The electronic spectrum of the d-dimensional tight-binding Hubbard Mod
el is examined near the point of half filled bands, The electronic spe
ctrum is calculated by treating the longitudinal and transverse spin f
luctuations in the random phase approximation. For zero doping, a comm
ensurate anti-ferromagnetic structure is found to be stable. The elect
ronic structure shows the opening up of a gap at the Fermi-level. As t
he system is doped, the anti-ferromagnetic structure immediately becom
es unstable to an incommensurate spiral spin density wave phase. Howev
er, the existence of small nearest-neighbor hopping matrix element sta
bilizes the Neel stale over the range of dopings close to half filling
, as this disturbs the perfect nesting of the Fermi-surface.