Abstract

Recent microscopic studies have underscored the relevance of classical percolation ideas to electron mobility in simple fluids. We show that Wigner phase-space averaging can be used to construct a semiclassical potential on which these concepts can be defined rigorously. The conduction-band threshold energy ${\mathit{V}}_{0}$ is then determined by solving a well-defined classical continuum percolation problem. Application of our model predicts the density dependence of ${\mathit{V}}_{0}$ quantitatively for the noble-gas fluids.

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