Centrality dependence of ${\rm AC}_{3,1}(2,3)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{1,3}(2,3)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{4,1}(2,3)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{1,4}(2,3)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm NAC}_{2,1}(2,3)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm NAC}_{1,2}(2,3)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm NAC}_{3,1}(2,3)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm NAC}_{1,3}(2,3)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm SC}(2,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{2,1}(2,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{1,2}(2,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{3,1}(2,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{1,3}(2,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{4,1}(2,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{1,4}(2,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm NAC}_{2,1}(2,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm NAC}_{1,2}(2,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm NAC}_{3,1}(2,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm SC}(3,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{2,1}(3,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{1,2}(3,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{3,1}(3,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{1,3}(3,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{4,1}(3,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm AC}_{1,4}(3,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm NAC}_{2,1}(3,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm NAC}_{1,2}(3,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of ${\rm NAC}_{3,1}(3,4)$ in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV.

Centrality dependence of $\langle \cos[6(\Psi_{6}-\Psi_{2})]\rangle_{\mathrm{GE}}$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.

Centrality dependence of $\langle \cos[2\Psi_{2}+3\Psi_{3}-5\Psi_{5}]\rangle_{\mathrm{GE}}$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.

Centrality dependence of $\langle \cos[2\Psi_{2}+4\Psi_{4}-6\Psi_{6}]\rangle_{\mathrm{GE}}$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.

Centrality dependence of $\langle \cos[8\Psi_{2}-3\Psi_{3}-5\Psi_{5}]\rangle_{\mathrm{GE}}$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.

Centrality dependence of $\langle \cos[2\Psi_{2}-6\Psi_{3}+4\Psi_{4}]\rangle_{\mathrm{GE}}$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.

Centrality dependence of $\langle \cos[2\Psi_{2}-3\Psi_{3}-4\Psi_{4}+5\Psi_{5}]\rangle_{\mathrm{GE}}$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$ TeV.

Charged-hadron spectrum in the centrality interval 5-10% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 10-20% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 20-30% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 30-40% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 40-60% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 60-90% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 0-90% for p+Pb, divided by 〈TPPB〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron cross-section in pp collisions. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 0-5% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron spectrum in the centrality interval 5-10% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron spectrum in the centrality interval 10-20% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron spectrum in the centrality interval 20-30% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron spectrum in the centrality interval 30-40% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron spectrum in the centrality interval 40-50% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron spectrum in the centrality interval 50-60% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron spectrum in the centrality interval 60-80% for Pb+Pb, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Charged-hadron cross-section in pp collisions. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 0-5% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 5-10% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 10-20% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 20-30% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 30-40% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 40-50% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 50-60% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Charged-hadron spectrum in the centrality interval 60-80% for Xe+Xe, divided by 〈TAA〉. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-60% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 5-10% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 10-20% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 20-30% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 30-40% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 40-50% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 50-60% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 60-80% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature. The systematic uncertainty on momentum bias is negligible at low pT; in such cases, it is omitted in the table below.

Nuclear modification factor in centrality interval 0-5% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-60% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-60% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-60% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-60% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-90% for p+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Pb+Pb. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 0-5% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 5-10% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 10-20% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 20-30% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 30-40% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 40-50% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 50-60% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Nuclear modification factor in centrality interval 60-80% for Xe+Xe. The systematic uncertainties are described in the section 7 of the paper. The total systematic uncertainties are determined by adding the contributions from all relevant sources in quadrature.

Centrality dependence of $v_2\{\Psi_{\mathrm{SP}}\}/v_2\{4\}$ and $v_2\{2,|\Delta\eta|>1\}/v_2\{4\}$ in Xe-Xe collisions at $\sqrt{s_{\mathrm{NN}}}=5.44~\mathrm{TeV}$.

Transverse momentum dependence of $v_2\{\Psi_{\mathrm{SP}}\}$ for different centrality classes in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76~\mathrm{TeV}$.

Transverse momentum dependence of $v_2\{4\}$ for different centrality classes in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76~\mathrm{TeV}$.

Transverse momentum dependence of $v_2\{\Psi_{\mathrm{SP}}\}/v_2\{4\}$ for different centrality classes in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76~\mathrm{TeV}$.

Slopes of the Linear fits to the transverse momentum dependence of $v_2\{\Psi_{\mathrm{SP}}\}/v_2\{4\}$ for different centrality classes in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76~\mathrm{TeV}$.

Ratios of $v_2/\varepsilon_2$ as a function of $1/S\ \mathrm{d}N_{\mathrm{ch}}/\mathrm{d}\eta$ in Xe--Xe collisions at $\sqrt{s_{\mathrm{NN}}}=5.44~\mathrm{TeV}$.

Ratios of $v_2/\varepsilon_2$ as a function of $1/S\ \mathrm{d}N_{\mathrm{ch}}/\mathrm{d}\eta$ in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76~\mathrm{TeV}$.

Ratios of $v_2/\varepsilon_2$ as a function of $1/S\ \mathrm{d}N_{\mathrm{ch}}/\mathrm{d}\eta$ in Xe--Xe collisions at $\sqrt{s_{\mathrm{NN}}}=5.44~\mathrm{TeV}$ divided by the linear Pb--Pb fits.

Ratios of $v_2/\varepsilon_2$ as a function of $1/S\ \mathrm{d}N_{\mathrm{ch}}/\mathrm{d}\eta$ for Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76~\mathrm{TeV}$ divided by the linear Pb--Pb fits.

Relative deviation of $v_2/\varepsilon_2$ as a function of $1/S\ \mathrm{d}N_{\mathrm{ch}}/\mathrm{d}\eta$ in Pb--Pb and Xe--Xe collisions.

Centrality dependence of ${\rm SC}(3,4,5)$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$~TeV.

Centrality dependence of ${\rm NSC}(2,3,4)$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$~TeV.

