A ferrimagnet that does not have the opposing magnetic components in a unit cell of atomic dimensions is termed a macroscopic ferrimagnet. It is shown that the temperature dependence of the coercive field of such a magnet seems very different from that of a homogeneous ferrimagnet in that it decreases as T approaches the compensation temperature. This is understood to be the result of a weak magnetic coupling at the interface between the opposing components. This leads to an enhanced high-field susceptibility near the compensation temperature, which eventually controls the apparent coercive field. These suggestions are born out by a simple molecular field calculation.>
No takes yet. Share an insight, caveat, or question.
Webb et al. (1988) studied this question.
Synapse has enriched 5 closely related papers on similar clinical questions. Consider them for comparative context: