Abstract
Crystal field theory has been used to examine the origin of magnetic anisotropy in CoCl2 and NiCl2. These salts are antiferromagnets in which the metal ions form ferromagnetic layers with alternate layers oriented in opposite directions. An exchange Hamiltonian is derived for ions in the ground state taking account of a ferromagnetic in-layer interaction J1 and an antiferromagnetic between-layer interaction J2, and it is found that the anisotropy may be approximately represented by including a single extra parameter. The cooperative problem is then treated by molecular field theory at extremes of high and low temperature, and by Green function techniques (using the results of the previous paper) for temperatures near the Néel point. Fitting low-temperature experimental results with the theory, the exchange interactions are calculated showing, in particular, that the ratio J1J2 is large in both salts (11.6 for CoCl2, 13.1 for NiCl2). Using these estimates the high-temperature susceptibility is derived and a good agreement between experiment and theory observed. For CoCl2 the anisotropy is considerable and g values gII=3.38 and g=4.84 are estimated.

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