$p_{\rm T}$ dependence of directed flow in centrality 40-50%.

$p_{\rm T}$ dependence of directed flow in centrality 50-60%.

$p_{\rm T}$ dependence of Delta v1 in centrality 10-20%.

$p_{\rm T}$ dependence of Delta v1 in centrality 20-30%.

$p_{\rm T}$ dependence of Delta v1 in centrality 30-40%.

$p_{\rm T}$ dependence of Delta v1 in centrality 40-50%.

$p_{\rm T}$ dependence of Delta v1 in centrality 50-60%.

$p_{\rm T}$ dependence of directed flow in centrality 10-40%.

$p_{\rm T}$ dependence of directed flow in centrality 10-40%.

$p_{\rm T}$ dependence of Delat v1 in centrality 10-40%.

$p_{\rm T}$ dependence of directed flow in centrality 10-40%.

eta dependence of directed flow in centrality 10-40%.

eta dependence of Delta v1 in centrality 10-40%.

Per-trigger yield versus $\Delta\phi$ for various trigger and partner $p_T$ ($p^a_T \otimes p^b_T$), arranged by increasing pair proxy energy (sum of $p^a_T$ and $p^b_T$), in p + p collisions for 3-4 $\otimes$ 0.4-1, 3-4 $\otimes$ 1-2, 3-4 $\otimes$ 2-3, and 3-4 $\otimes$ 3-4 GeV/c.

The 0-20% Au+Au jet-induced hadron-pair yield $\Delta\phi$ distributions calculated from the per-trigger yield using low-$p_T$ hadrons as triggers and high-$p_T$ hadrons as triggers. Data for 4 - 5 GeV/$c$.

Per-trigger yield versus $\Delta\phi$ for various trigger and partner $p_T$ ($p^a_T \otimes p^b_T$), arranged by increasing pair proxy energy (sum of $p^a_T$ and $p^b_T$), in Au + Au collisions for 3-4 $\otimes$ 0.4-1, 3-4 $\otimes$ 1-2, 3-4 $\otimes$ 2-3, and 3-4 $\otimes$ 3-4 GeV/c.

Per-trigger yield versus $\Delta\phi$ for various trigger and partner $p_T$ ($p^a_T \otimes p^b_T$), arranged by increasing pair proxy energy (sum of $p^a_T$ and $p^b_T$), in p + p collisions for 5-10 $\otimes$ 2-3, 4-5 $\otimes$ 4-5, 5-10 $\otimes$ 3-5, and 5-10 $\otimes$ 5-10 GeV/c.

Per-trigger yield versus $\Delta\phi$ for various trigger and partner $p_T$ ($p^a_T \otimes p^b_T$), arranged by increasing pair proxy energy (sum of $p^a_T$ and $p^b_T$), in Au + Au collisions for 5-10 $\otimes$ 2-3, 4-5 $\otimes$ 4-5, 5-10 $\otimes$ 3-5, and 5-10 $\otimes$ 5-10 GeV/c.

Per-trigger yield versus $\Delta\phi$ for various trigger and partner $p_T$ ($p^a_T \otimes p^b_T$), arranged by increasing pair proxy energy (sum of $p^a_T$ and $p^b_T$), in p + p collisions for 3-4 $\otimes$ 0.4-1, 3-4 $\otimes$ 1-2, 3-4 $\otimes$ 2-3, and 3-4 $\otimes$ 3-4 GeV/c.

RHS versus $p^b_T$ for p + p collisions for four trigger selections.

Per-trigger yield versus $\Delta\phi$ for various trigger and partner $p_T$ ($p^a_T \otimes p^b_T$), arranged by increasing pair proxy energy (sum of $p^a_T$ and $p^b_T$), in Au + Au collisions for 3-4 $\otimes$ 0.4-1, 3-4 $\otimes$ 1-2, 3-4 $\otimes$ 2-3, and 3-4 $\otimes$ 3-4 GeV/c.

RHS versus $p^b_T$ for Au + Au collisions for four trigger selections.

Per-trigger yield versus $\Delta\phi$ for various trigger and partner $p_T$ ($p^a_T \otimes p^b_T$), arranged by increasing pair proxy energy (sum of $p^a_T$ and $p^b_T$), in Au + Au collisions for 5-10 $\otimes$ 2-3, 4-5 $\otimes$ 4-5, 5-10 $\otimes$ 3-5, and 5-10 $\otimes$ 5-10 GeV/c.

