$\Upsilon$(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.

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

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

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.

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

$^3\overline{\mathrm{H}} /\,^3\mathrm{H}$ 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 $\sqrt{s_\mathrm{NN}} = 5.02$

$p_{\rm T}$-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.

Inclusive J/$\psi$ nuclear modification factor $R_{\rm AA}$ at midrapidity, integrated over $p_{\rm T}$, as a function of mean number of participating nucleons in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV. The correlated systematic uncertainty due to the pp reference is not included and amounts to 6.9%, shown as the red box around unity in the paper figure.

Inclusive J/$\psi$ nuclear modification factor $R_{\rm AA}$ at midrapidity for $p_{\rm T} > 0.15$ GeV as a function of mean number of participating nucleons in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV. The low-$p_{\rm T}$ interval is removed to reject J/$\psi$ from photo-production. The correlated systematic uncertainty due to the pp reference cross section is not listed and amounts to 6.9%, shown as the red box around unity in the paper figure.

Inclusive J/$\psi$ nuclear modification factor, $R_{\rm AA}$, at midrapidity in Pb$-$Pb collisions at $\sqrt{s_{\rm NN}} = 5.02$ TeV as a function of transverse momentum, $p_{\rm T}$, for different centrality intervals. The systematic uncertianty from the pp reference, which is correlated with centrality and shown as grey band in the paper figure, is listed as sys,Reference. The systematic uncertainties on the $T_{\rm AA}$ which are correlated in $p_{\rm T}$ for each centrality bin are not listed and amount additionally to 2\%, 3\%, and 5\% for 0-20\%, 20-40\%, and 40-90\% centrality, respectively. These uncertainties are shown as boxes around unity in the paper figure.

Nuclear modification factor $R_{\rm AA}$ of inclusive J/$\psi$ at mid-rapidity. For the midrapidity point all normalization uncertainties are included.

Near side ($|\Delta\varphi| < \pi/2$) longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ for central (0-5%) Pb--Pb collisions at $\sqrt{s_{\rm NN}}=2.76\;\text{TeV}$. Systematic uncertainty on the long-range mean correlator strength $\delta B = 6.9\times 10^{-4}$.

Near side ($|\Delta\varphi| < \pi/2$) longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ for semi-central (30-40%) Pb--Pb collisions at $\sqrt{s_{\rm NN}}=2.76\;\text{TeV}$. Systematic uncertainty on the long-range mean correlator strength $\delta B = 3.8\times 10^{-3}$.

Near side ($|\Delta\varphi| < \pi/2$) longitudinal projection of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ for perippheral (70-80%) Pb--Pb collisions at $\sqrt{s_{\rm NN}}=2.76\;\text{TeV}$. Systematic uncertainty on the long-range mean correlator strength $\delta B = 5.5\times 10^{-2}$.

Azimuthal projection ($|\Delta\eta|<1.6$) of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ for central (0-5%) Pb--Pb collisions at $\sqrt{s_{\rm NN}}=2.76\;\text{TeV}$. Systematic uncertainty on the long-range mean correlator strength $\delta B = 6.9\times 10^{-4}$.

Azimuthal projection ($|\Delta\eta|<1.6$) of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ for semi-central (30-40%) Pb--Pb collisions at $\sqrt{s_{\rm NN}}=2.76\;\text{TeV}$. Systematic uncertainty on the long-range mean correlator strength $\delta B = 3.8\times 10^{-3}$.

Azimuthal projection ($|\Delta\eta|<1.6$) of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ for perippheral (70-80%) Pb--Pb collisions at $\sqrt{s_{\rm NN}}=2.76\;\text{TeV}$. Systematic uncertainty on the long-range mean correlator strength $\delta B = 5.4\times 10^{-2}$.

Collision centrality evolution of the longitudinal widths of the two-particle transverse momentum correlations $G_{2}^{\rm CI}$ and $G_{2}^{\rm CD}$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}=2.76\;\text{TeV}$.

Collision centrality evolution of the azimuthal widths of the two-particle transverse momentum correlations $G_{2}^{\rm CI}$ and $G_{2}^{\rm CD}$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}=2.76\;\text{TeV}$.

