Establishes bounds for Sobolev norms in Navier-Stokes equations, indicating finite-time resolution.
In this paper, we establish time-independent global a priori bounds for the fractional Sobolev H^m(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.
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Efe SARICI (2026) studied this question.
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