The measured Z boson production cross section in pp collisions as a function of the Z boson rapidity for the dielectron decay channel.

Event centrality dependence of the $\mbox{Z}\rightarrow\mu^{+}\mu^{-}$ yields per MB event in PbPb collisions, divided by the expected average nuclear overlap function, $T_{\rm AA}$. On the horizontal axis, event centrality is depicted as the average number of participating nucleons, $N_{\rm part}$.

Event centrality dependence of the $\mbox{Z}\rightarrow e^{+}e^{-}$ yields per MB event in PbPb collisions, divided by the expected average nuclear overlap function, $T_{\rm AA}$. On the horizontal axis, event centrality is depicted as the average number of participating nucleons, $N_{\rm part}$.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson $p_{\rm T}$ for the dimuon decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson $p_{\rm T}$ for the dielectron decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson rapidity for the dimuon decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson rapidity for the dielectron decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson rapidity for the combined leptonic decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson $p_{\rm T}$ for the combined leptonic decay channel.

Event centrality dependence of the $\mbox{Z}\rightarrow l^{+}l^{-}$ yields per MB event in PbPb collisions, divided by the expected average nuclear overlap function, $T_{\rm AA}$. On the horizontal axis, event centrality is depicted as the average number of participating nucleons, $N_{\rm part}$.

The measured Z boson production cross section in pp collisions as a function of the Z boson rapidity for the combined leptonic decay channel.

The measured Z boson production cross section in pp collisions as a function of the Z boson pT for the combined leptonic decay channel in |y|<1.44.

Nuclear modification factor RAA of psi(2S) integrated over centrality, for the midrapidity and forward rapidity analysis bins.

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.

$v_{2,2}^{unsub}$ and $v_{2,2}$ as a function of $\Delta\eta$ calculated from the 2-D per-trigger yields in figure 4(a) and 4(b), respectively.

$v_{3,3}^{unsub}$ and $v_{3,3}$ as a function of $\Delta\eta$ calculated from the 2-D per-trigger yields in figure 4(a) and 4(b), respectively.

$v_{4,4}^{unsub}$ and $v_{4,4}$ as a function of $\Delta\eta$ calculated from the 2-D per-trigger yields in figure 4(a) and 4(b), respectively.

The per-trigger yield distributions $Y^{corr}(\Delta\phi)$ and $Y^{recoil}(\Delta\phi)$ for events with $N_{ch}^{rec} \geq$ 220 in the long-range region $|\Delta\eta| >$ 2.

The per-trigger yield distributions $Y^{corr}(\Delta\phi)$ and $Y^{recoil}(\Delta\phi)$ for events with $N_{ch}^{rec} \geq$ 220 in the long-range region $|\Delta\eta| >$ 2.

The per-trigger yield distributions $Y^{corr}(\Delta\phi)$ and $Y^{recoil}(\Delta\phi)$ for events with $N_{ch}^{rec} \geq$ 220 in the long-range region $|\Delta\eta| >$ 2.

The per-trigger yield distributions $Y^{corr}(\Delta\phi)$ and $Y^{recoil}(\Delta\phi)$ for events with $N_{ch}^{rec} \geq$ 220 in the long-range region $|\Delta\eta| >$ 2.

The per-trigger yield distributions $Y^{corr}(\Delta\phi)$ and $Y^{recoil}(\Delta\phi)$ for events with $N_{ch}^{rec} \geq$ 220 in the long-range region $|\Delta\eta| >$ 2.

The per-trigger yield distributions $Y^{corr}(\Delta\phi)$ and $Y^{recoil}(\Delta\phi)$ for events with $N_{ch}^{rec} \geq$ 220 in the long-range region $|\Delta\eta| >$ 2.

The per-trigger yield distributions $Y^{corr}(\Delta\phi)$ and $Y^{recoil}(\Delta\phi)$ for events with $N_{ch}^{rec} \geq$ 220 in the long-range region $|\Delta\eta| >$ 2.

