Abstract
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 these simple models give a fair over-all account of both the volume and temperature dependence of the Helmholtz energy. However, for (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.
- Received 13 January 1969
DOI:https://doi.org/10.1103/PhysRev.184.968
©1969 American Physical Society