Nucelar modification factor $R_{CP}$ for ($p+\bar{p}$)/2.

Nucelar modification factor $R_{CP}$ for $\pi^0$.

Charged hadron to $\pi^0$ ratio in central (0-10%) Au+Au collisions.

Charged hadron to $\pi^0$ ratio in peripheral (60-92%) Au+Au collisions. The peripheral data points are offset by +130 MeV/$c$ for clarity.

Systematic error on normalization a) common to both centralities b) that can move the $h$/$\pi^0$ ratios for each centrality independent of the other.

Transverse momentum dependepnce of $v_2$ for identified particle $\pi^-$.

Transverse momentum dependepnce of $v_2$ for identified particle $K^-$.

Transverse momentum dependepnce of $v_2$ for identified particle $\bar{p}$.

Transverse momentum dependepnce of $v_2$ for identified particle $\pi^+$.

Transverse momentum dependepnce of $v_2$ for identified particle $K$.

Transverse momentum dependepnce of $v_2$ for identified particle $p$.

Transverse momentum dependepnce of $v_2$ for combined particles $\pi^+$ and $\pi^-$.

Transverse momentum dependepnce of $v_2$ for combined particles $K^+$ and $K^-$.

Transverse momentum dependepnce of $v_2$ for combined particles $p$ and $\bar{p}$.

Transverse momentum dependepnce of $v_2$ for combined particles $\pi^+$ and $\pi^-$ scaled by quarks for each particle as motivated by a quark coalescence model.

Transverse momentum dependepnce of $v_2$ for combined particles $K^+$ and $K^-$ scaled by quarks for each particle as motivated by a quark coalescence model.

Transverse momentum dependepnce of $v_2$ for combined particles $p$ and $\bar{p}$ scaled by quarks for each particle as motivated by a quark coalescence model.

Transverse momentum dependence of $v_2$ for negative charged particle distributions at 0-20% centrality.

Transverse momentum dependence of $v_2$ for combined $\pi^-$ and $K^-$ at 0-20% centrality.

Transverse momentum dependence of $v_2$ for $\bar{p}$ at 0-20% centrality.

Transverse momentum dependence of $v_2$ for positive charged particle distributions at 0-20% centrality.

Transverse momentum dependence of $v_2$ for combined $\pi^+$ and $K^+$ at 0-20% centrality.

Transverse momentum dependence of $v_2$ for $p$ at 0-20% centrality.

Transverse momentum dependence of $v_2$ for negative charged particle distributions at 20-40% centrality.

Transverse momentum dependence of $v_2$ for combined $\pi^-$ and $K^-$ at 20-40% centrality.

Transverse momentum dependence of $v_2$ for $\bar{p}$ at 20-40% centrality.

Transverse momentum dependence of $v_2$ for positive charged particle distributions at 20-40% centrality.

Transverse momentum dependence of $v_2$ for combined $\pi^+$ and $K^+$ at 20-40% centrality.

Transverse momentum dependence of $v_2$ for $p$ at 20-40% centrality.

Transverse momentum dependence of $v_2$ for negative charged particle distributions at 40-60% centrality.

Transverse momentum dependence of $v_2$ for combined $\pi^-$ and $K^-$ at 40-60% centrality.

Transverse momentum dependence of $v_2$ for $\bar{p}$ at 40-60% centrality.

Transverse momentum dependence of $v_2$ for positive charged particle distributions at 40-60% centrality.

Transverse momentum dependence of $v_2$ for combined $\pi^+$ and $K^+$ at 40-60% centrality.

Transverse momentum dependence of $v_2$ for $p$ at 40-60% centrality.

Invariant $\pi^0$ yields at midrapidity as a function of $p_T$ for minimum bias and nine centralities in $Au\ +\ Au$ at $\sqrt{s_{NN}} = 200\ GeV$ [0%–10% (80%–92%) is most central (peripheral)]. The labels "uncorr." and "corr." include systematic errors that are uncorrelated and correlated point-to-point, respectively.

Invariant $\pi^0$ yields at midrapidity as a function of $p_T$ for minimum bias and nine centralities in $Au\ +\ Au$ at $\sqrt{s_{NN}} = 200\ GeV$ [0%–10% (80%–92%) is most central (peripheral)]. The labels "uncorr." and "corr." include systematic errors that are uncorrelated and correlated point-to-point, respectively.

Invariant $\pi^0$ yields at midrapidity as a function of $p_T$ for minimum bias and nine centralities in $Au\ +\ Au$ at $\sqrt{s_{NN}} = 200\ GeV$ [0%–10% (80%–92%) is most central (peripheral)]. The labels "uncorr." and "corr." include systematic errors that are uncorrelated and correlated point-to-point, respectively.

Invariant $\pi^0$ yields at midrapidity as a function of $p_T$ for minimum bias and nine centralities in $Au\ +\ Au$ at $\sqrt{s_{NN}} = 200\ GeV$ [0%–10% (80%–92%) is most central (peripheral)]. The labels "uncorr." and "corr." include systematic errors that are uncorrelated and correlated point-to-point, respectively.

