The spatial Vitali covering step of the statement CIV.timeZeroSingularSetNull #
This file proves the spatial analogue of Caffarelli–Kohn–Nirenberg's covering step
step:thmC-covering: if a set S of spatial points carries a uniform lower bound ε r on
the finite Dirichlet integral ∫⁻ |∇u|² of backward parabolic cylinders B(x, r) × (-r², 0)
at arbitrarily small radii, then S ∩ B(1) has one-dimensional Hausdorff measure zero. The
route covers S ∩ B(1) at each scale by a disjoint (Vitali) subfamily of such cylinders,
compares the sum of the lower bounds against the finite integral over a shrinking backward
time slab, and lets the scale tend to zero.
Spatial Vitali covering lemma (the spatial analogue of CKN's
step:thmC-covering). If S ⊆ Vec3 carries, at every point x ∈ S and every scale r₀ > 0,
a radius r < r₀ with ε r ≤ ∫_{B(x,r) × (-r²,0)} |∇u|² (the same integrand and measure
lintegral_gradSq_lt_top produces: ‖Du z‖ₑ ^ (2:ℝ) over the plain product-space volume
measure, restricted to the stated set), and the total ∫_{Q} |∇u|² over the unit cylinder is
finite, then S ∩ B(1) has one-dimensional Hausdorff measure zero.
The proof fixes a scale δ n = 1/(n+1) → 0, extracts at each n a disjoint (Vitali) family of
cylinders B(x_i, r_i) × (-r_i², 0), r_i < δ n, from the density hypothesis, and covers
S ∩ B(1) by the 5-enlarged spatial balls B(x_i, 5 r_i). The cylinders are disjoint, so the
lower bounds ε r_i sum to at most the (shrinking) integral over B(1) × (-δ n, 0), which
tendsto_lintegral_top_slab sends to 0; since each enlarged ball has sup-norm extended
diameter at most 10 r_i, the Hausdorff premeasure of the cover tends to 0 as well.
From a strict limsup lower density to the covering lemma's density hypothesis #
The bridge from a strict-limsup gradient density to
hausdorffMeasure_one_null_of_gradient_density's
hdens hypothesis. If ofReal ε₁ is at most the limsup, as the radius shrinks to 0 from
the right, of (ofReal r)⁻¹ times the Dirichlet integral of spatialGradientSq u Du over the
backward parabolic cylinder B(x,r) × (-r², 0), then at every scale r₀ > 0 there is a smaller
radius r < r₀ with ofReal (ε₁/18 * r) ≤ ∫ ‖Du‖ₑ² over that same cylinder — exactly the form
hausdorffMeasure_one_null_of_gradient_density consumes, at ε := ε₁ / 18. The constant loses a
factor of 2 because a strict limsup bound only gives, at every neighbourhood of 0, a point
where the halved level ε₁/2 is exceeded (not ε₁ itself), and a further factor of 9 bridging
spatialGradientSq to the enorm-squared integrand of
hausdorffMeasure_one_null_of_gradient_density
(ofReal_spatialGradientSq_le_nine), so only ε₁/(2·9) = ε₁/18 survives.