Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $5 < p_{\rm T} < 8~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ ($-0.96 < y_{\rm cms} < 0.04$) and charged particles with $p_{\rm T} > 0.3~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp (p-Pb) collisions at $\sqrt{s} = 7~{\rm TeV}$ ($\sqrt{s_{\rm NN}} = 5.02~{\rm TeV}$).

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $8 < p_{\rm T} < 16~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ ($-0.96 < y_{\rm cms} < 0.04$) and charged particles with $p_{\rm T} > 0.3~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp (p-Pb) collisions at $\sqrt{s} = 7~{\rm TeV}$ ($\sqrt{s_{\rm NN}} = 5.02~{\rm TeV}$).

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $3 < p_{\rm T} < 5~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ and charged particles with $0.3 < p_{\rm T} < 1~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp collisions at $\sqrt{s} = 7~{\rm TeV}$.

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $5 < p_{\rm T} < 8~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ ($-0.96 < y_{\rm cms} < 0.04$) and charged particles with $0.3 < p_{\rm T} < 1~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp (p-Pb) collisions at $\sqrt{s} = 7~{\rm TeV}$ ($\sqrt{s_{\rm NN}} = 5.02~{\rm TeV}$).

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $8 < p_{\rm T} < 16~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ ($-0.96 < y_{\rm cms} < 0.04$) and charged particles with $0.3 < p_{\rm T} < 1~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp (p-Pb) collisions at $\sqrt{s} = 7~{\rm TeV}$ ($\sqrt{s_{\rm NN}} = 5.02~{\rm TeV}$).

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $3 < p_{\rm T} < 5~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ and charged particles with $p_{\rm T} > 1~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp collisions at $\sqrt{s} = 7~{\rm TeV}$.

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $5 < p_{\rm T} < 8~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ ($-0.96 < y_{\rm cms} < 0.04$) and charged particles with $p_{\rm T} > 1~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp (p-Pb) collisions at $\sqrt{s} = 7~{\rm TeV}$ ($\sqrt{s_{\rm NN}} = 5.02~{\rm TeV}$).

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $8 < p_{\rm T} < 16~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ ($-0.96 < y_{\rm cms} < 0.04$) and charged particles with $p_{\rm T} > 1~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp (p-Pb) collisions at $\sqrt{s} = 7~{\rm TeV}$ ($\sqrt{s_{\rm NN}} = 5.02~{\rm TeV}$).

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 $p_{\rm T} > 0.3$ GeV/$c$, in pp collisions at $\sqrt{s} = 7$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV. 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 $p_{\rm T} > 0.3$ GeV/$c$, in pp collisions at $\sqrt{s} = 7$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV. 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 $0.3 < p_{\rm T} < 1$ GeV/$c$, in pp collisions at $\sqrt{s} = 7$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV. 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 $0.3 < p_{\rm T} < 1$ GeV/$c$, in pp collisions at $\sqrt{s} = 7$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV. 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 $p_{\rm T} > 1$ GeV/$c$, in pp collisions at $\sqrt{s} = 7$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV. 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 $p_{\rm T} > 1$ GeV/$c$, in pp collisions at $\sqrt{s} = 7$ TeV and p-Pb collisions at $\sqrt{s_{NN}} = 5.02$ TeV. 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 $0 < \Delta\varphi < \pi$.

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $3 < p_{\rm T} < 5~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ and charged particles with $p_{\rm T} > 0.3~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp collisions at $\sqrt{s} = 7~{\rm TeV}$. The points are shown after the subtraction of the baseline of the distribution, which is defined as the physical minimum of the distribution and estimated from the weighted average of the points in the transverse region ($\pi/4 < |\Delta\varphi| < \pi/2$).

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $5 < p_{\rm T} < 8~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ and charged particles with $p_{\rm T} > 0.3~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp collisions at $\sqrt{s} = 7~{\rm TeV}$. The points are shown after the subtraction of the baseline of the distribution, which is defined as the physical minimum of the distribution and estimated from the weighted average of the points in the transverse region ($\pi/4 < |\Delta\varphi| < \pi/2$).

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $8 < p_{\rm T} < 16~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ and charged particles with $p_{\rm T} > 0.3~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp collisions at $\sqrt{s} = 7~{\rm TeV}$. The points are shown after the subtraction of the baseline of the distribution, which is defined as the physical minimum of the distribution and estimated from the weighted average of the points in the transverse region ($\pi/4 < |\Delta\varphi| < \pi/2$).

