  We show that in strong (quantizing) magnetic fields "ordinary" free magnetic
polaron in diluted magnetic semiconductors (of type $A^2MeB^6$, where Me=Fe,
Mn) exists in the form of vortex lattice quite similar to that in type II
superconductors (Abricosov vortex lattice). The region of external parameters
(like external magnetic field and temperature), where such lattice exists, is
determined from the condition that lattice dimension is less or equal to
polaron localization radius.
