cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.89395.v1/t14
title: "Table 14" of "Linear and non-linear flow modes in Pb-Pb collisions at $\sqrt{s_{\rm NN}} =$ 2.76 TeV"

description: Centrality dependence of rho_mn in Pb–Pb collisions at 2.76 TeV.
description: The second and the third order anisotropic flow, V2 and V3, are mostly determined by the corresponding initial spatial anisotropy coefficients, epsilon2 and epsilon3, in the initial density distribution. In addition to their dependence on the same order initial anisotropy coefficient, higher order anisotropic flow, Vn (n &gt; 3), can also have a significant contribution from lower order initial anisotropy coefficients, which leads to mode-coupling effects. In this Letter we investigate the linear and non-linear modes in higher order anisotropic flow Vn for n = 4, 5, 6 with the ALICE detector at the Large Hadron Collider. The measurements are done for particles in the pseudorapidity range eta &lt; 0.8 and the transverse momentum range 0.2 &lt; pT &lt; 5.0 GeV/c as a function of collision centrality. The results are compared with theoretical calculations and provide important constraints on the nature of the initial geometry fluctuations as well as the ratio of the shear viscosity to entropy density of the produced system.
DOI: 10.17182/hepdata.89395.v1/t7
title: "Table 7" of "Linear and non-linear flow modes in Pb-Pb collisions at $\sqrt{s_{\rm NN}} =$ 2.76 TeV"

description: Centrality dependence of v4 (left), v5 (middle) and v6 (right) in Pb–Pb collisions at 2.76 TeV. Contributions from linear and non-linear modes are presented with open and solid markers, respectively.
description: The second and the third order anisotropic flow, V2 and V3, are mostly determined by the corresponding initial spatial anisotropy coefficients, epsilon2 and epsilon3, in the initial density distribution. In addition to their dependence on the same order initial anisotropy coefficient, higher order anisotropic flow, Vn (n &gt; 3), can also have a significant contribution from lower order initial anisotropy coefficients, which leads to mode-coupling effects. In this Letter we investigate the linear and non-linear modes in higher order anisotropic flow Vn for n = 4, 5, 6 with the ALICE detector at the Large Hadron Collider. The measurements are done for particles in the pseudorapidity range eta &lt; 0.8 and the transverse momentum range 0.2 &lt; pT &lt; 5.0 GeV/c as a function of collision centrality. The results are compared with theoretical calculations and provide important constraints on the nature of the initial geometry fluctuations as well as the ratio of the shear viscosity to entropy density of the produced system.
DOI: 10.17182/hepdata.89395.v1/t8
title: "Table 8" of "Linear and non-linear flow modes in Pb-Pb collisions at $\sqrt{s_{\rm NN}} =$ 2.76 TeV"

description: Centrality dependence of v4 (left), v5 (middle) and v6 (right) in Pb–Pb collisions at 2.76 TeV. Contributions from linear and non-linear modes are presented with open and solid markers, respectively.
description: The second and the third order anisotropic flow, V2 and V3, are mostly determined by the corresponding initial spatial anisotropy coefficients, epsilon2 and epsilon3, in the initial density distribution. In addition to their dependence on the same order initial anisotropy coefficient, higher order anisotropic flow, Vn (n &gt; 3), can also have a significant contribution from lower order initial anisotropy coefficients, which leads to mode-coupling effects. In this Letter we investigate the linear and non-linear modes in higher order anisotropic flow Vn for n = 4, 5, 6 with the ALICE detector at the Large Hadron Collider. The measurements are done for particles in the pseudorapidity range eta &lt; 0.8 and the transverse momentum range 0.2 &lt; pT &lt; 5.0 GeV/c as a function of collision centrality. The results are compared with theoretical calculations and provide important constraints on the nature of the initial geometry fluctuations as well as the ratio of the shear viscosity to entropy density of the produced system.
DOI: 10.17182/hepdata.89395.v1/t15
title: "Table 15" of "Linear and non-linear flow modes in Pb-Pb collisions at $\sqrt{s_{\rm NN}} =$ 2.76 TeV"

