Invariant yield of K$^{*0}$ meson for 5-10$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Invariant yield of K$^{*0}$ meson for 10-20$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Invariant yield of K$^{*0}$ meson for 20-30$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Invariant yield of K$^{*0}$ meson for 30-40$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Invariant yield of K$^{*0}$ meson for 40-50$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Invariant yield of $\phi$ meson for 0-5$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Invariant yield of $\phi$ meson for 5-10$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Invariant yield of $\phi$ meson for 10-20$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Invariant yield of $\phi$ meson for 20-30$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Invariant yield of $\phi$ meson for 30-40$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Invariant yield of $\phi$ meson for 40-50$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Invariant yield of $\phi$ meson for 60-80$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

K$^{*0}$/K ratio as a function of $p_{\rm T}$ for 0-5$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

K$^{*0}$/K ratio as a function of $p_{\rm T}$ for inelastic (INEL) pp collisions at $\sqrt{s}=2.76~{\rm TeV}$.

$\phi$/K ratio as a function of $p_{\rm T}$ for 0-5$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

$\phi$/K ratio as a function of $p_{\rm T}$ for inelastic (INEL) pp collisions at $\sqrt{s}=2.76~{\rm TeV}$.

K$^{*0}/\pi$ ratio as a function of $p_{\rm T}$ for 0-5$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

K$^{*0}/\pi$ ratio as a function of $p_{\rm T}$ for inelastic (INEL) pp collisions at $\sqrt{s}=2.76~{\rm TeV}$.

$\phi$/$\pi$ ratio as a function of $p_{\rm T}$ for 0-5$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$

$\phi$/$\pi$ ratio as a function of $p_{\rm T}$ for inelastic (INEL) pp collisions at $\sqrt{s}=2.76~{\rm TeV}$.

p/K$^{*0}$ ratio as a function of $p_{\rm T}$ for 0-5$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

p/K$^{*0}$ ratio as a function of $p_{\rm T}$ for 60-80$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

p/K$^{*0}$ ratio as a function of $p_{\rm T}$ for inelastic (INEL) pp collisions at $\sqrt{s}=2.76~{\rm TeV}$.

p/$\phi$ ratio as a function of $p_{\rm T}$ for 0-5$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

p/$\phi$ ratio as a function of $p_{\rm T}$ for 60-80$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

p/$\phi$ ratio as a function of $p_{\rm T}$ for inelastic (INEL) pp collisions at $\sqrt{s}=2.76~{\rm TeV}$.

Nuclear modification factor of average $K^{*0}$ and $\overline{K^{*0}}$ as a function of $p_{\rm T}$ for 0-5$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Nuclear modification factor of average $K^{*0}$ and $\overline{K^{*0}}$ as a function of $p_{\rm T}$ for 5-10$\%$ in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Nuclear modification factor of average $K^{*0}$ and $\overline{K^{*0}}$ as a function of $p_{\rm T}$ for 20-30$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Nuclear modification factor of average $K^{*0}$ and $\overline{K^{*0}}$ as a function of $p_{\rm T}$ for 40-50$\%$ centrality in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Nuclear modification factor of $\phi$ as a function of $p_{\rm T}$ for 0-5$\%$ in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Nuclear modification factor of $\phi$ as a function of $p_{\rm T}$ for 5-10$\%$ in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Nuclear modification factor of $\phi$ as a function of $p_{\rm T}$ for 20-30$\%$ in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Nuclear modification factor of $\phi$ as a function of $p_{\rm T}$ for 40-50$\%$ in Pb-Pb collisions at $\sqrt{s_{\rm NN}}=2.76~{\rm TeV}$.

Corrected Delta_{recoil} distribution of recoil jets with R=0.4 measured for p-Pb collisions at sqrt{s_{NN}} = 5.02 TeV with event activity V0A 0-20%.

Corrected Delta_{recoil} distribution of recoil jets with R=0.4 measured for p-Pb collisions at sqrt{s_{NN}} = 5.02 TeV with event activity V0A 50-100%.

Corrected Delta_{recoil} distribution of recoil jets with R=0.2 measured for p-Pb collisions at sqrt{s_{NN}} = 5.02 TeV without imposing event activity bias.

