$p_{\rm T}$-differential yield of prompt ${\rm D}^{0}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$ in the centrality class 30-50% in the rapidity interval |y|<0.5. Branching ratio of ${\rm D}^{0}$->${\rm K}^{0}\pi^{+}$ : 0.0388. The second (sys) error is the systematic uncertainty from the B feed-down contribution. The first (sys) error is the systematic uncertainty from the other sources.

$p_{\rm T}$-differential yield of prompt ${\rm D}^{+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$ in the centrality class 30-50% in the rapidity interval |y|<0.5. Branching ratio of ${\rm D}^{+}$->${\rm K}^{-}\pi^{+}\pi^{+}$ : 0.0913. The second (sys) error is the systematic uncertainty from the B feed-down contribution. The first (sys) error is the systematic uncertainty from the other sources.

$p_{\rm T}$-differential yield of prompt ${\rm D}^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$ in the centrality class 30-50% in the rapidity interval |y|<0.5. Branching ratio of ${\rm D}^{*+}$->${\rm D}^{0}\pi^{+}$->${\rm K}^{-}\pi^{+}\pi^{+}$ : 0.0388*0.677. The second (sys) error is the systematic uncertainty from the B feed-down contribution. The first (sys) error is the systematic uncertainty from the other sources.

Ratio of ${\rm D}^{+}$ to ${\rm D}^{0}$ meson yield in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$ in the centrality class 0-10% in |y| < 0.5 as a function of $p_{\rm T}$.

Ratio of ${\rm D}^{*+}$ to ${\rm D}^{0}$ meson yield in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$ in the centrality class 0-10% in |y| < 0.5 as a function of $p_{\rm T}$.

Nuclear modification factor $R_{\rm AA}$ of ${\rm D}^{0}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$ in the centrality class 0-10% in |y| < 0.5 as a function of $p_{\rm T}$.

Nuclear modification factor $R_{\rm AA}$ of ${\rm D}^{+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$ in the centrality class 0-10% in |y| < 0.5 as a function of $p_{\rm T}$.

Nuclear modification factor $R_{\rm AA}$ of ${\rm D}^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$ in the centrality class 0-10% in |y| < 0.5 as a function of $p_{\rm T}$.

Nuclear modification factor $R_{\rm AA}$ of ${\rm D}^{0}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$ in the centrality class 30-50% in |y| < 0.5 as a function of $p_{\rm T}$.

Nuclear modification factor $R_{\rm AA}$ of ${\rm D}^{+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$ in the centrality class 30-50% in |y| < 0.5 as a function of $p_{\rm T}$.

Nuclear modification factor $R_{\rm AA}$ of ${\rm D}^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$ in the centrality class 30-50% in |y| < 0.5 as a function of $p_{\rm T}$. Branching ratio of ${\rm D}^{*+}$->${\rm D}^{0}\pi^{+}$->${\rm K}^{-}\pi^{+}\pi^{+}$ : 0.0388*0.677.

Nuclear modification factor $R_{\rm AA}$ of Average ${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$ in the centrality class 0-10% in |y| < 0.5 as a function of $p_{\rm T}$.

Nuclear modification factor $R_{\rm AA}$ of Average ${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$ in the centrality class 30-50% in |y| < 0.5 as a function of $p_{\rm T}$.

Ratio of prompt D meson (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) and charged pion (charged particles for $p_{\rm T}>16~{\rm GeV/}c$) nuclear modification factors ($R_{\rm AA}$) as a function of $p_{\rm T}$ for D mesons with $|y|<0.5$ and charged pions (particles) with $|\eta|<0.8$, measured in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$ in the 0-10% centrality range.

Global variables for Pb+Pb collisions at the LHC from ALICE.

$p^{pp}_T$ dependence of $S_{loss}$ for $\pi^0$ in 200 GeV Au+Au collisions from 2007 data from the PHENIX experiment at RHIC.

