Abstract

Abstract We consider the large time behavior of the solution to the anisotropic Navier–Stokes equations in a $3$D half-space. Investigating the precise anisotropic nature of linearized solutions, we obtain the optimal decay estimates for the nonlinear global solutions in anisotropic Lebesgue norms. In particular, we reveal the enhanced dissipation mechanism for the third component of velocity field. We notice that, in contrast to the whole space case, some difficulties arises on the $L^{1}(\mathbb{R}^{3}_{+})$-estimates of the solution due to the nonlocal operators appearing in the linear solution formula. To overcome this, we introduce suitable Besov-type spaces and employ the Littlewood–Paley analysis on the tangential space.

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