The $\phi$-meson integrated nuclear modification factors $R_{AB}$ measured as a function of $N_{part}$

The comparison of $\phi$ meson (a) $v_2$ and (b) $v_2/(\epsilon N_{part}^{1/3})$ measured as a function of $p_T$ in Cu+Au collisions at $\sqrt{s}$ = 200 GeV and U+U collisions at $\sqrt{s}$ = 193 GeVat midrapidity (|η| < 0.35)

The comparison of elliptic flow (a) $v_2$ values measured for $\phi$ mesons as a function of $p_T$ in $0\%–20\%$ Cu+Au collisions

The comparison of elliptic flow (b) $v_2$ values measured for $\phi$ mesons as a function of $KE_T$ in $0\%–20\%$ Cu+Au collisions

The comparison of elliptic flow (c) $v_2/n_q$ values measured for $\phi$ mesons as a function of $KE_T/n_q$ in $0\%–20\%$ Cu+Au collisions

The comparison of elliptic flow (a) $v_2$ values measured for $\phi$ mesons as a function of $p_T$ in $20\%–60\%$ Cu+Au collisions

The comparison of elliptic flow (b) $v_2$ values measured for $\phi$ mesons as a function of $KE_T$ in $20\%–60\%$ Cu+Au collisions

The comparison of elliptic flow (c) $v_2/n_q$ values measured for $\phi$ mesons as a function of $KE_T/n_q$ in $20\%–60\%$ Cu+Au collisions

The comparison of elliptic flow (a) $v_2$ values measured for $\phi$ mesons as a function of $p_T$ in $0\%–50\%$ U+U collisions

The comparison of elliptic flow (b) $v_2$ values measured for $\phi$ mesons as a function of $KE_T$ in $0\%–50\%$ U+U collisions

The comparison of elliptic flow (c) $v_2/n_q$ values measured for $\phi$ mesons as a function of $KE_T/n_q$ in $0\%–50\%$ U+U collisions

Centrality dependence of (a) $v_2${2} and (b) $v_2${4}. (a) The red points indicate no pseudorapidity gap whereas the magenta points indicate a pseudorapidity gap of |$\Delta\eta$| > 2.0. (b) The black points indicate $v_2${4} with no pseudorapidity gap, the blue points indicate a two-subevent method with |$\Delta\eta$| > 2.0 but where some short-range pairs are allowed, and the red points indicate a two-subevent method with |$\Delta\eta$| > 2.0 where no short-range pairs are allowed.

Centrality dependence of (a) $v_2${2} and (b) $v_2${4}. (a) The red points indicate no pseudorapidity gap whereas the magenta points indicate a pseudorapidity gap of |$\Delta\eta$| > 2.0. (b) The black points indicate $v_2${4} with no pseudorapidity gap, the blue points indicate a two-subevent method with |$\Delta\eta$| > 2.0 but where some short-range pairs are allowed, and the red points indicate a two-subevent method with |$\Delta\eta$| > 2.0 where no short-range pairs are allowed.

Multi-particle $v_2$ as a function of centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The magenta open diamonds indicate the $v_2${SP }, the blue open squares indicate $v_2${4}, the black open circles indicate $v_2${6}, and the green filled diamonds indicate $v_2${8}.

Multi-particle $v_2$ as a function of centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The magenta open diamonds indicate the $v_2${SP }, the blue open squares indicate $v_2${4}, the black open circles indicate $v_2${6}, and the green filled diamonds indicate $v_2${8}.

Multi-particle $v_2$ as a function of centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The magenta open diamonds indicate the $v_2${SP }, the blue open squares indicate $v_2${4}, the black open circles indicate $v_2${6}, and the green filled diamonds indicate $v_2${8}.

Multi-particle $v_2$ as a function of centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The magenta open diamonds indicate the $v_2${SP }, the blue open squares indicate $v_2${4}, the black open circles indicate $v_2${6}, and the green filled diamonds indicate $v_2${8}.

