cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.84819.v1/t2
title: "Table 2" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t3
title: "Table 3" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t4
title: "Table 4" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t10
title: "Table 10" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t11
title: "Table 11" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t5
title: "Table 5" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t6
title: "Table 6" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t7
title: "Table 7" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t8
title: "Table 8" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t9
title: "Table 9" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t12
title: "Table 12" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t13
title: "Table 13" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t14
title: "Table 14" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t15
title: "Table 15" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t16
title: "Table 16" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t17
title: "Table 17" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t18
title: "Table 18" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t19
title: "Table 19" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t20
title: "Table 20" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t21
title: "Table 21" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.
DOI: 10.17182/hepdata.84819.v1/t22
title: "Table 22" of "Measurement of the nuclear modification factor for inclusive jets in Pb+Pb collisions at $\sqrt{s_\mathrm{NN}}=5.02$ TeV with the ATLAS detector"

description: No description provided.
description: CERN-LHC. Measurements of the yield and nuclear modification factor, $R_{\mathrm {AA}}$, for inclusive jets are performed using $0.49$ nb$^{-1}$ of Pb+Pb data at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV and 25 pb$^{-1}$ of pp data at $\sqrt{s}=5.02$ TeV. Jets are reconstructed with the anti-$k_{t}$ algorithm with radius parameter $R=0.4$ and are measured over the transverse momentum range of 50--1000 GeV in six rapidity intervals covering $|y|&lt;2.8$. The magnitude of $R_{\mathrm {AA}}$ increases with increasing $p_{\mathrm {T}}$ reaching a value of $\approx 0.6$ near the $p_{\mathrm {T}}$ of 1 TeV in the most central collisions. The magnitude of the $R_{\mathrm {AA}}$ decreases towards increasingly peripheral collisions. The $R_{\mathrm {AA}}$ is independent of rapidity at low jet-$p_{\mathrm {T}}$ but it is observed to decrease with increasing rapidity at high $p_{\mathrm {T}}$.