Longitudinal width evolution with the number of participants of the two-particle transverse momentum correlation $G_{2}^{\rm CI}$ in Pb--Pb collisions at $\sqrt{s_{\rm NN}}=2.76\;\text{TeV}$. The widths are extracted from bi-dimensional (2D) or projection (1D) fits of the correlation function.

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%

HFe cross section in Pb-Pb, 60-80 centrality

HFe RAA in Pb-Pb, 0-10 centrality

HFe RAA in Pb-Pb, 30-50 centrality

HFe RAA in Pb-Pb, 60-80 centrality

Elliptic flow ($v_{2}$) of (anti-)$^{3}$He measured in Pb-Pb collisions at \sqrt{s_{\mathrm{NN}}} = 5.02 TeV for the centrality classes 0--20$\%$, 20--40$\%$, and 40--60$\%$. The statistical uncertainties are shown as vertical bars, systematic uncertainties as boxes.

Fig. 1 Left, data for jet radius R=0.4. Unfolded pp full jet cross-section at $\sqrt{s}$ = 5.02 TeV for R = 0.1 − 0.6. No leading track requirement is imposed.

Fig. 1 Left, data for jet radius R=0.5. Unfolded pp full jet cross-section at $\sqrt{s}$ = 5.02 TeV for R = 0.1 − 0.6. No leading track requirement is imposed.

Fig. 1 Left, data for jet radius R=0.6. Unfolded pp full jet cross-section at $\sqrt{s}$ = 5.02 TeV for R = 0.1 − 0.6. No leading track requirement is imposed.

Fig. 2, values for jet radius R=0.1. Non-perturbative correction factor applied to parton-level NLO+NLL predictions, obtained from PYTHIA 8 tune A14 as the ratio of the inclusive jet spectrum at hadron-level with MPI compared to parton-level without MPI.

Fig. 2, values for jet radius R=0.2. Non-perturbative correction factor applied to parton-level NLO+NLL predictions, obtained from PYTHIA 8 tune A14 as the ratio of the inclusive jet spectrum at hadron-level with MPI compared to parton-level without MPI.

Fig. 2, values for jet radius R=0.3. Non-perturbative correction factor applied to parton-level NLO+NLL predictions, obtained from PYTHIA 8 tune A14 as the ratio of the inclusive jet spectrum at hadron-level with MPI compared to parton-level without MPI.

Fig. 2, values for jet radius R=0.4. Non-perturbative correction factor applied to parton-level NLO+NLL predictions, obtained from PYTHIA 8 tune A14 as the ratio of the inclusive jet spectrum at hadron-level with MPI compared to parton-level without MPI.

Fig. 2, values for jet radius R=0.5. Non-perturbative correction factor applied to parton-level NLO+NLL predictions, obtained from PYTHIA 8 tune A14 as the ratio of the inclusive jet spectrum at hadron-level with MPI compared to parton-level without MPI.

Fig. 2, values for jet radius R=0.6. Non-perturbative correction factor applied to parton-level NLO+NLL predictions, obtained from PYTHIA 8 tune A14 as the ratio of the inclusive jet spectrum at hadron-level with MPI compared to parton-level without MPI.

Fig. 3 Bottom, data for jet radius ratio R=0.1/R=0.2. Unfolded pp jet cross-section ratios for various R. With R = 0.1 in the numerator.

Fig. 3 Bottom, data for jet radius ratio R=0.1/R=0.3. Unfolded pp jet cross-section ratios for various R. With R = 0.1 in the numerator.

Fig. 3 Bottom, data for jet radius ratio R=0.1/R=0.4. Unfolded pp jet cross-section ratios for various R. With R = 0.1 in the numerator.

Fig. 3 Bottom, data for jet radius ratio R=0.1/R=0.5. Unfolded pp jet cross-section ratios for various R. With R = 0.1 in the numerator.

Fig. 3 Bottom, data for jet radius ratio R=0.1/R=0.6. Unfolded pp jet cross-section ratios for various R. With R = 0.1 in the numerator.

Fig. 3 Top, data for jet radius ratio R=0.2/R=0.3. Unfolded pp jet cross-section ratios for various R. With R = 0.2 in the numerator.

