$p_{\rm T}$-distributions of $\phi$ meson measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{\rm T}$-integrated yield ratio of $\rm{K}^{*0}$ (average of particle and anti-particle) to K (average of particle and anti-particle) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{\rm T}$-integrated yield ratio of $\rm{K}^{*0}$ (average of particle and anti-particle) to K (average of particle and anti-particle) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{\rm T}$-integrated yield ratio of $\phi$ to K (average of particle and anti-particle) measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{\rm T}$-integrated yield ratio of $\phi$ to K (average of particle and anti-particle) measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{\rm T}$ differential ratio $(\rm{K}^{*0} + \bar{\rm{K}}^{*0}) / (\rm{K}^{+}+\rm{K}^{-})$ measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{\rm T}$ differential ratio $(\rm{K}^{*0} + \bar{\rm{K}}^{*0}) / (\rm{K}^{+}+\rm{K}^{-})$ measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{\rm T}$ differential ratio $(2\phi) / (\rm{K}^{+}+\rm{K}^{-})$ measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{\rm T}$ differential ratio $(2\phi) / (\rm{K}^{+}+\rm{K}^{-})$ measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{\rm T}$ differential ratio $(\rm{K}^{*0} + \bar{\rm{K}}^{*0}) / (\pi^{+}+\pi^{-})$ measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{\rm T}$ differential ratio $(\rm{K}^{*0} + \bar{\rm{K}}^{*0}) / (\pi^{+}+\pi^{-})$ measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{\rm T}$ differential ratio $(2\phi) / (\pi^{+}+\pi^{-})$ measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{\rm T}$ differential ratio $(2\phi) / (\pi^{+}+\pi^{-})$ measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{\rm T}$ differential ratio $(\rm{p} + \bar{\rm p}) / (\rm{K}^{*0} + \bar{\rm{K}}^{*0})$ measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{\rm T}$ differential ratio $(\rm{p} + \bar{\rm p}) / (\rm{K}^{*0} + \bar{\rm{K}}^{*0})$ measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$p_{\rm T}$ differential ratio $(\rm{p} + \bar{\rm p}) / (2\phi)$ measured in Pb-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

$p_{\rm T}$ differential ratio $(\rm{p} + \bar{\rm p}) / (2\phi)$ measured in pp collisions at $\sqrt{s}$ = 5.02 TeV.

$^3\overline{\mathrm{H}} /\,^3\mathrm{H}$ ratio in $\mathrm{INEL}>0$ p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

Transverse momentum spectra obtained from the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for $\mathrm{INEL}>0$ events in p$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

Transverse momentum spectra obtained from the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for events in 0$-$10% multiplicity class in p$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

Transverse momentum spectra obtained from the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for events in 10$-$20% multiplicity class in p$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

Transverse momentum spectra obtained from the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for events in 20$-$40% multiplicity class in p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

Transverse momentum spectra obtained from the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for events in 40$-$100% multiplicity class in p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

Mean transverse momentum obtained from the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ as a function of the mean charged-particle multiplicity density in p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$ TeV

$(^3\mathrm{He} +\,^3\overline{\mathrm{He}}) / (\mathrm{p} + \overline{\mathrm{p}})$ ratio in p$-$Pb as a function of the mean charged-particle multiplicity density

$(^3\mathrm{H} +\,^3\overline{\mathrm{H}}) / (\mathrm{p} + \overline{\mathrm{p}})$ ratio in p$-$Pb as a function of the mean charged-particle multiplicity density

Coalescence parameter $B_3$ calculated using the average of $\mathrm{INEL}>0$ $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ yields

Coalescence parameter $B_3$ calculated using the average of $\mathrm{INEL}>0$ $^3\mathrm{H}$ and $^3\overline{\mathrm{H}}$ yields

Ratio of (anti-)$^3$H and (anti-)$^3$He yields

Coalescence parameter $B_3$ calculated using the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for $\mathrm{INEL}>0$ events in p$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

Coalescence parameter $B_3$ calculated using the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for events in 0$-$10% multiplicity class in p$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

Coalescence parameter $B_3$ calculated using the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for events in 10$-$20% multiplicity class in p$-$Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

