  We show that in the lattice Hamiltonian limit the static transverse
propagator $D(|\vec{p}|)\propto\int d p_0 D(|\vec{p}|,p_0)$ satisfies
multiplicative renormalizability. We give a procedure to calculate
$D(|\vec{p}|)$ on available lattices at finite temporal spacing. The result
agrees at all momenta with the Gribov formula $D(|\vec{p}|)\propto(|\vec{p}|^2+
M^4 |\vec{p}|^{-2})^{-{1/2}}$, with $M=0.88(1) {\rm GeV} \simeq 2
\sqrt{\sigma}$.
