Abstract
The two-particle contribution to the potential part of the stress tensor autocorrelation function of a dense hard sphere fluid is studied. It is shown that the long-time decay is given as the solution of a diffusion equation for the relative particle in a potential of mean force. The diffusion constant needed in order to accurately reproduce molecular dynamics results is found to be somewhat lower than the self-diffusion constant.
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Leegwater, J.A., van Beijeren, H. The orientational pair correlation functions in a dense hard sphere fluid at long times. J Stat Phys 57, 383–391 (1989). https://doi.org/10.1007/BF01023650
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DOI: https://doi.org/10.1007/BF01023650