$p^{pp}_T$ dependence of $S_{loss}$ for $\pi^0$ in 200 GeV Au+Au collisions from 2004 data from the PHENIX experiment at RHIC for $p_T$ <10 GeV/$c$.

$p^{pp}_T$ dependence of $S_{loss}$ for $\pi^0$ in 200 GeV Cu+Cu collisions using the spectra measured by PHENIX at RHIC in 2005.

$p^{pp}_T$ dependence of $S_{loss}$ for $\pi^0$ in 62 GeV Au+Au collisions using the spectra measured by PHENIX in 2010.

$p^{pp}_T$ dependence of $S_{loss}$ for $\pi^0$ in 62.4 GeV Cu+Cu collisions using the spectra measured by PHENIX in 2005.

$p^{pp}_T$ dependence of $S_{loss}$ for $\pi^0$ in 2.76 TeV Pb+Pb collisions using the result from the ALICE experiment.

Parameters from fitting the indicated power-law functions for $\delta p_T/p_T$ to the data as a function of $p^{pp}_T$ for Au+Au collisions from 2004 data at $\sqrt{s_{NN}}$ = 200 GeV.

Parameters from fitting the indicated power-law functions for $\delta p_T/p_T$ to the data as a function of $p^{pp}_T$ for Au+Au collisions from 2007 data at $\sqrt{s_{NN}}$ = 200 GeV.

Parameters from fitting the indicated power-law functions for $\delta p_T/p_T$ to the data as a function of $p^{pp}_T$ for Cu+Cu collisions from 2005 data at $\sqrt{s_{NN}}$ = 200 GeV.

Parameters from fitting the indicated power-law functions for $\delta p_T/p_T$ to the data as a function of $p^{pp}_T$ for Pb+Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

The nuclear modification factors $R_{p+A}^{\rm{FONLL}}(p_{\rm{T}})$ of $B^{+}$ measured in $p$ + Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV. The statistical and systematic uncertainties on the $p$ + Pb data are shown, followed by upper and lower systematic uncertainties from the FONLL predictions.

The nuclear modification factors $R_{p+A}^{\rm{FONLL}}(p_{\rm{T}})$ of $B^{0}$ measured in $p$ + Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV. The statistical and systematic uncertainties on the $p$ + Pb data are shown, followed by upper and lower systematic uncertainties from the FONLL predictions.

The nuclear modification factors $R_{p+A}^{\rm{FONLL}}(p_{\rm{T}})$ of $B_{s}^{0}$ measured in $p$ + Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV. The statistical and systematic uncertainties on the $p$ + Pb data are shown, followed by upper and lower systematic uncertainties from the FONLL predictions.

The measured $y_{\rm{CM}}$ (rapidity in the center-of-mass frame) differential production cross section of $B^{+}$ in $p$ + Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, together with the cross section calculated by the FONLL model.

The nuclear modification factors $R_{p+A}^{\rm{FONLL}}(y_{\rm{CM}})$ of $B^{+}$ measured in $p$ + Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV. The statistical and systematic uncertainties on the $p$ + Pb data are shown, followed by upper and lower systematic uncertainties from the FONLL predictions.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransDIF region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 1.96 TeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMAX region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 1.96 TeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMIN region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 1.96 TeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransAVE region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 1.96 TeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransDIF region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 1.96 TeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMAX region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMIN region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransAVE region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransDIF region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMAX region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMIN region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransAVE region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransDIF region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 900 GeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMAX region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMIN region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransAVE region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Average charged particle multiplicity for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransDIF region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMAX region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransMIN region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransAVE region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Average charged particle pT sum for charged particles with pT > 0.5 GeV and |eta| < 0.8 in the TransDIF region as defined by the leading charged particle, as a function of the transverse momentum of the leading charged-particle pTmax, at 300 GeV.

