Abstract
It was proved [Navier–Stokes Equations for Stochastic Particle System on the Lattice. Comm. Math. Phys. (1996) 182, 395; Lattice gases, large deviations, and the incompressible Navier–Stokes equations. Ann. Math. (1998) 148, 51] that stochastic lattice gas dynamics converge to the Navier–Stokes equations in dimension d=3 in the incompressible limits. In particular, the viscosity is finite. We proved that, on the other hand, the viscosity for a two dimensional lattice gas model diverges faster than (log t)1/2. Our argument indicates that the correct divergence rate is (log t)1/2. This problem is closely related to the logarithmic correction of the time decay rate for the velocity auto-correlation function of a tagged particle.
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Yau H.T., (log t)2/3 law of the two dimensional asymmetric simple exclusion process, to appear in Annals Math.
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Landim, C., Ramírez, J.A. & Yau, HT. Superdiffusivity of Two Dimensional Lattice Gas Models. J Stat Phys 119, 963–995 (2005). https://doi.org/10.1007/s10955-005-4297-1
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DOI: https://doi.org/10.1007/s10955-005-4297-1