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• W2555971495 abstract "In this paper, we prove global regularity, scattering, and the non-existence of small traveling waves for the $3D$ finite depth capillary waves system for small initial data. The non-existence of small traveling waves shows a fundamental difference between the capillary waves ($sigma=1, g=0$) and the gravity-capillary waves ($sigma=1,$ $ 0< g< 3$) in the finite depth setting. As, for the later case, there exists arbitrary small $L^2$ traveling waves. Different from the water waves system in the infinite depth setting, the quadratic terms of the same system in the finite depth setting are worse due to the absence of null structure inside the Dirichlet-Neumann operator. In the finite depth setting, the capillary waves system has the worst quadratic terms among the water waves systems with all possible values of gravity effect constant and surface tension coefficient. It loses favorable cancellations not only in the High $times$ Low type interaction but also in the High $times $ High type interaction. In the worst scenario, the best decay rate of the nonlinear solution that one could expect is $ (1+t) ^ {-1/2} $, because the $3D$ finite depth capillary waves system lacks null structures and there exists $Q(u, bar{u})$ type quadratic term, which causes a very large time resonance set and the definite growth of the associated profile. As a result, the problematic terms are not only the quadratic terms but also the cubic terms. To prove global regularity for the capillary waves system, we identify a good variable to prove the dispersion estimate, fully exploit the hidden structures inside the capillary waves system, and use a novel method to control the weighted norms." @default.
• W2555971495 created "2016-11-30" @default.
• W2555971495 creator A5004606905 @default.
• W2555971495 date "2016-11-16" @default.
• W2555971495 modified "2023-09-27" @default.
• W2555971495 title "Global regularity for the 3D finite depth capillary water waves" @default.
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• W2555971495 hasPublicationYear "2016" @default.
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