e+e- production cross section at mid rapidity for ultra peripheral Au+Au reactions.The results are given for 3 intervals of masses of the electron pair : 2.0 to 2.3, 2.3 to 2.8 and 2.0 to 2.8 Gev/c2.

Invariant cross section of electrons from charm decay versus PT These values has been obtained using g3data software which to extract the data from the plot and should therefore be used with caution. The values in the last column indicate the level of uncertainty intoduced by g3data.

Invariant cross section of electrons from bottom decay versus PT These values has been obtained using g3data software which to extract the data from the plot and should therefore be used with caution. The values in the last column indicate the level of uncertainty intoduced by g3data.

Total bottom cross section To obtain the total bottom cross section, the differential charm cross section has been extrapolated to the whole rapidity range, using a HVQMNR rapidity distribution with aCTEQ5M PDF.

direct $\gamma$-hadron yields per trigger p+p and Au+Au at 12<$p_{T}^{\gamma}$<15 GeV/c.

direct $\gamma$-hadron yields per trigger p+p and Au+Au at 5<$p_{T}^{\gamma}$<7 GeV/c.

direct $\gamma$-hadron yields per trigger p+p and Au+Au at 7<$p_{T}^{\gamma}$<9 GeV/c.

direct $\gamma$-hadron yields per trigger p+p and Au+Au at 9<$p_{T}^{\gamma}$<12 GeV/c.

direct $\gamma$-hadron yields per trigger p+p and Au+Au at 12<$p_{T}^{\gamma}$<15 GeV/c.

direct $\gamma$-hadron yields per trigger p+p and Au+Au at 5<$p_{T}^{\gamma}$<7 GeV/c.

direct $\gamma$-hadron yields per trigger p+p and Au+Au at 7<$p_{T}^{\gamma}$<9 GeV/c.

direct $\gamma$-hadron yields per trigger p+p and Au+Au at 9<$p_{T}^{\gamma}$<12 GeV/c.

direct $\gamma$-hadron yields per trigger p+p and Au+Au at 12<$p_{T}^{\gamma}$<15 GeV/c.

Ratio of $I_{AA}$ of Au+Au to p+p yields at 5<$p_{T}^{\gamma}$<7 GeV/c.

Ratio of $I_{AA}$ of Au+Au to p+p yields at 7<$p_{T}^{\gamma}$<9 GeV/c.

Ratio of $I_{AA}$ of Au+Au to p+p yields at 9<$p_{T}^{\gamma}$<12 GeV/c.

Ratio of $I_{AA}$ of Au+Au to p+p yields at 12<$p_{T}^{\gamma}$<15 GeV/c.

$I_{AA}(Z_T)$ for the 20% most central Au+Au data at 5<$p_{T}^{\gamma}$<7 GeV/c compared to predictions from an energy loss calculation.

$I_{AA}(Z_T)$ for the 20% most central Au+Au data at 7<$p_{T}^{\gamma}$<9 GeV/c compared to predictions from an energy loss calculation.

$I_{AA}(Z_T)$ for the 20% most central Au+Au data at 9<$p_{T}^{\gamma}$<12 GeV/c compared to predictions from an energy loss calculation.

$I_{AA}(Z_T)$ for the 20% most central Au+Au data at 12<$p_{T}^{\gamma}$<15 GeV/c compared to predictions from an energy loss calculation.

direct $\gamma$-hadron yields per trigger p+p at 5<$p_{T}^{\gamma}$<7 GeV/c.

direct $\gamma$-hadron yields per trigger p+p at 7<$p_{T}^{\gamma}$<9 GeV/c.

direct $\gamma$-hadron yields per trigger p+p at 9<$p_{T}^{\gamma}$<12 GeV/c.

direct $\gamma$-hadron yields per trigger p+p at 12<$p_{T}^{\gamma}$<15 GeV/c.

Rebinned $R_{AA}$ for $\Delta \phi$, $p_T$, and path length dependence,

HBT parameters for all centralities in 62.4 GeV Cu+Cu.

HBT parameters for all centralities in 200 GeV Cu+Cu.

HBT parameters for 200 GeV Au+Au, 0-5% and Cu+Cu, 0-10%

HBT parameters for 200 GeV and 62.4 GeV Cu+Cu, 0-10% and 62.4 GeV Au+Au, 0-5%

HBT radii for radii ratios in 200 GeV and 62.4 GeV Cu+Cu, 0-10% and 200 GeV & 62.4 GeV Au+Au, 0-5%. Note that on Figure 8 in the paper the radii ratios are shown while here we list the radii values.

Energy dependence of the pi- HBT Radii for Volume estimate (Rside*Rside*Rlong) in central Au+Au, Pb+Pb, and Pb+Au collisions (AGS,SPS and RHIC) at midrapidity and k_T ~ 0.2-0.3 GeV/c. Note that on Figure 9 in the paper Rside*Rside*Rlong is shown while here we list the Rside and Rlong values.

HBT Radii for Volume estimate(Rside*Rside*Rlong & Rout*Rout*Rlong) comparisons for 200 GeV and 62.4 GeV Au+Au with Npart and dNch/deta. Note that on Figure 10 in the paper specific combinations of the HBT radii are shown while here we list the radii values.

HBT Radii for Volume estimate(Rside*Rside*Rlong & Rout*Rout*Rlong) comparisons for 200 GeV and 62.4 GeV Au+Au & Cu+Cu with dNch/deta. Note that on Figure 11 in the paper specific combinations of the HBT radii are shown while here we list the radii values.

HBT radii comparisons for 200 GeV and 62.4 GeV Au+Au & Cu+Cu with dNch/deta1/3

Measured $C_2$($q_{inv}$) and restored $C_2$($q_{inv}$) from imaged $S(r)$, compared with angle-averaged Gaussian $C_2$($q_{inv}$) for charged kaon pairs measured for 0.3 < $k_T$ < 0.9 GeV/$c$ at 0-30% central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Measured $C_2$($q_{inv}$) and restored $C_2$($q_{inv}$) from imaged $S(r)$, compared with angle-averaged Gaussian $C_2$($q_{inv}$) for charged kaon pairs measured for 0.3 < $k_T$ < 0.9 GeV/$c$ at 0-30% central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Measured $C_2$($q_{inv}$) and restored $C_2$($q_{inv}$) from imaged $S(r)$, compared with angle-averaged Gaussian $C_2$($q_{inv}$) for charged kaon pairs measured for 0.3 < $k_T$ < 0.9 GeV/$c$ at 0-30% central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

Measured $C_2$($q_{inv}$) and restored $C_2$($q_{inv}$) from imaged $S(r)$, compared with angle-averaged Gaussian $C_2$($q_{inv}$) for charged kaon pairs measured for 0.3 < $k_T$ < 0.9 GeV/$c$ at 0-30% central Au+Au collisions at $\sqrt{s_{NN}}$ = 200 GeV.

PT distribution of the second jet in events with two or more jets.

PT distribution of the third jet in events with three or more jets with additional constraints on the electrons.

PT distribution of the third jet in events with three or more jets.

The P P --> P P X differential cross section as a function of the square ofthe missing mass (X) at incident beam energy of 2.0 GeV.