The insulating states of three model systems, the two-chain Hubbard mo
del, the two-layer two-dimensional Hubbard model and the two-dimension
al symmetric periodic Anderson model are discussed. All of these syste
ms at half-filling have a charge gap but they can exhibit various type
s of spin gaps ranging from a vanishing spin gap in systems with stron
g antiferromagaetic correlations to a spin gap which is equal to the c
harge gap in the band-insulator regime. The interchain, interplane, or
Anderson model f-d hybridization plays a key role in determining the
spin-to-charge gap ratio and the nature of the insulating state.