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We propose the existence of an inhomogeneous transport regime in the disordered materials in which a gradual metal-semiconductor transition occurs. This regime is sub-divided into pseudometallic and pseudosemiconducting parts by a percolation threshold. On the basis of an effective-medium theory, we propose that the pseudometallic regime falls in the density range 8.2-9.3 g/cm³ in liquid Hg and in the temperature range 1200^∘{}K to below 670^∘{}K in liquid Te.
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Cohen et al. (1973) studied this question.
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