Centrality dependence of ${\rm NSC}(2,3,5)$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}} = 2.76$~TeV.

The standard deviation of the jet charge distributions with different track $p_{T}$ thresholds and $\kappa$ value pf 0.7 for pp collisions and in the various event centrality bins for PbPb collisions compared with the PYTHIA6 prediction.

Fitting results for the extraction of gluon-like jet fractions in pp and PbPb data shown for different track $p_{T}$ threshold values and $p_{T}$-weighting factor $\kappa$ values of 0.5.

Fitting results for the extraction of gluon-like jet fractions in pp and PbPb data shown for $p_{T}$-weighting factor $\kappa$ values of 0.3, 0.5, and 0.7 and minimum track $p_{T}$ of 1 GeV.

Fitting results for the extraction of gluon-like jet fractions in pp and PbPb data shown for $p_{T}$-weighting factor $\kappa$ values of 0.3, 0.5, and 0.7 and minimum track $p_{T}$ of 2 GeV.

Unfolded jet charge measurements for the $p_{T}$-weighting factor $\kappa = 0.5$ and a minimum track $p_{T}$ of 2 GeV for inclusive jets in pp and PbPb data. The PbPb results are shown for different centrality regions.

Unfolded jet charge measurements for the $p_{T}$-weighting factor $\kappa = 0.5$ and a minimum track $p_{T}$ of 4 GeV for inclusive jets in pp and PbPb data. The PbPb results are shown for different centrality regions.

Unfolded jet charge measurements for the $p_{T}$-weighting factor $\kappa = 0.5$ and a minimum track $p_{T}$ of 5 GeV for inclusive jets in pp and PbPb data. The PbPb results are shown for different centrality regions.

Unfolded jet charge measurements for a minimum track $p_{T}$ threshold of 1 GeV and $p_{T}$-weighting factor $\kappa = 0.3$ for inclusive jets in pp and PbPb data. The PbPb results are shown for different centrality regions.

Unfolded jet charge measurements for a minimum track $p_{T}$ threshold of 1 GeV and $p_{T}$-weighting factor $\kappa = 0.7$ for inclusive jets in pp and PbPb data. The PbPb results are shown for different centrality regions.

Unfolded jet charge measurements for a minimum track $p_{T}$ threshold of 2 GeV and $p_{T}$-weighting factor $\kappa = 0.3$ for inclusive jets in pp and PbPb data. The PbPb results are shown for different centrality regions.

Unfolded jet charge measurements for a minimum track $p_{T}$ threshold of 2 GeV and $p_{T}$-weighting factor $\kappa = 0.7$ for inclusive jets in pp and PbPb data. The PbPb results are shown for different centrality regions.

Centrality dependence of flow harmonics from $v_2$ to $v_9$.

Centrality dependence of flow harmonics from $v_2$ to $v_9$.

Centrality dependence of flow harmonics from $v_2$ to $v_9$.

Centrality dependence of flow harmonics from $v_2$ to $v_9$.

Centrality dependence of flow harmonics from $v_2$ to $v_9$.

Centrality dependence of linear and non-linear flow modes.

Centrality dependence of linear and non-linear flow modes.

Centrality dependence of linear and non-linear flow modes.

Centrality dependence of linear and non-linear flow modes.

Centrality dependence of linear and non-linear flow modes.

Centrality dependence of linear and non-linear flow modes.

Centrality dependence of symmetry-plane correlations.

Centrality dependence of symmetry-plane correlations.

Centrality dependence of symmetry-plane correlations.

Centrality dependence of symmetry-plane correlations.

Centrality dependence of non-linear flow mode coefficients.

Centrality dependence of non-linear flow mode coefficients.

Centrality dependence of non-linear flow mode coefficients.

Centrality dependence of non-linear flow mode coefficients.

Centrality dependence of non-linear flow mode coefficients.

The widths of near-side peaks for trigger jets in-plane, mid-plane, and out-of-plane vs $p_{T}^{assoc}$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions. The background uncertainty is non-trivially correlated point-to-point. The correlated systematic uncertainties come from the shape uncertainty of the acceptance correction.

The widths of away-side peaks for trigger jets in-plane, mid-plane, and out-of-plane vs $p_{T}^{assoc}$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions. The background uncertainty is non-trivially correlated point-to-point. The correlated systematic uncertainties come from the shape uncertainty of the acceptance correction.

Background subtracted correlation functions for $1.0<p_{T}^{assoc}<1.5$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Background subtracted correlation functions for $1.5<p_{T}^{assoc}<2.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Background subtracted correlation functions for $2.0<p_{T}^{assoc}<3.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Background subtracted correlation functions for $3.0<p_{T}^{assoc}<4.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Background subtracted correlation functions for $4.0<p_{T}^{assoc}<5.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Background subtracted correlation functions for $5.0<p_{T}^{assoc}<6.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Background subtracted correlation functions for $6.0<p_{T}^{assoc}<10.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in background dominated region for $1.0<p_{T}^{assoc}<1.5$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in background dominated region for $1.5<p_{T}^{assoc}<2.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in background dominated region for $2.0<p_{T}^{assoc}<3.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in background dominated region for $3.0<p_{T}^{assoc}<4.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in background dominated region for $4.0<p_{T}^{assoc}<5.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in background dominated region for $5.0<p_{T}^{assoc}<6.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in background dominated region for $6.0<p_{T}^{assoc}<10.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.0<p_{T}^{assoc}<1.5$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.5<p_{T}^{assoc}<2.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $2.0<p_{T}^{assoc}<3.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $3.0<p_{T}^{assoc}<4.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $4.0<p_{T}^{assoc}<5.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $5.0<p_{T}^{assoc}<6.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $6.0<p_{T}^{assoc}<10.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Response matrices for all jets with kinematic cuts described in the paper for 30-50% centrality in Pb-Pb collisions

Response matrices for in-plane jets with kinematic cuts described in the paper for 30-50% centrality in Pb-Pb collisions

