Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle cumulant method at backward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the V0M estimator.

Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle cumulant method at forward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the CL1 estimator.

Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle cumulant method at forward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the ZDC estimator.

Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle cumulant method at backward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the CL1 estimator.

Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle cumulant method at backward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the ZDC estimator.

Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle correlation method at forward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the CL1 estimator.

Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle correlation method at forward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the ZDC estimator.

Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle corrrelation method at backward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the CL1 estimator.

Inclusive muon $v_{2}^{\mu}$ as a function of $p_{\mathrm{T}}$ is measured by two-particle correlation method at backward rapidities in high-multiplicity (0$-$20%) p$-$Pb collisions at $\sqrt{s_\mathrm{NN}}$= 8.16 TeV. The event activity is estimated with the ZDC estimator.

Nuclear modification factor of the $\psi$(2S) shown as a function of transverse momentum

Ratio of the $\psi$(2S) over J/$\psi$ cross sections, not corrected for the branching ratio, shown as a function of transverse momentum

Double ratio of the $\psi$(2S) over J/$\psi$ cross sections in Pb--Pb and pp collisions shown as a function of transverse momentum

Self-normalized Upsilon(2S) to Upsilon(1S) yield ratio as a function of the self-normalized charged-particle multiplicity.

Self-normalized Upsilon(3S) to Upsilon(1S) yield ratio as a function of the self-normalized charged-particle multiplicity.

Self-normalized Upsilon(1S) to J/PSI yield ratio as a function of the self-normalized charged-particle multiplicity.

The unfolded differential charge asymmetry as a function of the transverse momentum of the top pair system. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NNLO in QCD and NLO in EW theory are listed. The scale uncertainty is obtained by varying renormalisation and factorisation scales independently by a factor of 2 or 0.5 around $\mu_0$ to calculate the maximum and minimum value of the asymmetry, respectively. The nominal value $\mu_0$ is chosen as $H_T/4$. The variations in which one scale is multiplied by 2 while the other scale is divided by 2 are excluded. Finally, the scale and MC integration uncertainties are added in quadrature.

The unfolded differential charge asymmetry as a function of the longitudinal boost of the top pair system. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NNLO in QCD and NLO in EW theory are listed. The scale uncertainty is obtained by varying renormalisation and factorisation scales independently by a factor of 2 or 0.5 around $\mu_0$ to calculate the maximum and minimum value of the asymmetry, respectively. The nominal value $\mu_0$ is chosen as $H_T/4$. The variations in which one scale is multiplied by 2 while the other scale is divided by 2 are excluded. Finally, the scale and MC integration uncertainties are added in quadrature.

The unfolded inclusive leptonic asymmetry. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

The unfolded differential leptonic asymmetry as a function of the invariant mass of the di-lepton pair. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

The unfolded differential leptonic asymmetry as a function of the transverse momentum of the di-lepton pair. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

The unfolded differential leptonic asymmetry as a function of the longitudinal boost of the di-lepton pair. The unfolded $A_C^{\ell\bar{\ell}}$ is obtained in the reduced phase-space defined by the requirement $|\Delta |\eta_{\ell\bar{\ell}}||<2.5$. The measured values are given with statistical and systematic uncertainties. The SM theory predictions calculated at NLO in QCD and NLO in EW theory are listed. The theory uncertainty is obtained by varying both scales by a factor of 0.5 or 2.0 to calculate the minimum and maximum value of the asymmetry, respectively.

Individual 68% and 95% CL bounds on the relevant Wilson coefficients of the SM Effective Field Theory in units of $\text{TeV}^{-2}$. The bounds are derived from the $A_C^{t\bar{t}}$ inclusive measurement. The experimental uncertainties are accounted for, in the form of the complete covariance matrix that keeps track of correlations between bins for the differential measurement. The theory uncertainty from the NNLO QCD + NLO EW calculation is included by explicitly varying the renormalization and factorization scales, or the parton density functions, in the calculation and registering the variations in the intervals.

