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Abstract It is shown by a general theoretical argument that the variation of the magnetic specific heat of a ‘simple’ antiferromagnet, in particular the singular behaviour in the region of the transition, should be closely similar to the behaviour of the function ∂(χT)∂T, where χ is the zero-field susceptibility. This conclusion is compared with the experimental results for MnO and MnF2 and its general implications for the shape of the susceptibility curve near the transition are discussed.
Michael E. Fisher (Mon,) studied this question.
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