RHS versus $N_{part}$ for 2-3 $\otimes$ 2-3 GeV/$c$. Shaded bars (brackets) represent $p_T$ -correlated uncertainties due to elliptic flow (ZYAM procedure). The most left point is from p+p.

RHS versus $p^b_T$ for p + p collisions for four trigger selections.

Per-trigger yield $\Delta\phi$ distribution and corresponding fits for 2-3 $\otimes$ 2-3 GeV/c in 0-5% Au+Au collisions.

RHS versus $p^b_T$ for Au + Au collisions for four trigger selections.

a) D versus centrality from FIT 1 and FIT2 for 2 - 3 GeV/$c$ bin. The error bars are the statistical errors; The shaded bars and brackets are the systematic errors due to $v_2$. b) The fraction of the shoulder Gaussian yield relative to the total away-side yield as function of centrality determined from FIT2.

RHS versus $N_{part}$ for 2-3 $\otimes$ 2-3 GeV/$c$. Shaded bars (brackets) represent $p_T$ -correlated uncertainties due to elliptic flow (ZYAM procedure). The most left point is from p+p.

Values of D determined from FIT1 as function of partner $p_T$ for 2-3 GeV/c $p_T$ range in 0-20% Au+Au.

Per-trigger yield $\Delta\phi$ distribution and corresponding fits for 2−3 $\otimes$ 2−3 GeV/c in 0-5% Au+Au collisions.

Values of D determined from FIT1 as function of partner $p_T$ for 3-4 GeV/c $p_T$ range in 0-20% Au+Au.

a) D versus $N_{part}$ from FIT 1 and FIT2 for 2 - 3 GeV/$c$ bin. The error bars are the statistical errors; The shaded bars and brackets are the systematic errors due to $v_2$. b) The fraction of the shoulder Gaussian yield relative to the total away-side yield as function of $N_{part}$ determined from FIT2.

Values of D determined from FIT1 as function of partner $p_T$ for 4-5 GeV/c $p_T$ range in 0-20% Au+Au.

Values of D determined from FIT1 as function of partner $p_T$ for 2-3 GeV/c $p_T$ range in 0-20% Au+Au.

Values of D determined from FIT2 as function of partner $p_T$ for 2-3 GeV/c $p_T$ range in 0-20% Au+Au.

Values of D determined from FIT1 as function of partner $p_T$ for 3-4 GeV/c $p_T$ range in 0-20% Au+Au.

Values of D determined from FIT2 as function of partner $p_T$ for 3-4 GeV/c $p_T$ range in 0-20% Au+Au.

Values of D determined from FIT1 as function of partner $p_T$ for 4-5 GeV/c $p_T$ range in 0-20% Au+Au.

Values of D determined from FIT2 as function of partner $p_T$ for 4-5 GeV/c $p_T$ range in 0-20% Au+Au.

Values of D determined from FIT2 as function of partner $p_T$ for 2-3 GeV/c $p_T$ range in 0-20% Au+Au.

Per-trigger yield as function of partner $p_T$ for the HR region for the 0-20% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Values of D determined from FIT2 as function of partner $p_T$ for 3-4 GeV/c $p_T$ range in 0-20% Au+Au.

Per-trigger yield as function of partner $p_T$ for the HR region for the 20-40% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Values of D determined from FIT2 as function of partner $p_T$ for 4-5 GeV/c $p_T$ range in 0-20% Au+Au.

Per-trigger yield as function of partner $p_T$ for the HR region for the 40-60% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the HR region for the 0-20% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the HR region for the 60-92% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the HR region for the 20-40% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the HR region for the p + p collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the HR region for the 40-60% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the SR region for the 0-20% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the HR region for the 60-92% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the SR region for the 20-40% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the HR region for the p + p collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the SR region for the 40-60% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the SR region for the 0-20% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the SR region for the 60-92% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the SR region for the 20-40% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the SR region for the p + p collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Per-trigger yield as function of partner $p_T$ for the SR region for the 40-60% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Near-side Gaussian widths versus partner $p_T$ for four trigger $p_T$ ranges for 0-20 % Au + Au.

Per-trigger yield as function of partner $p_T$ for the SR region for the 60-92% Au + Au collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Near-side Gaussian widths versus partner $p_T$ for four trigger $p_T$ ranges for 0-20 % p + p.

