Differential cross section (multiplied by the dimuon branching fraction) of prompt J/$\psi$ mesons in pPb collisions at backward $y_{\mathrm{CM}}$.

Rapidity dependence of the cross section (multiplied by the dimuon branching fraction) for prompt J/$\psi$ mesons in the $p_{\mathrm{T}}$ intervals 6.5<$p_{\mathrm{T}}$<10 GeV and 10<$p_{\mathrm{T}}$<30 GeV in pp collisions.

Rapidity dependence of the cross section (multiplied by the dimuon branching fraction) for prompt J/$\psi$ mesons in the $p_{\mathrm{T}}$ intervals 6.5<$p_{\mathrm{T}}$<10 GeV and 10<$p_{\mathrm{T}}$<30 GeV in pPb collisions.

Transverse momentum dependence of $R_{\mathrm{pPb}}$ for prompt J/$\psi$ mesons in seven $y_{\mathrm{CM}}$ ranges.

Rapidity dependence of $R_{\mathrm{pPb}}$ for prompt J/$\psi$ mesons in $p_{\mathrm{T}}$ range 6.5<$p_{\mathrm{T}}$<10 GeV.

Rapidity dependence of $R_{\mathrm{pPb}}$ for prompt J/$\psi$ mesons in $p_{\mathrm{T}}$ range 10<$p_{\mathrm{T}}$<30 GeV.

Transverse momentum dependence of $R_{\mathrm{FB}}$ for prompt J/$\psi$ mesons in the 0<$y_{\mathrm{CM}}$<0.9 range.

Transverse momentum dependence of $R_{\mathrm{FB}}$ for prompt J/$\psi$ mesons in the 0.9<$y_{\mathrm{CM}}$<1.5 range.

Transverse momentum dependence of $R_{\mathrm{FB}}$ for prompt J/$\psi$ mesons in the 1.5<$y_{\mathrm{CM}}$<1.93 range.

Dependence of $R_{\mathrm{FB}}$ for prompt J/$\psi$ mesons on the hadronic activity in the event, given by the transverse energy deposited in the CMS detector at large pseudorapidities $E_{\mathrm{T}}^{\mathrm{HF}|\eta|>4}$.

Differential cross section (multiplied by the dimuon branching fraction) of nonprompt J/$\psi$ mesons in pp collisions at forward $y_{\mathrm{CM}}$.

Differential cross section (multiplied by the dimuon branching fraction) of nonprompt J/$\psi$ mesons in pp collisions at backward $y_{\mathrm{CM}}$.

Differential cross section (multiplied by the dimuon branching fraction) of nonprompt J/$\psi$ mesons in pPb collisions at forward $y_{\mathrm{CM}}$.

Differential cross section (multiplied by the dimuon branching fraction) of nonprompt J/$\psi$ mesons in pPb collisions at backward $y_{\mathrm{CM}}$.

Rapidity dependence of the cross section (multiplied by the dimuon branching fraction) for nonprompt J/$\psi$ mesons in the $p_{\mathrm{T}}$ intervals 6.5<$p_{\mathrm{T}}$<10 GeV and 10<$p_{\mathrm{T}}$<30 GeV in pp collisions.

Rapidity dependence of the cross section (multiplied by the dimuon branching fraction) for nonprompt J/$\psi$ mesons in the $p_{\mathrm{T}}$ intervals 6.5<$p_{\mathrm{T}}$<10 GeV and 10<$p_{\mathrm{T}}$<30 GeV in pPb collisions.

Transverse momentum dependence of $R_{\mathrm{pPb}}$ for nonprompt J/$\psi$ mesons in seven $y_{\mathrm{CM}}$ ranges.

Rapidity dependence of $R_{\mathrm{pPb}}$ for nonprompt J/$\psi$ mesons in $p_{\mathrm{T}}$ range 6.5<$p_{\mathrm{T}}$<10 GeV.

Rapidity dependence of $R_{\mathrm{pPb}}$ for nonprompt J/$\psi$ mesons in $p_{\mathrm{T}}$ range 10<$p_{\mathrm{T}}$<30 GeV.

Transverse momentum dependence of $R_{\mathrm{FB}}$ for nonprompt J/$\psi$ mesons in the 0<$y_{\mathrm{CM}}$<0.9 range.

Transverse momentum dependence of $R_{\mathrm{FB}}$ for nonprompt J/$\psi$ mesons in the 0.9<$y_{\mathrm{CM}}$<1.5 range.

