cometadata/datacite-titles-descriptions-related-identifiers huggingface dataset:
DOI: 10.17182/hepdata.146722.v1/t11
title: "Table 11" of "Pseudorapidity dependence of anisotropic flow and its decorrelations using long-range multiparticle correlations in Pb-Pb and Xe-Xe collisions"

description: $r_{3,3}$ versus $\eta$ for $x^{\pm}$ in $\mathrm{Pb}-\mathrm{Pb}$ at $\sqrt{s_{\mathrm{NN}}}=5.023\,\mathrm{Te\!V}$
description: The pseudorapidity dependence of elliptic ($v_{2}$), triangular ($v_{3}$), and quadrangular ($v_{4}$) flow coefficients of charged particles measured in Pb-Pb collisions at a centre-of-mass energy per nucleon pair of $\sqrt{s_{\mathrm{NN}}}=5.02\,\mathrm{TeV}$ and in Xe-Xe collisions at $\sqrt{s_{\mathrm{NN}}}=5.44\,\mathrm{TeV}$ with ALICE at the LHC are presented. The measurements are performed in the pseudorapidity range $-3.5 &lt; \eta &lt; 5$ for various centrality intervals using two- and multi-particle cumulants with the subevent method. The flow probability density function (p.d.f.) is studied with the ratio of flow coefficient $v_2$ calculated with four- and two-particle cumulant, and suggests that the variance of flow p.d.f. is independent of pseudorapidity. The decorrelation of the flow vector in the longitudinal direction is probed using two-particle correlations. The results measured with respect to different reference regions in pseudorapidity exhibit differences, argued to be a result of saturating decorrelation effect above a certain pseudorapidity separation, in contrast to previous publications which assign this observation to non-flow effects. The results are compared to $3+1$ dimensional hydrodynamic and the AMPT transport model calculations. Neither of the models is able to simultaneously describe the pseudorapidity dependence of measurements of anisotropic flow and its fluctuations. The results presented in this work highlight shortcomings in our current understanding of initial conditions and subsequent system expansion in the longitudinal direction. Therefore, they provide input for its improvement.
DOI: 10.17182/hepdata.146722.v1/t12
title: "Table 12" of "Pseudorapidity dependence of anisotropic flow and its decorrelations using long-range multiparticle correlations in Pb-Pb and Xe-Xe collisions"

description: $v_{2}\{2\}$ versus $\eta$ for $x^{\pm}$ in $\mathrm{Xe}-\mathrm{Xe}$ at $\sqrt{s_{\mathrm{NN}}}=5.44\,\mathrm{Te\!V}$
description: The pseudorapidity dependence of elliptic ($v_{2}$), triangular ($v_{3}$), and quadrangular ($v_{4}$) flow coefficients of charged particles measured in Pb-Pb collisions at a centre-of-mass energy per nucleon pair of $\sqrt{s_{\mathrm{NN}}}=5.02\,\mathrm{TeV}$ and in Xe-Xe collisions at $\sqrt{s_{\mathrm{NN}}}=5.44\,\mathrm{TeV}$ with ALICE at the LHC are presented. The measurements are performed in the pseudorapidity range $-3.5 &lt; \eta &lt; 5$ for various centrality intervals using two- and multi-particle cumulants with the subevent method. The flow probability density function (p.d.f.) is studied with the ratio of flow coefficient $v_2$ calculated with four- and two-particle cumulant, and suggests that the variance of flow p.d.f. is independent of pseudorapidity. The decorrelation of the flow vector in the longitudinal direction is probed using two-particle correlations. The results measured with respect to different reference regions in pseudorapidity exhibit differences, argued to be a result of saturating decorrelation effect above a certain pseudorapidity separation, in contrast to previous publications which assign this observation to non-flow effects. The results are compared to $3+1$ dimensional hydrodynamic and the AMPT transport model calculations. Neither of the models is able to simultaneously describe the pseudorapidity dependence of measurements of anisotropic flow and its fluctuations. The results presented in this work highlight shortcomings in our current understanding of initial conditions and subsequent system expansion in the longitudinal direction. Therefore, they provide input for its improvement.
