Ratio of inclusive $\psi(2{\rm S})$ over J/$\psi$ yields times their branching ratios as a function of $y_{\rm cms}$ in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV .The first uncertainty is statistical, while the second is the systematic.

Ratio of inclusive $\psi(2{\rm S})$ over J/$\psi$ yields times their branching ratios as a function of $p_{\rm T}$ in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV at forward rapidity.The first uncertainty is statistical, while the second is the systematic.

Ratio of inclusive $\psi(2{\rm S})$ over J/$\psi$ yields times their branching ratios as a function of $p_{\rm T}$ in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV at backward rapidity.The first uncertainty is statistical, while the second is the systematic.

Inclusive $\psi(2{\rm S})$ $R_{\rm pPb}$ values as a function of $y_{\rm {cms}}$ at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.

Inclusive $\psi(2{\rm S})$ $R_{\rm pPb}$ values as a function of $p_{\rm T}$ at $\sqrt{s_{\rm NN}}$ = 8.16 TeV at forward rapidity. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.

Inclusive $\psi(2{\rm S})$ $R_{\rm pPb}$ values as a function of $p_{\rm T}$ at $\sqrt{s_{\rm NN}}$ = 8.16 TeV at backward rapidity. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.

Double ratio of $\psi$(2S) and J/$\psi$ cross sections in p--Pb and pp collisions as a function of rapidity, at $\sqrt{s_{\mathrm{NN}}} = 8.16$ TeV. The first uncertainty is statistical, while the second is the systematic.

Double ratio of $\psi$(2S) and J/$\psi$ cross sections in p--Pb and pp collisions as a function of $p_{\rm T}$, at $\sqrt{s_{\mathrm{NN}}} = 8.16$ TeV at forward rapidity. The first uncertainty is statistical, while the second is the systematic.

Double ratio of $\psi$(2S) and J/$\psi$ cross sections in p--Pb and pp collisions as a function of $p_{\rm T}$, at $\sqrt{s_{\mathrm{NN}}} = 8.16$ TeV at backward rapidity. The first uncertainty is statistical, while the second is the systematic.

Inclusive $\psi(2{\rm S})$ cross section times branching ratio for backward and forward rapidity, in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.

Inclusive $\psi(2{\rm S})$ $R_{\rm pPb}$ values for backward and forward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a correlated systematic uncertainty.

Transverse momentum distributions of deuterons in the IV+V V0M multiplicity class

Transverse momentum distributions of deuterons in the VI V0M multiplicity class

Transverse momentum distributions of deuterons in the VII V0M multiplicity class

Transverse momentum distributions of deuterons in the IIX V0M multiplicity class

Transverse momentum distributions of deuterons in the IX V0M multiplicity class

Transverse momentum distributions of deuterons in the X V0M multiplicity class

Transverse momentum distributions of deuterons in the INEL>0 pp collisions

Transverse momentum distributions of deuterons in the INEL pp collisions

Transverse momentum distributions of anti-deuterons in the I V0M multiplicity class

Transverse momentum distributions of anti-deuterons in the II V0M multiplicity class

Transverse momentum distributions of anti-deuterons in the III V0M multiplicity class

Transverse momentum distributions of anti-deuterons in the IV+V V0M multiplicity class

Transverse momentum distributions of anti-deuterons in the VI V0M multiplicity class

Transverse momentum distributions of anti-deuterons in the VII V0M multiplicity class

Transverse momentum distributions of anti-deuterons in the IIX V0M multiplicity class

Transverse momentum distributions of anti-deuterons in the IX V0M multiplicity class

Transverse momentum distributions of anti-deuterons in the X V0M multiplicity class

Transverse momentum distributions of anti-deuterons in the INEL>0 pp collisions

Transverse momentum distributions of anti-deuterons in the INEL pp collisions

$\bar{d}$/d ratio as a function of transverse momentum in I V0M multiplicity class

$\bar{d}$/d ratio as a function of transverse momentum in II V0M multiplicity class

$\bar{d}$/d ratio as a function of transverse momentum in III V0M multiplicity class

$\bar{d}$/d ratio as a function of transverse momentum in IV+V V0M multiplicity class

$\bar{d}$/d ratio as a function of transverse momentum in VI V0M multiplicity class

$\bar{d}$/d ratio as a function of transverse momentum in VII V0M multiplicity class

$\bar{d}$/d ratio as a function of transverse momentum in IIX V0M multiplicity class