Integrated per-trigger yield, $Y_{int}$, on the near-side as a function of $p_{T}^{a}$ for 1 $< p_{T}^{b} <$ 3 GeV.

Integrated per-trigger yield, $Y_{int}$, on the near-side as a function of $p_{T}^{a}$ for 1 $< p_{T}^{b} <$ 3 GeV.

Integrated per-trigger yield, $Y_{int}$, on the near-side as a function of $p_{T}^{a}$ for 1 $< p_{T}^{b} <$ 3 GeV.

Integrated per-trigger yield, $Y_{int}$, on the near-side as a function of $p_{T}^{a}$ for 1 $< p_{T}^{b} <$ 3 GeV.

Integrated per-trigger yield, $Y_{int}$, on the near-side as a function of $p_{T}^{a}$ for 1 $< p_{T}^{b} <$ 3 GeV.

Integrated per-trigger yield, $Y_{int}$, on the away-side as a function of $p_{T}^{a}$ for 1 $< p_{T}^{b} <$ 3 GeV.

Integrated per-trigger yield, $Y_{int}$, on the away-side as a function of $p_{T}^{a}$ for 1 $< p_{T}^{b} <$ 3 GeV.

Integrated per-trigger yield, $Y_{int}$, on the away-side as a function of $p_{T}^{a}$ for 1 $< p_{T}^{b} <$ 3 GeV.

Integrated per-trigger yield, $Y_{int}$, on the away-side as a function of $p_{T}^{a}$ for 1 $< p_{T}^{b} <$ 3 GeV.

Integrated per-trigger yield, $Y_{int}$, on the away-side as a function of $p_{T}^{a}$ for 1 $< p_{T}^{b} <$ 3 GeV.

The integrated per-trigger yield, Y_{int}, on the near-side, the away-side and their difference and Y_{int} from the recoil as a function of event activity. Errors are statistical.

The integrated per-trigger yield, Y_{int}, on the near-side, the away-side and their difference and Y_{int} from the recoil as a function of event activity. Errors are statistical.

The Fourier coefficients $v_{n}$ as a function of $p_{T}^{a}$ extracted from the correlation functions, before and after the subtraction of the recoil component.

The Fourier coefficients $v_{n}$ as a function of $p_{T}^{a}$ extracted from the correlation functions, before and after the subtraction of the recoil component.

The Fourier coefficients $v_{n}$ as a function of $p_{T}^{a}$ extracted from the correlation functions, before and after the subtraction of the recoil component.

$v_{2}$, $v_{3}$, $v_{4}$ and $v_{5}$ as a function of $p_T^a$ for 1 $< p_{T}^{b} <$ 3 GeV for different $N_{ch}^{rec}$ intervals.

$v_{2}$, $v_{3}$, $v_{4}$ and $v_{5}$ as a function of $p_T^a$ for 1 $< p_{T}^{b} <$ 3 GeV for different $N_{ch}^{rec}$ intervals.

$v_{2}$, $v_{3}$, $v_{4}$ and $v_{5}$ as a function of $p_T^a$ for 1 $< p_{T}^{b} <$ 3 GeV for different $N_{ch}^{rec}$ intervals.

$v_{2}$, $v_{3}$, $v_{4}$ and $v_{5}$ as a function of $p_T^a$ for 1 $< p_{T}^{b} <$ 3 GeV for different $N_{ch}^{rec}$ intervals.

$v_{2}$, $v_{3}$, $v_{4}$ and $v_{5}$ as a function of $p_T^a$ for 1 $< p_{T}^{b} <$ 3 GeV for different $N_{ch}^{rec}$ intervals.

$v_{2}$, $v_{3}$, $v_{4}$ and $v_{5}$ as a function of $p_T^a$ for 1 $< p_{T}^{b} <$ 3 GeV for different $N_{ch}^{rec}$ intervals.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{2}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{3}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{3}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{3}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{3}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{3}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{3}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{3}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{3}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{3}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{3}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{3}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The values of factorization variable $r_{3}$ defined by Eq.(11) before and after the subtraction of the recoil component. Errors are total experimental uncertainties.

