Documentation

Anderson4D.DetParametrix.Paper42_Moment.R324InitialNestedContextFactorization

Honest physical-to-canonical boundary for the initial R-324 cross suffix #

The exact two-half bridge ends with a complex physical core on the literal initial nested carrier. The proper cross-prefix iteration, by contrast, consumes a nonnegative canonical majorant and stops at the block containing the selected projected covariance.

This file records the missing boundary without identifying those two objects pointwise:

Thus a value of R324InitialNestedContextFactorization is a local, proof-relevant factorization certificate. It is not a target-shaped pointwise density hypothesis and it does not discard the Step 4 endpoint payload.

The correctly weighted physical norm boundary #

noncomputable def Anderson4D.R324TwoHalfTerminalData.initialNestedWeightedNormDensity {ρ : SmoothCutoff} {lam ε : ℝ} {m : ℕ} {κp κm : PartialPairing (Fin m)} (terminal : R324TwoHalfTerminalData ρ lam ε κp κm) (π : ↥κp.singles ≃ ↥κm.singles) (selected : R324ResidualCovarianceSlot κp) (L : ℝ) (x y z w : T4) (v : terminal.NestedCoordinate π → T4) :

The physical norm density with exactly the perturbative weight carried by the initial residual cross schedule. In particular, the weight is not silently charged to the already completed within-half schedules.

Equations
  • One or more equations did not get rendered due to their size.
Instances For
    theorem Anderson4D.R324TwoHalfTerminalData.initialNestedWeightedNormDensity_nonneg {ρ : SmoothCutoff} {lam ε : ℝ} {m : ℕ} {κp κm : PartialPairing (Fin m)} (terminal : R324TwoHalfTerminalData ρ lam ε κp κm) (π : ↥κp.singles ≃ ↥κm.singles) (selected : R324ResidualCovarianceSlot κp) (L : ℝ) (x y z w : T4) (v : terminal.NestedCoordinate π → T4) :
    0 ≤ terminal.initialNestedWeightedNormDensity π selected L x y z w v
    theorem Anderson4D.R324TwoHalfTerminalData.initialNestedWeightedNormDensity_eq_absWeight {ρ : SmoothCutoff} {lam ε : ℝ} {m : ℕ} {κp κm : PartialPairing (Fin m)} (terminal : R324TwoHalfTerminalData ρ lam ε κp κm) (π : ↥κp.singles ≃ ↥κm.singles) (selected : R324ResidualCovarianceSlot κp) (L : ℝ) (x y z w : T4) (v : terminal.NestedCoordinate π → T4) :
    terminal.initialNestedWeightedNormDensity π selected L x y z w v = |lamEps lam ε| ^ (2 * (R324NestedCrossResidualPrefix.initial κp κm π).remainingOrder) * terminal.initialNestedMarkedNormDensity π selected L x y z w v

    Absolute-value spelling of the same weight. The equality uses only that the perturbative exponent is even.

    theorem Anderson4D.R324TwoHalfTerminalData.integrable_initialNestedWeightedNormDensity {ρ : SmoothCutoff} {lam ε : ℝ} {m : ℕ} {κp κm : PartialPairing (Fin m)} (terminal : R324TwoHalfTerminalData ρ lam ε κp κm) (π : ↥κp.singles ≃ ↥κm.singles) (selected : R324ResidualCovarianceSlot κp) (L : ℝ) (x y z w : T4) (hphysical : MeasureTheory.Integrable (terminal.initialNestedMarkedPhysicalCore π selected L x y z w) (MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure)) :
    theorem Anderson4D.R324TwoHalfTerminalData.initialWeight_mul_norm_integral_le_integral_weightedNorm {ρ : SmoothCutoff} {lam ε : ℝ} {m : ℕ} {κp κm : PartialPairing (Fin m)} (terminal : R324TwoHalfTerminalData ρ lam ε κp κm) (π : ↥κp.singles ≃ ↥κm.singles) (selected : R324ResidualCovarianceSlot κp) (L : ℝ) (x y z w : T4) :
    lamEps lam ε ^ (2 * (R324NestedCrossResidualPrefix.initial κp κm π).remainingOrder) * ‖∫ (v : terminal.NestedCoordinate π → T4), terminal.initialNestedMarkedPhysicalCore π selected L x y z w v ∂MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure‖ ≤ ∫ (v : terminal.NestedCoordinate π → T4), terminal.initialNestedWeightedNormDensity π selected L x y z w v ∂MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure

    The weighted physical integral is bounded by the integral of the weighted norm density. This is the last statement which does not mention any canonical proper-prefix majorant.

    theorem Anderson4D.R324TwoHalfTerminalData.absInitialWeight_mul_norm_integral_le_integral_weightedNorm {ρ : SmoothCutoff} {lam ε : ℝ} {m : ℕ} {κp κm : PartialPairing (Fin m)} (terminal : R324TwoHalfTerminalData ρ lam ε κp κm) (π : ↥κp.singles ≃ ↥κm.singles) (selected : R324ResidualCovarianceSlot κp) (L : ℝ) (x y z w : T4) :
    |lamEps lam ε| ^ (2 * (R324NestedCrossResidualPrefix.initial κp κm π).remainingOrder) * ‖∫ (v : terminal.NestedCoordinate π → T4), terminal.initialNestedMarkedPhysicalCore π selected L x y z w v ∂MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure‖ ≤ ∫ (v : terminal.NestedCoordinate π → T4), terminal.initialNestedWeightedNormDensity π selected L x y z w v ∂MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure

    Absolute-value form of the weighted integral boundary.

    theorem Anderson4D.R324TwoHalfTerminalData.norm_complexInitialWeight_mul_integral_eq {ρ : SmoothCutoff} {lam ε : ℝ} {m : ℕ} {κp κm : PartialPairing (Fin m)} (terminal : R324TwoHalfTerminalData ρ lam ε κp κm) (π : ↥κp.singles ≃ ↥κm.singles) (selected : R324ResidualCovarianceSlot κp) (L : ℝ) (x y z w : T4) :
    ‖↑(lamEps lam ε) ^ (2 * (R324NestedCrossResidualPrefix.initial κp κm π).remainingOrder) * ∫ (v : terminal.NestedCoordinate π → T4), terminal.initialNestedMarkedPhysicalCore π selected L x y z w v ∂MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure‖ = lamEps lam ε ^ (2 * (R324NestedCrossResidualPrefix.initial κp κm π).remainingOrder) * ‖∫ (v : terminal.NestedCoordinate π → T4), terminal.initialNestedMarkedPhysicalCore π selected L x y z w v ∂MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure‖

    Norm of the genuinely complex perturbative weight. This equality is the bridge between the complex coefficient identity and the real nonnegative factorization below.

    theorem Anderson4D.R324TwoHalfTerminalData.norm_complexInitialWeight_mul_integral_le_integral_weightedNorm {ρ : SmoothCutoff} {lam ε : ℝ} {m : ℕ} {κp κm : PartialPairing (Fin m)} (terminal : R324TwoHalfTerminalData ρ lam ε κp κm) (π : ↥κp.singles ≃ ↥κm.singles) (selected : R324ResidualCovarianceSlot κp) (L : ℝ) (x y z w : T4) :
    ‖↑(lamEps lam ε) ^ (2 * (R324NestedCrossResidualPrefix.initial κp κm π).remainingOrder) * ∫ (v : terminal.NestedCoordinate π → T4), terminal.initialNestedMarkedPhysicalCore π selected L x y z w v ∂MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure‖ ≤ ∫ (v : terminal.NestedCoordinate π → T4), terminal.initialNestedWeightedNormDensity π selected L x y z w v ∂MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure

    Direct complex-weight form of the physical-to-weighted-norm boundary.