Response matrices for mid-plane jets with kinematic cuts described in the paper for 30-50% centrality in Pb-Pb collisions

Response matrices for out-of-plane jets with kinematic cuts described in the paper for 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.0<p_{T}^{assoc}<1.5$ GeV/$c$ for in-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.0<p_{T}^{assoc}<1.5$ GeV/$c$ for mid-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.0<p_{T}^{assoc}<1.5$ GeV/$c$ for out-of-planes $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.0<p_{T}^{assoc}<1.5$ GeV/$c$ for all $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.5<p_{T}^{assoc}<2.0$ GeV/$c$ for in-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.5<p_{T}^{assoc}<2.0$ GeV/$c$ for mid-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.5<p_{T}^{assoc}<2.0$ GeV/$c$ for out-of-planes $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.5<p_{T}^{assoc}<2.0$ GeV/$c$ for all $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $2.0<p_{T}^{assoc}<3.0$ GeV/$c$ for in-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $2.0<p_{T}^{assoc}<3.0$ GeV/$c$ for mid-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $2.0<p_{T}^{assoc}<3.0$ GeV/$c$ for out-of-planes $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $2.0<p_{T}^{assoc}<3.0$ GeV/$c$ for all $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $3.0<p_{T}^{assoc}<4.0$ GeV/$c$ for in-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $3.0<p_{T}^{assoc}<4.0$ GeV/$c$ for mid-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $3.0<p_{T}^{assoc}<4.0$ GeV/$c$ for out-of-planes $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $3.0<p_{T}^{assoc}<4.0$ GeV/$c$ for all $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $4.0<p_{T}^{assoc}<5.0$ GeV/$c$ for in-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $4.0<p_{T}^{assoc}<5.0$ GeV/$c$ for mid-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $4.0<p_{T}^{assoc}<5.0$ GeV/$c$ for out-of-planes $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $4.0<p_{T}^{assoc}<5.0$ GeV/$c$ for all $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $5.0<p_{T}^{assoc}<6.0$ GeV/$c$ for in-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $5.0<p_{T}^{assoc}<6.0$ GeV/$c$ for mid-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $5.0<p_{T}^{assoc}<6.0$ GeV/$c$ for out-of-planes $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $5.0<p_{T}^{assoc}<6.0$ GeV/$c$ for all $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $6.0<p_{T}^{assoc}<10.0$ GeV/$c$ for in-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $6.0<p_{T}^{assoc}<10.0$ GeV/$c$ for mid-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $6.0<p_{T}^{assoc}<10.0$ GeV/$c$ for out-of-planes $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $6.0<p_{T}^{assoc}<10.0$ GeV/$c$ for all $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

$p_{T}$-distributions of kaons ($K^{+}+K^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{T}$-distributions of protons ($p+pbar$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{T}$-distributions of protons ($p+pbar$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{T}$-distributions of kaons ($K^{+}+K^{-}$)/pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{T}$-distributions of kaons ($K^{+}+K^{-}$)/pions ($\pi^{+}+\pi^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{T}$-distributions of protons ($p+pbar$)/pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{T}$-distributions of protons ($p+pbar$)/pions ($\pi^{+}+\pi^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

Integrated yield ratios of kaons ($K^{+}+K^{-}$) to pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

Integrated yield ratios of kaons ($K^{+}+K^{-}$) to pions ($\pi^{+}+\pi^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

Integrated yield ratios of protons ($p+pbar$) to pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

Integrated yield ratios of protons ($p+pbar$) to pions ($\pi^{+}+\pi^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{T}$-dependent nuclear modification factor of pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{T}$-dependent nuclear modification factor of kaons ($K^{+}+K^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{T}$-dependent nuclear modification factor of protons ($p+pbar$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

The V2 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 5-10%

The V2 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 10-20%

The V2 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 20-30%

The V2 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 30-40%

The V2 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 40-50%

The V2 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 50-60%

The V2 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 60-70%

The V2 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 70-80%

The V3 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 0-0.1%

The V3 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 0-1%

The V3 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 0-5%

The V3 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 5-10%

The V3 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 10-20%

The V3 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 20-30%

The V3 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 30-40%

The V3 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 40-50%

The V3 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 50-60%

The V3 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 60-70%

The V3 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 70-80%

The V4 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 0-0.1%

The V4 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 0-1%

The V4 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 0-5%

The V4 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 5-10%

The V4 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 10-20%

The V4 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 20-30%

The V4 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 30-40%

The V4 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 40-50%

The V4 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 50-60%

The V4 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 60-70%

The V4 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 70-80%

The V5 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 0-0.1%

The V5 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 0-1%

The V5 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 0-5%

The V5 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 5-10%

The V5 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 10-20%

The V5 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 20-30%

The V5 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 30-40%

The V5 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 40-50%

The V5 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 50-60%

The V5 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 60-70%

The V5 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 70-80%

The V6 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 0-5%

The V6 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 5-10%

The V6 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 10-20%

The V6 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 20-30%

The V6 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 30-40%

The V6 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 40-50%

The V6 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 50-60%

The V6 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 60-70%

The V6 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 70-80%

The V7 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 0-5%

The V7 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 5-10%

The V7 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 10-20%

The V7 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 20-30%

The V7 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 30-40%

The V7 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 40-50%

The V7 harmonic measured with the scalar product method as a funtion of transverse momentum in centrality bin 50-60%

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 0-5%

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 5-10%

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 10-20%

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 20-30%

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 30-40%

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 40-50%

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 50-60%

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 60-70%

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 70-80%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 0-5%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 5-10%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 10-20%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 20-30%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 30-40%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 40-50%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 50-60%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 60-70%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 70-80%

