$p_{\rm T}$-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.

$p_{\rm T}$-differential yields of $\Lambda$(1520) (sum of particle and anti-particle states) in p--Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ $\mathrm{=}$ 5.02 TeV in multiplicity interval 20--40\%. The uncertainty 'sys,$p_{\rm T}$-correlated' indicates the systematic uncertainty after removing the contributions of $p_{\rm T}$-uncorrelated uncertainty.

$p_{\rm T}$-differential yields of $\Lambda$(1520) (sum of particle and anti-particle states) in p--Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ $\mathrm{=}$ 5.02 TeV in multiplicity interval 40--60\%. The uncertainty 'sys,$p_{\rm T}$-correlated' indicates the systematic uncertainty after removing the contributions of $p_{\rm T}$-uncorrelated uncertainty.

$p_{\rm T}$-differential yields of $\Lambda$(1520) (sum of particle and anti-particle states) in p--Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ $\mathrm{=}$ 5.02 TeV in multiplicity interval 60--100\%. The uncertainty 'sys,$p_{\rm T}$-correlated' indicates the systematic uncertainty after removing the contributions of $p_{\rm T}$-uncorrelated uncertainty.

Ratio of $p_{\rm T}$-integrated yields of $\Lambda$(1520) (sum of particle and anti-particle states) to charged $\pi$ ($\pi^{+} + \pi^{-}$) at midrapidity as a function of $\langle {\rm d}N_{\rm ch}/{\rm d} \eta_{\rm lab} \rangle$ in inelastic pp collisions at $\sqrt{s}$ $\mathrm{=}$ 7 TeV.

Ratio of $p_{\rm T}$-integrated yields of $\Lambda$(1520) (sum of particle and anti-particle states) to charged $\pi$ ($\pi^{+} + \pi^{-}$) as a function of $\langle {\rm d}N_{\rm ch}/{\rm d} \eta_{\rm lab} \rangle$ in p--Pb collisions at $\sqrt{s}$ $\mathrm{=}$ 5.02 TeV. The uncertainty 'sys,uncorrelated' indicates the multiplicity uncorrelated systematic uncertainty.

Ratio of $p_{\rm T}$-integrated yields of $\Lambda$(1520) (sum of particle and anti-particle states) to K$^{-}$ at midrapidity as a function of $\langle {\rm d}N_{\rm ch}/{\rm d} \eta_{\rm lab} \rangle$ in inelastic pp collisions at $\sqrt{s}$ $\mathrm{=}$ 7 TeV.

Ratio of $p_{\rm T}$-integrated yields of $\Lambda$(1520) (sum of particle and anti-particle states) to K$^{-}$ as a function of $\langle {\rm d}N_{\rm ch}/{\rm d} \eta_{\rm lab} \rangle$ in p--Pb collisions at $\sqrt{s}$ $\mathrm{=}$ 5.02 TeV. The uncertainty 'sys,uncorrelated' indicates the multiplicity uncorrelated systematic uncertainty.

Ratio of $p_{\rm T}$-integrated yields of $\Lambda$(1520) (sum of particle and anti-particle states) to its ground state particle $\Lambda$ ($\Lambda + \bar{\Lambda}$) at midrapidity as a function of $\langle {\rm d}N_{\rm ch}/{\rm d} \eta_{\rm lab} \rangle$ in inelastic pp collisions at $\sqrt{s}$ $\mathrm{=}$ 7 TeV.

Ratio of $p_{\rm T}$-integrated yields of $\Lambda$(1520) (sum of particle and anti-particle states) to its ground state particle $\Lambda$ ($\Lambda + \bar{\Lambda}$) as a function of $\langle {\rm d}N_{\rm ch}/{\rm d} \eta_{\rm lab} \rangle$ in p--Pb collisions at $\sqrt{s}$ $\mathrm{=}$ 5.02 TeV. The uncertainty 'sys,uncorrelated' indicates the multiplicity uncorrelated systematic uncertainty.

$p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (NSD).

$p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (0-20% multiplicity class).

$p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (0-20% multiplicity class).

$p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-60% multiplicity class).

$p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-60% multiplicity class).

$p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-100% multiplicity class).

$p_{\rm{T}}$-differential yield of $\Sigma^{*+}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-100% multiplicity class).

$p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (NSD).

$p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (NSD).

$p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (0-20\% multiplicity class).

$p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (0-20\% multiplicity class).

$p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-40\% multiplicity class).

$p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-40\% multiplicity class).

$p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (40-60\% multiplicity class).

$p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (40-60\% multiplicity class).

$p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-100\% multiplicity class).

