  We consider the minigap in a disordered ferromagnet (F) in contact with a
superconductor (S) in the situation when the magnetization of the F layer is
inhomogeneous in space and noncollinear. If the magnetization is strongly
inhomogeneous, it effectively averages out, and the minigap survives up to the
exchange field $h_c ~ (L/a) E_{Th}$, where $L$ is the thickness of the F layer,
$a$ is the scale on which the magnetization varies, and $E_{Th}$ is the
Thouless energy. Technically, we use the "triplet" version of the Usadel
equations including both singlet and triplet components of the Green's
functions. In many cases, the effect of disordered magnetization may be
effectively included in the conventional Usadel equations as the spin-flip
scattering term. In the case of low-dimensional magnetic inhomogeneities (we
consider spiral magnetization as an example), however, the full set of
"triplet" equations must be solved.