Cumulant method estimate of $\sigma_{v_{2}}$ / $\langle v_{2} \rangle$ as a function of centrality in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. The data are shown as black open squares. The same calculation as done in data is done in ampt, shown as a solid green line. Calculations of $\sigma_{\epsilon_{2}}$ /$ \langle\epsilon_{2}\rangle$ performed in the Monte Carlo Glauber model are shown as blue lines. The solid blue line is the Monte Carlo Glauber calculation done using the same estimate as the data, the dashed blue line is the direct calculation of the moments of the MC Glauber $\epsilon_{2}$ distribution.

Centrality dependence of $v_3${2, |$\Delta\eta$| > 2} in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, shown as magenta diamonds. The systematic uncertainty is indicated as a shaded magenta band. Also shown as black squares are $\sqrt{\langle v^{2}_{3}\rangle}$ as determined from the folding analysis, which is shown in the next section.

Centrality dependence of $v_3${2, |$\Delta\eta$| > 2} in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV, shown as magenta diamonds. The systematic uncertainty is indicated as a shaded magenta band. Also shown as black squares are $\sqrt{\langle v^{2}_{3}\rangle}$ as determined from the folding analysis, which is shown in the next section.

Centrality dependence of $c_3${4} for Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. (a) Calculations using both arms: $c_3${4} (black circles), $c_3${4}$_{ab|ab}$ (blue diamonds), $c_3${4}$_{aa|bb}$ (red squares), and comparison to STAR [36] (black stars). (b) Comparison of $c_3${4} determined using both arms (open symbols) and a single arm (closed symbols). Note that the open black circles are the same in (a) and (b).

Centrality dependence of $c_3${4} for Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. (a) Calculations using both arms: $c_3${4} (black circles), $c_3${4}$_{ab|ab}$ (blue diamonds), $c_3${4}$_{aa|bb}$ (red squares), and comparison to STAR [36] (black stars). (b) Comparison of $c_3${4} determined using both arms (open symbols) and a single arm (closed symbols). Note that the open black circles are the same in (a) and (b).

Centrality dependence of $c_3${4} for Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV. (a) Calculations using both arms: $c_3${4} (black circles), $c_3${4}$_{ab|ab}$ (blue diamonds), $c_3${4}$_{aa|bb}$ (red squares), and comparison to STAR [36] (black stars). (b) Comparison of $c_3${4} determined using both arms (open symbols) and a single arm (closed symbols). Note that the open black circles are the same in (a) and (b).

Folding results for (a) $v_2$, (b) $\sigma_{v_{2}}$ , and (c) $\sigma_{v_{2}}$ / $\langle v_{2}\rangle$. The black lines above and below the points indicate the systematic uncertainties. The red (green) boxes indicate the statistical uncertainties at the 68.27% (95.45%) confidence level. In the case of $\langle v_{2}\rangle$, the statistical uncertainties at the 68.27% confidence level are too small to be seen, and the uncertainties at the 95.45% confidence level are visible but noticeably smaller than the marker size. Shown as blue squares are the same quantities as determined using the cumulant based calculation—these points are slightly offset in the x-coordinate to improve visibility.

Folding results for (a) $v_2$, (b) $\sigma_{v_{2}}$ , and (c) $\sigma_{v_{2}}$ / $\langle v_{2}\rangle$. The black lines above and below the points indicate the systematic uncertainties. The red (green) boxes indicate the statistical uncertainties at the 68.27% (95.45%) confidence level. In the case of $\langle v_{2}\rangle$, the statistical uncertainties at the 68.27% confidence level are too small to be seen, and the uncertainties at the 95.45% confidence level are visible but noticeably smaller than the marker size. Shown as blue squares are the same quantities as determined using the cumulant based calculation—these points are slightly offset in the x-coordinate to improve visibility.

Folding results for (a) $v_2$, (b) $\sigma_{v_{2}}$ , and (c) $\sigma_{v_{2}}$ / $\langle v_{2}\rangle$. The black lines above and below the points indicate the systematic uncertainties. The red (green) boxes indicate the statistical uncertainties at the 68.27% (95.45%) confidence level. In the case of $\langle v_{2}\rangle$, the statistical uncertainties at the 68.27% confidence level are too small to be seen, and the uncertainties at the 95.45% confidence level are visible but noticeably smaller than the marker size. Shown as blue squares are the same quantities as determined using the cumulant based calculation—these points are slightly offset in the x-coordinate to improve visibility.