Transverse momentum dependence of $R_{\mathrm{FB}}$ for nonprompt J/$\psi$ mesons in the 1.5<$y_{\mathrm{CM}}$<1.93 range.

Dependence of $R_{\mathrm{FB}}$ for nonprompt J/$\psi$ mesons on the hadronic activity in the event, given by the transverse energy deposited in the CMS detector at large pseudorapidities $E_{\mathrm{T}}^{\mathrm{HF}|\eta|>4}$.

Unfolded groomed jet radius distribution in PbPb normalized to the number of jets that pass the $x_J$>0.4 selection. All systematic uncertainties are bin-to-bin fully correlated (allowing for sign-changes bin-to-bin).The covaraince matrices are provided for the statistical uncertainties from data and MC in this HepData record.The negative (-0.05,0) bin accounts for jets that failed the soft-drop grooming condition.

Covariance matrix of the statistical uncertainty in data for the unfolded groomed jet radius distribution in PbPb for jets that pass the $x_J$>0.4 selection.The bin indices correspond to the bins used in the groomed jet radius distribution.

Covariance matrix of the statistical uncertainty in MC for the unfolded groomed jet radius distribution in PbPb for jets that pass the $x_J$>0.4 selection.The bin indices correspond to the bins used in the groomed jet radius distribution.

Unfolded jet girth distribution in PbPb normalized to the number of jets that pass the $x_J$>0.8 selection. All systematic uncertainties are bin-to-bin fully correlated (allowing for sign-changes bin-to-bin).The covaraince matrices are provided for the statistical uncertainties from data and MC in this HepData record.

Covariance matrix of the statistical uncertainty in data for the unfolded jet girth distribution in PbPb for jets that pass the $x_J$>0.4 selection.The bin indices correspond to the bins used in the jet girth distribution.

Covariance matrix of the statistical uncertainty in MC for the unfolded jet girth distribution in PbPb for jets that pass the $x_J$>0.8 selection.The bin indices correspond to the bins used in the jet girth distribution.

Unfolded groomed jet radius distribution in PbPb normalized to the number of jets that pass the $x_J$>0.8 selection. All systematic uncertainties are bin-to-bin fully correlated (allowing for sign-changes bin-to-bin).The covaraince matrices are provided for the statistical uncertainties from data and MC in this HepData record.The negative (-0.05,0) bin accounts for jets that failed the soft-drop grooming condition.

Covariance matrix of the statistical uncertainty in data for the unfolded groomed jet radius distribution in PbPb for jets that pass the $x_J$>0.8 selection.The bin indices correspond to the bins used in the groomed jet radius distribution.

Covariance matrix of the statistical uncertainty in MC for the unfolded groomed jet radius distribution in PbPb for jets that pass the $x_J$>0.8 selection.The bin indices correspond to the bins used in the groomed jet radius distribution.

Unfolded jet girth distribution in pp normalized to the number of jets that pass the $x_J$>0.4 selection. All systematic uncertainties are bin-to-bin fully correlated (allowing for sign-changes bin-to-bin).The covaraince matrices are provided for the statistical uncertainties from data and MC in this HepData record.

Covariance matrix of the statistical uncertainty in data for the unfolded jet girth distribution in pp for jets that pass the $x_J$>0.4 selection.The bin indices correspond to the bins used in the jet girth distribution.

Covariance matrix of the statistical uncertainty in MC for the unfolded jet girth distribution in pp for jets that pass the $x_J$>0.4 selection.The bin indices correspond to the bins used in the jet girth distribution.

Unfolded groomed jet radius distribution in pp normalized to the number of jets that pass the $x_J$>0.4 selection. All systematic uncertainties are bin-to-bin fully correlated (allowing for sign-changes bin-to-bin).The covaraince matrices are provided for the statistical uncertainties from data and MC in this HepData record.The negative (-0.05,0) bin accounts for jets that failed the soft-drop grooming condition.

Covariance matrix of the statistical uncertainty in data for the unfolded groomed jet radius distribution in pp for jets that pass the $x_J$>0.4 selection.The bin indices correspond to the bins used in the groomed jet radius distribution.

Covariance matrix of the statistical uncertainty in MC for the unfolded groomed jet radius distribution in pp for jets that pass the $x_J$>0.4 selection.The bin indices correspond to the bins used in the groomed jet radius distribution.

