$p_T$ spectra of charged hadrons for minimum bias collisions along with spectra for 9 centrality classes derived from the pseudo-rapidity region $|\eta|$ < 0.18. Stat. stands for statistical error, syst. stands for the systematic errors and occ. stands for occupancy error.

$p_T$ spectra of charged hadrons for minimum bias collisions along with spectra for 9 centrality classes derived from the pseudo-rapidity region $|\eta|$ < 0.18. Stat. stands for statistical error, syst. stands for the systematic errors and occ. stands for occupancy error.

Centrality dependence of $<p^{trunc}_T>$. Data points for truncated mean $p_T$ calculation for three $p_T$ ranges. The integral region is from 8 GeV/$c$ > $p_T$ > $p_{T_{min}}$ for the most peripheral bin. Since the data stop around 6.5 GeV/$c$, truncated mean $p_T$ is lower.

Ratio of charged hadron yields per nucleon-nucleon collision between central (0-10%) and peripheral (60-92%) Au + Au collisions. Stat. stands for statistical error, syst. stands for the systematic errors and occ. stands for occupancy error.

$R_{AA}$ for $(h^++h^-)/2$ and $\pi^0$ as function of $p_{T}$ for minimum bias and 9 centrality classes. Stat. stands for statistical error from Au+Au. The asymmetric uncertainty from the fit of the $\pi^0$ mass peak is denoted by fit. $\sigma_{ENBC}$ stands for error on number of binary collisions. Error from $pp$ parametrization that is not $p_T$ dependent. This error is not included in the calculation of the Upper bound of the systematic error and the Lower bound of the systematic error.

$R_{AA}$ for $(h^++h^-)/2$ and $\pi^0$ as function of $p_{T}$ for minimum bias and 9 centrality classes. Stat. stands for statistical error from Au+Au. The asymmetric uncertainty from the fit of the $\pi^0$ mass peak is denoted by fit. $\sigma_{ENBC}$ stands for error on number of binary collisions. Error from $pp$ parametrization that is not $p_T$ dependent. This error is not included in the calculation of the Upper bound of the systematic error and the Lower bound of the systematic error.

$R_{AA}$ for $(h^++h^-)/2$ and $\pi^0$ as function of $p_{T}$ for minimum bias and 9 centrality classes. Stat. stands for statistical error from Au+Au. The asymmetric uncertainty from the fit of the $\pi^0$ mass peak is denoted by fit. $\sigma_{ENBC}$ stands for error on number of binary collisions. Error from $pp$ parametrization that is not $p_T$ dependent. This error is not included in the calculation of the Upper bound of the systematic error and the Lower bound of the systematic error.

Charged hadron to $\pi^0$ ratios for minimum bias events and 9 centrality classes.

Charged hadron to $\pi^0$ ratios for minimum bias events and 9 centrality classes.

Charged hadron to $\pi^0$ ratios for minimum bias events and 9 centrality classes.

Charged hadron to $\pi^0$ ratios for minimum bias events and 9 centrality classes.

Charged hadron to $\pi^0$ ratios for minimum bias events and 9 centrality classes.

Charged hadron to $\pi^0$ ratios for minimum bias events and 9 centrality classes.

Au + Au yield integrated for $p_T$ > 4.5 (GeV/$c$) over the $N$ + $N$ yield, normalized using either $N_{coll}$ or $N_{part}$, plot as a function of $<N_{part}>$. Statistical and systematic error from Au+Au and $N$+$N$ reference includes: a) $NN$ reference error with 10.4% normalization error subtracted, this error is 11.2%, b) systematic error on Au+Au is 8.5% (correction), and c) 5% occupancy correction (it is centrality dependent). Error on $N_{coll}$+10.4% error on $N$+$N$ reference.

Au + Au yield integrated for $p_T$ > 4.5 (GeV/$c$) over the $N$ + $N$ yield, normalized using either $N_{coll}$ or $N_{part}$, plot as a function of $<N_{part}>$. Statistical and systematic error from Au+Au and $N$+$N$ reference includes: a) $NN$ reference error with 10.4% normalization error subtracted, this error is 11.2%, b) systematic error on Au+Au is 8.5% (correction), and c) 5% occupancy correction (it is centrality dependent). Error on $N_{coll}$+10.4% error on $N$+$N$ reference.