description: Centrality dependence of rho_mn in Pb–Pb collisions at 2.76 TeV.
description: The second and the third order anisotropic flow, V2 and V3, are mostly determined by the corresponding initial spatial anisotropy coefficients, epsilon2 and epsilon3, in the initial density distribution. In addition to their dependence on the same order initial anisotropy coefficient, higher order anisotropic flow, Vn (n &gt; 3), can also have a significant contribution from lower order initial anisotropy coefficients, which leads to mode-coupling effects. In this Letter we investigate the linear and non-linear modes in higher order anisotropic flow Vn for n = 4, 5, 6 with the ALICE detector at the Large Hadron Collider. The measurements are done for particles in the pseudorapidity range eta &lt; 0.8 and the transverse momentum range 0.2 &lt; pT &lt; 5.0 GeV/c as a function of collision centrality. The results are compared with theoretical calculations and provide important constraints on the nature of the initial geometry fluctuations as well as the ratio of the shear viscosity to entropy density of the produced system.
DOI: 10.17182/hepdata.89395.v1/t16
title: "Table 16" of "Linear and non-linear flow modes in Pb-Pb collisions at $\sqrt{s_{\rm NN}} =$ 2.76 TeV"

description: Centrality dependence of rho_mn in Pb–Pb collisions at 2.76 TeV.
description: The second and the third order anisotropic flow, V2 and V3, are mostly determined by the corresponding initial spatial anisotropy coefficients, epsilon2 and epsilon3, in the initial density distribution. In addition to their dependence on the same order initial anisotropy coefficient, higher order anisotropic flow, Vn (n &gt; 3), can also have a significant contribution from lower order initial anisotropy coefficients, which leads to mode-coupling effects. In this Letter we investigate the linear and non-linear modes in higher order anisotropic flow Vn for n = 4, 5, 6 with the ALICE detector at the Large Hadron Collider. The measurements are done for particles in the pseudorapidity range eta &lt; 0.8 and the transverse momentum range 0.2 &lt; pT &lt; 5.0 GeV/c as a function of collision centrality. The results are compared with theoretical calculations and provide important constraints on the nature of the initial geometry fluctuations as well as the ratio of the shear viscosity to entropy density of the produced system.
DOI: 10.17182/hepdata.89395.v1/t17
title: "Table 17" of "Linear and non-linear flow modes in Pb-Pb collisions at $\sqrt{s_{\rm NN}} =$ 2.76 TeV"

description: Centrality dependence of rho_mn in Pb–Pb collisions at 2.76 TeV.
description: The second and the third order anisotropic flow, V2 and V3, are mostly determined by the corresponding initial spatial anisotropy coefficients, epsilon2 and epsilon3, in the initial density distribution. In addition to their dependence on the same order initial anisotropy coefficient, higher order anisotropic flow, Vn (n &gt; 3), can also have a significant contribution from lower order initial anisotropy coefficients, which leads to mode-coupling effects. In this Letter we investigate the linear and non-linear modes in higher order anisotropic flow Vn for n = 4, 5, 6 with the ALICE detector at the Large Hadron Collider. The measurements are done for particles in the pseudorapidity range eta &lt; 0.8 and the transverse momentum range 0.2 &lt; pT &lt; 5.0 GeV/c as a function of collision centrality. The results are compared with theoretical calculations and provide important constraints on the nature of the initial geometry fluctuations as well as the ratio of the shear viscosity to entropy density of the produced system.
DOI: 10.17182/hepdata.89395.v1/t18
title: "Table 18" of "Linear and non-linear flow modes in Pb-Pb collisions at $\sqrt{s_{\rm NN}} =$ 2.76 TeV"

description: Centrality dependence of chi in Pb–Pb collisions at 2.76 TeV.
description: The second and the third order anisotropic flow, V2 and V3, are mostly determined by the corresponding initial spatial anisotropy coefficients, epsilon2 and epsilon3, in the initial density distribution. In addition to their dependence on the same order initial anisotropy coefficient, higher order anisotropic flow, Vn (n &gt; 3), can also have a significant contribution from lower order initial anisotropy coefficients, which leads to mode-coupling effects. In this Letter we investigate the linear and non-linear modes in higher order anisotropic flow Vn for n = 4, 5, 6 with the ALICE detector at the Large Hadron Collider. The measurements are done for particles in the pseudorapidity range eta &lt; 0.8 and the transverse momentum range 0.2 &lt; pT &lt; 5.0 GeV/c as a function of collision centrality. The results are compared with theoretical calculations and provide important constraints on the nature of the initial geometry fluctuations as well as the ratio of the shear viscosity to entropy density of the produced system.
DOI: 10.17182/hepdata.89395.v1/t19
title: "Table 19" of "Linear and non-linear flow modes in Pb-Pb collisions at $\sqrt{s_{\rm NN}} =$ 2.76 TeV"

