Results of detailed calculations of the anharmonic and the quantum corrections to the equation of state and to Grüneisen's parameter γ are given for pressures P from zero to 2B0 (where B0 is the bulk modulus at P = 0 and T = 0) and for temperatures T from zero to (0.6) Tε (where Tε = ∈/k,∈ is the depth of the potential well and k is Boltzmann's constant). Interionic potentials of the form A/r+ϕR with ϕR proportional to r−12, r−8, and e−αr were used. It was found, for example, that at T = (0.2) T∈ the anharmonic corrections to P for the potentials in the order just given were approximately 7, 6, and 4% at P = (0.1)B0, while they were approximately 1, 1, and ½% at P = (0.5)B0. Quantum corrections to P were found to depend very weakly on P and to be about 1% or less for (0.2)B0 < P < 2B0 for temperatures above the zero‐pressure Debye temperature. Anharmonic corrections decreased the values of γ and of P, while quantum corrections decreased the value of γ but increased the value of P.
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Robert J. Hardy (1980) studied this question.
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