cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.111123.v1/t4
title: "Table 4" of "Measurement of the nuclear modification factor for muons from charm and bottom hadrons in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of results for charm muon RAA as a function of pT for five different centrality. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Heavy flavour hadron production provides information about the transport properties and the microscopic structure of the quark-gluon plasma created in ultra-relativistic heavy-ion collisions. A measurement of the production of muons from the semi-leptonic decays of charm and bottom hadrons in Pb+Pb and pp collisions at a nucleon-nucleon center-of-mass energy of 5.02 TeV with the ATLAS detector at the Large Hadron Collider is presented. The Pb+Pb data were collected in 2015 and 2018 with sampled integrated luminosities of 208 mub^-1 and 38 mub^-1, respectively, and pp data with a sampled integrated luminosity of 1.17 pb^-1 were collected in 2017. The differential muons yield in Pb+Pb and pp cross section are measured in the transverse momentum range from 4 GeV to 30 GeV and pseudorapidity interval up to 2. Muons from heavy flavour semi-leptonic decays are separated from the light flavour hadronic background using the momentum imbalance between the inner detector and the muon spectrometer measurements, and muons coming from charm and bottom decays are further separated via the muon track transverse impact parameter. The nuclear modification factor for the charm and bottom muons is presented as a function of the muon transverse momentum in intervals of Pb+Pb collision centrality. The measured nuclear modification factors quantify significant suppression of the yields for muons coming from the decays of charm and bottom hadron, with stronger effects for muons coming from charm hadron decays.
DOI: 10.17182/hepdata.111123.v1/t5
title: "Table 5" of "Measurement of the nuclear modification factor for muons from charm and bottom hadrons in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of results for bottom muon RAA as a function of pT for five different centrality. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Heavy flavour hadron production provides information about the transport properties and the microscopic structure of the quark-gluon plasma created in ultra-relativistic heavy-ion collisions. A measurement of the production of muons from the semi-leptonic decays of charm and bottom hadrons in Pb+Pb and pp collisions at a nucleon-nucleon center-of-mass energy of 5.02 TeV with the ATLAS detector at the Large Hadron Collider is presented. The Pb+Pb data were collected in 2015 and 2018 with sampled integrated luminosities of 208 mub^-1 and 38 mub^-1, respectively, and pp data with a sampled integrated luminosity of 1.17 pb^-1 were collected in 2017. The differential muons yield in Pb+Pb and pp cross section are measured in the transverse momentum range from 4 GeV to 30 GeV and pseudorapidity interval up to 2. Muons from heavy flavour semi-leptonic decays are separated from the light flavour hadronic background using the momentum imbalance between the inner detector and the muon spectrometer measurements, and muons coming from charm and bottom decays are further separated via the muon track transverse impact parameter. The nuclear modification factor for the charm and bottom muons is presented as a function of the muon transverse momentum in intervals of Pb+Pb collision centrality. The measured nuclear modification factors quantify significant suppression of the yields for muons coming from the decays of charm and bottom hadron, with stronger effects for muons coming from charm hadron decays.
DOI: 10.17182/hepdata.111123.v1/t6
title: "Table 6" of "Measurement of the nuclear modification factor for muons from charm and bottom hadrons in Pb+Pb collisions at 5.02 TeV with the ATLAS detector"

description: Summary of results for charm muon RAA to bottom muon RAA ratio as a function of pT for five different centrality. Uncertainties are statistical and systematic, respectively.
description: CERN-LHC. Heavy flavour hadron production provides information about the transport properties and the microscopic structure of the quark-gluon plasma created in ultra-relativistic heavy-ion collisions. A measurement of the production of muons from the semi-leptonic decays of charm and bottom hadrons in Pb+Pb and pp collisions at a nucleon-nucleon center-of-mass energy of 5.02 TeV with the ATLAS detector at the Large Hadron Collider is presented. The Pb+Pb data were collected in 2015 and 2018 with sampled integrated luminosities of 208 mub^-1 and 38 mub^-1, respectively, and pp data with a sampled integrated luminosity of 1.17 pb^-1 were collected in 2017. The differential muons yield in Pb+Pb and pp cross section are measured in the transverse momentum range from 4 GeV to 30 GeV and pseudorapidity interval up to 2. Muons from heavy flavour semi-leptonic decays are separated from the light flavour hadronic background using the momentum imbalance between the inner detector and the muon spectrometer measurements, and muons coming from charm and bottom decays are further separated via the muon track transverse impact parameter. The nuclear modification factor for the charm and bottom muons is presented as a function of the muon transverse momentum in intervals of Pb+Pb collision centrality. The measured nuclear modification factors quantify significant suppression of the yields for muons coming from the decays of charm and bottom hadron, with stronger effects for muons coming from charm hadron decays.
DOI: 10.17182/hepdata.132663.v1/t1
title: "Figure 1a" of "Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV with the ATLAS detector"

