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Quantum corrections to the behavior of a nearly classical system may be determined via the Green's-function formalism, or via the Wigner-distribution-function (WDF) method. Recently, it appeared that there is a serious discrepancy between the results obtained by these methods for the melting temperature of the two-dimensional Wigner crystal. We resolve this problem by showing that the ``effective-potential'' technique of implementing the WDF method is invalid, and we present a correct approach.
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Dickman et al. (1985) studied this question.
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