Invariant yields from the $p$+$p$ reference data. The normalization uncertainty is labeled norm, the uncertainty from the fit is labeled fit, and the uncertainty $\pi^0$ is from the $\pi^0$ ratio.

$F_{p_T}$ (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).

$\Delta\phi$ 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.

Transverse momentum in GeV/$c$ for $K^{\pm}$.

Transverse momentum in GeV/$c$ for $K^{\pm}$.

Transverse momentum in GeV/$c$ for $p$ and $\bar{p}$.

Measured widths of the near- and away-angle $\pi^0$ - $h^{\pm}$ correlation peaks for various trigger momenta.

Measured widths of the near- and away-angle $\pi^0$ - $h^{\pm}$ correlation peaks for various trigger momenta.

Measured widths of the near- and away-angle $\pi^0$ - $h^{\pm}$ correlation peaks for various trigger momenta.

The $\sigma_N$ and $\sigma_A$ values in GeV/$c$.

The $\sqrt{<p^2_{out}>}$ values in GeV/$c$.

The $\sqrt{<p^2_{out}>}$ values in GeV/$c$.

The $\sqrt{<p^2_{out}>}$ values in GeV/$c$.

The near and away side conditional yield per number of triggers for 1.4 < $p_{Ta}$ < 5.0 GeV/$c$.

The $\sqrt{<j^2_T>}$ values in GeV/$c$.

The $\sqrt{<j^2_T>}$ values in GeV/$c$.

The $\sqrt{<j^2_T>}$ values in GeV/$c$.

The $\sqrt{<j^2_T>}$ values in GeV/$c$.

Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.

Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.

Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.

Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.

Measured $x_E$ distributions associated with various transverse momenta of the trigger $\pi^0$.

Extracted values of $D(x)$ parameters according from the fit to the LEP data and power $n$ of the unmeasured final state parton spectra $\Sigma_q(\bar{p_T})$ extracted from the fit to the single inclusive $\pi^0$ invariant cross section for corresponding fragmentation and fixed values of $\sqrt{<k^2_T>}$ = 2.5 GeV/$c$.

The $\bar{x^-1_h}$ $<z_t>$ $\sqrt{<k^2_T>}$ $\sqrt{<k^2_T>}$ values as a function of $p_{Ta}$ for two different trigger $\pi^0$ transverse momentum bins.

The $\bar{x^-1_h}$ $<z_t>$ $\sqrt{<k^2_T>}$ $\sqrt{<k^2_T>}$ values as a function of $p_{Ta}$ for two different trigger $\pi^0$ transverse momentum bins.

Values of $\bar{x^-1_h}$ $<z_t>$ $\sqrt{<k^2_T>}$ and $\sqrt{<k^2_T>}$ for various trigger particle $p_{Tt}$ and associated momenta in 1.4 < $p_{Ta}$ < 5.0 GeV/$c$ region.

The $<z_t>$ and $\bar{x_h}$ values with $p_{Tt}$

The $<z_t>$ and $\bar{x_h}$ values with $p_{Ta}$ for two trigger $\pi^0$ momenta bins.

The $<z_t>$ and $\bar{x_h}$ values with $p_{Ta}$ for two trigger $\pi^0$ momenta bins.

$I_{AA}$ versus $p_T^B$ for four trigger $p_T$ bins in HR+SR ($|\Delta\phi - \pi|$ < $\pi/2$) and HR ($|\Delta\phi - \pi|$ < $\pi/6$).

$I_{AA}$ versus $p_T^B$ for four trigger $p_T$ bins in HR+SR ($|\Delta\phi - \pi|$ < $\pi/2$) and HR ($|\Delta\phi - \pi|$ < $\pi/6$).

Truncated mean $<p_T^{\prime}>$ in 1 < $p_T^B$ < 5 GeV/$c$ versus $N_{part}$ for the near-side, away-side shoulder, and head regions for Au+Au and $p$+$p$ for three trigger $p_T$ bins.

The fraction of the direct photon component as a function of $p_T$.

