  The successive perturbative estimates of the pressure of QCD at high
temperature T show no sign of convergence, unless the coupling constant g is
unrealistically small. Exploiting known results of an effective field theory
which separates hard (order 2 pi T) and soft (order gT) contributions, we
explore the accuracy of simple resummations which at a given loop order
systematically treat hard contributions strictly perturbatively, but soft
contributions without truncations. This turns out to improve significantly the
two-loop and the three-loop results in that both remain below the ideal-gas
value, and the degree of renormalization scale dependence decreases as one goes
from two to three loop order, whereas it increases in the conventional
perturbative results. Including the four-loop logarithms recently obtained by
Kajantie et al., we find that this trend continues and that with a particular
sublogarithmic constant the untruncated four-loop result is close to the
three-loop result, which itself agrees well with available lattice results down
to temperatures of about 2.5 T_c. We also investigate the possibility of
optimization by using a variational (``screened'') perturbation theory in the
effective theory. At two loops, this gives a result below the ideal gas value,
and also closer to lattice results than the recent two-loop
hard-thermal-loop-screened result of Andersen et al. While at three-loop order
the gap equation of dimensionally reduced screened perturbation theory does not
have a solution in QCD, this is remedied upon inclusion of the four-loop
logarithms.