$\bar{d}$/d ratio as a function of transverse momentum in IX V0M multiplicity class

$\bar{d}$/d ratio as a function of transverse momentum in X V0M multiplicity class

$\bar{d}$/d ratio as a function of transverse momentum in INEL>0 pp collisions

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the I V0M multiplicity class V0M multiplicity class

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the II V0M multiplicity class V0M multiplicity class

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the III V0M multiplicity class V0M multiplicity class

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the IV+V V0M multiplicity class V0M multiplicity class

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the VI V0M multiplicity class V0M multiplicity class

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the VII V0M multiplicity class V0M multiplicity class

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the IIX V0M multiplicity class V0M multiplicity class

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the IX V0M multiplicity class V0M multiplicity class

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the X V0M multiplicity class V0M multiplicity class

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the INEL>0 pp collisions V0M multiplicity class

Deuteron over proton ratio in pp collisions as a function of the charged particle multiplicity density ad mid-rapidity

$K^{+} + K^{-}$ transverse momentum spectra in V0M multilpicity classes

$p + \bar{p}$ transverse momentum spectra in V0M multilpicity classes

$p + \bar{p}$ transverse momentum spectra in V0M multilpicity classes

$\pi^{+} + \pi^{-}$ transverse momentum spectra ratios, V0M multiplicity classes to INEL>0

$\pi^{+} + \pi^{-}$ transverse momentum spectra ratios, V0M multiplicity classes to INEL>0

$K^{+} + K^{-}$ transverse momentum spectra ratios, V0M multiplicity classes to INEL>0

$K^{+} + K^{-}$ transverse momentum spectra ratios, V0M multiplicity classes to INEL>0

$p + \bar{p}$ transverse momentum spectra ratios, V0M multiplicity classes to INEL>0

$p + \bar{p}$ transverse momentum spectra ratios, V0M multiplicity classes to INEL>0

Transverse momentum dependence of ($K^{+} + K^{-}$)/($\pi^{+} + \pi^{-}$) and ($p + \bar{p}$)/($\pi^{+} + \pi^{-}$) ratios in low-$p_T$ interval in pp collisions as a function of $\langle dN_{ch}/d\eta\rangle_{|\eta|<0.5}$

Transverse momentum dependence of ($K^{+} + K^{-}$)/($\pi^{+} + \pi^{-}$) and ($p + \bar{p}$)/($\pi^{+} + \pi^{-}$) ratios in mid-$p_T$ interval in pp collisions as a function of $\langle dN_{ch}/d\eta\rangle_{|\eta|<0.5}$

Transverse momentum dependence of ($K^{+} + K^{-}$)/($\pi^{+} + \pi^{-}$) and ($p + \bar{p}$)/($\pi^{+} + \pi^{-}$) ratios in high-$p_T$ interval in pp collisions as a function of $\langle dN_{ch}/d\eta\rangle_{|\eta|<0.5}$

Blast-wave fit parameters

$p_{T}$-integrated ($K^{+} + K^{-}$)/($\pi^{+} + \pi^{-}$) and ($p + \bar{p}$)/($\pi^{+} + \pi^{-}$) ratios in pp collisions as a function of $\langle dN_{ch}/d\eta\rangle_{|\eta|<0.5}$

$p_{T}$-integrated (multi)strange hadron to pion ratios in pp collisions as a function of $\langle dN_{ch}/d\eta\rangle_{|\eta|<0.5}$

$p_{T}$-integrated ($\Omega^{-} + \bar{\Omega}^{+}$)/($\pi^{+} + \pi^{-}$) ratios in pp collisions as a function of $\langle dN_{ch}/d\eta\rangle_{|\eta|<0.5}$

Average transverse momentum of $\pi^{+} + \pi^{-}$, $K^{+} + K^{-}$, and $p + \bar{p}$ as a function of $\langle dN_{ch}/d\eta\rangle_{|\eta|<0.5}$

Transverse momentum spectra ratios ($K^{+} + K^{-}$)/($\pi^{+} + \pi^{-}$) in V0M multiplicity classes

Transverse momentum spectra ratios ($K^{+} + K^{-}$)/($\pi^{+} + \pi^{-}$) in V0M multiplicity classes

Transverse momentum spectra ratios ($p + \bar{p}$)/($\pi^{+} + \pi^{-}$) in V0M multiplicity classes

Transverse momentum spectra ratios ($p + \bar{p}$)/($\pi^{+} + \pi^{-}$) in V0M multiplicity classes

Centrality dependence of flow harmonics from $v_2$ to $v_9$.