The centrality dependence of $v_{2}$ as a function of $N_{ch}^{rec}$. Values from before and after the recoil subtraction are included.

The centrality dependence of $v_{3}$ as a function of $N_{ch}^{rec}$. Values from before and after the recoil subtraction are included.

The centrality dependence of $v_{4}$ as a function of $N_{ch}^{rec}$. Values from before and after the recoil subtraction are included.

The centrality dependence of $v_{2}$ as a function of $E_{T}^{Pb}$. Values from before and after the recoil subtraction are included.

The centrality dependence of $v_{3}$ as a function of $E_{T}^{Pb}$. Values from before and after the recoil subtraction are included.

The centrality dependence of $v_{4}$ as a function of $E_{T}^{Pb}$. Values from before and after the recoil subtraction are included.

The $v_{2}$ as a function of $E_{T}^{Pb}$ obtained indirectly by mapping from the $N_{ch}^{rec}-dependence of $v_{2}$ using the correlation data shown in Fig. 2(b).

The $v_{3}$ as a function of $E_{T}^{Pb}$ obtained indirectly by mapping from the $N_{ch}^{rec}-dependence of $v_{3}$ using the correlation data shown in Fig. 2(b).

The first-order harmonic of 2PC before recoil subtraction, $v_{1,1}^{unsub}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

The first-order harmonic of 2PC before recoil subtraction, $v_{1,1}^{unsub}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

The first-order harmonic of 2PC before recoil subtraction, $v_{1,1}^{unsub}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

The first-order harmonic of 2PC before recoil subtraction, $v_{1,1}^{unsub}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

The first-order harmonic of 2PC before recoil subtraction, $v_{1,1}^{unsub}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

The first-order harmonic of 2PC before recoil subtraction, $v_{1,1}^{unsub}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

The first-order harmonic of 2PC after recoil subtraction, $v_{1,1}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

The first-order harmonic of 2PC after recoil subtraction, $v_{1,1}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

The first-order harmonic of 2PC after recoil subtraction, $v_{1,1}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

The first-order harmonic of 2PC after recoil subtraction, $v_{1,1}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

The first-order harmonic of 2PC after recoil subtraction, $v_{1,1}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

The first-order harmonic of 2PC after recoil subtraction, $v_{1,1}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

The first-order harmonic $v_1$ obtained using factorization from $v_{1,1}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

The first-order harmonic $v_1$ obtained using factorization from $v_{1,1}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

The first-order harmonic $v_1$ obtained using factorization from $v_{1,1}$, as a function of $p_T^a$ for different $p_T^b$ ranges for events with $N_{ch}^{rec} \geq$ 220.

$v_{2}$ for Pb+Pb collisions in 55-60% centrality interval obtained using an EP method.

$v_{2}$ for Pb+Pb collisions in 55-60% centrality interval obtained using an EP method, after the scaling.

$v_{3}$ for Pb+Pb collisions in 55-60% centrality interval obtained using an EP method.

$v_{3}$ for Pb+Pb collisions in 55-60% centrality interval obtained using an EP method, after the scaling.

$v_{4}$ for Pb+Pb collisions in 55-60% centrality interval obtained using an EP method.

$v_{4}$ for Pb+Pb collisions in 55-60% centrality interval obtained using an EP method, after the scaling.

Correlation between $E_{T}^{FCal}$ and $N_{ch}^{rec}$ for MB events (without weighting) and MB+HMT events (with weighting), errors are statistical.

Differential production yield per binary collision for $W^{-}$ bosons as a function of $|\eta_\ell|$.

The lepton charge asymmetry $A_{\ell}$ from $W^\pm$ bosons as a function of absolute pseudorapidity.

The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 10-15%.

The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 15-20%.