Per-trigger yield as function of partner $p_T$ for the SR region for the p + p collisions. Results for four trigger pT in 2-3, 3-4, 4-5, 5-10 GeV/c are shown.

Near-side Gaussian widths versus $N_{part}$ for five successively increasing $p^a_T$ $\otimes$ $p^b_T$. The most left point in each panel represents the value from p + p.

Near-side Gaussian widths versus partner $p_T$ for four trigger $p_T$ ranges for 0-20 % Au + Au.

Near-side yield in $\lvert \Delta\phi \rvert$ < $\pi$/3 versus partner $p_T$ for four trigger $p_T$ selections for 0-20% p + p.

Near-side Gaussian widths versus partner $p_T$ for four trigger $p_T$ ranges for 0-20 % p + p.

Near-side yield in $\lvert \Delta\phi \rvert$ < $\pi$/3 versus partner $p_T$ for four trigger $p_T$ selections for 0-20% Au + Au.

Near-side Gaussian widths versus $N_{part}$ for five successively increasing $p^a_T$ $\otimes$ $p^b_T$. The most left point in each panel represents the value from p + p.

Near-side yield in $\lvert \Delta\phi \rvert$ < $\pi$/3 versus partner $p_T$ for four trigger $p_T$ selections for 0-20% Au + Au.

Near-side yield in $\lvert \Delta\phi \rvert$ < $\pi$/3 versus partner $p_T$ for four trigger $p_T$ selections for 0-20% p + p.

Near-side yield in $\lvert \Delta\phi \rvert$ < $\pi$/3 versus partner $p_T$ for four trigger $p_T$ selections for 0-20% Au + Au.

Near-side yield in $\lvert \Delta\phi \rvert$ < $\pi$/3 versus partner $p_T$ for four trigger $p_T$ selections for 0-20% Au + Au.

Near-side yield in $\lvert \Delta\phi \rvert$ < $\pi$/3 versus partner $p_T$ for four trigger $p_T$ selections for 0-20% Au + Au.

Per-trigger yield versus $\Delta\eta$ for 0-20% central Au + Au collisions. Results are shown for four $p^a_T \otimes p^b_T$ selections as indicated.

Per-trigger yield versus $\Delta\eta$ for 0-20% central Au + Au collisions. Results are shown for four $p^a_T \otimes p^b_T$ selections as indicated.

Per-trigger yield versus $\Delta\eta$ for 0-20% central p + p collisions. Results are shown for four $p^a_T \otimes p^b_T$ selections as indicated.

Per-trigger yield versus $\Delta\eta$ for 0-20% central p + p collisions. Results are shown for four $p^a_T \otimes p^b_T$ selections as indicated.

The projection of 2-D per-trigger yield in $\lvert \Delta\eta \rvert$ < 0.7 $\otimes$ $\lvert \Delta\phi \rvert$ < 0.7 and 0-20% central Au+Au collisions onto $\Delta\eta$ for four $p^a_T \otimes p^b_T$ selections.

The projection of 2-D per-trigger yield in $\lvert \Delta\eta \rvert$ < 0.7 $\otimes$ $\lvert \Delta\phi \rvert$ < 0.7 and 0-20% central Au+Au collisions onto $\Delta\eta$ for four $p^a_T \otimes p^b_T$ selections.

The projection of 2-D per-trigger yield in $\lvert \Delta\eta \rvert$ < 0.7 $\otimes$ $\lvert \Delta\phi \rvert$ < 0.7 and 0-20% central Au+Au collisions onto $\Delta\phi$ for four $p^a_T \otimes p^b_T$ selections.

The projection of 2-D per-trigger yield in $\lvert \Delta\eta \rvert$ < 0.7 $\otimes$ $\lvert \Delta\phi \rvert$ < 0.7 and 0-20% central Au+Au collisions onto $\Delta\phi$ for four $p^a_T \otimes p^b_T$ selections.

Truncated mean $p_T$, $\langle p_T \rangle$, in 1 <pbT < 5 GeV/c versus $N_{part}$ for the head region for Au + Au and p + p for four trigger $p_T$ bins.

Truncated mean $p_T$, $\langle p_T \rangle$, in 1 <pbT < 5 GeV/c versus centrality for the head region for Au + Au for four trigger $p_T$ bins.

