We obtain a rigorous condition for the divergence of the staggered sus
ceptibility of the half filled Hubbard model in infinite dimensions by
differentiating the exact functional-integral equation for the local
Greens function with respect to a staggered magnetic field. In the wea
k-coupling regime, we make the reasonable assumption that the high tem
perature phase without broken symmetry is a Fermi liquid, and proof th
at the system develops long-range antiferromagnetic order at a finite
temperature.