Unfolded jet girth distribution in pp normalized to the number of jets that pass the $x_J$>0.8 selection. All systematic uncertainties are bin-to-bin fully correlated (allowing for sign-changes bin-to-bin).The covaraince matrices are provided for the statistical uncertainties from data and MC in this HepData record.

Covariance matrix of the statistical uncertainty in data for the unfolded jet girth distribution in pp for jets that pass the $x_J$>0.8 selection.The bin indices correspond to the bins used in the jet girth distribution.

Covariance matrix of the statistical uncertainty in MC for the unfolded jet girth distribution in pp for jets that pass the $x_J$>0.8 selection.The bin indices correspond to the bins used in the jet girth distribution.

Unfolded groomed jet radius distribution in pp normalized to the number of jets that pass the $x_J$>0.8 selection. All systematic uncertainties are bin-to-bin fully correlated (allowing for sign-changes bin-to-bin).The covaraince matrices are provided for the statistical uncertainties from data and MC in this HepData record.The negative (-0.05,0) bin accounts for jets that failed the soft-drop grooming condition.

Covariance matrix of the statistical uncertainty in data for the unfolded groomed jet radius distribution in pp for jets that pass the $x_J$>0.8 selection.The bin indices correspond to the bins used in the groomed jet radius distribution.

Covariance matrix of the statistical uncertainty in MC for the unfolded groomed jet radius distribution in pp for jets that pass the $x_J$>0.8 selection.The bin indices correspond to the bins used in the groomed jet radius distribution.

Ratio of yields in PbPb to pp for the unfolded jet girth distribution normalized to the number of jets that pass the $x_J$>0.4 selection. Each uncertainty is symmetrized and added in quadrature.All systematic uncertainties have been obtained assuming the PbPb and pp uncertainties are uncorrelated.

Ratio of yields in PbPb to pp for the unfolded groomed jet radius distribution normalized to the number of jets that pass the $x_J$>0.4 selection. Each uncertainty is symmetrized and added in quadrature.All systematic uncertainties have been obtained assuming the PbPb and pp uncertainties are uncorrelated.The negative (-0.05,0) bin accounts for jets that failed the soft-drop grooming condition.

Ratio of yields in PbPb to pp for the unfolded jet girth distribution normalized to the number of jets that pass the $x_J$>0.8 selection. Each uncertainty is symmetrized and added in quadrature.All systematic uncertainties have been obtained assuming the PbPb and pp uncertainties are uncorrelated.

Ratio of yields in PbPb to pp for the unfolded groomed jet radius distribution normalized to the number of jets that pass the $x_J$>0.8 selection. Each uncertainty is symmetrized and added in quadrature.All systematic uncertainties have been obtained assuming the PbPb and pp uncertainties are uncorrelated.The negative (-0.05,0) bin accounts for jets that failed the soft-drop grooming condition.

Distributions of $\Delta\phi_{\mathrm{trk,Z}}$ in 30-50% centrality PbPb collisions at 5.02 TeV.

Distributions of $\Delta\phi_{\mathrm{trk,Z}}$ in 0-30% centrality PbPb collisions at 5.02 TeV.

PbPb - pp difference of $\Delta\phi_{\mathrm{trk,Z}}$ distributions for 70-90% centrality PbPb collisions at 5.02 TeV.

PbPb - pp difference of $\Delta\phi_{\mathrm{trk,Z}}$ distributions for 50-70% centrality PbPb collisions at 5.02 TeV.

PbPb - pp difference of $\Delta\phi_{\mathrm{trk,Z}}$ distributions for 30-50% centrality PbPb collisions at 5.02 TeV.

PbPb - pp difference of $\Delta\phi_{\mathrm{trk,Z}}$ distributions for 0-30% centrality PbPb collisions at 5.02 TeV.

Distributions of $\xi^{\mathrm{trk,Z}}_{\mathrm{T}}$ in pp collisions at 5.02 TeV.

Distributions of $\xi^{\mathrm{trk,Z}}_{\mathrm{T}}$ in 70-90% centrality PbPb collisions at 5.02 TeV.

Distributions of $\xi^{\mathrm{trk,Z}}_{\mathrm{T}}$ in 50-70% centrality PbPb collisions at 5.02 TeV.

Distributions of $\xi^{\mathrm{trk,Z}}_{\mathrm{T}}$ in 30-50% centrality PbPb collisions at 5.02 TeV.

Distributions of $\xi^{\mathrm{trk,Z}}_{\mathrm{T}}$ in 0-30% centrality PbPb collisions at 5.02 TeV.