description: Centrality dependence of chi in Pb–Pb collisions at 2.76 TeV.
description: The second and the third order anisotropic flow, V2 and V3, are mostly determined by the corresponding initial spatial anisotropy coefficients, epsilon2 and epsilon3, in the initial density distribution. In addition to their dependence on the same order initial anisotropy coefficient, higher order anisotropic flow, Vn (n &gt; 3), can also have a significant contribution from lower order initial anisotropy coefficients, which leads to mode-coupling effects. In this Letter we investigate the linear and non-linear modes in higher order anisotropic flow Vn for n = 4, 5, 6 with the ALICE detector at the Large Hadron Collider. The measurements are done for particles in the pseudorapidity range eta &lt; 0.8 and the transverse momentum range 0.2 &lt; pT &lt; 5.0 GeV/c as a function of collision centrality. The results are compared with theoretical calculations and provide important constraints on the nature of the initial geometry fluctuations as well as the ratio of the shear viscosity to entropy density of the produced system.
DOI: 10.17182/hepdata.89395.v1/t20
title: "Table 20" of "Linear and non-linear flow modes in Pb-Pb collisions at $\sqrt{s_{\rm NN}} =$ 2.76 TeV"

description: Centrality dependence of chi in Pb–Pb collisions at 2.76 TeV.
description: The second and the third order anisotropic flow, V2 and V3, are mostly determined by the corresponding initial spatial anisotropy coefficients, epsilon2 and epsilon3, in the initial density distribution. In addition to their dependence on the same order initial anisotropy coefficient, higher order anisotropic flow, Vn (n &gt; 3), can also have a significant contribution from lower order initial anisotropy coefficients, which leads to mode-coupling effects. In this Letter we investigate the linear and non-linear modes in higher order anisotropic flow Vn for n = 4, 5, 6 with the ALICE detector at the Large Hadron Collider. The measurements are done for particles in the pseudorapidity range eta &lt; 0.8 and the transverse momentum range 0.2 &lt; pT &lt; 5.0 GeV/c as a function of collision centrality. The results are compared with theoretical calculations and provide important constraints on the nature of the initial geometry fluctuations as well as the ratio of the shear viscosity to entropy density of the produced system.
DOI: 10.17182/hepdata.89395.v1/t21
title: "Table 21" of "Linear and non-linear flow modes in Pb-Pb collisions at $\sqrt{s_{\rm NN}} =$ 2.76 TeV"

description: Centrality dependence of chi in Pb–Pb collisions at 2.76 TeV.
description: The second and the third order anisotropic flow, V2 and V3, are mostly determined by the corresponding initial spatial anisotropy coefficients, epsilon2 and epsilon3, in the initial density distribution. In addition to their dependence on the same order initial anisotropy coefficient, higher order anisotropic flow, Vn (n &gt; 3), can also have a significant contribution from lower order initial anisotropy coefficients, which leads to mode-coupling effects. In this Letter we investigate the linear and non-linear modes in higher order anisotropic flow Vn for n = 4, 5, 6 with the ALICE detector at the Large Hadron Collider. The measurements are done for particles in the pseudorapidity range eta &lt; 0.8 and the transverse momentum range 0.2 &lt; pT &lt; 5.0 GeV/c as a function of collision centrality. The results are compared with theoretical calculations and provide important constraints on the nature of the initial geometry fluctuations as well as the ratio of the shear viscosity to entropy density of the produced system.
DOI: 10.17182/hepdata.89396.v1/t1
title: "Table 1" of "Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV"

description: Nuclear modification factor RAA versus pT for charged particles at midrapidity in 0-5% central Pb-Pb collisions at 5.02 TeV
description: Charged-particle spectra at midrapidity are measured in Pb--Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\snn = 5.02$ TeV and presented in centrality classes ranging from most central~(0--5\%) to most peripheral~(95--100\%) collisions. Possible medium effects are quantified using the nuclear modification factor~($\RAA$) by comparing the measured spectra with those from proton--proton collisions, scaled by the number of independent nucleon--nucleon collisions obtained from a Glauber model.
DOI: 10.17182/hepdata.89396.v1/t2
title: "Table 2" of "Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV"