The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 20-25%.

The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 25-30%.

The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 30-35%.

The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 35-40%.

The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 40-45%.

The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 45-50%.

The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 50-55%.

The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 55-60%.

The second flow harmonic measured with the two-particle cumulants as a function of transverse momentum in centrality bin 60-80%.

The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 0-2%.

The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 2-5%.

The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 5-10%.

The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 10-15%.

The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 15-20%.

The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 20-25%.

The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 25-30%.

The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 30-35%.

The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 35-40%.

The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 40-45%.

The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 45-50%.

The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 50-55%.

The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 55-60%.

The second flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 60-80%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 2-5%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 5-10%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 10-15%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 15-20%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 20-25%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 25-30%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 30-35%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 35-40%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 40-45%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 45-50%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 50-55%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 55-60%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 60-80%.

The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 2-5%.

The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 5-10%.

The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 10-15%.

The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 15-20%.

The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 20-25%.

The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 25-30%.

The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 30-35%.

The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 35-40%.

The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 40-45%.

The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 45-50%.

The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 50-55%.

The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 55-60%.

The second flow harmonic measured with the six-particle cumulats as a function of transverse momentum in centrality bin 60-80%.

The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 2-5%.

The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 5-10%.

The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 10-15%.

The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 15-20%.

The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 20-25%.

The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 25-30%.

The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 30-35%.

The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 35-40%.

The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 40-45%.

The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 45-50%.

The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 50-55%.

The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 55-60%.

The second flow harmonic measured with the eight-particle cumulats as a function of transverse momentum in centrality bin 60-80%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 5-10%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 15-20%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 25-30%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 35-40%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 40-50%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 10-20%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 20-30%.

The second flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 30-40%.

The triangular flow harmonic measured with the two-particle cumulats as a function of transverse momentum in centrality bin 0-25%.

The triangular flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 0-25%.

The triangular flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 0-25%.

The triangular flow harmonic measured with the two-particle cumulats as a function of transverse momentum in centrality bin 25-60%.

The triangular flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 25-60%.

The triangular flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 25-60%.

The quadrangular flow harmonic measured with the two-particle cumulats as a function of transverse momentum in centrality bin 0-25%.

The quadrangular flow harmonic measured with the Event Plane method as a function of transverse momentum in centrality bin 0-25%.

The quadrangular flow harmonic measured with the four-particle cumulats as a function of transverse momentum in centrality bin 0-25%.

The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 0-2%.

The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 2-5%.

The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 5-10%.

The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 10-15%.

The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 15-20%.

The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 20-25%.

The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 25-30%.

The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 30-35%.

The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 35-40%.

The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 40-45%.

The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 45-50%.

The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 50-55%.

The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 55-60%.

The second flow harmonic measured with the two-particle cumulants as a function of pseudorapidity in centrality bin 60-80%.

The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 0-2%.

The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 2-5%.

The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 5-10%.

The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 10-15%.

The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 15-20%.

The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 20-25%.

The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 25-30%.

The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 30-35%.

The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 35-40%.

The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 40-45%.

The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 45-50%.

The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 50-55%.

The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 55-60%.

The second flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 60-80%.

The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 2-5%.

The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 5-10%.

The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 10-15%.

The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 15-20%.

The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 20-25%.

The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 25-30%.

The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 30-35%.

The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 35-40%.

The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 40-45%.

The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 45-50%.

The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 50-55%.

The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 55-60%.

The second flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 60-80%.

The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 2-5%.

The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 5-10%.

The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 10-15%.

The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 15-20%.

The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 20-25%.

The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 25-30%.

The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 30-35%.

The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 35-40%.

The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 40-45%.

The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 45-50%.

The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 50-55%.

The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 55-60%.

The second flow harmonic measured with the six-particle cumulats as a function of pseudorapidity in centrality bin 60-80%.

The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 2-5%.

The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 5-10%.

The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 10-15%.

