Log-free estimate for the resonant paraproduct in the 3D Navier-Stokes equations
Pylyp Cherevan
TL;DR
This work proves a log-free a priori estimate for the resonant high–high→low paraproduct in the 3D Navier–Stokes equations. It combines phase–geometric integration by parts along an adapted frame, wave-packet discretization at scale \(N^{-1/2}\), and an anisotropic Strichartz estimate on \(N^{-1/2}\)-long time windows, augmented by bilinear decoupling on a rank-3 phase surface. The analysis splits into a wide angular region, where a phase-time gain of \(\lambda^{-3/2}\) is achieved via two angular IBPs and TT* on short windows, and a narrow almost-collinear region where a null-form suppression near the interaction diagonal yields exact \(\lambda^{-1}\) decay in \(\dot H^{-1}\). The results are scale-consistent and hold without smallness assumptions, relying only on divergence-free structure; the method targets a specific resonant component with discussion of possible generalizations. The paper unfolds a modular, global strategy to merge the dyadic pieces into a global bound, paving the way for extending log-free estimates to other nonlinear interactions in the series on the Navier–Stokes problem.
Abstract
We consider the resonant paraproduct (high-high $\to$ low regime) in the nonlinearity $(u\cdot\nabla)u$ for the three-dimensional Navier-Stokes equations. For sufficiently smooth, divergence-free u, we establish the a priori estimate without logarithmic loss $$\|R_N(u)\|{\dot H^{-1}} \lesssim N^{-1}\,\|u\|{\dot H^{1/2}}\,\|u\|_{\dot H^{1}},$$ with a constant independent of the dyadic frequency $N$. The proof combines phase-geometric integration by parts along an adapted frame, wave-packet discretization at scale $N^{-1/2}$, and an anisotropic Strichartz estimate on time windows of length $N^{-1/2}$. In the wide angular region we apply bilinear decoupling on a rank-3 phase surface; in the geometry at hand the minimal curvature yields a gain of order $N^{-1/6+o(1)}$ (with $o(1)\to 0$ as $N\to\infty$), which suffices to remove the logarithmic loss. The contribution from the narrow region is handled separately by an energy argument in $\dot H^{-1}$ using null-form suppression near the interaction diagonal. The resulting bound is scale-consistent and requires no smallness assumptions, only the divergence-free condition on $u$. The analysis is restricted to a single resonant component of the paraproduct; potential extensions are discussed.
