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LeanPool.HighContrastHomogenization.Support.Sobolev.Foundations.CubeCalderonZygmund.AxisCubeHarmonicCovariance

Coarse-graining support: #

Support.Sobolev.Foundations.CubeCalderonZygmund.AxisCubeHarmonicCovariance

Imported from the Apache-2.0 CoarseGraining development at commit c7ddd76c08ade64fed1b8d2ca51be14dfee8deb4.

noncomputable def HCPolySupport.CubeCalderonZygmund.axisCubeCenter {d : ℕ} (z : Vec d) (L : ℝ) :
Vec d

The center of the open axis cube axisCube z L.

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    noncomputable def HCPolySupport.CubeCalderonZygmund.axisCubeAffine {d : ℕ} (z : Vec d) (L : ℝ) :
    Vec d → Vec d

    The affine formula which, for positive L, maps the centered unit triadic cube to axisCube z L.

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      noncomputable def HCPolySupport.CubeCalderonZygmund.axisCubeAffineInv {d : ℕ} (z : Vec d) (L : ℝ) :
      Vec d → Vec d

      The inverse affine formula, which is an actual inverse when L ≠ 0.

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        noncomputable def HCPolySupport.CubeCalderonZygmund.axisCubeAffineMeasurableEquiv {d : ℕ} (z : Vec d) {L : ℝ} (hL : L ≠ 0) :

        The affine parametrization as a measurable equivalence of the ambient Euclidean space when its scale is nonzero.

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          @[simp]
          theorem HCPolySupport.CubeCalderonZygmund.axisCubeAffine_comp {d : ℕ} (z w : Vec d) (L S : ℝ) (x : Vec d) :
          axisCubeAffine z L (axisCubeAffine w S x) = axisCubeAffine (fun (i : Fin d) => L * w i + axisCubeCenter z L i) (L * S) x

          An arbitrary positive-length axis cube is the centered-unit triadic cube, dilated by its side length and translated to its center.

          The positive affine parametrization maps the centered unit cube exactly onto its target axis cube.

          The target axis cube has the centered unit cube as its exact preimage under the positive affine parametrization.

          theorem HCPolySupport.CubeCalderonZygmund.axisCubeAffine_image_axisCube {d : ℕ} (z w : Vec d) (L S : ℝ) (hL : 0 < L) (hS : 0 < S) :
          axisCubeAffine z L '' axisCube w S = axisCube (fun (i : Fin d) => L * w i + axisCubeCenter z L i) (L * S)

          A positive affine cube parametrization maps every positive axis cube to the axis cube with the expected affine corner and product side length.

          theorem HCPolySupport.CubeCalderonZygmund.axisCubeAffine_preimage_axisCube_affine {d : ℕ} (z w : Vec d) (L S : ℝ) (hL : 0 < L) (hS : 0 < S) :
          axisCubeAffine z L ⁻¹' axisCube (fun (i : Fin d) => L * w i + axisCubeCenter z L i) (L * S) = axisCube w S

          Exact preimage form of axisCubeAffine_image_axisCube.

          Lower corner of the open axis-cube realization of a triadic cube.

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            Every open triadic cube is exactly its lower-corner axis cube.

            Side length of the concentric depth-n contraction of axisCube z L.

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              noncomputable def HCPolySupport.CubeCalderonZygmund.axisCubeConcentricDepthCorner {d : ℕ} (z : Vec d) (L : ℝ) (n : ℕ) :
              Vec d

              Lower corner of the concentric depth-n contraction of axisCube z L.

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                The outer affine parametrization maps the centered depth-n source cube exactly to the corresponding concentric contraction of its target cube.

                Exact preimage form of the fixed concentric depth transport.

                Homogeneous weak Poisson equations are invariant under the gradient-preserving pullback from a • U to U.

                Homogeneous weak Poisson equations are invariant under translation pullback.

                noncomputable def HCPolySupport.CubeCalderonZygmund.axisCubeHarmonicPullback {d : ℕ} (z : Vec d) {L : ℝ} (hL : 0 < L) (u : H1Function (axisCube z L)) :

                Pull an H¹ function on a positive-length axis cube back to the fixed centered unit triadic cube, with the standard value normalization that leaves the gradient unscaled.

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                  Pullback to the centered unit cube preserves the homogeneous weak Poisson equation.

                  The pushforward of centered-unit Lebesgue measure through the affine map. For positive L, axisCubeNormalizedMeasure_eq_smul_volume_restrict below identifies this with normalized Lebesgue measure on axisCube z L. No such axis-cube interpretation is claimed for nonpositive L.

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                    For positive side length, the affine pushforward is exactly normalized Lebesgue measure on the target axis cube.

                    On a triadic cube, the affine pushforward normalization agrees exactly with the project's canonical normalizedCubeMeasure.

                    Affine pushforward of an affine-cube normalized measure is the normalized measure with the composed affine corner and product scale. This identity is purely a pushforward identity and therefore does not require positive scales.

                    The affine map preserves the centered-unit source measure and its pushforward measure.

                    For nonzero scale, the inverse affine map preserves the pushforward measure back to centered-unit Lebesgue measure.

                    Strong a.e. measurability can be transported in either direction through the nondegenerate affine parametrization.

                    MemLp is equivalent on the source and target of every nondegenerate affine cube parametrization. In particular, target integrability can be deduced from source integrability without a circular target-measurability hypothesis.

                    The fixed centered depth-n source measure pushes forward to the exact normalized measure on the target concentric contraction.

                    Bidirectional strong a.e. measurability transport on a fixed concentric depth.

                    Bidirectional MemLp transport on the fixed centered depth-n source and its target concentric contraction.

                    The affine parametrization preserves every extended Lᵖ norm when the target axis cube carries axisCubeNormalizedMeasure.

                    Source-side measurability is also sufficient for exact affine norm transport when the affine map is nondegenerate.

                    Exact extended Lᵖ norm transport from the fixed centered depth-n source cube to the corresponding target concentric contraction.

                    MemLp on the fixed centered source supplies the measurability needed for the exact depth-n norm identity.

                    The corresponding real-valued normalized Lᵖ norms are affine invariant.

                    @[simp]

                    The fixed-depth MemLp transport specialized to a pulled-back harmonic gradient coordinate.

                    Exact fixed-depth norm transport specialized to a pulled-back harmonic gradient coordinate.

                    @[simp]