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A finite-temperature perturbation theory for the Heisenberg model of ferromagnetism is presented. A modified Wick theorem proved for S = ½ and finite temperature allows the terms in the expansion for the temperature-dependent Green function to be expressed by linked diagrams of the Feynman type. These differ from the normal boson and fermion diagrams in the appearance of time(temperature)-dependent broken lines between propagators, a modification caused by the spin statistics.
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Lewis et al. (1967) studied this question.
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