We investigate some geometric properties of the $\operatorname{ curl}$ operator, based on its diagonalizationand its expression as a non-local symmetry of the pseudo-derivative $(-\Delta)^{ 1/2}$ among divergence-free vector fieldswith finite energy. In this context, we introduce the notion of spin-definite fields, i.e. eigenvectorsof $(-\Delta)^{ -1/2}\operatorname{ curl}$.The two spin-definite components of a general 3D incompressible flow untangle the right-handed motion from the left-handed one. Having observed that the non-linearity of Navier-Stokes has the structure of a cross-productand its weak (distributional) form is a determinant that involves the vorticity, the velocity and a test function,we revisit the conservation of energy and the balance of helicity in a geometrical fashion. We show that in the caseof a finite-time blow-up, both spin-definite components of the flow will explose simultaneously and with equal rates,i.e. singularities in 3D are the result of a conflict of spin, which is impossible in the poorer geometry of 2D flows.We investigate the role of the local and non-local determinants $$\int_0^T\int_{ \mathbb{ R}^3}\det(\operatorname{ curl} u, u, (-\Delta)^{ \theta} u)$$ and their spin-definite counterparts, which drive the enstrophy and, more generally, are responsible forthe regularity of the flow and the emergence of singularities or quasi-singularities.As such, they are at the core of turbulence phenomena.
Categories: math.AP