Fig. A1: Number density $N_{ch}$ (left) and $\\Sigma p_{T}$ (right) distributions as a function of pleadingT and the comparisons to MC predictions in Toward (top), Transverse (middle), and Away (bottom) regions for $p_{T}^{track} >$ 0.5 GeV/$c$. The shaded areas in the upper panels represent the systematic uncertainties and vertical error bars indicate statistical uncertainties. In the lower panels, the shaded areas are the sum in quadrature of statistical and systematic uncertainties from the upper panels. No uncertainties are given for the MC calculations.

Fig. A2: Number density $N_{ch}$ (left) and $\\Sigma p_{T}$ (right) distributions as a function of pleadingT and the comparisons to MC predictions in Toward (top), Transverse (middle), and Away (bottom) regions for $p_{T}^{track} >$ 1.0 GeV/$c$. The shaded areas in the upper panels represent the systematic uncertainties and vertical error bars indicate statistical uncertainties. In the lower panels, the shaded areas are the sum in quadrature of statistical and systematic uncertainties from the upper panels. No uncertainties are given for the MC calculations.

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class IV+V, average of particle and antiparticle

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class VI, average of particle and antiparticle

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class VII, average of particle and antiparticle

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class VIII, average of particle and antiparticle

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class IX, average of particle and antiparticle

K$^{*0}$ transverse momentum spectrum - V0M multiplicity class X, average of particle and antiparticle

K$^{*0}$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class I

K$^{*0}$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class II

K$^{*0}$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class III

K$^{*0}$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class IV+V

K$^{*0}$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class VI

K$^{*0}$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class VII

K$^{*0}$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class VIII

K$^{*0}$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class IX

K$^{*0}$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class X

$\phi$ transverse momentum spectrum - V0M multiplicity class I

$\phi$ transverse momentum spectrum - V0M multiplicity class II

$\phi$ transverse momentum spectrum - V0M multiplicity class III

$\phi$ transverse momentum spectrum - V0M multiplicity class IV

$\phi$ transverse momentum spectrum - V0M multiplicity class V

$\phi$ transverse momentum spectrum - V0M multiplicity class VI

$\phi$ transverse momentum spectrum - V0M multiplicity class VII

$\phi$ transverse momentum spectrum - V0M multiplicity class VIII

$\phi$ transverse momentum spectrum - V0M multiplicity class IX

$\phi$ transverse momentum spectrum - V0M multiplicity class X

$\phi$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class I

$\phi$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class II

$\phi$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class III

$\phi$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class IV

$\phi$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class V

$\phi$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class VI

$\phi$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class VII

$\phi$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class VIII

$\phi$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class IX

$\phi$ transverse momentum spectrum ratio to INEL>0 - V0M multiplicity class X

K$^{*0}$ average transverse momentum vs multiplicity - V0M multiplicity classes

$\phi$ average transverse momentum vs multiplicity - V0M multiplicity classes

K$^{*0}$ transverse momentum integrated yield vs multiplicity - V0M multiplicity classes, average of particle and antiparticle

$\phi$ transverse momentum integrated yield vs multiplicity - V0M multiplicity classes

K$^{*0}$/K$_{\mathrm{S}}^{0}$ transverse momentum integrated yield ratio vs multiplicity - V0M multiplicity classes, average of particle and antiparticle

$\phi$/K$_{\mathrm{S}}^{0}$ transverse momentum integrated yield ratio vs multiplicity - V0M multiplicity classes

$(\Xi^{-} + \bar{\Xi}^{+})$/$\phi$ transverse momentum integrated yield ratio vs multiplicity - V0M multiplicity classes

$\phi$/$(\pi^{+} + \pi^{-})$ transverse momentum integrated yield ratio vs multiplicity - V0M multiplicity classes

K$^{*0}$/K$_{\mathrm{S}}^{0}$ yield ratio vs transverse momentum - V0M multiplicity class II, average of particle and antiparticle

K$^{*0}$/K$_{\mathrm{S}}^{0}$ yield ratio vs transverse momentum - V0M multiplicity class X, average of particle and antiparticle

$\phi$/K$_{\mathrm{S}}^{0}$ yield ratio vs transverse momentum - V0M multiplicity class II

$\phi$/K$_{\mathrm{S}}^{0}$ yield ratio vs transverse momentum - V0M multiplicity class X

K$^{*0}$/K$_{\mathrm{S}}^{0}$ double yield ratio vs transverse momentum - V0M multiplicity class II / V0M multiplicity class X, average of particle and antiparticle