Production rate for the $\pi^{0}$ production in the rapidity range $9.2 < y < 9.4$ in $p+p$ collisions and in the rapidity range $-9.2 > y_\rm{lab} > -9.4$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the rapidity range $9.4 < y < 9.6$ in $p+p$ collisions and in the rapidity range $-9.4 > y_\rm{lab} > -9.6$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the rapidity range $9.6 < y < 9.8$ in $p+p$ collisions and in the rapidity range $-9.6 > y_\rm{lab} > -9.8$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the rapidity range $9.8 < y < 10.0$ in $p+p$ collisions and in the rapidity range $-9.8 > y_\rm{lab} > -10.0$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the rapidity range $10.0 < y < 10.2$ in $p+p$ collisions and in the rapidity range $-10.0 > y_\rm{lab} > -10.2$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the rapidity range $10.2 < y < 10.4$ in $p+p$ collisions and in the rapidity range $-10.2 > y_\rm{lab} > -10.4$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the rapidity range $10.4 < y < 10.6$ in $p+p$ collisions and in the rapidity range $-10.4 > y_\rm{lab} > -10.6$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the rapidity range $10.6 < y < 10.8$ in $p+p$ collisions and in the rapidity range $-10.6 > y_\rm{lab} > -10.8$ in $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the $p_\rm{T}$ range $0.0 < p_\rm{T} < 0.2$ GeV in $p+p$ and $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the $p_\rm{T}$ range $0.2 < p_\rm{T} < 0.4$ GeV in $p+p$ and $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the $p_\rm{T}$ range $0.4 < p_\rm{T} < 0.6$ GeV in $p+p$ and $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the $p_\rm{T}$ range $0.6 < p_\rm{T} < 0.8$ GeV in $p+p$ and $p+\rm{Pb}$ collisions.

Production rate for the $\pi^{0}$ production in the $p_\rm{T}$ range $0.8 < p_\rm{T} < 1.0$ GeV in $p+p$ and $p+\rm{Pb}$ collisions.

Nuclear modification factor for the $\pi^{0}$s in the rapidity ranges $-8.8>y_\rm{lab}>-9.0$, $-9.0>y_\rm{lab}>-9.2$, and $-9.2>y_\rm{lab}>-9.4$ in $p+\rm{Pb}$ collisions at $\sqrt{s_\rm{NN}}=5.02$ TeV. The uncertainties include both statistical and systematic uncertainties.

Nuclear modification factor for the $\pi^{0}$s in the rapidity ranges $-9.4>y_\rm{lab}>-9.6$, $-9.6>y_\rm{lab}>-9.8$, and $-9.8>y_\rm{lab}>-10.0$ in $p+\rm{Pb}$ collisions at $\sqrt{s_\rm{NN}}=5.02$ TeV. The uncertainties include both statistical and systematic uncertainties.

Nuclear modification factor for the $\pi^{0}$s in the rapidity ranges $-10.0>y_\rm{lab}>-10.2$, $-10.2>y_\rm{lab}>-10.4$, and $-10.4>y_\rm{lab}>-10.6$ in $p+\rm{Pb}$ collisions at $\sqrt{s_\rm{NN}}=5.02$ TeV. The uncertainties include both statistical and systematic uncertainties.

Nuclear modification factor for the $\pi^{0}$s in the rapidity ranges $-10.6>y_\rm{lab}>-10.8$ in $p+\rm{Pb}$ collisions at $\sqrt{s_\rm{NN}}=5.02$ TeV. The uncertainties include both statistical and systematic uncertainties.

Fully corrected average charged particle scalar Sum(pT) per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momentum for proton-proton collisions at a centre-of-mass energy of 2.76 TeV in the TransMAX region.

Fully corrected average charged particle multiplicity per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momentum for proton-proton collisions at a centre-of-mass energy of 2.76 TeV in the TransMIN region.

Fully corrected average charged particle scalar Sum(pT) per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momentum for proton-proton collisions at a centre-of-mass energy of 2.76 TeV in the TransMIN region.

Fully corrected average charged particle multiplicity per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momentum for proton-proton collisions at a centre-of-mass energy of 2.76 TeV in the TransDIF region.

