OAI/Analysis/LipschitzHilbert/Fourier/PlanarSliceFourierSupport.lean
5 declarations, 0 contain sorry, 0 declared as axioms
Spectral rectangles and annular bounds for actual planar Schwartz
restrictions, using the proved fiber-vanishing identity. Frequencies use
the exp(-2πi xξ) convention throughout.
- theorem
OAI.LipschitzHilbert.frequency_rectangle_boundline 15 - theorem
OAI.LipschitzHilbert.planarSchwartzSlice_fourier_carrier_boundline 26Source documentation
The packet spectral rectangle projects to the expected carrier interval on every affine reference line.
theorem planarSchwartzSlice_fourier_carrier_bound (f : SchwartzMap (ℝ × ℝ) ℂ) (b s θ η₀ δ ε : ℝ) (hspectrum : ∀ ξ η, planarFourier f (ξ, η) ≠ 0 → |ξ + θ * η| ≤ δ ∧ |η - η₀| ≤ ε) {ω : ℝ} (hω : 𝓕 (planarSchwartzSlice f b s) ω ≠ 0) : |ω - η₀ * (s - θ)| ≤ δ + ε * |s - θ| := by …Mentions: OAI.LipschitzHilbert.planarFourier, OAI.LipschitzHilbert.planarSchwartzSlice
- theorem
OAI.LipschitzHilbert.planarSchwartzSlice_support_carrier_intervalline 43 - theorem
OAI.LipschitzHilbert.planarSchwartzSlice_tsupport_carrier_intervalline 55 - theorem
OAI.LipschitzHilbert.planarSchwartzSlice_fourier_annulusline 67Source documentation
Separating the carrier from zero turns the carrier interval into an annulus; the constants are retained exactly for subsequent rescaling.
theorem planarSchwartzSlice_fourier_annulus (f : SchwartzMap (ℝ × ℝ) ℂ) (b s θ η₀ δ ε : ℝ) (hspectrum : ∀ ξ η, planarFourier f (ξ, η) ≠ 0 → |ξ + θ * η| ≤ δ ∧ |η - η₀| ≤ ε) {a A : ℝ} (hlower : a ≤ |η₀ * (s - θ)| - (δ + ε * |s - θ|)) (hupper : |η₀ * (s - θ)| + (δ + ε * |s - θ|) ≤ A) {ω : ℝ} (hω : 𝓕 (planarSchwartzSlice f b s) ω ≠ 0) : a ≤ |ω| ∧ |ω| ≤ A := by …Mentions: OAI.LipschitzHilbert.planarFourier, OAI.LipschitzHilbert.planarSchwartzSlice