$dN/dy$ 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 $p$ $R_{CP}$.

The measured reduced neutral current charm cross sections and structure functions obtained using the NLO QCD fit correct for FL.

The measured reduced neutral current bottom cross sections and structure functions obtained using the NLO QCD fit correct for FL.

The measured reduced neutral current bottom cross sections and structure functions obtained using the NLO QCD fit correct for FL.

The measured charm fractional contribution to the neutral current total cross section.

The measured charm fractional contribution to the neutral current total cross section.

The measured bottom fractional contribution to the neutral current total cross section.

The measured bottom fractional contribution to the neutral current total cross section.

Two-particle CI joint autocorrelations $\widehat{N}(\widehat{r}-1)$ on $(\eta_{\Delta}, \phi_{\Delta})$ for peripheral collisions.

HBT parameters for the three possible fitting procedures to the correlation functions described in this paper depending on how Coulomb interaction is taken into account from the 0-5% most central events.

HBT parameters for the three possible fitting procedures to the correlation functions described in this paper depending on how Coulomb interaction is taken into account from the 0-5% most central events.

HBT parameters for the three possible fitting procedures to the correlation functions described in this paper depending on how Coulomb interaction is taken into account from the 0-5% most central events.

HBT parameters for the three possible fitting procedures to the correlation functions described in this paper depending on how Coulomb interaction is taken into account from the 0-5% most central events.

1D correlation function for pi+pi- compared to standard, Bowler-Sinyukov, and a thoretical calculation that includes Coulomb and strong interactions.

Momentum resolution for pions at midrapidity expressed by the widths dp_T/p_T, dphi and dtheta as a function of p.

Squared HBT radii relative to the reaction plane angle, without and with the reaction plane resolution applied, for two different centrality-kT ranges. 20-30%, 0.15 < kT < 0.25, RP uncorrected.

Squared HBT radii relative to the reaction plane angle, without and with the reaction plane resolution applied, for two different centrality-kT ranges. 20-30%, 0.15 < kT < 0.25, RP res. corrected.

Squared HBT radii relative to the reaction plane angle, without and with the reaction plane resolution applied, for two different centrality-kT ranges. 10-20%, 0.35 < kT < 0.45, RP uncorrected.

Squared HBT radii relative to the reaction plane angle, without and with the reaction plane resolution applied, for two different centrality-kT ranges. 10-20%, 0.35 < kT < 0.45, RP res. uncorrected.

Squared HBT radii relative to the reaction plane angle, for the case where the lambda parameter is averaged and fixed in the fit, and the case where lambda is a free fit parameter for each Phi. 20-30%, 0.15 < kT < 0.25, fixed lambda.

Squared HBT radii relative to the reaction plane angle, for the case where the lambda parameter is averaged and fixed in the fit, and the case where lambda is a free fit parameter for each Phi. 20-30%, 0.15 < kT < 0.25, lambda varied.

Squared HBT radii relative to the reaction plane angle, for the case where the lambda parameter is averaged and fixed in the fit, and the case where lambda is a free fit parameter for each Phi. 10-20%, 0.35 < kT < 0.45, lambda fixed.

Squared HBT radii relative to the reaction plane angle, for the case where the lambda parameter is averaged and fixed in the fit, and the case where lambda is a free fit parameter for each Phi. 10-20%, 0.35 < kT < 0.45, lambda varied.

Fourier coefficients as a function of the maximum fraction of merged hits for the 5% most central events and kT between 150 and 250 MeV/c.

Projections of the 3 dimensional correlation function and fits to Eq. (10) and with the Edgeworth expansion to Eq. (17) to 6th order.

HBT parameters for the 0-5% most central events for fits to Eq. (10) and to Eq. (17) with no expansion.

HBT parameters for the 0-5% most central events for fits to Eq. (10) and to Eq. (17) upto 4th order expansion.

HBT parameters for the 0-5% most central events for fits to Eq. (10) and to Eq. (17) upto 6th order expansion.

HBT parameters for the 0-5% most central events for pi+pi+ and pi-pi- correlation functions.

