The scaled density fluctuation field of a Glauber-Kawasaki lattice gas near a stationary flat interface converges to e(ϑ)√̟B_t in dimension 1 and to e(ϑ)Z_t(θ), with Z solving the additive-noise one-dimensional stochastic heat equation, in dimension 2.
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Linear fluctuation of interfaces in Glauber-Kawasaki dynamics
The scaled density fluctuation field of a Glauber-Kawasaki lattice gas near a stationary flat interface converges to e(ϑ)√̟B_t in dimension 1 and to e(ϑ)Z_t(θ), with Z solving the additive-noise one-dimensional stochastic heat equation, in dimension 2.