Truncated mean $p_T$, $\langle p_T \rangle$, in 1 <pbT < 5 GeV/c versus $N_{part}$ for the away-side shoulder region for Au + Au and p + p for four trigger $p_T$ bins.

Truncated mean $p_T$, $\langle p_T \rangle$, in 1 <pbT < 5 GeV/c versus centrality for the away-side shoulder region for Au + Au for four trigger $p_T$ bins.

Truncated mean $p_T$, $\langle p_T \rangle$, in 1 <pbT < 5 GeV/c versus $N_{part}$ for the near-side region for Au + Au and p + p for four trigger $p_T$ bins.

Truncated mean $p_T$, $\langle p_T \rangle$, in 1 <pbT < 5 GeV/c versus centrality for the near-side region for Au + Au for four trigger $p_T$ bins.

Truncated mean $p_T$, $\langle p_T \rangle$, calculated for five partner pT ranges in the HR. Results for triggers in 3 − 4 GeV/c.

Truncated mean $p_T$, $\langle p_T \rangle$, in 1 <pbT < 5 GeV/c versus centrality for the head region for p + p for four trigger $p_T$ bins.

Truncated mean $p_T$, $\langle p_T \rangle$, calculated for five partner pT ranges in the HR. Results for triggers in 4 − 5 GeV/c.

Truncated mean $p_T$, $\langle p_T \rangle$, in 1 <pbT < 5 GeV/c versus centrality for the away-side shoulder region for p + p for four trigger $p_T$ bins.

The near-side pair suppression factor $J_{AA}$ in 0-20% Au + Au collisions as function of $p^b_T$ for various ranges of $p^a_T$.

Truncated mean $p_T$, $\langle p_T \rangle$, in 1 <pbT < 5 GeV/c versus centrality for the near-side region for p + p for four trigger $p_T$ bins.

The near-side $J_{AA}$ as function of $p^b_T$ and $p^{sum}_T$ for four $p^a_T$ bins and three centrality bins. Data for 20-40%.

Truncated mean $p_T$, $\langle p_T \rangle$, calculated for five partner pT ranges in the HR. Results for triggers in 3-4 GeV/c.

The near-side $J_{AA}$ as function of $p^b_T$ and $p^{sum}_T$ for four $p^a_T$ bins and three centrality bins. Data for 40-60%.

Truncated mean $p_T$, $\langle p_T \rangle$, calculated for five partner pT ranges in the HR. Results for triggers in 4-5 GeV/c.

The near-side $J_{AA}$ as function of $p^b_T$ and $p^{sum}_T$ for four $p^a_T$ bins and three centrality bins. Data for 60-92%.

Truncated mean $p_T$, $\langle p_T \rangle$, calculated for five partner pT ranges in the HR. Results for triggers in 3-4 GeV/c.

The pair suppression factor $J_{AA}$ for the away-side HR in 0-20% Au + Au collisions as function of $p_b^T$ for various ranges of $p_a^T$.

Truncated mean $p_T$, $\langle p_T \rangle$, calculated for five partner pT ranges in the HR. Results for triggers in 4-5 GeV/c.

The pair suppression factor $J_{AA}$ for the away-side HR in 20-40% Au + Au collisions as function of $p_b^T$ for various ranges of $p_a^T$.

The near-side pair suppression factor $J_{AA}$ in 0-20% Au + Au collisions as function of $p^b_T$ for various ranges of $p^a_T$.

The pair suppression factor $J_{AA}$ for the away-side HR in 40-60% Au + Au collisions as function of $p_b^T$ for various ranges of $p_a^T$.

The near-side $J_{AA}$ as function of $p^b_T$ and $p^{sum}_T$ for four $p^a_T$ bins and three centrality bins. Data for 20-40%.

The pair suppression factor $J_{AA}$ for the away-side HR in 60-92% Au + Au collisions as function of $p_b^T$ for various ranges of $p_a^T$.

The near-side $J_{AA}$ as function of $p^b_T$ and $p^{sum}_T$ for four $p^a_T$ bins and three centrality bins. Data for 40-60%.

Per-trigger yield versus $\Delta\phi$ for successively increasing trigger and partner $p_T$ ($p^a_T \otimes p^b_T$) in 0-20 % Au + Au collisions.