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $3 < p_{\rm T} < 5~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ and charged particles with $0.3 < p_{\rm T} < 1~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp collisions at $\sqrt{s} = 7~{\rm TeV}$. The points are shown after the subtraction of the baseline of the distribution, which is defined as the physical minimum of the distribution and estimated from the weighted average of the points in the transverse region ($\pi/4 < |\Delta\varphi| < \pi/2$).

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $5 < p_{\rm T} < 8~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ and charged particles with $0.3 < p_{\rm T} < 1~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp collisions at $\sqrt{s} = 7~{\rm TeV}$. The points are shown after the subtraction of the baseline of the distribution, which is defined as the physical minimum of the distribution and estimated from the weighted average of the points in the transverse region ($\pi/4 < |\Delta\varphi| < \pi/2$).

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $8 < p_{\rm T} < 16~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ and charged particles with $0.3 < p_{\rm T} < 1~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp collisions at $\sqrt{s} = 7~{\rm TeV}$. The points are shown after the subtraction of the baseline of the distribution, which is defined as the physical minimum of the distribution and estimated from the weighted average of the points in the transverse region ($\pi/4 < |\Delta\varphi| < \pi/2$).

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $3 < p_{\rm T} < 5~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ and charged particles with $p_{\rm T} > 1~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp collisions at $\sqrt{s} = 7~{\rm TeV}$. The points are shown after the subtraction of the baseline of the distribution, which is defined as the physical minimum of the distribution and estimated from the weighted average of the points in the transverse region ($\pi/4 < |\Delta\varphi| < \pi/2$).

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $5 < p_{\rm T} < 8~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ and charged particles with $p_{\rm T} > 1~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp collisions at $\sqrt{s} = 7~{\rm TeV}$. The points are shown after the subtraction of the baseline of the distribution, which is defined as the physical minimum of the distribution and estimated from the weighted average of the points in the transverse region ($\pi/4 < |\Delta\varphi| < \pi/2$).

Azimuthal correlation of D mesons (${\rm D}^{0}$, ${\rm D}^{+}$, ${\rm D}^{*+}$ average) with $8 < p_{\rm T} < 16~{\rm GeV}/c$ and $|y_{\rm cms}| < 0.5$ and charged particles with $p_{\rm T} > 1~{\rm GeV}/c$ for $|\Delta\eta| = |\eta_{\rm ch}-\eta_{\rm D}| < 1$ measured in pp collisions at $\sqrt{s} = 7~{\rm TeV}$. The points are shown after the subtraction of the baseline of the distribution, which is defined as the physical minimum of the distribution and estimated from the weighted average of the points in the transverse region ($\pi/4 < |\Delta\varphi| < \pi/2$).

Near-side-peak associated yield values measured in pp collisions at $\sqrt{s} = 7$ TeV, for correlations of D mesons (D$^{0}$, D$^{+}$, D$^{*+}$ average) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated track $p_{\rm T} > 0.3$ GeV/$c$. Rapidity range for the D mesons is $|y^{\rm D}_{\rm cms}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Near-side-peak associated yield values measured in pp collisions at $\sqrt{s} = 7$ TeV, for correlations of D mesons (D$^{0}$, D$^{+}$, D$^{*+}$ average) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated track $0.3 < p_{\rm T} < 1$ GeV/$c$. Rapidity range for the D mesons is $|y^{\rm D}_{\rm cms}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Near-side-peak associated yield values measured in pp collisions at $\sqrt{s} = 7$ TeV, for correlations of D mesons (D$^{0}$, D$^{+}$, D$^{*+}$ average) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated track $p_{\rm T} > 1$ GeV/$c$. Rapidity range for the D mesons is $|y^{\rm D}_{\rm cms}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Near-side-peak width values measured in pp collisions at $\sqrt{s} = 7$ TeV, for correlations of D mesons (D$^{0}$, D$^{+}$, D$^{*+}$ average) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated track $p_{\rm T} > 0.3$ GeV/$c$. Rapidity range for the D mesons is $|y^{\rm D}_{\rm cms}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Near-side-peak width values measured in pp collisions at $\sqrt{s} = 7$ TeV, for correlations of D mesons (D$^{0}$, D$^{+}$, D$^{*+}$ average) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated track $0.3 < p_{\rm T} < 1$ GeV/$c$. Rapidity range for the D mesons is $|y^{\rm D}_{\rm cms}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Near-side-peak width values measured in pp collisions at $\sqrt{s} = 7$ TeV, for correlations of D mesons (D$^{0}$, D$^{+}$, D$^{*+}$ average) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated track $p_{\rm T} > 1$ GeV/$c$. Rapidity range for the D mesons is $|y^{\rm D}_{\rm cms}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Baseline values measured in pp collisions at $\sqrt{s} = 7$ TeV, for correlations of D mesons (D$^{0}$, D$^{+}$, D$^{*+}$ average) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated track $p_{\rm T} > 0.3$ GeV/$c$. Rapidity range for the D mesons is $|y^{\rm D}_{\rm cms}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Baseline values measured in pp collisions at $\sqrt{s} = 7$ TeV, for correlations of D mesons (D$^{0}$, D$^{+}$, D$^{*+}$ average) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated track $0.3 < p_{\rm T} < 1$ GeV/$c$. Rapidity range for the D mesons is $|y^{\rm D}_{\rm cms}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