HBT parameters from STAR and PHENIX at the same beam energy for the 0-30% most central events.

Energy dependence of the pi- HBT parameters for central Au+Au, Pb+Pb, and Pb+Au collisions at midrapidity and k_T ~ 0.2 GeV/c.

HBT parameters vs. m_T for 6 different centralities.

Fourier coefficients of azimuthal oscillations of HBT radii vs. numer of participating nucleons, for pi+ and pi- pairs separately (0.25 < kT < 0.35 GeV/c).

Comparison between the HBT radii obtained from the azimuthally integrated (traditional) HBT analysis and the 0th-order Fourier coefficients from the azimuthally-sensitive HBT analysis.

HBT radius parametres for 6 different centralities.

Extracted parameters R' and alpha, from the power-law fits to the HBT radius parameters.

Extracted freeze-out source radius extracted from a blast wave fit; source radius Rgeom from fits to Rside; and 2*Rside for the lowest k_T bin as a function of the number of participants.

HBT parameter Rside.

R - Rinitial (top panel) and R/Rinitial (bottom panel) for the azimuthally integrated analysis for the azimuthally-sensitive case vs. number of participants.

R - Rinitial (top panel) and R/Rinitial (bottom panel) for in the x (in-plane) and y (out-of-plane) directions for the azimuthally-sensitive case vs. number of participants.

R - Rinitial for the azimuthally integrated analysis for the azimuthally-sensitive case vs. (dN/dy)/Rinitial.

R - Rinitial in the x (in-plane) direction for the azimuthally-sensitive case vs. (dN/dy)/Rinitial.

R - Rinitial in the y (out-of-plane) direction for the azimuthally-sensitive case vs. (dN/dy)/Rinitial.

Longitudinal HBT radius Rl.

Evolution time tau vs. number of participants as extracted from a fit to Rl, lines in Fig. 26 (triangles), and from a blast wave fit to HBT parameters and spectra (circles).

R - Rinital for the azimuthally integrated analysis and for the in-plane and out-of-plane directions vs. beta_T,max*tau.

R - Rinital for the azimuthally integrated analysis and for the in-plane and out-of-plane directions vs. beta_T,max*tau.

R - Rinital for the azimuthally integrated analysis and for the in-plane and out-of-plane directions vs. beta_T,max*tau.

Emission duration time dTau vs. number of participants as extracted using a blast wave fit to HBT parameters and spectra.

Final source eccentricity as calculated from the Fourier coefficients (2R_{s,2}^2/R_{s,0}^2) and from the final in-plane and out-of-plane radii vs. initial eccentricity.

Differential anisotropy $v_2$($p_T$) for charged hadrons in Au + Au collisions at $\sqrt{s_{NN}}$ = 200 GeV obtained via reaction plane methods

Differential anisotropy as a function of centrality for $\sqrt{s_{NN}}$ = 62.4 GeV/$c$

Differential anisotropy as a function of centrality for $\sqrt{s_{NN}}$ = 130 GeV/$c$

Differential anisotropy as a function of centrality for $\sqrt{s_{NN}}$ = 200 GeV/$c$

Differential anisotropy $v_2$($p_T$) for centrality selection 13 - 26%.

Differential anisotropy $v_2$($p_T$) for centrality selection 13 - 26%.

Differential $v_2$ vs. $\sqrt{S_{NN}}$ for charged hadrons in nucleus-nucleus collisions. Results are shown for the centrality cut of 13 - 26% and $p_T$ selections of 1.75 GeV/$c$ and 0.65 GeV/$c$.

$R_{cp}$ as a function of $\eta$ for 1.5 < $p_T$ < 4.0 GeV/$c$ for different centrality classes. Systematic uncertainties which are point-to-point uncorrelated (sys-uncorr) and correlated (sys-corr) are shown.

Inclusive differential cross sections for bottom-hadron produced and prompt J/PSIs times branching ratio (5.88+-0.10PCT) into mu+mu- at a centre-of-mass enrgy 1960 GeV.

Total inclusive single b-hadron cross section.

Differential cross section distribution of b-hadron production as a function of b-hadron transverse momenta.. Errors are the total errors.