The V4 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 0-5%

The V4 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 5-10%

The V4 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 10-20%

The V4 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 20-30%

The V4 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 30-40%

The V4 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 40-50%

The V4 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 50-60%

The V4 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 60-70%

The V4 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 70-80%

The V5 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 0-5%

The V5 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 5-10%

The V5 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 10-20%

The V5 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 20-30%

The V5 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 30-40%

The V5 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 40-50%

The V5 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 50-60%

The V5 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 60-70%

The V6 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 0-5%

The V6 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 5-10%

The V6 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 10-20%

The V6 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 20-30%

The V6 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 30-40%

The V6 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 40-50%

The V6 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 50-60%

The V6 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 60-70%

The ratio of V2{SP} over V2{EP} as a funtion of transverse momentum in centrality bin 0-5%

The ratio of V2{SP} over V2{EP} as a funtion of transverse momentum in centrality bin 20-30%

The ratio of V2{SP} over V2{EP} as a funtion of transverse momentum in centrality bin 40-50%

The ratio of V3{SP} over V3{EP} as a funtion of transverse momentum in centrality bin 0-5%

The ratio of V3{SP} over V3{EP} as a funtion of transverse momentum in centrality bin 20-30%

The ratio of V3{SP} over V3{EP} as a funtion of transverse momentum in centrality bin 40-50%

The ratio of V4{SP} over V4{EP} as a funtion of transverse momentum in centrality bin 0-5%

The ratio of V4{SP} over V4{EP} as a funtion of transverse momentum in centrality bin 20-30%

The ratio of V4{SP} over V4{EP} as a funtion of transverse momentum in centrality bin 40-50%

The ratio of V5{SP} over V5{EP} as a funtion of transverse momentum in centrality bin 0-5%

The ratio of V5{SP} over V5{EP} as a funtion of transverse momentum in centrality bin 20-30%

The ratio of V5{SP} over V5{EP} as a funtion of transverse momentum in centrality bin 40-50%

The ratio of V6{SP} over V6{EP} as a funtion of transverse momentum in centrality bin 0-5%

The ratio of V6{SP} over V6{EP} as a funtion of transverse momentum in centrality bin 20-30%

The ratio of V6{SP} over V6{EP} as a funtion of transverse momentum in centrality bin 40-50%

The ratio of V2{SP} over V2{EP} as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The ratio of V3{SP} over V3{EP} as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The ratio of V4{SP} over V4{EP} as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The ratio of V5{SP} over V5{EP} as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The ratio of V6{SP} over V6{EP} as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The ratio of V2{SP} over V2{2PC} as a funtion of transverse momentum in centrality bin 0-5%

The ratio of V2{SP} over V2{2PC} as a funtion of transverse momentum in centrality bin 20-30%

The ratio of V2{SP} over V2{2PC} as a funtion of transverse momentum in centrality bin 40-50%

The ratio of V3{SP} over V3{2PC} as a funtion of transverse momentum in centrality bin 0-5%

The ratio of V3{SP} over V3{2PC} as a funtion of transverse momentum in centrality bin 20-30%

The ratio of V3{SP} over V3{2PC} as a funtion of transverse momentum in centrality bin 40-50%

The ratio of V4{SP} over V4{2PC} as a funtion of transverse momentum in centrality bin 0-5%

The ratio of V4{SP} over V4{2PC} as a funtion of transverse momentum in centrality bin 20-30%

The ratio of V4{SP} over V4{2PC} as a funtion of transverse momentum in centrality bin 40-50%

The ratio of V5{SP} over V5{2PC} as a funtion of transverse momentum in centrality bin 0-5%

The ratio of V5{SP} over V5{2PC} as a funtion of transverse momentum in centrality bin 20-30%

The ratio of V5{SP} over V5{2PC} as a funtion of transverse momentum in centrality bin 40-50%

The V2 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-5%. PT binning matched to RUN1.

The V2 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 20-30%. PT binning matched to RUN1.

The V2 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 40-50%. PT binning matched to RUN1.

The V3 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-5%. PT binning matched to RUN1.

The V3 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 20-30%. PT binning matched to RUN1.

The V3 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 40-50%. PT binning matched to RUN1.

The V4 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-5%. PT binning matched to RUN1.

The V4 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 20-30%. PT binning matched to RUN1.

The V4 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 40-50%. PT binning matched to RUN1.

The V5 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-5%. PT binning matched to RUN1.

The V5 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 20-30%. PT binning matched to RUN1.

The V5 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 40-50%. PT binning matched to RUN1.

The V6 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-5%. PT binning matched to RUN1.

The V6 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 20-30%. PT binning matched to RUN1.

The V6 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 40-50%. PT binning matched to RUN1.

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-0.1%

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-5%

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 10-20%

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 30-40%

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 60-70%

The V3 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-0.1%

The V3 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-5%

The V3 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 10-20%

The V3 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 30-40%

The V3 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 60-70%

The V4 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-0.1%

The V4 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-5%

The V4 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 10-20%

The V4 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 30-40%

The V4 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 60-70%

The V5 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-0.1%

The V5 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-5%

The V5 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 10-20%

The V5 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 30-40%

The V5 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 60-70%

The V6 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-5%

The V6 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 10-20%

The V6 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 30-40%

The V6 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 60-70%

The V7 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-5%

The V7 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 10-20%

The V7 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 30-40%

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-0.1%

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-5%

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 10-20%

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 30-40%

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 60-70%

The V3 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-0.1%

The V3 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-5%

The V3 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 10-20%

The V3 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 30-40%

The V3 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 60-70%

The V4 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-0.1%

The V4 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-5%

The V4 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 10-20%

The V4 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 30-40%

The V4 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 60-70%

The V5 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-0.1%

The V5 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-5%

The V5 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 10-20%

The V5 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 30-40%

The V5 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 60-70%

The V6 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-5%

The V6 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 10-20%

The V6 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 30-40%

The V6 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 60-70%

The V7 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-5%

The V7 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 10-20%

The V7 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 30-40%

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 0-0.1%

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 0-5%

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 10-20%

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 30-40%

The V2 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 60-70%

The V3 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 0-0.1%

The V3 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 0-5%

The V3 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 10-20%

The V3 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 30-40%

The V4 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 0-0.1%

The V4 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 0-5%

The V4 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 10-20%

The V4 harmonic measured with the scalar product method as a funtion of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 30-40%

