StepSevenWireBridge #
Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.
t.regularity Step 7d: the summability conversion B^{-1}_{2,1} ← B^{-t}_{2,2} #
The maneuver, on the proved carriers #
Both sides are already scale-normalized in CoarseGraining, with depth weight
3^{-s j} and the same depth average A_j = ⨍_{R ⊂ Q, depth j} |(F)_R|²:
q = 1 at index 1 : Σ_j 3^{-j} √A_j = 3^{-m}‖F‖_{B^{-1}_{2,1}(Q)}
q = 2 at index t : (Σ_j (3^{-tj}√A_j)²)^{1/2} = 3^{-tm}‖F‖_{B^{-t}_{2,2}(Q)}
Split the weight 3^{-j} = 3^{-(1-t)j}·3^{-tj} (depthSeminorm_one_eq),
Cauchy--Schwarz the scale sum, and evaluate the geometric factor:
Σ_j 3^{-j}√A_j ≤ (Σ_j 3^{-2(1-t)j})^{1/2} · (Σ_j (3^{-tj}√A_j)²)^{1/2}
≤ (1 - 3^{-2(1-t)})^{-1/2} · 3^{-tm}‖F‖_{B^{-t}_{2,2}(Q)} .
The 3^{-m} outer weight stays on the B^{-1}_{2,1} side and the 3^{-tm} on
the B^{-t}_{2,2} side, because both CoarseGraining carriers put their whole
scale dependence in the depth index j and none in the cube; no 3-power and
no exponent moves anywhere.
What this discharges #
The scale-normalized bridge is the hbridge slot in CoarseGraining's
carriers:
scaleNormalizedNegativeBesovVectorNorm Q 1 (.finite 1) F
≤ Cbr(t) · scaleNormalizedNegativeBesovVectorNorm Q t (.finite 2) F ,
the left side being exactly what Algsuperdiff.Section3.Provider.Besov's
embedding consumes (through cubeBesovNegativeVectorSeminorm, CoarseGraining's
proved
scaleNormalizedNegativeBesovVectorNorm_finite_one_eq_cubeBesovNegativeVectorSeminorm)
and the right side exactly what coarsePoincareRHSTheory produces. hbridge is
therefore no longer a conditional input.
References #
- ABK26, the summability conversion; Step 7d.
- CoarseGraining,
Homogenization/Deterministic/WeakNormInterfaces/Definitions.lean;Homogenization/Book/Ch03/Theorems/PublicInternalBridges/EndPoints.lean.
1. The geometric factor #
The conversion constant (1 - 3^{-2(1-t)})^{-1/2}. At the §4.4 pin t = 1/4 it is (1 - 3^{-3/2})^{-1/2} ≈ 1.1128, absolute.
Equations
Instances For
2. The weight split #
The scale-weight split: 3^{-j} = 3^{-(1-t)j}·3^{-tj} on the proved depth
seminorms.
3. The conversion at every finite depth #
The summability conversion, at every finite depth. The scale-sum Cauchy--Schwarz, with the geometric factor evaluated.
4. hbridge, discharged #
hbridge from a uniform bound. Whenever B dominates every finite-depth
B^{-t}_{2,2} partial seminorm of F, the note-normalized B^{-1}_{2,1}
seminorm is at most C(t)·B.