DOI: 10.17182/hepdata.130943.v1/t6
title: "Table 6" of "Strong constraints on jet quenching in centrality-dependent $p$+Pb collisions at 5.02 TeV from ATLAS"

description: The ratio of per-jet charged particle yields in pPb and pp collisions, $I_{pPb}$, for hadrons opposite to a $p_{T}^{\textrm{jet}} &gt; 30~\textrm{GeV}$ jet ($\Delta\phi_{\textrm{ch,jet}} &gt; 7\pi/8$).
description: No data abstract available.
DOI: 10.17182/hepdata.130943.v1/t7
title: "Table 7" of "Strong constraints on jet quenching in centrality-dependent $p$+Pb collisions at 5.02 TeV from ATLAS"

description: The ratio of per-jet charged particle yields in pPb and pp collisions, $I_{pPb}$, for hadrons near a $p_{T}^{\textrm{jet}} &gt; 60~\textrm{GeV}$ jet ($\Delta\phi_{\textrm{ch,jet}} &lt; \pi/8$).
description: No data abstract available.
DOI: 10.17182/hepdata.130943.v1/t8
title: "Table 8" of "Strong constraints on jet quenching in centrality-dependent $p$+Pb collisions at 5.02 TeV from ATLAS"

description: The ratio of per-jet charged particle yields in pPb and pp collisions, $I_{pPb}$, for hadrons opposite to a $p_{T}^{\textrm{jet}} &gt; 60~\textrm{GeV}$ jet ($\Delta\phi_{\textrm{ch,jet}} &gt; 7\pi/8$).
description: No data abstract available.
DOI: 10.17182/hepdata.132904.v1/t18
title: "Table 18" of "Measurement of substructure-dependent jet suppression in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of results for jet RAA as a function of rg and in bins of pT for 0-10% centrality interval. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Jet substructure modification and suppression are measured in Pb+Pb collisions with respect to pp collisions with the ATLAS detector at the Large Hadron Collider. Jets used in this analysis are clustered using the anti-kT algorithm with a radius parameter R = 0.4. The jet constituents, defined by both tracking and calorimeter information, are used to define the angular scale rg of the first hard splitting inside the jet by reclustering them using the Cambridge-Aachen algorithm and employing the soft drop grooming technique with parameters 𝛽 = 0 and 𝑧cut = 0.2. The jet nuclear modification factor, RAA, used to characterize the jet suppression in Pb+Pb collisions, is presented differentially in rg, jet transverse momentum, and in intervals of collision centrality. The RAA is observed to depend significantly on jet 𝑟g, with the production of jets with the largest measured rg found to be twice as suppressed compared to those with the smallest rg in central Pb+Pb collisions. The RAA values do not exhibit a strong variation with jet pT in any of the rg intervals. The rg and pT dependence of jet RAA is qualitatively consistent with a picture of jet quenching arising from coherence and provides the most direct evidence in support of this approach.
DOI: 10.17182/hepdata.29583.v1/t1
title: "Table 1" of "$K^- p$ elastic scattering at 10 GeV/c"

description: No description provided.
description: PRELIMINARY REPORT BASED ON PARTIAL SET OF DATA. FULL RESULTS ARE GIVEN IN J. BARTSCH ET AL., NP B29, 398 (1971).
DOI: 10.17182/hepdata.139684.v1/t1
title: "Table 1" of "Measurements of the suppression and correlations of dijets in Xe+Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV"

description: The centrality intervals in Xe+Xe collisions and their corresponding TAA with absolute uncertainties.
description: A measurement of the suppression and correlations of dijets is performed using 3~$\mu$b$^{-1}$ of Xe+Xe data at $\sqrt{s_{\mathrm{NN}}} = 5.44$~TeV collected with the ATLAS detector at the LHC. Dijets with jets reconstructed using the $R=0.4$ anti-$k_t$ algorithm are measured differentially in jet $p_{\text{T}}$ over the range of 32~GeV to 398~GeV and centrality of the collision. Significant dijet momentum imbalance is found in the most central Xe+Xe collisions, which decreases in more peripheral collisions. Results from the measurement of per-pair normalized and absolutely normalized dijet $p_{\text{T}}$ balance are compared with previous Pb+Pb measurement at $\sqrt{s_{\mathrm{NN}}} =5.02$~TeV. The differences between the dijet suppression in Xe+Xe and Pb+Pb are further quantified by the ratio of pair nuclear modification factors. The results are found to be consistent with those measured in Pb+Pb data when compared in classes of the same event activity and when taking into account the difference in the centre-of-mass energy of the initial parton scattering process between Xe+Xe and Pb+Pb collisions. These results provide a better understanding of the role of energy density, system size, path-length, and fluctuations in the parton energy loss.
DOI: 10.17182/hepdata.139684.v1/t2
title: "Table 2" of "Measurements of the suppression and correlations of dijets in Xe+Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV"

