High-contrast homogenization: Provider.Response.WeakNormAPI #
Imported from the Apache-2.0 HighContrastHomogenization development at commit
7a13dbcd8d6609264a713373f5c69ceeac870472.
The scale-average seminorm: the estimates its proofs read #
The weak-norm estimate for the optimizer state uses the concrete scale-average seminorm through five operations, all recorded here.
- At each scale, the normalized
ℓ^2length(avsum_z|·|^2)^{1/2}obeys Cauchy-Schwarz and the triangle inequality; the triangle inequality is what the recent-scale decomposition `(X_t){U_k(z)} - (X_t){U_t} = ((X(U_k(z))){U_k(z)} - (X_t){U_t})- (X_t - X(U_k(z)))_{U_k(z)}` is summed through, and the uniform bound is what turns the cell-averaged energy bound into the scale-by-scale energy bound.
- Across scales, a scalewise majorant majorizes the seminorm, and a scalewise splitting splits it; this is the passage from the scale-by-scale energy bound to the weak-norm bound on the bad event and to the contribution of the old scales.
- The normalization
3^{-st}[·]of the printed left side is the seminorm with3^{sk}replaced by3^{-s(t-k)}. - The value is recovered as a real number exactly on the summable branch, the estimate being asserted also when the sum diverges; the geometric sum that makes both scale sums converge is the companion module.
The ℓ^2 inequalities are proved once on the flattened index 𝒵 × (d ⊕ d),
where the doubled Euclidean structure of ℝ^{2d} and the normalized counting
structure of the aligned index are a single finite sum.
The normalized ℓ^2 length of one scale #
The doubled Euclidean pairing expands on the flattened index.
Cauchy-Schwarz for the doubled pairing over a finite index set.
Cauchy-Schwarz for the normalized cell average.
The doubled Euclidean square of a sum.
The triangle inequality of one scale: the normalized ℓ^2 length is
subadditive. This is the inequality the recent-scale decomposition of the
weak-norm estimate is summed through.
The seminorm across scales #
The normalized left side 3^{-st}[F]_{B^{-s}_{2,1}(U_t)} of the
weak-norm estimate: the scale weights become the decay factors
3^{-s(t-k)}.