Nuclear modification factor of $\Upsilon(1\mathrm{S})$ as a function of the average number of participants $\langle N_{\mathrm{part}} \rangle$ or as a function of the collision centrality.

Nuclear modification factor of $\Upsilon(2\mathrm{S})$ as a function of the average number of participants $\langle N_{\mathrm{part}} \rangle$ or as a function of the collision centrality.

Ratio of $\Upsilon(2\mathrm{S})$ and $\Upsilon(1\mathrm{S})$ yields (cf. equation 2 in the article for the definition) as a function of the average number of participants $\langle N_{\mathrm{part}} \rangle$ or as a function of the collision centrality. The global uncertainty is the quadratic sum of the branching ratio uncertainties.

Relative nuclear modification factor or double yield ratio between $\Upsilon(2\mathrm{S})$ and $\Upsilon(1\mathrm{S})$ as a function of the average number of participants $\langle N_{\mathrm{part}} \rangle$ or as a function of the collision centrality. The global uncertainty corresponds to the systematic uncertainty on the cross-section ratio in proton–proton collisions.

Nuclear modification factor of $\Upsilon(1\mathrm{S})$ as a function of transverse momentum for the 0–90% centrality interval.

Nuclear modification factor of $\Upsilon(1\mathrm{S})$ as a function of rapidity for the 0–90% centrality interval.

Nuclear modification factor of $\Upsilon(2\mathrm{S})$ as a function of rapidity for the 0–90% centrality interval.

Interpolated production cross sections and cross-section ratio for $\Upsilon(1\mathrm{S}) \rightarrow \mu^{+}\mu^{-}$ and $\Upsilon(2\mathrm{S}) \rightarrow \mu^{+}\mu^{-}$ in proton–proton collisions, integrated over the rapidity interval 2.5–4.0 and $p_{\mathrm{T}} <$ 15 GeV/$c$. Results used for the determination of the integrated nuclear modification factors and of the nuclear modification factors as a function of centrality (Figures 4 and 5 (right)).

Interpolated $p_{\mathrm{T}}$-differential cross section for $\Upsilon(1\mathrm{S}) \rightarrow \mu^{+}\mu^{-}$ in proton–proton collisions. Results used for the determination of the nuclear modification factor of $\Upsilon(1\mathrm{S})$ as a function of its transverse momentum (Figure 6).

Interpolated rapidity-differential cross section for $\Upsilon(1\mathrm{S}) \rightarrow \mu^{+}\mu^{-}$ in proton–proton collisions. Results used for the determination of the nuclear modification factor of $\Upsilon(1\mathrm{S})$ as a function of rapidity (Figure 7).

Interpolated rapidity-differential cross section for $\Upsilon(2\mathrm{S}) \rightarrow \mu^{+}\mu^{-}$ in proton–proton collisions. Results used for the determination of the nuclear modification factor of $\Upsilon(2\mathrm{S})$ as a function of rapidity (Figure 7).

Double-differential yields, $\frac{d^{2}n}{x_{_F}p_{_T}}$ and $f_n(x_{_F},p_{T})$, for $x_{_F}>0$.

$p_{_T}$ integrated yield $\frac{dn}{dy}$, the inverse slope parameter $T$ and the mean transverse mass $\langle m_{_T}\rangle - m_{\Lambda}$.

$p_{_T}$ integrated yield $\frac{dn}{x_{_F}}$ and the invariant cross section $F(x_{_F})$.

$p_{\rm T}$-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.

D$^{0}$-meson relative yields for the sum of particle and antiparticle in several multiplicity and PT intervals for pp collisions at $\sqrt{s}=7$ TeV as a function of the relative average multiplicity in the V0 detector, $N_{V0} \big/ \langle N_{V0} \rangle$. The yields reported here are not corrected by the trigger selection efficiency, they are normalised to the visible cross section.

Fraction of non-prompt JPSI measured for PT > 1.3 GeV/c, $f_{\rm B}$(%), and extrapolated down to PT > 0, $f_{\rm B}^{\rm extr}$(%) in the various multiplicity intervals. The first and second uncertainties correspond to the statistical and systematic uncertainties, respectively.

Prompt and non-prompt relative JPSI relative yields for PT > 0 in the in different multiplicity bins. The first and second uncertainties correspond to the statistical and systematic uncertainties respectively. The yields reported here are normalised to the inelastic cross section.

