We present the first Monte Carlo study of the dynamics of the formation of the wet phase far from the wetting transition for a short-range attractive wall potential. A nearest-neighbor, simple-cubic, ferromagnetic Ising lattice gas with single spin-flip dynamics in a slab geometry (L×{}L cross section) is used. We show that there are two distinct dynamical regimes with crossover from fluctuation-dominated logarithmic growth for large L and short time t to quasi-one-dimensional diffusive growth for small L and large t. For any finite system, the long-time behavior (i.e., t{}L⁴[ln(L)²]) is predicted to always be quasi-one-dimensionally diffusive in nature.
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Mon et al. (1987) studied this question.
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