Baseline values measured in pp collisions at $\sqrt{s} = 7$ TeV, for correlations of D mesons (D$^{0}$, D$^{+}$, D$^{*+}$ average) and charged particles, as a function of the D-meson $p_{\rm T}$, for associated track $p_{\rm T} > 1$ GeV/$c$. Rapidity range for the D mesons is $|y^{\rm D}_{\rm cms}| < 0.5$. Correlations are integrated for $|\Delta\eta|=|\eta_{\rm ch}-\eta_{\rm D}| < 1$.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

d$\sigma$/dy for non-prompt J/$\psi$ in p-Pb collisions at $\sqrt{s_NN}=5.02 TeV$

d$^2\sigma$/d$y$d$p_{\rm T}$ in bins of $p_T^{J/\psi}$ for non-prompt J/$\psi$ in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. The data point in the first $p_{\rm T}$ bin is un upper limit at 95% Confidence Level.

Nuclear modification factor ($R_{pPb}$) in bins of $p_T^{J/\psi}$ for non-prompt J/$\psi$ in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV. The data point in the first $p_{\rm T}$ bin is un upper limit at 95% Confidence Level.

Nuclear modification factor ($R_{pPb}$) for non-prompt J/$\psi$ integrated over $p_{\rm T}$ in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV at mid-rapidity.

d$^2\sigma$/d $p_{\rm{T}}$dy versus $p_T^{J/\psi}$ for prompt J/$\psi$ in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

Nuclear modification factor ($R_{pPb}$) in bins of $p_T^{J/\psi}$ for prompt J/$\psi$ in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

Nuclear modification factor ($R_{pPb}$) for prompt J/$\psi$ integrated over $p_{\rm T}$ in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV at mid-rapidity.

Beauty production cross section at mid-rapidity (d$sigma$/d$y$) in p-Pb collisions at $\sqrt{s_{NN}}$ = 5.02 TeV.

d$\sigma$/dy for prompt J/$\psi$ in p-Pb collisions at $\sqrt{s_NN}=5.02 TeV$ integrated over $p_{\rm T}$>0.

Transverse momentum dependence of inclusive J/$\psi$ $v_2$ at $\sqrt{s_{\rm NN}}=5.02$ TeV for the 40-60% centrality class (forward rapidity). The first uncertainty (stat) is statistical, the second (sys,uncorrel) is the uncorrelated systematic, while the third one (sys,correl) is a $p_{\rm T}$-correlated systematic uncertainty.

Variance of near-side peak in the 0-10% centrality bin divided by the variance of the near-side peak in the 50-80% centrality bin.

Depletion yield calculated by taking the difference of the fit and the data, and normalized by the total yield of the peak.

RFB of inclusive JPSI(1S) in p-Pb collisions as a function of relative charged-particle pseudorapidity density.

Relative mean transverse momentum of JPSI(1S) mesons for backward rapidity as a function of the relative charged-particle pseudorapidity density.

Relative mean transverse momentum of JPSI(1S) mesons for forward rapidity as a function of the relative charged-particle pseudorapidity density.

$y$-differential production cross section of $\phi$ in p-Pb at $\sqrt{s_{\rm NN}}$=5.02 TeV, in $p_{\rm T}$ range 2.03 < $p_{\rm T}$ < 3.53

Centrality dependence of observables SC(5,3) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables SC(4,3) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables SC(4,3) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(5,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(5,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(5,3) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(5,3) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,3) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,3) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(3,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables SC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(3,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables NSC(4,2) in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_2$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_3$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Transeverse momemtum dependence of observables $v_4$ in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables $v_5$ in Pb-Pb collisions at 2.76 TeV.

Centrality dependence of observables $v_5$ in Pb-Pb collisions at 2.76 TeV.

$v_2$ vs. $p_{\rm T}$ of $D_s^+$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$=5.02 TeV in the centrality class 30-50% in the rapidity interval |$y$|<0.8. The second (sys) error is the systematic uncertainty from the B feed-down contribution. The first (sys) error is the systematic uncertainty from the other sources.

