cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.135676.v1/t10
title: "Table 9" of "Charged-hadron production in $pp$, $p$+Pb, Pb+Pb, and Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5$ TeV with the ATLAS detector at the LHC"

description: Charged-hadron spectrum in the centrality interval 0-90% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.
description: CERN-LHC. Charged-hadron spectra obtained in $pp$, $p$+Pb, and Pb+Pb collisions at $\sqrt{s}$ or $\sqrt{s_{_\text{NN}}}=5.02$TeV, and in Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5.44$TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25pb${}^{-1}$, 28nb${}^{-1}$, 0.50nb${}^{-1}$, and 3$\mu$b${}^{-1}$, respectively. The nuclear modification factors $R_{p\text{Pb}}$ and $R_\text{AA}$ are obtained by comparing the spectra in heavy-ion and $pp$ collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor $R_{p\text{Pb}}$ shows a moderate enhancement above unity with maximum at $p_{\mathrm{T}} \approx 3$GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct $p_{\mathrm{T}}$-dependence with a local maximum at $p_{\mathrm{T}} \approx 2$GeV and local minimum at $p_{\mathrm{T}} \approx 7$GeV. This dependence is more distinguishable in more central collisions. No significant $|\eta|$-dependence is found.
DOI: 10.17182/hepdata.135676.v1/t11
title: "Table 10" of "Charged-hadron production in $pp$, $p$+Pb, Pb+Pb, and Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5$ TeV with the ATLAS detector at the LHC"

description: Charged-hadron cross-section in pp collisions. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.
description: CERN-LHC. Charged-hadron spectra obtained in $pp$, $p$+Pb, and Pb+Pb collisions at $\sqrt{s}$ or $\sqrt{s_{_\text{NN}}}=5.02$TeV, and in Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5.44$TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25pb${}^{-1}$, 28nb${}^{-1}$, 0.50nb${}^{-1}$, and 3$\mu$b${}^{-1}$, respectively. The nuclear modification factors $R_{p\text{Pb}}$ and $R_\text{AA}$ are obtained by comparing the spectra in heavy-ion and $pp$ collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor $R_{p\text{Pb}}$ shows a moderate enhancement above unity with maximum at $p_{\mathrm{T}} \approx 3$GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct $p_{\mathrm{T}}$-dependence with a local maximum at $p_{\mathrm{T}} \approx 2$GeV and local minimum at $p_{\mathrm{T}} \approx 7$GeV. This dependence is more distinguishable in more central collisions. No significant $|\eta|$-dependence is found.
DOI: 10.17182/hepdata.135676.v1/t12
title: "Table 11" of "Charged-hadron production in $pp$, $p$+Pb, Pb+Pb, and Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5$ TeV with the ATLAS detector at the LHC"

description: Charged-hadron spectrum in the centrality interval 0-5% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.
description: CERN-LHC. Charged-hadron spectra obtained in $pp$, $p$+Pb, and Pb+Pb collisions at $\sqrt{s}$ or $\sqrt{s_{_\text{NN}}}=5.02$TeV, and in Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5.44$TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25pb${}^{-1}$, 28nb${}^{-1}$, 0.50nb${}^{-1}$, and 3$\mu$b${}^{-1}$, respectively. The nuclear modification factors $R_{p\text{Pb}}$ and $R_\text{AA}$ are obtained by comparing the spectra in heavy-ion and $pp$ collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor $R_{p\text{Pb}}$ shows a moderate enhancement above unity with maximum at $p_{\mathrm{T}} \approx 3$GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct $p_{\mathrm{T}}$-dependence with a local maximum at $p_{\mathrm{T}} \approx 2$GeV and local minimum at $p_{\mathrm{T}} \approx 7$GeV. This dependence is more distinguishable in more central collisions. No significant $|\eta|$-dependence is found.
DOI: 10.17182/hepdata.135676.v1/t13
title: "Table 12" of "Charged-hadron production in $pp$, $p$+Pb, Pb+Pb, and Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5$ TeV with the ATLAS detector at the LHC"