description: Nuclear modification factor RAA versus pT for charged particles at midrapidity in 5-10% central Pb-Pb collisions at 5.02 TeV
description: Charged-particle spectra at midrapidity are measured in Pb--Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\snn = 5.02$ TeV and presented in centrality classes ranging from most central~(0--5\%) to most peripheral~(95--100\%) collisions. Possible medium effects are quantified using the nuclear modification factor~($\RAA$) by comparing the measured spectra with those from proton--proton collisions, scaled by the number of independent nucleon--nucleon collisions obtained from a Glauber model.
DOI: 10.17182/hepdata.89396.v1/t3
title: "Table 3" of "Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV"

description: Nuclear modification factor RAA versus pT for charged particles at midrapidity in 10-15% central Pb-Pb collisions at 5.02 TeV
description: Charged-particle spectra at midrapidity are measured in Pb--Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\snn = 5.02$ TeV and presented in centrality classes ranging from most central~(0--5\%) to most peripheral~(95--100\%) collisions. Possible medium effects are quantified using the nuclear modification factor~($\RAA$) by comparing the measured spectra with those from proton--proton collisions, scaled by the number of independent nucleon--nucleon collisions obtained from a Glauber model.
DOI: 10.17182/hepdata.89396.v1/t4
title: "Table 4" of "Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV"

description: Nuclear modification factor RAA versus pT for charged particles at midrapidity in 15-20% central Pb-Pb collisions at 5.02 TeV
description: Charged-particle spectra at midrapidity are measured in Pb--Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\snn = 5.02$ TeV and presented in centrality classes ranging from most central~(0--5\%) to most peripheral~(95--100\%) collisions. Possible medium effects are quantified using the nuclear modification factor~($\RAA$) by comparing the measured spectra with those from proton--proton collisions, scaled by the number of independent nucleon--nucleon collisions obtained from a Glauber model.
DOI: 10.17182/hepdata.89396.v1/t5
title: "Table 5" of "Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV"

description: Nuclear modification factor RAA versus pT for charged particles at midrapidity in 20-25% central Pb-Pb collisions at 5.02 TeV
description: Charged-particle spectra at midrapidity are measured in Pb--Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\snn = 5.02$ TeV and presented in centrality classes ranging from most central~(0--5\%) to most peripheral~(95--100\%) collisions. Possible medium effects are quantified using the nuclear modification factor~($\RAA$) by comparing the measured spectra with those from proton--proton collisions, scaled by the number of independent nucleon--nucleon collisions obtained from a Glauber model.
DOI: 10.17182/hepdata.89396.v1/t6
title: "Table 6" of "Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV"

description: Nuclear modification factor RAA versus pT for charged particles at midrapidity in 25-30% central Pb-Pb collisions at 5.02 TeV
description: Charged-particle spectra at midrapidity are measured in Pb--Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\snn = 5.02$ TeV and presented in centrality classes ranging from most central~(0--5\%) to most peripheral~(95--100\%) collisions. Possible medium effects are quantified using the nuclear modification factor~($\RAA$) by comparing the measured spectra with those from proton--proton collisions, scaled by the number of independent nucleon--nucleon collisions obtained from a Glauber model.
DOI: 10.17182/hepdata.89396.v1/t7
title: "Table 7" of "Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV"

description: Nuclear modification factor RAA versus pT for charged particles at midrapidity in 30-35% central Pb-Pb collisions at 5.02 TeV
description: Charged-particle spectra at midrapidity are measured in Pb--Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\snn = 5.02$ TeV and presented in centrality classes ranging from most central~(0--5\%) to most peripheral~(95--100\%) collisions. Possible medium effects are quantified using the nuclear modification factor~($\RAA$) by comparing the measured spectra with those from proton--proton collisions, scaled by the number of independent nucleon--nucleon collisions obtained from a Glauber model.
DOI: 10.17182/hepdata.89396.v1/t8
title: "Table 8" of "Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV"

