NegNormToL2 #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
The negative-norm-to-L² step: the L² distance from the negative fractional norm #
ABK26's Step 1 closes with the two-step chain
‖u - v‖_{L²(x+□_n)} ≤ C ‖∇u - ∇v‖_{H_hat^{-1}(x+□_n)}
≤ C 3^{(1 - s/2)n} ‖∇u - ∇v‖_{H_hat^{-s/2}(x+□_n)} ,
for u - v ∈ H¹₀(x+□_n), whose second inequality the graph records as an
unexplained "Besov-scale comparison on a cube of side 3^n".
Finding: CoarseGraining proves the whole chain in one theorem, and the printed scale factor comes out exactly. The theorem is
cubeBesovScaleWeight 1 Q · ‖u‖_{L²(Q)}
≤ C(d) · sqrt((1 - 3^{-2(1/2 - t)})⁻¹) · [∇u]_{B^{-2t}_{2,2}(Q)}
(Homogenization.Book.Ch03.cubeBesovScaleWeight_one_mul_cubeLpNorm_h10_le_grad_
negativeBesovTwo, for u ∈ H¹₀(cubeSet Q) and 0 < t < 1/2). Since
cubeBesovScaleWeight 1 Q = 3^{-Q.scale} and CoarseGraining's negative
seminorm carries the manuscript's own outer normalization 3^{-σ·scale}, the
conclusion reads
‖u‖_{L²(□_n)} ≤ C(d) 3^{n} · 3^{-2tn} [∇u]_{H_hat^{-2t}(□_n)}
= C(d) 3^{(1-2t)n} [∇u]_{H_hat^{-2t}(□_n)} ,
No separate H_hat^{-1} ← H_hat^{-s/2} comparison is needed: the two printed
inequalities are one theorem.
This module contributes the two bounded pieces:
negNormSqrtFactor_le_two: att = s/4ands ≤ 1the analytic factorsqrt((1 - 3^{-2(1/2 - s/4)})⁻¹)is at most2— so the whole constant isC(d), as printed;cubeLpNorm_h10_le_negativeBesov_quarter: the specialization att = s/4, with the negative index displayed ass/2and the analytic factor absorbed.
The norm on the right is the manuscript's own substitute (recorded) #
CoarseGraining's right-hand object is the concrete block-average negative
seminorm B^{-σ}_{2,2}, not the hatted H_hat^{-σ} the display prints. The
manuscript itself performs exactly this substitution — records
‖·‖_{H_hat^{-s}(□)} ≤ C ‖·‖_{B^{-s}_{2,2}(□)} ≤ C ‖·‖_{B^{-s}_{2,1}(□)} — so
the inequality below is the printed one with the printed norm replaced by the
dominating one, i.e. a weaker statement per step. The composition with the
coarse-graining leg must therefore be made at the
B^{-σ}_{2,2} level, which is also the level at which CoarseGraining's
coarse-graining machinery produces its bounds. Nothing here claims the hatted
norm.
What is still missing (disclosed frontier) #
The frozen theorem's left-hand side is eLpNorm (u - v) 2 (normalizedVolumeMeasureOn ((x + □_n) image)), on an off-grid window,
while CoarseGraining's theorem is stated at a triadic cube in the
cubeSet/cubeLpNorm carriers. Two bridges therefore remain, neither of them
attempted here: the normalizedVolumeMeasureOn-vs-normalizedCubeMeasure
identification on the open/closed cube pair, and the A4 frame change (this leg
lives naturally in the frame translated by x, while the energy leg lives in
the frame translated by z).
References #
- ABK26,
l.harmonic.approximation.good.scales.
1. The analytic factor at t = s/4 #
2. The negative-norm step at the parameter choice t = s/4 #
The dimensional constant of CoarseGraining's zero-trace value estimate.
Equations
Instances For
The negative-norm-to-L² step at t = s/4.
3^{-Q.scale} ‖u‖_{L²(Q)} ≤ 2 C(d) [∇u]_{B^{-s/2}_{2,2}(Q)} (u ∈ H¹₀(Q)) .
This is the printed two-step chain, in one inequality, at the negative index
s/2 and with the analytic tail factor discharged by
negNormSqrtFactor_le_two. Nonnegativity of the right-hand seminorm is
derived from the inequality itself (the left side is nonnegative and the
constant is positive), so no BddAbove hypothesis is imposed.