description: The JES for R = 0.2 jets in Pb+Pb collisions as a function of $p_T^{truth}$ for centrality selections of 0-5%, 5-10%, 10-20%, 20-40% and 40-60%.
description: CERN-LHC. The azimuthal variation of jet yields in heavy-ion collisions provides information about the path-length dependence of the energy loss experienced by partons passing through the hot, dense nuclear matter known as the quark-gluon plasma. This paper presents the azimuthal anisotropy coefficients, $v_2$, $v_3$, and $v_4$, for jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using the ATLAS detector at the LHC. The measurement uses data collected in 2015 and 2018, corresponding to an integrated luminosity of 2.2 nb$^{-1}$. The $v_n$ values are measured as a function of the transverse momentum of the jets between 71 and 398 GeV and the event centrality. A non-zero value of $v_2$ is measured in all but the most central collisions. The value of $v_2$ is largest for jets with lower transverse momentum, with values up to 0.05 in mid-central collisions. A smaller, non-zero value of $v_3$ of approximately 0.01 is measured with no significant dependence on jet $p_\mathrm{T}$ or centrality, suggesting that fluctuations in the initial state play a small but distinct role in jet energy loss. No significant $v_4$ is observed in any kinematic region.
DOI: 10.17182/hepdata.132663.v1/t2
title: "Figure 1b" of "Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV with the ATLAS detector"

description: The JER for R = 0.2 jets in Pb+Pb collisions as a function of $p_T^{truth}$ for centrality selections of 0-5%, 5-10%, 10-20%, 20-40% and 40-60%.
description: CERN-LHC. The azimuthal variation of jet yields in heavy-ion collisions provides information about the path-length dependence of the energy loss experienced by partons passing through the hot, dense nuclear matter known as the quark-gluon plasma. This paper presents the azimuthal anisotropy coefficients, $v_2$, $v_3$, and $v_4$, for jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using the ATLAS detector at the LHC. The measurement uses data collected in 2015 and 2018, corresponding to an integrated luminosity of 2.2 nb$^{-1}$. The $v_n$ values are measured as a function of the transverse momentum of the jets between 71 and 398 GeV and the event centrality. A non-zero value of $v_2$ is measured in all but the most central collisions. The value of $v_2$ is largest for jets with lower transverse momentum, with values up to 0.05 in mid-central collisions. A smaller, non-zero value of $v_3$ of approximately 0.01 is measured with no significant dependence on jet $p_\mathrm{T}$ or centrality, suggesting that fluctuations in the initial state play a small but distinct role in jet energy loss. No significant $v_4$ is observed in any kinematic region.
DOI: 10.17182/hepdata.132663.v1/t3
title: "Figure 2a" of "Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV with the ATLAS detector"

description: The JES for R = 0.2 jets in Pb+Pb collisions as a function of $2|\Psi_2-\phi^{reco}|$ for centrality selections of 0-5%, 5-10%, 10-20%, 20-40% and 40-60%.
description: CERN-LHC. The azimuthal variation of jet yields in heavy-ion collisions provides information about the path-length dependence of the energy loss experienced by partons passing through the hot, dense nuclear matter known as the quark-gluon plasma. This paper presents the azimuthal anisotropy coefficients, $v_2$, $v_3$, and $v_4$, for jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using the ATLAS detector at the LHC. The measurement uses data collected in 2015 and 2018, corresponding to an integrated luminosity of 2.2 nb$^{-1}$. The $v_n$ values are measured as a function of the transverse momentum of the jets between 71 and 398 GeV and the event centrality. A non-zero value of $v_2$ is measured in all but the most central collisions. The value of $v_2$ is largest for jets with lower transverse momentum, with values up to 0.05 in mid-central collisions. A smaller, non-zero value of $v_3$ of approximately 0.01 is measured with no significant dependence on jet $p_\mathrm{T}$ or centrality, suggesting that fluctuations in the initial state play a small but distinct role in jet energy loss. No significant $v_4$ is observed in any kinematic region.
DOI: 10.17182/hepdata.132663.v1/t4
title: "Figure 2b" of "Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV with the ATLAS detector"

description: The JER for R = 0.2 jets in Pb+Pb collisions as a function of $2|\Psi_2-\phi^{reco}|$ for centrality selections of 0-5%, 5-10%, 10-20%, 20-40% and 40-60%.
description: CERN-LHC. The azimuthal variation of jet yields in heavy-ion collisions provides information about the path-length dependence of the energy loss experienced by partons passing through the hot, dense nuclear matter known as the quark-gluon plasma. This paper presents the azimuthal anisotropy coefficients, $v_2$, $v_3$, and $v_4$, for jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using the ATLAS detector at the LHC. The measurement uses data collected in 2015 and 2018, corresponding to an integrated luminosity of 2.2 nb$^{-1}$. The $v_n$ values are measured as a function of the transverse momentum of the jets between 71 and 398 GeV and the event centrality. A non-zero value of $v_2$ is measured in all but the most central collisions. The value of $v_2$ is largest for jets with lower transverse momentum, with values up to 0.05 in mid-central collisions. A smaller, non-zero value of $v_3$ of approximately 0.01 is measured with no significant dependence on jet $p_\mathrm{T}$ or centrality, suggesting that fluctuations in the initial state play a small but distinct role in jet energy loss. No significant $v_4$ is observed in any kinematic region.
DOI: 10.17182/hepdata.132663.v1/t5
title: "Figure 3a" of "Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV with the ATLAS detector"

description: The systematic uncertainties in v2 for 20-40% centrality Pb+Pb collisions as a function of pT.
description: CERN-LHC. The azimuthal variation of jet yields in heavy-ion collisions provides information about the path-length dependence of the energy loss experienced by partons passing through the hot, dense nuclear matter known as the quark-gluon plasma. This paper presents the azimuthal anisotropy coefficients, $v_2$, $v_3$, and $v_4$, for jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using the ATLAS detector at the LHC. The measurement uses data collected in 2015 and 2018, corresponding to an integrated luminosity of 2.2 nb$^{-1}$. The $v_n$ values are measured as a function of the transverse momentum of the jets between 71 and 398 GeV and the event centrality. A non-zero value of $v_2$ is measured in all but the most central collisions. The value of $v_2$ is largest for jets with lower transverse momentum, with values up to 0.05 in mid-central collisions. A smaller, non-zero value of $v_3$ of approximately 0.01 is measured with no significant dependence on jet $p_\mathrm{T}$ or centrality, suggesting that fluctuations in the initial state play a small but distinct role in jet energy loss. No significant $v_4$ is observed in any kinematic region.
DOI: 10.17182/hepdata.132663.v1/t6
title: "Figure 3b" of "Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV with the ATLAS detector"

