We find the exact Green's functions of the Anderson s-d mixing model for ma
gnetic trilayers with arbitrary spin canting angle between two ferromagneti
c layers within the mean-field theory of the on-site Coulomb repulsion. A b
ilinear exchange coupling and an intrinsic biquadratic coupling which does
not vanish in the limit of flat interfaces is obtained by those Green's fun
ctions. It is shown that both of these couplings oscillate in the experimen
tal range of the spacer thickness only when the s-d mixing is strong enough
. When the mixing strength is large enough one finds that the oscillation p
eriod of the intrinsic biquadratic term is equal to half of the correspondi
ng one for the bilinear term. We also find that the temperature dependence
of those interlayer couplings is considerably enhanced with the decrease of
the Hubbard coupling. It is also shown that the biquadratic coupling falls
off much more rapidly with increasing temperature than the bilinear one.