In this paper static properties of two kinds of point defects in an antiferromagnet are examined. The topology of the two defects, vacancies and interstitials, is different, the first belonging to a well-defined sublattice, and the other acting symmetrically on both sublattices. The perpendicular susceptibility of the vacancy is found to be positive due to a polarization of the medium, overcompensating the lack of magnetization due to the removal of one atomic moment. The additional susceptibility due to the interaction of pairs of vacancies is investigated; its sign depends on whether the two are on the same or different sublattices. It is shown that an interstitial embedded in an antiferromagnetic crystal has a moment that is linked to a plane of easy magnetization, perpendicular to the axis of the crystal, by a pseudoanisotropy field of the order of magnitude of an exchange field. The coupling of such interstitials is shown to decrease as r−7 but could be strong enough to induce cooperative effects.
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B Dreyfus (1963) studied this question.
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