description: The systematic uncertainties in v2 for 5-10% centrality Pb+Pb collisions as a function of pT.
description: CERN-LHC. The azimuthal variation of jet yields in heavy-ion collisions provides information about the path-length dependence of the energy loss experienced by partons passing through the hot, dense nuclear matter known as the quark-gluon plasma. This paper presents the azimuthal anisotropy coefficients, $v_2$, $v_3$, and $v_4$, for jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using the ATLAS detector at the LHC. The measurement uses data collected in 2015 and 2018, corresponding to an integrated luminosity of 2.2 nb$^{-1}$. The $v_n$ values are measured as a function of the transverse momentum of the jets between 71 and 398 GeV and the event centrality. A non-zero value of $v_2$ is measured in all but the most central collisions. The value of $v_2$ is largest for jets with lower transverse momentum, with values up to 0.05 in mid-central collisions. A smaller, non-zero value of $v_3$ of approximately 0.01 is measured with no significant dependence on jet $p_\mathrm{T}$ or centrality, suggesting that fluctuations in the initial state play a small but distinct role in jet energy loss. No significant $v_4$ is observed in any kinematic region.
DOI: 10.17182/hepdata.132663.v1/t10
title: "Figure 3f" of "Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV with the ATLAS detector"

description: The systematic uncertainties in v4 for 5-10% centrality Pb+Pb collisions as a function of pT.
description: CERN-LHC. The azimuthal variation of jet yields in heavy-ion collisions provides information about the path-length dependence of the energy loss experienced by partons passing through the hot, dense nuclear matter known as the quark-gluon plasma. This paper presents the azimuthal anisotropy coefficients, $v_2$, $v_3$, and $v_4$, for jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using the ATLAS detector at the LHC. The measurement uses data collected in 2015 and 2018, corresponding to an integrated luminosity of 2.2 nb$^{-1}$. The $v_n$ values are measured as a function of the transverse momentum of the jets between 71 and 398 GeV and the event centrality. A non-zero value of $v_2$ is measured in all but the most central collisions. The value of $v_2$ is largest for jets with lower transverse momentum, with values up to 0.05 in mid-central collisions. A smaller, non-zero value of $v_3$ of approximately 0.01 is measured with no significant dependence on jet $p_\mathrm{T}$ or centrality, suggesting that fluctuations in the initial state play a small but distinct role in jet energy loss. No significant $v_4$ is observed in any kinematic region.
DOI: 10.17182/hepdata.132663.v1/t11
title: "Figure 4a" of "Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV with the ATLAS detector"

description: The systematic uncertainties in v2 for pT = 71--398 GeV jets as a function of centrality.
description: CERN-LHC. The azimuthal variation of jet yields in heavy-ion collisions provides information about the path-length dependence of the energy loss experienced by partons passing through the hot, dense nuclear matter known as the quark-gluon plasma. This paper presents the azimuthal anisotropy coefficients, $v_2$, $v_3$, and $v_4$, for jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using the ATLAS detector at the LHC. The measurement uses data collected in 2015 and 2018, corresponding to an integrated luminosity of 2.2 nb$^{-1}$. The $v_n$ values are measured as a function of the transverse momentum of the jets between 71 and 398 GeV and the event centrality. A non-zero value of $v_2$ is measured in all but the most central collisions. The value of $v_2$ is largest for jets with lower transverse momentum, with values up to 0.05 in mid-central collisions. A smaller, non-zero value of $v_3$ of approximately 0.01 is measured with no significant dependence on jet $p_\mathrm{T}$ or centrality, suggesting that fluctuations in the initial state play a small but distinct role in jet energy loss. No significant $v_4$ is observed in any kinematic region.
DOI: 10.17182/hepdata.132663.v1/t12
title: "Figure 4b" of "Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV with the ATLAS detector"

description: The systematic uncertainties in v3 for pT = 71--398 GeV jets as a function of centrality.
description: CERN-LHC. The azimuthal variation of jet yields in heavy-ion collisions provides information about the path-length dependence of the energy loss experienced by partons passing through the hot, dense nuclear matter known as the quark-gluon plasma. This paper presents the azimuthal anisotropy coefficients, $v_2$, $v_3$, and $v_4$, for jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using the ATLAS detector at the LHC. The measurement uses data collected in 2015 and 2018, corresponding to an integrated luminosity of 2.2 nb$^{-1}$. The $v_n$ values are measured as a function of the transverse momentum of the jets between 71 and 398 GeV and the event centrality. A non-zero value of $v_2$ is measured in all but the most central collisions. The value of $v_2$ is largest for jets with lower transverse momentum, with values up to 0.05 in mid-central collisions. A smaller, non-zero value of $v_3$ of approximately 0.01 is measured with no significant dependence on jet $p_\mathrm{T}$ or centrality, suggesting that fluctuations in the initial state play a small but distinct role in jet energy loss. No significant $v_4$ is observed in any kinematic region.
DOI: 10.17182/hepdata.132663.v1/t13
title: "Figure 4c" of "Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV with the ATLAS detector"

