OAI/MeasureTheory/Falconer/Estimates/SeparatedInverse.lean
9 declarations, 0 contain sorry, 0 declared as axioms
Finite endpoint separation of the actual inverse amplitudes
The finite expansion is constructed from product rules and chart pullbacks. Every factor is globally smooth and depends on one endpoint only. This is an identity for the original masked inverse, with no extra analytic input.
- def
OAI.Falconer.SmoothSeparation.stationaryJetMultiplierline 21 - theorem
OAI.Falconer.SmoothSeparation.stationaryJetMultiplier_contDiffline 25 - def
OAI.Falconer.SmoothSeparation.stationaryJointDensityline 29 - theorem
OAI.Falconer.SmoothSeparation.stationaryJointDensity_contDiffline 32 - def
OAI.Falconer.SmoothSeparation.stationaryJetline 36 - theorem
OAI.Falconer.SmoothSeparation.stationaryJet_valueline 44 - def
OAI.Falconer.SmoothSeparation.inverseline 55 - theorem
OAI.Falconer.SmoothSeparation.inverse_valueline 64 - theorem
OAI.Falconer.localInverseAmplitude_product_separatedline 89Source documentation
The exact finite endpoint expansion used in weighted-shell conversion. No endpoint parameter occurs in the opposite factor, and all angular factors are globally smooth.
theorem localInverseAmplitude_product_separated (m j : ℕ) (B : X → Space (m+3) → ℂ) (C : Y → Space (m+3) → ℂ) (hB : ∀ x, ContDiff ℝ ∞ (B x)) (hC : ∀ y, ContDiff ℝ ∞ (C y)) : ∃ S : SmoothSeparation X Y (Space (m+3)), ∀ x y e, localInverseAmplitude m (fun w => B x w*C y w) j e = S.value x y e := by …Mentions: OAI.Falconer.Space, OAI.Falconer.SmoothSeparation, OAI.Falconer.localInverseAmplitude