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LeanPool.Superdiffusion.Algsuperdiff.Section4.Provider.Homogenization.HomStepOneMoment

HomStepOneMoment #

Ported from scottnarmstrong/Superdiffusion at 7f20476385d4af418f110303085ad0740c9eba46. Module imports, support namespace and local option directives adapted for Lean Pool.

Theorem B, §4.5, Step 1: the Hölder assembly of the EthmB(m) moment #

The target #

Step 1 ends with the sentence

"Combining this estimate with the bounds_mathcal_E_aL lemma, using Hölder's inequality and s = |log γ|⁻¹, we obtain the moment bound announced in the 𝓔 estimate."

It is recorded that the Hölder bookkeeping is asserted, not displayed. This module reconstructs it in full. EthmB(m) is the sum of two products

T₁ = s⁻¹ · Y · ( 𝓔_{s₁} · (1 + 𝓔_{1/4}) ),     T₂ = C γ⁵ · ( 1 + 𝓔²_{s₁/2} ),

so the exponent boosts are 2 on the outer product, 4 on the inner one and 2 on the square — NOT the uniform 3 a naive three-factor Hölder would ask for. The assembly is therefore:

objectexponent at which it is consumed
Y = 3^{(1-α)X_m(α)}2p
𝓔_{s₁,∞,2}(□_m, n; ·)4p
𝓔_{1/4,∞,2}(□_m; ·)4p
𝓔_{s₁/2,∞,2}(□_m, n; ·)2p

The conditional edge (the ONE in this lane) #

Y and its moment are the only inputs this module does not produce. Y is the minimal-scale factor 3^{(1-α) X_m(α)} and its moment bound

𝔼[ (3^{(1-α)X_m(α)})^{2p} ] ≤ 2^{2p}

is the Markov/Γ₁ step of Step 1, whose input is clause (a) of Theorem C (X_m(α) = 𝒪_{Γ₁}(C γ (1-α)^{-2})). Per the conditional-edge device it enters here as a NAMED TRANSCRIBED HYPOTHESIS (hY), at the single exponent 2p at which it is consumed — never by importing Theorem C itself. Theorem C is a declared dependency of this step, so this is a node-internal edge, not a side assumption. NOTE for the consumer: the printed range of the Markov step is p ≤ C⁻¹(1-α)γ⁻¹ with 1 - α = s/2; the caller must respect it when discharging hY.

The output shape #

The assembled majorant is left FACTORED,

s⁻¹ · ( R_Y · ( R₁ · (1 + R₂) ) )  +  C γ⁵ · ( 1 + R₃² ),

with R_Y, R₁, R₂, R₃ the caller's own factor majorants (R_Y = 2 at the plain Theorem-C edge; the enlarged-Y re-pin passes the 𝓔-boosted majorant instead — the interface generalization). This is the honest output of Hölder: not one power of γ, of s, or of |log γ| has been moved or absorbed ( forbids silent absorption of s-powers, since s = s(γ) is not a constant). The numeric collapse to the printed display C(√p + √|log γ|)√γ |log γ|² is a separate, separately auditable step.

1. Two generic ℝ≥0∞ moment tools #

theorem Algsuperdiff.Section4.Provider.Homogenization.lintegral_rpow_le_of_exponent_le {Omega : Type u_1} [MeasurableSpace Omega] {mu : MeasureTheory.Measure Omega} [MeasureTheory.IsProbabilityMeasure mu] {F : Omega → ENNReal} {R a b : ℝ} (hFm : AEMeasurable F mu) (ha : 0 < a) (hab : a ≤ b) (h : ∫⁻ (omega : Omega), F omega ^ b ∂mu ≤ ENNReal.ofReal R ^ b) :
∫⁻ (omega : Omega), F omega ^ a ∂mu ≤ ENNReal.ofReal R ^ a

Exponent monotonicity (Lyapunov) in the normal form.