    An endpoint-preserving local factorization certificate #

    @[simp]
    theorem Anderson4D.R324NestedCrossTerminalPayload.ofContext_unscaledDensity {m : ℕ} {κp κm : PartialPairing (Fin m)} {π : ↥κp.singles ≃ ↥κm.singles} (lam ε : ℝ) (step : R324NestedCrossStepContext κp κm π) (context : T4 → T4 → T4 → T4 → (step.SurvivingCoordinate → T4) → ℝ) (x y z w : T4) :
    (ofContext lam ε step context x y z w).unscaledDensity = context x y z w
    @[simp]
    theorem Anderson4D.R324NestedCrossTerminalPayload.ofContext_density {m : ℕ} {κp κm : PartialPairing (Fin m)} {π : ↥κp.singles ≃ ↥κm.singles} (lam ε : ℝ) (step : R324NestedCrossStepContext κp κm π) (context : T4 → T4 → T4 → T4 → (step.SurvivingCoordinate → T4) → ℝ) (x y z w : T4) :
    (ofContext lam ε step context x y z w).density = fun (v : step.SurvivingCoordinate → T4) => lamEps lam ε ^ (2 * step.residual.remainingOrder) * context x y z w v
    theorem Anderson4D.R324NestedCrossStepContext.ae_post_comp_le {m : ℕ} {κp κm : PartialPairing (Fin m)} {π : ↥κp.singles ≃ ↥κm.singles} (ctx : R324NestedCrossStepContext κp κm π) {f g : (ctx.PostCoordinate → T4) → ℝ} (hfg : f ≤ᵐ[MeasureTheory.Measure.pi fun (x : ctx.PostCoordinate) => paperMeasure] g) :
    (fun (v : ctx.SurvivingCoordinate → T4) => f fun (i : ctx.PostCoordinate) => v (ctx.postSurvivingCoordinate i)) ≤ᵐ[MeasureTheory.Measure.pi fun (x : ctx.SurvivingCoordinate) => paperMeasure] fun (v : ctx.SurvivingCoordinate → T4) => g fun (i : ctx.PostCoordinate) => v (ctx.postSurvivingCoordinate i)

    Pull an a.e. comparison on the next suffix back to the current surviving carrier. This is the measure-theoretic step needed to compose honest one-head comparisons; it is not an additional majorization hypothesis.

    inductive Anderson4D.R324NestedCrossContextFactorization {m : ℕ} {κp κm : PartialPairing (Fin m)} {π : ↥κp.singles ≃ ↥κm.singles} (ρ : SmoothCutoff) (lam ε : ℝ) (stopCarrier : Finset (Fin (2 * m))) (x y z w : T4) (res : R324NestedCrossResidualPrefix κp κm π) :
    ((↥res.activeCarrier → T4) → ℝ) → ((↥res.activeCarrier → T4) → ℝ) → ℕ → ℕ → Prop

    A local, a.e. physical factorization along the proper prefix before a chosen stop carrier.

    The source field is the physical density still to be controlled at the current suffix. The majorant field is forced constructor-by-constructor to be the canonical run density. At stop, its context still receives all four external endpoints. Integrability is stored recursively so every suffix needed by the later Bochner/Fubini iteration is available.

    Instances For
      theorem Anderson4D.R324NestedCrossContextFactorization.toProperPrefixRun {m : ℕ} {κp κm : PartialPairing (Fin m)} {π : ↥κp.singles ≃ ↥κm.singles} {ρ : SmoothCutoff} {lam ε : ℝ} {stopCarrier : Finset (Fin (2 * m))} {x y z w : T4} {res : R324NestedCrossResidualPrefix κp κm π} {source majorant : (↥res.activeCarrier → T4) → ℝ} {prefixOrder terminalOrder : ℕ} (factorization : R324NestedCrossContextFactorization ρ lam ε stopCarrier x y z w res source majorant prefixOrder terminalOrder) :
      R324NestedCrossProperPrefixRun ρ lam ε stopCarrier res majorant prefixOrder terminalOrder

      Forgetting the physical comparison leaves exactly the canonical proper-prefix run consumed by the cross iteration.

