$\Upsilon(1S)$ production cross-section in $p$Pb and Pb$p$, as a function of $y^*$. The uncertainty is the sum in quadrature of the statistical and systematic components.

$\Upsilon(2S)$ production cross-section in $p$Pb and Pb$p$, as a function of $p_{T}$. The uncertainty is the sum in quadrature of the statistical and systematic components.

$\Upsilon(2S)$ production cross-section in $p$Pb and Pb$p$, as a function of $y^*$. The uncertainty is the sum in quadrature of the statistical and systematic components.

Scaled $pp$ differential cross-section in $p_{T}$ at $\sqrt{s_{NN}}=8.16$ TeV. The first uncertainty is statistical, the second is systematic, which includes the systematic uncertainty from the $pp$ measurement and that estimated by changing the interpolation function.

Scaled $pp$ differential cross-section in $y$ at $\sqrt{s_{NN}}=8.16$ TeV. The first uncertainty is statistical, the second is systematic, which includes the systematic uncertainty from the $pp$ measurement and that estimated by changing the interpolation function.

$\Upsilon(1S)$ nuclear modification factor, $R_{p{\rm Pb}}^{\Upsilon(1S)}$, in $p$Pb and Pb$p$ as a function of $p_{T}$ integrated over $y^*$ in the range $1.5 < y^* < 4.0$ for $p$Pb and $-5.0 < y^* < -2.5$ for Pb$p$. The quoted uncertainties are the sum in quadrature of the statistical and systematic components.

$\Upsilon(1S)$ nuclear modification factor, $R_{p{\rm Pb}}^{\Upsilon(1S)}$, in $p$Pb and Pb$p$ as a function of $y^*$ integrated over $p_{T}$ in the range $0 < p_{T} < 25$ GeV$/c$. The quoted uncertainties are the sum in quadrature of the statistical and systematic components.

$\Upsilon(2S)$ nuclear modification factor, $R_{p{\rm Pb}}^{\Upsilon(2S)}$, in $p$Pb and Pb$p$ as a function of $p_{T}$ integrated over $y^*$ in the range $1.5 < y^* < 4.0$ for $p$Pb and $-5.0 < y^* < -2.5$ for Pb$p$. The quoted uncertainties are the sum in quadrature of the statistical and systematic components.

$\Upsilon(2S)$ nuclear modification factor, $R_{p{\rm Pb}}^{\Upsilon(2S)}$, in $p$Pb and Pb$p$ as a function of $y^*$ integrated over $p_{T}$ in the range $0 < p_{T} < 25$ GeV$/c$. The quoted uncertainties are the sum in quadrature of the statistical and systematic components.

$\Upsilon(1S)$ forward-to-backward ratio, $R_{{\rm FB}}^{\Upsilon(1S)}$, as a function of $p_{T}$ integrated over $\vert y^* \vert$ in the range $2.5 < \vert y^* \vert < 4.0$. The quoted uncertainties are the sum in quadrature of the statistical and systematic components.

$\Upsilon(1S)$ forward-to-backward ratio, $R_{{\rm FB}}^{\Upsilon(1S)}$, as a function of $\vert y^* \vert$ integrated over $p_{T}$ in the range $0 < p_{T} < 25$ GeV/c. The quoted uncertainties are the sum in quadrature of the statistical and systematic components.

$\Upsilon(2S)$ to $\Upsilon(1S)$ ratio, in $p$Pb and Pb$p$ as a function of $p_{T}$ integrated over $y^*$ in the range $1.5 < y^* < 4.0$ for $p$Pb and $-5.0 < y^* < -2.5$ for Pb$p$. The quoted uncertainties are the sum in quadrature of the statistical and systematic components.

$\Upsilon(2S)$ to $\Upsilon(1S)$ ratio, in $p$Pb and Pb$p$ as a function of $y^*$ integrated over $p_{T}$ in the range $0 < p_{T} < 25$ GeV/c. The quoted uncertainties are the sum in quadrature of the statistical and systematic components.

$\Upsilon(1S)$ to non-prompt $J/\psi$, in $p$Pb and Pb$p$ as a function of $y^*$ integrated over $p_{T}$ in the range $0 < p_{T} < 25$ GeV/c. The quoted uncertainties are the sum in quadrature of the statistical and systematic components.

The double-differential cross sections for $J/\psi$ production from $b$-decays as a function of transverse momentum for the rapidity range $1.5 < y^* < 4.0$ in the nucleon-nucleon centre-of-mass frame. The first quoted uncertainty indicates the bin-by-bin correlated systematic uncertainty and the second is the bin-by-bin uncorrelated systematic uncertainty.

