The magnetic behaviour of amorphous (RCo)/(RCo)' bilayers and the influence
of an optional intermediate layer have been studied. in the first analysed
bilayer, the monolayers have the same M-S and competing individual anisotr
opies, with their anisotropy axes mutually orthogonal. The magnetic couplin
g of YCo2 (40 nm)/Y/YCo2 (40 nm)', for Y layer thickness in the 0-40 nm ran
ge. has been analyzed by bulk magnetometry and Magneto-Optic Kerr Effect. T
he exchange coupling produces that the easy axis of both YCo2 layers are co
llinear when the intermediate Y layer is not present. On the other hand. fo
r Y layer 2 nm in thickness, a magnetostatic coupling is observed: and, for
Y intermediate layer thick enough (40 nm, no magnetic coupling is present.
The second system studied is Gd4Co1-x/Gdx 'Co1-x. (0.21 less than or equal
tox, x ' less than or equal to 0.38). In this case the system is a Ferrima
gnetic/(Ferrimagnetic)' bilayer where each individual layer has different c
ompensation temperature. In particular for, Gd0.38Co0.62/Gd0.21Co0.79 the G
d magnetic subnetwork dominates at room temperature in Gd0.38Co0.62 (T-comp
> 300 K), while the opposite is found for Gd0.21Co0.79 (T-comp =230 K). The
strong Co-Co exchange interaction at the bilayer interface leads to a 'mac
roscopic ferrimagnet behaviour'. The magnetization processes of this bilaye
r have also been studied. Reversible coherent rotation of the magnetization
is found when the held is applied perpendicular to the easy axis of the bi
layer. (C) 2001 Elsevier Science B.V. All rights reserved.