Fig. 3 Top, data for jet radius ratio R=0.2/R=0.4. Unfolded pp jet cross-section ratios for various R. With R = 0.2 in the numerator.

Fig. 3 Top, data for jet radius ratio R=0.2/R=0.5. Unfolded pp jet cross-section ratios for various R. With R = 0.2 in the numerator.

Fig. 3 Top, data for jet radius ratio R=0.2/R=0.6. Unfolded pp jet cross-section ratios for various R. With R = 0.2 in the numerator.

Fig. 4 Left, data for pp. Unfolded pp and Pb-Pb full jet spectra at $\sqrt{s}=5.02$ TeV for $R=0.2$, with 5 GeV leading track requirement. The pp data points correspond to $\frac{\mathrm{d}^{2}\sigma}{\mathrm{d}p_{\mathrm{T,jet}} \mathrm{d}\eta_{\mathrm{jet}}}$.

Fig. 4 Left, data for PbPb. Unfolded pp and Pb-Pb full jet spectra at $\sqrt{s}=5.02$ TeV for $R=0.2$, with 5 GeV leading track requirement. The pp data points correspond to $\frac{\mathrm{d}^{2}\sigma}{\mathrm{d}p_{\mathrm{T,jet}} \mathrm{d}\eta_{\mathrm{jet}}}$.

Fig. 4 Right, data for pp. Unfolded pp and Pb-Pb full jet spectra at $\sqrt{s}=5.02$ TeV for $R=0.4$, with 7 GeV leading track requirement.

Fig. 4 Right, data for PbPb. Unfolded pp and Pb-Pb full jet spectra at $\sqrt{s}=5.02$ TeV for $R=0.4$, with 7 GeV leading track requirement.

Fig. 5 Left, data for pp jet cross section with leading track bias ratio 5/0. Ratio of the pp jet cross-section with various leading charged particle requirements

Fig. 5 Left, data for pp jet cross section with leading track bias ratio 7/0. Ratio of the pp jet cross-section with various leading charged particle requirements

Fig. 5 Left, data for pp jet cross section with leading track bias ratio 7/5. Ratio of the pp jet cross-section with various leading charged particle requirements

Fig. 5 Right. Ratio of the R = 0.2 Pb–Pb jet cross-section with a 7 GeV/c leading charged particle requirement compared to a 5 GeV/c leading charged particle requirement.

Fig. 6 Top Left. Jet $R_{\mathrm{AA}}$ at $\sqrt{s}=5.02$ TeV for $R=0.2$. Same leading track requirement of 5 GeV is imposed on the numerator as well as denominator.

Fig. 6 Top Right. Jet $R_{\mathrm{AA}}$ at $\sqrt{s}=5.02$ TeV for $R=0.4$. Same leading track requirement of 7 GeV is imposed on the numerator as well as denominator.

Fig. 6 Bottom Left. Jet $R_{\mathrm{AA}}$ at $\sqrt{s}=5.02$ TeV for $R=0.2$. PbPb with leading track requirement of 5 GeV. pp reference without a leading track requirement.

Fig. 6 Bottom Right. Jet $R_{\mathrm{AA}}$ at $\sqrt{s}=5.02$ TeV for $R=0.4$. PbPb with leading track requirement of 7 GeV. pp reference without a leading track requirement.

Rapidity dependence (in 0-90% centrality class) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a rapidity-correlated systematic uncertainty.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 4. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

Rapidity dependence (in 0-90% centrality class) of the ratio of the inclusive J/$\psi$ $R_{\rm AA}$ at $\sqrt{s_{NN}}$= 5.02 and 2.76 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a rapidity-correlated systematic uncertainty.

Transverse momentum dependence (in 0-20% centrality class) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a $p_{\rm T}$-correlated systematic uncertainty.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 7. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

Transverse momentum dependence (in 0-20% centrality class) of the ratio of the inclusive J/$\psi$ $R_{\rm AA}$ at $\sqrt{s_{NN}}$= 5.02 and 2.76 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a $p_{\rm T}$-correlated systematic uncertainty.