Fully corrected average charged particle scalar Sum(pT) per unit of pseudorapidity and per radian as a function of the leading track-jet transverse momentum for proton-proton collisions at a centre-of-mass energy of 2.76 TeV in the TransDIF region.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm small-q_{2}^{V0C}$ to unbiased sample, centrality 0-5%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm large-q_{2}^{TPC}$ to unbiased sample, centrality 5-10%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm small-q_{2}^{TPC}$ to unbiased sample, centrality 5-10%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm large-q_{2}^{V0C}$ to unbiased sample, centrality 5-10%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm small-q_{2}^{V0C}$ to unbiased sample, centrality 5-10%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm large-q_{2}^{TPC}$ to unbiased sample, centrality 10-20%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm small-q_{2}^{TPC}$ to unbiased sample, centrality 10-20%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm large-q_{2}^{V0C}$ to unbiased sample, centrality 10-20%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm small-q_{2}^{V0C}$ to unbiased sample, centrality 10-20%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm large-q_{2}^{TPC}$ to unbiased sample, centrality 20-30%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm small-q_{2}^{TPC}$ to unbiased sample, centrality 20-30%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm large-q_{2}^{V0C}$ to unbiased sample, centrality 20-30%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm small-q_{2}^{V0C}$ to unbiased sample, centrality 20-30%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm large-q_{2}^{TPC}$ to unbiased sample, centrality 30-40%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm small-q_{2}^{TPC}$ to unbiased sample, centrality 30-40%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm large-q_{2}^{V0C}$ to unbiased sample, centrality 30-40%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm small-q_{2}^{V0C}$ to unbiased sample, centrality 30-40%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm large-q_{2}^{TPC}$ to unbiased sample, centrality 40-50%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm small-q_{2}^{TPC}$ to unbiased sample, centrality 40-50%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm large-q_{2}^{V0C}$ to unbiased sample, centrality 40-50%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm small-q_{2}^{V0C}$ to unbiased sample, centrality 40-50%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm large-q_{2}^{TPC}$ to unbiased sample, centrality 50-60%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm small-q_{2}^{TPC}$ to unbiased sample, centrality 50-60%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm large-q_{2}^{V0C}$ to unbiased sample, centrality 50-60%.

Ratio of $\rm v_{2}\{{SP}\}$ in the $\rm small-q_{2}^{V0C}$ to unbiased sample, centrality 50-60%.

Centrality dependence of the average $\rm v_{2}\{{SP}\}$ variation in the $\rm large-q_{2}^{TPC}$.

Centrality dependence of the average $\rm v_{2}\{{SP}\}$ variation in the $\rm small-q_{2}^{TPC}$.

Centrality dependence of the average $\rm v_{2}\{{SP}\}$ variation in the $\rm large-q_{2}^{V0C}$.

Centrality dependence of the average $\rm v_{2}\{{SP}\}$ variation in the $\rm small-q_{2}^{V0C}$.

Average $\rm v_{2}\{{SP}\}$ variation as a function of the absolute values of the $q_{2}^{TPC}$, centrality 5-10%.

Average $\rm v_{2}\{{SP}\}$ variation as a function of the absolute values of the $q_{2}^{V0C}$, centrality 5-10%.

Average $\rm v_{2}\{{SP}\}$ variation as a function of the self-normalized values of the $q_{2}^{TPC}$, centrality 5-10%.

Average $\rm v_{2}\{{SP}\}$ variation as a function of the self-normalized values of the $q_{2}^{V0C}$, centrality 5-10%.

Average $\rm v_{2}\{{SP}\}$ variation as a function of the absolute values of the $q_{2}^{TPC}$, centrality 30-40%.

Average $\rm v_{2}\{{SP}\}$ variation as a function of the absolute values of the $q_{2}^{V0C}$, centrality 30-40%.

Average $\rm v_{2}\{{SP}\}$ variation as a function of the self-normalized values of the $q_{2}^{TPC}$, centrality 30-40%.

Average $\rm v_{2}\{{SP}\}$ variation as a function of the self-normalized values of the $q_{2}^{V0C}$, centrality 30-40%.

