Abstract

A dynamic theory of magnetic kinks in a two-layered ferromagnet, which propagate in the direction of the normal to the interlayer boundary (planar “defect”), has been developed. Conditions for the passage of kinks through the boundary have been determined and the critical velocity for their absorption has been found. It has been shown that at kink velocities exceeding critical, the boundary, when absorbing a kink, emits an antikink. The dependence of the delay time of the kink in the defect on its velocity has been established.

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