Abstract
The magnetic couplings in insulating LaMnO3, CaMnO3, and the planar analogs Lan+1 Mnn O3n+1 are estimated using standard superexchange arguments. The orbital ordering observed in LaMnO3 is found to lead to the observed magnetic exchange constants if the effective Mn on-site interaction UMn is larger than the charge transfer energy. Differences between the pseudocubic and the planar materials are accounted for. The effect of doping is discussed.