Centrality dependence of flow harmonics from $v_2$ to $v_9$.

Centrality dependence of flow harmonics from $v_2$ to $v_9$.

Centrality dependence of flow harmonics from $v_2$ to $v_9$.

Centrality dependence of flow harmonics from $v_2$ to $v_9$.

Centrality dependence of linear and non-linear flow modes.

Centrality dependence of linear and non-linear flow modes.

Centrality dependence of linear and non-linear flow modes.

Centrality dependence of linear and non-linear flow modes.

Centrality dependence of linear and non-linear flow modes.

Centrality dependence of linear and non-linear flow modes.

Centrality dependence of symmetry-plane correlations.

Centrality dependence of symmetry-plane correlations.

Centrality dependence of symmetry-plane correlations.

Centrality dependence of symmetry-plane correlations.

Centrality dependence of non-linear flow mode coefficients.

Centrality dependence of non-linear flow mode coefficients.

Centrality dependence of non-linear flow mode coefficients.

Centrality dependence of non-linear flow mode coefficients.

Centrality dependence of non-linear flow mode coefficients.

$p_{\rm T}$-differential invariant cross section of electrons from heavy-flavour hadron decays in p--Pb collisions in 40--60\% centrality

$p_{\rm T}$-differential invariant cross section of electrons from heavy-flavour hadron decays in p--Pb collisions in 60--100\% centrality

HFe $R_{\rm pPb}$ in p--Pb

HFe $Q_{\rm pPb}$ in p--Pb, 0--20\% centrality

HFe $Q_{\rm pPb}$ in p--Pb, 20--40\% centrality

HFe $Q_{\rm pPb}$ in p--Pb, 40--60\% centrality

HFe $Q_{\rm pPb}$ in p--Pb, 60--100\% centrality

HFe $Q_{\rm cp}$ in p--Pb, 0--20\% centrality

HFe $Q_{\rm cp}$ in p--Pb, 20--40\% centrality

HFe $Q_{\rm cp}$ in p--Pb, 40--60\% centrality

Comparison of the azimuthal-correlation distributions of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) with $16 < p_{\rm T} < 24$ GeV/$c$ and charged particles with $p_{\rm T} > 0.3$ GeV/$c$, in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, after baseline subtraction. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi < \pi$.

Comparison of the azimuthal-correlation distributions of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) with $3 < p_{\rm T} < 5$ GeV/$c$ and charged particles with $0.3 < p_{\rm T} < 1.0$ GeV/$c$, in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, after baseline subtraction. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi < \pi$.

Comparison of the azimuthal-correlation distributions of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) with $5 < p_{\rm T} < 8$ GeV/$c$ and charged particles with $0.3 < p_{\rm T} < 1.0$, in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, after baseline subtraction. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi < \pi$.

Comparison of the azimuthal-correlation distributions of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) with $8 < p_{\rm T} < 16$ GeV/$c$ and charged particles with $0.3 < p_{\rm T} < 1.0$ GeV/$c$, in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, after baseline subtraction. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi < \pi$.

Comparison of the azimuthal-correlation distributions of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) with $16 < p_{\rm T} < 24$ GeV/$c$ and charged particles with $0.3 < p_{\rm T} < 1.0$ GeV/$c$, in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, after baseline subtraction. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi < \pi$.

Comparison of the azimuthal-correlation distributions of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) with $3 < p_{\rm T} < 5$ GeV/$c$ and charged particles with $1.0 < p_{\rm T} < 2.0$ GeV/$c$, in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, after baseline subtraction. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi < \pi$.

Comparison of the azimuthal-correlation distributions of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) with $5 < p_{\rm T} < 8$ GeV/$c$ and charged particles with $1.0 < p_{\rm T} < 2.0$ GeV/$c$, in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, after baseline subtraction. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi < \pi$.

Comparison of the azimuthal-correlation distributions of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) with $8 < p_{\rm T} < 16$ GeV/$c$ and charged particles with $1.0 < p_{\rm T} < 2.0$ GeV/$c$, in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, after baseline subtraction. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi < \pi$.

Comparison of the azimuthal-correlation distributions of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) with $16 < p_{\rm T} < 24$ GeV/$c$ and charged particles with $1.0 < p_{\rm T} < 2.0$ GeV/$c$, in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, after baseline subtraction. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi < \pi$.