$\phi$/K$_{\mathrm{S}}^{0}$ double yield ratio vs transverse momentum - V0M multiplicity class II / V0M multiplicity class X

Significance of K$^{*0}$/K$_{\mathrm{S}}^{0}$ double yield ratio vs transverse momentum - V0M multiplicity class II / V0M multiplicity class X

Significance of $\phi$/K$_{\mathrm{S}}^{0}$ double yield ratio vs transverse momentum - V0M multiplicity class II / V0M multiplicity class X

($\rm{K}^{*0}$+$\bar{\rm{K}}^{*0}$)/(K$^{+}$+K$^{-}$) transverse momentum integrated yield ratio vs multiplicity - V0M multiplicity classes

($\rm{K}^{*0}$+$\bar{\rm{K}}^{*0}$)/($\pi^{+}$+$\pi^{-}$) transverse momentum integrated yield ratio vs multiplicity - V0M multiplicity classes

2$\phi$/(K$^{+}$+K$^{-}$) transverse momentum integrated yield ratio vs multiplicity - V0M multiplicity classes

$\phi$/($\rm{P}$ + $\bar{\rm{P}}$) transverse momentum integrated yield ratio vs multiplicity - V0M multiplicity classes

$\phi$/$(\Lambda~+~\bar{\Lambda})$ transverse momentum integrated yield ratio vs multiplicity - V0M multiplicity classes

$(\Omega^{-}~+~\bar{\Omega}^{+})$/$\phi$ transverse momentum integrated yield ratio vs multiplicity - V0M multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}$ transverse momentum spectrum - V0M multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$K^{0}_{S}$ transverse momentum spectrum ratios to INEL>0 - V0M multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum ratios to INEL>0 - V0M multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Xi^{-}+\bar{\Xi^{+}}$ transverse momentum spectrum ratios to INEL>0 - V0M multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Omega^{-}+\bar{\Omega^{+}}$ transverse momentum spectrum ratios to INEL>0 - V0M multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$K^{0}_{S}$ transverse momentum spectrum - SPDtracklets08 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum - SPDtracklets08 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Xi^{-}+\bar{\Xi^{+}}$ transverse momentum spectrum - SPDtracklets08 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Omega^{-}+\bar{\Omega^{+}}$ transverse momentum spectrum - SPDtracklets08 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$K^{0}_{S}$ transverse momentum spectrum ratios to INEL>0 - SPDtracklets08 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum ratios to INEL>0 - SPDtracklets08 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Xi^{-}+\bar{\Xi^{+}}$ transverse momentum spectrum ratios to INEL>0 - SPDtracklets08 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Omega^{-}+\bar{\Omega^{+}}$ transverse momentum spectrum ratios to INEL>0 - SPDtracklets08 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$K^{0}_{S}$ transverse momentum spectrum - SPDtracklets0815 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum - SPDtracklets0815 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Xi^{-}+\bar{\Xi^{+}}$ transverse momentum spectrum - SPDtracklets0815 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Omega^{-}+\bar{\Omega^{+}}$ transverse momentum spectrum - SPDtracklets0815 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$K^{0}_{S}$ transverse momentum spectrum ratios to INEL>0 - SPDtracklets0815 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum ratios to INEL>0 - SPDtracklets0815 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Xi^{-}+\bar{\Xi^{+}}$ transverse momentum spectrum ratios to INEL>0 - SPDtracklets0815 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$\Omega^{-}+\bar{\Omega^{+}}$ transverse momentum spectrum ratios to INEL>0 - SPDtracklets0815 multiplicity classes. Total systematic uncertainties include both correlated and uncorrelated uncertainties across multiplicity. Uncorrelated systematic originating from the multiplicity dependence of the efficiency (2%) is not included.

$K^{0}_{S}$, $\Lambda+\bar{\Lambda}$, $\Xi^{-}+\bar{\Xi^{+}}$ average transverse momentum vs multiplicity - SPDtracklets08 multiplicity classes

$K^{0}_{S}$, $\Lambda+\bar{\Lambda}$, $\Xi^{-}+\bar{\Xi^{+}}$ average transverse momentum vs multiplicity - SPDtracklets0815 multiplicity classes

$K^{0}_{S}$, $\Lambda+\bar{\Lambda}$, $\Xi^{-}+\bar{\Xi^{+}}$ average transverse momentum vs multiplicity - V0M multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}$ average transverse momentum vs multiplicity - SPDtracklets08 multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}$ average transverse momentum vs multiplicity - SPDtracklets0815 multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}$ average transverse momentum vs multiplicity - V0M multiplicity classes

