Direct $\gamma$ invariant yields as a function of transverse momentum for 9 centrality selections and minimum bias Au+AU collisions at $\sqrt{s_{NN}}$ = 200 GeV. Data with no errors represents 90% confidence level upper limit. The bin range is not an uncertainty in the x-axis because the actual uncertainty by having the finite bin width is corrected for by the bin-shift correction. These bins were constructed using the corrected finite values as centers.

Ratio of Au+Au yield to $p$+$p$ yield normalized by the number of binary nucleon collisions as a function of centrality given by $N_{part}$ for direct $\gamma$ and $\pi^0$ yields integrated above 6 GeV/$c$. Data with no errors represents 90% confidence level upper limit.

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.

Correlation function, C(q) for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.

Correlation function, C(q) for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.

Correlation function, C(q) for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.

Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.

Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.

Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.

Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.

Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.

Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.

Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.

Correlation functions, C(q), for $\pi^+\pi^+$ and $\pi^-\pi^-$ pairs.

$k_T$ dependence of extracted spheroidal source parameters for pion source functions (a) $R_T$ , (b) $a$, and (c) $\lambda$ for most central collisions & perhipheral collisions.

$k_T$ dependence of extracted spheroidal source parameters for pion source functions (a) $R_T$ , (b) $a$, and (c) $\lambda$ for most central collisions & perhipheral collisions.

$k_T$ dependence of extracted spheroidal source parameters for pion source functions (a) $R_T$ , (b) $a$, and (c) $\lambda$ for most central collisions & perhipheral collisions.

$v_2$ 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$.

$\Delta\phi$ distributions for meson triggers with 2.5 < $p_T$ < 4.0 GeV/$c$ and associated charged hadrons with 1.7 < $p_T$ < 2.5 GeV/$c$ for 60-70% centrality in Au+Au collisions.

$\Delta\phi$ distributions for baryon triggers with 2.5 < $p_T$ < 4.0 GeV/$c$ and associated charged hadrons with 1.7 < $p_T$ < 2.5 GeV/$c$ for 60-70% centrality in Au+Au collisions.

Combinatorial Background Levels from Figure 1 Top Panels.

Combinatorial Background Levels from Figure 1 Bottom Panels.

Trigger Particle $v_2$ values.

Partner Particle $v_2$ values.

Yield per trigger for associated charged hadrons between 1.7 < $p_T$ < 2.5 GeV/$c$ for the near- (top) and away- (bottom) side jets.

Yield per trigger for associated charged hadrons between 1.7 < $p_T$ < 2.5 GeV/$c$ for the near- (top) and away- (bottom) side jets.

Uncertainties in Figure 2 as a function of $N_{part}$ and trigger type for AuAu and $d$+Au.

Uncertainties in Figure 2 as a function of $N_{part}$ and trigger type for AuAu and $d$+Au.

$p_T$ spectra of the near side associated charged hadrons corrected to the full jet yield for meson triggers at 2.5 < $p_T$ < 4.0 GeV/$c$ and $|\eta|$ < 0.35 for six centralities in Au+Au and $d$+Au collisions.

$p_T$ spectra of the near side associated charged hadrons corrected to the full jet yield for meson triggers at 2.5 < $p_T$ < 4.0 GeV/$c$ and $|\eta|$ < 0.35 for six centralities in Au+Au and $d$+Au collisions.

$p_T$ spectra of the near side associated charged hadrons corrected to the full jet yield for baryon triggers at 2.5 < $p_T$ < 4.0 GeV/$c$ and $|\eta|$ < 0.35 for six centralities in Au+Au, $d$+Au and $p$+$p$ collisions.

Inverse slopes from the fits in Figure 3.

Inverse slopes from the fits in Figure 3.

Inverse slopes from the fits in Figure 3.

Fit results based on $k(\delta_{\eta})$=$1/{{2\alpha\xi}/{\delta_{\eta}}}$ ($\xi << \delta_{\eta}$).

The ratio of the hadronic decay photon $v_2$ over inclusive photon $v_2$ ($v_2^{b.g}/v_2^{inclusive \gamma}$) compared with the direct photon excess ratio $R = (N_{direct \gamma} + N_{b.g})/N_{b.g}$.

The ratio of the hadronic decay photon $v_2$ over inclusive photon $v_2$ ($v_2^{b.g}/v_2^{inclusive \gamma}$) compared with the direct photon excess ratio $R = (N_{direct \gamma} + N_{b.g})/N_{b.g}$.

$F_{p_T}$ (in percent) of non-random fluctuations as a function of the $p_T$ range over which $M_{p_T}$ is calculated, 0.2 GeV/$c$ < $p_T$ < $p^{max}_T$, for the 20-25% centrality class ($N_{part}$ = 181.6).

$v(Q)$, for central events, as a function of the azimuthal coverage of the detector for data. (Angles in degrees.)

The effect on $v(Q)$ of varying the acceptance in $\varphi_r$. The solid curve shows the expectation from global charge conservation. The 10% most central events are used for data and RQMD. (Angles in degrees.)

$dN/dy$ and $T$ for different centrality bins.

Blast wave model parameters as a function of centrality from fitting $\pi^±$, $K^±$, $p$, and $\bar{p}$ spectra.

$m_T$ spectra of $\phi$ mesons in different centrality bins.

Centrality dependence of the $\phi$ mass centroid and $\phi$ intrinsic width.

Minimum-bias $m_T$ spectra of $\phi$ for different subsystem combinations.

Minimum-bias $m_T$ spectra of $\phi$ for different subsystem combinations.

Minimum-bias $m_T$ spectra of $\phi$ for different subsystem combinations.

Minimum-bias $m_T$ spectra of $\phi$ for different subsystem combinations.

$\phi$ $m_T$ spectra in different centrality bins.

Centrality dependence of $\phi$ yield at midrapidity.

Centrality dependence of $\phi$ yield at midrapidity.

Centrality dependence of the inverse slope, $T$.

Centrality dependence of particle ratios for $K^+$/$\pi^+$ and $K^-$/$\pi^-$.

Centrality dependence of particle ratios for $\phi$/$\pi$ and $\phi$/$K$.

Centrality dependence of $\phi$ yields at different collision energies.

Centrality dependence of $\phi$ yields at different collision energies.

$\phi$/$\pi$ and $\phi$/$K^-$ ratios as a function of collision energies.

Inverse slope parameteres $T$ in $m_T$ spectra.

$N_{coll}$ scaled central to peripheral ratio $R_{CP}$ for $\phi$. The total systematic error is 19%, but 7% is uncorrelated between the $\phi$ and $p$ $R_{CP}$.