Comparison of the azimuthal-correlation distributions of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) with $3 < p_{\rm T} < 5$ GeV/$c$ and charged particles with $2.0 < p_{\rm T} < 3.0$ GeV/$c$, in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, after baseline subtraction. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi < \pi$.

Comparison of the azimuthal-correlation distributions of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) with $5 < p_{\rm T} < 8$ GeV/$c$ and charged particles with $2.0 < p_{\rm T} < 3.0$ GeV/$c$, in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, after baseline subtraction. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi < \pi$.

Comparison of the azimuthal-correlation distributions of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) with $8 < p_{\rm T} < 16$ GeV/$c$ and charged particles with $2.0 < p_{\rm T} < 3.0$ GeV/$c$, in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, after baseline subtraction. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi < \pi$.

Comparison of the azimuthal-correlation distributions of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) with $16 < p_{\rm T} < 24$ GeV/$c$ and charged particles with $2.0 < p_{\rm T} < 3.0$ GeV/$c$, in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, after baseline subtraction. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi < \pi$.

Comparison of the near-side associated peak yields measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $p_{\rm T} > 0.3$ GeV/$c$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the near-side associated peak yields measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $0.3 < p_{\rm T} < 1.0$ GeV/$c$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the near-side associated peak yields measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $1.0 < p_{\rm T} < 2.0$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the near-side associated peak yields measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $2.0 < p_{\rm T} < 3.0$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the near-side associated peak width measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $p_{\rm T} > 0.3$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the near-side associated peak width measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $0.3 < p_{\rm T} < 1.0$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the near-side associated peak width measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $1.0 < p_{\rm T} < 2.0$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the near-side associated peak width measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $2.0 < p_{\rm T} < 3.0$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the away-side associated peak yields measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $p_{\rm T} > 0.3$ GeV/$c$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the away-side associated peak yields measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $0.3 < p_{\rm T} < 1.0$ GeV/$c$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the away-side associated peak yields measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $1.0 < p_{\rm T} < 2.0$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the away-side associated peak yields measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $2.0 < p_{\rm T} < 3.0$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the away-side associated peak width measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $p_{\rm T} > 0.3$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the away-side associated peak width measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $0.3 < p_{\rm T} < 1.0$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the away-side associated peak width measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $1.0 < p_{\rm T} < 2.0$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the away-side associated peak width measured in pp collisions at $\sqrt{s} = 5.02$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $2.0 < p_{\rm T} < 3.0$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp, $-0.96 < y^{\rm D}_{\rm cms} < 0.04$ in p-Pb. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Azimuthal-correlation distributions of D mesons and charged particles obtained for D$^0$, D$^{+}$ and D$^{*+}$ mesons for $3 < p_{\rm T} < 5$ GeV/$c$, charged particles $p_{\rm T} > 0.3$ GeV/$c$, in p-Pb collisions at $\sqrt{s} = 5.02$ TeV in 0-20%, 20-60% and 60-100% centrality classes. Rapidity range for the D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi< \pi$.

Azimuthal-correlation distributions of D mesons and charged particles obtained for D$^0$, D$^{+}$ and D$^{*+}$ mesons for $5 < p_{\rm T} < 8$ GeV/$c$, charged particles $p_{\rm T} > 0.3$ GeV/$c$, in p-Pb collisions at $\sqrt{s} = 5.02$ TeV in 0-20%, 20-60% and 60-100% centrality classes. Rapidity range for the D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi< \pi$.

Azimuthal-correlation distributions of D mesons and charged particles obtained for D$^0$, D$^{+}$ and D$^{*+}$ mesons for $8 < p_{\rm T} < 16$ GeV/$c$, charged particles $p_{\rm T} > 0.3$ GeV/$c$, in p-Pb collisions at $\sqrt{s} = 5.02$ TeV in 0-20%, 20-60% and 60-100% centrality classes. Rapidity range for the D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi< \pi$.

Azimuthal-correlation distributions of D mesons and charged particles obtained for D$^0$, D$^{+}$ and D$^{*+}$ mesons for $3 < p_{\rm T} < 5$ GeV/$c$, charged particles $0.3 < p_{\rm T}< 1.0$ GeV/$c$, in p-Pb collisions at $\sqrt{s} = 5.02$ TeV in 0-20%, 20-60% and 60-100% centrality classes. Rapidity range for the D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi< \pi$.