Transverse momentum dependence (in 20-40% centrality class) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a $p_{\rm T}$-correlated systematic uncertainty.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 10. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

Transverse momentum dependence (in 20-40% centrality class) of the ratio of the inclusive J/$\psi$ $R_{\rm AA}$ at $\sqrt{s_{NN}}$= 5.02 and 2.76 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a $p_{\rm T}$-correlated systematic uncertainty.

Transverse momentum dependence (in 40-90% centrality class) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a $p_{\rm T}$-correlated systematic uncertainty.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 13. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

Transverse momentum dependence (in 40-90% centrality class) of the ratio of the inclusive J/$\psi$ $R_{\rm AA}$ at $\sqrt{s_{NN}}$= 5.02 and 2.76 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a $p_{\rm T}$-correlated systematic uncertainty.

Rapidity dependence (in 0-20% centrality class) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a rapidity-correlated systematic uncertainty.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 16. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

Rapidity dependence (in 20-40% centrality class) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a rapidity-correlated systematic uncertainty.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 18. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

Rapidity dependence (in 40-90% centrality class) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a rapidity-correlated systematic uncertainty.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 20. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

$\langle N_{part} \rangle$-dependence (for 0.3 < $p_{\rm T}$ < 2 $GeV/c$) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty. The $\langle N_{part} \rangle$ values correspond descendingly to the centrality classes 0–10%, 10–20%, 20–30%, 30–40%, 40–50%, 50–60%, and 60–90%.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 22. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

$\langle N_{part} \rangle$-dependence (for 0.3 < $p_{\rm T}$ < 2 $GeV/c$) of the ratio of the inclusive J/$\psi$ $R_{\rm AA}$ at $\sqrt{s_{NN}}$= 5.02 and 2.76 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty. The $\langle N_{part} \rangle$ values correspond descendingly to the centrality classes 0–10%, 10–20%, 20–30%, 30–40%, 40–50%, 50–60%, and 60–90%.

$\langle N_{part} \rangle$-dependence (for 2 < $p_{\rm T}$ < 5 $GeV/c$) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty. The $\langle N_{part} \rangle$ values correspond descendingly to the centrality classes 0–10%, 10–20%, 20–30%, 30–40%, 40–50%, 50–60%, and 60–90%.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 25. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

$\langle N_{part} \rangle$-dependence (for 2 < $p_{\rm T}$ < 5 $GeV/c$) of the ratio of the inclusive J/$\psi$ $R_{\rm AA}$ at $\sqrt{s_{NN}}$= 5.02 and 2.76 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty. The $\langle N_{part} \rangle$ values correspond descendingly to the centrality classes 0–10%, 10–20%, 20–30%, 30–40%, 40–50%, 50–60%, and 60–90%.

$\langle N_{part} \rangle$-dependence (for 5 < $p_{\rm T}$ < 8 $GeV/c$) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty. The $\langle N_{part} \rangle$ values correspond descendingly to the centrality classes 0–10%, 10–20%, 20–30%, 30–40%, 40–50%, 50–60%, and 60–90%.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 28. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

$\langle N_{part} \rangle$-dependence (for 5 < $p_{\rm T}$ < 8 $GeV/c$) of the ratio of the inclusive J/$\psi$ $R_{\rm AA}$ at $\sqrt{s_{NN}}$= 5.02 and 2.76 TeV. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty. The $\langle N_{part} \rangle$ values correspond descendingly to the centrality classes 0–10%, 10–20%, 20–30%, 30–40%, 40–50%, 50–60%, and 60–90%.

$\langle N_{part} \rangle$-dependence (for 8 < $p_{\rm T}$ < 12 $GeV/c$) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty. The $\langle N_{part} \rangle$ values correspond descendingly to the centrality classes 0–10%, 10–20%, 20–30%, 30–40%, 40–50%, 50–60%, and 60–90%.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 31. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

$\langle N_{part} \rangle$-dependence (for 0.3 < $p_{\rm T}$ < 8 $GeV/c$) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty. The $\langle N_{part} \rangle$ values correspond descendingly to the centrality classes 0–10%, 10–20%, 20–30%, 30–40%, 40–50%, 50–60%, 60–70%, 70–80% and 80–90%. The values, already published in https://doi.org/10.1016/j.physletb.2016.12.064 (Figure.4), were updated with the improved $\langle T_{AA} \rangle$ calculations reported in https://cds.cern.ch/record/2636623.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 33. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