The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 15-20%.

The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 20-25%.

The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 25-30%.

The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 30-35%.

The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 35-40%.

The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 40-45%.

The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 45-50%.

The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 50-55%.

The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 55-60%.

The second flow harmonic measured with the eight-particle cumulats as a function of pseudorapidity in centrality bin 60-80%.

The triangular flow harmonic measured with the two-particle cumulats as a function of pseudorapidity in centrality bin 0-60%.

The triangular flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 0-60%.

The triangular flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 0-60%.

The quadrangular flow harmonic measured with the two-particle cumulats as a function of pseudorapidity in centrality bin 0-25%.

The quadrangular flow harmonic measured with the Event Plane method as a function of pseudorapidity in centrality bin 0-25%.

The quadrangular flow harmonic measured with the four-particle cumulats as a function of pseudorapidity in centrality bin 0-25%.

The second flow harmonic measured with the two-particle cumulats as a function of <Npart>.

The second flow harmonic measured with the four-particle cumulats as a function of <Npart>.

The second flow harmonic measured with the six-particle cumulats as a function of <Npart>.

The second flow harmonic measured with the eight-particle cumulats as a function of <Npart>.

The ratio of second flow harmonics measured with the six- and four-particle cumulants as a function of <Npart>.

The ratio of second flow harmonics measured with the eight- and four-particle cumulants as a function of <Npart>.

The second flow harmonic measured with the Event Plane method as a function of <Npart>.

The triangular flow harmonic measured with the Event Plane method as a function of <Npart>.

The triangular flow harmonic measured with the two-particle cumulants as a function of <Npart>.

The triangular flow harmonic measured with the two-particle cumulants as a function of <Npart>.

The quadrangular flow harmonic measured with the Event Plane method as a function of <Npart>.

The quadrangular flow harmonic measured with the two-particle cumulants as a function of <Npart>.

The quadrangular flow harmonic measured with the two-particle cumulants as a function of <Npart>.

The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 2-5%.

The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 5-10%.

The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 10-15%.

The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 15-20%.

The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 20-25%.

The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 25-30%.

The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 30-35%.

The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 35-40%.

The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 40-45%.

The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 45-50%.

The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 50-55%.

The second flow harmonic fluctiuations, F(v2), as a function of transverse momentum in centrality bin 55-60%.

The second flow harmonic fluctuations, F(v2), as a function of <Npart>.

The triangular flow harmonic fluctuations, F(v3), as a function of <Npart>.

The triangular flow harmonic fluctuations, F(v4), as a function of <Npart>.

The second flow harmonic measured with the two-particle cumulats as a function of <Npart>.

The second flow harmonic measured with the four-particle cumulats as a function of <Npart>.

The second flow harmonic measured with the six-particle cumulats as a function of <Npart>.

The second flow harmonic measured with the eight-particle cumulats as a function of <Npart>.

The ratio of second flow harmonics measured with the six- and four-particle cumulants as a function of <Npart>.

The ratio of second flow harmonics measured with the eight- and four-particle cumulants as a function of <Npart>.

The triangular flow harmonic measured with the two-particle cumulants as a function of <Npart>.

The quadrangular flow harmonic measured with the Event Plane method as a function of <Npart>.

The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 2-5%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 5-10%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 10-15%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 15-20%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 20-25%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 25-30%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 30-35%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 35-40%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 40-45%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 45-50%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 50-55%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{EP} and v2{4}, as a function of transverse momentum in centrality bin 55-60%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 2-5%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 5-10%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 10-15%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 15-20%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 20-25%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 25-30%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 30-35%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 35-40%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 40-45%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 45-50%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 50-55%.

The second flow harmonic fluctiuations, F(v2), calculated from v2{2} and v2{4}, as a function of transverse momentum in centrality bin 55-60%.

The second flow harmonic fluctuations, F(v2), as a function of <Npart>.

The triangular flow harmonic fluctuations, F(v3), as a function of <Npart>.