DOI: 10.17182/hepdata.146722.v1/t13
title: "Table 13" of "Pseudorapidity dependence of anisotropic flow and its decorrelations using long-range multiparticle correlations in Pb-Pb and Xe-Xe collisions"

description: $v_{3}\{2\}$ versus $\eta$ for $x^{\pm}$ in $\mathrm{Xe}-\mathrm{Xe}$ at $\sqrt{s_{\mathrm{NN}}}=5.44\,\mathrm{Te\!V}$
description: The pseudorapidity dependence of elliptic ($v_{2}$), triangular ($v_{3}$), and quadrangular ($v_{4}$) flow coefficients of charged particles measured in Pb-Pb collisions at a centre-of-mass energy per nucleon pair of $\sqrt{s_{\mathrm{NN}}}=5.02\,\mathrm{TeV}$ and in Xe-Xe collisions at $\sqrt{s_{\mathrm{NN}}}=5.44\,\mathrm{TeV}$ with ALICE at the LHC are presented. The measurements are performed in the pseudorapidity range $-3.5 &lt; \eta &lt; 5$ for various centrality intervals using two- and multi-particle cumulants with the subevent method. The flow probability density function (p.d.f.) is studied with the ratio of flow coefficient $v_2$ calculated with four- and two-particle cumulant, and suggests that the variance of flow p.d.f. is independent of pseudorapidity. The decorrelation of the flow vector in the longitudinal direction is probed using two-particle correlations. The results measured with respect to different reference regions in pseudorapidity exhibit differences, argued to be a result of saturating decorrelation effect above a certain pseudorapidity separation, in contrast to previous publications which assign this observation to non-flow effects. The results are compared to $3+1$ dimensional hydrodynamic and the AMPT transport model calculations. Neither of the models is able to simultaneously describe the pseudorapidity dependence of measurements of anisotropic flow and its fluctuations. The results presented in this work highlight shortcomings in our current understanding of initial conditions and subsequent system expansion in the longitudinal direction. Therefore, they provide input for its improvement.
DOI: 10.17182/hepdata.146722.v1/t14
title: "Table 14" of "Pseudorapidity dependence of anisotropic flow and its decorrelations using long-range multiparticle correlations in Pb-Pb and Xe-Xe collisions"

description: $v_{2}\{2\}$ versus $\eta$ for $x^{\pm}$ in $\mathrm{Xe}-\mathrm{Xe}$ at $\sqrt{s_{\mathrm{NN}}}=5.44\,\mathrm{Te\!V}$
description: The pseudorapidity dependence of elliptic ($v_{2}$), triangular ($v_{3}$), and quadrangular ($v_{4}$) flow coefficients of charged particles measured in Pb-Pb collisions at a centre-of-mass energy per nucleon pair of $\sqrt{s_{\mathrm{NN}}}=5.02\,\mathrm{TeV}$ and in Xe-Xe collisions at $\sqrt{s_{\mathrm{NN}}}=5.44\,\mathrm{TeV}$ with ALICE at the LHC are presented. The measurements are performed in the pseudorapidity range $-3.5 &lt; \eta &lt; 5$ for various centrality intervals using two- and multi-particle cumulants with the subevent method. The flow probability density function (p.d.f.) is studied with the ratio of flow coefficient $v_2$ calculated with four- and two-particle cumulant, and suggests that the variance of flow p.d.f. is independent of pseudorapidity. The decorrelation of the flow vector in the longitudinal direction is probed using two-particle correlations. The results measured with respect to different reference regions in pseudorapidity exhibit differences, argued to be a result of saturating decorrelation effect above a certain pseudorapidity separation, in contrast to previous publications which assign this observation to non-flow effects. The results are compared to $3+1$ dimensional hydrodynamic and the AMPT transport model calculations. Neither of the models is able to simultaneously describe the pseudorapidity dependence of measurements of anisotropic flow and its fluctuations. The results presented in this work highlight shortcomings in our current understanding of initial conditions and subsequent system expansion in the longitudinal direction. Therefore, they provide input for its improvement.
DOI: 10.17182/hepdata.146722.v1/t15
title: "Table 15" of "Pseudorapidity dependence of anisotropic flow and its decorrelations using long-range multiparticle correlations in Pb-Pb and Xe-Xe collisions"

description: $v_{3}\{2\}$ versus $\eta$ for $x^{\pm}$ in $\mathrm{Xe}-\mathrm{Xe}$ at $\sqrt{s_{\mathrm{NN}}}=5.44\,\mathrm{Te\!V}$
description: The pseudorapidity dependence of elliptic ($v_{2}$), triangular ($v_{3}$), and quadrangular ($v_{4}$) flow coefficients of charged particles measured in Pb-Pb collisions at a centre-of-mass energy per nucleon pair of $\sqrt{s_{\mathrm{NN}}}=5.02\,\mathrm{TeV}$ and in Xe-Xe collisions at $\sqrt{s_{\mathrm{NN}}}=5.44\,\mathrm{TeV}$ with ALICE at the LHC are presented. The measurements are performed in the pseudorapidity range $-3.5 &lt; \eta &lt; 5$ for various centrality intervals using two- and multi-particle cumulants with the subevent method. The flow probability density function (p.d.f.) is studied with the ratio of flow coefficient $v_2$ calculated with four- and two-particle cumulant, and suggests that the variance of flow p.d.f. is independent of pseudorapidity. The decorrelation of the flow vector in the longitudinal direction is probed using two-particle correlations. The results measured with respect to different reference regions in pseudorapidity exhibit differences, argued to be a result of saturating decorrelation effect above a certain pseudorapidity separation, in contrast to previous publications which assign this observation to non-flow effects. The results are compared to $3+1$ dimensional hydrodynamic and the AMPT transport model calculations. Neither of the models is able to simultaneously describe the pseudorapidity dependence of measurements of anisotropic flow and its fluctuations. The results presented in this work highlight shortcomings in our current understanding of initial conditions and subsequent system expansion in the longitudinal direction. Therefore, they provide input for its improvement.