$\langle N_{part} \rangle$-dependence (for 2.5 < $y$ < 3) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty. The $\langle N_{part} \rangle$ values correspond descendingly to the centrality classes 0–10%, 10–20%, 20–30%, 30–40%, 40–50%, 50–60%, and 60–90%.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 35. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

$\langle N_{part} \rangle$-dependence (for 3 < $y$ < 3.5) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty. The $\langle N_{part} \rangle$ values correspond descendingly to the centrality classes 0–10%, 10–20%, 20–30%, 30–40%, 40–50%, 50–60%, and 60–90%.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 37. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

$\langle N_{part} \rangle$-dependence (for 3.5 < $y$ < 4) of the inclusive J/$\psi$ $R_{\rm AA}$. The first uncertainty is statistical, the second is the uncorrelated systematic, while the third one is a centrality-correlated systematic uncertainty. The $\langle N_{part} \rangle$ values correspond descendingly to the centrality classes 0–10%, 10–20%, 20–30%, 30–40%, 40–50%, 50–60%, and 60–90%.

The minimum and maximum variations for the $R_{\rm AA}$ of prompt J/$\psi$ with respect to the $R_{\rm AA}$ values of inclusive J/$\psi$ reported in Table 39. The variations correspond to two extreme hypotheses on the unknown contribution of non-prompt J/$\psi$.

$p_{\rm T}$-differential yields of the inclusive J/$\psi$ in various centrality classes. The first uncertainty is statistical, while the second is the uncorrelated systematic.

$\langle N_{part} \rangle$-dependence of the inclusive J/$\psi$ average $p_{\rm T}$. The first uncertainty is statistical, while the second is the uncorrelated systematic. The $\langle N_{part} \rangle$ values correspond descendingly to the centrality classes 0–10%, 10–20%, 20–30%, 30–40%, 40–50%, 50–60%, and 60–90%.

$\langle N_{part} \rangle$-dependence of the inclusive J/$\psi$ $r_{\rm AA}$. The first uncertainty is the quadratic sum of the statistical and uncorrelated systematic ones, while the second is a centrality-correlated systematic uncertainty. The $\langle N_{part} \rangle$ values correspond descendingly to the centrality classes 0–10%, 10–20%, 20–30%, 30–40%, 40–50%, 50–60%, and 60–90%.

The $\Lambda$ global polarization as function of centrality for Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$~TeV.

The $\bar\Lambda$ global polarization as function of centrality for Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$~TeV.

The $\Lambda$ global polarization as function of centrality for Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$~TeV.

The $\bar\Lambda$ global polarization as function of centrality for Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$~TeV.

The $\Lambda$ global polarization as function of centrality for Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$~TeV.

The $\bar\Lambda$ global polarization as function of centrality for Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$~TeV.

The $\Lambda$ global polarization as function of centrality for Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$~TeV.

The $\bar\Lambda$ global polarization as function of centrality for Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$~TeV.

The average $(\Lambda+\bar\Lambda) \times (2.76+5.02)$ global polarization in Pb-Pb collisions for centrality 15-50%.

The $\Lambda$ global polarization as function of transverse momentum ($p_{\mathrm{T}}$) for 5-15% centrality in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$~TeV.

The $\Lambda$ global polarization as function of transverse momentum ($p_{\mathrm{T}}$) for 15-50% centrality in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$~TeV.

The $\bar\Lambda$ global polarization as function of transverse momentum ($p_{\mathrm{T}}$) for 5-15% centrality in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$~TeV.

The $\bar\Lambda$ global polarization as function of transverse momentum ($p_{\mathrm{T}}$) for 15-50% centrality in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=2.76$~TeV.

The $\Lambda$ global polarization as function of transverse momentum ($p_{\mathrm{T}}$) for 5-15% centrality in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$~TeV.

The $\Lambda$ global polarization as function of transverse momentum ($p_{\mathrm{T}}$) for 15-50% centrality in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$~TeV.