Prompt and non-prompt relative JPSI relative yields for PT > 0 in the in different multiplicity bins. The first and second uncertainties correspond to the statistical and systematic uncertainties respectively. The yields reported here are not corrected by the trigger selection efficiency, they are normalised to the visible cross section.

dN/dy and MEAN(PT) extracted from Levy-Tsallis fits to the measured PI, K, P spectra at mid-rapidity in inelastic pp collisions at SQRT(S) = 7 TeV. Combined statistical and systematic uncertainties (statistical uncertainties are negligible) are reported. The systematic uncertainty on dN/dy due to normalization to inelastic collisions (+7-4%) is not included. Integrated yields of Kaon/Pion and Proton/Pion ratios are also reported with combined statistical and systematic uncertainties (statistical uncertainties are negligible).

dN/dy and MEAN(PT) extracted from Levy-Tsallis fits to the measured PI, K, P spectra at mid-rapidity in inelastic pp collisions at SQRT(S) = 2.76 TeV. Combined statistical and systematic uncertainties (statistical uncertainties are negligible) are reported. The systematic uncertainty on dN/dy due to normalization to inelastic collisions (+6-4%) is not included. Integrated yields of Kaon/Pion and Proton/Pion ratios are also reported with combined statistical and systematic uncertainties (statistical uncertainties are negligible).

The measured Z boson production cross section in pp collisions as a function of the Z boson rapidity for the dielectron decay channel.

Event centrality dependence of the $\mbox{Z}\rightarrow\mu^{+}\mu^{-}$ yields per MB event in PbPb collisions, divided by the expected average nuclear overlap function, $T_{\rm AA}$. On the horizontal axis, event centrality is depicted as the average number of participating nucleons, $N_{\rm part}$.

Event centrality dependence of the $\mbox{Z}\rightarrow e^{+}e^{-}$ yields per MB event in PbPb collisions, divided by the expected average nuclear overlap function, $T_{\rm AA}$. On the horizontal axis, event centrality is depicted as the average number of participating nucleons, $N_{\rm part}$.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson $p_{\rm T}$ for the dimuon decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson $p_{\rm T}$ for the dielectron decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson rapidity for the dimuon decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson rapidity for the dielectron decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson rapidity for the combined leptonic decay channel.

The measured Z boson yields per MB event in PbPb collisions as a function of the Z boson $p_{\rm T}$ for the combined leptonic decay channel.

Event centrality dependence of the $\mbox{Z}\rightarrow l^{+}l^{-}$ yields per MB event in PbPb collisions, divided by the expected average nuclear overlap function, $T_{\rm AA}$. On the horizontal axis, event centrality is depicted as the average number of participating nucleons, $N_{\rm part}$.

The measured Z boson production cross section in pp collisions as a function of the Z boson rapidity for the combined leptonic decay channel.

The measured Z boson production cross section in pp collisions as a function of the Z boson pT for the combined leptonic decay channel in |y|<1.44.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 20 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse momentum spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 20 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 20 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 20 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 20 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 31 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 40 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 80 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Transverse mass spectra of $\pi^-$ mesons produced in inelastic $p p$ interactions at 158 GeV in various rapidity ranges.

Inverse slope parameter T as a function of rapidity for the 5 beam momenta.

Rapidity spectra for the 5 beam momenta.

Mean transverse mass as a function of rapidity for the 5 beam momenta.

Numerical values of the parameters fitted to the rapidiy distributions.

pT-differential production yields for Xi- and XiBar+ baryons with centrality 40-60%.

pT-differential production yields for Xi- and XiBar+ baryons with centrality 60-80%.

pT-differential production yields for Omega- and OmegaBar+ baryons with centrality 0-10%.

pT-differential production yields for Omega- and OmegaBar+ baryons with centrality 10-20%.

pT-differential production yields for Omega- and OmegaBar+ baryons with centrality 20-40%.

pT-differential production yields for Omega- and OmegaBar+ baryons with centrality 40-60%.

pT-differential production yields for Omega- and OmegaBar+ baryons with centrality 60-80%.

Total integrated mid-rapidity yields for multi-strange baryon production in Pb-Pb collisions at sqrt(sNN) = 2.76 TeV, for different centrality intervals. For each centrality interval the average number of participants, Npart, is also reported.

Enhancements with respect to pp collisions for multi-strange baryon production.

Ratios to pions for multi-strange baryons produced in pp collisions.

Ratios to pions for multi-strange baryons produced in Pb-Pb collisions.

The corrected per-event transverse momentum distribution of Z bosons in the centrality region 10-20%.

The corrected per-event transverse momentum distribution of Z bosons in the centrality region 20-40%.

