The cumulant $c_2\{8\}$ extracted for all charged particles with $0.3 < p_T < 3.0$ GeV/c as a function of $N_{trk}^{offline}$ in pPb collisions.

The elliptic flow $v_2\{6\}$ extracted for all charged particles with $0.3 < p_T < 3.0$ GeV/c as a function of $N_{trk}^{offline}$ in PbPb collisions.

The elliptic flow $v_2\{8\}$ extracted for all charged particles with $0.3 < p_T < 3.0$ GeV/c as a function of $N_{trk}^{offline}$ in PbPb collisions.

The elliptic flow $v_2\{\text{LYZ}\}$ extracted for all charged particles with $0.3 < p_T < 3.0$ GeV/c as a function of $N_{trk}^{offline}$ in PbPb collisions.

The elliptic flow $v_2\{6\}$ extracted for all charged particles with $0.3 < p_T < 3.0$ GeV/c as a function of $N_{trk}^{offline}$ in pPb collisions.

The elliptic flow $v_2\{8\}$ extracted for all charged particles with $0.3 < p_T < 3.0$ GeV/c as a function of $N_{trk}^{offline}$ in pPb collisions.

The elliptic flow $v_2\{\text{LYZ}\}$ extracted for all charged particles with $0.3 < p_T < 3.0$ GeV/c as a function of $N_{trk}^{offline}$ in pPb collisions.

The cumulant ratio $c_2\{6\}/v_2\{4\}$ as a function of $c_2\{4\}/v_2\{2\}$ in pPb collisions.

The cumulant ratio $c_2\{8\}/v_2\{6\}$ as a function of $c_2\{4\}/v_2\{2\}$ in pPb collisions.

The cumulant ratio $c_2\{6\}/v_2\{4\}$ as a function of $c_2\{4\}/v_2\{2\}$ in PbPb collisions.

The cumulant ratio $c_2\{8\}/v_2\{6\}$ as a function of $c_2\{4\}/v_2\{2\}$ in PbPb collisions.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $K^{0}_{S}$ as a function of $p_{T}$ from the correlation in the $N_{offline}^{trk}$ < 35 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $K_{S}^{0}$ as a function of $p_{T}$ from the correlation in the 35 $\leq N_{offline}^{trk}$ < 60 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $K_{S}^{0}$ as a function of $p_{T}$ from the correlation in the 60 $\leq N_{offline}^{trk}$ < 120 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the $N_{offline}^{trk}$ < 35 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the 35 $\leq N_{offline}^{trk}$ < 60 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the 60 $\leq N_{offline}^{trk}$ < 120 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the $N_{offline}^{trk}$ < 35 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the 35 $\leq N_{offline}^{trk}$ < 60 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the 60 $\leq N_{offline}^{trk}$ < 120 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $K_{S}^{0}$ as a function of $p_{T}$ from the correlation in the $N_{offline}^{trk}$ < 35 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $K_{S}^{0}$ as a function of $p_{T}$ from the correlation in the 35 $\leq N_{offline}^{trk}$ < 60 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $K_{S}^{0}$ as a function of $p_{T}$ from the correlation in the 60 $\leq N_{offline}^{trk}$ < 120 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the $N_{offline}^{trk}$ < 35 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the 35 $\leq N_{offline}^{trk}$ < 60 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the 60 $\leq N_{offline}^{trk}$ < 120 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the 120 $\leq N_{offline}^{trk}$ < 150 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the 150 $\leq N_{offline}^{trk}$ < 185 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 220 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the 220 $\leq N_{offline}^{trk}$ < 260 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $K^{0}_{S}$ as a function of $p_{T}$ from the correlation in the 120 $\leq N_{offline}^{trk}$ < 150 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $K^{0}_{S}$ as a function of $p_{T}$ from the correlation in the 150 $\leq N_{offline}^{trk}$ < 185 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $K^{0}_{S}$ as a function of $p_{T}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 220 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $K^{0}_{S}$ as a function of $p_{T}$ from the correlation in the 220 $\leq N_{offline}^{trk}$ < 260 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the 120 $\leq N_{offline}^{trk}$ < 150 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the 150 $\leq N_{offline}^{trk}$ < 185 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 220 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the 220 $\leq N_{offline}^{trk}$ < 260 multiplicity class in pPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $K^{0}_{S}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 120 $\leq N_{offline}^{trk}$ < 150 multiplicity class in pPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $K^{0}_{S}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 150 $\leq N_{offline}^{trk}$ < 185 multiplicity class in pPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $K^{0}_{S}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 220 multiplicity class in pPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $K^{0}_{S}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 220 $\leq N_{offline}^{trk}$ < 260 multiplicity class in pPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $\Lambda/\bar{\Lambda}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 120 $\leq N_{offline}^{trk}$ < 150 multiplicity class in pPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $\Lambda/\bar{\Lambda}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 150 $\leq N_{offline}^{trk}$ < 185 multiplicity class in pPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $\Lambda/\bar{\Lambda}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 220 multiplicity class in pPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $\Lambda/\bar{\Lambda}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 220 $\leq N_{offline}^{trk}$ < 260 multiplicity class in pPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the 120 $\leq N_{offline}^{trk}$ < 150 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the 150 $\leq N_{offline}^{trk}$ < 185 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 220 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the 220 $\leq N_{offline}^{trk}$ < 260 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $K^{0}_{S}$ as a function of $p_{T}$ from the correlation in the 120 $\leq N_{offline}^{trk}$ < 150 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $K^{0}_{S}$ as a function of $p_{T}$ from the correlation in the 150 $\leq N_{offline}^{trk}$ < 185 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $K^{0}_{S}$ as a function of $p_{T}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 220 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $K^{0}_{S}$ as a function of $p_{T}$ from the correlation in the 220 $\leq N_{offline}^{trk}$ < 260 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the 120 $\leq N_{offline}^{trk}$ < 150 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the 150 $\leq N_{offline}^{trk}$ < 185 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 220 multiplicity class in PbPb.