Azimuthal-correlation distributions of D mesons and charged particles obtained for D$^0$, D$^{+}$ and D$^{*+}$ mesons for $5 < p_{\rm T} < 8$ GeV/$c$, charged particles $0.3 < p_{\rm T}< 1.0$ GeV/$c$, in p-Pb collisions at $\sqrt{s} = 5.02$ TeV in 0-20%, 20-60% and 60-100% centrality classes. Rapidity range for the D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi< \pi$.

Azimuthal-correlation distributions of D mesons and charged particles obtained for D$^0$, D$^{+}$ and D$^{*+}$ mesons for $8 < p_{\rm T} < 16$ GeV/$c$, charged particles $0.3 < p_{\rm T}< 1.0$ GeV/$c$, in p-Pb collisions at $\sqrt{s} = 5.02$ TeV in 0-20%, 20-60% and 60-100% centrality classes. Rapidity range for the D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi< \pi$.

Azimuthal-correlation distributions of D mesons and charged particles obtained for D$^0$, D$^{+}$ and D$^{*+}$ mesons for $3 < p_{\rm T} < 5$ GeV/$c$, charged particles $p_{\rm T}> 1.0$ GeV/$c$, in p-Pb collisions at $\sqrt{s} = 5.02$ TeV in 0-20% and 60-100% centrality classes. Rapidity range for the D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi< \pi$.

Azimuthal-correlation distributions of D mesons and charged particles obtained for D$^0$, D$^{+}$ and D$^{*+}$ mesons for $5 < p_{\rm T} < 8$ GeV/$c$, charged particles $p_{\rm T}> 1.0$ GeV/$c$, in p-Pb collisions at $\sqrt{s} = 5.02$ TeV in 0-20%, 20-60% and 60-100% centrality classes. Rapidity range for the D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi< \pi$.

Azimuthal-correlation distributions of D mesons and charged particles obtained for D$^0$, D$^{+}$ and D$^{*+}$ mesons for $8 < p_{\rm T} < 16$ GeV/$c$, charged particles $p_{\rm T}> 1.0$ GeV/$c$, in p-Pb collisions at $\sqrt{s} = 5.02$ TeV in 0-20%, 20-60% and 60-100% centrality classes. Rapidity range for the D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$. The azimuthal-correlation distributions are reported in the range $0 < \Delta\varphi< \pi$.

Comparison of the near-side associated peak yields measured in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV in 0-20%, 20-60% and 60-100% centrality classes, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $p_{\rm T} > 0.3$ GeV/$c$. The rapidity range of D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the near-side associated peak yields measured in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV in 0-20%, 20-60% and 60-100% centrality classes, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $0.3 < p_{\rm T} < 1.0$ GeV/$c$. The rapidity range of D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the near-side associated peak yields measured in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV in 0-20%, 20-60% and 60-100% centrality classes, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $p_{\rm T} > 1.0$ GeV/$c$. The rapidity range of D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the near-side peak widths measured in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV in 0-20%, 20-60% and 60-100% centrality classes, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $p_{\rm T} > 0.3$ GeV/$c$. The rapidity range of D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the near-side peak widths measured in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV in 0-20%, 20-60% and 60-100% centrality classes, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $0.3 < p_{\rm T} < 1.0$ GeV/$c$. The rapidity range of D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Comparison of the near-side peak widths measured in p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV in 0-20%, 20-60% and 60-100% centrality classes, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $p_{\rm T} > 1.0$ GeV/$c$. The rapidity range of D mesons is $-0.96 < y^{\rm D}_{\rm cms} < 0.04$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Baseline height measured in pp collisions at $\sqrt{s} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $p_{\rm T} > 0.3$ GeV/$c$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Baseline height measured in pp collisions at $\sqrt{s} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $0.3 < p_{\rm T} < 1.0$ GeV/$c$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Baseline height measured in pp collisions at $\sqrt{s} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $1.0 < p_{\rm T} < 2.0$ GeV/$c$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Baseline height measured in pp collisions at $\sqrt{s} = 5.02$ TeV, for correlations of D mesons (average of D$^{0}$, D$^{+}$, D$^{*+}$) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated particle $2.0 < p_{\rm T} < 3.0$ GeV/$c$. Rapidity range for the D mesons are $|y^{\rm D}_{\rm cms}| < 0.5$ in pp. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

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%

$cos\theta^{*}$ 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.