description: Nuclear modification factor RAA versus pT for charged particles at midrapidity in 35-40% central Pb-Pb collisions at 5.02 TeV
description: Charged-particle spectra at midrapidity are measured in Pb--Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\snn = 5.02$ TeV and presented in centrality classes ranging from most central~(0--5\%) to most peripheral~(95--100\%) collisions. Possible medium effects are quantified using the nuclear modification factor~($\RAA$) by comparing the measured spectra with those from proton--proton collisions, scaled by the number of independent nucleon--nucleon collisions obtained from a Glauber model.
DOI: 10.17182/hepdata.89396.v1/t10
title: "Table 10" of "Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV"

description: Nuclear modification factor RAA versus pT for charged particles at midrapidity in 45-50% central Pb-Pb collisions at 5.02 TeV
description: Charged-particle spectra at midrapidity are measured in Pb--Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\snn = 5.02$ TeV and presented in centrality classes ranging from most central~(0--5\%) to most peripheral~(95--100\%) collisions. Possible medium effects are quantified using the nuclear modification factor~($\RAA$) by comparing the measured spectra with those from proton--proton collisions, scaled by the number of independent nucleon--nucleon collisions obtained from a Glauber model.
DOI: 10.17182/hepdata.89396.v1/t11
title: "Table 11" of "Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV"

description: Nuclear modification factor RAA versus pT for charged particles at midrapidity in 50-55% central Pb-Pb collisions at 5.02 TeV
description: Charged-particle spectra at midrapidity are measured in Pb--Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\snn = 5.02$ TeV and presented in centrality classes ranging from most central~(0--5\%) to most peripheral~(95--100\%) collisions. Possible medium effects are quantified using the nuclear modification factor~($\RAA$) by comparing the measured spectra with those from proton--proton collisions, scaled by the number of independent nucleon--nucleon collisions obtained from a Glauber model.
DOI: 10.17182/hepdata.89396.v1/t12
title: "Table 12" of "Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV"

description: Nuclear modification factor RAA versus pT for charged particles at midrapidity in 55-60% central Pb-Pb collisions at 5.02 TeV
description: Charged-particle spectra at midrapidity are measured in Pb--Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\snn = 5.02$ TeV and presented in centrality classes ranging from most central~(0--5\%) to most peripheral~(95--100\%) collisions. Possible medium effects are quantified using the nuclear modification factor~($\RAA$) by comparing the measured spectra with those from proton--proton collisions, scaled by the number of independent nucleon--nucleon collisions obtained from a Glauber model.
DOI: 10.17182/hepdata.89396.v1/t13
title: "Table 13" of "Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV"

description: Nuclear modification factor RAA versus pT for charged particles at midrapidity in 60-65% central Pb-Pb collisions at 5.02 TeV
description: Charged-particle spectra at midrapidity are measured in Pb--Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\snn = 5.02$ TeV and presented in centrality classes ranging from most central~(0--5\%) to most peripheral~(95--100\%) collisions. Possible medium effects are quantified using the nuclear modification factor~($\RAA$) by comparing the measured spectra with those from proton--proton collisions, scaled by the number of independent nucleon--nucleon collisions obtained from a Glauber model.
DOI: 10.17182/hepdata.89396.v1/t14
title: "Table 14" of "Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV"

description: Nuclear modification factor RAA versus pT for charged particles at midrapidity in 65-70% central Pb-Pb collisions at 5.02 TeV
description: Charged-particle spectra at midrapidity are measured in Pb--Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\snn = 5.02$ TeV and presented in centrality classes ranging from most central~(0--5\%) to most peripheral~(95--100\%) collisions. Possible medium effects are quantified using the nuclear modification factor~($\RAA$) by comparing the measured spectra with those from proton--proton collisions, scaled by the number of independent nucleon--nucleon collisions obtained from a Glauber model.
DOI: 10.17182/hepdata.89396.v1/t16
title: "Table 16" of "Analysis of the apparent nuclear modification in peripheral Pb-Pb collisions at 5.02 TeV"

description: Nuclear modification factor RAA versus pT for charged particles at midrapidity in 75-80% central Pb-Pb collisions at 5.02 TeV
description: Charged-particle spectra at midrapidity are measured in Pb--Pb collisions at the centre-of-mass energy per nucleon--nucleon pair $\snn = 5.02$ TeV and presented in centrality classes ranging from most central~(0--5\%) to most peripheral~(95--100\%) collisions. Possible medium effects are quantified using the nuclear modification factor~($\RAA$) by comparing the measured spectra with those from proton--proton collisions, scaled by the number of independent nucleon--nucleon collisions obtained from a Glauber model.