$p_{\rm{T}}$-differential yield of ($\Xi^{*0}+\overline{\Xi}^{*0}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-100\% multiplicity class).

$p_{\rm T}$-integrated yield d$N$/d$y$ of ($\Sigma^{*\pm}+\overline{\Sigma}^{*\mp}$)/4 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV. Yields are normalised to the visible cross section for each V0A multiplicity event class and to NSD events for the minimum bias case.

$p_{\rm T}$-integrated yield d$N$/d$y$ of ($\Sigma^{*\pm}+\overline{\Sigma}^{*\mp}$)/4 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV. Yields are normalised to the visible cross section for each V0A multiplicity event class and to NSD events for the minimum bias case.

Mean $p_{\rm T}$ of $\Sigma^{*\pm}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.

Mean $p_{\rm T}$ of $\Sigma^{*\pm}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.

$p_{\rm T}$-integrated yield d$N$/d$y$ of ($\Xi^{*0}+\overline{\Xi}^{0})$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV. Yields are normalised to the visible cross section for each V0A multiplicity event class and to NSD events for the minimum bias case.

$p_{\rm T}$-integrated yield d$N$/d$y$ of ($\Xi^{*0}+\overline{\Xi}^{0})$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV. Yields are normalised to the visible cross section for each V0A multiplicity event class and to NSD events for the minimum bias case.

Mean $p_{\rm T}$ of $\Xi^{*0}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.

Mean $p_{\rm T}$ of $\Xi^{*0}$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.

Integrated yield ratio.

Integrated yield ratio.

Integrated yield ratio.

Integrated yield ratio.

Integrated yield ratio.

Integrated yield ratio.

Integrated yield ratio.

Integrated yield ratio.

p-T differential invariant yield of Lambda + anti-Lambda in pp collisions with center-of-mass energy/nucleon = 7 TeV.

p-T differential invariant yield of Xi+ + Xi- in pp collisions with center-of-mass energy/nucleon = 7 TeV.

p-T differential invariant yield of Xi+ + Xi- in pp collisions with center-of-mass energy/nucleon = 7 TeV.

p-T differential invariant yield of K0s in pPb collisions with center-of-mass energy/nucleon = 5.02 TeV.

p-T differential invariant yield of K0s in pPb collisions with center-of-mass energy/nucleon = 5.02 TeV.

p-T differential invariant yield of Lambda + anti-Lambda in pPb collisions with center-of-mass energy/nucleon = 5.02 TeV.

p-T differential invariant yield of Lambda + anti-Lambda in pPb collisions with center-of-mass energy/nucleon = 5.02 TeV.

p-T differential invariant yield of Xi+ + Xi- in pPb collisions with center-of-mass energy/nucleon = 5.02 TeV.

p-T differential invariant yield of Xi+ + Xi- in pPb collisions with center-of-mass energy/nucleon = 5.02 TeV.

p-T differential invariant yield of K0s in PbPb collisions with center-of-mass energy/nucleon = 2.76 TeV.

p-T differential invariant yield of K0s in PbPb collisions with center-of-mass energy/nucleon = 2.76 TeV.

p-T differential invariant yield of Lambda + anti-Lambda in PbPb collisions with center-of-mass energy/nucleon = 2.76 TeV.

p-T differential invariant yield of Lambda + anti-Lambda in PbPb collisions with center-of-mass energy/nucleon = 2.76 TeV.

p-T differential invariant yield of Xi+ + Xi- in PbPb collisions with center-of-mass energy/nucleon = 2.76 TeV.

p-T differential invariant yield of Xi+ + Xi- in PbPb collisions with center-of-mass energy/nucleon = 2.76 TeV.

pT-dependent Lambda+anti-Lambda to K0S production ratios in pp collisions with centre-of-mass energy = 7 TeV.

pT-dependent Lambda+anti-Lambda to K0S production ratios in pPb collisions with centre-of-mass energy/nucleon = 5.02 TeV.

pT-dependent Lambda+anti-Lambda to K0S production ratios in PbPb collisions with centre-of-mass energy/nucleon = 2.76 TeV.

pT-dependent Xi+ + Xi- to Lambda+anti-Lambda production ratios in pp collisions with centre-of-mass energy = 7 TeV.

pT-dependent Xi+ + Xi- to Lambda+anti-Lambda production ratios in pPb collisions with centre-of-mass energy/nucleon = 5.02 TeV.

pT-dependent Xi+ + Xi- to Lambda+anti-Lambda production ratios in PbPb collisions with centre-of-mass energy/nucleon = 2.76 TeV.