The elliptic flow v2(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the 220 $\leq N_{offline}^{trk}$ < 260 multiplicity class in PbPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $K^{0}_{S}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 120 $\leq N_{offline}^{trk}$ < 150 multiplicity class in PbPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $K^{0}_{S}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 150 $\leq N_{offline}^{trk}$ < 185 multiplicity class in PbPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $K^{0}_{S}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 220 multiplicity class in PbPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $K^{0}_{S}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 220 $\leq N_{offline}^{trk}$ < 260 multiplicity class in PbPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $\Lambda/\bar{\Lambda}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 120 $\leq N_{offline}^{trk}$ < 150 multiplicity class in PbPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $\Lambda/\bar{\Lambda}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 150 $\leq N_{offline}^{trk}$ < 185 multiplicity class in PbPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $\Lambda/\bar{\Lambda}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 220 multiplicity class in PbPb.

The elliptic flow per constituent quark v2(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $\Lambda/\bar{\Lambda}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 220 $\leq N_{offline}^{trk}$ < 260 multiplicity class in PbPb.

The triangular flow v3(2, $|\Delta\eta| > 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 350 multiplicity class in PbPb.

The triangular flow v3(2, $|\Delta\eta| > 2$) extracted for $K^{0}_{S}$ as a function of $p_{T}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 350 multiplicity class in PbPb.

The triangular flow v3(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 350 multiplicity class in PbPb.

The triangular flow per constituent quark v3(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $K^{0}_{S}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 350 multiplicity class in PbPb.

The triangular flow per constituent quark v3(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $\Lambda/\bar{\Lambda}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 350 multiplicity class in PbPb.

The triangular flow v3(2, $|\Delta\eta| > 2$) extracted for all charged particles as a function of $p_{T}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 350 multiplicity class in pPb.

The triangular flow v3(2, $|\Delta\eta| > 2$) extracted for $K^{0}_{S}$ as a function of $p_{T}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 350 multiplicity class in pPb.

The triangular flow v3(2, $|\Delta\eta| > 2$) extracted for $\Lambda/\bar{\Lambda}$ as a function of $p_{T}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 350 multiplicity class in pPb.