Corrected Delta_{recoil} distribution of recoil jets with R=0.2 measured for p-Pb collisions at sqrt{s_{NN}} = 5.02 TeV with event activity ZNA 0-20%.

Corrected Delta_{recoil} distribution of recoil jets with R=0.2 measured for p-Pb collisions at sqrt{s_{NN}} = 5.02 TeV with event activity ZNA 50-100%.

Corrected Delta_{recoil} distribution of recoil jets with R=0.2 measured for p-Pb collisions at sqrt{s_{NN}} = 5.02 TeV with event activity V0A 0-20%.

Corrected Delta_{recoil} distribution of recoil jets with R=0.2 measured for p-Pb collisions at sqrt{s_{NN}} = 5.02 TeV with event activity V0A 50-100%.

Ratio of event activity biased Delta_{recoil} distributions corresponding to recoil jets with R=0.4.

Ratio of event activity biased Delta_{recoil} distributions corresponding to recoil jets with R=0.4.

Ratio of event activity biased Delta_{recoil} distributions corresponding to recoil jets with R=0.2.

Ratio of event activity biased Delta_{recoil} distributions corresponding to recoil jets with R=0.2.

Invariant yields of the $\eta$ meson in the centrality class 20-50% in Pb-Pb collisions at sqrt{s_NN} = 2.76 TeV at mid-rapidity.

Nuclear modification factor R_AA of $\pi^{0}$ produced in 0-10% central Pb-Pb collisions at sqrt{s_NN} = 2.76 TeV at mid-rapidity, T_AA uncertainty of 3.25% and uncertainty of \sigma_{inel} of 3.9% included in systematic uncertainties.

Nuclear modification factor R_AA of $\pi^{0}$ produced in 20-50% central Pb-Pb collisions at sqrt{s_NN} = 2.76 TeV at mid-rapidity, T_AA uncertainty of 3.3% and uncertainty of \sigma_{inel} of 3.9% included in systematic uncertainties.

Nuclear modification factor R_AA of $\eta$ produced in 0-10% central Pb-Pb collisions at sqrt{s_NN} = 2.76 TeV at mid-rapidity, T_AA uncertainty of 3.25% and uncertainty of \sigma_{inel} of 3.9% included in systematic uncertainties.

Nuclear modification factor R_AA of $\eta$ produced in 20-50% central Pb-Pb collisions at sqrt{s_NN} = 2.76 TeV at mid-rapidity, T_AA uncertainty of 3.3% and uncertainty of \sigma_{inel} of 3.9% included in systematic uncertainties.

Ratio of the $\eta$ to $\pi^{0}$ invariant yields in 0-10% central Pb-Pb collisions at sqrt{s_NN} = 2.76 TeV at mid-rapidity.

Ratio of the $\eta$ to $\pi^{0}$ invariant yields in 20-50% central Pb-Pb collisions at sqrt{s_NN} = 2.76 TeV at mid-rapidity.

pT-differential nuclear modification factor of heavy-flavour decay muons at forward rapidity (proton-going side)

pT-differential nuclear modification factor of heavy-flavour decay muons at backward rapidity (Pb-going side)

pT-differential forward-to-backward ratio of heavy-flavour decay muons

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 $|\Delta\eta| =|\eta_{\rm ch}-\eta_{\rm D}|< 1$.

$K^{0}_{S}$ transverse momentum spectrum: V0M Class IV (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class V (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class VI (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class VII (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class VIII (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class IX (pp at $\sqrt{s}=7$ TeV).

$K^{0}_{S}$ transverse momentum spectrum: V0M Class X (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class I (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class II (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class III (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class IV (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class V (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class VI (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class VII (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class VIII (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class IX (pp at $\sqrt{s}=7$ TeV).

$\Lambda+\bar{\Lambda}$ transverse momentum spectrum: V0M Class X (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class I (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class II (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class III (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class IV (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class V (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class VI (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class VII (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class VIII (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class IX (pp at $\sqrt{s}=7$ TeV).

$\Xi^{-}+\bar{\Xi}^{+}$ transverse momentum spectrum: V0M Class X (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class I+II (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class III+IV (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class V+VI (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class VII+VIII (pp at $\sqrt{s}=7$ TeV).