The near-side $J_{AA}$ as function of $p^b_T$ and $p^{sum}_T$ for four $p^a_T$ bins and three centrality bins. Data for 60-92%.

Per-trigger yield versus $\Delta\phi$ for successively increasing trigger and partner $p_T$ ($p^a_T \otimes p^b_T$) in p + p collisions.

The pair suppression factor $J_{AA}$ for the away-side HR in 0-20% Au + Au collisions as function of $p_b^T$ for various ranges of $p_a^T$.

Per-trigger yield versus $\Delta\phi$ for successively increasing trigger and partner $p_T$ ($p^a_T \otimes p^b_T$) in 20-40 % Au + Au collisions.

The pair suppression factor $J_{AA}$ for the away-side HR in 20-40% Au + Au collisions as function of $p_b^T$ for various ranges of $p_a^T$.

Per-trigger yield versus $\Delta\phi$ for successively increasing trigger and partner $p_T$ ($p^a_T \otimes p^b_T$) in p + p collisions.

The pair suppression factor $J_{AA}$ for the away-side HR in 40-60% Au + Au collisions as function of $p_b^T$ for various ranges of $p_a^T$.

Per-trigger yield versus $\Delta\phi$ for successively increasing trigger and partner $p_T$ ($p^a_T \otimes p^b_T$) in 60-92 % Au + Au collisions.

The pair suppression factor $J_{AA}$ for the away-side HR in 60-92% Au + Au collisions as function of $p_b^T$ for various ranges of $p_a^T$.

Per-trigger yield versus $\Delta\phi$ for successively increasing trigger and partner $p_T$ ($p^a_T \otimes p^b_T$) in p + p collisions.

Per-trigger yield versus $\Delta\phi$ for successively increasing trigger and partner $p_T$ ($p^a_T \otimes p^b_T$) in 0-20 % Au + Au collisions.

Per-trigger yield versus $\Delta\phi$ for successively increasing trigger and partner $p_T$ ($p^a_T \otimes p^b_T$) in 20-40 % Au + Au collisions.

Per-trigger yield versus $\Delta\phi$ for successively increasing trigger and partner $p_T$ ($p^a_T \otimes p^b_T$) in 40-60 % Au + Au collisions.

Per-trigger yield versus $\Delta\phi$ for successively increasing trigger and partner $p_T$ ($p^a_T \otimes p^b_T$) in 60-92 % Au + Au collisions.

Per-trigger yield versus $\Delta\phi$ for successively increasing trigger and partner $p_T$ ($p^a_T \otimes p^b_T$) in p + p collisions.

$D_s^{\pm}$ invariant yield as a function of $p_{T}$ in 40-80% centrality bin of Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV. The $p_T$ bins are 1.5 < $p_T$ < 2.5 GeV/c, 2.5 < $p_T$ < 3.5 GeV/c, 3.5 < $p_T$ < 5.0 GeV/c and 5.0 < $p_T$ < 8.0 GeV/c.

$D_{s}/D^{0}$ yield ratio as a function of $p_{T}$ in 0-10% centrality bin of Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV. The $p_T$ bins are 1.5 < $p_T$ < 2.5 GeV/c, 2.5 < $p_T$ < 3.5 GeV/c, 3.5 < $p_T$ < 5.0 GeV/c and 5.0 < $p_T$ < 8.0 GeV/c.

$D_{s}/D^{0}$ yield ratio as a function of $p_{T}$ in 10-40% centrality bin of Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV. The $p_T$ bins are 1.0 < $p_T$ < 2.0 GeV/c, 2.0 < $p_T$ < 2.5 GeV/c, 2.5 < $p_T$ < 3.5 GeV/c, 3.5 < $p_T$ < 5.0 GeV/c and 5.0 < $p_T$ < 8.0 GeV/c.

$D_{s}/D^{0}$ yield ratio as a function of $p_{T}$ in 40-80% centrality bin of Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV. The $p_T$ bins are 1.5 < $p_T$ < 2.5 GeV/c, 2.5 < $p_T$ < 3.5 GeV/c, 3.5 < $p_T$ < 5.0 GeV/c and 5.0 < $p_T$ < 8.0 GeV/c.

$D_{s}/D^{0}$ yield ratio as a function of $p_{T}$ in 10-20% centrality bin of Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV. The $p_T$ bins are 1.5 < $p_T$ < 2.5 GeV/c, 2.5 < $p_T$ < 3.5 GeV/c, 3.5 < $p_T$ < 5.0 GeV/c and 5.0 < $p_T$ < 8.0 GeV/c.

