cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.132663.v1/t24
title: "Figure 11a" 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 v2 as a function of pT for jets in 20-40% centrality collisions.
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/t26
title: "Figure 12a" 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 v2 for jets in 10-20% centrality collisions.
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/t27
title: "Figure 12b" 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 v3 for jets in 10-20% centrality collisions.
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/t28
title: "Figure 13a" of "Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV with the ATLAS detector"

description: R2max as a function of pT (filled circles). Also shown is 1 - 4v2/(1+2v2).
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/t29
title: "Figure 13b" of "Measurements of azimuthal anisotropies of jet production in Pb+Pb collisions at $\sqrt{s_{NN}} =$ 5.02 TeV with the ATLAS detector"

description: R3max as a function of pT (filled circles). Also shown is 1 - 4v3/(1+2v3).
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/t31
title: "Aux. 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 systematic uncertainties in v3 for 40-60% 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/t32
title: "Aux. Figure 1c" 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 40-60% 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/t30
title: "Aux. 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 systematic uncertainties in v2 for 40-60% 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/t33
title: "Aux. 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 systematic uncertainties in v2 for 10-20% 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/t34
title: "Aux. 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 systematic uncertainties in v3 for 10-20% 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/t35
title: "Aux. Figure 2c" 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 10-20% 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/t36
title: "Aux. 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 0-5% 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/t37
title: "Aux. 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 v3 for 0-5% 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/t38
title: "Aux. Figure 3c" 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 0-5% 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/t40
title: "Aux. Figure 5" 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 v2 as a function of pT for jets in 5-10% centrality collisions.
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/t41
title: "Aux. Figure 6" 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 v2 as a function of pT for jets in 0-5% centrality collisions.
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.