The double-differential cross sections for prompt $J/\psi$ production, assuming no polarisation, as a function of transverse momentum for the rapidity range $-5.0 < y^* < -2.5$ in the nucleon-nucleon centre-of-mass frame. The first quoted uncertainty indicates the bin-by-bin correlated systematic uncertainty and the second is the bin-by-bin uncorrelated systematic uncertainty.

The double-differential cross sections for $J/\psi$ production from $b$-hadron decays as a function of transverse momentum for the rapidity range $-5.0 < y^* < -2.5$ in the nucleon-nucleon centre-of-mass frame. The first quoted uncertainty indicates the bin-by-bin correlated systematic uncertainty and the second is the bin-by-bin uncorrelated systematic uncertainty.

Fraction of $J/\psi$ from $b$-hadron decay in bins of transverse momentum and rapidity in the nucleon-nucleon rest frame, assuming no polarisation, in the proton-lead beam configuration corresponding to rapidity range $1.5< y^* <4.0$ in the nucleon-nucleon centre-of-mass frame. The uncertainty is uncorrelated between bins.

Fraction of $J/\psi$ from $b$-hadron decay in bins of transverse momentum and rapidity, assuming no polarisation, in the proton-lead beam configuration corresponding to the rapidity range $-5.0 < y^* < -2.5$ in the nucleon-nucleon centre-of-mass frame. The uncertainty is uncorrelated between bins.

The nuclear modification factor $R_{p \mathrm{Pb}}$ of prompt $J/\psi$ for transverse momentum smaller than 14 GeV/c as a function of transverse momentum integrated over the rapidity ranges $1.5 < y^* < 4.0$ for $p$Pb and $-5.0 < y^* < -2.5$ for Pb$p$. The quoted uncertainties are the quadratic sums of statistical and systematic uncertainties.

The nuclear modification factor $R_{p\mathrm{Pb}}$ of prompt $J/\psi$ integrated over transverse momentum smaller than 14 GeV/$c$ as a function of rapidity in the nucleon-nucleon centre-of-mass frame ($y^*$). The quoted uncertainties are the quadratic sums of statistical and systematic uncertainties.

The nuclear modification factor $R_{p\mathrm{Pb}}$ of $J/psi$ from the decay of $b$-hadrons for transverse momentum smaller than 14 GeV/$c$ as a function of transverse momentum integrated over the rapidity range $1.5 < y^* < 4.0$ for $p$Pb and $-5.0 < y^* < -2.5$ for Pb$p$. The quoted uncertainties are the quadratic sums of statistical and systematic uncertainties.

The nuclear modification factor $R_{p\mathrm{Pb}}$ of $J/\psi$ from decay of $b$-hadrons integrated over transverse momentum smaller than 14 GeV/$c$ as a function of rapidity in the nucleon-nucleon centre-of-mass frame. The quoted uncertainties are the quadratic sums of statistical and systematic uncertainties.

The FORWARD/BACKWARD production ratio $R_{\mathrm{FB}}$ of prompt $J/\psi$ as a function of transverse momentum integrated over $|y^*|$ in the range $2.5 < |y^*| < 4.0$. The quoted uncertainties are the quadratic sums of statistical and systematic uncertainties.

The FORWARD/BACKWARD production ratio $R_{\mathrm{FB}}$ of prompt $J/\psi$ as a function of rapidity $y^*$ in the nucleon-nucleon centre-of-mass frame integrated over transverse momentum smaller than 14 GeV/$c$. The quoted uncertainties are the quadratic sums of statistical and systematic uncertainties.

The FORWARD/BACKWARD production ratio $R_{\mathrm{FB}}$ of $J/\psi$ from $b$-hadron decays as a function of transverse momentum integrated over $|y^*|$ in the range $2.5 < |y^*| < 4.0$. The quoted uncertainties are the quadratic sums of statistical and systematic uncertainties.

The FORWARD/BACKWARD production ratio $R_{\mathrm{FB}}$ of $J/\psi$ from $b$-hadron decays as a function of rapidity $y^*$ in the nucleon-nucleon centre-of-mass frame integrated over transverse momentum smaller than 14 GeV/$c$. The quoted uncertainties are the quadratic sums of statistical and systematic uncertainties.

Differential production cross-sections for prompt $D^{+} + D^{-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.

Differential production cross-sections for prompt $D_{s}^{+} + D_{s}^{-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.

Differential production cross-sections for prompt $D_{s}^{+} + D_{s}^{-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.

Differential production cross-sections for prompt $D^{*+} + D^{*-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.

Differential production cross-sections for prompt $D^{*+} + D^{*-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.