On a probability space the normal form at a LARGER exponent implies it at a smaller one, with the SAME majorant. This is what lets the Step-1 assembly consume the anchor at the boosted exponent q = max(4p, 2d s'⁻¹) and still read the result at 4p:'s threshold q ≥ 2 d s'⁻¹ is respected without weakening the conclusion.

theorem Algsuperdiff.Section4.Provider.Homogenization.lintegral_rpow_add_le_of_moments {Omega : Type u_1} [MeasurableSpace Omega] {mu : MeasureTheory.Measure Omega} {F G : Omega → ENNReal} {RF RG q : ℝ} (hq : 1 ≤ q) (hF : AEMeasurable F mu) (hG : AEMeasurable G mu) (hRF : 0 ≤ RF) (hRG : 0 ≤ RG) (h1 : ∫⁻ (omega : Omega), F omega ^ q ∂mu ≤ ENNReal.ofReal RF ^ q) (h2 : ∫⁻ (omega : Omega), G omega ^ q ∂mu ≤ ENNReal.ofReal RG ^ q) :
∫⁻ (omega : Omega), (F omega + G omega) ^ q ∂mu ≤ ENNReal.ofReal (RF + RG) ^ q

The two-term Minkowski step, in the normal form.

The constant observable 1 sits in the normal form with majorant 1.

2. The assembly #

theorem Algsuperdiff.Section4.Provider.Homogenization.ethmB_moment_of_factor_moments {d : ℕ} (M : Section3.ABKModel d) {m n : ℤ} (hnm : n ≤ m) (s : { s : ℝ // 0 < s }) (Y : Section3.Cutoff.CutoffSample d → ENNReal) (hYm : AEMeasurable Y ↑(Section3.Cutoff.cutoffSampleLaw M)) {Cgap : ℝ} (hCgap : 0 ≤ Cgap) {p : ℝ} (hp : 1 ≤ p) {RY R1 R2 R3 : ℝ} (hRY : 0 ≤ RY) (hR1 : 0 ≤ R1) (hR2 : 0 ≤ R2) (hR3 : 0 ≤ R3) (hY : ∫⁻ (omega : Section3.Cutoff.CutoffSample d), Y omega ^ (2 * p) ∂↑(Section3.Cutoff.cutoffSampleLaw M) ≤ ENNReal.ofReal RY ^ (2 * p)) (h1 : ∫⁻ (omega : Section3.Cutoff.CutoffSample d), Support.fluxCorrectedTwoScaleErrorObservableSup M m n (homHalf s) omega ^ (4 * p) ∂↑(Section3.Cutoff.cutoffSampleLaw M) ≤ ENNReal.ofReal R1 ^ (4 * p)) (h2 : ∫⁻ (omega : Section3.Cutoff.CutoffSample d), Support.fluxCorrectedTwoScaleErrorObservableSup M m m homQuarter omega ^ (4 * p) ∂↑(Section3.Cutoff.cutoffSampleLaw M) ≤ ENNReal.ofReal R2 ^ (4 * p)) (h3 : ∫⁻ (omega : Section3.Cutoff.CutoffSample d), Support.fluxCorrectedTwoScaleErrorObservableSup M m n (homQuarterOf s) omega ^ (2 * p) ∂↑(Section3.Cutoff.cutoffSampleLaw M) ≤ ENNReal.ofReal R3 ^ (2 * p)) :
∫⁻ (omega : Section3.Cutoff.CutoffSample d), ethmB M Cgap Y m n s omega ^ p ∂↑(Section3.Cutoff.cutoffSampleLaw M) ≤ ENNReal.ofReal ((↑s)⁻¹ * (RY * (R1 * (1 + R2))) + Cgap * M.gamma ^ 5 * (1 + R3 ^ 2)) ^ p

STEP 1's HÖLDER ASSEMBLY.

Given the four factor moments — the minimal-scale factor Y at exponent 2p with majorant R_Y and the three 𝓔-factors at 4p, 4p, 2p — the defect EthmB(m) obeys this development normal form at p with the factored majorant

s⁻¹ · ( R_Y · ( R₁ · (1 + R₂) ) )  +  C γ⁵ · ( 1 + R₃² ).

Nothing is absorbed: this is the source's "using Hölder's inequality" written out.