In this paper, we establish time-independent global a priori bounds for the fractional Sobolev Hᵐ (R) norms (m > 5/2) of smooth solutions to the three-dimensional incompressible Navier- Stokes equations. Rather than employing geometric modifications, low-dimensional foliation dynamics, or non-standard metric spaces, we embed the sharp Calder´on-Zygmund commutator estimates recently established in Sarıcı, 2026 for the non-local pressure Hessian directly into the high-order energy budget. By combining these commutator identities with localized Littlewood- Paley dyadic decompositions and logarithmic Sobolev integration, we demonstrate that the non-linear vortex stretching mechanism is strictly absorbed by the viscous dissipation pathways at high frequencies. This provides a closed, deterministic analytical bridge proving that the H m norm of the velocity field cannot undergo finite-time blow-up.
Efe SARICI (Tue,) studied this question.