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This paper contributes to the theory of the long-range attractive polarization force between a neutral atom and a crystalline solid surface in the nonrelativistic limit. The first two terms in the asymptotic expansion of the polarization energy are used to define an atom-solid potential of the form Vₚₒₗ=-C(Z-Z₀)^-3. The constant C appearing in this expression is known from the earlier work of E. M. Lifshitz. The present paper gives a theory of the position of the "reference plane," Z₀, which is important in applications to physisorption. An explicit expression for Z₀ is first derived for atoms interacting with a jellium metal and with an insulating crystal consisting of atoms which interact via dipole-dipole forces. These model calculations are then incorporated into a computation of the polarization energies of rare-gas atoms physisorbed on noble-metal surfaces. The computed energies are found to be consistent with observed adsorption energies.
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Zaremba et al. (1976) studied this question.
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