Coalescence parameter $B_3$ calculated using the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for events in 20$-$40% multiplicity class in p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

Coalescence parameter $B_3$ calculated using the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for events in 40$-$100% multiplicity class in p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

Integrated production yield obtained from the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ corrected for the spin degeneracy factor $(2J +1)$ for minimum-bias p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

Upper limit on the integrated production yield of $^4\overline{\mathrm{He}}$ at 90$\%$ confidence level corrected for the spin degeneracy factor $(2J +1)$ for minimum-bias p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

Integrated production yield obtained from the average of $^3\mathrm{He}$ and $^3\overline{\mathrm{He}}$ for the different multiplicity classes and $\mathrm{INEL} > 0$ p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

Integrated production yield obtained from the average of $^3\mathrm{H}$ and $^3\overline{\mathrm{H}}$ for $\mathrm{INEL} > 0$ p--Pb collisions at $\sqrt{s_\mathrm{NN}} = 5.02$

$\Upsilon$(1S) differential cross section as a function of $p_{\rm T}$, at forward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV .The first uncertainty is statistical, while the second is the systematic.

$\Upsilon$(1S) differential cross section as a function of $p_{\rm T}$, at backward rapidity at $\sqrt{s_{\rm NN}}$ = 8.16 TeV .The first uncertainty is statistical, while the second is the systematic.

Ratio of $\Upsilon$(2S) over $\Upsilon$(1S) yields 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 $\Upsilon$(3S) over $\Upsilon$(1S) yields in p--Pb collisions at $\sqrt{s_{\rm NN}}$ = 8.16 TeV .The first uncertainty is statistical, while the second is the systematic.

$\Upsilon$(1S) $R_{\rm pPb}$ values 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.

$\Upsilon$(1S) $R_{\rm pPb}$ 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.

$\Upsilon$(1S) $R_{\rm pPb}$ as a function of $p_{\rm T}$ at backward 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.

$\Upsilon$(1S) $R_{\rm pPb}$ as a function of $p_{\rm T}$ at 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.

$\Upsilon$(1S) $Q_{\rm pPb}$ as a function of $<N_{\rm coll}>$ at backward 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.

$\Upsilon$(1S) $Q_{\rm pPb}$ as a function of $<N_{\rm coll}>$ at 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.

$\Upsilon$(1S) $R_{\rm pPb}$ values 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.

$\Upsilon$(2S) $R_{\rm pPb}$ values 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.

$\Upsilon$(3S) $R_{\rm pPb}$ values 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.

Ratio of $\Upsilon$(2S) to $\Upsilon$(1S) $R_{\rm pPb}$ at $\sqrt{s_{\rm NN}}$ = 8.16 TeV as a function of $y_{\rm cms}$ .The first uncertainty is statistical, while the second is the systematic.

Ratio of $\Upsilon$(3S) to $\Upsilon$(1S) $R_{\rm pPb}$ at $\sqrt{s_{\rm NN}}$ = 8.16 TeV as a function of $y_{\rm cms}$ .The first uncertainty is statistical, while the second is the systematic.

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

Measured second cumulants of anti-protons.

Measured first cumulants of protons.

Measured first cumulants of anti-protons.

Measured R1 values.

Measured R2 values.

R2 values from Model.

R1 values vs. delaY.

Global baryon number conservation.

Local baryon number conservation, deltaY_corr = 5.

Local baryon number conservation, deltaY_corr = 2.

HIJING results.

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%

The widths of near-side peaks for trigger jets in-plane, mid-plane, and out-of-plane vs $p_{T}^{assoc}$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions. The background uncertainty is non-trivially correlated point-to-point. The correlated systematic uncertainties come from the shape uncertainty of the acceptance correction.

The widths of away-side peaks for trigger jets in-plane, mid-plane, and out-of-plane vs $p_{T}^{assoc}$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions. The background uncertainty is non-trivially correlated point-to-point. The correlated systematic uncertainties come from the shape uncertainty of the acceptance correction.