$\Omega^{-}+\bar{\Omega}^{+}$ transverse momentum spectrum: V0M Class IX+X (pp at $\sqrt{s}=7$ TeV).

$2K^{0}_{S}/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.

$(\Lambda+\bar{\Lambda})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.

$(\Xi^{-}+\bar{\Xi}^{+})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.

$(\Omega^{-}+\bar{\Omega}^{+})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of the average charged particle multiplicity density at midrapidity.

$\pi^{+}+\pi^{-}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$p+\bar{p}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$K^{0}_{S}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$\Lambda+\bar{\Lambda}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$\Xi^{-}+\bar{\Xi}^{+}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$\Omega^{-}+\bar{\Omega}^{+}$ integrated yields, pp at $\sqrt{s}=7$ TeV (V0M Multiplicity Classes).

$(\Lambda+\bar{\Lambda})/2K^{0}_{S}$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of charged particle multiplicity density at midrapidity.

$(p+\bar{p})/(\pi^{+}+\pi^{-})$ ratio for pp collisions at $\sqrt{s}=7$ TeV as a function of charged particle multiplicity density at midrapidity.

$(2K^{0}_{S})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.

$(\Lambda+\bar{\Lambda})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.

$(\Xi^{-}+\bar{\Xi}^{+})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.

$(\Omega^{-}+\bar{\Omega}^{+})/(\pi^{+}+\pi^{-})$ double-ratio vs multiplicity for pp collisions at $\sqrt{s}=7$ TeV.

Event multiplicity classes, their corresponding fraction of the INEL>0 cross-section and their corresponding average charged particle density at midrapidity ($|\eta|<0.5$). The value of in the inclusive (INEL>0) class is 5.96 $\pm$ 0.23. The uncertainties are the quadratic sum of statistical and systematic contributions.

ALICE inclusive J/psi polarization parameters lambda_theta in the helicity frame as a function of p_T in pp collisions at sqrt{s} = 8 TeV in the rapidity interval 2.5 < y < 4.0. The error bars represent the total uncertainties.

ALICE inclusive J/psi polarization parameters lambda_phi in the helicity frame as a function of p_T in pp collisions at sqrt{s} = 8 TeV in the rapidity interval 2.5 < y < 4.0. The error bars represent the total uncertainties.

ALICE inclusive J/psi polarization parameters lambda_thetaphi in the helicity frame as a function of p_T in pp collisions at sqrt{s} = 8 TeV in the rapidity interval 2.5 < y < 4.0. The error bars represent the total uncertainties.

ALICE inclusive J/psi frame-invariant quantity \widetilde{\lambda} in the Collins-Soper frame as a function of p_T in pp collisions at sqrt{s} = 8 TeV in the rapidity interval 2.5 < y < 4.0. The error bars represent the total uncertainties.

ALICE inclusive J/psi frame-invariant quantity \widetilde{\lambda} in the helicity frame as a function of p_T in pp collisions at sqrt{s} = 8 TeV in the rapidity interval 2.5 < y < 4.0. The error bars represent the total uncertainties.

Contour plot (68% CL) of ALICE inclusive J/psi average pT-integrated (3 < pT < 15 GeV/c in the rapidity interval 2.5 < y < 4.0) polarisation parameters in the plane (<lambda_theta>, <lambda_phi>) in the Collins-Soper frame in pp collisions at sqrt{s} = 8 TeV . The error bars represent the total uncertainties.

Contour plot (95% CL) of ALICE inclusive J/psi average pT-integrated (3 < pT < 15 GeV/c in the rapidity interval 2.5 < y < 4.0) polarisation parameters in the plane (<lambda_theta>, <lambda_phi>) in the Collins-Soper frame in pp collisions at sqrt{s} = 8 TeV . The error bars represent the total uncertainties.

Contour plot (68% CL) of ALICE inclusive J/psi average pT-integrated (3 < pT < 15 GeV/c in the rapidity interval 2.5 < y < 4.0) polarisation parameters in the plane (<lambda_theta>, <lambda_phi>) in the helicity frame in pp collisions at sqrt{s} = 8 TeV . The error bars represent the total uncertainties.

