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We present a computer simulation study of orientational correlations in a molecular liquid approaching the isotropic-nematic transition, including the first calculation of the direct correlation function $c(1,2)$ in this regime. While the second-rank orientational correlation length diverges, the associated component of $c(1,2)$ remains short ranged, and its spatial integral approaches the mechanical instability limit for the isotropic phase as predicted by density-functional theory. Orientational correlation lengths and times are quite well described by Landau--de Gennes theory.
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Allen et al. (1997) studied this question.
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