PbPb / pp ratio of $\xi^{\mathrm{trk,Z}}_{\mathrm{T}}$ distributions for 70-90% centrality PbPb collisions at 5.02 TeV.

PbPb / pp ratio of $\xi^{\mathrm{trk,Z}}_{\mathrm{T}}$ distributions for 50-70% centrality PbPb collisions at 5.02 TeV.

PbPb / pp ratio of $\xi^{\mathrm{trk,Z}}_{\mathrm{T}}$ distributions for 30-50% centrality PbPb collisions at 5.02 TeV.

PbPb / pp ratio of $\xi^{\mathrm{trk,Z}}_{\mathrm{T}}$ distributions for 0-30% centrality PbPb collisions at 5.02 TeV.

Distributions of p$^{\mathrm{trk}}_{\mathrm{T}}$ in pp collisions at 5.02 TeV.

Distributions of p$^{\mathrm{trk}}_{\mathrm{T}}$ in pp collisions at 5.02 TeV.

Distributions of p$^{\mathrm{trk}}_{\mathrm{T}}$ in 70-90% centrality PbPb collisions at 5.02 TeV.

Distributions of p$^{\mathrm{trk}}_{\mathrm{T}}$ in 50-70% centrality PbPb collisions at 5.02 TeV.

Distributions of p$^{\mathrm{trk}}_{\mathrm{T}}$ in 30-50% centrality PbPb collisions at 5.02 TeV.

Distributions of p$^{\mathrm{trk}}_{\mathrm{T}}$ in 0-30% centrality PbPb collisions at 5.02 TeV.

PbPb / pp ratio of p$^{\mathrm{trk}}_{\mathrm{T}}$ distributions for 70-90% centrality PbPb collisions at 5.02 TeV.

PbPb / pp ratio of p$^{\mathrm{trk}}_{\mathrm{T}}$ distributions for 50-70% centrality PbPb collisions at 5.02 TeV.

PbPb / pp ratio of p$^{\mathrm{trk}}_{\mathrm{T}}$ distributions for 30-50% centrality PbPb collisions at 5.02 TeV.

PbPb / pp ratio of p$^{\mathrm{trk}}_{\mathrm{T}}$ distributions for 0-30% centrality PbPb collisions at 5.02 TeV.

Invariant charged particle differential yield in the centrality regions 30 TO 50%, 50 TO 70% and 70 TO 90%.

Nuclear modification factor RAA in the centrality regions 0 TO 5%, 5 TO 10% and 10 TO 30%.

Nuclear modification factor RAA in the centrality regions 30 TO 50%, 50 TO 70% and 70 TO 90%.

TAA-scaled ratio of PT spectra in central and peripheral bins, RCP.

Nuclear modification factor RAA as a function of ET.

The measured nuclear modification factor as functions of the PB PB centrality given by Npart.

The measured nuclear modification factor as functions of the PB PB centrality given by Npart.

The b-jet yield as a function of pT is for the 30-50% centrality class of PbPb collisions. The yields are scaled by the equivalent number of minimum bias events sampled and by TAA.

The b-jet yield as a function of pT is for the 50-100% centrality class of PbPb collisions. The yields are scaled by the equivalent number of minimum bias events sampled and by TAA.

The b-jet cross section as a function of pT in pp collisions.

The b-jet nuclear modification factor as a function of the pT for the centrality class 0-100%.

The b-jet nuclear modification factor as a function of centrality for 80 < jet pT < 90 GeV/c.

The b-jet nuclear modification factor as a function centrality for 80 < jet pT < 90 GeV/c.

The b-jet nuclear modification factor as a function of the pT for the centrality class 0-10%.

The b-jet nuclear modification factor as a function of the pT for the centrality class 10-30%.

The b-jet nuclear modification factor as a function of the pT for the centrality class 30-50%.

The b-jet nuclear modification factor as a function of the pT for the centrality class 50-100%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 15-20%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 20-25%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 25-30%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 30-35%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 35-40%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 40-50%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 50-60%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 60-70%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 70-80%.

Measurements of the second-order elliptic anisotropy parameter using the cumulant method, V2(C2) v PT for the centrality range 0-5%.

Measurements of the second-order elliptic anisotropy parameter using the cumulant method, V2(C2) v PT for the centrality range 5-10%.

Measurements of the second-order elliptic anisotropy parameter using the cumulant method, V2(C2) v PT for the centrality range 10-15%.

Measurements of the second-order elliptic anisotropy parameter using the cumulant method, V2(C2) v PT for the centrality range 15-20%.