The triangular flow per constituent quark v3(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $K^{0}_{S}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 350 multiplicity class in pPb.

The triangular flow per constituent quark v3(2, $|\Delta\eta| > 2$)/$n_{q}$ extracted for $\Lambda/\bar{\Lambda}$ as a function of transverse kinetic energy per constituent quark $KE_{T}/n_{q}$ from the correlation in the 185 $\leq N_{offline}^{trk}$ < 350 multiplicity class in pPb.

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.

The Fourier coefficient V_n,n vs. |Delta(ETARAP)| for individual n values.

The Fourier coefficient V_n vs. |Delta(ETARAP)| from the 2PC anaysis for individual n values from 2 to n.

The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 0 TO 5%.

The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 5 TO 10%.

The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 10 TO 20%.

The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 20 TO 30%.

The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 30 TO 40%.

The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 40 TO 50%.

The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 50 TO 60%.

The Fourier coefiiciant V_n vs eta for PT 0.5 TO 1 GeV and centrality 60 TO 70%.

The Fourier coefiiciant V_n vs eta for PT 1 TO 2 GeV and centrality 0 TO 5%.

The Fourier coefiiciant V_n vs eta for PT 1 TO 2 GeV and centrality 5 TO 10%.

The Fourier coefiiciant V_n vs eta for PT 1 TO 2 GeV and centrality 10 TO 20%.

The Fourier coefiiciant V_n vs eta for PT 1 TO 2 GeV and centrality 20 TO 30%.

The Fourier coefiiciant V_n vs eta for PT 1 TO 2 GeV and centrality 30 TO 40%.

The Fourier coefiiciant V_n vs eta for PT 1 TO 2 GeV and centrality 40 TO 50%.

The Fourier coefiiciant V_n vs eta for PT 1 TO 2 GeV and centrality 50 TO 60%.

The Fourier coefiiciant V_n vs eta for PT 1 TO 2 GeV and centrality 60 TO 70%.

The Fourier coefiiciant V_n vs eta for PT 2 TO 3 GeV and centrality 0 TO 5%.

The Fourier coefiiciant V_n vs eta for PT 2 TO 3 GeV and centrality 5 TO 10%.

The Fourier coefiiciant V_n vs eta for PT 2 TO 3 GeV and centrality 10 TO 20%.

The Fourier coefiiciant V_n vs eta for PT 2 TO 3 GeV and centrality 20 TO 30%.

The Fourier coefiiciant V_n vs eta for PT 2 TO 3 GeV and centrality 30 TO 40%.

The Fourier coefiiciant V_n vs eta for PT 2 TO 3 GeV and centrality 40 TO 50%.

The Fourier coefiiciant V_n vs eta for PT 2 TO 3 GeV and centrality 50 TO 60%.

The Fourier coefiiciant V_n vs eta for PT 2 TO 3 GeV and centrality 60 TO 70%.

The Fourier coefiiciant V_n vs eta for PT 3 TO 4 GeV and centrality 0 TO 5%.

The Fourier coefiiciant V_n vs eta for PT 3 TO 4 GeV and centrality 5 TO 10%.

The Fourier coefiiciant V_n vs eta for PT 3 TO 4 GeV and centrality 10 TO 20%.

The Fourier coefiiciant V_n vs eta for PT 3 TO 4 GeV and centrality 20 TO 30%.

The Fourier coefiiciant V_n vs eta for PT 3 TO 4 GeV and centrality 30 TO 40%.

The Fourier coefiiciant V_n vs eta for PT 3 TO 4 GeV and centrality 40 TO 50%.

The Fourier coefiiciant V_n vs eta for PT 3 TO 4 GeV and centrality 50 TO 60%.

The Fourier coefiiciant V_n vs eta for PT 3 TO 4 GeV and centrality 60 TO 70%.

The Fourier coefiiciant V_n vs eta for PT 4 TO 8 GeV and centrality 0 TO 5%.

The Fourier coefiiciant V_n vs eta for PT 4 TO 8 GeV and centrality 5 TO 10%.

The Fourier coefiiciant V_n vs eta for PT 4 TO 8 GeV and centrality 10 TO 20%.

