Sum of invariant mass spectra of XI-PI-, XI-PI+, XI+PI-, XI+PI+.

Sum of invariant mass spectra of XI-PI-, XI-PI+, XI+PI-, XI+PI+ with mix-background subtracted compared with NA49 result.

Numerical values of double-differential yields $d^{2}n/dydp_{T}$ presented in Fig. 10, given in units of $10^{−3} (GeV/c)^{−1}$. The first uncertainty is statistical, while the second one is systematic

Numerical values of double-differential yields $1/m_T d^{2}n/dm_{T}dy$ given in units of $10^{−3}(GeV)^{−2}$ and presented in Fig. 11; the values of $m_T−m_0$ specify the bin centers. The first uncertainty is statistical, while the second one is systematic

Numerical values of double-differential yields $1/m_T d^{2}n/dm_{T}dy$ given in units of $10^{−3}(GeV)^{−2}$ and presented in Fig. 11; the values of $m_T−m_0$ specify the bin centers. The first uncertainty is statistical, while the second one is systematic

Numerical values of double-differential yields $1/m_T d^{2}n/dm_{T}dy$ given in units of $10^{−3}(GeV)^{−2}$ and presented in Fig. 11; the values of $m_T−m_0$ specify the bin centers. The first uncertainty is statistical, while the second one is systematic

Numerical values of the $p_T$-integrated and extrapolated $dn/dy$ distribution presented in Fig. 12. The first uncertainty is statistical, while the second one is systematic. Additionally, the width of the Gaussian fit to the $dn/dy$ distribution, as well as the mean multiplicity of $K^{*}(892)^0$ mesons are shown (see the text for details)

The mean multiplicities $\langle K^{*}(892)^0\rangle$ and the widths of the rapidity distributions $\sigma_y$ obtained from $dn/dy$ distributions (see the text for details). The first uncertainty is statistical and the second systematic

The mean multiplicity of $K^{*}(892)^0$ mesons for 158 GeV/$c$ inelastic p+p interactions compared to theoretical multiplicities obtained within Hadron Gas Models

The mean multiplicities of different particle species measured in nucleus-nucleus collisions at 158$A$ GeV/$c$ by NA49 and NA61/SHINE. The total uncertainties of $\langle K^{*}(892)^0\rangle$, $\langle K^{+}\rangle$ and $\langle K^{-}\rangle$ were taken as the square roots of the sums of squares of statistical and systematic uncertainties. For NA49 p+p data, the $\langle K^{+}\rangle$ and $\langle K^{-}\rangle$ results include statistical uncertainties only($\langle K^{+}\rangle$ =0.2267$\pm$0.0006 and $\langle K^{-}\rangle$=0.1303$\pm$0.0004), whereas systematic uncertainties for total yields were not reported. Therefore, NA61/SHINE $\langle K^{+}\rangle$ and $\langle K^{-}\rangle$ values were used in the $\langle K^{*}(892)^0 \rangle / \langle K^{+} \rangle$ and $\langle K^{*}(892)^{0}\rangle / \langle K^{-} \rangle$ ratios. The numbers of $\langle K^{+} \rangle$ and $\langle K^{−}\rangle$ and their uncertainties for the 5% most central Pb+Pb collisions were multiplied by a factor 262/362 in orderto estimate charged kaon multiplicities in the 23.5% most central Pb+Pb reactions

$\lambda_{\phi}$ measured in $J/\psi$ transverse momentum bins of 0.0 < $p_T$ < 3.0 GeV/$c$ and 3.0 < $p_T$ < 10.0 GeV/$c$ overlaid with NRQCD predictions in the Helicity and Collins-Soper frames.

$\lambda_{\theta \phi}$ measured in $J/\psi$ transverse momentum bins of 0.0 < $p_T$ < 3.0 GeV/$c$ and 3.0 < $p_T$ < 10.0 GeV/$c$ overlaid with NRQCD predictions in the Helicity and Collins-Soper frames.

