$K^{+} + K^{-}$ transverse momentum spectra in V0M multilpicity classes

$p + \bar{p}$ transverse momentum spectra in V0M multilpicity classes

$p + \bar{p}$ transverse momentum spectra in V0M multilpicity classes

$\pi^{+} + \pi^{-}$ transverse momentum spectra ratios, V0M multiplicity classes to INEL>0

$\pi^{+} + \pi^{-}$ transverse momentum spectra ratios, V0M multiplicity classes to INEL>0

$K^{+} + K^{-}$ transverse momentum spectra ratios, V0M multiplicity classes to INEL>0

$K^{+} + K^{-}$ transverse momentum spectra ratios, V0M multiplicity classes to INEL>0

$p + \bar{p}$ transverse momentum spectra ratios, V0M multiplicity classes to INEL>0

$p + \bar{p}$ transverse momentum spectra ratios, V0M multiplicity classes to INEL>0

Transverse momentum dependence of ($K^{+} + K^{-}$)/($\pi^{+} + \pi^{-}$) and ($p + \bar{p}$)/($\pi^{+} + \pi^{-}$) ratios in low-$p_T$ interval in pp collisions as a function of $\langle dN_{ch}/d\eta\rangle_{|\eta|<0.5}$

Transverse momentum dependence of ($K^{+} + K^{-}$)/($\pi^{+} + \pi^{-}$) and ($p + \bar{p}$)/($\pi^{+} + \pi^{-}$) ratios in mid-$p_T$ interval in pp collisions as a function of $\langle dN_{ch}/d\eta\rangle_{|\eta|<0.5}$

Transverse momentum dependence of ($K^{+} + K^{-}$)/($\pi^{+} + \pi^{-}$) and ($p + \bar{p}$)/($\pi^{+} + \pi^{-}$) ratios in high-$p_T$ interval in pp collisions as a function of $\langle dN_{ch}/d\eta\rangle_{|\eta|<0.5}$

Blast-wave fit parameters

$p_{T}$-integrated ($K^{+} + K^{-}$)/($\pi^{+} + \pi^{-}$) and ($p + \bar{p}$)/($\pi^{+} + \pi^{-}$) ratios in pp collisions as a function of $\langle dN_{ch}/d\eta\rangle_{|\eta|<0.5}$

$p_{T}$-integrated (multi)strange hadron to pion ratios in pp collisions as a function of $\langle dN_{ch}/d\eta\rangle_{|\eta|<0.5}$

$p_{T}$-integrated ($\Omega^{-} + \bar{\Omega}^{+}$)/($\pi^{+} + \pi^{-}$) ratios in pp collisions as a function of $\langle dN_{ch}/d\eta\rangle_{|\eta|<0.5}$

Average transverse momentum of $\pi^{+} + \pi^{-}$, $K^{+} + K^{-}$, and $p + \bar{p}$ as a function of $\langle dN_{ch}/d\eta\rangle_{|\eta|<0.5}$

Transverse momentum spectra ratios ($K^{+} + K^{-}$)/($\pi^{+} + \pi^{-}$) in V0M multiplicity classes

Transverse momentum spectra ratios ($K^{+} + K^{-}$)/($\pi^{+} + \pi^{-}$) in V0M multiplicity classes

Transverse momentum spectra ratios ($p + \bar{p}$)/($\pi^{+} + \pi^{-}$) in V0M multiplicity classes

Transverse momentum spectra ratios ($p + \bar{p}$)/($\pi^{+} + \pi^{-}$) in V0M multiplicity classes

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

Fig. A1: Number density $N_{ch}$ (left) and $\\Sigma p_{T}$ (right) distributions as a function of pleadingT and the comparisons to MC predictions in Toward (top), Transverse (middle), and Away (bottom) regions for $p_{T}^{track} >$ 0.5 GeV/$c$. The shaded areas in the upper panels represent the systematic uncertainties and vertical error bars indicate statistical uncertainties. In the lower panels, the shaded areas are the sum in quadrature of statistical and systematic uncertainties from the upper panels. No uncertainties are given for the MC calculations.

Fig. A2: Number density $N_{ch}$ (left) and $\\Sigma p_{T}$ (right) distributions as a function of pleadingT and the comparisons to MC predictions in Toward (top), Transverse (middle), and Away (bottom) regions for $p_{T}^{track} >$ 1.0 GeV/$c$. The shaded areas in the upper panels represent the systematic uncertainties and vertical error bars indicate statistical uncertainties. In the lower panels, the shaded areas are the sum in quadrature of statistical and systematic uncertainties from the upper panels. No uncertainties are given for the MC calculations.