Folding results for (a) $\langle v_{3}\rangle$, (b) $\sigma_{v_{3}}$ , and (c) $\sigma_{v_{3}}$ /$\langle v_{3}\rangle$. The black lines above and below the points indicate the systematic uncertainties. The red (green) boxes indicate the statistical uncertainties at the 68.27% (95.45%) confidence level. The $\sigma_{v_{3}}$ /$\langle v_{3}\rangle$ values are all ≈ 0.52, the apparent limiting value of this quantity for the Bessel-Gaussian distribution.

Folding results for (a) $\langle v_{3}\rangle$, (b) $\sigma_{v_{3}}$ , and (c) $\sigma_{v_{3}}$ /$\langle v_{3}\rangle$. The black lines above and below the points indicate the systematic uncertainties. The red (green) boxes indicate the statistical uncertainties at the 68.27% (95.45%) confidence level. The $\sigma_{v_{3}}$ /$\langle v_{3}\rangle$ values are all ≈ 0.52, the apparent limiting value of this quantity for the Bessel-Gaussian distribution.

Folding results for (a) $\langle v_{3}\rangle$, (b) $\sigma_{v_{3}}$ , and (c) $\sigma_{v_{3}}$ /$\langle v_{3}\rangle$. The black lines above and below the points indicate the systematic uncertainties. The red (green) boxes indicate the statistical uncertainties at the 68.27% (95.45%) confidence level. The $\sigma_{v_{3}}$ /$\langle v_{3}\rangle$ values are all ≈ 0.52, the apparent limiting value of this quantity for the Bessel-Gaussian distribution.

Signal-to-background (S/B) ratio as a function of transverse momentum, Au+Au 62.4 GeV, 0-60% central events with minimum bias trigger

Inclusive electron elliptic flow v2\{2\} as a function of transverse momentum, Au+Au 200 GeV, 0-60% central events with minimum bias trigger

Inclusive electron elliptic flow v2\{4\} as a function of transverse momentum, Au+Au 200 GeV, 0-60% central events with minimum bias trigger

Inclusive electron elliptic flow v2\{2\} as a function of transverse momentum, Au+Au 39 GeV, 0-60% central events with minimum bias trigger

Inclusive electron elliptic flow v2\{2\} as a function of transverse momentum, Au+Au 62.4 GeV, 0-60% central events with minimum bias trigger

Inclusive electron elliptic flow v2\{2\} as a function of transverse momentum, Au+Au 200 GeV, 0-60% central events with High Tower (high pT) trigger

Photonic electron elliptic flow v2 as a function of transverse momentum, Au+Au 39 GeV, 0-60% central events with minimum bias trigger

Photonic electron elliptic flow v2 as a function of transverse momentum, Au+Au 62.4 GeV, 0-60% central events with minimum bias trigger

Photonic electron elliptic flow v2 as a function of transverse momentum, Au+Au 200 GeV, 0-60% central events with minimum bias trigger

Elliptic flow v2\{2\} of electrons from heavy-flavor hadron decays, Au+Au 200 GeV, 0-60% central events with minimum bias trigger

Elliptic flow v2\{4\} of electrons from heavy-flavor hadron decays, Au+Au 200 GeV, 0-60% central events with minimum bias trigger

Elliptic flow v2\{2\} of electrons from heavy-flavor hadron decays, Au+Au 200 GeV, 0-60% central events with High Tower (high pT) trigger

Elliptic flow v2\{EP\} of electrons from heavy-flavor hadron decays, Au+Au 200 GeV, 0-60% central events with High Tower (high pT) trigger

Elliptic flow v2\{2\} of electrons from heavy-flavor hadron decays, Au+Au 39 GeV, 0-60% central events with minimum bias trigger

Elliptic flow v2\{2}\ of electrons from heavy-flavor hadron decays, Au+Au 62.4 GeV, 0-60% central events with minimum bias trigger

$p_T$ dependence of $v_2$ for charged hadrons for several centrality selections as indicated.

$p_T$ dependence of $v_4$ for charged hadrons for several centrality selections as indicated.

$v_2$ vs. $N_{part}$ and $v_4$ vs. $N_{part}$ for charged hadrons for several $p_T$ selections as indicated.

