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LeanPool.Superdiffusion.Algsuperdiff.StochasticProcess.Common.DivergenceForm.Decay.WeightedToBall

WeightedToBall #

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

From a weighted mass bound to a local L² bound #

The exponentially weighted mass estimate controls the square of a solution against a weight that is bounded below on the region of interest. Dividing by that lower bound turns the weighted statement into the plain local L² statement consumed by the pointwise estimate.

Main results #

theorem DivergenceFormProcess.Decay.setIntegral_sq_le_exp_mul_weighted {d : ℕ} {U B : Set (HCPolySupport.Vec d)} (hBU : B ⊆ U) (hBmeas : MeasurableSet B) {w theta : HCPolySupport.Vec d → ℝ} {c : ℝ} (hthetaNonneg : ∀ (y : HCPolySupport.Vec d), 0 ≤ theta y) (hlower : ∀ y ∈ B, 1 ≤ Real.exp c * theta y) (hsq : MeasureTheory.IntegrableOn (fun (y : HCPolySupport.Vec d) => w y ^ 2) U MeasureTheory.volume) (hint : MeasureTheory.IntegrableOn (fun (y : HCPolySupport.Vec d) => w y ^ 2 * theta y) U MeasureTheory.volume) :
∫ (y : HCPolySupport.Vec d) in B, w y ^ 2 ≤ Real.exp c * ∫ (y : HCPolySupport.Vec d) in U, w y ^ 2 * theta y

A weight bounded below on a subset converts a weighted integral bound into a plain one on that subset.

theorem DivergenceFormProcess.Decay.setIntegral_sq_le_exp_mul_localizedWeight {d : ℕ} {U B : Set (HCPolySupport.Vec d)} (hBU : B ⊆ U) (hBmeas : MeasurableSet B) {w eta psi : HCPolySupport.Vec d → ℝ} {kappa t : ℝ} (hkappa : 0 ≤ kappa) (hetaOne : ∀ y ∈ B, 1 ≤ eta y ^ 2) (hpsiLow : ∀ y ∈ B, t ≤ psi y) (hsq : MeasureTheory.IntegrableOn (fun (y : HCPolySupport.Vec d) => w y ^ 2) U MeasureTheory.volume) (hint : MeasureTheory.IntegrableOn (fun (y : HCPolySupport.Vec d) => w y ^ 2 * (eta y ^ 2 * Real.exp (kappa * psi y) ^ 2)) U MeasureTheory.volume) :
∫ (y : HCPolySupport.Vec d) in B, w y ^ 2 ≤ Real.exp (-(2 * kappa * t)) * ∫ (y : HCPolySupport.Vec d) in U, w y ^ 2 * (eta y ^ 2 * Real.exp (kappa * psi y) ^ 2)

The localized exponential weight of the Agmon estimate is bounded below on any region where the localization is at least one and the phase is at least t.