Abstract

In this paper we extend the calculation of the free energy in systems with separable interactions given in a previous paper, to a more general class of systems characterized by a hamiltonian which contains a number of separable two-particle operators of the antiferromagnetic type in addition to separable ferromagnetic interactions and one-particle operators. By deriving an upper bound and a lower bound we establish an expression for the free energy which is of the molecular-field type. In the derivation of the lower bound we have used Laplace's method in order to evaluate a multidimensional integral of a function e NG . The proof that the second derivatives at the absolute minimum do not give a contribution in the thermodynamic limit is more complicated than in the ferromagnetic case and is given in detail.

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