  The symmetry of the superconducting states arising directly from
ferromagnetic states in the crystals with cubic and orthorombic symmetries is
described. The symmetry nodes in the quasiparticle spectra of such the states
are pointed out if they exist. The superconducting phase transition in the
ferromagnet is accompanied by the formation of superconducting domain structure
consisting of complex conjugate states imposed on the ferromagnet domain
structure with the opposite direction of the magnetization in the adjacent
domains. The interplay between stimulation of a nonunitary superconducting
state by the ferromagnetic moment and supression of the superconductivity by
the diamagnetic orbital currents is established.
