GLYPH<s48> GLYPH<s49> GLYPH<s50> GLYPH<s51> GLYPH<s52> GLYPH<s53> GLYPH<s49>GLYPH<s48> GLYPH<s45>GLYPH<s52> GLYPH<s49>GLYPH<s48> GLYPH<s45>GLYPH<s51> GLYPH<s49>GLYPH<s48> GLYPH<s45>GLYPH<s50> GLYPH<s49>GLYPH<s48> GLYPH<s45>GLYPH<s49> GLYPH<s49>GLYPH<s48> GLYPH<s48> GLYPH<s49>GLYPH<s48> GLYPH<s49> GLYPH<s49>GLYPH<s48> GLYPH<s50> GLYPH<s49>GLYPH<s48> GLYPH<s51> GLYPH<s32> GLYPH<s40> GLYPH<s50> GLYPH<s112> GLYPH<s84> GLYPH<s41> GLYPH<s45> GLYPH<s49> GLYPH<s32>GLYPH<s100> GLYPH<s50> GLYPH<s78> GLYPH<s47>GLYPH<s100> GLYPH<s121> GLYPH<s100> GLYPH<s112> GLYPH<s84> GLYPH<s32>GLYPH<s32> GLYPH<s91> GLYPH<s40> GLYPH<s71> GLYPH<s101> GLYPH<s86> GLYPH<s47>GLYPH<s99> GLYPH<s41> GLYPH<s45> GLYPH<s50> GLYPH<s93> GLYPH<s112> GLYPH<s84> GLYPH<s32>GLYPH<s40>GLYPH<s71>GLYPH<s101>GLYPH<s86>GLYPH<s47>GLYPH<s99>GLYPH<s41> GLYPH<s32> GLYPH<s100> GLYPH<s71> GLYPH<s61>GLYPH<s49>GLYPH<s54> GLYPH<s32> GLYPH<s100> GLYPH<s71> GLYPH<s61>GLYPH<s52>GLYPH<s48> GLYPH<s32> GLYPH<s80>GLYPH<s72>GLYPH<s79>GLYPH<s66>GLYPH<s79>GLYPH<s83>GLYPH<s32>GLYPH<s40>GLYPH<s48>GLYPH<s45>GLYPH<s54>GLYPH<s37> GLYPH<s41>GLYPH<s58>GLYPH<s32>GLYPH<s32>GLYPH<s40>GLYPH<s104> GLYPH<s43> GLYPH<s43>GLYPH<s104> GLYPH<s45> GLYPH<s41>GLYPH<s47>GLYPH<s50> FIG. 6: (Color online) Momentum spectrum for central collisions. the production rates R$_{gg}$$_{→}$$_{ggg}$ are almost the same in both cases, the chemical equilibration of the system with d$_{G}$ = 40 proceeds always behind the process in the system with d$_{G}$ = 16. The production of more particles from the same energy content leads to a smaller tem- perature at the (chemical) freeze-out. This clearly relates the softening of the transverse spectrum dN/ ( p$_{T}$dp$_{T}$dy ) shown in Fig. 6 as an example for most central collisions. Both re- sults of the mean transverse momenta and the transverse momentum spectrum come closer to the experimental data [31, 32], if the effective quark degrees of freedom are included into the parton cascade calculations. On the one hand, the p$_{T}$ averaged elliptic flow v$_{2}$ is almost unchanged, when enlarging d$_{G}$ from 16 to 40. On the other hand, the slope of the transverse momentum spectrum increases due to the production of more particles with larger d$_{G}$ . Thus, there must be a simultaneous change in the differential elliptic flow v$_{2}$ ( p$_{T}$ ), because v$_{2}$ = ∫ dp$_{T}$ v$_{2}$ ( p$_{T}$ ) dN/N/dp$_{T}$ . The change of v$_{2}$ ( p$_{T}$ ) is shown in Fig. 7 for the most central 50% collisions and in Fig. 8 for the mid-central class. The dotted curves are just the dashed curves times an effective factor, which enhances the p$_{T}$ averaged v$_{2}$ values of the calculations with d$_{G}$ = 40 to be equal with 12