OAI/Geometry/RCD/Coordinates/NormalizedBochnerMass.lean

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2 declarations, 0 contain sorry, 0 declared as axioms

Scaled Bochner mass from a first-order splitting map

This connects the actual averaged component errors in the splitting hypothesis to the dimensionless full mass used in the metric iteration.

  1. theorem OAI.RegularPointCoordinates.FirstOrderSplittingOn.closed_error_le line 25

    Source documentation

    Restricting the averaged error on the large harmonic ball controls the unnormalized error on every closed interior ball.

    theorem FirstOrderSplittingOn.closed_error_le {n : ℕ} {p : X} {r ε R : ℝ}
        {u : Fin n → SobolevSpace μ hQ} {w : X → Euclidean n}
        (h : FirstOrderSplittingOn μ hQ p r ε u w) (hR : R < r)
        (hvol : 0 < μ.real (ball p r)) (hfinite : μ (ball p r) ≠ ∞) (i j : Fin n) :
        (∫ x in closedBall p R,
          |localGamma μ hQ (u i) (u j) x - (if i = j then 1 else 0)| ∂μ) ≤
          ε * μ.real (ball p r) := by
    …

    Mentions: OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.Euclidean, OAI.RegularPointCoordinates.FirstOrderSplittingOn, OAI.RegularPointCoordinates.localGamma

  2. theorem OAI.RegularPointCoordinates.splitting_normalized_bochner_mass_le line 46

    Source documentation

    The normalized full Bochner mass is small when the splitting error and the rescaled curvature are small.

    theorem splitting_normalized_bochner_mass_le [IsFiniteMeasureOnCompacts μ]
        {n : ℕ} {p : X} {r ε C κ : ℝ} {L : ℝ≥0}
        {u : Fin n → SobolevSpace μ hQ} {w : X → Euclidean n}
        (h : FirstOrderSplittingOn μ hQ p (8 * r) ε u w)
        (hr : 0 < r) (hε : 0 ≤ ε) (hC : 0 ≤ C) (hκ : 0 ≤ κ)
        (hvol : 0 < μ.real (ball p (8 * r)))
        (χ : GoodLaplacianCutoff μ hQ p (r / 2) C)
        (M : PositiveBilinearMeasure X (Euclidean n))
        (G : ∀ v, LocalHarmonicEnergy μ hQ (sobolevColumnMap μ hQ u) M κ p r L v)
        (v : Euclidean n) :
        (r ^ 2 / μ.real (ball p (8 * r))) * ⟪v, M.massOperator (ball p (r / 2)) v⟫_ℝ ≤
          (2 * C * (n : ℝ) ^ 2 * ε + κ * r ^ 2 * ((n : ℝ) ^ 2 * ε + 1)) * ‖v‖ ^ 2 := by
    …

    Mentions: OAI.RegularPointCoordinates.SobolevSpace, OAI.RegularPointCoordinates.Euclidean, OAI.RegularPointCoordinates.FirstOrderSplittingOn, OAI.RegularPointCoordinates.GoodLaplacianCutoff, OAI.RegularPointCoordinates.PositiveBilinearMeasure, OAI.RegularPointCoordinates.LocalHarmonicEnergy, OAI.RegularPointCoordinates.sobolevColumnMap