The V2 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 0.8 GeV

The V2 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.8 < PT < 1 GeV

The V2 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 1 < PT < 2 GeV

The V2 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 2 < PT < 4 GeV

The V2 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 4 < PT < 8 GeV

The V2 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 8 < PT < 60 GeV

The V2 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The V3 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 0.8 GeV

The V3 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.8 < PT < 1 GeV

The V3 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 1 < PT < 2 GeV

The V3 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 2 < PT < 4 GeV

The V3 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 4 < PT < 8 GeV

The V3 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 8 < PT < 60 GeV

The V3 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The V4 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 0.8 GeV

The V4 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.8 < PT < 1 GeV

The V4 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 1 < PT < 2 GeV

The V4 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 2 < PT < 4 GeV

The V4 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 4 < PT < 8 GeV

The V4 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 8 < PT < 60 GeV

The V4 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The V5 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 0.8 GeV

The V5 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.8 < PT < 1 GeV

The V5 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 1 < PT < 2 GeV

The V5 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 2 < PT < 4 GeV

The V5 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 4 < PT < 8 GeV

The V5 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 8 < PT < 60 GeV

The V5 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The V6 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 0.8 GeV

The V6 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.8 < PT < 1 GeV

The V6 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 1 < PT < 2 GeV

The V6 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 2 < PT < 4 GeV

The V6 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 4 < PT < 8 GeV

The V6 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 8 < PT < 60 GeV

The V6 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The V7 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 0.8 GeV

The V7 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.8 < PT < 1 GeV

The V7 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 1 < PT < 2 GeV

The V7 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 2 < PT < 4 GeV

The V7 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 4 < PT < 8 GeV

The V7 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 8 < PT < 60 GeV

The V7 harmonic measured with the scalar product method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 0-5%

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 10-15%

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 20-25%

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 30-35%

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 40-45%

The V2 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 50-55%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 0-5%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 10-15%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 20-25%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 30-35%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 40-45%

The V3 harmonic measured with the two particle correlation method as a funtion of transverse momentum in centrality bin 50-55%

The scaled-V2(PT) measured with the two particle correlation method in centrality bin 0-5%

The scaled-V2(PT) measured with the two particle correlation method in centrality bin 10-15%

The scaled-V2(PT) measured with the two particle correlation method in centrality bin 20-25%

The scaled-V2(PT) measured with the two particle correlation method in centrality bin 30-35%

The scaled-V2(PT) measured with the two particle correlation method in centrality bin 40-45%

The scaled-V2(PT) measured with the two particle correlation method in centrality bin 50-55%

The scaled-V3(PT) measured with the two particle correlation method in centrality bin 0-5%

The scaled-V3(PT) measured with the two particle correlation method in centrality bin 10-15%

The scaled-V3(PT) measured with the two particle correlation method in centrality bin 20-25%

The scaled-V3(PT) measured with the two particle correlation method in centrality bin 30-35%

The scaled-V3(PT) measured with the two particle correlation method in centrality bin 40-45%

The scaled-V3(PT) measured with the two particle correlation method in centrality bin 50-55%

The PT scale factor for V2(PT) as a funtion of collision centrality

The PT scale factor for V3(PT) as a funtion of collision centrality

The V2 scale factor as a funtion of collision centrality

The V3 scale factor as a funtion of collision centrality

The V2 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-0.1%

The V2 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-1%

The V2 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-5%

The V2 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 5-10%

The V2 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 10-20%

The V2 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 20-30%

The V2 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 30-40%

The V2 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 40-50%

The V2 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 50-60%

The V2 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 60-70%

The V2 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 70-80%

The V3 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-0.1%

The V3 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-1%

The V3 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-5%

The V3 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 5-10%

The V3 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 10-20%

The V3 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 20-30%

The V3 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 30-40%

The V3 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 40-50%

The V3 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 50-60%

The V3 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 60-70%

The V3 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 70-80%

The V4 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-0.1%

The V4 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-1%

The V4 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-5%

The V4 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 5-10%

The V4 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 10-20%

The V4 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 20-30%

The V4 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 30-40%

The V4 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 40-50%

The V4 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 50-60%

The V4 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 60-70%

The V4 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 70-80%

The V5 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-0.1%

The V5 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-1%

The V5 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-5%

The V5 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 5-10%

The V5 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 10-20%

The V5 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 20-30%

The V5 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 30-40%

The V5 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 40-50%

The V5 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 50-60%

The V5 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 60-70%

The V5 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 70-80%

The V6 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-5%

The V6 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 5-10%

The V6 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 10-20%

The V6 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 20-30%

The V6 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 30-40%

The V6 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 40-50%

The V6 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 50-60%

The V6 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 60-70%

The V6 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 70-80%

The V7 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 0-5%

The V7 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 5-10%

The V7 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 10-20%

The V7 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 20-30%

The V7 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 30-40%

The V7 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 40-50%

The V7 harmonic measured with the event plane method as a funtion of transverse momentum in centrality bin 50-60%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-0.1%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-5%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 10-20%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 30-40%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 60-70%

The V3 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-0.1%

The V3 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-5%

The V3 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 10-20%

The V3 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 30-40%

The V3 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 60-70%

The V4 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-0.1%

The V4 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-5%

The V4 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 10-20%

The V4 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 30-40%

The V4 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 60-70%

The V5 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-0.1%

The V5 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-5%

The V5 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 10-20%

The V5 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 30-40%

The V5 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 60-70%

The V6 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-5%

The V6 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 10-20%

The V6 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 30-40%

The V6 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 60-70%

The V7 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 0-5%

The V7 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 10-20%

The V7 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 0.8 < PT < 1 GeV in centrality bin 30-40%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-0.1%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-5%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 10-20%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 30-40%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 60-70%

