cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.84819.v1/t23
title: "Table 23" 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/t24
title: "Table 24" 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/t25
title: "Table 25" 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/t26
title: "Table 26" 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/t27
title: "Table 27" 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/t28
title: "Table 28" 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/t29
title: "Table 29" 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/t30
title: "Table 30" 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/t31
title: "Table 31" 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/t32
title: "Table 32" 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/t33
title: "Table 33" 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/t34
title: "Table 34" 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.103082.v1/t1
title: "Table 1" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: Per-event-yield of prompt jpsi production in 5.02 TeV PbPb collision data as a function of pT for three different centrality slices in the rapidity range |y| &lt; 2.
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t2
title: "Table 2" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: Per-event-yield of non-prompt jpsi production in 5.02 TeV PbPb collision data as a function of pT for three different centrality slices in the rapidity range |y| &lt; 2.
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t3
title: "Table 3" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: Non-prompt fraction of jpsi production in 5.02 TeV PbPb collision data as a function of pT for three different centrality slices in the rapidity range |y| &lt; 2.
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t4
title: "Table 4" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: Non-prompt fraction of jpsi production in 5.02 TeV PbPb collision data as a function of pT for integrated centrality in the rapidity range |y| &lt; 2.
description: No data abstract available.
DOI: 10.17182/hepdata.84819.v1/t35
title: "Table 35" 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.103082.v1/t5
title: "Table 5" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: The nuclear modification factor as a function of pT for the prompt jpsi for |y|&lt;2, in 0--80% centrality bin.
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t6
title: "Table 6" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: The nuclear modification factor as a function of pT for the prompt jpsi for |y|&lt;2, in 0--10%, 20--40%, and 40--80% centrality bin.
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t7
title: "Table 7" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: The nuclear modification factor as a function of pT for the non-prompt jpsi for |y|&lt;2, in 0--80% centrality bin.
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t8
title: "Table 8" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: The nuclear modification factor as a function of pT for the non-prompt jpsi for |y|&lt;2, in 0--10%, 20--40%, and 40--80% centrality bin.
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t10
title: "Table 10" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: The nuclear modification factor as a function of eta for the prompt jpsi for 9 &lt; pT &lt; 40 GeV, in 0--80% centrality bin.
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t12
title: "Table 12" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: The nuclear modification factor as a function of eta for the non-prompt jpsi for 9 &lt; pT &lt; 40 GeV, in 0--80% centrality bin.
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t9
title: "Table 9" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: The nuclear modification factor as a function of pT for the prompt and non-prompt jpsi for |y|&lt;2, in 0--20% centrality bin.
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t11
title: "Table 11" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: The nuclear modification factor as a function of eta for the prompt jpsi for 9 &lt; pT &lt; 40 GeV, in 0--10%, 20--40%, and 40--80% centrality bin.
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t13
title: "Table 13" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: The nuclear modification factor as a function of eta for the non-prompt jpsi for 9 &lt; pT &lt; 40 GeV, in 0--10%, 20--40%, and 40--80% centrality bin.
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t14
title: "Table 14" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: The nuclear modification factor as a function of Npart for the prompt jpsi for |y|&lt;2, and 9 &lt; pT &lt; 40 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t15
title: "Table 15" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: The nuclear modification factor as a function of Npart for the non-prompt jpsi for |y|&lt;2, and 9 &lt; pT &lt; 40 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t16
title: "Table 16" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: The double ratio of nuclear modification factor as a function of Npart for the prompt jpsi and psi(2S) for |y|&lt;2, and 9 &lt; pT &lt; 40 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.103082.v1/t17
title: "Table 17" of "Prompt and non-prompt $J/\psi$ and $\psi(2\mathrm{S})$ suppression at high transverse momentum in 5.02 TeV Pb+Pb collisions with the ATLAS experiment"

description: The double ratio nuclear modification factor as a function of Npart for the non-prompt jpsi and psi(2S) for |y|&lt;2, and 9 &lt; pT &lt; 40 GeV
description: No data abstract available.
DOI: 10.17182/hepdata.77761.v1/t2
title: "Table 2" of "Evidence for light-by-light scattering in heavy-ion collisions with the ATLAS detector at the LHC"

description: Detector-level diphoton invariant mass distribution
description: CERN-LHC. Measurement of the total fiducial cross section for light-by-light scattering in lead-lead collisions at a centre-of-mass energy of 5.02 TeV with 0.48 nb^-1 of data collected in 2015. The final states used are 2 photons and no further activity in the detector.

The fiducial region is defined as:
- 2Gamma
- pt_Gamma &gt; 3 GeV
- |eta_Gamma| &lt; 2.4
- m_GammaGamma must be above 6 GeV
- pt_GammaGamma must be below 2 GeV
- aco_GammaGamma must be below 0.01
DOI: 10.17182/hepdata.77761.v1/t3
title: "Table 3" of "Evidence for light-by-light scattering in heavy-ion collisions with the ATLAS detector at the LHC"

description: The measured total fiducial cross section
description: CERN-LHC. Measurement of the total fiducial cross section for light-by-light scattering in lead-lead collisions at a centre-of-mass energy of 5.02 TeV with 0.48 nb^-1 of data collected in 2015. The final states used are 2 photons and no further activity in the detector.

The fiducial region is defined as:
- 2Gamma
- pt_Gamma &gt; 3 GeV
- |eta_Gamma| &lt; 2.4
- m_GammaGamma must be above 6 GeV
- pt_GammaGamma must be below 2 GeV
- aco_GammaGamma must be below 0.01
DOI: 10.17909/c2qe-2177
title: TESS Light Curves for TIC 399725538

description: All light curve files for TESS observations from Sectors 5, 32, and 71.