Integrated per-trigger yields as a function of associated particle angle relative to $\psi_2$ event plane $\phi^a - \psi_2$ integrated over the near side $|\Delta\phi|<\pi/4$.

Integrated per-trigger yields as a function of associated particle angle relative to $\psi_2$ event plane $\phi^a - \psi_2$ integrated over the away side $|\Delta\phi|<\pi/4$.

Integrated per-trigger yields as a function of associated particle angle relative to $\psi_2$ event plane for near-side $|\Delta\phi|<\pi/4$ and for away-side $|\Delta\phi|<\pi/4$.

Integrated per-trigger yields as a function of associated particle angle relative to $\psi_2$ event plane for near-side $|\Delta\phi|<\pi/4$ and for away-side $|\Delta\phi|<\pi/4$.

Per-trigger yields $Y(\Delta\phi)$ of dihadrons pairs measured in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200~{\rm GeV}$ after subtracting the underlying event model with several $p_T$ selections. Systematic uncertainties due to track matching are given.

Per-trigger yields $Y(\Delta\phi)$ of dihadrons pairs measured in Au$+$Au collisions at $\sqrt{s_{_{NN}}}=200~{\rm GeV}$ after subtracting the underlying event model with several $p_T$ selections. Systematic uncertainties due to track matching are given.

$\Psi_{2}$-dependent $C(\Delta\phi)$ for $2<p_{T}^{trig}<4$ GeV/c and $1<p_{T}^{assoc}<2$ GeV/c.

$\Psi_{2}$-dependent $C(\Delta\phi)$ for $2<p_{T}^{trig}<4$ GeV/c and $2<p_{T}^{assoc}<4$ GeV/c.

$\Psi_{2}$-dependent $C(\Delta\phi)$ for $4<p_{T}^{trig}<10$ GeV/c and $2<p_{T}^{assoc}<4$ GeV/c.

$\Psi_{3}$-dependent $C(\Delta\phi)$ for $2<p_{T}^{trig}<4$ GeV/c and $1<p_{T}^{assoc}<2$ GeV/c.

$\Psi_{3}$-dependent $C(\Delta\phi)$ for $2<p_{T}^{trig}<4$ GeV/c and $2<p_{T}^{assoc}<4$ GeV/c.

$\Psi_{3}$-dependent $C(\Delta\phi)$ for $4<p_{T}^{trig}<10$ GeV/c and $1<p_{T}^{assoc}<2$ GeV/c.

$\Psi_{2}$-dependent $Y(\Delta\phi)$ for $2<p_{T}^{trig}<4$ GeV/c and $1<p_{T}^{assoc}<2$ GeV/c.

$\Psi_{2}$-dependent $C(\Delta\phi)$ for $2<p_{T}^{trig}<4$ GeV/c and $2<p_{T}^{assoc}<4$ GeV/c.

$\Psi_{2}$-dependent $C(\Delta\phi)$ for $4<p_{T}^{trig}<10$ GeV/c and $2<p_{T}^{assoc}<4$ GeV/c.

$\Psi_{3}$-dependent $C(\Delta\phi)$ for $2<p_{T}^{trig}<4$ GeV/c and $1<p_{T}^{assoc}<2$ GeV/c.

$\Psi_{3}$-dependent $C(\Delta\phi)$ for $2<p_{T}^{trig}<4$ GeV/c and $2<p_{T}^{assoc}<4$ GeV/c.

$\Psi_{3}$-dependent $C(\Delta\phi)$ for $4<p_{T}^{trig}<10$ GeV/c and $2<p_{T}^{assoc}<4$ GeV/c.

$\Psi_2$-dependent C for 2 $< p_T^t <$ 4 and 1 $< p_T^a <$ 2 GeV/c.

$\Psi_2$-dependent C for 2 $< p_T^t <$ 4 and 2 $< p_T^a <$ 4 GeV/c.

$\Psi_2$-dependent C for 4 $< p_T^t <$ 10 and 2 $< p_T^a <$ 4 GeV/c.

$\Psi_2$-dependent Y for 2 $< p_T^t <$ 4 and 1 $< p_T^a <$ 2 GeV/c.

$\Psi_2$-dependent Y for 2 $< p_T^t <$ 4 and 2 $< p_T^a <$ 4 GeV/c.

$\Psi_2$-dependent Y for 4 $< p_T^t <$ 10 and 2 $< p_T^a <$ 4 GeV/c.

$\Psi_3$-dependent C for 2 $< p_T^t <$ 4 and 1 $< p_T^a <$ 2 GeV/c.

$\Psi_3$-dependent C for 2 $< p_T^t <$ 4 and 2 $< p_T^a <$ 4 GeV/c.

$\Psi_3$-dependent C for 4 $< p_T^t <$ 10 and 2 $< p_T^a <$ 4 GeV/c.

$\Psi_3$-dependent Y for 2 $< p_T^t <$ 4 and 1 $< p_T^a <$ 2 GeV/c.

$\Psi_3$-dependent Y for 2 $< p_T^t <$ 4 and 2 $< p_T^a <$ 4 GeV/c.

$\Psi_3$-dependent Y for 4 $< p_T^t <$ 10 and 2 $< p_T^a <$ 4 GeV/c.

$p_T$ 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.