Measurement of the fractions of 1neutron (1n), 2 neutrons (2n), 3 neutrons (3n) events with respect to the total number of events (Ntot) for single EMD minus mutual EMD process in Pb-Pb collisions at 2.76 TeV per nucleon.

Measurements of the parameter D for two values of midrapidity range.

Measurements of D from the HIJING event generator for two values of midrapidity range.

Measurements of D in P P collisions from the PYTHIA event generator for two values of midrapidity range.

Measurements of MEAN(NCH)*NU(+-DYN) as a function of the Delta(ETARAP) range for three centrality ranges.

Correlation function as a function of pair relative momentum for 20-40% multiplicity class and pair transverse momentum range (0.5-1.0) GeV/c.

Correlation function as a function of pair relative momentum for 40-90% multiplicity class and pair transverse momentum range (0.2-0.5) GeV/c.

Correlation function as a function of pair relative momentum for 40-90% multiplicity class and pair transverse momentum range (0.5-1.0) GeV/c.

Femtoscopic radii as a function of the pair transverse momentum.

Correlation strengths as a function of the pair transverse momentum.

Data-to-cocktail ratio as a function of the invariant-mass. In the hadronic cocktail, random correlations of dielectrons from charm decays are assumed to simulate the effects of the interaction between charm quarks and the medium. The statistical and systematic uncertainties of data are represented by vertical bars and boxes.

Dielectron invariant-mass spectrum measured in central Pb-Pb collisions for the transverse-momentum interval 1.0 < $p_{\rm T,ee}$ < 2.0 GeV/$c. The statistical and systematic uncertainties of the data are represented by vertical bars and boxes.

Dielectron invariant-mass spectrum measured in central Pb--Pb collisions for the transverse-momentum interval 2.0 < $p_{\rm T,ee}$ < 4.0 GeV/$c. The statistical and systematic uncertainties of the data are represented by vertical bars and boxes.

Direct photon ratio $R_{\gamma^{(*)}}=1+\gamma^{(*)}_{\mathrm{dir}}/\gamma^{(*)}_{\mathrm{decay}}$ measured using virtual photons in the centrality range 0$-$10$\%$. The statistical and systematic uncertainties of the data are represented by vertical bars and boxes.

The radius $r_0$ as a function of m$_T$ obtained with the p$-$p $\oplus$ $\overline{\mathrm{p}}-\overline{\mathrm{p}}$ and the p$-\Lambda$ $\oplus$ $\overline{\mathrm{p}}-\overline{\Lambda}$ correlation functions.

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%.

$cos\theta^{*}$ distribution of $\phi$ meson w.r.t. Production Plane in transverse momentum range 0.5-0.8 GeV/$c$ measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$cos\theta^{*}$ distribution of $\rm{K}^{*0}$ (average of particle and anti-particle) meson w.r.t. Random Plane in transverse momentum range 0.8-1.2 GeV/$c$ measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$cos\theta^{*}$ distribution of $\phi$ meson w.r.t. Random Plane in transverse momentum range 0.5-0.7 GeV/$c$ measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$cos\theta^{*}$ distribution of K$^{0}_{S}$ meson w.r.t. Event Plane in transverse momentum range 0.6-0.8 GeV/$c$ measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$cos\theta^{*}$ distribution of K$^{0}_{S}$ meson w.r.t. Production Plane in transverse momentum range 0.6-0.8 GeV/$c$ measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$cos\theta^{*}$ distribution of $\rm{K}^{*0}$ (average of particle and anti-particle) meson w.r.t. Production Plane in transverse momentum range 0-0.6 GeV/$c$ measured in pp collisions at $\sqrt{s}$ = 13 TeV.

$cos\theta^{*}$ distribution of $\phi$ meson w.r.t. Production Plane in transverse momentum range 0.5-0.8 GeV/$c$ measured in pp collisions at $\sqrt{s}$ = 13 TeV.

$\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Event Plane for $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Event Plane for $\rm{K}^{0}_{S}$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Event Plane for $\phi$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Production Plane for $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Production Plane for $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in pp collisions at $\sqrt{s}$ = 13 TeV.

$\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Production Plane for $\rm{K}^{0}_{S}$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Production Plane for $\phi$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Production Plane for $\phi$ meson measured in pp collisions at $\sqrt{s}$ = 13 TeV.

$\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Random Plane for $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $p_{\rm T}$ w.r.t. Random Plane for $\phi$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Production Plane in transverse momentum range 0.4-1.2 GeV/$c$ for $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Production Plane in transverse momentum range 3.0-5.0 GeV/$c$ for $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Production Plane in transverse momentum range 0.5-0.8 GeV/$c$ for $\phi$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Production Plane in transverse momentum range 3.0-5.0 GeV/$c$ for $\phi$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Event Plane in transverse momentum range 0.8-1.2 GeV/$c$ for $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Event Plane in transverse momentum range 3.0-5.0 GeV/$c$ for $\rm{K}^{*0}$ (average of particle and anti-particle) meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Event Plane in transverse momentum range 0.5-0.7 GeV/$c$ for $\phi$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$\rho_{00}$ as a function of $\langle N_{\rm{part}} \rangle$ w.r.t. Event Plane in transverse momentum range 3.0-5.0 GeV/$c$ for $\phi$ meson measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 2.76 TeV.

$p_{T}$-distributions of kaons ($K^{+}+K^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{T}$-distributions of protons ($p+pbar$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{T}$-distributions of protons ($p+pbar$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{T}$-distributions of kaons ($K^{+}+K^{-}$)/pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{T}$-distributions of kaons ($K^{+}+K^{-}$)/pions ($\pi^{+}+\pi^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{T}$-distributions of protons ($p+pbar$)/pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{T}$-distributions of protons ($p+pbar$)/pions ($\pi^{+}+\pi^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

Integrated yield ratios of kaons ($K^{+}+K^{-}$) to pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

Integrated yield ratios of kaons ($K^{+}+K^{-}$) to pions ($\pi^{+}+\pi^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

Integrated yield ratios of protons ($p+pbar$) to pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

Integrated yield ratios of protons ($p+pbar$) to pions ($\pi^{+}+\pi^{-}$) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{T}$-dependent nuclear modification factor of pions ($\pi^{+}+\pi^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{T}$-dependent nuclear modification factor of kaons ($K^{+}+K^{-}$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{T}$-dependent nuclear modification factor of protons ($p+pbar$) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

Directed flow D0 meson 10-40%

Directed flow D0-bar meson 10-40%

Delta Directed flow D0 meson 10-40%

Slope Dv1 charged hadrons 540%

Slope Dv1 D0 meson 540%