OAI/Geometry/RCD/Heat/FiniteHeatMassShells.lean

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3 declarations, 0 contain sorry, 0 declared as axioms

Finite shell bounds for the full Bochner heat mass

  1. theorem OAI.RegularPointCoordinates.finite_dyadicShell_union line 19

    Source documentation

    The first N+1 shells partition exactly the corresponding outer ball.

    theorem finite_dyadicShell_union (p : X) {r : ℝ} (hr : 0 ≤ r) (N : ℕ) :
        (⋃ j ∈ Finset.range (N + 1), dyadicShell p r j) = ball p (2 ^ N * r) := by
    …

    Mentions: OAI.RegularPointCoordinates.dyadicShell

  2. theorem OAI.RegularPointCoordinates.integral_le_finite_shell_mass line 30

    Source documentation

    Integrate finitely many controlled shells and use a single bound on the exterior. This applies directly to singular finite mass measures.

    theorem integral_le_finite_shell_mass (ν : Measure X) [IsFiniteMeasure ν]
        (p : X) {r : ℝ} (hr : 0 ≤ r) (N : ℕ) {f : X → ℝ} (hf : Integrable f ν)
        (W : ℕ → ℝ) (hW : ∀ j, 0 ≤ W j)
        (hlocal : ∀ j ≤ N, ∀ᵐ z ∂ν.restrict (dyadicShell p r j), f z ≤ W j)
        {T : ℝ} (hT : 0 ≤ T)
        (htail : ∀ᵐ z ∂ν.restrict (ball p (2 ^ N * r))ᶜ, f z ≤ T) :
        (∫ z, f z ∂ν) ≤
          (∑ j ∈ Finset.range (N + 1), W j * ν.real (ball p (2 ^ j * r))) + T * ν.real univ := by
    …

    Mentions: OAI.RegularPointCoordinates.dyadicShell

  3. theorem OAI.RegularPointCoordinates.cutoffHeatMass_le_finite_shells line 63

    Source documentation

    The shell bound controls the actual heat mass of the full positive Bochner measure, not just an assumed density.

    theorem cutoffHeatMass_le_finite_shells (M : PositiveBilinearMeasure X E)
        (p : X) {r t : ℝ} (hr : 0 ≤ r) (ht : 0 < t) (N : ℕ)
        (W : ℕ → ℝ) (hW : ∀ j, 0 ≤ W j)
        (hlocal : ∀ j ≤ N, ∀ z ∈ dyadicShell p r j, χ z * ker t p z ≤ W j)
        {T : ℝ} (hT : 0 ≤ T)
        (htail : ∀ z ∉ ball p (2 ^ N * r), χ z * ker t p z ≤ T) (v : E) :
        ⟪v, cutoffHeatMass μ hQ hk hχ hsχ M ht p v⟫_ℝ ≤
          (∑ j ∈ Finset.range (N + 1), W j * (M.measure v).real (ball p (2 ^ j * r))) +
            T * (M.measure v).real univ := by
    …

    Mentions: OAI.RegularPointCoordinates.PositiveBilinearMeasure, OAI.RegularPointCoordinates.dyadicShell, OAI.RegularPointCoordinates.cutoffHeatMass