DOI: 10.17182/hepdata.146644.v1/t1
title: "Figure3_Panel1" of "Measurements of inclusive J/$\psi$ production at midrapidity and forward rapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Inclusive J$/psi$ invariant yield as a function of pT in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV for 0-10% centrality interval and |y|&lt; 0.9. The given systematic uncertainties are the total systematic ones and are mostly considered as fully correlated over pT.;
description: No data abstract available.
DOI: 10.17182/hepdata.146644.v1/t2
title: "Figure3_Panel2" of "Measurements of inclusive J/$\psi$ production at midrapidity and forward rapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Inclusive J$/psi$ invariant yield as a function of pT in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV for 30-50% centrality interval and |y|&lt; 0.9. The given systematic uncertainties are the total systematic ones and are mostly considered as fully correlated over pT.;
description: No data abstract available.
DOI: 10.17182/hepdata.146644.v1/t3
title: "Figure4_Panel1" of "Measurements of inclusive J/$\psi$ production at midrapidity and forward rapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Inclusive J$/psi$ invariant yield as a function of pT in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV for 0-20% centrality interval and 2.5 &lt; y &lt; 4. The given systematic uncertainties are the total systematic ones. It contains the correlated uncertainties over pT which amount to 1.69%. ;
description: No data abstract available.
DOI: 10.17182/hepdata.146644.v1/t4
title: "Figure4_Panel2" of "Measurements of inclusive J/$\psi$ production at midrapidity and forward rapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Inclusive J$/psi$ invariant yield as a function of pT in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV for 20-40% centrality interval and 2.5 &lt; y &lt; 4. The given systematic uncertainties are the total systematic ones. It contains the correlated uncertainties over pT which amount to 1.41%.;
description: No data abstract available.
DOI: 10.17182/hepdata.146644.v1/t5
title: "Figure4_Panel3" of "Measurements of inclusive J/$\psi$ production at midrapidity and forward rapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Inclusive J$/psi$ invariant yield as a function of pT in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV for 40-90% centrality interval and 2.5 &lt; y &lt; 4. The given systematic uncertainties are the total systematic ones. It contains the correlated uncertainties over pT which amount to 2.95%.;
description: No data abstract available.
DOI: 10.17182/hepdata.146644.v1/t10
title: "Figure6-Panel2_fwdy_20-40" of "Measurements of inclusive J/$\psi$ production at midrapidity and forward rapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Nuclear modification factor for inclusive J$/psi$ as a function of pT in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV for 20-40% centrality interval and 2.5
description: No data abstract available.
DOI: 10.17182/hepdata.146644.v1/t11
title: "Figure6-Panel2_fwdy_40-90" of "Measurements of inclusive J/$\psi$ production at midrapidity and forward rapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Nuclear modification factor for inclusive J$/psi$ as a function of pT in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV for 40-90% centrality interval and 2.5
description: No data abstract available.
DOI: 10.17182/hepdata.146644.v1/t6
title: "Figure5" of "Measurements of inclusive J/$\psi$ production at midrapidity and forward rapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Nuclear modification factor for inclusive J$/psi$ as a function of Npart in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV and |y|&lt; 0.9. The given systematic uncertainties are the uncorrelated systematic ones over pT. The correlated systematic uncertainties over Npart amount to 7.36%.;
description: No data abstract available.
DOI: 10.17182/hepdata.146644.v1/t7
title: "Figure6-Panel1_midy_0-10" of "Measurements of inclusive J/$\psi$ production at midrapidity and forward rapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Nuclear modification factor for inclusive J$/psi$ as a function of pT in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV for 0-10% centrality interval and |y|&lt; 0.9. The given systematic uncertainties are the uncorrelated systematic ones over pT. The correlated systematic uncertainties over pT amount to 2.31%.;
description: No data abstract available.
