  Lattice power-counting is extended to QCD with staggered fermions. As
preparation, the difficulties encountered by Reisz's original formulation of
the lattice power-counting theorem are illustrated. One of the assumptions that
is used in his proof does not hold for staggered fermions, as was pointed out
long ago by Luscher. Finally, I generalize the power-counting theorem, and the
methods of Reisz's proof, such that the difficulties posed by staggered
fermions are overcome.