The V3 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-0.1%

The V3 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-5%

The V3 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 10-20%

The V3 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 30-40%

The V3 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 60-70%

The V4 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-0.1%

The V4 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-5%

The V4 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 10-20%

The V4 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 30-40%

The V4 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 60-70%

The V5 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-0.1%

The V5 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-5%

The V5 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 10-20%

The V5 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 30-40%

The V5 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 60-70%

The V6 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-5%

The V6 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 10-20%

The V6 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 30-40%

The V6 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 60-70%

The V7 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 0-5%

The V7 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 10-20%

The V7 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 2 < PT < 3 GeV in centrality bin 30-40%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 0-0.1%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 0-5%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 10-20%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 30-40%

The V2 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 60-70%

The V3 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 0-0.1%

The V3 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 0-5%

The V3 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 10-20%

The V3 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 30-40%

The V4 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 0-0.1%

The V4 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 0-5%

The V4 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 10-20%

The V4 harmonic measured with the event plane method as a function of pseudorapidity for transverse momentum range 7 < PT < 60 GeV in centrality bin 30-40%

The V2 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 0.8 GeV

The V2 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.8 < PT < 1 GeV

The V2 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 1 < PT < 2 GeV

The V2 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 2 < PT < 4 GeV

The V2 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 4 < PT < 8 GeV

The V2 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 8 < PT < 60 GeV

The V2 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The V3 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 0.8 GeV

The V3 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.8 < PT < 1 GeV

The V3 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 1 < PT < 2 GeV

The V3 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 2 < PT < 4 GeV

The V3 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 4 < PT < 8 GeV

The V3 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 8 < PT < 60 GeV

The V3 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The V4 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 0.8 GeV

The V4 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.8 < PT < 1 GeV

The V4 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 1 < PT < 2 GeV

The V4 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 2 < PT < 4 GeV

The V4 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 4 < PT < 8 GeV

The V4 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 8 < PT < 60 GeV

The V4 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The V5 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 0.8 GeV

The V5 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.8 < PT < 1 GeV

The V5 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 1 < PT < 2 GeV

The V5 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 2 < PT < 4 GeV

The V5 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 4 < PT < 8 GeV

The V5 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 8 < PT < 60 GeV

The V5 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The V6 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 0.8 GeV

The V6 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.8 < PT < 1 GeV

The V6 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 1 < PT < 2 GeV

The V6 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 2 < PT < 4 GeV

The V6 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 4 < PT < 8 GeV

The V6 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 8 < PT < 60 GeV

The V6 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

The V7 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 0.8 GeV

The V7 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.8 < PT < 1 GeV

The V7 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 1 < PT < 2 GeV

The V7 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 2 < PT < 4 GeV

The V7 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 4 < PT < 8 GeV

The V7 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 8 < PT < 60 GeV

The V7 harmonic measured with the event plane method as a funtion of MEAN(Npart) integrated over 0.5 < PT < 60 GeV

Values of $2/\langle N_\mathrm{part} \rangle \langle \mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle$ and $2/\langle N_\mathrm{part} \rangle N^\mathrm{tot}_\mathrm{ch}$ in Xe--Xe collisions at $\sqrt{s_{_{\mathrm{NN}}}} = 5.44\,\mathrm{TeV}$ for the top 5$\%$ central collisions.

Values of $2/\langle N_\mathrm{part} \rangle \langle \mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle$ and $2/\langle N_\mathrm{part} \rangle N^\mathrm{tot}_\mathrm{ch}$ as a function of $\langle N_\mathrm{part} \rangle$ in Xe--Xe collisions at $\sqrt{s_{_{\mathrm{NN}}}} = 5.44\,\mathrm{TeV}$.

Values of $2/\langle N_\mathrm{part} \rangle \langle \mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle$ and $2/\langle N_\mathrm{part} \rangle N^\mathrm{tot}_\mathrm{ch}$ as a function of $\langle N_\mathrm{part} \rangle$ in Xe--Xe collisions at $\sqrt{s_{_{\mathrm{NN}}}} = 5.44\,\mathrm{TeV}$.

Values of $2/\langle N_\mathrm{part} \rangle \langle \mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle$ and $2/\langle N_\mathrm{part} \rangle N^\mathrm{tot}_\mathrm{ch}$ as a function of $(\langle N_\mathrm{part} \rangle -2)/(2A)$ in Xe--Xe collisions at $\sqrt{s_{_{\mathrm{NN}}}} = 5.44\,\mathrm{TeV}$.

Values of $2/\langle N_\mathrm{part} \rangle \langle \mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle$ and $2/\langle N_\mathrm{part} \rangle N^\mathrm{tot}_\mathrm{ch}$ as a function of $(\langle N_\mathrm{part} \rangle -2)/(2A)$ in Xe--Xe collisions at $\sqrt{s_{_{\mathrm{NN}}}} = 5.44\,\mathrm{TeV}$.

Values of $2/\langle N_\mathrm{part} \rangle \langle \mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle$ and $2/\langle N_\mathrm{part} \rangle N^\mathrm{tot}_\mathrm{ch}$ as a function of $\langle N_\mathrm{part} \rangle$ in Pb--Pb collisions at $\sqrt{s_{_{\mathrm{NN}}}} = 5.02\,\mathrm{TeV}$.

Values of $2/\langle N_\mathrm{part} \rangle \langle \mathrm{d}N_\mathrm{ch}/\mathrm{d}\eta\rangle$ and $2/\langle N_\mathrm{part} \rangle N^\mathrm{tot}_\mathrm{ch}$ as a function of $(\langle N_\mathrm{part} \rangle -2)/(2A)$ in Pb--Pb collisions at $\sqrt{s_{_{\mathrm{NN}}}} = 5.02\,\mathrm{TeV}$.