The ratio ${v_4}/{(v_2)^2}$ vs. $N_{part}$ for the same $p_T$ selections.

Charged hadron $v_2$($p_T$) in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the two-particle cumulant method, the BBC event plane, and the ZDC-SMD event plane for the indicated centralities.

Charged hadron $v_2$($p_T$) in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the two-particle cumulant method, the BBC event plane, and the ZDC-SMD event plane for the indicated centralities.

Charged hadron $v_2$($p_T$) in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the two-particle cumulant method, the BBC event plane, and the ZDC-SMD event plane for the indicated centralities.

Charged hadron $v_2$($p_T$) in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the two-particle cumulant method, the BBC event plane, and the ZDC-SMD event plane for the indicated centralities.

Charged hadron $v_2$($p_T$) in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the two-particle cumulant method, the BBC event plane, and the ZDC-SMD event plane for the indicated centralities.

Charged hadron $v_2$($p_T$) in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the two-particle cumulant method, the BBC event plane, and the ZDC-SMD event plane for the indicated centralities.

Charged hadron $v_2$($p_T$) in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the two-particle cumulant method, the BBC event plane, and the ZDC-SMD event plane for the indicated centralities.

Charged hadron $v_2$($p_T$) in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the two-particle cumulant method, the BBC event plane, and the ZDC-SMD event plane for the indicated centralities.

Charged hadron $v_2$($p_T$) in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the two-particle cumulant method, the BBC event plane, and the ZDC-SMD event plane for the indicated centralities.

Charged hadron $v_2$($p_T$) in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the two-particle cumulant method, the BBC event plane, and the ZDC-SMD event plane for the indicated centralities.

Charged hadron $v_2$($p_T$) in Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV from the two-particle cumulant method, the BBC event plane, and the ZDC-SMD event plane for the indicated centralities.

Anisotropy parameter $v_2$ as a function of pseudorapidity within the PHENIX central arms using event planes from the BBC and ZDC-SMD, and from the two-particle cumulant method for centrality 20–40%. The results are shown for three $p_T$ bins, which are from top to bottom: 2.0–3.0, 1.2–1.4 and 0.6–0.8 GeV/$c$.

Comparison of the $v_2${BBC} and $v_2${ZDC-SMD} obtained from the S-N and ZDC-BBC-CNT subevents as a function of pT in the 20–60% centrality range.

Charged hadron $v_2${2} for the PHENIX experiment as a function of $p_T$ in centrality 20–60%.

The PHENIX $v_2${BBC} and $v_2${ZDC-SMD} from the modified event-plane method for charged hadrons as a function of $p_T$ in different centralities.

The PHENIX $v_2${BBC} and $v_2${ZDC-SMD} from the modified event-plane method for charged hadrons as a function of $p_T$ in different centralities.

The PHENIX $v_2${BBC} and $v_2${ZDC-SMD} from the modified event-plane method for charged hadrons as a function of $p_T$ in different centralities.

The PHENIX $v_2${BBC} and $v_2${ZDC-SMD} from the modified event-plane method for charged hadrons as a function of $p_T$ in different centralities.

The PHENIX $v_2${BBC} and $v_2${ZDC-SMD} from the modified event-plane method for charged hadrons as a function of $p_T$ in different centralities.

The PHENIX $v_2${BBC} and $v_2${ZDC-SMD} from the modified event-plane method for charged hadrons as a function of $p_T$ in different centralities.

$m^2$ (signal+background) distribution for $\bar{d}$,$d$ for $p_T$ = 1.6-2.9 GeV/$c$.

$m^2$ (background) distribution for $\bar{d}$,$d$ for $p_T$ = 1.6-2.9 GeV/$c$.

$m^2$ (signal) distribution for $\bar{d}$,$d$ for $p_T$ = 1.6-2.9 GeV/$c$.

Comparison of differential $v_2(p_T)$ for $\pi^{\pm}$. Results are shown for 20-60% central Au+Au collisions.

Comparison of differential $v_2(p_T)$ for $K^{\pm}$. Results are shown for 20-60% central Au+Au collisions.

Comparison of differential $v_2(p_T)$ for $(\bar{p})p$. Results are shown for 20-60% central Au+Au collisions.

