  Proximity effects between ferromagnets (F) and superconductors (S) with
broken time-reversal symmetry (T) are studied theoretically. For the S side we
consider a chiral (p_x \pm ip_y)-wave, and a d_{x^2-y^2}-wave superconductor,
the latter of which can form T-breaking surface state, i.e., (d_{x^2-y^2} \pm
is)-state. The Bogoliubov de Gennes equation which describes the spatial
variations of the superconducting order parameter and the magnetization is
derived and solved numerically. It is found that a spontaneous spin current
flows along the interface between the (p_x \pm ip_y)-wave superconductor and
the ferromagnet. On the contrary, in the case of a [110] interface of the
d_{x^2-y^2}-wave SC, the surface state has a (d \pm p_x \pm p_y)-wave (or
(d_{x^2-y^2} \pm is)-wave) symmetry, and thus no (only charge) spontaneous
current arises.
