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The method of constant-stress molecular dynamics using the Parrinello-Rahman Lagrangian is described, particularly as applied to Coulomb systems. The method is used to simulate the phase behavior of silver iodide. The {β}, {α}, rocksalt, and liquid phases are reproduced and the boundaries are similar to those observed for real AgI. Evidence is found for the order-disorder transition in the {α} phase proposed by Perrott and Fletcher. This is characterized by a heat-capacity anomaly and a rise in the cation diffusion coefficient. The supercooled {α} phase and the equilibrium rocksalt phase both have diffuse fast-ion transitions and the latter cuts the rocksalt--{α}-phase boundary, causing it to cusp in to an apparent triple point with the {α}-phase order-disorder transition.
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J. L. Tallon (1988) studied this question.
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