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.

Ratio of the electron data to the calculated background as a function of $p_T$ in minimum bias collisions (upper panel) and relative contributions to the background from various sources (lower panel). The curves for $\omega$ and $\phi$ show the sum of the Dalitz and the di-electron decay modes.

The background-subtracted electron spectra for central (0-10%) collisions compared with the expected contributions from open charm decays. Also shown, for central collisions only, are the expected contribution from bottom decays (dashed) and the conversion electron spectrum from a direct phonon prediction (dotted).

The background-subtracted electron spectra for minimum bias (0-92%) collisions compared with the expected contributions from open charm decays. Also shown, for central collisions only, are the expected contribution from bottom decays (dashed) and the conversion electron spectrum from a direct phonon prediction (dotted).

Single electron cross sections $\frac{d\sigma_e}{dy}|_{y=0}$ of this measurement and ISR experiments [9,11,31] are displayed (bottom of figure, right-hand scale) with charm decay contributions calculated with PYTHIA. Open and filled symbols for 1.0 < $p_T$ < 1.4 GeV/$c$ and $p_T$ > 1.4 GeV/$c$, respectively. The derived charm cross section of this measurement is compared with charm cross sections from SPS/FNAL experiments (top of figure, left-hand scale). The thick curve and the shaded band represent the charm cross section in the PYTHIA model and in a NLO pQCD calculation [30], respectively.

Single electron cross sections $\frac{d\sigma_e}{dy}|_{y=0}$ of this measurement and ISR experiments [9,11,31] are displayed (bottom of figure, right-hand scale) with charm decay contributions calculated with PYTHIA. Open and filled symbols for 1.0 < $p_T$ < 1.4 GeV/$c$ and $p_T$ > 1.4 GeV/$c$, respectively. The derived charm cross section of this measurement is compared with charm cross sections from SPS/FNAL experiments (top of figure, left-hand scale). The thick curve and the shaded band represent the charm cross section in the PYTHIA model and in a NLO pQCD calculation [30], respectively.

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

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

$\bar{d}/d$ ratio vs. $p_T$ for minimum bias data.

Differential anisotropy $v_2$($p_T$) for charged hadrons in Au + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV obtained via reaction plane methods

Differential anisotropy as a function of centrality for $\sqrt{s_{NN}}$ = 62.4 GeV/$c$

Differential anisotropy as a function of centrality for $\sqrt{s_{NN}}$ = 130 GeV/$c$

Differential anisotropy as a function of centrality for $\sqrt{s_{NN}}$ = 200 GeV/$c$

Differential anisotropy $v_2$($p_T$) for centrality selection 13 - 26%.

Differential anisotropy $v_2$($p_T$) for centrality selection 13 - 26%.

Differential $v_2$ vs. $\sqrt{S_{NN}}$ for charged hadrons in nucleus-nucleus collisions. Results are shown for the centrality cut of 13 - 26% and $p_T$ selections of 1.75 GeV/$c$ and 0.65 GeV/$c$.

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.

$I_{dAu}$ vs. $p_T^{assoc}$ for different centrality, $p_T^{trig}$ and $\eta^{trig}$ bins.

The ratio of correlation peak widths between $d + Au$ and $p + p$ collisions. Only statistic errors are shown.

The ratio of correlation peak widths between $d + Au$ and $p + p$ collisions. Only statistic errors are shown.

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.

The top panel shows the measured $R_{side}$ from identical pions for PHENIX. The bottom panel shows the ratio $R_{out}/R_{side}$ as a function of $k_T$. Longitudinal Co-Moving System (LCMS) frame for $\pi^-$

The top panel shows the measured $R_{side}$ from identical pions for PHENIX. The bottom panel shows the ratio $R_{out}/R_{side}$ as a function of $k_T$. Pair Center-of-Mass System (PCMS) frame for $\pi^+$

The top panel shows the measured $R_{side}$ from identical pions for PHENIX. The bottom panel shows the ratio $R_{out}/R_{side}$ as a function of $k_T$. Pair Center-of-Mass System (PCMS) frame for $\pi^-$

Centrality dependence of the $p_{T}$ distribution for $K^{-}$ in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Errors are statistical only.

Centrality dependence of the $p_{T}$ distribution for protons in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Errors are statistical only.

Centrality dependence of the $p_{T}$ distribution for antiprotons in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Errors are statistical only.

Centrality dependence of the $p_{T}$ distribution for antiprotons in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Errors are statistical only.

Inverse slope parameters for $\pi^{+}$, $\pi^{-}$, $K^{+}$, $K^{-}$, proton, and antiproton for the 0-5%, 40-50%, and 60-92% centrality bins. Errors are statistical only.

Mean transverse momentum as a function of centrality for pions, kaons, protons,and antiprotons in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Errors are systematic only.

dN/dy as a function of centrality for pions, kaons, protons,and antiprotons in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. Errors are systematic only.

Particle ratios of $\pi^{-}$/$\pi^{+}$ for centrality 0-5% and 60-92%. Errors are statistical and systematic.

Particle ratios of $K^{-}$/$K^{+}$ for centrality 0-5% and 60-92%. Errors are statistical and systematic.

Particle ratios of antiprotons/protons for centrality 0-5%, 60-92%, and minimum bias. Errors are statistical and systematic.

Particle ratios of kaons/pions for centrality 0-5% and 60-92%. Errors are statistical and systematic.

Particle ratios of proton/$\pi^{+}$ and antiproton/$\pi^{-}$ for centrality 0-10%, 20-30%, and 60-92%. Errors are statistical and systematic.

Particle ratios of proton/$\pi^{0}$ and antiproton/$\pi^{0}$ for centrality 0-10%, 20-30%, and 60-92%. Errors are statistical and systematic.

Centrality dependence of particle ratios for $\pi^{-}$/$\pi^{+}$, $K^{-}$/$K^{+}$, and antiprotons/protons. Errors are statistical and systematic.

Rcp as a function of centrality 0-10% and 60-92% for ($\pi^{+}$ + $\pi^{-}$)/2. Errors are statistical only.

Rcp as a function of centrality 0-10% and 60-92% for ($K^{+}$ + $K^{-}$)/2. Errors are statistical only.

Rcp as a function of centrality 0-10% and 60-92% for charged (p+pbar)/2. Errors are statistical only.

Rcp as a function of centrality 0-10% and 60-92% for neutral pions. Errors are statistical only.

Integrated Rcp above $p_{T}$ = 1.5 GeV/c as a function of centrality 60-92% for pions, kaons, and (p+pbar)/2. Errors are statistical only.