$D_{s}/D^{0}$ yield ratio as a function of $p_{T}$ in 20-40% centrality bin of Au+Au collisions at $\sqrt{s_{_{\rm NN}}}$ = 200 GeV. The $p_T$ bins are 1.5 < $p_T$ < 2.5 GeV/c, 2.5 < $p_T$ < 3.5 GeV/c, 3.5 < $p_T$ < 5.0 GeV/c and 5.0 < $p_T$ < 8.0 GeV/c.

The integrated $D_{s}/D^{0}$ yield ratio within 1.5 < $p_{T}$ < 5.0 GeV/c as a function of collision centrality. The centrality bins are 60-80%, 40-60%, 20-40%, 10-20% and 0-10%.

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.

Fit paramaters $T_{0}^{+}$ and $T_{0}^{-}$. Errors are statistical only.

Fit paramaters $u_{t}^{+}$ and $u_{t}^{-}$. Errors are statistical only.

Relationship between $N_{part}$ and centrality.

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.

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.

I_AA vs xi varying integration range

I_AA vs xi varying integration range

$p^{a}_{T} = 4-5$ GeV/$c$

$p^{a}_{T} = 5-7$ GeV/$c$

$p^{a}_{T} = 3-4$ GeV/$c$

$p^{a}_{T} = 4-5$ GeV/$c$

$p^{a}_{T} = 5-7$ GeV/$c$

$I^{out}_{AA}/I^{in}_{AA}$ ratio, central collisions

$I^{out}_{AA}/I^{in}_{AA}$ ratio, central collisions

$I^{out}_{AA}/I^{in}_{AA}$ ratio, mid-central collisions

$I^{out}_{AA}/I^{in}_{AA}$ ratio, mid-central collisions

Per-Trigger Azimuthal Yields, central collisions, 4-7 x 3-4 GeV/c

Per-Trigger Azimuthal Yields, central collisions, 4-7 x 4-5 GeV/c

Per-Trigger Azimuthal Yields, central collisions, 4-7 x 5-7 GeV/c

Per-Trigger Azimuthal Yields, mid-central collisions, 4-7 x 3-4 GeV/c

Per-Trigger Azimuthal Yields, mid-central collisions, 4-7 x 4-5 GeV/c

Per-Trigger Azimuthal Yields, mid-central collisions, 4-7 x 5-7 GeV/c

Per-Trigger Azimuthal Yields, central collisions, 4-7 x 3-4 GeV/c

$p^{a}_{T} = 3-4$ GeV/$c$

$p^{a}_{T} = 4-5$ GeV/$c$

$p^{a}_{T} = 5-7$ GeV/$c$

pion dAu Invariant yields versus $p_T$

proton AuAu Invariant yields versus $p_T$

proton dAu Invariant yields versus $p_T$

AuAu Ratio kaon versus $p_T$

dAu Ratio kaon versus $p_T$

AuAu Ratio pion versus $p_T$

dAu Ratio pion versus $p_T$

AuAu Ratio proton versus $p_T$

dAu Ratio proton versus $p_T$

AuAu Ratio $kaon/\pi$ versus $p_T$

dAu Ratio $kaon/\pi$ versus $p_T$

AuAu Ratio $p/\pi$ versus $p_T$

dAu Ratio $p/\pi$ versus $p_T$

AuAu kaon $R_{CP}$ versus $p_T$

AuAu pion $R_{CP}$ versus $p_T$

AuAu proton $R_{CP}$ versus $p_T$

AuAu kaon $R_{AA}$ versus $p_T$ (Uncertainity type C is not included)

AuAu pion $R_{AA}$ versus $p_T$ (Uncertainity type C is not included)

AuAu proton $R_{AA}$ versus $p_T$ (Uncertainity type C is not included)

dAu kaon $R_{dA}$ versus $p_T$ (Uncertainity type C is not included)

dAu pion $R_{dA}$ versus $p_T$ (Uncertainity type C is not included)

dAu proton $R_{dA}$ versus $p_T$ (Uncertainity type C is not included)

kaon AuAu Ratio of Invariant yields versus $p_T$

pion AuAu Ratio of Invariant yields versus $p_T$

proton AuAu Ratio of Invariant yields versus $p_T$