The Fourier coefiiciant V_n vs eta for PT 4 TO 8 GeV and centrality 20 TO 30%.

The Fourier coefiiciant V_n vs eta for PT 4 TO 8 GeV and centrality 30 TO 40%.

The Fourier coefiiciant V_n vs eta for PT 4 TO 8 GeV and centrality 40 TO 50%.

The Fourier coefiiciant V_n vs eta for PT 4 TO 8 GeV and centrality 50 TO 60%.

The Fourier coefiiciant V_n vs eta for PT 4 TO 8 GeV and centrality 60 TO 70%.

V_n vs PT for centrality 0 TO 5%.

V_n vs PT for centrality 5 TO 10%.

V_n vs PT for centrality 10 TO 20%.

V_n vs PT for centrality 20 TO 30%.

V_n vs PT for centrality 30 TO 40%.

V_n vs PT for centrality 40 TO 50%.

V_n vs PT for centrality 50 TO 60%.

V_n vs PT for centrality 60 TO 70%.

V_n vs Centrality for PT 1 TO 2 GeV.

V_n vs Centrality for PT 2 TO 3 GeV.

V_n vs Centrality for PT 3 TO 4 GeV.

V_n vs Centrality for PT 4 TO 8 GeV.

V_n vs Centrality for PT 8 TO 12 GeV.

V_n vs Centrality for PT 12 TO 20 GeV.

2PC.V_n vs n for Centrality 0 TO 1 %.

2PC.V_n vs n for Centrality 0 TO 5 %.

2PC.V_n vs n for Centrality 5 TO 10 %.

2PC.V_n vs n for Centrality 0 TO 10 %.

2PC.V_n vs n for Centrality 10 TO 20 %.

2PC.V_n vs n for Centrality 20 TO 30 %.

2PC.V_n vs n for Centrality 30 TO 40 %.

2PC.V_n vs n for Centrality 40 TO 50 %.

2PC.V_n vs n for Centrality 50 TO 60 %.

2PC.V_n vs n for Centrality 60 TO 70 %.

2PC.V_n vs n for Centrality 70 TO 80 %.

V_nn vs n for Centrality 0 TO 1 %.

V_nn vs n for Centrality 0 TO 5 %.

V_nn vs n for Centrality 5 TO 10 %.

V_nn vs n for Centrality 0 TO 10 %.

V_nn vs n for Centrality 10 TO 20 %.

V_nn vs n for Centrality 20 TO 30 %.

V_nn vs n for Centrality 30 TO 40 %.

V_nn vs n for Centrality 40 TO 50 %.

V_nn vs n for Centrality 50 TO 60 %.

V_nn vs n for Centrality 60 TO 70 %.

V_nn vs n for Centrality 70 TO 80 %.

correlation funcitons in various pT bins.

correlation funcitons in various pT bins.

correlation funcitons in various pT bins.

correlation funcitons in various pT bins.

v_{1,1} vs eta for different combinations of pTa and pTb. Figure 18.

v_{1,1} vs eta for different combinations of pTa and pTb. Figure 18.

v_{1,1} vs eta for different combinations of pTa and pTb. Figure 18.

v_{1,1} vs eta for different combinations of pTa and pTb. Figure 18.

v_{1} vs pT for different centrality selections, Figure 21.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_n extracted from 2PC method utilizing the factorization relation.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v_ vs pta for various centrality pta combinations.

v2(pT) for centrality interval 30-40% and |eta| <1.

v2(pT) for centrality interval 40-50% and |eta| <1.

v2(pT) for centrality interval 50-60% and |eta| <1.

v2(pT) for centrality interval 60-70% and |eta| <1.

v2(pT) for centrality interval 70-80% and |eta| <1.

v2(pT) for centrality interval 0-10% and 1< |eta| <2.

v2(pT) for centrality interval 10-20% and 1< |eta| <2.

v2(pT) for centrality interval 20-30% and 1< |eta| <2.

v2(pT) for centrality interval 30-40% and 1< |eta| <2.

v2(pT) for centrality interval 40-50% and 1< |eta| <2.