Comparison of differential $v_2(p_T)$ for $\phi$ mesons. Results are shown for 20-60% central Au+Au collisions.

Comparison of differential $v_2(p_T)$ for $(\bar{d})d$. Results are shown for 20-60% central Au+Au collisions.

$v_2$ vs $KE_T$ for several identified particle species obtained in mid-central Au+Au collisions, and ${v_2}/{n_q}$ vs ${KE_T}/{n_q}$ for the same particle species.

$v_2$ vs $KE_T$ for several identified particle species obtained in mid-central Au+Au collisions, and ${v_2}/{n_q}$ vs ${KE_T}/{n_q}$ for the same particle species.

$v_2$ vs $KE_T$ for several identified particle species obtained in mid-central Au+Au collisions, and ${v_2}/{n_q}$ vs ${KE_T}/{n_q}$ for the same particle species.

$v_2$ vs $KE_T$ for several identified particle species obtained in mid-central Au+Au collisions, and ${v_2}/{n_q}$ vs ${KE_T}/{n_q}$ for the same particle species.

$v_2$ vs $KE_T$ for several identified particle species obtained in mid-central Au+Au collisions, and ${v_2}/{n_q}$ vs ${KE_T}/{n_q}$ for the same particle species.

$v_2$ vs $KE_T$ for several identified particle species obtained in mid-central Au+Au collisions, and ${v_2}/{n_q}$ vs ${KE_T}/{n_q}$ for the same particle species.

$v_2$ vs $KE_T$ for several identified particle species obtained in mid-central Au+Au collisions, and ${v_2}/{n_q}$ vs ${KE_T}/{n_q}$ for the same particle species.

$v_2$ vs $KE_T$ for several identified particle species obtained in mid-central Au+Au collisions, and ${v_2}/{n_q}$ vs ${KE_T}/{n_q}$ for the same particle species.

$v_2$ vs $KE_T$ for several identified particle species obtained in mid-central Au+Au collisions, and ${v_2}/{n_q}$ vs ${KE_T}/{n_q}$ for the same particle species.

$v_2$ vs $KE_T$ for several identified particle species obtained in mid-central Au+Au collisions, and ${v_2}/{n_q}$ vs ${KE_T}/{n_q}$ for the same particle species.

$v_2$ vs $p_T$ for identified particle species obtained in minimum bias Au+Au collisions.

$v_2$ vs $p_T$ for identified particle species obtained in minimum bias Au+Au collisions.

$v_2$ vs $p_T$ for identified particle species obtained in minimum bias Au+Au collisions.

$v_2$ vs $KE_T$ for identified particle species obtained in minimum bias Au+Au collisions.

$v_2$ vs $KE_T$ for identified particle species obtained in minimum bias Au+Au collisions.

$v_2$ vs $KE_T$ for identified particle species obtained in minimum bias Au+Au collisions.

${v_2}/{n_q}$ vs ${p_T}/{n_q}$ for identified particle species obtained in minimum bias Au+Au collisions.

${v_2}/{n_q}$ vs ${p_T}/{n_q}$ for identified particle species obtained in minimum bias Au+Au collisions.

${v_2}/{n_q}$ vs ${p_T}/{n_q}$ for identified particle species obtained in minimum bias Au+Au collisions.

${v_2}/{n_q}$ vs ${KE_T}/{n_q}$ for identified particle species obtained in minimum bias Au+Au collisions.

${v_2}/{n_q}$ vs ${KE_T}/{n_q}$ for identified particle species obtained in minimum bias Au+Au collisions.

${v_2}/{n_q}$ vs ${KE_T}/{n_q}$ for identified particle species obtained in minimum bias Au+Au collisions.

Charged hadron v2 for the centrality bin 0-50%.

v2(4) vs. p_T for pions for 20 - 60% centrality

v2(4) vs. p_T for kaons for 20 - 60% centrality

v2(4) vs. p_T for anti-protons for 20 - 60% centrality

v2(2) vs. centrality for pions

v2(2) vs. centrality for kaons

v2(2) vs. centrality for anti-protons

v2 vs. p_T for particles identified in the RICH (min. bias) for pions+kaons and protons/antiprotons

v2 for Kshort for min. bias

v2 for kaons from kinks for min. bias

v2 for kaons from dE/dx for min. bias

v2 for Lambda+Lambdabar for min. bias [PRL/92/052302/2004]. The PHENIX data are from [PRL/91/182301/2003]. The hydro calculations are from [P. Huovinen/private communication].

v2 for charged pions for min. bias. kaon data points are from Figure 9.

v2 for anti-protons for min. bias. kaon data points are from Figure 9.

