On Liouiville Type Theorem for the 3D Isentropic Navier-Stokes System without D-condition

preprint2026arXivOpen access

Abstract

In this paper, we establish Liouville-type theorems for the steady compressible Navier-Stokes system. Assuming a smooth solution u∈Lp(R3)u \in L^p(\mathbb{R}^3), 3≤p≤923 \le p \le \frac{9}{2}, with bounded density, one obtains u≡0u \equiv0. This generalizes the result of Li-Yu \cite{Li-Yu} by removing the Dirichlet condition ∫R3∣∇u∣2 dx<∞\int_{\mathbb{R}^3} |\nabla u|^2 \, dx < \infty. If 92<p<6\frac{9}{2} < p < 6, Liouville-type theorem holds under the additional oscillation condition for momentum ρu∈B˙∞,∞3p−32(R3)ρu \in \dot{B}^{\frac{3}{p} - \frac{3}{2}}_{\infty,\infty}(\mathbb{R}^3). For the marginal case u∈L6(R3)u \in L^6(\mathbb{R}^3), the oscillation condition can be replaced by ρu∈BMO−1(R3)ρu \in BMO^{-1}(\mathbb{R}^3). We also present results in Morrey-type spaces: u∈M˙s,6(R3)u \in \dot{M}^{s,6}(\mathbb{R}^3) and ρu∈M˙wq,3(R3)ρu \in \dot{M}_w^{q,3}(\mathbb{R}^3) for 2≤s≤62 \le s \le 6 and 32<q≤3\frac{3}{2} < q \le 3.

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