The Onsager-reaction-field correction to Hartree-Fock theory recently
derived by Georges and Yedidia [Phys. Rev. B 43, 3475 (1991)] is evalu
ated analytically for the half-filled positive-U Hubbard model on a d-
dimensional hypercubic lattice. It is shown that the Onsager correctio
n is for all d greater-than-or-equal-to 3 irrelevant in the weak-coupl
ing limit, while for d = 1 and d = 2 it strongly renormalizes the Hart
ree-Fock result, although it does not completely destabilize the spin-
density wave. We examine the perturbation theory for the energy change
induced by a small staggered magnetization m to all orders in U, and
show that one obtains an infinite series in powers of (U/t)ln[m-1ln(m-
1)] for d = 1, and in powers of (U/t)ln2[m-1ln2(m-1)] for d = 2. The c
lose similarity between d = 1 and d = 2 is interpreted as evidence tha
t antiferromagnetism in the weak coupling regime is not stable in d =
2.