Ratio of transverse momentum spectra in Xe-Xe and Pb-Pb.

Raa vs $\langle dNch/d\eta \rangle$.

Raa vs $\langle dNch/d\eta \rangle$.

Raa vs $\langle dNch/d\eta \rangle$.

Average transverse momentum vs centrality percentage for PbPb and XeXe. And the ratio between collision systems.

The difference between the PbPb and pp measurements from Table 3.

The distribution of jet-correlated charged-particle tracks as a function of $\Delta\mathrm{r}$ in pp and PbPb collisions. The PbPb results are shown for different centrality regions.

The difference between the PbPb and pp measurements from Table 5.

The distribution of jet-correlated charged-particle tracks with $\Delta\mathrm{r} <1$ as a function of ${p_{\mathrm{T}}^{\text{trk}}}$ in PbPb and pp collisions. The PbPb results are shown for different centrality regions.

The corresponding results for the difference between the PbPb and pp measurements from Table 7.

The radial jet momentum distribution $\mathrm{P}(\Delta\mathrm{r})$ of jets in pp and PbPb collisions. The PbPb results are shown for different centrality regions.

The ratio between PbPb and pp measurements from Table 9 for the indicated intervals of ${p_{\mathrm{T}}^{\text{trk}}}$.

The jet shape $\rho(\Delta\mathrm{r})$ in pp and PbPb collisions. The PbPb results are shown for different centrality regions.

The ratio between the PbPb and pp measurements from Table 11 for the inclusive range $0.7< {p_{\mathrm{T}}^{\text{trk}}} <300GeV$.

Transverse momentum spectra of charged particles in pp collisions.

Ratio Data/MC

Additional systematic error for pp data: +3.0 pct -3.0 pct Additional systematic error for PBPB 0-5 pct data: +0.08 pct -0.08 pct Additional systematic error for PBPB 5-10 pct data: +0.24 pct -0.24 pct Additional systematic error for PBPB 10-20 pct data: +0.46 pct -0.46 pct Additional systematic error for PBPB 20-30 pct data: +0.81 pct -0.81 pct Additional systematic error for PBPB 30-40 pct data: +1.26 pct -1.26 pct Additional systematic error for PBPB 40-50 pct data: +1.86 pct -1.86 pct Additional systematic error for PBPB 50-60 pct data: +2.64 pct -2.64 pct Additional systematic error for PBPB 60-70 pct data: +3.67 pct -3.67 pct Additional systematic error for PBPB 70-80 pct data: +5.01 pct -5.01 pct.

Additional systematic error for PBPB 0-5 pct data: +2.2 pct -2.2 pct Additional systematic error for PBPB 5-10 pct data: +2.2 pct -2.2 pct Additional systematic error for PBPB 10-20 pct data: +2.4 pct -2.4 pct Additional systematic error for PBPB 20-30 pct data: +2.7 pct -2.7 pct Additional systematic error for PBPB 30-40 pct data: +3.4 pct -3.4 pct Additional systematic error for PBPB 40-50 pct data: +3.7 pct -3.7 pct Additional systematic error for PBPB 50-60 pct data: +4.9 pct -4.9 pct Additional systematic error for PBPB 60-70 pct data: +6.7 pct -6.7 pct Additional systematic error for PBPB 70-80 pct data: +7.1 pct -7.1 pct.

Additional systematic error for PBPB 0-5 pct data: +2.7 pct -2.7 pct Additional systematic error for PBPB 5-10 pct data: +3.5 pct -3.5 pct Additional systematic error for PBPB 10-20 pct data: +3.5 pct -3.5 pct Additional systematic error for PBPB 20-30 pct data: +4.1 pct -4.1 pct Additional systematic error for PBPB 30-40 pct data: +3.7 pct -3.7 pct Additional systematic error for PBPB 40-50 pct data: +3.9 pct -3.9 pct Additional systematic error for PBPB 50-60 pct data: +3.6 pct -3.6 pct Additional systematic error for PBPB 60-70 pct data: +4.6 pct -4.6 pct Additional systematic error for PBPB 70-80 pct data: +5.9 pct -5.9 pct.

Additional systematic error for P-PB NSD data: +4.6 pct -4.6 pct.

The Symmetric cumulant $SC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

The Symmetric cumulant $SC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in pPb collisions at $\sqrt{s_{NN}}$ = 8.16 TeV.

The Symmetric cumulant $SC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in pp collisions at $\sqrt{s}$ = 13.0 TeV.

The Normalized Symmetric cumulant $NSC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. The results are normalized by $\left<(v_2^{\text{sub}})^{2}\right> \, \left<(v_3^{\text{sub}})^{2}\right>$ and $\left<(v_2^{\text{sub}})^{2}\right> \, \left<(v_4^{\text{sub}})^{2}\right>$ from two-particle correlations.

The Normalized Symmetric cumulant $NSC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in pPb collisions at $\sqrt{s_{NN}}$ = 8.16 TeV. The results are normalized by $\left<(v_2^{\text{sub}})^{2}\right> \, \left<(v_3^{\text{sub}})^{2}\right>$ and $\left<(v_2^{\text{sub}})^{2}\right> \, \left<(v_4^{\text{sub}})^{2}\right>$ from two-particle correlations.

The Normalized Symmetric cumulant $NSC(n,m)$ results as a function of multiplicity ($N_{trk}^{offline}$) in pp collisions at $\sqrt{s}$ = 13.0 TeV. The results are normalized by $\left<(v_2^{\text{sub}})^{2}\right> \, \left<(v_3^{\text{sub}})^{2}\right>$ and $\left<(v_2^{\text{sub}})^{2}\right> \, \left<(v_4^{\text{sub}})^{2}\right>$ from two-particle correlations.