The corrected per-event transverse momentum distribution of Z bosons in the centrality region 40-80%.

Combined results for the centrality (Npart) dependence of Z boson yields divided by Ncoll for the PT range > 0 GeV/c. The systematic error includes the uncertainty in Ncoll.

Combined results for the centrality (Npart) dependence of Z boson yields divided by Ncoll for the PT range 0 to 10 GeV/c. The systematic error includes the uncertainty in Ncoll.

Combined results for the centrality (Npart) dependence of Z boson yields divided by Ncoll for the PT range 10 to 30 GeV/c. The systematic error includes the uncertainty in Ncoll.

Combined results for the centrality (Npart) dependence of Z boson yields divided by Ncoll for the PT range > 30 GeV/c. The systematic error includes the uncertainty in Ncoll.

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV.

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV.

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV.

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 1 (Nrec=0-9).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 2 (Nrec=10-19).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 3 (Nrec=20-29).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 4 (Nrec=30-39).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 5 (Nrec=40-49).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 6 (Nrec=50-59).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 900 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 900 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 7 (Nrec=60-69).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 8 (Nrec=70-79).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 8 (Nrec=70-79).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 8 (Nrec=70-79).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 8 (Nrec=70-79).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 2760 GeV for multiplicity class 9 (Nrec=80-89).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 2760 GeV for multiplicity class 9 (Nrec=80-89).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 9 (Nrec=80-89).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 9 (Nrec=80-89).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 10 (Nrec=90-99).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 10 (Nrec=90-99).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 11 (Nrec=100-109).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 11 (Nrec=100-109).

Measured transverse momentum distributions of identified charged hadrons (PI+, K+ and P) and at a centre-of-mass energy of 7000 GeV for multiplicity class 12 (Nrec=110-119).

Measured transverse momentum distributions of identified charged hadrons (PI-, K- and PBAR) and at a centre-of-mass energy of 7000 GeV for multiplicity class 12 (Nrec=110-119).

Tsallis-Pareto-type fits to the PI+ data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI- data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K+ data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K- data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the P data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PBAR data at a centre-of-mass energy of 900 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI+ data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI- data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K+ data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K- data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the P data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PBAR data at a centre-of-mass energy of 2760 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI+ data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PI- data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K+ data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the K- data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the P data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

Tsallis-Pareto-type fits to the PBAR data at a centre-of-mass energy of 7000 GeV tabulated as a function of the multiplicity class Fit A - using the combined statistical and systematic error. Fit B - using the systematic error only as the statistical error is small.

The corrected transverse momentum distribution of KS mesons at 900 GeV.

The corrected rapidity distribution of KS mesons at 900 GeV.

The corrected multiplicity distribution of KS mesons at 900 GeV.

The corrected transverse momentum distribution of LAMBDA baryons at 7000 GeV.

The corrected rapidity distribution of LAMBDA baryons at 7000 GeV.

The corrected multiplicity distribution of LAMBDA baryons at 7000 GeV.

The corrected transverse momentum distribution of LAMBDA baryons at 900 GeV.

The corrected rapidity distribution of LAMBDA baryons at 900 GeV.

The corrected multiplicity distribution of LAMBDA baryons at 900 GeV.

The production ratio between LAMBDABAR and LAMBDA baryons at 7000 GeV as a function of rapidity.

The production ratio between LAMBDABAR and LAMBDA baryons at 7000 GeV as a function of transverse momentum.

The production ratio between LAMBDABAR and LAMBDA baryons at 900 GeV as a function of rapidity.

The production ratio between LAMBDABAR and LAMBDA baryons at 900 GeV as a function of transverse momentum.

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.

CHI distribution for mass bin > 1200 GeV.

Centrality Ratio.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

Double differential cross sections for PI+ and PI- in P P interactions at 158 GeV.

PT integrated invariant cross sections and density distributions together with mean values of PT and PT**2 as a function of Feynman X for positive pion production.

PT integrated invariant cross sections and density distributions together with mean values of PT and PT**2 as a function of Feynman X for negative pion production.

PT integrated rapidity distribution.

The total mean multiplicities.

PI- transverse mass spectra, in the midrapidity region 0.0 > y > 0.2, from PB PB collisions at incident beam momentum 40 GeV/nucleon.

PI- transverse mass spectra, in the midrapidity region 0.0 > y > 0.2, from PB PB collisions at incident beam momentum 80 GeV/nucleon.

PI- transverse mass spectra, in the midrapidity region 0.0 > y > 0.2, from PB PB collisions at incident beam momentum 158 GeV/nucleon.

