The temperature dependence of the magnetization in fee Fe on Cu(100) is cal
culated using a self-consistent local mean-field theory. The model reproduc
es an experimental magnetization oscillation as a function of film thicknes
s and supports a picture where the top two layers are ferromagnetically cou
pled, and the remaining layers are antiferromagnetically coupled. The origi
n of the puzzling linear temperature dependence in oscillation amplitude is
understood as a "surface phenomena" of the antiferromagnetic layer at the
Fe/Cu interface. Proximity effects between a thin antiferromagnet with a lo
w Neel temperature and a neighboring ferromagnet with a higher Curie temper
ature are discussed.