Thermal quark production in pure glue and quark gluon plasmas

Abstract

We calculate production rates for massless $(u,d)$ and massive $(s,c,b)$ quarks in pure glue and quark gluon plasmas to leading order in the strong coupling constant $g$. The leading contribution comes from gluon decay into $q\bar{q}$ pairs, using a thermal gluon propagator with finite thermal mass and damping rate. The rate behaves as ${\alpha }_S^2(\ln 1/{\alpha }_S{)}^2{T}^4$ when $m,{\alpha }_S\to 0$ and depends linearly on the transverse gluon damping rate for all values of the quark mass $m$. The light quark ($u$, $d$, $s$) chemical equilibration time is approximately 10-100 $T^{-1}$ for $g=$2-3, so that quarks are likely to remain far from chemical equilibrium in ultrarelativistic nuclear collisions.

Comments: 7 pages, 5 figures (available upon request), CERN preprint CERN-TH-6882/93