Invariant $\pi^0$ yields at midrapidity as a function of $p_T$ for minimum bias and nine centralities in $Au\ +\ Au$ at $\sqrt{s_{NN}} = 200\ GeV$ [0%–10% (80%–92%) is most central (peripheral)]. The labels "uncorr." and "corr." include systematic errors that are uncorrelated and correlated point-to-point, respectively.

Invariant $\pi^0$ yields at midrapidity as a function of $p_T$ for minimum bias and nine centralities in $Au\ +\ Au$ at $\sqrt{s_{NN}} = 200\ GeV$ [0%–10% (80%–92%) is most central (peripheral)]. The labels "uncorr." and "corr." include systematic errors that are uncorrelated and correlated point-to-point, respectively.

Invariant $\pi^0$ yields at midrapidity as a function of $p_T$ for minimum bias and nine centralities in $Au\ +\ Au$ at $\sqrt{s_{NN}} = 200\ GeV$ [0%–10% (80%–92%) is most central (peripheral)]. The labels "uncorr." and "corr." include systematic errors that are uncorrelated and correlated point-to-point, respectively.

Invariant $\pi^0$ yields at midrapidity as a function of $p_T$ for minimum bias and nine centralities in $Au\ +\ Au$ at $\sqrt{s_{NN}} = 200\ GeV$ [0%–10% (80%–92%) is most central (peripheral)]. The labels "uncorr." and "corr." include systematic errors that are uncorrelated and correlated point-to-point, respectively.

Invariant $\pi^0$ yields at midrapidity as a function of $p_T$ for minimum bias and nine centralities in $Au\ +\ Au$ at $\sqrt{s_{NN}} = 200\ GeV$ [0%–10% (80%–92%) is most central (peripheral)]. The labels "uncorr." and "corr." include systematic errors that are uncorrelated and correlated point-to-point, respectively.

Invariant $\pi^0$ yields at midrapidity as a function of $p_T$ for minimum bias and nine centralities in $Au\ +\ Au$ at $\sqrt{s_{NN}} = 200\ GeV$ [0%–10% (80%–92%) is most central (peripheral)]. The labels "uncorr." and "corr." include systematic errors that are uncorrelated and correlated point-to-point, respectively.

Nuclear modification factor $R_{AA}(p_T)$ for $\pi^0$ in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The error bars include all point-to-point experimental ($p+p$, Au+Au) errors. The label "sys(uncorr)" refers to the uncorrelated point-to-point uncertainty (which includes statistical errors), while "sys(norm)" is the normalization uncertainty.

Nuclear modification factor $R_{AA}(p_T)$ for $\pi^0$ in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The error bars include all point-to-point experimental ($p+p$, Au+Au) errors. The label "sys(uncorr)" refers to the uncorrelated point-to-point uncertainty (which includes statistical errors), while "sys(norm)" is the normalization uncertainty.

Nuclear modification factor $R_{AA}(p_T)$ for $\pi^0$ in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The error bars include all point-to-point experimental ($p+p$, Au+Au) errors. The label "sys(uncorr)" refers to the uncorrelated point-to-point uncertainty (which includes statistical errors), while "sys(norm)" is the normalization uncertainty.

Nuclear modification factor $R_{AA}(p_T)$ for $\pi^0$ in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The error bars include all point-to-point experimental ($p+p$, Au+Au) errors. The label "sys(uncorr)" refers to the uncorrelated point-to-point uncertainty (which includes statistical errors), while "sys(norm)" is the normalization uncertainty.

Nuclear modification factor $R_{AA}(p_T)$ for $\pi^0$ in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The error bars include all point-to-point experimental ($p+p$, Au+Au) errors. The label "sys(uncorr)" refers to the uncorrelated point-to-point uncertainty (which includes statistical errors), while "sys(norm)" is the normalization uncertainty.

Nuclear modification factor $R_{AA}(p_T)$ for $\pi^0$ in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The error bars include all point-to-point experimental ($p+p$, Au+Au) errors. The label "sys(uncorr)" refers to the uncorrelated point-to-point uncertainty (which includes statistical errors), while "sys(norm)" is the normalization uncertainty.

Nuclear modification factor $R_{AA}(p_T)$ for $\pi^0$ in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The error bars include all point-to-point experimental ($p+p$, Au+Au) errors. The label "sys(uncorr)" refers to the uncorrelated point-to-point uncertainty (which includes statistical errors), while "sys(norm)" is the normalization uncertainty.

Nuclear modification factor $R_{AA}(p_T)$ for $\pi^0$ in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The error bars include all point-to-point experimental ($p+p$, Au+Au) errors. The label "sys(uncorr)" refers to the uncorrelated point-to-point uncertainty (which includes statistical errors), while "sys(norm)" is the normalization uncertainty.

Nuclear modification factor $R_{AA}(p_T)$ for $\pi^0$ in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The error bars include all point-to-point experimental ($p+p$, Au+Au) errors. The label "sys(uncorr)" refers to the uncorrelated point-to-point uncertainty (which includes statistical errors), while "sys(norm)" is the normalization uncertainty.

