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The detailed structure of correlation functions in nonequilibrium stationary states is analyzed. The theory is applied to time-correlation functions and static-correlation functions in simple dense fluids. We find that the breaking of time-reversal symmetry induces important changes that cannot be predicted from local-equilibrium theories. The spectrum of light scattered from argon at 235 K and 1 g/cm³ subject to a temperature gradient of 0.5 K/cm is computed. We find a pronounced asymmetry in the Brillouin peaks. The static-correlation functions that are usually zero due to time-reversal symmetry are calculated and found to be nonzero and show the existence of a long-range order (1/r decay in physical space). The connection to phenomenology is discussed and a regressionlike hypothesis is shown to be consistent with the microscopic theory once the changes due to symmetry breaking are made.
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Ronis et al. (1979) studied this question.
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