Weighted limits for the Carleman density argument #
Finite sums of weak derivative components retain L² convergence, so the weighted quadratic
terms in lem:carleman-sobolev of the Escauriaza–Seregin–Šverák manuscript converge on a fixed
compact support neighborhood.
Finite sums of Lᵖ scalar fields remain in Lᵖ (lem:carleman-sobolev, ESS).
Space-time mollification is additive for globally L² fields (lem:carleman-sobolev, ESS).
Space-time mollification commutes with finite sums of globally L² fields
(lem:carleman-sobolev, ESS).
A bounded measurable coefficient makes a finite weighted sum of L² squares integrable
(lem:carleman-sobolev, ESS).
If an integrand vanishes almost everywhere off a compact subset, its integral reduces to
that subset (lem:carleman-sobolev, ESS).
Space-time mollification preserves global L² membership (lem:carleman-sobolev, ESS).
Global L² convergence of mollifications restricts to every measurable subset
(lem:carleman-sobolev, ESS).
The squared Euclidean norm on Vec3 is the sum of coordinate squares
(lem:carleman-sobolev, ESS).
A scalar field vanishes off any set containing its topological support
(lem:carleman-sobolev, ESS).
Bounded weights preserve convergence of finite sums of componentwise quadratic integrals.
This is the mass, gradient, and parabolic residual limit used by lem:carleman-sobolev (ESS).