The fraction of the direct photon component as a function of $p_T$.

Invariant yield (Au+Au) of direct photons as a function of $p_T$.

Invariant yield (Au+Au) of direct photons as a function of $p_T$.

Invariant yield (Au+Au) of direct photons as a function of $p_T$.

Invariant cross section ($p$+$p$) of direct photons as a function of $p_T$.

Additional information containing number of events which were used to reconstruct the numvers matching to Figure 1 and 2.

Additional information containing number of events which were used to reconstruct the numvers matching to Figure 1 and 2.

Additional information containing number of events which were used to reconstruct the numvers matching to Figure 1 and 2.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Au+Au collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Cu+Cu collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Cu+Cu collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Cu+Cu collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Cu+Cu collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Cu+Cu collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Cu+Cu collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV Cu+Cu collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Cu+Cu collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Cu+Cu collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Cu+Cu collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Cu+Cu collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 62.4 GeV Cu+Cu collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 22.5 GeV Cu+Cu collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 22.5 GeV Cu+Cu collisions.

The uncorrected multiplicity distributions of charged hadrons with 0.2 < $p_T$ < 2.0 GeV/$c$ for 200 GeV $p$+$p$ collisions.

The mean from the NBD fit as a function of $N_{part}$ for 200 GeV Au+Au collisions over the range 0.2 < $p_T$ < 2.0 GeV/$c$.

The mean from the NBD fit as a function of $N_{part}$ for 62.4 GeV Au+Au collisions over the range 0.2 < $p_T$ < 2.0 GeV/$c$.

The mean from the NBD fit as a function of $N_{part}$ for 200 GeV Cu+Cu collisions over the range 0.2 < $p_T$ < 2.0 GeV/$c$.

The mean from the NBD fit as a function of $N_{part}$ for 62.4 GeV Cu+Cu collisions over the range 0.2 < $p_T$ < 2.0 GeV/$c$.

The mean from the NBD fit as a function of $N_{part}$ for 22.5 GeV Cu+Cu collisions over the range 0.2 < $p_T$ < 2.0 GeV/$c$.

Fluctuations expressed as the scaled variance as a function of centrality for 200 GeV Au+Au collisions in the range 0.2 < $p_T$ < 2.0 GeV/$c$.

Fluctuations expressed as the scaled variance as a function of $N_{part}$ for 200 GeV Au+Au collisions for 0.2 < $p_T$ < 2.0 GeV/$c$.

Fluctuations expressed as the scaled variance as a function of $N_{part}$ for 62.4 GeV Au+Au collisions for 0.2 < $p_T$ < 2.0 GeV/$c$.

Fluctuations expressed as the scaled variance as a function of $N_{part}$ for 200 GeV Cu+Cu collisions for 0.2 < $p_T$ < 2.0 GeV/$c$.

Fluctuations expressed as the scaled variance as a function of $N_{part}$ for 62.4 GeV Cu+Cu collisions for 0.2 < $p_T$ < 2.0 GeV/$c$.

Fluctuations expressed as the scaled variance as a function of $N_{part}$ for 22.5 GeV Cu+Cu collisions for 0.2 < $p_T$ < 2.0 GeV/$c$.

Scaled variance for 200 GeV Au+Au collisions plotted as a function of $N_{part}$ for several $p_T$ ranges.

Scaled variance for 200 GeV Au+Au collisions plotted as a function of $N_{part}$ for several $p_T$ ranges.

Scaled variance for 62.4 GeV Au+Au collisions plotted as a function of $N_{part}$ for several $p_T$ ranges.

Scaled variance for 62.4 GeV Au+Au collisions plotted as a function of $N_{part}$ for several $p_T$ ranges.

Scaled variance for 62.4 GeV Au+Au collisions plotted as a function of $N_{part}$ for several $p_T$ ranges.

Scaled variance for 200 GeV Cu+Cu collisions plotted as a function of $N_{part}$ for several $p_T$ ranges.

Scaled variance for 200 GeV Cu+Cu collisions plotted as a function of $N_{part}$ for several $p_T$ ranges.

