We reexamine the scenario of homogeneous nucleation of the quark-gluon
plasma produced in ultra-relativistic heavy ion collisions. A general
ization of the standard nucleation theory to rapidly expanding system
is proposed. The nucleation rate is derived via the new scaling parame
ter lambda(Z). It is shown that the size distribution of hadronic clus
ters plays an important role in the dynamics of the phase transition.
The longitudinally expanding system is supercooled to about 3-6%, then
it is reheated, and the hadronization is completed within 6-10 fm/c,
i.e. 5-10 times faster than it was estimated earlier, in a strongly no
nequilibrium way. (C) 1998 Elsevier Science B.V.