Thermally reduced QCD leads to three dimensional SU(3) gaugefields coupled
to an adjoint scalar field A,. We compute the effective potential in the on
e-loop approximation and evaluate the VEVs of TrA(2)(0) and TrA(3)(0). In t
he Higgs phase not only the former, but also the latter has a VEV. This hap
pens where the SU(3) gauge symmetry is broken minimally with U(2) still unb
roken. The VEV of the cubic invariant breaks charge conjugation and CP. It
is plausible that in the Higgs phase one has a transition for large enough
Higgs selfcoupling to a region where TrA(3)(0) has no VEV and where the gau
gesymmetry is broken maximally to U(1) x U(1). For a number of colours larg
er than 3 an even richer phase structure is possible. (C) 1999 Elsevier Sci
ence B.V. All rights reserved. PACS: 78.60.Mq; 43.35. fd; 95.75.Kk; 25.75.G
z.