      theorem Anderson4D.R324NestedCrossContextFactorization.ae_le {m : ℕ} {κp κm : PartialPairing (Fin m)} {π : ↥κp.singles ≃ ↥κm.singles} {ρ : SmoothCutoff} {lam ε : ℝ} {stopCarrier : Finset (Fin (2 * m))} {x y z w : T4} {res : R324NestedCrossResidualPrefix κp κm π} {source majorant : (↥res.activeCarrier → T4) → ℝ} {prefixOrder terminalOrder : ℕ} (factorization : R324NestedCrossContextFactorization ρ lam ε stopCarrier x y z w res source majorant prefixOrder terminalOrder) :
      source ≤ᵐ[MeasureTheory.Measure.pi fun (x : ↥res.activeCarrier) => paperMeasure] majorant

      The source-to-majorant comparison obtained by composing the honest one-head comparison with the recursively generated next-suffix comparison.

      theorem Anderson4D.R324NestedCrossContextFactorization.majorant_integrable {m : ℕ} {κp κm : PartialPairing (Fin m)} {π : ↥κp.singles ≃ ↥κm.singles} {ρ : SmoothCutoff} {lam ε : ℝ} {stopCarrier : Finset (Fin (2 * m))} {x y z w : T4} {res : R324NestedCrossResidualPrefix κp κm π} {source majorant : (↥res.activeCarrier → T4) → ℝ} {prefixOrder terminalOrder : ℕ} (factorization : R324NestedCrossContextFactorization ρ lam ε stopCarrier x y z w res source majorant prefixOrder terminalOrder) :

      Integrability is retained at every suffix, not merely at the initial carrier. This is the recursive datum required by the proper-head Bochner/Fubini iteration.

      theorem Anderson4D.R324NestedCrossContextFactorization.majorant_nonneg {m : ℕ} {κp κm : PartialPairing (Fin m)} {π : ↥κp.singles ≃ ↥κm.singles} {ρ : SmoothCutoff} {lam ε : ℝ} {stopCarrier : Finset (Fin (2 * m))} {x y z w : T4} {res : R324NestedCrossResidualPrefix κp κm π} {source majorant : (↥res.activeCarrier → T4) → ℝ} {prefixOrder terminalOrder : ℕ} (factorization : R324NestedCrossContextFactorization ρ lam ε stopCarrier x y z w res source majorant prefixOrder terminalOrder) (v : ↥res.activeCarrier → T4) :
      0 ≤ majorant v

      Every canonical majorant produced by the certificate is pointwise nonnegative.

      The initial package and its integral-level consumer #

      structure Anderson4D.R324InitialNestedContextFactorization (ρ : SmoothCutoff) (lam ε : ℝ) {m : ℕ} (κp κm : PartialPairing (Fin m)) (π : ↥κp.singles ≃ ↥κm.singles) (selected : R324ResidualCovarianceSlot κp) (terminal : R324TwoHalfTerminalData ρ lam ε κp κm) (L : ℝ) (x y z w : T4) :

      Complete factorization datum at the output of the exact two-half bridge, including the local certificate and its suffix-by-suffix integrability data.

      Instances For
        theorem Anderson4D.R324InitialNestedContextFactorization.toProperPrefixRun {ρ : SmoothCutoff} {lam ε : ℝ} {m : ℕ} {κp κm : PartialPairing (Fin m)} {π : ↥κp.singles ≃ ↥κm.singles} {selected : R324ResidualCovarianceSlot κp} {terminal : R324TwoHalfTerminalData ρ lam ε κp κm} {L : ℝ} {x y z w : T4} (factorization : R324InitialNestedContextFactorization ρ lam ε κp κm π selected terminal L x y z w) :
        R324NestedCrossProperPrefixRun ρ lam ε (r324MarkedResidualBlock κp κm π selected) (R324NestedCrossResidualPrefix.initial κp κm π) factorization.majorant factorization.prefixOrder factorization.terminalOrder

        The packaged majorant carries the canonical stop-at-marked run.

        theorem Anderson4D.R324InitialNestedContextFactorization.majorant_integrable {ρ : SmoothCutoff} {lam ε : ℝ} {m : ℕ} {κp κm : PartialPairing (Fin m)} {π : ↥κp.singles ≃ ↥κm.singles} {selected : R324ResidualCovarianceSlot κp} {terminal : R324TwoHalfTerminalData ρ lam ε κp κm} {L : ℝ} {x y z w : T4} (factorization : R324InitialNestedContextFactorization ρ lam ε κp κm π selected terminal L x y z w) :

