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LeanPool.Superdiffusion.Algsuperdiff.Section3.Observable.CutoffMultiscaleEllipticity

CutoffMultiscaleEllipticity #

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

Measurable multiscale ellipticity of the actual cutoff #

The raw quantities below are the Chapter 4 canonical coefficient-family observables of the literal cutoff a_r = nu Id + k_r. On the source range 0 < s, the exported functions are the literal observables clamped at 0; they are genuinely measurable, and they agree with the literals everywhere on the source range, not merely almost everywhere. The positivity proof is a well-definedness input, not a probabilistic or analytic hypothesis: every Section 3 source window already entails it.

Main definitions #

Main results #

noncomputable def Algsuperdiff.Section3.Observable.cutoffLowerEllipticityInvLiteral {d : ℕ} (M : ABKModel d) (domainScale cutoffScale : ℤ) (s : ℝ) (q : CoarseEllipticityExponent) :

Literal inverse lower multiscale ellipticity of the actual cutoff field. This is not selected as a measurable representative.

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    noncomputable def Algsuperdiff.Section3.Observable.cutoffUpperEllipticityLiteral {d : ℕ} (M : ABKModel d) (domainScale cutoffScale : ℤ) (s : ℝ) (q : CoarseEllipticityExponent) :

    Literal upper multiscale ellipticity of the actual cutoff field. This is not selected as a measurable representative.

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      theorem Algsuperdiff.Section3.Observable.measurable_cutoffLowerEllipticityInvLiteral {d : ℕ} (M : ABKModel d) (domainScale cutoffScale : ℤ) {s : ℝ} (hs : 0 < s) (q : CoarseEllipticityExponent) :
      Measurable (cutoffLowerEllipticityInvLiteral M domainScale cutoffScale s q)

      Genuine measurability of the centered inverse lower multiscale ellipticity literal, from the carrier-source engine at the centered cube.

      theorem Algsuperdiff.Section3.Observable.measurable_cutoffUpperEllipticityLiteral {d : ℕ} (M : ABKModel d) (domainScale cutoffScale : ℤ) {s : ℝ} (hs : 0 < s) (q : CoarseEllipticityExponent) :
      Measurable (cutoffUpperEllipticityLiteral M domainScale cutoffScale s q)

      Genuine measurability of the centered upper multiscale ellipticity literal, from the carrier-source engine at the centered cube.

      noncomputable def Algsuperdiff.Section3.Observable.cutoffLowerEllipticityInv {d : ℕ} (M : ABKModel d) (domainScale cutoffScale : ℤ) (s : ℝ) (_hs : 0 < s) (q : CoarseEllipticityExponent) :

      The actual inverse lower multiscale ellipticity: the literal, clamped at 0.

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      • One or more equations did not get rendered due to their size.
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        noncomputable def Algsuperdiff.Section3.Observable.cutoffUpperEllipticity {d : ℕ} (M : ABKModel d) (domainScale cutoffScale : ℤ) (s : ℝ) (_hs : 0 < s) (q : CoarseEllipticityExponent) :

        The actual upper multiscale ellipticity: the literal, clamped at 0.

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        • One or more equations did not get rendered due to their size.
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          theorem Algsuperdiff.Section3.Observable.measurable_cutoffLowerEllipticityInv {d : ℕ} (M : ABKModel d) (domainScale cutoffScale : ℤ) (s : ℝ) (hs : 0 < s) (q : CoarseEllipticityExponent) :
          Measurable (cutoffLowerEllipticityInv M domainScale cutoffScale s hs q)
          theorem Algsuperdiff.Section3.Observable.measurable_cutoffUpperEllipticity {d : ℕ} (M : ABKModel d) (domainScale cutoffScale : ℤ) (s : ℝ) (hs : 0 < s) (q : CoarseEllipticityExponent) :
          Measurable (cutoffUpperEllipticity M domainScale cutoffScale s hs q)
          theorem Algsuperdiff.Section3.Observable.cutoffLowerEllipticityInv_nonneg {d : ℕ} (M : ABKModel d) (domainScale cutoffScale : ℤ) (s : ℝ) (hs : 0 < s) (q : CoarseEllipticityExponent) (omega : Cutoff.CutoffSample d) :
          0 ≤ cutoffLowerEllipticityInv M domainScale cutoffScale s hs q omega
          theorem Algsuperdiff.Section3.Observable.cutoffUpperEllipticity_nonneg {d : ℕ} (M : ABKModel d) (domainScale cutoffScale : ℤ) (s : ℝ) (hs : 0 < s) (q : CoarseEllipticityExponent) (omega : Cutoff.CutoffSample d) :
          0 ≤ cutoffUpperEllipticity M domainScale cutoffScale s hs q omega
          theorem Algsuperdiff.Section3.Observable.cutoffLowerEllipticityInv_eq_literal {d : ℕ} (M : ABKModel d) (domainScale cutoffScale : ℤ) (s : ℝ) (hs : 0 < s) (q : CoarseEllipticityExponent) :
          cutoffLowerEllipticityInv M domainScale cutoffScale s hs q = cutoffLowerEllipticityInvLiteral M domainScale cutoffScale s q

          The exported inverse lower observable is its literal, at every sample point. This is the payoff of the body swap: the clamp is inert because the literal is nonnegative on the source range 0 < s.

          theorem Algsuperdiff.Section3.Observable.cutoffUpperEllipticity_eq_literal {d : ℕ} (M : ABKModel d) (domainScale cutoffScale : ℤ) (s : ℝ) (hs : 0 < s) (q : CoarseEllipticityExponent) :
          cutoffUpperEllipticity M domainScale cutoffScale s hs q = cutoffUpperEllipticityLiteral M domainScale cutoffScale s q

          The exported upper observable is its literal, at every sample point.

          theorem Algsuperdiff.Section3.Observable.cutoffLowerEllipticityInv_ae_eq_literal {d : ℕ} (M : ABKModel d) (domainScale cutoffScale : ℤ) (s : ℝ) (hs : 0 < s) (q : CoarseEllipticityExponent) :
          cutoffLowerEllipticityInv M domainScale cutoffScale s hs q =ᵐ[↑(Cutoff.cutoffSampleLaw M)] cutoffLowerEllipticityInvLiteral M domainScale cutoffScale s q
          theorem Algsuperdiff.Section3.Observable.cutoffUpperEllipticity_ae_eq_literal {d : ℕ} (M : ABKModel d) (domainScale cutoffScale : ℤ) (s : ℝ) (hs : 0 < s) (q : CoarseEllipticityExponent) :
          cutoffUpperEllipticity M domainScale cutoffScale s hs q =ᵐ[↑(Cutoff.cutoffSampleLaw M)] cutoffUpperEllipticityLiteral M domainScale cutoffScale s q