Thermodynamic properties of the rare-gas solids Ar, Kr, and Xe are calculated using phenomenological two-body central potentials. The cubic and quartic anharmonic terms in the crystal Hamiltonian have been included, using conventional perturbation theory. Although some definite discrepancies with experiment exist for T<1/3Tmelting these simple models give a fair over-all account of both the volume and temperature dependence of the Helmholtz energy. However, for T>1/3Tmelting (rms deviations greater than {~}6% of the nearest-neighbor distance), anharmonic contributions to the thermodynamic properties become unrealistically large, indicating, we believe, the breakdown of perturbation theory to the order considered in this work.
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Klein et al. (1969) studied this question.
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