Background subtracted correlation functions for $1.0<p_{T}^{assoc}<1.5$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Background subtracted correlation functions for $1.5<p_{T}^{assoc}<2.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Background subtracted correlation functions for $2.0<p_{T}^{assoc}<3.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Background subtracted correlation functions for $3.0<p_{T}^{assoc}<4.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Background subtracted correlation functions for $4.0<p_{T}^{assoc}<5.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Background subtracted correlation functions for $5.0<p_{T}^{assoc}<6.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Background subtracted correlation functions for $6.0<p_{T}^{assoc}<10.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in background dominated region for $1.0<p_{T}^{assoc}<1.5$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in background dominated region for $1.5<p_{T}^{assoc}<2.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in background dominated region for $2.0<p_{T}^{assoc}<3.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in background dominated region for $3.0<p_{T}^{assoc}<4.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in background dominated region for $4.0<p_{T}^{assoc}<5.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in background dominated region for $5.0<p_{T}^{assoc}<6.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in background dominated region for $6.0<p_{T}^{assoc}<10.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.0<p_{T}^{assoc}<1.5$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.5<p_{T}^{assoc}<2.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $2.0<p_{T}^{assoc}<3.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $3.0<p_{T}^{assoc}<4.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $4.0<p_{T}^{assoc}<5.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $5.0<p_{T}^{assoc}<6.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $6.0<p_{T}^{assoc}<10.0$ GeV/$c$ for $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Response matrices for all jets with kinematic cuts described in the paper for 30-50% centrality in Pb-Pb collisions

Response matrices for in-plane jets with kinematic cuts described in the paper for 30-50% centrality in Pb-Pb collisions

Response matrices for mid-plane jets with kinematic cuts described in the paper for 30-50% centrality in Pb-Pb collisions

Response matrices for out-of-plane jets with kinematic cuts described in the paper for 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.0<p_{T}^{assoc}<1.5$ GeV/$c$ for in-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.0<p_{T}^{assoc}<1.5$ GeV/$c$ for mid-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.0<p_{T}^{assoc}<1.5$ GeV/$c$ for out-of-planes $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.0<p_{T}^{assoc}<1.5$ GeV/$c$ for all $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.5<p_{T}^{assoc}<2.0$ GeV/$c$ for in-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.5<p_{T}^{assoc}<2.0$ GeV/$c$ for mid-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.5<p_{T}^{assoc}<2.0$ GeV/$c$ for out-of-planes $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $1.5<p_{T}^{assoc}<2.0$ GeV/$c$ for all $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $2.0<p_{T}^{assoc}<3.0$ GeV/$c$ for in-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $2.0<p_{T}^{assoc}<3.0$ GeV/$c$ for mid-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $2.0<p_{T}^{assoc}<3.0$ GeV/$c$ for out-of-planes $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $2.0<p_{T}^{assoc}<3.0$ GeV/$c$ for all $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $3.0<p_{T}^{assoc}<4.0$ GeV/$c$ for in-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $3.0<p_{T}^{assoc}<4.0$ GeV/$c$ for mid-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $3.0<p_{T}^{assoc}<4.0$ GeV/$c$ for out-of-planes $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $3.0<p_{T}^{assoc}<4.0$ GeV/$c$ for all $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $4.0<p_{T}^{assoc}<5.0$ GeV/$c$ for in-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $4.0<p_{T}^{assoc}<5.0$ GeV/$c$ for mid-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $4.0<p_{T}^{assoc}<5.0$ GeV/$c$ for out-of-planes $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $4.0<p_{T}^{assoc}<5.0$ GeV/$c$ for all $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $5.0<p_{T}^{assoc}<6.0$ GeV/$c$ for in-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $5.0<p_{T}^{assoc}<6.0$ GeV/$c$ for mid-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $5.0<p_{T}^{assoc}<6.0$ GeV/$c$ for out-of-planes $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $5.0<p_{T}^{assoc}<6.0$ GeV/$c$ for all $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $6.0<p_{T}^{assoc}<10.0$ GeV/$c$ for in-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $6.0<p_{T}^{assoc}<10.0$ GeV/$c$ for mid-plane $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $6.0<p_{T}^{assoc}<10.0$ GeV/$c$ for out-of-planes $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

Correlation functions in signal plus background region for $6.0<p_{T}^{assoc}<10.0$ GeV/$c$ for all $20<p_T^{jet}<40$ GeV/$c$ full jets of 30-50% centrality in Pb-Pb collisions

$cos\theta^{*}$ 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.