  The magnetic arrangement in the vicinity of the interface between a
ferromagnet and an antiferromagnet is investigated, in particular its
dependence on the exchange couplings and the temperature. Applying a Heisenberg
model, both sc(001) and fcc(001) lattices are considered and solved by a mean
field approximation. Depending on the parameter values a variety of different
magnetic configurations emerge. Usually the subsystem with the larger ordering
temperature induces a magnetic order into the other one (magnetic proximity
effect). With increasing temperature a reorientation of the magnetic
sublattices is obtained. For coupled sc(001) systems both FM and AFM films are
disturbed from their collinear magnetic order, hence exhibit a similar
behavior. This symmetry is absent for fcc(001) films which, under certain
circumstances, may exhibit two different critical temperatures. Analytical
results are derived for simple bilayer systems.
