For a high temperature non-Abelian plasma, we reformulate the hard the
rmal loop approximation as an effective classical thermal field theory
for the soft modes. The effective theory is written in local Hamilton
ian form, and the thermal partition function is explicitly constructed
. It involves an ultraviolet cutoff which separates between hard and s
oft degrees of freedom in a gauge-invariant way, together with counter
terms which cancel the cutoff dependence in the soft correlation funct
ions. The effective theory is well suited for numerical studies of the
non-perturbative dynamics in real time, in particular, for the comput
ation of the baryon number violation rate at high temperature. (C) 199
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