$K^{0}_{S}$, $\Lambda+\bar{\Lambda}$, $\Xi^{-}+\bar{\Xi^{+}}$ self-normalized yields vs self-normalized multiplicity - V0M multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}$ self-normalized yields vs self-normalized multiplicity - V0M multiplicity classes

$K^{0}_{S}$, $\Lambda+\bar{\Lambda}$, $\Xi^{-}+\bar{\Xi^{+}}$ self-normalized yields vs self-normalized multiplicity - SPDTracklets08 multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}$ self-normalized yields vs self-normalized multiplicity - SPDTracklets08 multiplicity classes

$K^{0}_{S}$, $\Lambda+\bar{\Lambda}$, $\Xi^{-}+\bar{\Xi^{+}}$ self-normalized yields vs self-normalized multiplicity - SPDTracklets0815 multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}$ self-normalized yields vs self-normalized multiplicity - SPDTracklets0815 multiplicity classes

$K^{0}_{S}$ transverse momentum spectra ratios SPDTracklets-to-V0M

$\Lambda+\bar{\Lambda}$ transverse momentum spectra ratios SPDTracklets-to-V0M

$\Xi^{-}+\bar{\Xi^{+}}$ transverse momentum spectra ratios SPDTracklets-to-V0M

$K^{0}_{S}$, $\Lambda+\bar{\Lambda}$, $\Xi^{-}+\bar{\Xi^{+}}$ integrated yields vs multiplicity - SPDtracklets08 multiplicity classes

$K^{0}_{S}$, $\Lambda+\bar{\Lambda}$, $\Xi^{-}+\bar{\Xi^{+}}$ integrated yields vs multiplicity - SPDtracklets0815 multiplicity classes

$K^{0}_{S}$, $\Lambda+\bar{\Lambda}$, $\Xi^{-}+\bar{\Xi^{+}}$ integrated yields vs multiplicity - V0M multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}$, $K^{0}_{S}$ integrated yields vs multiplicity - SPDtracklets08 multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}$, $K^{0}_{S}$ integrated yields vs multiplicity - SPDtracklets0815 multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}$, $K^{0}_{S}$ integrated yields vs multiplicity - V0M multiplicity classes

$K^{0}_{S}$, $\Lambda+\bar{\Lambda}$, $\Xi^{-}+\bar{\Xi^{+}}$ integrated yields (no extr.) vs multiplicity - SPDtracklets08 multiplicity classes

$K^{0}_{S}$, $\Lambda+\bar{\Lambda}$, $\Xi^{-}+\bar{\Xi^{+}}$ integrated yields (no extr.) vs multiplicity - SPDtracklets0815 multiplicity classes

$K^{0}_{S}$, $\Lambda+\bar{\Lambda}$, $\Xi^{-}+\bar{\Xi^{+}}$ integrated yields (no extr.) vs multiplicity - V0M multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}$ integrated yields (no extr.) vs multiplicity - SPDtracklets08 multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}$ integrated yields (no extr.) vs multiplicity - SPDtracklets0815 multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}$ integrated yields (no extr.) vs multiplicity - V0M multiplicity classes

$K^{0}_{S}$, $\Lambda+\bar{\Lambda}$, $\Xi^{-}+\bar{\Xi^{+}}$, $\Omega^{-}+\bar{\Omega^{+}}$ integrated yields - INEL>0. V0M multiplicity dependent yields are already listed in Table 8c.

$K^{0}_{S}$, $\Lambda+\bar{\Lambda}$, $\Xi^{-}+\bar{\Xi^{+}}$, $\Omega^{-}+\bar{\Omega^{+}}$ integrated yields - INEL>0. V0M multiplicity dependent yields at 7 TeV are listed in the corresponding repository ("https://www.hepdata.net/record/77284").

$\Lambda+\bar{\Lambda}/K^{0}_{S}$, $\Xi^{-}+\bar{\Xi^{+}}/K^{0}_{S}$ - Tracklets08 multiplicity classes

$\Lambda+\bar{\Lambda}/K^{0}_{S}$, $\Xi^{-}+\bar{\Xi^{+}}/K^{0}_{S}$ - Tracklets0815 multiplicity classes

$\Lambda+\bar{\Lambda}/K^{0}_{S}$, $\Xi^{-}+\bar{\Xi^{+}}/K^{0}_{S}$ - V0M multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}/K^{0}_{S}$ - Tracklets08 multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}/K^{0}_{S}$ - Tracklets0815 multiplicity classes

$\Omega^{-}+\bar{\Omega^{+}}/K^{0}_{S}$ - V0M multiplicity classes

$\overline{\mathrm{K}}$-p correlation function in p-p collisions at $\sqrt{s}=5$ TeV.