Contour plot (95% CL) of ALICE inclusive J/psi average pT-integrated (3 < pT < 15 GeV/c in the rapidity interval 2.5 < y < 4.0) polarisation parameters in the plane (<lambda_theta>, <lambda_phi>) in the helicity frame in pp collisions at sqrt{s} = 8 TeV . The error bars represent the total uncertainties.

Contour plot (68% CL) of ALICE inclusive J/psi average pT-integrated (3 < pT < 15 GeV/c in the rapidity interval 2.5 < y < 4.0) polarisation parameters in the plane (<lambda_theta>, <lambda_thetaphi>) in the Collins-Soper frame in pp collisions at sqrt{s} = 8 TeV . The error bars represent the total uncertainties.

Contour plot (95% CL) of ALICE inclusive J/psi average pT-integrated (3 < pT < 15 GeV/c in the rapidity interval 2.5 < y < 4.0) polarisation parameters in the plane (<lambda_theta>, <lambda_thetaphi>) in the Collins-Soper frame in pp collisions at sqrt{s} = 8 TeV . The error bars represent the total uncertainties.

Contour plot (68% CL) of ALICE inclusive J/psi average pT-integrated (3 < pT < 15 GeV/c in the rapidity interval 2.5 < y < 4.0) polarisation parameters in the plane (<lambda_theta>, <lambda_thetaphi>) in the helicity frame in pp collisions at sqrt{s} = 8 TeV . The error bars represent the total uncertainties.

Contour plot (95% CL) of ALICE inclusive J/psi average pT-integrated (3 < pT < 15 GeV/c in the rapidity interval 2.5 < y < 4.0) polarisation parameters in the plane (<lambda_theta>, <lambda_thetaphi>) in the helicity frame in pp collisions at sqrt{s} = 8 TeV . The error bars represent the total uncertainties.

Contour plot (68% CL) of ALICE inclusive J/psi average pT-integrated (3 < pT < 15 GeV/c in the rapidity interval 2.5 < y < 4.0) polarisation parameters in the plane (<lambda_phi>, <lambda_thetaphi>) in the Collins-Soper frame in pp collisions at sqrt{s} = 8 TeV . The error bars represent the total uncertainties.

Contour plot (95% CL) of ALICE inclusive J/psi average pT-integrated (3 < pT < 15 GeV/c in the rapidity interval 2.5 < y < 4.0) polarisation parameters in the plane (<lambda_phi>, <lambda_thetaphi>) in the Collins-Soper frame in pp collisions at sqrt{s} = 8 TeV . The error bars represent the total uncertainties.

Contour plot (68% CL) of ALICE inclusive J/psi average pT-integrated (3 < pT < 15 GeV/c in the rapidity interval 2.5 < y < 4.0) polarisation parameters in the plane (<lambda_phi>, <lambda_thetaphi>) in the helicity frame in pp collisions at sqrt{s} = 8 TeV . The error bars represent the total uncertainties.

Contour plot (95% CL) of ALICE inclusive J/psi average pT-integrated (3 < pT < 15 GeV/c in the rapidity interval 2.5 < y < 4.0) polarisation parameters in the plane (<lambda_theta>, <lambda_thetaphi>) in the helicity frame in pp collisions at sqrt{s} = 8 TeV . The error bars represent the total uncertainties.

Invariant differential cross section of $\eta$ produced in inelastic pp collisions at center of mass energy 8 TeV, the uncertainty of $\sigma_{MB}$ of 2.6% is not included in the systematic error.

Integrated yields of $\pi^0$ mesons produced in inelastic pp collisions at center-of-mass energies of 2.76 and 8 TeV. The uncertainties of $\sigma_{MB}$ of $^{+3.9\%}_{-6.4\%}(model)\pm2.0(lumi)$% for $\sqrt{s}=2.76$ TeV and $\pm2.3$% for 8 TeV are not included in the systematic error.

Integrated yields of $\pi^{0}$ mesons produced in inelastic pp collisions at center of mass energies of 2.76 and 8 TeV. The uncertainty of $\sigma_{MB}$ of $^{+3.9\%}_{-6.4\%}(model)\pm2.0(lumi)$% for $\sqrt{s}=2.76$ TeV and $\pm2.3$% for 8 TeV is not included in the systematic error.