The ratios of differential production cross-sections, $R_{13/5}$, for prompt $D^{0} + \bar{D}^{0}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.

The ratios of differential production cross-sections, $R_{13/5}$, for prompt $D^{0} + \bar{D}^{0}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.

The ratios of differential production cross-sections, $R_{13/5}$, for prompt $D^{+} + D^{-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.

The ratios of differential production cross-sections, $R_{13/5}$, for prompt $D^{+} + D^{-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.

The ratios of differential production cross-sections, $R_{13/5}$, for prompt $D_{s}^{+} + D_{s}^{-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.

The ratios of differential production cross-sections, $R_{13/5}$, for prompt $D_{s}^{+} + D_{s}^{-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.

The ratios of differential production cross-sections, $R_{13/5}$, for prompt $D^{*+} + D^{*-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.

The ratios of differential production cross-sections, $R_{13/5}$, for prompt $D^{*+} + D^{*-}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic.

The ratios of differential production cross-section-times-branching fraction measurements for prompt $D^{+}$ and $D^{0}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic. All values are given in percent.

The ratios of differential production cross-section-times-branching fraction measurements for prompt $D^{+}$ and $D^{0}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic. All values are given in percent.

The ratios of differential production cross-section-times-branching fraction measurements for prompt $D_{s}^{+}$ and $D^{0}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic. All values are given in percent.

The ratios of differential production cross-section-times-branching fraction measurements for prompt $D_{s}^{+}$ and $D^{0}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic. All values are given in percent.

The ratios of differential production cross-section-times-branching fraction measurements for prompt $D^{*+}$ and $D^{0}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic. All values are given in percent.

The ratios of differential production cross-section-times-branching fraction measurements for prompt $D^{*+}$ and $D^{0}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic. All values are given in percent.

The ratios of differential production cross-section-times-branching fraction measurements for prompt $D_{s}^{+}$ and $D^{+}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic. All values are given in percent.

The ratios of differential production cross-section-times-branching fraction measurements for prompt $D_{s}^{+}$ and $D^{+}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic. All values are given in percent.

The ratios of differential production cross-section-times-branching fraction measurements for prompt $D^{*+}$ and $D^{+}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic. All values are given in percent.

The ratios of differential production cross-section-times-branching fraction measurements for prompt $D^{*+}$ and $D^{+}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic. All values are given in percent.

The ratios of differential production cross-section-times-branching fraction measurements for prompt $D_{s}^{+}$ and $D^{*+}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic. All values are given in percent.

The ratios of differential production cross-section-times-branching fraction measurements for prompt $D_{s}^{+}$ and $D^{*+}$ mesons in bins of $(p_{\mathrm{T}}, y)$. The first uncertainty is statistical, and the second is the total systematic. All values are given in percent.

Differential cross-section $\mathrm{d} \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d}p_T$ [pb/(GeV/$c$)] for $2.0 < y < 4.5$.

Differential cross-section $\mathrm{d} \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d}y$ [pb] for $p_T < 30$ GeV.

Ratio of double-differential cross-sections $( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(2S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y ) / ( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(1S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y )$.

Ratio of double-differential cross-sections $( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(3S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y ) / ( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(1S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y )$.

Ratio of double-differential cross-sections $( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(3S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y ) / ( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(2S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y )$.

The ratio of differential cross-sections $( \mathrm{d} \sigma ( pp \to ( \Upsilon(iS) \to \mu^+ \mu^- ) X ) / \mathrm{d}p_T ) / ( \mathrm{d} \sigma ( pp \to ( \Upsilon(jS) \to \mu^+ \mu^- ) X ) / \mathrm{d}p_T )$ for $2.0 < y < 4.5$.

The ratio of differential cross-sections $( \mathrm{d} \sigma ( pp \to ( \Upsilon(iS) \to \mu^+ \mu^- ) X ) / \mathrm{d}y ) / ( \mathrm{d} \sigma ( pp \to ( \Upsilon(jS) \to \mu^+ \mu^- ) X ) / \mathrm{d}y )$ for $p_T < 30$ GeV/$c$.

Double-differential cross-section $\mathrm{d}^2 \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d}y$ [pb/(GeV/$c$)].

Double-differential cross-section $\mathrm{d}^2 \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d}y$ [pb/(GeV/$c$)].

Double-differential cross-section $\mathrm{d}^2 \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d}y$ [pb/(GeV/$c$)].

Differential cross-section $\mathrm{d} \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d}p_T$ [pb/(GeV/$c$)] for $2.0 < y < 4.5$.

Differential cross-section $\mathrm{d} \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d}y$ [pb] for $p_T < 30$ GeV.