Average $\rm v_{2}\{{SP}\}$ variation as a function of the absolute values of the $q_{2}^{TPC}$, centrality 50-60%.

Average $\rm v_{2}\{{SP}\}$ variation as a function of the absolute values of the $q_{2}^{V0C}$, centrality 50-60%.

Average $\rm v_{2}\{{SP}\}$ variation as a function of the self-normalized values of the $q_{2}^{TPC}$, centrality 50-60%.

Average $\rm v_{2}\{{SP}\}$ variation as a function of the self-normalized values of the $q_{2}^{V0C}$, centrality 50-60%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm large-q_{2}^{TPC}$ to unbiased sample, centrality 0-5%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm small-q_{2}^{TPC}$ to unbiased sample, centrality 0-5%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm large-q_{2}^{V0C}$ to unbiased sample, centrality 0-5%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm small-q_{2}^{V0C}$ to unbiased sample, centrality 0-5%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm large-q_{2}^{TPC}$ to unbiased sample, centrality 5-10%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm small-q_{2}^{TPC}$ to unbiased sample, centrality 5-10%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm large-q_{2}^{V0C}$ to unbiased sample, centrality 5-10%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm small-q_{2}^{V0C}$ to unbiased sample, centrality 5-10%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm large-q_{2}^{TPC}$ to unbiased sample, centrality 10-20%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm small-q_{2}^{TPC}$ to unbiased sample, centrality 10-20%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm large-q_{2}^{V0C}$ to unbiased sample, centrality 10-20%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm small-q_{2}^{V0C}$ to unbiased sample, centrality 10-20%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm large-q_{2}^{TPC}$ to unbiased sample, centrality 20-30%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm small-q_{2}^{TPC}$ to unbiased sample, centrality 20-30%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm large-q_{2}^{V0C}$ to unbiased sample, centrality 20-30%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm small-q_{2}^{V0C}$ to unbiased sample, centrality 20-30%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm large-q_{2}^{TPC}$ to unbiased sample, centrality 30-40%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm small-q_{2}^{TPC}$ to unbiased sample, centrality 30-40%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm large-q_{2}^{V0C}$ to unbiased sample, centrality 30-40%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm small-q_{2}^{V0C}$ to unbiased sample, centrality 30-40%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm large-q_{2}^{TPC}$ to unbiased sample, centrality 40-50%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm small-q_{2}^{TPC}$ to unbiased sample, centrality 40-50%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm large-q_{2}^{V0C}$ to unbiased sample, centrality 40-50%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm small-q_{2}^{V0C}$ to unbiased sample, centrality 40-50%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm large-q_{2}^{TPC}$ to unbiased sample, centrality 50-60%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm small-q_{2}^{TPC}$ to unbiased sample, centrality 50-60%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm large-q_{2}^{V0C}$ to unbiased sample, centrality 50-60%.

Ratio of the $p_{\rm T}$ distribution of charged hadrons in the $\rm small-q_{2}^{V0C}$ to unbiased sample, centrality 50-60%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 0-5%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 0-5%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 0-5%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 0-5%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 0-5%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 0-5%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 5-10%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 5-10%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 5-10%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 5-10%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 5-10%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 5-10%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 10-20%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 10-20%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 10-20%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 10-20%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 10-20%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 10-20%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 20-30%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 20-30%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 20-30%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 20-30%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 20-30%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 20-30%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 30-40%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 30-40%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 30-40%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 30-40%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 30-40%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 30-40%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 40-50%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 40-50%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 40-50%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 40-50%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 40-50%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 40-50%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 50-60%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 50-60%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm large-q_{2}^{TPC}$ sample to the unbiased sample, centrality 50-60%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 50-60%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 50-60%.