$\lambda_{\theta \phi}$ measured in $J/\psi$ transverse momentum bins of 0.0 < $p_T$ < 3.0 GeV/$c$ and 3.0 < $p_T$ < 10.0 GeV/$c$ overlaid with NRQCD predictions in the Helicity and Collins-Soper frames.

$\bar{\lambda}$ measured in $J/\psi$ transverse momentum bins of 0.0 < $p_T$ < 3.0 GeV/$c$ and 3.0 < $p_T$ < 10.0 GeV/$c$ overlaid with CSM and NRQCD predictions in the Helicity frame.

$\bar{\lambda}$ measured in $J/\psi$ transverse momentum bins of 0.0 < $p_T$ < 3.0 GeV/$c$ and 3.0 < $p_T$ < 10.0 GeV/$c$ overlaid with CSM and NRQCD predictions in the Helicity frame.

Invariant $F$ measured in $J/\psi$ transverse momentum bins of 0.0 < $p_T$ < 3.0 GeV/$c$ and 3.0 < $p_T$ < 10.0 GeV/$c$ overlaid with CSM and NRQCD predictions in the Helicity frame.

Invariant $F$ measured in $J/\psi$ transverse momentum bins of 0.0 < $p_T$ < 3.0 GeV/$c$ and 3.0 < $p_T$ < 10.0 GeV/$c$ overlaid with CSM and NRQCD predictions in the Helicity frame.

$b\bar{b}$ invariant yield measured via B meson decay to like-sign dimuons as a function of pair $p_{T}$. The statistical and systematic uncertainties vary point-to-point and are listed for each measured value. An additional global systematic uncertainty is provided in each column heading, which applies to all data points per column.

Integrated away-side $\gamma_{dir}$-h per-trigger $I_{AA}$ and $I_{dA}$ of Au+Au, d+Au, and p+p, as a function of $\xi$.

$I_{AA}$ vs $\xi$ for direct photon $p_{T}^{\gamma}$ of 5-7 GeV/$c$, 7-9 GeV/$c$, and 9-12 GeV/$c$.

$I_{AA}$ vs $\xi$ for direct photon $p_{T}^{\gamma}$ of 5-7 GeV/$c$, 7-9 GeV/$c$, and 9-12 GeV/$c$.

$I_{AA}$ vs $\xi$ for direct photon $p_{T}^{\gamma}$ of 5-7 GeV/$c$, 7-9 GeV/$c$, and 9-12 GeV/$c$.

$I_{AA}$ as a function of $\xi$ for direct photon $p_{T}^{\gamma}$ of 5-7, 7-9, and 9-12 GeV/$c$. Three away-side integration ranges are chosen to calculate the per-trigger yield and the corresponding $I_{AA}$, $|\Delta\phi-\pi|<\pi/2$, $|\Delta\phi-\pi|<\pi/3$, and $|\Delta\phi-\pi|<\pi/6$.

$I_{AA}$ as a function of $\xi$ for direct photon $p_{T}^{\gamma}$ of 5-7, 7-9, and 9-12 GeV/$c$. Three away-side integration ranges are chosen to calculate the per-trigger yield and the corresponding $I_{AA}$, $|\Delta\phi-\pi|<\pi/2$, $|\Delta\phi-\pi|<\pi/3$, and $|\Delta\phi-\pi|<\pi/6$.

$I_{AA}$ as a function of $\xi$ for direct photon $p_{T}^{\gamma}$ of 5-7, 7-9, and 9-12 GeV/$c$. Three away-side integration ranges are chosen to calculate the per-trigger yield and the corresponding $I_{AA}$, $|\Delta\phi-\pi|<\pi/2$, $|\Delta\phi-\pi|<\pi/3$, and $|\Delta\phi-\pi|<\pi/6$.

