OAI/Geometry/SurfaceImmersion/Atlas/WeightedModulatedJets.lean
5 declarations, 0 contain sorry, 0 declared as axioms
Slow-scale bounds on the amplitudes of fast oscillatory jets.
- lemma
OAI.ClosedSurfaceR4.JetPolynomial.ModulatedJets.weighted_complexifyline 12 - lemma
OAI.ClosedSurfaceR4.JetPolynomial.ModulatedJets.weighted_amplitudeDerivativeline 24 - def
OAI.ClosedSurfaceR4.JetPolynomial.ModulatedJets.jetConstantline 50 - lemma
OAI.ClosedSurfaceR4.JetPolynomial.ModulatedJets.jetConstant_nonnegline 54 - theorem
OAI.ClosedSurfaceR4.JetPolynomial.ModulatedJets.weighted_amplitudeJetline 61Source documentation
Output derivatives remain at the slow scale. Only the length of the jet word contributes short-scale powers.
theorem weighted_amplitudeJet {U : Set Base} (hU : IsOpen U) {φ : Base → ℝ} {Z : Base → ℂ} {τ s C P : ℝ} (hτ : 0 < τ) (hs : 0 < s) (hτs : τ ≤ s) (hC : 0 ≤ C) (hP : 0 ≤ P) (hφ : ContDiff ℝ ∞ φ) (hZ : ContDiff ℝ ∞ Z) (w : List Base) (hw : ∀ v ∈ w, ‖v‖ ≤ 1) (m : ℕ) (hb : WeightedBound U s (m + w.length) C Z) (hp : ∀ v ∈ w, WeightedBound U s (m + w.length) P (fun p => fderiv ℝ φ p v)) : WeightedBound U s m (jetConstant P m w.length * C / τ ^ w.length) (amplitudeJet τ φ w Z) := by …Mentions: OAI.ClosedSurfaceR4.JetPolynomial.Base, OAI.ClosedSurfaceR4.JetPolynomial.ModulatedJets.jetConstant, OAI.ClosedSurfaceR4.JetPolynomial.ModulatedJets.amplitudeJet