2025/09/25 by Fujii, Mikihiro, Tsurumi, Hiroyuki · 1 citation
#Analysis of PDEs (math.AP) #FOS: Mathematics
paper · doi:10.48550/arxiv.2509.21272
The asymptotic stability is one of the classical problems in the field of mathematical analysis of fluid mechanics. In ℝn with n ≥ 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 Bp,qn/p-1(ℝn) with 1 ≤ p < n and 1 ≤ q < ∞. In the present paper, we show that this asymptotic stability fails for p ≥ n with n ≥ 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 → ∞ in the framework of the critical Besov spaces Bp,qn/p-1(ℝn). 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 Bp,12/p-1(ℝ2) for all 1 ≤ p ≤ ∞. Our instability does not appear in the linear level but is caused by the nonlinear interaction from external forces.