Ratios of $I_{AA}$ as a function of direct photon $p_T$ for three different away-side integration ranges.

Measured $I_{AA}$ for direct photon $p_T$ of 5-7, 7-9, and 9-12 GeV/$c$, as a function of $\xi$, are compared with theoretical model calculations.

Measured $I_{AA}$ for direct photon $p_T$ of 5-7, 7-9, and 9-12 GeV/$c$, as a function of $\xi$, are compared with theoretical model calculations.

Measured $I_{AA}$ for direct photon $p_T$ of 5-7, 7-9, and 9-12 GeV/$c$, as a function of $\xi$, are compared with theoretical model calculations.

$\pi^0$ spectra from figure 2a from 40-60% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data.

$\pi^0$ spectra from figure 2a from 60-80% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data.

$\eta$ spectra from figure 2b from minimum bias U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data.

$\eta$ spectra from figure 2b from 0-20% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data.

$\eta$ spectra from figure 2b from 20-40% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data.

$\eta$ spectra from figure 2b from 40-60% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data.

$\eta$ spectra from figure 2b from 60-80% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data.

Ratio of $\pi^0$ yield to the fit from figure 2c from minimum bias U+U collisions. Sys. uncertainties include B and C uncertainties from data points.

Ratio of $\pi^0$ yield to the fit from figure 2c from 0-20% U+U collisions. Sys. uncertainties include B and C uncertainties from data points.

Ratio of $\pi^0$ yield to the fit from figure 2c from 60-80% U+U collisions. Sys. uncertainties include B and C uncertainties from data points.

Ratio of $\eta$ yield to the fit from figure 2d from minimum bias U+U collisions. Sys. uncertainties include B and C uncertainties from data points.

Ratio of $\eta$ yield to the fit from figure 2d from 0-20% U+U collisions. Sys. uncertainties include B and C uncertainties from data points.

Ratio of $\eta$ yield to the fit from figure 2d from 40-60% U+U collisions. Sys. uncertainties include B and C uncertainties from data points.

$\eta/\pi^0$ ratio from figure 3 from minimum bias U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point.

$\eta/\pi^0$ ratio from figure 3 from 0-20% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point.

$\eta/\pi^0$ ratio from figure 3 from 20-40% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point.

$\eta/\pi^0$ ratio from figure 3 from 40-60% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point.

$\eta/\pi^0$ ratio from figure 3 from 60-80% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point.

$\eta/\pi^0$ ratio from figure 3 from minimum bias Au+Au collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point.

$\pi^0$ $R_{AA}$ from figure 4a from 0-20% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data. Calculation is carried out for Glauber 1 set.

$\eta$ $R_{AA}$ from figure 4a from 0-20% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data. Calculation is carried out for Glauber 1 set.

$\pi^0$ $R_{AA}$ from figure 4b from 20-40% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data. Calculation is carried out for Glauber 1 set.

$\eta$ $R_{AA}$ from figure 4b from 20-40% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data. Calculation is carried out for Glauber 1 set.

$\pi^0$ $R_{AA}$ from figure 4c from 40-60% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data. Calculation is carried out for Glauber 1 set.

$\eta$ $R_{AA}$ from figure 4c from 40-60% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data. Calculation is carried out for Glauber 1 set.

$\pi^0$ $R_{AA}$ from figure 4d from minimum bias U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data. Calculation is carried out for Glauber 1 set.

$\eta$ $R_{AA}$ from figure 4d from minimum bias U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data. Calculation is carried out for Glauber 1 set.

$\pi^0$ $R_{AA}$ from figure 5a from 0-20% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data. Calculation is carried out for Glauber 2 set.

$\pi^0$ $R_{AA}$ from figure 5a from 0-5% Au+Au collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data.

$\pi^0$ $R_{AA}$ from figure 5a from 40-60% U+U collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data. Calculation is carried out for Glauber 2 set.

