{ "id": "1910.08911", "version": "v1", "published": "2019-10-20T06:44:14.000Z", "updated": "2019-10-20T06:44:14.000Z", "title": "New Regularity Criteria for the Navier-Stokes Equations in Terms of Pressure", "authors": [ "Benjamin Pineau", "Xinwei Yu" ], "comment": "9 pages", "categories": [ "math.AP" ], "abstract": "In this paper, we generalize the main results of [1] and [31] to Lorentz spaces, using a simple procedure. The main results are the following. Let $n\\geq 3$ and let $u$ be a Leray-Hopf solution to the $n$-dimensional Navier-Stokes equations with viscosity $\\nu$ and divergence free initial condition $u_0\\in L^2(\\mathbb{R}^n)\\cap L^{k}(\\mathbb{R}^n)$ (where $k=k(s)$ is sufficiently large). Then there exists a constant $c>0$ such that if \\begin{equation} \\|p\\|_{L^{r,\\infty}(0,\\infty;L^{s,\\infty}(\\mathbb{R}^n))}\\frac{n}{2} \\end{equation} or \\begin{equation} \\|\\nabla p\\|_{L^{r,\\infty}(0,\\infty;L^{s,\\infty}(\\mathbb{R}^n))}\\frac{n}{3} \\end{equation} then $u$ is smooth on $(0, \\infty) \\times \\mathbb{R}^n$. Partial results in the case $n=3$ were obtained in [32], [33] and then recently extended to all appropriate pairs of $r,s$ in [14]. Our results present a unified proof which works for all dimensions $n\\geq 3$ and the full range or admissible pairs, $(s,r)$.", "revisions": [ { "version": "v1", "updated": "2019-10-20T06:44:14.000Z" } ], "analyses": { "keywords": [ "regularity criteria", "divergence free initial condition", "main results", "dimensional navier-stokes equations", "appropriate pairs" ], "note": { "typesetting": "TeX", "pages": 9, "language": "en", "license": "arXiv", "status": "editable" } } }