纳维-斯托克斯方程在 $\big(C((0,T];L^d(\mathbb{R}^d))\cap L\infty((0,T);L^d(\mathbb{R}^d))\big)^d$ 中的温和解的唯一性

Zhirun Zhan
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摘要

本文论述了强制或非强制纳维-斯托克斯方程的温和解在整个空间中的唯一性。众所周知,当 $d\geq 4$ 时,非强迫纳维-斯托克斯方程的温和解的唯一性在$\big(L^{\infty}((0,T);L^d(\mathbb{R}^d))\big)^d$ 中成立;当 $d\geq3$ 时,温和解的唯一性在$\big(C([0,T];L^d(\mathbb{R}^d))\big)^d$ 中成立。至于受迫纳维尔-斯托克斯方程,当 $d\geq3$ 时,$\big(C([0,T];L^{d}(\mathbb{R}^d))\big^d$ 中的温和解的唯一性与某个洛伦兹空间中的力 $f$ 是已知的。在本文中,我们证明了对于 $d\geq3$,在$\big(C((0,T];L^d(\mathbb{R}^d))\cap L^\infty((0,T);当$\big(C([0,T];L^d(\mathbb{R}^d))\big)^d$中存在温和解且初始数据和作用力相同时,L^d(\mathbb{R}^d))\big)^d$成立。作为这一结果的推论,我们在 $\big(C((0,T];L^3(\mathbb{R}^3))\capL^\infty((0,T);L^3(\mathbb{R}^3))\big^3$ 中建立了非受迫 Navier-Stokesequations 的温和解的唯一性。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Uniqueness of mild solutions to the Navier-Stokes equations in $\big(C((0,T];L^d(\mathbb{R}^d))\cap L^\infty((0,T);L^d(\mathbb{R}^d))\big)^d$
This paper deals with the uniqueness of mild solutions to the forced or unforced Navier-Stokes equations in the whole space. It is known that the uniqueness of mild solutions to the unforced Navier-Stokes equations holds in $\big(L^{\infty}((0,T);L^d(\mathbb{R}^d))\big)^d$ when $d\geq 4$, and in $\big(C([0,T];L^d(\mathbb{R}^d))\big)^d$ when $d\geq3$. As for the forced Navier-Stokes equations, when $d\geq3$ the uniqueness of mild solutions in $\big(C([0,T];L^{d}(\mathbb{R}^d))\big)^d$ with force $f$ in some Lorentz space is known. In this paper we show that for $d\geq3$, the uniqueness of mild solutions to the forced Navier-Stokes equations in $\big(C((0,T];L^d(\mathbb{R}^d))\cap L^\infty((0,T);L^d(\mathbb{R}^d))\big)^d$ holds when there is a mild solution in $\big(C([0,T];L^d(\mathbb{R}^d))\big)^d$ with the same initial data and force. As a corollary of this result, we establish the uniqueness of mild solutions to the unforced Navier-Stokes equations in $\big(C((0,T];L^3(\mathbb{R}^3))\cap L^\infty((0,T);L^3(\mathbb{R}^3))\big)^3$.
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