Abstract
High temperature series expansions have been calculated in terms of a general spin variable S, and anisotropy parameter eta , and and arbitrary lattice structure for the longitudinal version of the anisotropic Heisenberg model defined by the hamiltonian HN=- Sigma ijJ(SizSjz+ eta (Si+Sj-+Si-Sj+))- mu H Sigma i=1NSiz where the initial sum extends over the set of nearest neighbour sites of a regular crystal lattice structure of N sites, situated in an external magnetic field H. This model contains the Ising model and the isotropic Heisenberg model at the points eta =0, and eta =1/2 respectively. The expansions of the partition function Z in zero field and the zero field susceptibility have been obtained through orders T-7 and T-6 respectively.