The $\bar\Lambda$ global polarization as function of transverse momentum ($p_{\mathrm{T}}$) for 5-15% centrality in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$~TeV.

The $\bar\Lambda$ global polarization as function of transverse momentum ($p_{\mathrm{T}}$) for 15-50% centrality in Pb-Pb collisions at $\sqrt{s_{\mathrm{NN}}}=5.02$~TeV.

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

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

The $\Upsilon$(1S) $v_2$ coefficient in three centrality intervals integrated over the transverse momentum range 2~$<$~$p_{\rm T}$~$<$~15 GeV/$c$ in Pb-Pb collisions at $\sqrt{s_{\rm NN}}$ = 5.02 TeV.

$p_{\rm{T}}$ differential cross section of prompt D0 mesons in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$. For $0<p_{\rm{T}}<1$ GeV/$c$ the cross section is obtained from the analysis without vertexing recostruction and for $p_{\rm{T}}>1$ GeV/c the analysis with vertexing reconstruction is used.

$p_{\rm{T}}$ differential cross section of prompt D0 mesons in pp collisions at $\mathbf{\sqrt{\textit s}~=~5.02~TeV}$ multiplied by A=208. For $0<p_{\rm{T}}<1$ GeV/$c$ the cross section is obtained from the analysis without vertexing recostruction and for $p_{\rm{T}}>1$ GeV/c the analysis with vertexing reconstruction is used.

$p_{\rm{T}}$ differential cross section of prompt D* mesons in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.

$p_{\rm{T}}$ differential cross section of prompt D* mesons in pp collisions at $\mathbf{\sqrt{{\textit s}}~=~5.02~TeV}$ multiplied by A=208.

$p_{\rm{T}}$ differential cross section of prompt D+ mesons in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.

$p_{\rm{T}}$ differential cross section of prompt D+ mesons in pp collisions at $\mathbf{\sqrt{{\textit s}}~=~5.02~TeV}$ multiplied by A=208.

$p_{\rm{T}}$ differential cross section of prompt Ds mesons in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.

$p_{\rm{T}}$ differential cross section of prompt Ds mesons in pp collisions at $\mathbf{\sqrt{{\textit s}}~=~5.02~TeV}$ multiplied by A=208.

$R_{\rm{pPb}}$ of prompt D0 mesons in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.

$R_{\rm{pPb}}$ of prompt D* mesons in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.

$R_{\rm{pPb}}$ of prompt D+ mesons in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.

$R_{\rm{pPb}}$ of prompt Ds mesons in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.

$R_{\rm{pPb}}$ of prompt non-strange D mesons in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.

$Q_{\rm pPb}$ of prompt D mesons in different centrality classes in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$

$Q_{\rm CP}$ of prompt D mesons in different centrality classes in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$

Ratio of prompt D+ over D0 production cross section as a function of transverse momentum in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$

Ratio of prompt D*+ over D0 production cross section as a function of transverse momentum in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$

Ratio of prompt Ds+ over D0 production cross section as a function of transverse momentum in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$

Ratio of prompt Ds+ over D+ production cross section as a function of transverse momentum in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$

Ratio of prompt Ds+ over D+ production cross section as a function of the charged particle pseudorapidity density in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.

Ratio of prompt Ds+ over D+ production cross section as a function of the charged particle pseudorapidity density in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.

Ratio of prompt Ds+ over D+ production cross section as a function of the charged particle pseudorapidity density in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.

Ratio of prompt Ds+ over D+ production cross section as a function of the charged particle pseudorapidity density in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.

Ratio of prompt Ds+ over D+ production cross section as a function of the charged particle pseudorapidity density in p-Pb collisions at $\mathbf{\sqrt{{\textit s}_{\rm NN}}~=~5.02~TeV}$.

