So far, magnetic polarons in antiferromagnetic semiconductors (ferrons) wer
e assumed to arise due to the charge carrier self-trapping by a ferromagnet
ic or canted antiferromagnetic region. If the ferron size is not very large
, they should have much more complicated structure: the magnetically deform
ed region consists not only of a magnetized core, which traps the electron,
but also of its surrounding with the oppositely directed total moment, whi
ch repulses the trapped electron. The compensating moment of the surroundin
g oscillates with a period of the doubled lattice constant and with the amp
litude diminishing very smoothly on an increase in the distance from the co
re. (C) 2001 MAIK "Nauka/Interperiodica".