description: Charged-hadron spectrum in the centrality interval 5-10% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.
description: CERN-LHC. Charged-hadron spectra obtained in $pp$, $p$+Pb, and Pb+Pb collisions at $\sqrt{s}$ or $\sqrt{s_{_\text{NN}}}=5.02$TeV, and in Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5.44$TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25pb${}^{-1}$, 28nb${}^{-1}$, 0.50nb${}^{-1}$, and 3$\mu$b${}^{-1}$, respectively. The nuclear modification factors $R_{p\text{Pb}}$ and $R_\text{AA}$ are obtained by comparing the spectra in heavy-ion and $pp$ collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor $R_{p\text{Pb}}$ shows a moderate enhancement above unity with maximum at $p_{\mathrm{T}} \approx 3$GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct $p_{\mathrm{T}}$-dependence with a local maximum at $p_{\mathrm{T}} \approx 2$GeV and local minimum at $p_{\mathrm{T}} \approx 7$GeV. This dependence is more distinguishable in more central collisions. No significant $|\eta|$-dependence is found.
DOI: 10.17182/hepdata.135676.v1/t14
title: "Table 13" of "Charged-hadron production in $pp$, $p$+Pb, Pb+Pb, and Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5$ TeV with the ATLAS detector at the LHC"

description: Charged-hadron spectrum in the centrality interval 10-20% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.
description: CERN-LHC. Charged-hadron spectra obtained in $pp$, $p$+Pb, and Pb+Pb collisions at $\sqrt{s}$ or $\sqrt{s_{_\text{NN}}}=5.02$TeV, and in Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5.44$TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25pb${}^{-1}$, 28nb${}^{-1}$, 0.50nb${}^{-1}$, and 3$\mu$b${}^{-1}$, respectively. The nuclear modification factors $R_{p\text{Pb}}$ and $R_\text{AA}$ are obtained by comparing the spectra in heavy-ion and $pp$ collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor $R_{p\text{Pb}}$ shows a moderate enhancement above unity with maximum at $p_{\mathrm{T}} \approx 3$GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct $p_{\mathrm{T}}$-dependence with a local maximum at $p_{\mathrm{T}} \approx 2$GeV and local minimum at $p_{\mathrm{T}} \approx 7$GeV. This dependence is more distinguishable in more central collisions. No significant $|\eta|$-dependence is found.
DOI: 10.17182/hepdata.135676.v1/t15
title: "Table 14" of "Charged-hadron production in $pp$, $p$+Pb, Pb+Pb, and Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5$ TeV with the ATLAS detector at the LHC"

description: Charged-hadron spectrum in the centrality interval 20-30% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.
description: CERN-LHC. Charged-hadron spectra obtained in $pp$, $p$+Pb, and Pb+Pb collisions at $\sqrt{s}$ or $\sqrt{s_{_\text{NN}}}=5.02$TeV, and in Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5.44$TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25pb${}^{-1}$, 28nb${}^{-1}$, 0.50nb${}^{-1}$, and 3$\mu$b${}^{-1}$, respectively. The nuclear modification factors $R_{p\text{Pb}}$ and $R_\text{AA}$ are obtained by comparing the spectra in heavy-ion and $pp$ collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor $R_{p\text{Pb}}$ shows a moderate enhancement above unity with maximum at $p_{\mathrm{T}} \approx 3$GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct $p_{\mathrm{T}}$-dependence with a local maximum at $p_{\mathrm{T}} \approx 2$GeV and local minimum at $p_{\mathrm{T}} \approx 7$GeV. This dependence is more distinguishable in more central collisions. No significant $|\eta|$-dependence is found.
DOI: 10.17182/hepdata.135676.v1/t16
title: "Table 15" of "Charged-hadron production in $pp$, $p$+Pb, Pb+Pb, and Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5$ TeV with the ATLAS detector at the LHC"

description: Charged-hadron spectrum in the centrality interval 30-40% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.
description: CERN-LHC. Charged-hadron spectra obtained in $pp$, $p$+Pb, and Pb+Pb collisions at $\sqrt{s}$ or $\sqrt{s_{_\text{NN}}}=5.02$TeV, and in Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5.44$TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25pb${}^{-1}$, 28nb${}^{-1}$, 0.50nb${}^{-1}$, and 3$\mu$b${}^{-1}$, respectively. The nuclear modification factors $R_{p\text{Pb}}$ and $R_\text{AA}$ are obtained by comparing the spectra in heavy-ion and $pp$ collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor $R_{p\text{Pb}}$ shows a moderate enhancement above unity with maximum at $p_{\mathrm{T}} \approx 3$GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct $p_{\mathrm{T}}$-dependence with a local maximum at $p_{\mathrm{T}} \approx 2$GeV and local minimum at $p_{\mathrm{T}} \approx 7$GeV. This dependence is more distinguishable in more central collisions. No significant $|\eta|$-dependence is found.
DOI: 10.17182/hepdata.135676.v1/t8
title: "Table 7" of "Charged-hadron production in $pp$, $p$+Pb, Pb+Pb, and Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5$ TeV with the ATLAS detector at the LHC"