description: The systematic uncertainties in v4 for pT = 71--398 GeV jets as a function of centrality.
description: CERN-LHC. The azimuthal variation of jet yields in heavy-ion collisions provides information about the path-length dependence of the energy loss experienced by partons passing through the hot, dense nuclear matter known as the quark-gluon plasma. This paper presents the azimuthal anisotropy coefficients, $v_2$, $v_3$, and $v_4$, for jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using the ATLAS detector at the LHC. The measurement uses data collected in 2015 and 2018, corresponding to an integrated luminosity of 2.2 nb$^{-1}$. The $v_n$ values are measured as a function of the transverse momentum of the jets between 71 and 398 GeV and the event centrality. A non-zero value of $v_2$ is measured in all but the most central collisions. The value of $v_2$ is largest for jets with lower transverse momentum, with values up to 0.05 in mid-central collisions. A smaller, non-zero value of $v_3$ of approximately 0.01 is measured with no significant dependence on jet $p_\mathrm{T}$ or centrality, suggesting that fluctuations in the initial state play a small but distinct role in jet energy loss. No significant $v_4$ is observed in any kinematic region.
DOI: 10.17182/hepdata.132663.v1/t14
title: "Figure 5a" of "Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV with the ATLAS detector"

description: Angular distribution of jets as a function of the observed psi2 plane for jets with 71 &lt; pT &lt; 79 GeV in the 10-20% centrality bin.
description: CERN-LHC. The azimuthal variation of jet yields in heavy-ion collisions provides information about the path-length dependence of the energy loss experienced by partons passing through the hot, dense nuclear matter known as the quark-gluon plasma. This paper presents the azimuthal anisotropy coefficients, $v_2$, $v_3$, and $v_4$, for jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using the ATLAS detector at the LHC. The measurement uses data collected in 2015 and 2018, corresponding to an integrated luminosity of 2.2 nb$^{-1}$. The $v_n$ values are measured as a function of the transverse momentum of the jets between 71 and 398 GeV and the event centrality. A non-zero value of $v_2$ is measured in all but the most central collisions. The value of $v_2$ is largest for jets with lower transverse momentum, with values up to 0.05 in mid-central collisions. A smaller, non-zero value of $v_3$ of approximately 0.01 is measured with no significant dependence on jet $p_\mathrm{T}$ or centrality, suggesting that fluctuations in the initial state play a small but distinct role in jet energy loss. No significant $v_4$ is observed in any kinematic region.
DOI: 10.17182/hepdata.132663.v1/t15
title: "Figure 5b" of "Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV with the ATLAS detector"

description: Angular distribution of jets as a function of the observed psi3 plane for jets with 71 &lt; pT &lt; 79 GeV in the 10-20% centrality bin.
description: CERN-LHC. The azimuthal variation of jet yields in heavy-ion collisions provides information about the path-length dependence of the energy loss experienced by partons passing through the hot, dense nuclear matter known as the quark-gluon plasma. This paper presents the azimuthal anisotropy coefficients, $v_2$, $v_3$, and $v_4$, for jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV using the ATLAS detector at the LHC. The measurement uses data collected in 2015 and 2018, corresponding to an integrated luminosity of 2.2 nb$^{-1}$. The $v_n$ values are measured as a function of the transverse momentum of the jets between 71 and 398 GeV and the event centrality. A non-zero value of $v_2$ is measured in all but the most central collisions. The value of $v_2$ is largest for jets with lower transverse momentum, with values up to 0.05 in mid-central collisions. A smaller, non-zero value of $v_3$ of approximately 0.01 is measured with no significant dependence on jet $p_\mathrm{T}$ or centrality, suggesting that fluctuations in the initial state play a small but distinct role in jet energy loss. No significant $v_4$ is observed in any kinematic region.