The phase diagram and the single-domain uniform state for a uniaxial ferrom
agnetic film with the superconducting layers covering one or both sides of
a ferromagnet are investigated. The superconductor is supposed to be a seco
nd-order one and the interaction between the magnetic sub-system and with t
he conductivity electrons in a superconductor is purely electromagnetic and
the vortices in a superconductor are pinned. The critical thickness of the
magnetic film for which the uniform state becomes absolutely stable is cal
culated when the external magnetic field is supposed to be in-plane of the
film. It is shown that the critical thickness of the film from the magnetic
material with the quality factor Q > 1 monotonically decreases as the magn
etic field increases in the range from zero value to the value of the trans
ition field where the collinear phase transforms into the angular (canted)
phase. Further the critical thickness increases with the increase of the fi
eld. The quasi-single-domain magnetic film states were considered when the
film thickness was close to the critical one. It is shown that for a thin i
solated magnetic film the domain period exponentially increases with the de
crease of the film thickness. Such dependence, however fbr the film with do
uble-side superconducting cover and close to the transition into the single
domain state becomes logarithmic and for the him covered by superconductor
only on the one side varies as the power series. The single-domain state e
xistence and the asymptotic behaviour of the domain structure is explained
by the features of the asymptotic behaviour of the domain walls within the
system. As for isolated magnetic film and for a film with the superconducto
r cover layers the transition from the collinear phase to the inhomogeneous
state is the second-order phase transition and the transition from the uni
form angular phase to the inhomogeneous phase is the first-order transition
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