Unusual domain walls have been found in ferrofluid patterns on thin film materials with low magnetization that is in or near the plane of the film. These walls carry a net magnetic charge and are characteristically kinked in a regular manner to form a zigzag. A simple account is given of the energetics of such walls whose form follows from a compromise between magnetostatic terms and the energy of anisotropy. It is argued that an array of closure domains at straight edges in these materials should have a boundary of similar character, and these too have been observed.
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M. J. Freiser (1979) studied this question.
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