  The induced magnetic moment, provided by the bands electrons, is calculated
in a variety of Josephson junctions with multilayered ferromagnetic (F) weak
link. The noncollinear magnetization of the F layers provides the conditions
necessary to generate triplet superconducting correlations. It leads to the
long-range induced magnetic moment, emerging in the superconducting (S) layers.
It is shown to be dependent on the Josephson phase. By tuning the Josephson
current, one may control the long-range induced magnetic moment. Alternatively,
applying the voltage we can generate an oscillatory magnetic moment. The
detection of such a spin effect may serve as independent evidence of the
triplet superconductivity. The proposed mechanism seems to be attractive for
superconducting spintronic devices with low dissipation.
