This paper is devoted to the global solvability of the Navier−Stokes system with a fractional Laplacian (−Δ) α in for n ≥ 2, where the convective term has the form (| u | m −1 u )·∇ u for m ≥ 1. By establishing the estimates for the difference in homogeneous Besov spaces and employing the maximal regularity property of (−Δ) α in Lorentz−Besov spaces, we prove global existence and uniqueness of the strong solution of the Navier−Stokes system in critical Besov spaces for both m = 1 and m > 1.
Zhang et al. (Thu,) studied this question.
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