$p_{\rm T}$-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.

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.

Non photonic electrons yield versus transverse momentum in D+AU collisions.

Non photonic electrons yield versus transverse momentum in P+P collisions.

D0 differential yield at mid rapidity and corresponding calculated differential charm cross section at midrapidity.

Sum of the non photonic electrons/positrons and D0 differential yield at mid rapidity and corresponding calculated differential charm cross section at midrapidity.

Total charm cross section per nucleon nucleon collision IN D+AU collisions.

Spectrum in transverse momentum of electrons created in open heavy flavor decays, for 0-10% centrality.

Spectrum in transverse momentum of electrons created in open heavy flavor decays, for 10-20% centrality.

Spectrum in transverse momentum of electrons created in open heavy flavor decays, for 20-40% centrality.

Spectrum in transverse momentum of electrons created in open heavy flavor decays, for 40-60% centrality.

Spectra in transverse momentum of electrons created in open heavy flavor decays, for 60-92% centrality.

Non photonic electrons differential yield scaled by the number of collisions, as a function of centrality. PT belongs to 0.8-4.0 GeV/c.

Non photonic electrons differential yield scaled by the number of collisions, for minimum bias collisions. PT belongs to 0.8-4.0 GeV/c.

Number of collisions as a fonction of centrality There are only systematic errors due to the calculation of Ncoll.

Number of collisions for minimum bias events There are only systematic errors due to the calculation of Ncoll.

Nuclear overlap function TAA as a function of centrality The axis is labelled with 1/SIG, because the unit of the nuclear overlap function is barn-1 There are only systematic errors due to the calculation of TAA.

Nuclear overlap function TAA for minimum bias events The axis is labelled with 1/SIG, as the unit of the nuclear overlap function is barn-1 There are only systematic errors due to the calculation of TAA.

Differential charm cross section scaled by the number of collisions, at mid rapidity, as a function of centrality The differential cross section per number of collisions D(SIG)/Ncoll is calculated as following : D(SIG)/Ncoll = D(N(cc_bar))/TAA.

Differential charm cross section scaled by the number of collisions, at mid rapidity, for minimum bias events The differential cross section per number of collisions D(SIG)/Ncoll is calculated as following : D(SIG)/Ncoll = D(N(cc_bar))/TAA.

Total charm cross section scaled by the number of collisions, as a function of centrality The total cross section per number of collisions SIG/Ncoll is calculated as following : SIG/Ncoll = N(cc_bar)/TAA.

Total charm cross section scaled by the number of collisions, for minimum bias events The total cross section per number of collisions SIG/Ncoll is calculated as following : SIG/Ncoll = N(cc_bar)/TAA.

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.

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.

$p_{\rm{T}}$-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.

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.

$p_{\rm T}$-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.