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High-temperature expansions of the susceptibility and internal energy (specific heat) are presented for general lattice structure for a system of isotropically interacting unit vectors (or "classical spins") which are constrained to lie in a plane. A phase transition (T₂>0) is indicated for two-dimensional lattices; the expected result T₂=0 is found in one dimension, but only upon choosing a more suitable expansion parameter than JkT. Similarities with the corresponding expansions of the S=12 Ising and classical Heisenberg models are pointed out; in particular, it is found that certain critical properties of this planar model appear to be bounded on one side by the Ising model and on the other side by the Heisenberg model.
H. Eugene Stanley (Mon,) studied this question.