Nuclear modification factor $R_{AA}(p_T)$ for $\pi^0$ in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The error bars include all point-to-point experimental ($p+p$, Au+Au) errors. The label "sys(uncorr)" refers to the uncorrelated point-to-point uncertainty (which includes statistical errors), while "sys(norm)" is the normalization uncertainty.

Nuclear modification factor $R_{AA}(p_T)$ for $\pi^0$ in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The error bars include all point-to-point experimental ($p+p$, Au+Au) errors. The label "sys(uncorr)" refers to the uncorrelated point-to-point uncertainty (which includes statistical errors), while "sys(norm)" is the normalization uncertainty.

Nuclear modification factor $R_{AA}(p_T)$ for $\pi^0$ in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The error bars include all point-to-point experimental ($p+p$, Au+Au) errors. The label "sys(uncorr)" refers to the uncorrelated point-to-point uncertainty (which includes statistical errors), while "sys(norm)" is the normalization uncertainty.

Nuclear modification factor $R_{AA}(p_T)$ for $\pi^0$ in Au+Au collisions at $\sqrt{s_{NN}} = 200$ GeV. The error bars include all point-to-point experimental ($p+p$, Au+Au) errors. The label "sys(uncorr)" refers to the uncorrelated point-to-point uncertainty (which includes statistical errors), while "sys(norm)" is the normalization uncertainty.

Inclusive differential cross sections for K0S production as a function of PT**2 extrapolated to the full XL range.

Inclusive differential cross sections for LAMBDA production as a function of PT**2 extrapolated to the full XL range.

Inclusive differential cross sections for LAMBDABAR production as a function of PT**2 extrapolated to the full XL range.

Total cross sections per nucleon and the values of the power resulting fromfitting the cross sections to SIG ~ A**POWER.

Ratio of direct CHIC to direct J/PSI production cross section in P C and P Ti interactions.

Centrality dependence of $⟨p^{trunc}_T⟩$, the average $p_T$ of charged particles with $p_T$ above a threshold $p^{min}_T$ minus the threshold $p^{min}_T$. Shown are values for two $p^{min}_T$ cuts, one at $p_T >$ 0.5 GeV/$c$ representing all data presented in Fig. 2 and the other one at $p_T >$ 2 GeV/$c$.

Nuclear modification factor ($R_{AA}$) for the 60-80%, 30-60%, 15-30%, and 5-15% centrality selections compared to the one for the most central sample (0-5%). Due to insufficient statistics $R_{AA}$ is not shown for the 80-92% sample.

The top panel gives the nuclear modification factor $R_{AA}$ for three exclusive $p_T$ regions as a function of the centrality of the collision. The lower panel shows essentially the same quantity but normalized to the number of participant pairs rather than to the number of binary collisions. The dotted line indicates the expectation for scaling with the number of binary collisions (top) or with the number of participants (bottom). Only statistical errors are shown. The systematic error on the scale and the centrality dependence are identical to the errors shown in Fig. 5. These errors are correlated, i.e. take their maximum or minimum value simultaneously for all centrality and $p_T$ selections. In addition, there are also $p_T$ dependent systematic errors, which are given in Table 1. The systematic errors do not alter the trends in the data.

Spectra of inclusive $\Lambda$ ($\bar{\Lambda}$) for minimum-bias events.

Spectra of inclusive feed-down corrected protons (antiprotons) for minimum-bias events.

Inclusive $\Lambda$ and feed-down corrected proton yields for minimum bias and for the 5% most central events. Systematic errors are 17% for protons and 16% for $\Lambda$

Inclusive $\Lambda$ and feed-down corrected average transverse momentum for minimum bias and for the 5% most central events. Systematic errors are 17% for protons and 16% for $\Lambda$

Inclusive $\Lambda$ and feed-down corrected slope parameters for minimum bias and for the 5% most central events. Systematic errors are 17% for protons and 16% for $\Lambda$

Total measured and predicted baryon yields for minimum-bias and for the 5% most central events. The proton yields are corrected for feed-down. The systematic errors are 24% for the protons and 23% for the $\Lambda$

$v_2$ vs Fixed $p_T$ for several centrality selections. [F] and [A] follow the notation Fig. 2. Systematic errors are estimated to be $\sim 5$%.

$v_2$ vs Assorted $p_T$ for several centrality selections. [F] and [A] follow the notation Fig. 2. Systematic errors are estimated to be $\sim 5$%.

$v_2$ vs Assorted $p_T$ for several centrality selections. [F] and [A] follow the notation Fig. 2. Systematic errors are estimated to be $\sim 5$%.

The centrality dependence of $A_2$ for two different $p_T$ selections. [F] and [A] follow the notation in Fig. 2. Systematic errors are estimated to be $\sim 10$%, dominated by the normalization of the correction function and the model determination of$ \varepsilon$.

The centrality dependence of $A_2$ for two different $p_T$ selections. [F] and [A] follow the notation in Fig. 2. Systematic errors are estimated to be $\sim 10$%, dominated by the normalization of the correction function and the model determination of$ \varepsilon$.