$\overline{\mathrm{K}}$-p correlation function in p-p collisions at $\sqrt{s}=7$ TeV.

$\overline{\mathrm{K}}$-p correlation function in p-p collisions at $\sqrt{s}=13$ TeV.

Combination of $\overline{\mathrm{K}}$-p correlation function in p-p collisions.

Exclusion plot for the $\Lambda$-$\Lambda$ scattering parameters (1$\sigma$ contour).

Exclusion plot for the $\Lambda$-$\Lambda$ scattering parameters (2$\sigma$ contour).

Exclusion plot for the $\Lambda$-$\Lambda$ scattering parameters (3$\sigma$ contour).

Exclusion plot for the $\Lambda$-$\Lambda$ binding energy (statistical uncertainty).

Exclusion plot for the $\Lambda$-$\Lambda$ binding energy (total uncertainty).

Charged jet differential cross sections without UE subtraction in pp collisions at $\sqrt{s}$ = 5.02 TeV with the leading track bias. All jets must contain at least one track with $p_{T}$ > 5 GeV/$c$. Statistical uncertainties are displayed as vertical error bars. The total systematic uncertainties are shown as shaded bands around the data points. Data are scaled to enhance visibility

$v_2\{4\}$ with 3-subevent method in pp collisions at $\sqrt{s} = 13$ TeV.

$v_2\{6\}$ in pp collisions at $\sqrt{s} = 13$ TeV.

SC$(4,2)$ with 3-subevent method in pp collisions at $\sqrt{s} = 13$ TeV.

SC$(3,2)$ with 3-subevent method in pp collisions at $\sqrt{s} = 13$ TeV.

SC$(4,2)$ with 3-subevent method divided with $\langle v_4\{2\}^2\rangle\langle v_2\{2\}^2\rangle$ with $|\Delta \eta| > 1.0$ and 1.4 in pp collisions at $\sqrt{s} = 13$ TeV.

SC$(3,2)$ with 3-subevent method divided with $\langle v_3\{2\}^2\rangle\langle v_2\{2\}^2\rangle$ with $|\Delta \eta| > 1.0$ and 1.4 in pp collisions at $\sqrt{s} = 13$ TeV.

$v_2\{2\}$ with $|\Delta \eta| > 1.4$ in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

$v_3\{2\}$ with $|\Delta \eta| > 1.0$ in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

$v_4\{2\}$ with $|\Delta \eta| > 1.0$ in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

$v_2\{4\}$ in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

$v_2\{4\}$ with 3-subevent method in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

$v_2\{6\}$ in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

SC$(4,2)$ with 3-subevent method in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

SC$(3,2)$ with 3-subevent method in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

SC$(4,2)$ with 3-subevent method divided with $\langle v_4\{2\}^2\rangle\langle v_2\{2\}^2\rangle$ with $|\Delta \eta| > 1.0$ and 1.4 in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

SC$(3,2)$ with 3-subevent method divided with $\langle v_3\{2\}^2\rangle\langle v_2\{2\}^2\rangle$ with $|\Delta \eta| > 1.0$ and 1.4 in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

$v_2\{2\}$ with $|\Delta \eta| > 1.4$ in Xe-Xe collisions at $\sqrt{s_{NN}} = 5.44$ TeV.

$v_3\{2\}$ with $|\Delta \eta| > 1.0$ in Xe-Xe collisions at $\sqrt{s_{NN}} = 5.44$ TeV.

$v_4\{2\}$ with $|\Delta \eta| > 1.0$ in Xe-Xe collisions at $\sqrt{s_{NN}} = 5.44$ TeV.

$v_2\{4\}$ in Xe-Xe collisions at $\sqrt{s_{NN}} = 5.44$ TeV.

$v_2\{4\}$ with 3-subevent method in Xe-Xe collisions at $\sqrt{s_{NN}} = 5.44$ TeV.

$v_2\{6\}$ in Xe-Xe collisions at $\sqrt{s_{NN}} = 5.44$ TeV.

$v_2\{8\}$ in Xe-Xe collisions at $\sqrt{s_{NN}} = 5.44$ TeV.

