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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.

Log-free estimate for the resonant paraproduct in the 3D Navier-Stokes equations

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 , and an anisotropic Strichartz estimate on -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 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 decay in . 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 low regime) in the nonlinearity for the three-dimensional Navier-Stokes equations. For sufficiently smooth, divergence-free u, we establish the a priori estimate without logarithmic loss with a constant independent of the dyadic frequency . The proof combines phase-geometric integration by parts along an adapted frame, wave-packet discretization at scale , and an anisotropic Strichartz estimate on time windows of length . 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 (with as ), which suffices to remove the logarithmic loss. The contribution from the narrow region is handled separately by an energy argument in 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 . The analysis is restricted to a single resonant component of the paraproduct; potential extensions are discussed.

Paper Structure

This paper contains 153 sections, 25 theorems, 268 equations.

Key Result

Theorem 2.1

Let $u:[0,T]\times\mathbb{R}^3\to\mathbb{R}^3$ be a divergence-free solution with $u\in C([0,T];\dot H^{1/2}\cap \dot H^{1})$ (see also §subsec:init, §subsec:hyp). Then for each $N\in 2^{\mathbb{Z}}$ and all $t\in[0,T]$ one has In integral form, where $X_\sigma$ is given in eq:Xsigma. The constant is independent of $N$ and $T$ and depends on $u$ only through the indicated norms.

Theorems & Definitions (66)

  • Theorem 2.1: Log-free estimate for the resonant block
  • Remark 2.2: Periodic case
  • Remark 2.3: Context
  • Remark 3.1: On variables
  • Lemma 3.2: Block structure and radial component
  • proof : Idea of the proof
  • Lemma 3.3: Nondegeneracy of $A_{\mathrm{eff}}$
  • proof
  • Corollary 3.4: Two angular IBPs
  • proof : Idea of the proof
  • ...and 56 more