Simultenous blast-wave fits parameters in pp collisions with center-of-mass energy/nucleon = 7 TeV.

Simultenous blast-wave fits parameters in pPb collisions with center-of-mass energy/nucleon = 5.02 TeV.

Simultenous blast-wave fits parameters in PbPb collisions with center-of-mass energy/nucleon = 2.76 TeV.

Mean transverse kinetic energy MEAN(KE_T) of K0s in pp collisions with centre-of-mass energy/nucleon=7 TeV.

Mean transverse kinetic energy MEAN(KE_T) of Lambda+anti-Lambda in pp collisions with centre-of-mass energy/nucleon=7 TeV.

Mean transverse kinetic energy MEAN(KE_T) of K0s in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Mean transverse kinetic energy MEAN(KE_T) of Lambda+anti-Lambda in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Mean transverse kinetic energy MEAN(KE_T) of Xi+ + Xi- in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Mean transverse kinetic energy MEAN(KE_T) of K0s in PbPb collisions with centre-of-mass energy/nucleon=2.76 TeV.

Mean transverse kinetic energy MEAN(KE_T) of Lambda + anti-Lambda in PbPb collisions with centre-of-mass energy/nucleon=2.76 TeV.

p-T differential invariant yield of K0s in pPb collisions with center-of-mass energy/nucleon = 5.02 TeV.

p-T differential invariant yield of Lambda + anti-Lambda in pPb collisions with center-of-mass energy/nucleon = 5.02 TeV.

p-T differential invariant yield of K0s in pPb collisions with center-of-mass energy/nucleon = 5.02 TeV.

p-T differential invariant yield of Lambda + anti-Lambda in pPb collisions with center-of-mass energy/nucleon = 5.02 TeV.

p-T differential invariant yield of K0s in pPb collisions with center-of-mass energy/nucleon = 5.02 TeV.

p-T differential invariant yield of Lambda + anti-Lambda in pPb collisions with center-of-mass energy/nucleon = 5.02 TeV.

pT-dependent Lambda+Anti-Lambda to K0S production ratios in pPb collisions with centre-of-mass energy/nucleon = 5.02 TeV.

Mean transverse kinetic energy MEAN(KE_T) of K0s in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Mean transverse kinetic energy MEAN(KE_T) of Lambda + anti-Lambda in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

$p_{\rm T}$-differential yield of (K$^{*0}$ + $\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-40% multiplicity class).

$p_{\rm T}$-differential yield of (K$^{*0}$ + $\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (40-60% multiplicity class).

$p_{\rm T}$-differential yield of (K$^{*0}$ + $\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-80% multiplicity class).

$p_{\rm T}$-differential yield of (K$^{*0}$ + $\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (80-100multiplicity class).

$p_{\rm T}$-differential invariant yield of $phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (NSD). Additional systematic error: +- 3.1% (normalization).

$p_{\rm T}$-differential yield of $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (0-5% multiplicity class).

$p_{\rm T}$-differential yield of $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (5-10% multiplicity class).

$p_{\rm T}$-differential yield of $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (10-20% multiplicity class).

$p_{\rm T}$-differential yield of $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-40% multiplicity class).

$p_{\rm T}$-differential yield of $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (40-60% multiplicity class).

$p_{\rm T}$-differential yield of $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-80% multiplicity class).

$p_{\rm T}$-differential yield of $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (80-100% multiplicity class).

$p_{\rm T}$-integrated yield d$N$/d$y$ of (K$^{*0}$ + $\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV. Yields are normalised to the visible cross section for each V0A multiplicity event class and to NSD events for the minimum bias case (additional normalization systematic error: +- 3.1%).

Mean $p_{\rm T}$ of (K$^{*0}$ + $\overline{K^{*0}}$)/2 in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.

$p_{\rm T}$-integrated yield d$N$/d$y$ of $phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV. Yields are normalised to the visible cross section for each V0A multiplicity event class and to NSD events for the minimum bias case (additional normalization systematic error: +- 3.1%).

Mean $p_{\rm T}$ of $phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV for each V0A multiplicity event class.

Mean $p_{\rm T}$ as function of the mass for particles measured with the ALICE detector in INEL pp collisions at $\sqrt{s}$ = 7 TeV in |y| < 0.5.

Mean $p_{\rm T}$ as function of the mass for particles measured with the ALICE detector in 0-20% p-Pb collisions at $\sqrt{s_{\mathrm{NN}}}$ = 5.02 TeV in -0.5 < y < 0.

