A method shows global regularity of the 3D incompressible Navier–Stokes equations, indicating a new proof framework.
This upload contains a self-contained research manuscript proposing a single, unified proof program for global regularity of the three-dimensional incompressible Navier--Stokes equations, organized around the critical L³ dissipation identity and an explicit algebraic cancellation in the pressure Hessian. We consider the incompressible Navier--Stokes system (on T³ or R³ with decay)\[∂_t v + (v·∇)v = -∇ p + ν Δ v, ∇· v = 0,\]with viscosity ν>0. The pressure is determined by\[-Δ p = ∂_j∂_k(v_j v_k), = R_jR_k(v_j v_k),\]where Rⱼ are Riesz transforms. The starting point is the critical L³ identity\[d/dt\|v(t)\|_3^3 + 3ν D_3(v(t)) = -3∫ |v|\, v·∇ p\,dx,\]with\[D_3(v) := ∫(|v|\,|∇ v|^2 + (v·∇ v)^2/|v|)\,dx.\]Global regularity follows if the pressure work satisfies\[|∫ |v|\, v·∇ p\,dx| ≤ c\,D_3(v) some c<ν,\]because then \|v(t)\|₃ is monotone and the endpoint criterion applies. The manuscript reduces the pressure work to a Calderon--Zygmund commutator in the ∂ⱼ∂ₖΔ⁻¹ (equivalently RⱼRₖ) channel and rewrites the commutator in a two-point increment form. The critical obstruction is the borderline radial measure $dr/r$ produced by a degree $-3$ kernel. The main structural lever is an exact quadrupole property of the pressure Hessian kernel:\[Kⱼₖ(z) ∝ p.v.{3 z_j z_k-δⱼₖ}{|z|^3}, z=z/|z|,\]whose angular factor is traceless and lies purely in the spherical harmonic channel =2 (zero mean on S²). Projecting onto =2 forces an angular-derivative gain that cancels the borderline $dr/r$ accumulation and yields log-free square-function control. This yields a single explicit scale-invariant depletion functional:\[Θ(v):=y0<ρ≤ L1/ρ∫B(y,ρ) {|P(y-x)/|y-x|\,∇ |v|(x)|^2}{|v(x)|}\,dx,\]where P_σ denotes tangential projection onto the plane orthogonal to σ and L is a fixed outer scale. The quadrupole estimate takes the form\[|∫ |v|\, v·∇ p\,dx|≤ √K_0\,Θ(v)\,D_3(v),\]with a universal constant K₀. Hence the monotonicity condition holds whenever\[Θ(v) < ν^2/K_0.\] Two closure directions are developed, both designed to reuse the same quadrupole mechanism: (A) Localized speed-entropy plus packing.Define the speed $u:=|v|$ and the critical speed-gradient density\[q := |∇ u|^2/u(on \{u>0\}).\]A localized entropy identity is derived by testing the local speed equation against a cutoff weight and log(u/r₀), which produces the coercive term ν∫ q exactly. A tube/ball packing mechanism is then proposed to convert largeness of Θ at a scale into a quantitative dissipation payment on that scale (up to a slow logarithmic factor related to the viscous core scale). (B) Coherent tubes imply depletion.Under a coherent-tube regime (vorticity-direction coherence plus a circulation lower bound of the form u ρ|ω| on high-vorticity sets), one obtains a Carleson/Morrey bound that forces Θ(v) to be small, giving an explicit conditional global regularity theorem with a falsifiable scale-selection rule for the threshold parameter. The manuscript concludes with three concrete remaining tasks for an unconditional proof:(i) a fully detailed localized quadrupole-commutator estimate (with tail control suitable for scale extraction);(ii) elimination of the remaining slow logarithm in the packing route via a scale-invariant gate in hypothetical blow-up regimes;(iii) a rigidity alternative showing that any attempt for Θ to cross the threshold forces dissipation incompatible with global L³ / energy budgets.
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David Thomson (2026) studied this question.
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