DOI: 10.17182/hepdata.146644.v1/t8
title: "Figure6-Panel1_midy_30-50" of "Measurements of inclusive J/$\psi$ production at midrapidity and forward rapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Nuclear modification factor for inclusive J$/psi$ as a function of pT in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV for 30-50% centrality interval and |y|&lt; 0.9. The given systematic uncertainties are the uncorrelated systematic ones over pT. The correlated systematic uncertainties over pT amount to 2.72%.;
description: No data abstract available.
DOI: 10.17182/hepdata.146644.v1/t9
title: "Figure6-Panel2_fwdy_0-20" of "Measurements of inclusive J/$\psi$ production at midrapidity and forward rapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Nuclear modification factor for inclusive J$/psi$ as a function of pT in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV for 0-20% centrality interval and 2.5
description: No data abstract available.
DOI: 10.17182/hepdata.146644.v1/t12
title: "Figure11-Panel1" of "Measurements of inclusive J/$\psi$ production at midrapidity and forward rapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Average pT for inclusive J$/psi$ as a function of Npart in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV and |y|&lt; 0.9. The given systematic uncertainties are the total ones. ;
description: No data abstract available.
DOI: 10.17182/hepdata.146644.v1/t13
title: "Figure11-Panel2" of "Measurements of inclusive J/$\psi$ production at midrapidity and forward rapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Ratio rAA for inclusive J$/psi$ as a function of Npart in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV and |y|&lt; 0.9. The correlated systematic uncertainties over Npart amount to 4.61%;
description: No data abstract available.
DOI: 10.17182/hepdata.146644.v1/t14
title: "Figure13" of "Measurements of inclusive J/$\psi$ production at midrapidity and forward rapidity in Pb$-$Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV"

description: Inclusive J$/psi$ over prompt D0 invariant yield at 0-10% and 30-50% centrality intervals in Pb-Pb collisions at $\sqrt{{s}_{NN}}$ = 5.02 TeV and |y|&lt; 0.9. The given systematic uncertainties are the total ones. ;
description: No data abstract available.
DOI: 10.17182/hepdata.153810.v1/t1
title: "Table1_1" of "Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Inclusive charged-particle $v_{2}$ as a function of $p_{\mathrm{T}}$ in high-multiplicity (0$-$10%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV
description: The azimuthal anisotropy of particles associated with jets (jet particles) at midrapidity is measured for the first time in p--Pb and Pb--Pb collisions at $\sqrt{s_{NN}}$ $=$ 5.02 TeV down to transverse momentum ($\it{p}_{\rm T}$) of 0.5 GeV/$c$ and 2 GeV/$c$, respectively, with ALICE. The second-order Fourier coefficient of the jet-particle azimuthal distribution ($v_2$) in high-multiplicity p--Pb collisions is positive, with a significance reaching 6.8$\sigma$ at low $\it{p}_{\rm T}$. Comparisons with the inclusive charged-particle $v_2$ and with AMPT calculations are discussed. The model describes qualitatively the main features of the jet-particle $v_2$ in high-multiplicity p--Pb collisions and indicates that the positive jet-particle $v_2$ is generated by parton interactions.
DOI: 10.17182/hepdata.153810.v1/t2
title: "Table1_2" of "Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Jet-particle $v_{2}$ as a function of $p_{\mathrm{T}}$ in high-multiplicity (0$-$10%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV, the $p_{\mathrm{T}}$ of associated particles is larger than 0.5 GeV/$\it{c}$
description: The azimuthal anisotropy of particles associated with jets (jet particles) at midrapidity is measured for the first time in p--Pb and Pb--Pb collisions at $\sqrt{s_{NN}}$ $=$ 5.02 TeV down to transverse momentum ($\it{p}_{\rm T}$) of 0.5 GeV/$c$ and 2 GeV/$c$, respectively, with ALICE. The second-order Fourier coefficient of the jet-particle azimuthal distribution ($v_2$) in high-multiplicity p--Pb collisions is positive, with a significance reaching 6.8$\sigma$ at low $\it{p}_{\rm T}$. Comparisons with the inclusive charged-particle $v_2$ and with AMPT calculations are discussed. The model describes qualitatively the main features of the jet-particle $v_2$ in high-multiplicity p--Pb collisions and indicates that the positive jet-particle $v_2$ is generated by parton interactions.