The triangular flow harmonic fluctuations, F(v4), as a function of <Npart>.

Inclusive relative fluctuation $\sqrt{C}/M(p_{\rm T})$ as a function of $\sqrt{s}$ in pp collisions.

Relative fluctuation $\sqrt{C_m}/M(p_{\rm T})_m$ as a function of $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle$ in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV.

Relative fluctuation $\sqrt{C_m}/M(p_{\rm T})_m$ as a function of $\langle N_{\rm part} \rangle$ in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV.

Relative fluctuation $\sqrt{C_m}/M(p_{\rm T})_m$ normalized to $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle^{-0.5}$ as a function of $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle$ in pp collisions at $\sqrt{s}$ = 2.76 TeV.

Relative fluctuation $\sqrt{C_m}/M(p_{\rm T})_m$ normalized to $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle^{-0.5}$ as a function of $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle$ in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV.

D(z) distribution for R=0.4 jets.

D(z) distribution for R=0.4 jets.

D(z) distribution for R=0.4 jets.

D(z) distribution for R=0.4 jets.

D(z) distribution for R=0.4 jets.

D(z) distribution for R=0.4 jets.

D(z) distribution for R=0.3 jets.

D(z) distribution for R=0.3 jets.

D(z) distribution for R=0.3 jets.

D(z) distribution for R=0.3 jets.

D(z) distribution for R=0.3 jets.

D(z) distribution for R=0.3 jets.

D(z) distribution for R=0.3 jets.

D(z) distribution for R=0.2 jets.

D(z) distribution for R=0.2 jets.

D(z) distribution for R=0.2 jets.

D(z) distribution for R=0.2 jets.

D(z) distribution for R=0.2 jets.

D(z) distribution for R=0.2 jets.

D(z) distribution for R=0.2 jets.

D(pt) distribution for R=0.4 jets.

D(pt) distribution for R=0.4 jets.

D(pt) distribution for R=0.4 jets.

D(pt) distribution for R=0.4 jets.

D(pt) distribution for R=0.4 jets.

D(pt) distribution for R=0.4 jets.

D(pt) distribution for R=0.4 jets.

D(pt) distribution for R=0.3 jets.

D(pt) distribution for R=0.3 jets.

D(pt) distribution for R=0.3 jets.

D(pt) distribution for R=0.3 jets.

D(pt) distribution for R=0.3 jets.

D(pt) distribution for R=0.3 jets.

D(pt) distribution for R=0.3 jets.

D(pt) distribution for R=0.2 jets.

D(pt) distribution for R=0.2 jets.

D(pt) distribution for R=0.2 jets.

D(pt) distribution for R=0.2 jets.

D(pt) distribution for R=0.2 jets.

D(pt) distribution for R=0.2 jets.

D(pt) distribution for R=0.2 jets.

Ratio of D(z) distributions for R=0.4 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.4 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.4 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.4 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.4 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.4 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.3 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.3 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.3 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.3 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.3 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.3 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.2 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.2 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.2 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.2 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.2 jets for central to peripheral events.

Ratio of D(z) distributions for R=0.2 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.4 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.4 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.4 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.4 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.4 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.4 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.3 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.3 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.3 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.3 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.3 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.3 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.2 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.2 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.2 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.2 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.2 jets for central to peripheral events.

Ratio of D(pt) distributions for R=0.2 jets for central to peripheral events.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

No description provided.

Charged pions v2 as a function of pT for centrality: 20-30%.

Charged pions v2 as a function of pT for centrality: 30-40%.

Charged pions v2 as a function of pT for centrality: 40-50%.

Charged pions v2 as a function of pT for centrality: 50-60%.

Charged kaons v2 as a function of pT for centrality: 0-5%.

Charged kaons v2 as a function of pT for centrality: 5-10%.

Charged kaons v2 as a function of pT for centrality: 10-20%.

Charged kaons v2 as a function of pT for centrality: 20-30%.

