A well-defined order-disorder transition occurs in the capillary waves on a fluid layer driven by vertical oscillation. The transition is characterized by a sharp decline in both the translational correlation length and the long-range orientational order of the pattern, and an onset in the characteristic frequency f* of chaotic fluctuations varying approximately as (A-Ad)1/2, for driving amplitudes above a threshold Ad. The transition is geometry dependent even when the container size is 50-100 times the wavelength.
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Tufillaro et al. (1989) studied this question.
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