description: Charged-hadron spectrum in the centrality interval 40-60% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.
description: CERN-LHC. Charged-hadron spectra obtained in $pp$, $p$+Pb, and Pb+Pb collisions at $\sqrt{s}$ or $\sqrt{s_{_\text{NN}}}=5.02$TeV, and in Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5.44$TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25pb${}^{-1}$, 28nb${}^{-1}$, 0.50nb${}^{-1}$, and 3$\mu$b${}^{-1}$, respectively. The nuclear modification factors $R_{p\text{Pb}}$ and $R_\text{AA}$ are obtained by comparing the spectra in heavy-ion and $pp$ collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor $R_{p\text{Pb}}$ shows a moderate enhancement above unity with maximum at $p_{\mathrm{T}} \approx 3$GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct $p_{\mathrm{T}}$-dependence with a local maximum at $p_{\mathrm{T}} \approx 2$GeV and local minimum at $p_{\mathrm{T}} \approx 7$GeV. This dependence is more distinguishable in more central collisions. No significant $|\eta|$-dependence is found.
DOI: 10.17182/hepdata.135676.v1/t9
title: "Table 8" of "Charged-hadron production in $pp$, $p$+Pb, Pb+Pb, and Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5$ TeV with the ATLAS detector at the LHC"

description: Charged-hadron spectrum in the centrality interval 60-90% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.
description: CERN-LHC. Charged-hadron spectra obtained in $pp$, $p$+Pb, and Pb+Pb collisions at $\sqrt{s}$ or $\sqrt{s_{_\text{NN}}}=5.02$TeV, and in Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5.44$TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25pb${}^{-1}$, 28nb${}^{-1}$, 0.50nb${}^{-1}$, and 3$\mu$b${}^{-1}$, respectively. The nuclear modification factors $R_{p\text{Pb}}$ and $R_\text{AA}$ are obtained by comparing the spectra in heavy-ion and $pp$ collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor $R_{p\text{Pb}}$ shows a moderate enhancement above unity with maximum at $p_{\mathrm{T}} \approx 3$GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct $p_{\mathrm{T}}$-dependence with a local maximum at $p_{\mathrm{T}} \approx 2$GeV and local minimum at $p_{\mathrm{T}} \approx 7$GeV. This dependence is more distinguishable in more central collisions. No significant $|\eta|$-dependence is found.
DOI: 10.17182/hepdata.135676.v1/t17
title: "Table 16" of "Charged-hadron production in $pp$, $p$+Pb, Pb+Pb, and Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5$ TeV with the ATLAS detector at the LHC"

description: Charged-hadron spectrum in the centrality interval 40-50% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.
description: CERN-LHC. Charged-hadron spectra obtained in $pp$, $p$+Pb, and Pb+Pb collisions at $\sqrt{s}$ or $\sqrt{s_{_\text{NN}}}=5.02$TeV, and in Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5.44$TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25pb${}^{-1}$, 28nb${}^{-1}$, 0.50nb${}^{-1}$, and 3$\mu$b${}^{-1}$, respectively. The nuclear modification factors $R_{p\text{Pb}}$ and $R_\text{AA}$ are obtained by comparing the spectra in heavy-ion and $pp$ collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor $R_{p\text{Pb}}$ shows a moderate enhancement above unity with maximum at $p_{\mathrm{T}} \approx 3$GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct $p_{\mathrm{T}}$-dependence with a local maximum at $p_{\mathrm{T}} \approx 2$GeV and local minimum at $p_{\mathrm{T}} \approx 7$GeV. This dependence is more distinguishable in more central collisions. No significant $|\eta|$-dependence is found.
DOI: 10.17182/hepdata.135676.v1/t18
title: "Table 17" of "Charged-hadron production in $pp$, $p$+Pb, Pb+Pb, and Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5$ TeV with the ATLAS detector at the LHC"

description: Charged-hadron spectrum in the centrality interval 50-60% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.
description: CERN-LHC. Charged-hadron spectra obtained in $pp$, $p$+Pb, and Pb+Pb collisions at $\sqrt{s}$ or $\sqrt{s_{_\text{NN}}}=5.02$TeV, and in Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5.44$TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25pb${}^{-1}$, 28nb${}^{-1}$, 0.50nb${}^{-1}$, and 3$\mu$b${}^{-1}$, respectively. The nuclear modification factors $R_{p\text{Pb}}$ and $R_\text{AA}$ are obtained by comparing the spectra in heavy-ion and $pp$ collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor $R_{p\text{Pb}}$ shows a moderate enhancement above unity with maximum at $p_{\mathrm{T}} \approx 3$GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct $p_{\mathrm{T}}$-dependence with a local maximum at $p_{\mathrm{T}} \approx 2$GeV and local minimum at $p_{\mathrm{T}} \approx 7$GeV. This dependence is more distinguishable in more central collisions. No significant $|\eta|$-dependence is found.
DOI: 10.17182/hepdata.135676.v1/t19
title: "Table 18" of "Charged-hadron production in $pp$, $p$+Pb, Pb+Pb, and Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5$ TeV with the ATLAS detector at the LHC"

