OAI/Geometry/RCD/Coordinates/CommonFrameRadialFits.lean

GitHub source file

4 declarations, 0 contain sorry, 0 declared as axioms

Transporting the actual radial fits to a common frame and region

  1. theorem OAI.RegularPointCoordinates.common_frame_radial_residual line 21

    Source documentation

    The common-frame residual is exactly the original residual at the transported covector, including its recentering constant.

    theorem common_frame_radial_residual {n : ℕ}
        (u : Fin n → SobolevSpace μ hQ) (η : SobolevSpace μ hQ)
        (G : Euclidean n →L[ℝ] SobolevSpace μ hQ) (x z : Euclidean n)
        (N M : Euclidean n ≃L[ℝ] Euclidean n) (C : Euclidean n →L[ℝ] Euclidean n)
        (b : Euclidean n) :
        G (M.symm (N b)) -
          (centeredSobolevMap μ hQ u η z).comp N.toContinuousLinearMap
            (rebasedRadialOperator N M C b) -
          ⟪z - x, C (M.symm (N b))⟫_ℝ • η =
        G (M.symm (N b)) - centeredAffineSobolev μ hQ u η x (C (M.symm (N b))) := by
    …

    Mentions: OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.Euclidean, OAI.RegularPointCoordinates.centeredSobolevMap, OAI.RegularPointCoordinates.rebasedRadialOperator, OAI.RegularPointCoordinates.centeredAffineSobolev

  2. theorem OAI.RegularPointCoordinates.common_frame_radial_bounds line 37

    Source documentation

    The volume ratio and frame operator norm account for all losses when the original all-covector radial fit is used on the common commutator region.

    theorem common_frame_radial_bounds {n : ℕ}
        (u : Fin n → SobolevSpace μ hQ) (η : SobolevSpace μ hQ)
        (G : Euclidean n →L[ℝ] SobolevSpace μ hQ) (x z : Euclidean n)
        (N M : Euclidean n ≃L[ℝ] Euclidean n) (C : Euclidean n →L[ℝ] Euclidean n)
        {Ωv Ωe Ω : Set X} (hΩv : Ω ⊆ Ωv) (hΩe : Ω ⊆ Ωe)
        (hvfin : μ Ωv ≠ ∞) (hfin : μ Ω ≠ ∞)
        (hvpos : 0 < μ.real Ωv) (hepos : 0 < μ.real Ωe) (hpos : 0 < μ.real Ω)
        {V W E D : ℝ} (hE : 0 ≤ E) (hD : 0 ≤ D)
        (hvolv : μ.real Ωv ≤ V * μ.real Ω) (hvole : μ.real Ωe ≤ W * μ.real Ω)
        (hvalue : ∀ a, ‖normalizeLocalL2 μ Ωv hvfin (SobolevSpace.restrictLp μ hQ Ωv
          (G a - centeredAffineSobolev μ hQ u η x (C a)))‖ ^ 2 ≤ E * ‖a‖ ^ 2)
        (henergy : ∀ a, (μ.real Ωe)⁻¹ * (∫ t in Ωe, localGamma μ hQ
    …

    Mentions: OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.Euclidean, OAI.RegularPointCoordinates.normalizeLocalL2, OAI.RegularPointCoordinates.SobolevSpace.restrictLp, OAI.RegularPointCoordinates.centeredAffineSobolev, OAI.RegularPointCoordinates.localGamma

  3. theorem OAI.RegularPointCoordinates.centered_sobolev_constant_difference line 84

    Source documentation

    Centering the common harmonic column changes each covector by a locally constant function, represented by the same compact cutoff.

    theorem centered_sobolev_constant_difference {n : ℕ}
        (Ω : Set X) (u : Fin n → SobolevSpace μ hQ) (η : SobolevSpace μ hQ)
        (z b : Euclidean n)
        (hη : SobolevSpace.toLp μ hQ η =ᵐ[μ.restrict Ω] fun _ => (1 : ℝ)) :
        SobolevSpace.toLp μ hQ (centeredSobolevMap μ hQ u η z b - sobolevColumnMap μ hQ u b)
          =ᵐ[μ.restrict Ω] fun _ => -⟪z, b⟫_ℝ := by
    …

    Mentions: OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.Euclidean, OAI.RegularPointCoordinates.SobolevSpace.toLp, OAI.RegularPointCoordinates.centeredSobolevMap, OAI.RegularPointCoordinates.sobolevColumnMap

  4. theorem OAI.RegularPointCoordinates.common_frame_radial_representative line 105

    Source documentation

    The transported radial family remains a representative of the derivative of the same centered coordinate map in the common frame.

    theorem common_frame_radial_representative {n : ℕ}
        (Ω : Set X) (f : SobolevSpace μ hQ) (u : Fin n → SobolevSpace μ hQ)
        (η : SobolevSpace μ hQ) (z : Euclidean n)
        (N M : Euclidean n ≃L[ℝ] Euclidean n)
        (G : Euclidean n →L[ℝ] SobolevSpace μ hQ)
        (hη : SobolevSpace.toLp μ hQ η =ᵐ[μ.restrict Ω] fun _ => (1 : ℝ))
        (hG : ∀ a, SobolevSpace.toLp μ hQ (G a) =ᵐ[μ.restrict Ω]
          localGamma μ hQ f (sobolevColumnMap μ hQ u (M a))) (b : Euclidean n) :
        SobolevSpace.toLp μ hQ (G (M.symm (N b))) =ᵐ[μ.restrict Ω]
          localGamma μ hQ f ((centeredSobolevMap μ hQ u η z).comp N.toContinuousLinearMap b) := by
    …

    Mentions: OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.Euclidean, OAI.RegularPointCoordinates.SobolevSpace.toLp, OAI.RegularPointCoordinates.localGamma, OAI.RegularPointCoordinates.sobolevColumnMap, OAI.RegularPointCoordinates.centeredSobolevMap