description: The centrality intervals in Xe+Xe and Pb+Pb collisions for matching SUM ET FCAL intervals and respective TAA values for Xe+Xe collisions.
description: A measurement of the suppression and correlations of dijets is performed using 3~$\mu$b$^{-1}$ of Xe+Xe data at $\sqrt{s_{\mathrm{NN}}} = 5.44$~TeV collected with the ATLAS detector at the LHC. Dijets with jets reconstructed using the $R=0.4$ anti-$k_t$ algorithm are measured differentially in jet $p_{\text{T}}$ over the range of 32~GeV to 398~GeV and centrality of the collision. Significant dijet momentum imbalance is found in the most central Xe+Xe collisions, which decreases in more peripheral collisions. Results from the measurement of per-pair normalized and absolutely normalized dijet $p_{\text{T}}$ balance are compared with previous Pb+Pb measurement at $\sqrt{s_{\mathrm{NN}}} =5.02$~TeV. The differences between the dijet suppression in Xe+Xe and Pb+Pb are further quantified by the ratio of pair nuclear modification factors. The results are found to be consistent with those measured in Pb+Pb data when compared in classes of the same event activity and when taking into account the difference in the centre-of-mass energy of the initial parton scattering process between Xe+Xe and Pb+Pb collisions. These results provide a better understanding of the role of energy density, system size, path-length, and fluctuations in the parton energy loss.
DOI: 10.17182/hepdata.139684.v1/t3
title: "Figure 1a" of "Measurements of the suppression and correlations of dijets in Xe+Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV"

description: The performance of the jet energy scale (JES) for jets with $|y| &lt; 2.1$ evaluated as a function of pT_truth in different centrality bins. Simulated hard scatter events were overlaid onto events from a dedicated sample of minimum-bias Xe+Xe data.
description: A measurement of the suppression and correlations of dijets is performed using 3~$\mu$b$^{-1}$ of Xe+Xe data at $\sqrt{s_{\mathrm{NN}}} = 5.44$~TeV collected with the ATLAS detector at the LHC. Dijets with jets reconstructed using the $R=0.4$ anti-$k_t$ algorithm are measured differentially in jet $p_{\text{T}}$ over the range of 32~GeV to 398~GeV and centrality of the collision. Significant dijet momentum imbalance is found in the most central Xe+Xe collisions, which decreases in more peripheral collisions. Results from the measurement of per-pair normalized and absolutely normalized dijet $p_{\text{T}}$ balance are compared with previous Pb+Pb measurement at $\sqrt{s_{\mathrm{NN}}} =5.02$~TeV. The differences between the dijet suppression in Xe+Xe and Pb+Pb are further quantified by the ratio of pair nuclear modification factors. The results are found to be consistent with those measured in Pb+Pb data when compared in classes of the same event activity and when taking into account the difference in the centre-of-mass energy of the initial parton scattering process between Xe+Xe and Pb+Pb collisions. These results provide a better understanding of the role of energy density, system size, path-length, and fluctuations in the parton energy loss.
DOI: 10.17182/hepdata.139684.v1/t4
title: "Figure 1b" of "Measurements of the suppression and correlations of dijets in Xe+Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV"

description: The performance of jet energy resolution (JER) for jets with |y| &lt; 2.1 evaluated as a function of pT_truth in different centrality bins. Simulated hard scatter events were overlaid onto events from a dedicated sample of minimum-bias Xe+Xe data. The fit parameters are listed in a sperate table (Extras 1)
description: A measurement of the suppression and correlations of dijets is performed using 3~$\mu$b$^{-1}$ of Xe+Xe data at $\sqrt{s_{\mathrm{NN}}} = 5.44$~TeV collected with the ATLAS detector at the LHC. Dijets with jets reconstructed using the $R=0.4$ anti-$k_t$ algorithm are measured differentially in jet $p_{\text{T}}$ over the range of 32~GeV to 398~GeV and centrality of the collision. Significant dijet momentum imbalance is found in the most central Xe+Xe collisions, which decreases in more peripheral collisions. Results from the measurement of per-pair normalized and absolutely normalized dijet $p_{\text{T}}$ balance are compared with previous Pb+Pb measurement at $\sqrt{s_{\mathrm{NN}}} =5.02$~TeV. The differences between the dijet suppression in Xe+Xe and Pb+Pb are further quantified by the ratio of pair nuclear modification factors. The results are found to be consistent with those measured in Pb+Pb data when compared in classes of the same event activity and when taking into account the difference in the centre-of-mass energy of the initial parton scattering process between Xe+Xe and Pb+Pb collisions. These results provide a better understanding of the role of energy density, system size, path-length, and fluctuations in the parton energy loss.
DOI: 10.17182/hepdata.139684.v1/t6
title: "Figure 2b" of "Measurements of the suppression and correlations of dijets in Xe+Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV"