v2(pT) for centrality interval 50-60% and 1< |eta| <2.

v2(pT) for centrality interval 60-70% and 1< |eta| <2.

v2(pT) for centrality interval 70-80% and 1< |eta| <2.

v2(pT) for centrality interval 0-10% and 2< |eta| <2.5.

v2(pT) for centrality interval 10-20% and 2< |eta| <2.5.

v2(pT) for centrality interval 20-30% and 2< |eta| <2.5.

v2(pT) for centrality interval 30-40% and 2< |eta| <2.5.

v2(pT) for centrality interval 40-50% and 2< |eta| <2.5.

v2(pT) for centrality interval 50-60% and 2< |eta| <2.5.

v2(pT) for centrality interval 60-70% and 2< |eta| <2.5.

v2(pT) for centrality interval 70-80% and 2< |eta| <2.5.

v2(eta) for centrality interval 0-10% and 0.5< pT <0.7 GeV.

v2(eta) for centrality interval 10-20% and 0.5< pT <0.7 GeV.

v2(eta) for centrality interval 20-30% and 0.5< pT <0.7 GeV.

v2(eta) for centrality interval 30-40% and 0.5< pT <0.7 GeV.

v2(eta) for centrality interval 40-50% and 0.5< pT <0.7 GeV.

v2(eta) for centrality interval 50-60% and 0.5< pT <0.7 GeV.

v2(eta) for centrality interval 60-70% and 0.5< pT <0.7 GeV.

v2(eta) for centrality interval 70-80% and 0.5< pT <0.7 GeV.

v2(eta) for centrality interval 0-10% and 0.8< pT <1.2 GeV.

v2(eta) for centrality interval 10-20% and 0.8< pT <1.2 GeV.

v2(eta) for centrality interval 20-30% and 0.8< pT <1.2 GeV.

v2(eta) for centrality interval 30-40% and 0.8< pT <1.2 GeV.

v2(eta) for centrality interval 40-50% and 0.8< pT <1.2 GeV.

v2(eta) for centrality interval 50-60% and 0.8< pT <1.2 GeV.

v2(eta) for centrality interval 60-70% and 0.8< pT <1.2 GeV.

v2(eta) for centrality interval 70-80% and 0.8< pT <1.2 GeV.

v2(eta) for centrality interval 0-10% and 2< pT <4 GeV.

v2(eta) for centrality interval 10-20% and 2< pT <4 GeV.

v2(eta) for centrality interval 20-30% and 2< pT <4 GeV.

v2(eta) for centrality interval 30-40% and 2< pT <4 GeV.

v2(eta) for centrality interval 40-50% and 2< pT <4 GeV.

v2(eta) for centrality interval 50-60% and 2< pT <4 GeV.

v2(eta) for centrality interval 60-70% and 2< pT <4 GeV.

v2(eta) for centrality interval 70-80% and 2< pT <4 GeV.

v2(eta) for centrality interval 0-10% and 4< pT <7 GeV.

v2(eta) for centrality interval 10-20% and 4< pT <7 GeV.

v2(eta) for centrality interval 20-30% and 4< pT <7 GeV.

v2(eta) for centrality interval 30-40% and 4< pT <7 GeV.

v2(eta) for centrality interval 40-50% and 4< pT <7 GeV.

v2(eta) for centrality interval 50-60% and 4< pT <7 GeV.

v2(eta) for centrality interval 60-70% and 4< pT <7 GeV.

v2(eta) for centrality interval 70-80% and 4< pT <7 GeV.

v2(eta) for centrality interval 0-10% and 9< pT <20 GeV.

v2(eta) for centrality interval 10-20% and 9< pT <20 GeV.

v2(eta) for centrality interval 20-30% and 9< pT <20 GeV.

v2(eta) for centrality interval 30-40% and 9< pT <20 GeV.

v2(eta) for centrality interval 40-50% and 9< pT <20 GeV.

v2(eta) for centrality interval 50-60% and 9< pT <20 GeV.

v2(eta) for centrality interval 60-70% and 9< pT <20 GeV.

v2(eta) for centrality interval 70-80% and 9< pT <20 GeV.