Ratio of double-differential cross-sections $( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(2S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y ) / ( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(1S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y )$.

Ratio of double-differential cross-sections $( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(3S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y ) / ( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(1S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y )$.

Ratio of double-differential cross-sections $( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(3S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y ) / ( \mathrm{d}^2 \sigma ( pp \to ( \Upsilon(2S) \to \mu^+ \mu^- ) X ) / \mathrm{d} p_T/\mathrm{d} y )$.

The ratio of differential cross-sections $( \mathrm{d} \sigma ( pp \to ( \Upsilon(iS) \to \mu^+ \mu^- ) X ) / \mathrm{d}p_T ) / ( \mathrm{d} \sigma ( pp \to ( \Upsilon(jS) \to \mu^+ \mu^- ) X ) / \mathrm{d}p_T )$ for $2.0 < y < 4.5$.

The ratio of differential cross-sections $( \mathrm{d} \sigma ( pp \to ( \Upsilon(iS) \to \mu^+ \mu^- ) X ) / \mathrm{d}y ) / ( \mathrm{d} \sigma ( pp \to ( \Upsilon(jS) \to \mu^+ \mu^- ) X ) / \mathrm{d}y )$ for $p_T < 30$ GeV/$c$.

The ratio of differential cross-section $\mathrm{d} \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d}p_T$ [pb/(GeV/$c$)] for $\sqrt{s}=8$ and $\sqrt{s}=7$ TeV in $2.0 < y < 4.5$.

The ratio of differential cross-section $\mathrm{d} \sigma ( pp \to ( \Upsilon \to \mu^+ \mu^- ) X ) / \mathrm{d}y$ for $\sqrt{s}=8$ and $\sqrt{s}=7$ TeV and $p_T < 30$ GeV/$c$.

The double-differential cross sections for prompt J/PSI production (assuming no polarisation) and production of J/PSI from b-hadron decays as a function of transverse momentum for the rapidity range 2.5-3.0. Also shown in the final column is the fraction (in %) of J/PSIs from the latter.

The double-differential cross sections for prompt J/PSI production (assuming no polarisation) and production of J/PSI from b-hadron decays as a function of transverse momentum for the rapidity range 3.0-3.5. Also shown in the final column is the fraction (in %) of J/PSIs from the latter.

The double-differential cross sections for prompt J/PSI production (assuming no polarisation) and production of J/PSI from b-hadron decays as a function of transverse momentum for the rapidity range 3.5-4.0. Also shown in the final column is the fraction (in %) of J/PSIs from the latter.

The double-differential cross sections for prompt J/PSI production (assuming no polarisation) and production of J/PSI from b-hadron decays as a function of transverse momentum for the rapidity range 4.0-4.5. Also shown in the final column is the fraction (in %) of J/PSIs from the latter.

The total integrated cross sections for UPSILON 1S 2S and 3S times their dimuon branching ratio in the rapidity range 2.0-4.5 and transverse momentum 0-15 GeV/c.

Differential production cross section for UPSILON 1S 2s and 3S mesons times their dimuon branching fraction as a function of transverse momentum ;.

Differential production cross section for UPSILON 1S 2s and 3S mesons times their dimuon branching fraction as a function of rapidity ;.

The double-differential cross section (times the dimuon decay probability) for the production of UPSILON 1S, 2S and 3S mesons as a function of their transverse momentum for the rapidity range 2.0-2.5, assuming no polarisation.

The double-differential cross section (times the dimuon decay probability) for the production of UPSILON 1S, 2S and 3S mesons as a function of their transverse momentum for the rapidity range 2.5-3.0, assuming no polarisation.

The double-differential cross section (times the dimuon decay probability) for the production of UPSILON 1S, 2S and 3S mesons as a function of their transverse momentum for the rapidity range 3.0-3.5, assuming no polarisation.

The double-differential cross section (times the dimuon decay probability) for the production of UPSILON 1S, 2S and 3S mesons as a function of their transverse momentum for the rapidity range 3.5-4.0, assuming no polarisation.

The double-differential cross section (times the dimuon decay probability) for the production of UPSILON 1S, 2S and 3S mesons as a function of their transverse momentum for the rapidity range 4.0-4.5, assuming no polarisation.

Ratios of the cross-sections for UPSILON(2S)->MU+MU- and UPSILON(3S)->MU+MU- with respect toe UPSILON(1S)->MU+MU- as a function of PT in the rapidity range 2.0-4.0 ;.

Ratios of the cross-sections for UPSILON(2S)->MU+MU- and UPSILON(3S)->MU+MU- with respect to UPSILON(1S)->MU+MU- as a function of rapidity in the rapidity range 2.0-4.0 ;.