Measurements of the second-order elliptic anisotropy parameter using the cumulant method, V2(C2) v PT for the centrality range 20-25%.

Measurements of the second-order elliptic anisotropy parameter using the cumulant method, V2(C2) v PT for the centrality range 25-30%.

Measurements of the second-order elliptic anisotropy parameter using the cumulant method, V2(C2) v PT for the centrality range 30-35%.

Measurements of the second-order elliptic anisotropy parameter using the cumulant method, V2(C2) v PT for the centrality range 35-40%.

Measurements of the second-order elliptic anisotropy parameter using the cumulant method, V2(C2) v PT for the centrality range 40-50%.

Measurements of the second-order elliptic anisotropy parameter using the cumulant method, V2(C2) v PT for the centrality range 50-60%.

Measurements of the second-order elliptic anisotropy parameter using the cumulant method, V2(C2) v PT for the centrality range 60-70%.

Measurements of the second-order elliptic anisotropy parameter using the cumulant method, V2(C2) v PT for the centrality range 70-80%.

Measurements of the fourth-order elliptic anisotropy parameter using the cumulant method, V2(C4) v PT for the centrality range 5-10%.

Measurements of the fourth-order elliptic anisotropy parameter using the cumulant method, V2(C4) v PT for the centrality range 10-15%.

Measurements of the fourth-order elliptic anisotropy parameter using the cumulant method, V2(C4) v PT for the centrality range 15-20%.

Measurements of the fourth-order elliptic anisotropy parameter using the cumulant method, V2(C4) v PT for the centrality range 20-25%.

Measurements of the fourth-order elliptic anisotropy parameter using the cumulant method, V2(C4) v PT for the centrality range 25-30%.

Measurements of the fourth-order elliptic anisotropy parameter using the cumulant method, V2(C4) v PT for the centrality range 30-35%.

Measurements of the fourth-order elliptic anisotropy parameter using the cumulant method, V2(C4) v PT for the centrality range 35-40%.

Measurements of the fourth-order elliptic anisotropy parameter using the cumulant method, V2(C4) v PT for the centrality range 40-50%.

Measurements of the fourth-order elliptic anisotropy parameter using the cumulant method, V2(C4) v PT for the centrality range 50-60%.

Measurements of the fourth-order elliptic anisotropy parameter using the cumulant method, V2(C4) v PT for the centrality range 60-70%.

Measurements of the elliptic anisotropy parameter using the Lee-Yang zeros method, V2(LYZ) v PT for the centrality range 5-10%.

Measurements of the elliptic anisotropy parameter using the Lee-Yang zeros method, V2(LYZ) v PT for the centrality range 10-15%.

Measurements of the elliptic anisotropy parameter using the Lee-Yang zeros method, V2(LYZ) v PT for the centrality range 15-20%.

Measurements of the elliptic anisotropy parameter using the Lee-Yang zeros method, V2(LYZ) v PT for the centrality range 20-25%.

Measurements of the elliptic anisotropy parameter using the Lee-Yang zeros method, V2(LYZ) v PT for the centrality range 25-30%.

Measurements of the elliptic anisotropy parameter using the Lee-Yang zeros method, V2(LYZ) v PT for the centrality range 30-35%.

Measurements of the elliptic anisotropy parameter using the Lee-Yang zeros method, V2(LYZ) v PT for the centrality range 35-40%.

Measurements of the elliptic anisotropy parameter using the Lee-Yang zeros method, V2(LYZ) v PT for the centrality range 40-50%.

Integrtated V2 as a function of centrality.

Pseudorapidity dependence of V2 for centrality 0-5%.

Pseudorapidity dependence of V2 for centrality 5-10%.

Pseudorapidity dependence of V2 for centrality 10-15%.

Pseudorapidity dependence of V2 for centrality 15-20%.

Pseudorapidity dependence of V2 for centrality 20-25%.

Pseudorapidity dependence of V2 for centrality 25-30%.

Pseudorapidity dependence of V2 for centrality 30-35%.

Pseudorapidity dependence of V2 for centrality 35-40%.

Pseudorapidity dependence of V2 for centrality 40-50%.

Pseudorapidity dependence of V2 for centrality 50-60%.

Pseudorapidity dependence of V2 for centrality 60-70%.

Pseudorapidity dependence of V2 for centrality 70-80%.

PT dependence of V2(EP) for centrality 0-5% and |eta| ranges 0.0-0.4, 0.4-0.8 and 0.8-1.2.