Ratio of $p_{\rm T}$-differential yields of (p + $\bar{p}$) and $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (0-5$\%$ multiplicity class).

Ratio of $p_{\rm T}$-differential yields of (p + $\bar{p}$) and $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (5-10% multiplicity class).

Ratio of $p_{\rm T}$-differential yields of (p + $\bar{p}$) and $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (10-20% multiplicity class).

Ratio of $p_{\rm T}$-differential yields of (p + $\bar{p}$) and $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (20-40% multiplicity class).

Ratio of $p_{\rm T}$-differential yields of (p + $\bar{p}$) and $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (40-60% multiplicity class).

Ratio of $p_{\rm T}$-differential yields of (p + $\bar{p}$) and $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (60-80% multiplicity class).

Ratio of $p_{\rm T}$-differential yields of (p + $\bar{p}$) and $\phi$ in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV (80-100% multiplicity class).

Ratio of $p_{\rm T}$-integrated yields of $(K^{*0}+\overline{K^{*0}})$ to long lived hadrons for different V0A multiplicity classes in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Ratio of $p_{\rm T}$-integrated yields of 2$\phi$ to long lived hadrons for different V0A multiplicity classes in p-Pb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of charged pions in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of charged kaons in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of charged kaons in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of charged kaons in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of charged kaons in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of k0s in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of k0s in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of k0s in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of k0s in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of protons+antiprotons in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of protons+antiprotons in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of protons+antiprotons in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of protons+antiprotons in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of lambdas+antilambdas in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of lambdas+antilambdas in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of lambdas+antilambdas in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-differential invariant yield of lambdas+antilambdas in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-dependent charged kaon to charged pion production ratios in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-dependent charged kaon to charged pion production ratios in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-dependent charged kaon to charged pion production ratios in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-dependent charged kaon to charged pion production ratios in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-dependent proton+antiproton to charged pion production ratios in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-dependent proton+antiproton to charged pion production ratios in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-dependent proton+antiproton to charged pion production ratios in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-dependent proton+antiproton to charged pion production ratios in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-dependent lambda+antilambda to k0s production ratios in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-dependent lambda+antilambda to k0s production ratios in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-dependent lambda+antilambda to k0s production ratios in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

pT-dependent lambda+antilambda to k0s production ratios in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Mean transverse momentum of lambdas+antilambdas in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Mean transverse momentum of lambdas+antilambdas in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Mean transverse momentum of protons+antiprotons in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Mean transverse momentum of protons+antiprotons in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Mean transverse momentum of k0s in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Mean transverse momentum of k0s in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Mean transverse momentum of charged kaons in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Mean transverse momentum of charged kaons in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Mean transverse momentum of charged pions in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Mean transverse momentum of charged pions in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Integrated production ratios in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Integrated production ratios in pPb collisions with centre-of-mass energy/nucleon=5.02 TeV.

Integrated production yield of pions in pPb collisions at sqrts 5.02 TeV.

Integrated production yield of charged kaons in pPb collisions at sqrts 5.02 TeV.

Integrated production yield of K0S in pPb collisions at sqrts 5.02 TeV.

Integrated production yield of protons+antiprotons in pPb collisions at sqrts 5.02 TeV.

Integrated production yield of lambda+antilambda in pPb collisions at sqrts 5.02 TeV.

PHI transverse momentum spectra at incident energy 80 GeV/nucleon integrated over the rapidity range 0 to 1.7.

PHI transverse momentum spectra at incident energy 158 GeV/nucleon integrated over the rapidity range 0 to 1.0.

PHI transverse mass spectra at incident energy 20 GeV/nucleon integrated over the rapidity range 0 to 1.8.

PHI transverse mass spectra at incident energy 30 GeV/nucleon integrated over the rapidity range 0 to 1.8.

PHI transverse mass spectra at incident energy 40 GeV/nucleon integrated over the rapidity range 0 to 1.5.

PHI transverse mass spectra at incident energy 80 GeV/nucleon integrated over the rapidity range 0 to 1.7.

PHI transverse mass spectra at incident energy 158 GeV/nucleon integrated over the rapidity range 0 to 1.0.

Slope parameter as a function of rapidity for incident energy 158 GeV/nucleon. Here slope is defined as :-. DN/DPT = CONST*PT*EXP(-MT/SLOPE).

PHI rapidity distributions for incident energy 20 GeV/nucleon.

PHI rapidity distributions for incident energy 30 GeV/nucleon.

PHI rapidity distributions for incident energy 40 GeV/nucleon.

PHI rapidity distributions for incident energy 80 GeV/nucleon.

PHI rapidity distributions for incident energy 158 GeV/nucleon.