Individual 68% and 95% CL bounds on the relevant Wilson coefficients of the SM Effective Field Theory in units of $\text{TeV}^{-2}$. The bounds are derived from the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement. The experimental uncertainties are accounted for, in the form of the complete covariance matrix that keeps track of correlations between bins for the differential measurement. The theory uncertainty from the NNLO QCD + NLO EW calculation is included by explicitly varying the renormalization and factorization scales, or the parton density functions, in the calculation and registering the variations in the intervals.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ inclusive measurement. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0,0.3]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0.3,0.6]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0.6,0.8]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement for $\beta_{z,t\bar{t}}$ $\in$ [0.8,1]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ < 500 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ $\in$ [500,750] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ $\in$ [750,1000] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ $\in$ [1000,1500] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement for $m_{t\bar{t}}$ > 1500 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement for $p_{T,t\bar{t}}$ < 30 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement for $p_{T,t\bar{t}}$ $\in$ [30,120] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement for $p_{T,t\bar{t}}$ > 120 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ inclusive measurement. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0,0.3]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0.3,0.6]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0.6,0.8]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement for $\beta_{z,\ell\bar{\ell}}$ $\in$[0.8,1]. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ < 200 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ $\in$ [200,300] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ $\in$ [300,400] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement for $m_{\ell\bar{\ell}}$ > 400 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement for $p_{T,\ell\bar{\ell}}$ < 20 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement for $p_{T,\ell\bar{\ell}}$ $\in$ [20, 70] GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Ranking of the systematic uncertainties with marginalisation for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement for $p_{T,\ell\bar{\ell}}$ > 70 GeV. The effect on unfolded $A_C$ for down and up variation of the systematic uncertainty is shown, respectively. The pulls and constraints of the ranked NPs are obtained from data.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ inclusive measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ inclusive measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Post-marginalisation correlation coefficients $\rho_{ij}$ of nuisance parameters for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement. Only $|\rho_{ij}| > 0.05$ values are included.

Covariance matrix for the $A_C^{t\bar{t}}$ vs $m_{t\bar{t}}$ measurement. The total (stat. + syst.) uncertainties are considered.

Covariance matrix for the $A_C^{t\bar{t}}$ vs $p_{T,t\bar{t}}$ measurement. The total (stat. + syst.) uncertainties are considered.

Covariance matrix for the $A_C^{t\bar{t}}$ vs $\beta_{z,t\bar{t}}$ measurement. The total (stat. + syst.) uncertainties are considered.

Covariance matrix for the $A_C^{\ell\ell}$ vs $m_{\ell\bar{\ell}}$ measurement. The total (stat. + syst.) uncertainties are considered.

Covariance matrix for the $A_C^{\ell\ell}$ vs $p_{T,\ell\bar{\ell}}$ measurement. The total (stat. + syst.) uncertainties are considered.

Covariance matrix for the $A_C^{\ell\ell}$ vs $\beta_{z,\ell\bar{\ell}}$ measurement. The total (stat. + syst.) uncertainties are considered.

$f_{0}(980)$ to pions ($(\pi^{+}+\pi^{-})/2$), $p_{\rm T}$-integrated yield ratio at midrapidity as a function of $\langle {\rm d}N_{\rm ch}/{\rm d}\eta \rangle$. The uncertainty 'stat,syst' indicates the total uncertainty (stat+syst) on the measurement. The branching ratio correction amounts to BR = (46 $\pm$ 6)% [ Phys. Rev. Lett. 111 no. 6, (2013) 062001] assuming dominance of $\pi\pi$ and KK channel has been applied to the $p_{\rm T}$-differential yields of $f_{0}(980)$. Here, the branching ratio relative uncertainty (13%) for $f_{0}(980)$ is not included.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with two-particle correlations with a pseudorapidity gap of $|\Delta \eta| > 0.8$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The $p_{T}$-differential $v_2$ measured with four-particle correlations for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the mean value of $v_2$ ($\langle v_2 \rangle$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The dependence of the standard deviation of $v_2$ ($\sigma_{v_2}$) on $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The relative elliptic flow fluctuations ($F(v_2)$) as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

The ratio $v_2\{4\}/v_2\{2,|\Delta \eta| > 0.8\}$ as a function of $p_{T}$ for different particle species and centralities in Pb--Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV.

Delta_eta dependence of Kappa_2(p-pbar)/<p+pbar>, momentum range: 0.6 < p < 1.5 GeV/c.

Centrality dependence of Kappa_2(p-pbar)/<p+pbar>, momentum range: 0.6 < p < 1.5 GeV/c.

Centrality dependence of Kappa_2(p-pbar)/<p+pbar>, momentum range: 0.6 < p < 1.5 GeV/c.