DOI: 10.17182/hepdata.153810.v1/t3
title: "Table1_3" of "Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Jet-particle $v_{2}$ as a function of $p_{\mathrm{T}}$ in high-multiplicity (0$-$10%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV, the $p_{\mathrm{T}}$ of associated particles is larger than 1 GeV/$\it{c}$
description: The azimuthal anisotropy of particles associated with jets (jet particles) at midrapidity is measured for the first time in p--Pb and Pb--Pb collisions at $\sqrt{s_{NN}}$ $=$ 5.02 TeV down to transverse momentum ($\it{p}_{\rm T}$) of 0.5 GeV/$c$ and 2 GeV/$c$, respectively, with ALICE. The second-order Fourier coefficient of the jet-particle azimuthal distribution ($v_2$) in high-multiplicity p--Pb collisions is positive, with a significance reaching 6.8$\sigma$ at low $\it{p}_{\rm T}$. Comparisons with the inclusive charged-particle $v_2$ and with AMPT calculations are discussed. The model describes qualitatively the main features of the jet-particle $v_2$ in high-multiplicity p--Pb collisions and indicates that the positive jet-particle $v_2$ is generated by parton interactions.
DOI: 10.17182/hepdata.153810.v1/t4
title: "Table1_4" of "Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Jet-particle $v_{2}$ as a function of $p_{\mathrm{T}}$ in high-multiplicity (0$-$10%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV, the $p_{\mathrm{T}}$ of associated particles is larger than 1.5 GeV/$\it{c}$
description: The azimuthal anisotropy of particles associated with jets (jet particles) at midrapidity is measured for the first time in p--Pb and Pb--Pb collisions at $\sqrt{s_{NN}}$ $=$ 5.02 TeV down to transverse momentum ($\it{p}_{\rm T}$) of 0.5 GeV/$c$ and 2 GeV/$c$, respectively, with ALICE. The second-order Fourier coefficient of the jet-particle azimuthal distribution ($v_2$) in high-multiplicity p--Pb collisions is positive, with a significance reaching 6.8$\sigma$ at low $\it{p}_{\rm T}$. Comparisons with the inclusive charged-particle $v_2$ and with AMPT calculations are discussed. The model describes qualitatively the main features of the jet-particle $v_2$ in high-multiplicity p--Pb collisions and indicates that the positive jet-particle $v_2$ is generated by parton interactions.
DOI: 10.17182/hepdata.153810.v1/t5
title: "Table2_1" of "Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Inclusive charged-particle $v_{2}$ as a function of $p_{\mathrm{T}}$ in 20$-$60% semi-central Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV
description: The azimuthal anisotropy of particles associated with jets (jet particles) at midrapidity is measured for the first time in p--Pb and Pb--Pb collisions at $\sqrt{s_{NN}}$ $=$ 5.02 TeV down to transverse momentum ($\it{p}_{\rm T}$) of 0.5 GeV/$c$ and 2 GeV/$c$, respectively, with ALICE. The second-order Fourier coefficient of the jet-particle azimuthal distribution ($v_2$) in high-multiplicity p--Pb collisions is positive, with a significance reaching 6.8$\sigma$ at low $\it{p}_{\rm T}$. Comparisons with the inclusive charged-particle $v_2$ and with AMPT calculations are discussed. The model describes qualitatively the main features of the jet-particle $v_2$ in high-multiplicity p--Pb collisions and indicates that the positive jet-particle $v_2$ is generated by parton interactions.
DOI: 10.17182/hepdata.153810.v1/t6
title: "Table2_2" of "Azimuthal anisotropy of jet particles in p-Pb and Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV"

description: Jet-particle $v_{2}$ as a function of $p_{\mathrm{T}}$ in high-multiplicity (20$-$60%) Pb$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$ = 5.02 TeV, the $p_{\mathrm{T}}$ of associated particles is larger than 2 GeV/$\it{c}$
description: The azimuthal anisotropy of particles associated with jets (jet particles) at midrapidity is measured for the first time in p--Pb and Pb--Pb collisions at $\sqrt{s_{NN}}$ $=$ 5.02 TeV down to transverse momentum ($\it{p}_{\rm T}$) of 0.5 GeV/$c$ and 2 GeV/$c$, respectively, with ALICE. The second-order Fourier coefficient of the jet-particle azimuthal distribution ($v_2$) in high-multiplicity p--Pb collisions is positive, with a significance reaching 6.8$\sigma$ at low $\it{p}_{\rm T}$. Comparisons with the inclusive charged-particle $v_2$ and with AMPT calculations are discussed. The model describes qualitatively the main features of the jet-particle $v_2$ in high-multiplicity p--Pb collisions and indicates that the positive jet-particle $v_2$ is generated by parton interactions.