description: Charged-hadron spectrum in the centrality interval 60-80% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.
description: CERN-LHC. Charged-hadron spectra obtained in $pp$, $p$+Pb, and Pb+Pb collisions at $\sqrt{s}$ or $\sqrt{s_{_\text{NN}}}=5.02$TeV, and in Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5.44$TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25pb${}^{-1}$, 28nb${}^{-1}$, 0.50nb${}^{-1}$, and 3$\mu$b${}^{-1}$, respectively. The nuclear modification factors $R_{p\text{Pb}}$ and $R_\text{AA}$ are obtained by comparing the spectra in heavy-ion and $pp$ collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor $R_{p\text{Pb}}$ shows a moderate enhancement above unity with maximum at $p_{\mathrm{T}} \approx 3$GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct $p_{\mathrm{T}}$-dependence with a local maximum at $p_{\mathrm{T}} \approx 2$GeV and local minimum at $p_{\mathrm{T}} \approx 7$GeV. This dependence is more distinguishable in more central collisions. No significant $|\eta|$-dependence is found.
DOI: 10.17182/hepdata.135676.v1/t20
title: "Table 19" of "Charged-hadron production in $pp$, $p$+Pb, Pb+Pb, and Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5$ TeV with the ATLAS detector at the LHC"

description: Charged-hadron cross-section in pp collisions. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.
description: CERN-LHC. Charged-hadron spectra obtained in $pp$, $p$+Pb, and Pb+Pb collisions at $\sqrt{s}$ or $\sqrt{s_{_\text{NN}}}=5.02$TeV, and in Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5.44$TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25pb${}^{-1}$, 28nb${}^{-1}$, 0.50nb${}^{-1}$, and 3$\mu$b${}^{-1}$, respectively. The nuclear modification factors $R_{p\text{Pb}}$ and $R_\text{AA}$ are obtained by comparing the spectra in heavy-ion and $pp$ collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor $R_{p\text{Pb}}$ shows a moderate enhancement above unity with maximum at $p_{\mathrm{T}} \approx 3$GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct $p_{\mathrm{T}}$-dependence with a local maximum at $p_{\mathrm{T}} \approx 2$GeV and local minimum at $p_{\mathrm{T}} \approx 7$GeV. This dependence is more distinguishable in more central collisions. No significant $|\eta|$-dependence is found.
DOI: 10.17182/hepdata.135676.v1/t21
title: "Table 20" of "Charged-hadron production in $pp$, $p$+Pb, Pb+Pb, and Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5$ TeV with the ATLAS detector at the LHC"

description: Charged-hadron spectrum in the centrality interval 0-5% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.
description: CERN-LHC. Charged-hadron spectra obtained in $pp$, $p$+Pb, and Pb+Pb collisions at $\sqrt{s}$ or $\sqrt{s_{_\text{NN}}}=5.02$TeV, and in Xe+Xe collisions at $\sqrt{s_{_\text{NN}}}=5.44$TeV. The data recorded by the ATLAS detector at the LHC have total integrated luminosities of 25pb${}^{-1}$, 28nb${}^{-1}$, 0.50nb${}^{-1}$, and 3$\mu$b${}^{-1}$, respectively. The nuclear modification factors $R_{p\text{Pb}}$ and $R_\text{AA}$ are obtained by comparing the spectra in heavy-ion and $pp$ collisions in a wide range of charged-particle transverse momenta and pseudorapidity. The nuclear modification factor $R_{p\text{Pb}}$ shows a moderate enhancement above unity with maximum at $p_{\mathrm{T}} \approx 3$GeV; the enhancement is stronger in the Pb-going direction. The nuclear modification factors in both Pb+Pb and Xe+Xe collisions feature a significant, centrality-dependent suppression. They show a similar distinct $p_{\mathrm{T}}$-dependence with a local maximum at $p_{\mathrm{T}} \approx 2$GeV and local minimum at $p_{\mathrm{T}} \approx 7$GeV. This dependence is more distinguishable in more central collisions. No significant $|\eta|$-dependence is found.