Transverse momentum distributions of deuterons in the 40-60% V0A multiplicity class

Transverse momentum distributions of deuterons in the 60-100% V0A multiplicity class

Transverse momentum distributions of anti-deuterons in the 0-10% V0A multiplicity class

Transverse momentum distributions of anti-deuterons in the 10-20% V0A multiplicity class

Transverse momentum distributions of anti-deuterons in the 20-40% V0A multiplicity class

Transverse momentum distributions of anti-deuterons in the 40-60% V0A multiplicity class

Transverse momentum distributions of anti-deuterons in the 60-100% V0A multiplicity class

$\bar{d}$/d ratio as a function of transverse momentum in the 0-10% V0A multiplicity class

$\bar{d}$/d ratio as a function of transverse momentum in the 10-20% V0A multiplicity class

$\bar{d}$/d ratio as a function of transverse momentum in the 20-40% V0A multiplicity class

$\bar{d}$/d ratio as a function of transverse momentum in the 40-60% V0A multiplicity class

$\bar{d}$/d ratio as a function of transverse momentum in the 60-100% V0A multiplicity class

Transverse momentum distribution of $^{3}\overline{\mathrm{He}}$ for all non single diffractive (NSD) p-Pb collisions.

Transverse momentum distribution of $^{3}\mathrm{He}$ for all non single diffractive (NSD) p-Pb collisions.

Integrated yield of nuclei produced in NSD p-Pb collisions normalised by the spin degeneracy factor as a function of the mass number

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the 0-10% V0A multiplicity class

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the 10-20% V0A multiplicity class

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the 20-40% V0A multiplicity class

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the 40-60% V0A multiplicity class

Coalescence parameter $B_2$ as a function of $p_{\mathrm{T}}$ in the 60-100% V0A multiplicity class

Mean transverse momentum of deuteron produced in p-Pb collisions as a function of the charged particle multiplicity density ad mid-rapidity

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

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

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

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

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

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

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

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

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

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

Transverse momentum spectra as a function of the event multiplicity for pp collisions at 5.02 TeV. Event multiplicity is estimated with the signal in the VZERO detector. Uncorrelated systematic uncertainties are the multiplicity dependent systematic uncertainties.

Average transverse momentum as a function of event multiplicity in pp collisions at 13 TeV. Results for the 0-100% spherocity class are presented. Spherocty-dependent uncertainties are indicated as uncorrelated.

Average transverse momentum as a function of event multiplicity in pp collisions at 13 TeV. Results for the 0-10% spherocity class are presented. Spherocty-dependent uncertainties are indicated as uncorrelated.

Average transverse momentum as a function of event multiplicity in pp collisions at 13 TeV. Results for the 10-20% spherocity class are presented. Spherocty-dependent uncertainties are indicated as uncorrelated.

Average transverse momentum as a function of event multiplicity in pp collisions at 13 TeV. Results for the 20-30% spherocity class are presented. Spherocty-dependent uncertainties are indicated as uncorrelated.

Average transverse momentum as a function of event multiplicity in pp collisions at 13 TeV. Results for the 30-40% spherocity class are presented. Spherocty-dependent uncertainties are indicated as uncorrelated.

Average transverse momentum as a function of event multiplicity in pp collisions at 13 TeV. Results for the 40-50% spherocity class are presented. Spherocty-dependent uncertainties are indicated as uncorrelated.

Average transverse momentum as a function of event multiplicity in pp collisions at 13 TeV. Results for the 50-60% spherocity class are presented. Spherocty-dependent uncertainties are indicated as uncorrelated.

Average transverse momentum as a function of event multiplicity in pp collisions at 13 TeV. Results for the 60-70% spherocity class are presented. Spherocty-dependent uncertainties are indicated as uncorrelated.

Average transverse momentum as a function of event multiplicity in pp collisions at 13 TeV. Results for the 70-80% spherocity class are presented. Spherocty-dependent uncertainties are indicated as uncorrelated.

Average transverse momentum as a function of event multiplicity in pp collisions at 13 TeV. Results for the 80-90% spherocity class are presented. Spherocty-dependent uncertainties are indicated as uncorrelated.

Average transverse momentum as a function of event multiplicity in pp collisions at 13 TeV. Results for the 90-100% spherocity class are presented. Spherocty-dependent uncertainties are indicated as uncorrelated.

Spherocity intervals used in this analysis.

Average transverse momentum as a function of event multiplicity in pp collisions at 13 TeV. Results for the 90-100% spherocity class are presented. Spherocty-dependent uncertainties are indicated as uncorrelated.

Spherocity intervals used in this analysis.