Delta_eta dependence of Kappa_2(p-pbar)/<p+pbar>, momentum range: 0.6 < p < 1.5 GeV/c.

Delta_eta dependence of Kappa_2(p-pbar)/<p+pbar>, momentum range: 0.6 < p < 2.0 GeV/c.

Centrality dependence of Kappa_2(p-pbar)/<p+pbar>, momentum range: 0.6 < p < 1.5 GeV/c.

Centrality dependence of Kappa_2(p-pbar)/<p+pbar>, momentum range: 0.6 < p < 2.0 GeV/c.

Delta_eta dependence of Kappa_3(p-pbar)/Kappa_2(p-pbar), without efficiency correction, momentum range: 0.6 < p < 1.5 GeV/c.

Centrality dependence of Kappa_3(p-pbar)/Kappa_2(p-pbar), without efficiency correction, momentum range: 0.6 < p < 1.5 GeV/c.

Delta_eta dependence of Kappa_3(p-pbar)/Kappa_2(p-pbar), momentum range: 0.6 < p < 1.5 GeV/c.

Centrality dependence of Kappa_3(p-pbar)/Kappa_2(p-pbar), momentum range: 0.6 < p < 1.5 GeV/c.

Measured p-p-p three-particle correlation function. The average transverse mass of the p-p pairs in the triplets at $Q_3 < 0.8$ GeV/$c$ is 1.27 GeV/$c^2$.

Measured p-p-$\Lambda$ three-particle correlation function. The average transverse mass of the p-p (p-$\Lambda$) pairs in the triplets at $Q_3 < 0.8$ GeV/$c$ is 1.30 (1.43) GeV/$c^2$.

p-p-p cumulant

p-p-$\mathrm{\overline{p}}$ cumulant

p-p-$\Lambda$ cumulant

Measured p-p-$\mathrm{\overline{p}}$ three-particle correlation function

The (p-p)-$\mathrm{\overline{p}}$ correlation function obtained using the data-driven approach

The p-(p-$\mathrm{\overline{p}}$) correlation function obtained using the data-driven approach

K$^+$p (K$^+$p $\oplus$ K$^-\overline{\mathrm p}$) correlation function in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV (40-100%).

K$^+$p (K$^+$p $\oplus$ K$^-\overline{\mathrm p}$) correlation function in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV (60-70%).

K$^+$p (K$^+$p $\oplus$ K$^-\overline{\mathrm p}$) correlation function in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV (70-80%).

K$^+$p (K$^+$p $\oplus$ K$^-\overline{\mathrm p}$) correlation function in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV (80-90%).

K$^-$p (K$^-$p $\oplus$ K$^+\overline{\mathrm p}$) correlation function in pp collisions at $\sqrt{s}=13$ TeV.

K$^-$p (K$^-$p $\oplus$ K$^+\overline{\mathrm p}$) correlation function in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV (0-20%).

K$^-$p (K$^-$p $\oplus$ K$^+\overline{\mathrm p}$) correlation function in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV (20-40%).

K$^-$p (K$^-$p $\oplus$ K$^+\overline{\mathrm p}$) correlation function in p-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV (40-100%).

K$^-$p (K$^-$p $\oplus$ K$^+\overline{\mathrm p}$) correlation function in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV (60-70%).

K$^-$p (K$^-$p $\oplus$ K$^+\overline{\mathrm p}$) correlation function in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV (70-80%).

K$^-$p (K$^-$p $\oplus$ K$^+\overline{\mathrm p}$) correlation function in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}} = 5.02$ TeV (80-90%).

Scaling factor ($\alpha_j $) for $\mathrm{\overline{K}^0 n}$ extracted from the different fits of the K$^-$ p correlation function as a function of the core radius $r_{\mathrm{core}}$.

Scaling factor ($\alpha_j $) for $\pi \Sigma$ extracted from the different fits of the K$^-$ p correlation function as a function of the core radius $r_{\mathrm{core}}$.

This table shows the correlation coefficient between the $\alpha_{\mathrm{\overline{K}^0 n}}$ and $\alpha_{\pi \Sigma}$ parameters extracted from the different fits to the K$^-$ p correlation function with free weights. The results are shown as a function of the core radius $r_{\mathrm{core}}$ shown in Table 7. The error on the correlation coefficient, shown as statistical errors in the table, are obteined by using the Pearson's formula to evaluate the probable error of correlation coefficient.