Charged kaons v2 as a function of pT for centrality: 30-40%.

Charged kaons v2 as a function of pT for centrality: 40-50%.

Charged kaons v2 as a function of pT for centrality: 50-60%.

K0s v2 as a function of pT for centrality: 0-5%.

K0s v2 as a function of pT for centrality: 5-10%.

K0s v2 as a function of pT for centrality: 10-20%.

K0s v2 as a function of pT for centrality: 20-30%.

K0s v2 as a function of pT for centrality: 30-40%.

K0s v2 as a function of pT for centrality: 40-50%.

K0s v2 as a function of pT for centrality: 50-60%.

Average kaons v2 as a function of pT for centrality: 0-5%.

Average kaons v2 as a function of pT for centrality: 5-10%.

Average kaons v2 as a function of pT for centrality: 10-20%.

Average kaons v2 as a function of pT for centrality: 20-30%.

Average kaons v2 as a function of pT for centrality: 30-40%.

Average kaons v2 as a function of pT for centrality: 40-50%.

Average kaons v2 as a function of pT for centrality: 50-60%.

Protons+AntiProtons v2 as a function of pT for centrality: 0-5%.

Protons+AntiProtons v2 as a function of pT for centrality: 5-10%.

Protons+AntiProtons v2 as a function of pT for centrality: 10-20%.

Protons+AntiProtons v2 as a function of pT for centrality: 20-30%.

Protons+AntiProtons v2 as a function of pT for centrality: 30-40%.

Protons+AntiProtons v2 as a function of pT for centrality: 40-50%.

Protons+AntiProtons v2 as a function of pT for centrality: 50-60%.

Phi v2 as a function of pT for centrality: 10-20%.

Phi v2 as a function of pT for centrality: 20-30%.

Phi v2 as a function of pT for centrality: 30-40%.

Phi v2 as a function of pT for centrality: 40-50%.

Phi v2 as a function of pT for centrality: 50-60%.

Lambda+AntiLambda v2 as a function of pT for centrality: 0-5%.

Lambda+AntiLambda v2 as a function of pT for centrality: 5-10%.

Lambda+AntiLambda v2 as a function of pT for centrality: 10-20%.

Lambda+AntiLambda v2 as a function of pT for centrality: 20-30%.

Lambda+AntiLambda v2 as a function of pT for centrality: 30-40%.

Lambda+AntiLambda v2 as a function of pT for centrality: 40-50%.

Lambda+AntiLambda v2 as a function of pT for centrality: 50-60%.

Xi+AntiXi v2 as a function of pT for centrality: 0-5%.

Xi+AntiXi v2 as a function of pT for centrality: 5-10%.

Xi+AntiXi v2 as a function of pT for centrality: 10-20%.

Xi+AntiXi v2 as a function of pT for centrality: 20-30%.

Xi+AntiXi v2 as a function of pT for centrality: 30-40%.

Xi+AntiXi v2 as a function of pT for centrality: 40-50%.

Xi+AntiXi v2 as a function of pT for centrality: 50-60%.

Omega+AntiOmega v2 as a function of pT for centrality: 5-10%.

Omega+AntiOmega v2 as a function of pT for centrality: 10-20%.

Omega+AntiOmega v2 as a function of pT for centrality: 20-30%.

Omega+AntiOmega v2 as a function of pT for centrality: 30-40%.

Omega+AntiOmega v2 as a function of pT for centrality: 40-50%.

Omega+AntiOmega v2 as a function of pT for centrality: 50-60%.

Charged pions v2 as a function of pT for centrality: 20-40%.

Charged pions v2 as a function of pT for centrality: 40-60%.

Average kaons v2 as a function of pT for centrality: 20-40%.

Average kaons v2 as a function of pT for centrality: 40-60%.

Protons+AntiProtons v2 as a function of pT for centrality: 20-40%.

Protons+AntiProtons v2 as a function of pT for centrality: 40-60%.