        Initial-carrier integrability, projected from the recursive suffix-by-suffix certificate.

        theorem Anderson4D.R324InitialNestedContextFactorization.majorant_nonneg {ρ : SmoothCutoff} {lam ε : ℝ} {m : ℕ} {κp κm : PartialPairing (Fin m)} {π : ↥κp.singles ≃ ↥κm.singles} {selected : R324ResidualCovarianceSlot κp} {terminal : R324TwoHalfTerminalData ρ lam ε κp κm} {L : ℝ} {x y z w : T4} (factorization : R324InitialNestedContextFactorization ρ lam ε κp κm π selected terminal L x y z w) (v : terminal.NestedCoordinate π → T4) :
        0 ≤ factorization.majorant v

        Initial canonical majorant is pointwise nonnegative.

        theorem Anderson4D.R324InitialNestedContextFactorization.prefixOrder_add_terminalOrder {ρ : SmoothCutoff} {lam ε : ℝ} {m : ℕ} {κp κm : PartialPairing (Fin m)} {π : ↥κp.singles ≃ ↥κm.singles} {selected : R324ResidualCovarianceSlot κp} {terminal : R324TwoHalfTerminalData ρ lam ε κp κm} {L : ℝ} {x y z w : T4} (factorization : R324InitialNestedContextFactorization ρ lam ε κp κm π selected terminal L x y z w) :

        The exact perturbative weight splits into the proper-prefix order and the terminal marked/suffix order recorded by the canonical run.

        theorem Anderson4D.R324InitialNestedContextFactorization.initialWeight_mul_norm_integral_le_majorant {ρ : SmoothCutoff} {lam ε : ℝ} {m : ℕ} {κp κm : PartialPairing (Fin m)} {π : ↥κp.singles ≃ ↥κm.singles} {selected : R324ResidualCovarianceSlot κp} {terminal : R324TwoHalfTerminalData ρ lam ε κp κm} {L : ℝ} {x y z w : T4} (factorization : R324InitialNestedContextFactorization ρ lam ε κp κm π selected terminal L x y z w) (hphysical : MeasureTheory.Integrable (terminal.initialNestedMarkedPhysicalCore π selected L x y z w) (MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure)) :
        lamEps lam ε ^ (2 * (R324NestedCrossResidualPrefix.initial κp κm π).remainingOrder) * ‖∫ (v : terminal.NestedCoordinate π → T4), terminal.initialNestedMarkedPhysicalCore π selected L x y z w v ∂MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure‖ ≤ ∫ (v : terminal.NestedCoordinate π → T4), factorization.majorant v ∂MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure

        Main integral-level handoff. It keeps the four external endpoints in the terminal payload while allowing every earlier proper block to be consumed by the canonical cross iteration.

        theorem Anderson4D.R324InitialNestedContextFactorization.norm_complexInitialWeight_mul_integral_le_majorant {ρ : SmoothCutoff} {lam ε : ℝ} {m : ℕ} {κp κm : PartialPairing (Fin m)} {π : ↥κp.singles ≃ ↥κm.singles} {selected : R324ResidualCovarianceSlot κp} {terminal : R324TwoHalfTerminalData ρ lam ε κp κm} {L : ℝ} {x y z w : T4} (factorization : R324InitialNestedContextFactorization ρ lam ε κp κm π selected terminal L x y z w) (hphysical : MeasureTheory.Integrable (terminal.initialNestedMarkedPhysicalCore π selected L x y z w) (MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure)) :
        ‖↑(lamEps lam ε) ^ (2 * (R324NestedCrossResidualPrefix.initial κp κm π).remainingOrder) * ∫ (v : terminal.NestedCoordinate π → T4), terminal.initialNestedMarkedPhysicalCore π selected L x y z w v ∂MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure‖ ≤ ∫ (v : terminal.NestedCoordinate π → T4), factorization.majorant v ∂MeasureTheory.Measure.pi fun (x : terminal.NestedCoordinate π) => paperMeasure

        Consumer-facing complex form of the same endpoint-preserving handoff.