Abstract
We have investigated the magnetization as a function of T and H of a spin system with both isotropic Heisenberg exchange and dipole-dipole interactions for S12 and a hexagonal crystal structure. The Green's functions for such a system, recently derived by Becker, are decoupled in a first-order random-phase approximation. For both Heisenberg-dipole and simple-dipole crystals, we find a lowering of the magnetization below saturation at T=0. The Curie-Weiss temperature θ and the ordering temperature Tc are calculated and compared with experimental values on GdCl3. In the limit of zero exchange, we obtain a condition for the type of lattice and shape of domains which make ferromagnetic ordering possible.