Azimuthal correlations (\sum_i cos(2(\phi_pT -\phi_i))) in Au+Au collisions as a function of p_T along with results from p+p collisions.

Azimuthal correlations (\sum_i cos(2(\phi_pT -\phi_i))) from d+Au as a function of p_T for min bias collisions.

Azimuthal correlations (\sum_i cos(2(\phi_pT -\phi_i))) from d+Au as a function of p_T for three centralities.

Charged hadron v2 and v4{EP_2} as a function of pseudorapidity for minimum bias.

v2(2) and v2(4) vs. pseudorapidity

v2(2) and v2(4) vs. pseudorapidity,FTPC only

v2(4) 20-70% in TPC+FTPC and v2(2) 20-70% in FTPC.

MC v2 with FTPC momentum resolution.

Charged hadron v2 for the centrality bin 0-5% in standard and modified event plane methods.

Charged hadron v2 for the centrality bin 5-10% in standard and modified event plane methods.

Charged hadron v2 for the centrality bin 10-20% in standard and modified event plane methods.

Charged hadron v2 for the centrality bin 20-30% in standard and modified event plane methods.

Charged hadron v2 for the centrality bin 30-40% in standard and modified event plane methods.

Charged hadron v2 for the centrality bin 40-60% in standard and modified event plane methods.

Charged hadron v2{2} from modified reaction plane method and two-particle cumulant results (after subtracting the correlations measured in p+p collisions) for centrality bin 20-60% .

v4(EP2) for charged hadrons min. bias

v4(EP2) vs. centrality for charged hadrons

v4(EP2) for pions in min. bias

v4(EP2) for protons in min. bias

v4(EP2) for kaons in min. bias

v4(EP2) for Lambda in min. bias

Charged hadron v4{EP_2} as a function of pseudorapidity for minimum bias (TPC only).

charged hadrons high p_T (3 - 6 GeV/c) v4(3)

charged hadron integrated v2 as a function of centrality for the different methods

charged hadron v2(6) vs. centrality bin. v2(2) and v2(4) are from Figure 29(a).

g2 as a function of centrality from 200 GeV, 130 GeV,NA49 and q-dist methods. The solid points are from the cumulant method, while open circles are from the q distribution method. Please note that centrality percentage differs from different method. For 200 GeV-cumulant (0, 64.1, 53.9,44.7,35.2,25.4,15.1,7.7,0), for 200 GeV-q-dist (73.8,64.1,53.9,44.7,35.2,25.4,15.1,7.7,2.3), for 130 GeV (65,47,36,27.5,20,13,7.5,2.5,0) and for 17 GeV (0,0,0,61.2,38.2,29.1,18.2,8.5,3.8).

wounded nucleons as a function of centrality from 200 GeV, 130 GeV,NA49 and q-dist methods.Please note that centrality percentage differs from different method. For 200 GeV-cumulant (0, 64.1, 53.9,44.7,35.2,25.4,15.1,7.7,0), for 200 GeV-q-dist (73.8,64.1,53.9,44.7,35.2,25.4,15.1,7.7,2.3), for 130 GeV (65,47,36,27.5,20,13,7.5,2.5,0) and for 17 GeV (0,0,0,61.2,38.2,29.1,18.2,8.5,3.8).

v2/n for pions for three centrality bins

v2/n for protons for three centrality bins

v2/n for Kshort for three centrality bins

v2/n for Lambda + Lambda bar for three centrality bins

Blast Wave parameters rho_2 from pion v2(2),pion v2 and hadron v2

Blast Wave parameters rho_4 from hadron v2

Blast Wave parameters epsilon from pion v2(2),pion v2, hadron v2 and initial

Blast Wave parameters rho_0 from pion v2(2),pion v2 and hadron v2

Blast Wave parameters T from pion v2(2),pion v2 and hadron v2