$v_2$ vs. $p_{\rm T}$ of $D^0$, $D^+$, $D^{*+}$ mesons in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$=5.02 TeV in the centrality class 30-50% in the rapidity interval |$y$|<0.8. The second (sys) error is the systematic uncertainty from the B feed-down contribution. The first (sys) error is the systematic uncertainty from the other sources.

$p_{\rm T}$-differential cross section of prompt $\rm{D_{s}}$ mesons in pp collisions at $\sqrt{s_{\rm{NN}}}$=7 TeV in the rapidity interval $|y|$<0.5. Branching ratio of $\rm{D_{s}}\rightarrow\phi\pi\rightarrow K K \pi$ : 0.0227.

Ratio of $\rm {D}^{+}$ to $\rm{D}^{0}$ meson yield in pp collisions at $\sqrt{s_{\rm{NN}}}$=7 TeV in -0.5 $<y<$ 0.5 as a function of $p_{\rm T}$. Branching ratio of $\rm{D^{+}}\rightarrow K\pi\pi$ : 0.0946. Branching ratio of $\rm{D^{0}}\rightarrow K\pi$ : 0.0393.

Ratio of $\rm {D}^{*+}$ to $\rm{D}^{0}$ meson yield in pp collisions at $\sqrt{s_{\rm{NN}}}$=7 TeV in -0.5 $<y<$ 0.5 as a function of $p_{\rm T}$. Branching ratio of $\rm D^{+-}\rightarrow K{\rm{\pi}}{\rm{\pi}}$: 0.0393*0.677. Branching ratio of $\rm{D^{0}}\rightarrow K\pi$ : 0.0393.

Ratio of $\rm {D}_{s}$ to $\rm{D}^{0}$ meson yield in pp collisions at $\sqrt{s_{\rm{NN}}}$=7 TeV in -0.5 $<y<$ 0.5 as a function of $p_{\rm T}$. Branching ratio of $\rm{D_s}\rightarrow \phi \pi \rightarrow KK\pi$ : 0.0227. Branching ratio of $\rm{D^{0}}\rightarrow K\pi$ : 0.0393.

Ratio of $\rm {D}_{s}$ to $\rm {D}^{+}$ meson yield in pp collisions at $\sqrt{s_{\rm{NN}}}$=7 TeV in -0.5 $<y<$ 0.5 as a function of $p_{\rm T}$. Branching ratio of $\rm{D_s}\rightarrow \phi \pi \rightarrow KK\pi$ : 0.0227. Branching ratio of $\rm{D^{+}}\rightarrow K\pi\pi$ : 0.0946.

Production cross sections per unit of rapidity for prompt $\rm{D}^{0}$ mesons at mid-rapidity in pp collisions at 7 TeV. The second (sys) error is from the luminosity uncertainty, the third (sys) error is from the branching-ratio uncertainty.

Production cross sections per unit of rapidity for prompt $\rm{D}^{+}$ mesons at mid-rapidity in pp collisions at 7 TeV. The second (sys) error is from the luminosity uncertainty, the third (sys) error is from the branching-ratio uncertainty.

Production cross sections per unit of rapidity for prompt $\rm D^{*+}$ mesons at mid-rapidity in pp collisions at 7 TeV. The second (sys) error is from the luminosity uncertainty, the third (sys) error is from the branching-ratio uncertainty.

Production cross sections per unit of rapidity for prompt $\rm D_{s}$) mesons at mid-rapidity in pp collisions at 7 TeV. The second (sys) error is from the luminosity uncertainty, the third (sys) error is from the branching-ratio uncertainty.

Production cross sections per unit of rapidity for charm quarks at mid-rapidity in pp collisions at 7 TeV. The second (sys) error is from the luminosity uncertainty, the third (sys) error is from the Fragmentation Function uncertainties, the fourth (sys) error is from the rapidity shapes of D0 mesons and single charm quarks.

value of <$p_{\rm T}$> of prompt $\rm{D}^{0}$ mesons in |$y$|<0.5. The first uncertainty is statistical, the second is the systematic uncertainty.

Total production cross sections, extrapolated to the full phase space, for prompt D0 mesons. The second (sys) error is the from the extrapolation uncertainty, the third from the luminosity uncertainty and the fourth from the branching-ratio uncertainties.

Total production cross sections, extrapolated to the full phase space, for charm quarks. The second (sys) error is from the extrapolation, the third is from the luminosity uncertainty and the fourth is from the Fragmentation Function uncertainties.