SC$(4,2)$ with 3-subevent method in Xe-Xe collisions at $\sqrt{s_{NN}} = 5.44$ TeV.

SC$(3,2)$ with 3-subevent method in Xe-Xe collisions at $\sqrt{s_{NN}} = 5.44$ TeV.

SC$(4,2)$ with 3-subevent method divided with $\langle v_4\{2\}^2\rangle\langle v_2\{2\}^2\rangle$ with $|\Delta \eta| > 1.0$ and 1.4 in Xe-Xe collisions at $\sqrt{s_{NN}} = 5.44$ TeV.

SC$(3,2)$ with 3-subevent method divided with $\langle v_3\{2\}^2\rangle\langle v_2\{2\}^2\rangle$ with $|\Delta \eta| > 1.0$ and 1.4 in Xe-Xe collisions at $\sqrt{s_{NN}} = 5.44$ TeV.

$v_2\{2\}$ with $|\Delta \eta| > 1.4$ in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

$v_3\{2\}$ with $|\Delta \eta| > 1.0$ in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

$v_4\{2\}$ with $|\Delta \eta| > 1.0$ in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

$v_2\{4\}$ in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

$v_2\{4\}$ with 3-subevent method in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

$v_2\{6\}$ in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

$v_2\{6\}$ with 2-subevent method in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

$v_2\{8\}$ in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

$v_2\{8\}$ with 2-subevent method in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

SC$(4,2)$ with 3-subevent method in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

SC$(3,2)$ with 3-subevent method in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

SC$(4,2)$ with 3-subevent method divided with $\langle v_4\{2\}^2\rangle\langle v_2\{2\}^2\rangle$ with $|\Delta \eta| > 1.0$ and 1.4 in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

SC$(3,2)$ with 3-subevent method divided with $\langle v_3\{2\}^2\rangle\langle v_2\{2\}^2\rangle$ with $|\Delta \eta| > 1.0$ and 1.4 in Pb-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV.

Differential production cross sections of $\psi(2S)$ as a function of rapidity.

$\psi(2S)$ over $J/\psi$ ratio as a function of $p_{\rm T}$.

$\psi(2S)$ over $J/\psi$ ratio as a function of y.

Differential production cross sections of $J/\psi$ as a function of $p_{\rm T}$.

Differential production cross sections of $J/\psi$ as a function of rapidity.

$J/\psi$ mean transversee momentum vs collision energy. $p_{\rm T}$ integration ranges are 0<$p_{\rm T}$<8 GeV/$c$ at $\sqrt{s}$ =2700 GeV, 0<$p_{\rm T}$<12 GeV/$c$ at $\sqrt{s}$ =5020, 0<$p_{\rm T}$<20 GeV/$c$ at $\sqrt{s}$ =7000, 0<$p_{\rm T}$<20 GeV/$c$ at $\sqrt{s}$ =8000 and 0<$p_{\rm T}$<20 GeV/$c$ at $\sqrt{s}$ =13000.

$J/\psi$ mean transversee momentum square vs collision energy. $p_{\rm T}$ integration ranges are 0<$p_{\rm T}$<8 GeV/$c$ at $\sqrt{s}$ =2700 GeV, 0<$p_{\rm T}$<12 GeV/$c$ at $\sqrt{s}$ =5020, 0<$p_{\rm T}$<20 GeV/$c$ at $\sqrt{s}$ =7000, 0<$p_{\rm T}$<20 GeV/$c$ at $\sqrt{s}$ =8000 and 0<$p_{\rm T}$<20 GeV/$c$ at $\sqrt{s}$ =13000.

$\psi(2S)$ mean transversee momentum vs collision energy. $p_{\rm T}$ integration ranges are 0<$p_{\rm T}$<12 GeV/$c$ at $\sqrt{s}$ =7000, 0<$p_{\rm T}$<12 GeV/$c$ at $\sqrt{s}$ =8000 and 0<$p_{\rm T}$<16 GeV/$c$ at $\sqrt{s}$ =13000.

$\psi(2S)$ mean transversee momentum square vs collision energy. $p_{\rm T}$ integration ranges are 0<$p_{\rm T}$<12 GeV/$c$ at $\sqrt{s}$ =7000, 0<$p_{\rm T}$<12 GeV/$c$ at $\sqrt{s}$ =8000 and 0<$p_{\rm T}$<16 GeV/$c$ at $\sqrt{s}$ =13000.

Differential production cross sections of $J/\psi$ vs collision energy.

Differential production cross sections of $\psi(2S)$ vs collision energy.