Integrated yields of $\eta$ mesons produced in inelastic pp collisions at center-of-mass energies of 2.76 and 8 TeV. The uncertainties of $\sigma_{MB}$ of $^{+3.9\%}_{-6.4\%}(model)\pm2.0(lumi)$% for $\sqrt{s}=2.76$ TeV and $\pm2.3$% for 8 TeV are not included in the systematic error.

Integrated yields of $\eta$ mesons produced in inelastic pp collisions at center of mass energies of 2.76 and 8 TeV. The uncertainty of $\sigma_{MB}$ of $^{+3.9\%}_{-6.4\%}(model)\pm2.0(lumi)$% for $\sqrt{s}=2.76$ TeV and $\pm2.3$% for 8 TeV is not included in the systematic error.

Integrated $\eta$/$\pi^0$ ratio produced in inelastic pp collisions at center-of-mass energies of 2.76 and 8 TeV.

Integrated $\eta$/$\pi^{0}$ ratio produced in inelastic pp collisions at center of mass energies of 2.76 and 8 TeV.

Mean transverse momenta $\langle p_\text{T}\rangle$ of $\pi^0$ mesons produced in inelastic pp collisions at center-of-mass energies of 2.76 and 8 TeV. The uncertainties of $\sigma_{MB}$ of $^{+3.9\%}_{-6.4\%}(model)\pm2.0(lumi)$% for $\sqrt{s}=2.76$ TeV and $\pm2.3$% for 8 TeV are not included in the systematic error.

Mean transverse momenta $\langle p_\text{T}\rangle$ of $\pi^{0}$ mesons produced in inelastic pp collisions at center of mass energies of 2.76 and 8 TeV. The uncertainty of $\sigma_{MB}$ of $^{+3.9\%}_{-6.4\%}(model)\pm2.0(lumi)$% for $\sqrt{s}=2.76$ TeV and $\pm2.3$% for 8 TeV is not included in the systematic error.

Mean transverse momenta $\langle p_\text{T}\rangle$ of $\eta$ mesons produced in inelastic pp collisions at center-of-mass energies of 2.76 and 8 TeV. The uncertainties of $\sigma_{MB}$ of $^{+3.9\%}_{-6.4\%}(model)\pm2.0(lumi)$% for $\sqrt{s}=2.76$ TeV and $\pm2.3$% for 8 TeV are not included in the systematic error.

Mean transverse momenta $\langle p_\text{T}\rangle$ of $\eta$ mesons produced in inelastic pp collisions at center of mass energies of 2.76 and 8 TeV. The uncertainty of $\sigma_{MB}$ of $^{+3.9\%}_{-6.4\%}(model)\pm2.0(lumi)$% for $\sqrt{s}=2.76$ TeV and $\pm2.3$% for 8 TeV is not included in the systematic error.

The measured ratio of cross sections for inclusive $\eta$ to $\pi^0$ production at a centre-of-mass energy of 8 TeV.

The measured ratio of cross sections for inclusive $\eta$ to $\pi^{0}$ production at a center of mass energy of 8 TeV.

The rapidity dependence of the inclusive JPsi nuclear modification factor obtained in p-Pb and Pb-p collisions. The first uncertainty is statistical, the second one is the uncorrelated systematic uncertainty, while the third is a global uncertainty common to p-Pb and Pb-p results.

The pt-differential inclusive JPsi nuclear modification factor obtained in Pb-p collisions. The first uncertainty is statistical, the second one is the uncorrelated systematic uncertainty, while the third one is the global uncertainty common to all the pT values.

The pt-differential inclusive JPsi nuclear modification factor obtained in p-Pb collisions. The first uncertainty is statistical, the second one is the uncorrelated systematic uncertainty, while the third one is the global uncertainty common to all the pT values.

The forward to backward ratio RFB of the inclusive JPsi nuclear modification factors. The first uncertainty is statistical, the second one is systematic.

The pT dependence of the forward to backward ratio RFB of the inclusive JPsi nuclear modification factors. The first uncertainty is statistical, while the second is the systematic uncertainty.