K+ transverse mass spectra, in the midrapidity region -0.1 > y > 0.1, from PB PB collisions at incident beam momentum 40 GeV/nucleon.

K+ transverse mass spectra, in the midrapidity region -0.1 > y > 0.1, from PB PB collisions at incident beam momentum 80 GeV/nucleon.

K+ transverse mass spectra, in the midrapidity region -0.1 > y > 0.1, from PB PB collisions at incident beam momentum 158 GeV/nucleon.

K- transverse mass spectra, in the midrapidity region -0.1 > y > 0.1, from PB PB collisions at incident beam momentum 40 GeV/nucleon.

K- transverse mass spectra, in the midrapidity region -0.1 > y > 0.1, from PB PB collisions at incident beam momentum 80 GeV/nucleon.

K- transverse mass spectra, in the midrapidity region -0.1 > y > 0.1, from PB PB collisions at incident beam momentum 158 GeV/nucleon.

PI- rapidity spectra from PB PB collisions at incident beam momentum 40 GeV/nucleon.

PI- rapidity spectra from PB PB collisions at incident beam momentum 80 GeV/nucleon.

PI- rapidity spectra from PB PB collisions at incident beam momentum 158 GeV/nucleon.

K+ rapidity spectra from PB PB collisions at incident beam momentum 40 GeV/nucleon.

K+ rapidity spectra from PB PB collisions at incident beam momentum 80 GeV/nucleon.

K+ rapidity spectra from PB PB collisions at incident beam momentum 158 GeV/nucleon.

K- rapidity spectra from PB PB collisions at incident beam momentum 40 GeV/nucleon.

K- rapidity spectra from PB PB collisions at incident beam momentum 80 GeV/nucleon.

K- rapidity spectra from PB PB collisions at incident beam momentum 158 GeV/nucleon.

Total pion multiplicity per wounded nucleon as a function of Fermi. s energy measure, for central NUCLEUS NUCLEUS collisions.. The commmon systematic error on the NA49 points is +-5%.

Total pion multiplicity for all inelastic PBAR P collisions from the compilation presented in Gazdzicki and Rohrich ZP C65(95)215, C71(96)55.

Total pion multiplicity for all inelastic P P collisions from the compilation presented in Gazdzicki and Rohrich ZP C65(95)215, C71(96)55. Statistical errors (not given) are in the range 1-3%).

The energy dependence of the K+/PI+ ratio at y = 0 in PB PB and AU AU collisions. This table includes the present NA49 data as well as other data CT.= The commmon systematic error on the NA49 points is +-7%. including PHENIX and AGS data.

The energy dependence of the K-/PI- ratio at y = 0 in PB PB and AU AU collisions. This table includes the present NA49 data as well as other data includingPHENIX and AGS data, and preliminary E895 data.. The commmon systematic error on the NA49 points is +-7%.

The energy dependence of the ratio of the K+ to PI+ multiplicities in full phase space from PB PB and AU AU collisions. This table includes the present NA49 data as well as other data including AGS data.. The commmon systematic error on the NA49 points is +-7%.

A compilation of the energy dependence of the ratio of the K+ to PI+ multiplicities in full phase space from P P interactions.

The energy dependence of the ratio of the K- to PI- multiplicities in full phase space from PB PB and AU AU collisions. This table includes the present NA49 data as well as other data including AGS data.. The commmon systematic error on the NA49 points is +-7%.

The energy dependence of the K-/K+ ratio at y = 0 in PB PB and AU AU collisions. This table includes the present NA49 data as well as other data including PHENIX, PHOBOS and AGS data.. The commmon systematic error on the NA49 points is +-7%.

The energy dependence of the ratio of the LAMBDA + (KAON+KAONBAR) muliplicity total PION (PI+ + PI- + PI0) multiplicity in central PB PB and AU AU collisions. This table includes the present NA49 data as well as other data including AGS data.. The commmon systematic error on the NA49 points is +-7%.

A compilation of the energy dependence of the ratio of the LAMBDA + (KAON+KAONBAR) muliplicity to total PION (PI+ + PI- + PI0) multiplicity in P P collisions.

Rapidity distributions for PHI mesons produced in P P collisions.

Integrated yields of PHI and PI mesons and their ratio.

Multiplicity dependence of the PHI/PI ratio in P P collisions.

Centrality dependence of the PHI/PI ratio in the forward hemisphere in P PBcollisions normalised to the average P P values. Here N(C=CD) is the number emi tted in the backward direction in P PB collisions and is essentially related to the mean number of collisions of the projectile in the target.

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