PT dependence of V2(EP) for centrality 0-5% and |eta| ranges 1.2-1.6, 1.6-2.0 and 2.0-2.4.

PT dependence of V2(EP) for centrality 5-10% and |eta| ranges 0.0-0.4, 0.4-0.8 and 0.8-1.2.

PT dependence of V2(EP) for centrality 5-10% and |eta| ranges 1.2-1.6, 1.6-2.0 and 2.0-2.4.

PT dependence of V2(EP) for centrality 10-15% and |eta| ranges 0.0-0.4, 0.4-0.8 and 0.8-1.2.

PT dependence of V2(EP) for centrality 10-15% and |eta| ranges 1.2-1.6, 1.6-2.0 and 2.0-2.4.

PT dependence of V2(EP) for centrality 15-20% and |eta| ranges 0.0-0.4, 0.4-0.8 and 0.8-1.2.

PT dependence of V2(EP) for centrality 15-20% and |eta| ranges 1.2-1.6, 1.6-2.0 and 2.0-2.4.

PT dependence of V2(EP) for centrality 20-25% and |eta| ranges 0.0-0.4, 0.4-0.8 and 0.8-1.2.

PT dependence of V2(EP) for centrality 20-25% and |eta| ranges 1.2-1.6, 1.6-2.0 and 2.0-2.4.

PT dependence of V2(EP) for centrality 25-30% and |eta| ranges 0.0-0.4, 0.4-0.8 and 0.8-1.2.

PT dependence of V2(EP) for centrality 25-30% and |eta| ranges 1.2-1.6, 1.6-2.0 and 2.0-2.4.

PT dependence of V2(EP) for centrality 30-35% and |eta| ranges 0.0-0.4, 0.4-0.8 and 0.8-1.2.

PT dependence of V2(EP) for centrality 30-35% and |eta| ranges 1.2-1.6, 1.6-2.0 and 2.0-2.4.

PT dependence of V2(EP) for centrality 35-40% and |eta| ranges 0.0-0.4, 0.4-0.8 and 0.8-1.2.

PT dependence of V2(EP) for centrality 35-40% and |eta| ranges 1.2-1.6, 1.6-2.0 and 2.0-2.4.

PT dependence of V2(EP) for centrality 40-50% and |eta| ranges 0.0-0.4, 0.4-0.8 and 0.8-1.2.

PT dependence of V2(EP) for centrality 40-50% and |eta| ranges 1.2-1.6, 1.6-2.0 and 2.0-2.4.

PT dependence of V2(EP) for centrality 50-60% and |eta| ranges 0.0-0.4, 0.4-0.8 and 0.8-1.2.

PT dependence of V2(EP) for centrality 50-60% and |eta| ranges 1.2-1.6, 1.6-2.0 and 2.0-2.4.

PT dependence of V2(EP) for centrality 60-70% and |eta| ranges 0.0-0.4, 0.4-0.8 and 0.8-1.2.

PT dependence of V2(EP) for centrality 60-70% and |eta| ranges 1.2-1.6, 1.6-2.0 and 2.0-2.4.

PT dependence of V2(EP) for centrality 70-80% and |eta| ranges 0.0-0.4, 0.4-0.8 and 0.8-1.2.

PT dependence of V2(EP) for centrality 70-80% and |eta| ranges 1.2-1.6, 1.6-2.0 and 2.0-2.4.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 0-10%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 10-20%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 20-30%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 30-40%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 40-50%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 50-60%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 60-70%.

Measurements of the elliptic anisotropy parameter using the event-plane method, V2(EP) v PT for the centrality range 70-80%.

Measurements of the second- and fourth-order elliptic anisotropy parameters using the cumulant method v PT for the centrality range 20-60%.

Integrated V2 value extrapolated to PT=0 for the 20-30% centrality range using the event-plane method. Error is combined statistical and systematic.

Integrated V2 values from the event-plane method divided by the participant eccentricity (EPSILON) as a function of the number of participating nucleons (NPART) for the |eta| range <0.8 and PT range 0-3 GeV. Also shown are the correspnding centrality bin ranges.

Eccentricity-scaled V2 as a function of the transverse charged-particle density normalised by the transverse overlap area (S).

The dependence of V2 from the event-plane method on the pseudorapidity, transformed to the rest frame of nuclei moving separately in the positive(negative) directions by adding(subtracting) the beam rapidity,YBEAM. +(-)ve values are from +(-)YBEAM.

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