$\pi^0$ $R_{AA}$ from figure 5a from 40-50% Au+Au collisions. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data.

$\pi^0$ integrated $R_{AA}$ for $p_T>5$ GeV/$c$ in U+U collisions as a function of centrality from figure 6a. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data. Calculation is carried out for Glauber 1 set.

$\eta$ integrated $R_{AA}$ for $p_T>5$ GeV/$c$ in U+U collisions as a function of centrality from figure 6a. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data. Calculation is carried out for Glauber 1 set.

$\pi^0$ integrated $R_{AA}$ for $p_T>5$ GeV/$c$ in Au+Au collisions as a function of centrality from figure 6a. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data.

$\eta$ integrated $R_{AA}$ for $p_T>5$ GeV/$c$ in U+U collisions as a function of centrality from figure 6b. Type A uncertainties are uncorrelated point-to-point. Type B uncertainties are correlated point-to-point. Type C uncertainties affect the scale of the data. Calculation is carried out for Glauber 2 set.

Number of participant nucleons of in dep U$+$U collisions

Number of participant nucleons of in dep U$+$U collisions

Number of participant nucleons of in dep Au$+$Au collisions

Inverse slope of mT fit of XI- and XIBAR+ produced in inelastic p+p interactions at 158 GeV/c.

The XIBAR+/Xi-ratio in inelastic p+p interactions at 158 GeV/c beam momentum.

Ratio of pT integrated yields versus rapidity of XIBAR+ and Xi- produced in inelastic p+p interactions at 158 GeV/c beam momentum.

Transverse momentum spectra of PI− in rapidity slices produced in the 5% most central Be+Be collisions at 75A GeV/c.

Transverse momentum spectra of PI− in rapidity slices produced in the 5% most central Be+Be collisions at 150A GeV/c.

Transverse mass spectra 1/mT d2n/(dydmT) of negatively charged pions produced in central Be+Be collisions at the SPS energies.

Rapidity spectra of PI− produced in the 5% most central Be+Be collisions at the SPS energies.

Collision energy dependence of the ratio of the width sigma_y of the rapidity distribution to the beam rapidity y_beam for central Be+Be.

Energy dependence of the mean transverse mass of PI- measured at mid-rapidity in central Be+Be collisions.

The "kink" plot showing the ratio of pion multiplicity <PI> to number of wounded nucleons <W> versus the Fermi energy variable F=s^1/4_NN from central Be+Be collisions.

Transverse momentum spectra in rapidity slices of K+ produced in the 20% most central Be+Be collisions at beam momentum 40A GeV/c (collision energy 8.87 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of K+ produced in the 20% most central Be+Be collisions at beam momentum 40A GeV/c (collision energy 8.87 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using tof-dE/dx analysis method.

Transverse momentum spectra in rapidity slices of K+ produced in the 20% most central Be+Be collisions at beam momentum 75A GeV/c (collision energy 11.95 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of K+ produced in the 20% most central Be+Be collisions at beam momentum 75A GeV/c (collision energy 11.95 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using tof-dE/dx analysis method.

Transverse momentum spectra in rapidity slices of K+ produced in the 20% most central Be+Be collisions at beam momentum 150A GeV/c (collision energy 16.83 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of K+ produced in the 20% most central Be+Be collisions at beam momentum 150A GeV/c (collision energy 16.83 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using tof-dE/dx analysis method.

Transverse momentum spectra in rapidity slices of K- produced in the 20% most central Be+Be collisions at beam momentum 19A GeV/c (collision energy 6.27 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of K- produced in the 20% most central Be+Be collisions at beam momentum 30A GeV/c (collision energy 7.62 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval.

Transverse momentum spectra in rapidity slices of K- produced in the 20% most central Be+Be collisions at beam momentum 30A GeV/c (collision energy 7.62 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using tof-dE/dx analysis method.