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

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

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

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

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

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

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

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

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

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

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

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 $D^{+} + D^{-}$ 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 $D^{*+} + D^{*-}$ 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 $D_{s}^{+}$ 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 $D_{s}^{+}$ 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 $D_{s}^{+}$ 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 FSR correction applied as a function of $\phi ^ * _ \eta$ for electrons.

The FSR correction applied as a function of the boson transverse momentum.

The measured differential cross-sections as a function of the boson rapidity for muons. The first uncertainty is due to the size of the dataset, the second is due to experimental systematic uncertainties, and the third is due to the luminosity.

The measured differential cross-sections as a function of the boson rapidity for electrons. The first uncertainty is due to the size of the dataset, the second is due to experimental systematic uncertainties, and the third is due to the luminosity.

The measured differential cross-sections as a function of $\phi ^ * _ \eta$ for muons. The first uncertainty is due to the size of the dataset, the second is due to experimental systematic uncertainties, and the third is due to the luminosity.

The measured differential cross-sections as a function of $\phi ^ * _ \eta$ for electrons. The first uncertainty is due to the size of the dataset, the second is due to experimental systematic uncertainties, and the third is due to the luminosity.

The measured differential cross-sections as a function of pT . The first uncertainty is due to the size of the dataset, the second is due to experimental systematic uncertainties, and the third is due to the luminosity.

The correlation matrix for the differential cross-section measurement as a function of Z boson rapidity, for the dimuon final state, excluding the luminosity uncertainty, which is fully correlated between bins.

The correlation matrix for the differential cross-section measurements as a function of the Z boson rapidity, for the dielectron final state, excluding the luminosity uncertainty, which is fully correlated between bins.

The correlation matrix for the differential cross-section measurement as a function of $\phi ^ * _ \eta$ , for the dimuon final state, excluding the luminosity uncertainty, which is fully correlated between bins.

The correlation matrix for the differential cross-section measurements as a function of $\phi ^ * _ \eta$ , for the dielectron final state, excluding the luminosity uncertainty, which is fully correlated between bins.

The correlation matrix for the differential cross-section measurements as a function of boson pT , for the dimuon final state, excluding the luminosity uncertainty, which is fully correlated between bins.

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, $R_{13/7}$, 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, $R_{13/7}$, 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, $R_{13/7}$, 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, $R_{13/7}$, 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 $D_{s}^{+}$ 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 $D_{s}^{+}$ 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 $D_{s}^{+}$ 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-sections as a function of $p_\perp$ integrated over $y$ for prompt $J/\psi$ mesons. The first uncertainties are statistical and the second (third) are uncorrelated (correlated) systematic uncertainties amongst bins.

Differential cross-sections as a function of $p_\perp$ integrated over $y$ for $J/\psi$-from-$b$ mesons. The first uncertainties are statistical and the second (third) are uncorrelated (correlated) systematic uncertainties amongst bins.

Differential cross-sections as a function of $y$ integrated over $p_\perp$ for prompt $J/\psi$ mesons. The first uncertainties are statistical and the second (third) are the correlated (uncorrelated) systematic uncertainties.

Differential cross-sections as a function of $y$ integrated over $p_\perp$ for $J/\psi$-from-$b$ mesons. The first uncertainties are statistical and the second (third) are the correlated (uncorrelated) systematic uncertainties.

Ratios of differential cross-sections between measurements at $\sqrt{s} = 13$ TeV and $\sqrt{s} = 8$ TeV as a function of $p_\perp$ in bins of $y$ for prompt $J/\psi$ mesons. The systematic errors are negligible.

Ratios of differential cross-sections between measurements at $\sqrt{s} = 13$ TeV and $\sqrt{s} = 8$ TeV as a function of $p_\perp$ in bins of $y$ for $J/\psi$-from-$b$ mesons. The systematic errors are negligible.

Ratios of differential cross-sections between measurements at $\sqrt{s} = 13$ TeV and $\sqrt{s} = 8$ TeV as a function of $y$ integrated over $p_\perp$ for prompt $J/\psi$ mesons. The systematic errors are negligible.

Ratios of differential cross-sections between measurements at $\sqrt{s} = 13$ TeV and $\sqrt{s} = 8$ TeV as a function of $y$ integrated over $p_\perp$ for $J/\psi$-from-$b$ mesons. The systematic errors are negligible.

Ratios of differential cross-sections between measurements at $\sqrt{s} = 13$ TeV and $\sqrt{s} = 8$ TeV as a function of $p_\perp$ integrated over $y$ for prompt $J/\psi$ mesons.

Ratios of differential cross-sections between measurements at $\sqrt{s} = 13$ TeV and $\sqrt{s} = 8$ TeV as a function of $p_\perp$ integrated over $y$ for $J/\psi$-from-$b$ mesons. The systematic errors are negligible.