On the existence of self-similar solutions to the steady Navier-Stokes equations in high dimensions
Jeaheang Bang, Changfeng Gui, Hao Liu, Yun Wang, Chunjing Xie
TL;DR
This work establishes the existence of self-similar $(-1)$-homogeneous solutions to the steady Navier–Stokes equations in dimensions $4\le n\le 16$ under a $(-3)$-homogeneous, locally Lipschitz external force $\boldsymbol f$, with regularity away from the origin. The authors develop a novel a priori energy framework that links the radial velocity component to the total head pressure on the sphere, enabling control of nonlinear terms and higher integrability of $H_+$, and they close the estimates via a Leray–Schauder degree argument to obtain existence; global uniqueness is shown when the forcing is small, and a dimension-free result is achieved for forces with nonnegative radial component. The approach combines sphere-based identities, decomposition into tangential and radial parts, and elliptic regularity to bootstrap regularity up to $C^{2,\alpha}_{loc}$, extending Shi’s 4D results to higher dimensions. This advances understanding of scale-invariant steady flows under large, translation-invariant forcing and provides a rigorous fixed-point construction for self-similar solutions in higher-dimensional settings.
Abstract
We prove that the steady incompressible Navier-Stokes equations with any given $(-3)$-homogeneous, locally Lipschitz external force on $\mathbb{R}^n\setminus\{0\}$, $4\leq n\leq 16$, have at least one $(-1)$-homogeneous solution which is scale-invariant and regular away from the origin. The global uniqueness of the self-similar solution is obtained as long as the external force is small. The key observation is to exploit a nice relation between the radial component of the velocity and the total head pressure under the self-similarity assumption. It plays an essential role in establishing the energy estimates. If the external force has only the nonnegative radial component, we can prove the existence of $(-1)$-homogeneous solutions for all $n\geq 4$. The regularity of the solution follows from integral estimates of the positive part of the total head pressure, which is due to the maximum principle and a ``dimension-reduction" effect arising from the self-similarity.