Transverse momentum spectra in rapidity slices of K- produced in the 20% most central Be+Be collisions at beam momentum 40A GeV/c (collision energy 8.87 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of K- produced in the 20% most central Be+Be collisions at beam momentum 40A GeV/c (collision energy 8.87 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using tof-dE/dx analysis method.

Transverse momentum spectra in rapidity slices of K- produced in the 20% most central Be+Be collisions at beam momentum 75A GeV/c (collision energy 11.95 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of K- produced in the 20% most central Be+Be collisions at beam momentum 75A GeV/c (collision energy 11.95 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using tof-dE/dx analysis method.

Transverse momentum spectra in rapidity slices of K- produced in the 20% most central Be+Be collisions at beam momentum 150A GeV/c (collision energy 16.83 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of K- produced in the 20% most central Be+Be collisions at beam momentum 150A GeV/c (collision energy 16.83 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using tof-dE/dx analysis method.

Transverse momentum spectra in rapidity slices of PI+ produced in the 20% most central Be+Be collisions at beam momentum 19A GeV/c (collision energy 6.27 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of PI+ produced in the 20% most central Be+Be collisions at beam momentum 30A GeV/c (collision energy 7.62 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of PI+ produced in the 20% most central Be+Be collisions at beam momentum 40A GeV/c (collision energy 8.87 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of PI+ produced in the 20% most central Be+Be collisions at beam momentum 75A GeV/c (collision energy 11.95 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of PI+ produced in the 20% most central Be+Be collisions at beam momentum 150A GeV/c (collision energy 16.83 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of PI- produced in the 20% most central Be+Be collisions at beam momentum 19A GeV/c (collision energy 6.27 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of PI- produced in the 20% most central Be+Be collisions at beam momentum 30A GeV/c (collision energy 7.62 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of PI- produced in the 20% most central Be+Be collisions at beam momentum 40A GeV/c (collision energy 8.87 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of PI- produced in the 20% most central Be+Be collisions at beam momentum 75A GeV/c (collision energy 11.95 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of PI- produced in the 20% most central Be+Be collisions at beam momentum 150A GeV/c (collision energy 16.83 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of protons produced in the 20% most central Be+Be collisions at beam momentum 19A GeV/c (collision energy 6.27 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of protons produced in the 20% most central Be+Be collisions at beam momentum 30A GeV/c (collision energy 7.62 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of protons produced in the 20% most central Be+Be collisions at beam momentum 40A GeV/c (collision energy 8.87 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of protons produced in the 20% most central Be+Be collisions at beam momentum 75A GeV/c (collision energy 11.95 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of protons produced in the 20% most central Be+Be collisions at beam momentum 150A GeV/c (collision energy 16.83 GeV). Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of antiprotons produced in the 20% most central Be+Be collisions. Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of antiprotons produced in the 20% most central Be+Be collisions. Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

Transverse momentum spectra in rapidity slices of antiprotons produced in the 20% most central Be+Be collisions. Rapidity values given in the legends correspond to the middle of the corresponding interval. Results presented in this table were obtained using dE/dx analysis method.

The beam momentum dependence of the inverse slope parameter of transverse momentum spectra at mid-rapidity (0<y< 0.2 for 40A GeV/c, 75A GeV/c and 150A GeV/c; -0.2<y<0.0 for 30A GeV/c) of positively charged K mesons for central 20% Be+Be collisions. Incoming beam momentum translates to collision energy (SQRT(SNN)) as following 30A GeV/c (7.62 GeV), 40AGeV/c (8.87 GeV), 75A GeV/c (11.95 GeV), 150A GeV/c (16.83 GeV).

The energy dependence of the inverse slope parameter of transverse momentum spectra at mid-rapidity (0<y< 0.2 for 40A GeV/c, 75A GeV/c and 150A GeV/c; -0.2<y<0.0 for 30A GeV/c) of negatively charged K mesons for 20% central Be+Be collisions. Incoming beam momentum translates to collision energy (SQRT(SNN)) as following 30A GeV/c (7.62 GeV), 40AGeV/c (8.87 GeV), 75A GeV/c (11.95 GeV), 150A GeV/c (16.83 GeV).