PHI/PI ratio extrapolated to final phase space.

PHI/PI ratio at mid rapidity.

PHI multiplicity.

Values of slope parameter, mean PT and mean MT as a function of energy.

Mean PT^2 values at forward rapidities (absolute value of y belongs to [1.2;2.2]), for different bins of centrality.

J/PSI invariant yield versus rapidity for 0-20%, 20-40%, 40-60%, 60-92% centrality, at mid rapidity :,-0.35<y<0.35 An up/down correction, to translate each point at the center of it's relative bin, have been applied to the data.

J/PSI invariant yield versus rapidity for 0-20%, 20-40%, 40-60%, 60-92% centrality,at forward rapidities (absolute value of y belongs to [1.2;2.2]). An up/down correction, to translate each point at the center of it's relative bin, have been applied to the data.

Nuclear modification factor Raa versus transverse momentum for 0-20%, 20-40%, 40-60%, 60-92% centrality, at mid rapidities :-0.35<y<0.35. An additional +- 10% (resp. +- 10%, +- 13%, +- 28%) global uncertainty, associated with the calculation of the number of binary collisions and the J/PSI yield in p+p, is not shown for the 0-20% (resp. 20-40%,40-60%, 60-92%) centrality bin.

Nuclear modification factor Raa versus transverse momentum for 0-20%, 20-40%, 40-60%, 60-92% centrality, at forward rapidities : absolute value of y belongs to [1.2;2.2] An additional +- 10% (resp. +- 10%, +- 13%, +- 28%) global uncertainty, associated with the calculation of the number of binary collisions and the J/PSI yield in p+p, is not shown for the 0-20% (resp. 20-40%,40-60%, 60-92%) centrality bin. An up/down correction, to translate each point at the center of it's relative bin, have been applied to the data.

Nuclear modification factor Raa versus rapidity for 0-20%, 20-40%, 40-60%, 60-92% centrality, at mid rapidities :,-0.35<y<0.35. An additional +- 10% (resp. +- 10%, +- 13%, +- 28%) global uncertainty, associated with the calculation of the number of binary collisions and the J/PSI yield in p+p, is not shown for the 0-20% (resp. 20-40%,40-60%, 60-92%) centrality bin.

Nuclear modification factor Raa versus rapidity for 0-20%, 20-40%, 40-60%, 60-92% centrality, at forward rapidities : absolute value of y belongs to [1.2;2.2] An additional +- 10% (resp. +- 10%, +- 13%, +- 28%) global uncertainty, associated with the calculation of the number of binary collisions and the J/PSI yield in p+p, is not shown for the 0-20% (resp. 20-40%,40-60%, 60-92%) centrality bin.

The number of participants Npart and the nuclear modification factor Raa versus centrality at mid rapidities :,-0.35<y<0.35. An additional +- 12% global uncertainty, associated with the calculation of the number of binary collisions and the J/PSI yield in p+p, is not shown.

The number of participants Npart and the nuclear modification factor Raa versus centrality at forward rapidities : absolute value of y belongs to [1.2;2.2] An additional +- 7% global uncertainty, associated with the calculation of the number of binary collisions and the J/PSI yield in p+p, is not shown.

Ratio of nuclear modification factors RAA(forward rapidity)/RAA(mid rapidity), versus centrality. For the two most central bins, mid rapidity points have been combined to form the ratio with the forward rapidity points. See previous tables. An additional globaluncertainty of +- 14% is not included.

Nuclear modification factor as a function of PT, for 10-20% central reactions Note that the systematic error given is related to the the uncertainties in the p+p measurements.An additional systematic error, symmetrical on the + and - side, related to the uncertainties in the Au+Au measurement, is given in the second column. Another, PT-independant, 13%systematic error due to the uncertainty on the overlap function and the Pi0 yield normalization is to add.

Nuclear modification factor as a function of PT, for 20-40% central reactions Note that the systematic error given is related to the the uncertainties in the p+p measurements.An additional systematic error, symmetrical on the + and - side, related to the uncertainties in the Au+Au measurement, is given in the second column. Another, PT-independant, 13%systematic error due to the uncertainty on the overlap function and the Pi0 yield normalization is to add.

Nuclear modification factor as a function of PT, for 40-60% central reactions Note that the systematic error given is related to the the uncertainties in the p+p measurements.An additional systematic error, symmetrical on the + and - side, related to the uncertainties in the Au+Au measurement, is given in the second column. Another, PT-independant, 13%systematic error due to the uncertainty on the overlap function and the Pi0 yield normalization is to add.