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Anderson4D.DetParametrix.Paper41_Renorm.R322OneBlockCollapse

Closing one proper-block collapse #

Paper: R-322 — §4.1 — closing one proper-block collapse

This file inserts the three-region inner estimate into the concrete two-variable collapse of (4.8). The first step records the Haar change of variables u = q - w; the second is the Fubini identity which exposes r322GreenDifferenceSection in the outer integral.

Translation-reflection invariance of paper measure in exactly the orientation used by the proper-block collapse.

Fubini and the translated Haar change of variables turn the concrete collapse into the outer convolution of the left input with the Green difference section.

Joint integrability of the concrete collapse supplies integrability of its section form; no separate Fubini hypothesis is needed later.

Integrability of the three outer profiles #

theorem Anderson4D.integrable_r322TaylorDensity_convolution {supportConstant C lam ε : ℝ} {n : ℕ} {x : T4} (hsupport : 0 < supportConstant) (hC : 0 ≤ C) (hlam : 0 ≤ lam) (hε : 0 < ε) (hε1 : ε ≤ 1) (hlog : 1 ≤ |Real.log ε|) :
MeasureTheory.Integrable (fun (q : T4) => invSqKer (x - q) * r322TaylorDensity C lam ε supportConstant n q) paperMeasure
theorem Anderson4D.integrable_r322RegionTwoDensity_convolution {supportConstant C lam ε : ℝ} {n : ℕ} {x : T4} (hsupport : 0 < supportConstant) (hC : 0 ≤ C) (hlam : 0 ≤ lam) (hε : 0 < ε) (hε1 : ε ≤ 1) (hlog : 1 ≤ |Real.log ε|) (hx : x ≠ 0) :
MeasureTheory.Integrable (fun (q : T4) => invSqKer (x - q) * r322RegionTwoDensity C lam ε supportConstant n q) paperMeasure
theorem Anderson4D.integrable_r322RegionThreeDensity_convolution {supportConstant C lam ε : ℝ} {n : ℕ} {x : T4} (hsupport : 0 < supportConstant) (hC : 0 ≤ C) (hlam : 0 ≤ lam) (hε : 0 < ε) (hε1 : ε ≤ 1) (hlog : 1 ≤ |Real.log ε|) :
MeasureTheory.Integrable (fun (q : T4) => invSqKer (x - q) * r322RegionThreeDensity C lam ε supportConstant n q) paperMeasure

Quantitative closure of one block #

theorem Anderson4D.exists_r322Collapse_le {supportConstant : ℝ} (hsupport : 0 < supportConstant) :
∃ (K : ℝ), 0 < K ∧ ∀ (C lam ε A : ℝ) (n : ℕ) (Gp J : T4 → ℝ) (x : T4), 0 ≤ C → 0 ≤ lam → 0 ≤ A → 0 < ε → ε ≤ 1 → 1 ≤ |Real.log ε| → x ≠ 0 → Measurable J → MemEClassT4 J → (∀ (u : T4), |J u| ≤ primitiveKernelMajorant C lam ε supportConstant n u) → (∀ (z : T4), z ≠ 0 → |Gp z| ≤ A * invSqKer z) → MeasureTheory.Integrable (r322CollapseIntegrand Gp J greenFn x) (paperMeasure.prod paperMeasure) → |r322Collapse Gp J greenFn x| ≤ A * (C * lam) ^ (2 * n) * K * invSqKer x

A proper primitive block can be collapsed without losing the inverse-square input class. The constant is chosen once before the scale, coupling, order, input kernel, primitive block, and endpoint.

theorem Anderson4D.exists_normalized_r322Collapse_admissible {supportConstant : ℝ} (hsupport : 0 < supportConstant) :
∃ (K : ℝ), 0 < K ∧ ∀ (C lam ε A : ℝ) (n : ℕ) (Gp J : T4 → ℝ), 0 < C → 0 < lam → 0 < A → 0 < ε → ε ≤ 1 → 1 ≤ |Real.log ε| → Measurable J → MemEClassT4 Gp → MemEClassT4 J → (∀ (u : T4), |J u| ≤ primitiveKernelMajorant C lam ε supportConstant n u) → (∀ (z : T4), z ≠ 0 → |Gp z| ≤ A * invSqKer z) → (∀ (x : T4), MeasureTheory.Integrable (r322CollapseIntegrand Gp J greenFn x) (paperMeasure.prod paperMeasure)) → ∀ (m : ℕ), IsAdmissiblePrimitiveInput m fun (x : Fin (2 * m - 1)) => normalizedOffDiagonalRepresentative (A * (C * lam) ^ (2 * n) * K) (r322Collapse Gp J greenFn)

After dividing by its proved scale factor and changing only the null diagonal, a collapsed kernel is an admissible input in every later use of Proposition 4.1. This is the analytic induction interface behind (4.13).

Abstract iteration of the analytic collapse #

structure Anderson4D.R322AnalyticStage (C lam ε supportConstant : ℝ) :

One already-summed primitive coordinate in the interval reduction. Its fields are exactly the outputs of Proposition 4.1 used in (4.13).

Instances For
    def Anderson4D.r322Iterate {C lam ε supportConstant : ℝ} (Gp : T4 → ℝ) :
    List (R322AnalyticStage C lam ε supportConstant) → T4 → ℝ

    Successively insert the collapsed input produced by each primitive coordinate into the left Green slot of the next coordinate.

    Equations
    Instances For
      def Anderson4D.R322IterationIntegrable {C lam ε supportConstant : ℝ} (Gp : T4 → ℝ) :
      List (R322AnalyticStage C lam ε supportConstant) → Prop

      Exact Fubini licenses required by the successive concrete collapses.

      Equations
      Instances For
        theorem Anderson4D.r322Iterate_memE {C lam ε supportConstant : ℝ} {Gp : T4 → ℝ} (hGp : MemEClassT4 Gp) (stages : List (R322AnalyticStage C lam ε supportConstant)) :
        theorem Anderson4D.exists_r322Iterate_le {supportConstant : ℝ} (hsupport : 0 < supportConstant) :
        ∃ (K : ℝ), 0 < K ∧ ∀ (C lam ε A : ℝ) (stages : List (R322AnalyticStage C lam ε supportConstant)) (Gp : T4 → ℝ) (x : T4), 0 ≤ C → 0 ≤ lam → 0 ≤ A → 0 < ε → ε ≤ 1 → 1 ≤ |Real.log ε| → x ≠ 0 → (∀ (z : T4), z ≠ 0 → |Gp z| ≤ A * invSqKer z) → R322IterationIntegrable Gp stages → |r322Iterate Gp stages x| ≤ A * K ^ stages.length * (C * lam) ^ (2 * (List.map R322AnalyticStage.order stages).sum) * invSqKer x

        Quantitative induction for paper (4.13). Every removed primitive coordinate contributes its exact perturbative order and one universal collapse constant; no scale or order dependence is hidden in that constant.