Rapidity spectra of K+ produced in the 20% most central Be+Be at beam momentum of 19A GeV/c, 30A GeV/c, 40A GeV/c 75A GeV/c and 150A GeV/c. Incoming beam momentum translates to collision energy (SQRT(SNN)) as following 19A GeV/c -> 6.27 GeV, 30A GeV/c -> 7.62 GeV, 40A GeV/c -> 8.87 GeV, 75A GeV/c -> 11.95 GeV, 150A GeV/c -> 16.83 GeV.

Rapidity spectra of K- produced in the 20% most central Be+Be at beam momentum of 19A GeV/c, 30A GeV/c, 40A GeV/c 75A GeV/c and 150A GeV/c. Incoming beam momentum translates to collision energy (SQRT(SNN)) as following 19A GeV/c -> 6.27 GeV, 30A GeV/c -> 7.62 GeV, 40A GeV/c -> 8.87 GeV, 75A GeV/c -> 11.95 GeV, 150A GeV/c -> 16.83 GeV.

Rapidity spectra of PI+ produced in the 20% most central Be+Be at beam momentum of 19A GeV/c, 30A GeV/c, 40A GeV/c 75A GeV/c and 150A GeV/c. Incoming beam momentum translates to collision energy (SQRT(SNN)) as following 19A GeV/c -> 6.27 GeV, 30A GeV/c -> 7.62 GeV, 40A GeV/c -> 8.87 GeV, 75A GeV/c -> 11.95 GeV, 150A GeV/c -> 16.83 GeV.

Rapidity spectra of PI- produced in the 20% most central Be+Be at beam momentum of 19A GeV/c, 30A GeV/c, 40A GeV/c 75A GeV/c and 150A GeV/c. Incoming beam momentum translates to collision energy (SQRT(SNN)) as following 19A GeV/c -> 6.27 GeV, 30A GeV/c -> 7.62 GeV, 40A GeV/c -> 8.87 GeV, 75A GeV/c -> 11.95 GeV, 150A GeV/c -> 16.83 GeV.

Rapidity spectra of protons produced in the 20% most central Be+Be at beam momentum of 19A GeV/c, 30A GeV/c, 40A GeV/c 75A GeV/c and 150A GeV/c. Incoming beam momentum translates to collision energy (SQRT(SNN)) as following 19A GeV/c -> 6.27 GeV, 30A GeV/c -> 7.62 GeV, 40A GeV/c -> 8.87 GeV, 75A GeV/c -> 11.95 GeV, 150A GeV/c -> 16.83 GeV.

Rapidity spectra of antiprotons produced in the 20% most central Be+Beat beam momentum of 40A GeV/c 75A GeV/c and 150A GeV/c. Incoming beam momentum translates to collision energy (SQRT(SNN)) as following 40A GeV/c -> 8.87 GeV, 75A GeV/c -> 11.95 GeV, 150A GeV/c -> 16.83 GeV.

Collision energy dependence of mean multiplicities of K+ produced in the 20% most central Be+Be collisions.

Collision energy dependence of mean multiplicities of K- produced in the 20% most central Be+Be collisions.

Collision energy dependence of mean multiplicities of PI+ produced in the 20% most central Be+Be collisions.

Collision energy dependence of mean multiplicities of PI- produced in the 20% most central Be+Be collisions.

Collision energy dependence of mean multiplicities of antiprotons produced in the 20% most central Be+Be collisions.

The energy dependence of the K+/PI+ particle yields ratio at mid-rapidity for the 20% most central Be+Be collisions.

The energy dependence of the K+/PI+ particle yields ratio at full acceptance for the 20% most central Be+Be collisions.