Scaled variance for 200 GeV Cu+Cu collisions plotted as a function of $N_{part}$ for several $p_T$ ranges.

Scaled variance for 62.4 GeV Cu+Cu collisions plotted as a function of $N_{part}$ for several $p_T$ ranges.

Scaled variance for 62.4 GeV Cu+Cu collisions plotted as a function of $N_{part}$ for several $p_T$ ranges.

The inverse of the parameter $k_{NBD}$ from the Negative Binomial Distribution fits for 200 GeV Au+Au collisions. The fluctuations are plotted as a function of $N_{part}$ for several $p_T$ ranges.

The inverse of the parameter $k_{NBD}$ from the Negative Binomial Distribution fits for 200 GeV Au+Au collisions. The fluctuations are plotted as a function of $N_{part}$ for several $p_T$ ranges.

The inverse of the parameter $k_{NBD}$ from the Negative Binomial Distribution fits for 62.4 GeV Au+Au collisions. The fluctuations are plotted as a function of $N_{part}$ for several $p_T$ ranges.

The inverse of the parameter $k_{NBD}$ from the Negative Binomial Distribution fits for 62.4 GeV Au+Au collisions. The fluctuations are plotted as a function of $N_{part}$ for several $p_T$ ranges.

The inverse of the parameter $k_{NBD}$ from the Negative Binomial Distribution fits for 62.4 GeV Au+Au collisions. The fluctuations are plotted as a function of $N_{part}$ for several $p_T$ ranges.

The inverse of the parameter $k_{NBD}$ from the Negative Binomial Distribution fits for 200 GeV Cu+Cu collisions. The fluctuations are plotted as a function of $N_{part}$ for several $p_T$ ranges.

The inverse of the parameter $k_{NBD}$ from the Negative Binomial Distribution fits for 200 GeV Cu+Cu collisions. The fluctuations are plotted as a function of $N_{part}$ for several $p_T$ ranges.

The inverse of the parameter $k_{NBD}$ from the Negative Binomial Distribution fits for 200 GeV Cu+Cu collisions. The fluctuations are plotted as a function of $N_{part}$ for several $p_T$ ranges.

The inverse of the parameter $k_{NBD}$ from the Negative Binomial Distribution fits for 62.4 GeV Cu+Cu collisions. The fluctuations are plotted as a function of $N_{part}$ for several $p_T$ ranges.

The inverse of the parameter $k_{NBD}$ from the Negative Binomial Distribution fits for 62.4 GeV Cu+Cu collisions. The fluctuations are plotted as a function of $N_{part}$ for several $p_T$ ranges.

The scaled variance as a funciton of $N_{part}$ for 200 GeV Au+Au collisions in the range 0.2 < $p_T$ < 2.0 GeV/$c$.

The correlation of the clan model parameters $\bar{n_c}$ and $\bar{N_c}$ for all of the collision species measured as a function of centrality.

The correlation of the clan model parameters $\bar{n_c}$ and $\bar{N_c}$ for all of the collision species measured as a function of centrality.

The correlation of the clan model parameters $\bar{n_c}$ and $\bar{N_c}$ for all of the collision species measured as a function of centrality.

The correlation of the clan model parameters $\bar{n_c}$ and $\bar{N_c}$ for all of the collision species measured as a function of centrality.

The correlation of the clan model parameters $\bar{n_c}$ and $\bar{N_c}$ for all of the collision species measured as a function of centrality.

The correlation of the clan model parameters $\bar{n_c}$ and $\bar{N_c}$ for all of the collision species measured as a function of centrality.

The correlation of the clan model parameters $\bar{n_c}$ and $\bar{N_c}$ for all of the collision species measured as a function of centrality.

The correlation of the clan model parameters $\bar{n_c}$ and $\bar{N_c}$ for all of the collision species measured as a function of centrality.

The correlation of the clan model parameters $\bar{n_c}$ and $\bar{N_c}$ for all of the collision species measured as a function of centrality.

The correlation of the clan model parameters $\bar{n_c}$ and $\bar{N_c}$ for all of the collision species measured as a function of centrality.

The correlation of the clan model parameters $\bar{n_c}$ and $\bar{N_c}$ for all of the collision species measured as a function of centrality.