Asymptotic instability for the forced Navier--Stokes equations in critical Besov spaces

Abstract

The asymptotic stability is one of the classical problems in the field of mathematical analysis of fluid mechanics. In ${\mathbb{R}}^n$ with $n\ge 3$, it is easily proved by the standard argument that if the given small external force decays at temporal infinity, then the small forced Navier--Stokes flow also strongly converges to zero as time tends to infinity in the framework of the critical Besov spaces ${\dot{B}}_{p,q}^{n/p-1}({\mathbb{R}}^n)$ with $1\le p<n$ and $1\le q<\infty$. In the present paper, we show that this asymptotic stability fails for $p\ge n$ with $n\ge 3$ in the sense that there exist arbitrary small external forces whose critical Besov norm decays in large time, whereas the corresponding Navier--Stokes flows oscillate and do not strongly converge as $t\to \infty$ in the framework of the critical Besov spaces ${\dot{B}}_{p,q}^{n/p-1}({\mathbb{R}}^n)$. Moreover, we find that the situation is different in the two-dimensional case $n=2$ and show the forced Navier--Stokes flow is asymptotically unstable in ${\dot{B}}_{p,1}^{2/p-1}({\mathbb{R}}^2)$ for all $1\le p\le \infty$. Our instability does not appear in the linear level but is caused by the nonlinear interaction from external forces.