Abstract
Using the (lowest-order) perturbative QCD, we argue that high energy heavy ion collisions proceed as follows: (i) 0 < ρ < 0.3 fm/c entropy production, momenta equilibration due to gg → gg, qg → qg; (ii) 0.3 < ρ < 2. fm/c: gluon chemical equilibration due to gg → ng; (ii) 3 < ρ < ρc = 5-7 fm/c: expansion of gluonic plasma till formation of the 'mixed phase', or hadronization. Much higher initial temperatures are suggested, namely Ti = 400-500 MeV mat RHIC and Ti = 600-900 MeV at LHC. This leads to enhanced charm production and significant modifications of photon and dilepton production.
| Original language | English |
|---|---|
| Pages (from-to) | 559-562 |
| Number of pages | 4 |
| Journal | Nuclear Physics, Section A |
| Volume | 566 |
| Issue number | C |
| DOIs | |
| State | Published - Jan 3 1994 |
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