Centrality dependence of observables SC(5,3) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables SC(4,3) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables SC(4,3) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(5,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(5,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(5,3) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(5,3) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,3) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,3) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables $v_5$ in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables $v_5$ in Pb-Pb collisions at 2.76 TeV.

The $v_{2}$ result from SP method as a function of $p_{T}$ in 20-30\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{2}$ result from SP method as a function of $p_{T}$ in 30-40\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{2}$ result from SP method as a function of $p_{T}$ in 40-50\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{2}$ result from SP method as a function of $p_{T}$ in 50-60\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{3}$ result from SP method as a function of $p_{T}$ in 0-5\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{3}$ result from SP method as a function of $p_{T}$ in 5-10\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{3}$ result from SP method as a function of $p_{T}$ in 10-20\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{3}$ result from SP method as a function of $p_{T}$ in 20-30\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{3}$ result from SP method as a function of $p_{T}$ in 30-40\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{3}$ result from SP method as a function of $p_{T}$ in 40-50\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{3}$ result from SP method as a function of $p_{T}$ in 50-60\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{2}$ result from 4-, 6- and 8-particle cumulant methods as a function of $p_{T}$ in 5-10\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{2}$ result from 4-, 6- and 8-particle cumulant methods as a function of $p_{T}$ in 10-20\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{2}$ result from 4-, 6- and 8-particle cumulant methods as a function of $p_{T}$ in 20-30\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{2}$ result from 4-, 6- and 8-particle cumulant methods as a function of $p_{T}$ in 30-40\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{2}$ result from 4-, 6- and 8-particle cumulant methods as a function of $p_{T}$ in 40-50\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{2}$ result from 4-, 6- and 8-particle cumulant methods as a function of $p_{T}$ in 50-60\% centrality bin of PbPb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. Shaded boxes represent systematic uncertainties.

The $v_{2}^{high}$ as a function of $v_{2}^{low}$ results from SP method in PbPb collisions at $sqrt{s_{NN}}$ = 5.02 TeV. Only statistical uncertainties are shown.

The $v_{2}^{high}$ as a function of $v_{2}^{low}$ results from 4-particle cumulant method in PbPb collisions at $sqrt{s_{NN}}$ = 5.02 TeV. Only statistical uncertainties are shown.

Estimation of $\mathrm{d}N_{\mathrm{ch}}/\mathrm{d}y$ for in the most central Pb-Pb collisions at $\sqrt{s_{_{\mathrm{NN}}}}=5.02\,\mathrm{TeV}$. Also shown is a fit of Gaussian distribution to the data.

Scaling behaviour as a function $\sqrt{s_{_{\mathrm{NN}}}}$ of the width of the charged-particle or -pion rapidity-density distribution with respect to the Landau-Carruthers width (top) and rapidity range (bottom). Charged-pion points from AGS and SPS are adapted from the literature [PRL94.162301], while the PHOBOS (filled crosses) [PRL91,052303] and BRAHMS (open crosses) [PRL88.202301] charged-hadron points are translated from the corresponding $\mathrm{d}N_{\mathrm{ch}}/\mathrm{d}\eta$ results.

Charged-particle per-event yields measured in 5-10% PbPb centrality class.

Charged-particle per-event yields measured in 10-30% PbPb centrality class.

Charged-particle per-event yields measured in 10-30% PbPb centrality class.

Charged-particle per-event yields measured in 30-50% PbPb centrality class.

Charged-particle per-event yields measured in 30-50% PbPb centrality class.

Charged-particle per-event yields measured in 50-70% PbPb centrality class.

Charged-particle per-event yields measured in 50-70% PbPb centrality class.

Charged-particle per-event yields measured in 70-90% PbPb centrality class.

Charged-particle per-event yields measured in 70-90% PbPb centrality class.

Charged-particle per-event yields measured in pp collisions. A factor of 70 mb is used to scale the pp spectrum from a differential cross section to a per-event yield for direct comparison to the PbPb spectra. The lumi uncertainty is a 2.3% fully correlated uncertainty.

Charged-particle per-event yields measured in pp collisions. A factor of 70 mb is used to scale the pp spectrum from a differential cross section to a per-event yield for direct comparison to the PbPb spectra. The lumi uncertainty is a 2.3% fully correlated uncertainty.

PbPb nuclear modification factor measured in 0-5% PbPb centrality class.

PbPb nuclear modification factor measured in 0-5% PbPb centrality class.

PbPb nuclear modification factor measured in 5-10% PbPb centrality class.

PbPb nuclear modification factor measured in 5-10% PbPb centrality class.

PbPb nuclear modification factor measured in 10-30% PbPb centrality class.

PbPb nuclear modification factor measured in 10-30% PbPb centrality class.

PbPb nuclear modification factor measured in 30-50% PbPb centrality class.

PbPb nuclear modification factor measured in 30-50% PbPb centrality class.

PbPb nuclear modification factor measured in 50-70% PbPb centrality class.

PbPb nuclear modification factor measured in 50-70% PbPb centrality class.

PbPb nuclear modification factor measured in 70-90% PbPb centrality class.

PbPb nuclear modification factor measured in 70-90% PbPb centrality class.

PbPb nuclear modification factor measured in 0-10% PbPb centrality class.

PbPb nuclear modification factor measured in 0-10% PbPb centrality class.

PbPb nuclear modification factor measured in 0-100% PbPb centrality class.

PbPb nuclear modification factor measured in 0-100% PbPb centrality class.

pPb nuclear modification factor.

pPb nuclear modification factor.

Per-trigger yield modification, $I_{\rm AA}$, on the away side with trigger $\pi^{0}$ particle at $8 < p_{T}^{trig} < 16~GeV/c$ for $0$-$10$$\%$ Pb-Pb collisions at $\sqrt{s_{NN}}$= 2.76 TeV.

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Centrality dependence of normalized observables SC(4,2) and SC(3,2) in Pb-Pb collisions at 2.76 TeV, in 0-10% most central collisions.