cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.132663.v1/t7
title: "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 v3 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/t8
title: "Figure 3d" 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 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/t9
title: "Figure 3e" 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 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.87256.v1/t1
title: "Table 1" of "Measurement of prompt photon production in $\sqrt{s_\mathrm{NN}} = 8.16$ TeV $p$+Pb collisions with ATLAS"

description: The measured cross sections for prompt, isolated photons with rapidity in (1.09,1.90).
description: The inclusive production rates of isolated, prompt photons in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV are studied with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb^−1 recorded in 2016. The cross-section and nuclear modification factor R_{pPb} are measured as a function of photon transverse energy from 20 GeV to 550 GeV and in three nucleon-nucleon centre-of-mass pseudorapidity regions, (−2.83,−2.02), (−1.84,0.91), and (1.09,1.90).
DOI: 10.17182/hepdata.132663.v1/t16
title: "Figure 5c" 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 psi4 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/t17
title: "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 values for R = 0.2 jets as a function of centrality for jets in several pT ranges.
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/t18
title: "Figure 7" 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 values for R = 0.2 jets as a function of pT for 0-5%, 5-10%, and 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/t19
title: "Figure 8" 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, v3, and v4 as a function of centrality for jets with pT = 71-398 GeV.
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.87256.v1/t2
title: "Table 2" of "Measurement of prompt photon production in $\sqrt{s_\mathrm{NN}} = 8.16$ TeV $p$+Pb collisions with ATLAS"

description: The measured cross sections for prompt, isolated photons with rapidity in (−1.84,0.91).
description: The inclusive production rates of isolated, prompt photons in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV are studied with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb^−1 recorded in 2016. The cross-section and nuclear modification factor R_{pPb} are measured as a function of photon transverse energy from 20 GeV to 550 GeV and in three nucleon-nucleon centre-of-mass pseudorapidity regions, (−2.83,−2.02), (−1.84,0.91), and (1.09,1.90).
DOI: 10.17182/hepdata.87256.v1/t3
title: "Table 3" of "Measurement of prompt photon production in $\sqrt{s_\mathrm{NN}} = 8.16$ TeV $p$+Pb collisions with ATLAS"

description: The measured cross sections for prompt, isolated photons with rapidity in (−2.83,−2.02).
description: The inclusive production rates of isolated, prompt photons in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV are studied with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb^−1 recorded in 2016. The cross-section and nuclear modification factor R_{pPb} are measured as a function of photon transverse energy from 20 GeV to 550 GeV and in three nucleon-nucleon centre-of-mass pseudorapidity regions, (−2.83,−2.02), (−1.84,0.91), and (1.09,1.90).
DOI: 10.17182/hepdata.87256.v1/t4
title: "Table 4" of "Measurement of prompt photon production in $\sqrt{s_\mathrm{NN}} = 8.16$ TeV $p$+Pb collisions with ATLAS"

description: The nuclear modification factor R_pPb for prompt, isolated photons with rapidity in (1.09,1.90).
description: The inclusive production rates of isolated, prompt photons in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV are studied with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb^−1 recorded in 2016. The cross-section and nuclear modification factor R_{pPb} are measured as a function of photon transverse energy from 20 GeV to 550 GeV and in three nucleon-nucleon centre-of-mass pseudorapidity regions, (−2.83,−2.02), (−1.84,0.91), and (1.09,1.90).
DOI: 10.17182/hepdata.132663.v1/t20
title: "Figure 9a" 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 values for R = 0.2 jets as a function of centrality for jets in several pT ranges.
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/t21
title: "Figure 9b" 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 v4 values for R = 0.2 jets as a function of centrality for jets in several pT ranges.
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/t22
title: "Figure 10a" 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 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/t23
title: "Figure 10b" 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 as a function of pT 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/t25
title: "Figure 11b" 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 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.87256.v1/t5
title: "Table 5" of "Measurement of prompt photon production in $\sqrt{s_\mathrm{NN}} = 8.16$ TeV $p$+Pb collisions with ATLAS"

description: The nuclear modification factor R_pPb for prompt, isolated photons with rapidity in (−1.84,0.91).
description: The inclusive production rates of isolated, prompt photons in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV are studied with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb^−1 recorded in 2016. The cross-section and nuclear modification factor R_{pPb} are measured as a function of photon transverse energy from 20 GeV to 550 GeV and in three nucleon-nucleon centre-of-mass pseudorapidity regions, (−2.83,−2.02), (−1.84,0.91), and (1.09,1.90).
DOI: 10.17182/hepdata.87256.v1/t6
title: "Table 6" of "Measurement of prompt photon production in $\sqrt{s_\mathrm{NN}} = 8.16$ TeV $p$+Pb collisions with ATLAS"

description: The nuclear modification factor R_pPb for prompt, isolated photons with rapidity in (−2.83,−2.02).
description: The inclusive production rates of isolated, prompt photons in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV are studied with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb^−1 recorded in 2016. The cross-section and nuclear modification factor R_{pPb} are measured as a function of photon transverse energy from 20 GeV to 550 GeV and in three nucleon-nucleon centre-of-mass pseudorapidity regions, (−2.83,−2.02), (−1.84,0.91), and (1.09,1.90).
DOI: 10.17182/hepdata.87256.v1/t7
title: "Table 7" of "Measurement of prompt photon production in $\sqrt{s_\mathrm{NN}} = 8.16$ TeV $p$+Pb collisions with ATLAS"

description: The ratio of R_{pPb} from rapidity (1.09,1.90) to that of rapidity (−2.83,−2.02).
description: The inclusive production rates of isolated, prompt photons in $p$+Pb collisions at $\sqrt{s_{NN}}=8.16$ TeV are studied with the ATLAS detector at the Large Hadron Collider using a dataset with an integrated luminosity of 165 nb^−1 recorded in 2016. The cross-section and nuclear modification factor R_{pPb} are measured as a function of photon transverse energy from 20 GeV to 550 GeV and in three nucleon-nucleon centre-of-mass pseudorapidity regions, (−2.83,−2.02), (−1.84,0.91), and (1.09,1.90).