Fig. 10: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm large-q_{2}^{V0C}$ sample to the unbiased sample, centrality 50-60%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 0-5%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 0-5%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 0-5%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 0-5%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 0-5%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 0-5%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 5-10%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 5-10%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 5-10%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 5-10%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 5-10%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 5-10%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 10-20%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 10-20%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 10-20%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 10-20%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 10-20%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 10-20%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 20-30%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 20-30%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 20-30%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 20-30%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 20-30%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 20-30%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 30-40%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 30-40%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 30-40%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 30-40%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 30-40%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 30-40%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 40-50%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 40-50%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 40-50%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 40-50%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 40-50%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 40-50%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 50-60%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 50-60%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm small-q_{2}^{TPC}$ sample to the unbiased sample, centrality 50-60%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified pions in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 50-60%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified kaons in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 50-60%.

Fig. 11: Ratio of the $p_{\rm T}$ distribution of identified protons in the $\rm small-q_{2}^{V0C}$ sample to the unbiased sample, centrality 50-60%.

pT-differential inclusive muon $v_{2}$ extracted with two-particle $Q$ cumulants method.

pT-differential inclusive muon $v_{2}$ extracted with scalar product method.

pT-differential inclusive muon $v_{2}$ extracted with two-particle cumulants method.

pT-differential inclusive muon $v_{2}$ extracted with four-particle cumulants method.

pT-differential inclusive muon $v_{2}$ extracted with Lee-Yang zeros (Sum) method.

pT-differential inclusive muon $v_{2}$ extracted with Lee-Yang zeros (Prod) method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with scalar product method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with two-particle $Q$ cumulants method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with scalar product method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with two-particle $Q$ cumulants method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with scalar product method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with two-particle cumulants method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with four-particle cumulants method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with Lee-Yang zeros (Sum) method.

pT-differential $v_{2}$ of muons from heavy-flavour decays extracted with Lee-Yang zeros (Prod) method.

Elliptic flow of muons from heavy-flavour hadron decays as a function of the collision centrality extracted with scalar product method.

Elliptic flow of muons from heavy-flavour hadron decays as a function of the collision centrality extracted with two-particle cumulants method.

$y$-differential production cross section of $\phi$ in p-Pb at $\sqrt{s_{\rm NN}}$=5.02 TeV, in $p_{\rm T}$ range 2.03 < $p_{\rm T}$ < 3.53

Anti-$^{3}$He over $^{3}$He ratio versus pT per nucleon for 0-20% centrality class.

Anti-$^{3}$He over $^{3}$He ratio versus pT per nucleon for 20-80% centrality class.

Anti-$^{3}$He over $^{3}$He ratio versus pT per nucleon for 20-80% centrality class.

Invariant transverse momentum distribution of deuteron for various centrality classes for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV.

Invariant transverse momentum distribution of deuteron for various centrality classes for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV.

Invariant transverse momentum distribution of deuteron for inelastic pp collisions at $\sqrt{s}$ = 7 TeV.

Invariant transverse momentum distribution of deuteron for inelastic pp collisions at $\sqrt{s}$ = 7 TeV.

Invariant transverse momentum distribution of $^{3}$He for 0-20% and 20-80% centrality classes for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV.

Invariant transverse momentum distribution of $^{3}$He for 0-20% and 20-80% centrality classes for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV.

d/p ratio as a function of event multiplicity.

d/p ratio as a function of event multiplicity.

$^{3}$He/p ratio as a function of event multiplicity. NOTE: $^{3}$He/p ratio is divided by 150 for plotting in Fig. 16.

$^{3}$He/p ratio as a function of event multiplicity. NOTE: $^{3}$He/p ratio is divided by 150 for plotting in Fig. 16.

The coalescence parameters B$_{2}$ as a function of the transverse momentum per nucleon for various centrality classes for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV.

The coalescence parameters B$_{2}$ as a function of the transverse momentum per nucleon for various centrality classes for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV.

The coalescence parameters B$_{3}$ as a function of the transverse momentum per nucleon for 0-20% and 20-80% centrality classes for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV.

The coalescence parameters B$_{3}$ as a function of the transverse momentum per nucleon for 0-20% and 20-80% centrality classes for Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 2.76 TeV.