description: The relative magnitude of systematic uncertainties for absolutely normalized xJ distributions in 0-10% Xe+Xe centrality
description: A measurement of the suppression and correlations of dijets is performed using 3~$\mu$b$^{-1}$ of Xe+Xe data at $\sqrt{s_{\mathrm{NN}}} = 5.44$~TeV collected with the ATLAS detector at the LHC. Dijets with jets reconstructed using the $R=0.4$ anti-$k_t$ algorithm are measured differentially in jet $p_{\text{T}}$ over the range of 32~GeV to 398~GeV and centrality of the collision. Significant dijet momentum imbalance is found in the most central Xe+Xe collisions, which decreases in more peripheral collisions. Results from the measurement of per-pair normalized and absolutely normalized dijet $p_{\text{T}}$ balance are compared with previous Pb+Pb measurement at $\sqrt{s_{\mathrm{NN}}} =5.02$~TeV. The differences between the dijet suppression in Xe+Xe and Pb+Pb are further quantified by the ratio of pair nuclear modification factors. The results are found to be consistent with those measured in Pb+Pb data when compared in classes of the same event activity and when taking into account the difference in the centre-of-mass energy of the initial parton scattering process between Xe+Xe and Pb+Pb collisions. These results provide a better understanding of the role of energy density, system size, path-length, and fluctuations in the parton energy loss.
DOI: 10.17182/hepdata.139684.v1/t10
title: "Figure 3c" of "Measurements of the suppression and correlations of dijets in Xe+Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV"

description: Per-pair normalized xJ distribution evaluated in four centrality intervals and given pT1 interval.
description: A measurement of the suppression and correlations of dijets is performed using 3~$\mu$b$^{-1}$ of Xe+Xe data at $\sqrt{s_{\mathrm{NN}}} = 5.44$~TeV collected with the ATLAS detector at the LHC. Dijets with jets reconstructed using the $R=0.4$ anti-$k_t$ algorithm are measured differentially in jet $p_{\text{T}}$ over the range of 32~GeV to 398~GeV and centrality of the collision. Significant dijet momentum imbalance is found in the most central Xe+Xe collisions, which decreases in more peripheral collisions. Results from the measurement of per-pair normalized and absolutely normalized dijet $p_{\text{T}}$ balance are compared with previous Pb+Pb measurement at $\sqrt{s_{\mathrm{NN}}} =5.02$~TeV. The differences between the dijet suppression in Xe+Xe and Pb+Pb are further quantified by the ratio of pair nuclear modification factors. The results are found to be consistent with those measured in Pb+Pb data when compared in classes of the same event activity and when taking into account the difference in the centre-of-mass energy of the initial parton scattering process between Xe+Xe and Pb+Pb collisions. These results provide a better understanding of the role of energy density, system size, path-length, and fluctuations in the parton energy loss.
DOI: 10.17182/hepdata.139684.v1/t11
title: "Figure 4a" of "Measurements of the suppression and correlations of dijets in Xe+Xe collisions at $\sqrt{s_{NN}}$ = 5.44 TeV"

description: Absolutely normalized xJ distribution evaluated in four centrality intervals and given pT1 interval.
description: A measurement of the suppression and correlations of dijets is performed using 3~$\mu$b$^{-1}$ of Xe+Xe data at $\sqrt{s_{\mathrm{NN}}} = 5.44$~TeV collected with the ATLAS detector at the LHC. Dijets with jets reconstructed using the $R=0.4$ anti-$k_t$ algorithm are measured differentially in jet $p_{\text{T}}$ over the range of 32~GeV to 398~GeV and centrality of the collision. Significant dijet momentum imbalance is found in the most central Xe+Xe collisions, which decreases in more peripheral collisions. Results from the measurement of per-pair normalized and absolutely normalized dijet $p_{\text{T}}$ balance are compared with previous Pb+Pb measurement at $\sqrt{s_{\mathrm{NN}}} =5.02$~TeV. The differences between the dijet suppression in Xe+Xe and Pb+Pb are further quantified by the ratio of pair nuclear modification factors. The results are found to be consistent with those measured in Pb+Pb data when compared in classes of the same event activity and when taking into account the difference in the centre-of-mass energy of the initial parton scattering process between Xe+Xe and Pb+Pb collisions. These results provide a better understanding of the role of energy density, system size, path-length, and fluctuations in the parton energy loss.