OAI/MathematicalPhysics/DefocusingNLS/Linear/LocalizationFourierEnergy.lean
6 declarations, 0 contain sorry, 0 declared as axioms
The exact homogeneous Fourier energy of a finite localized polynomial
The dilation identity supplies the factor L^(12-2s). The weighted mixed estimate then controls both orders of Y by the exact Y_L coefficient norm.
- def
OAI.DefocusingNLS.homogeneousFourierEnergyline 19 - theorem
OAI.DefocusingNLS.homogeneousKernel_density_scaleline 22 - theorem
OAI.DefocusingNLS.homogeneousKernel_dilationline 38 - theorem
OAI.DefocusingNLS.homogeneousKernel_bessel_controlline 52 - theorem
OAI.DefocusingNLS.integrable_localizedFourierPolynomial_energyline 78Source documentation
Each finite physical cutoff has finite homogeneous Fourier energy.
theorem integrable_localizedFourierPolynomial_energy (s L : ℝ) (hs : 0 ≤ s) (hL : 0 < L) (χ : 𝓢(E, ℂ)) (S : Finset frequencyLattice) (v : frequencyLattice → ℂ) : Integrable (fun ξ => ‖ξ‖ ^ (2 * s) * ‖radianFourierIntegral (localizedFourierPolynomial L χ S v) ξ‖ ^ 2) := by …Mentions: OAI.DefocusingNLS.frequencyLattice, OAI.DefocusingNLS.radianFourierIntegral, OAI.DefocusingNLS.localizedFourierPolynomial
- theorem
OAI.DefocusingNLS.exists_localizedFourierPolynomial_energy_boundline 92Source documentation
The finite Fourier version of the manuscript's uniform cutoff estimate. The right side is the exact Y_L coefficient density, before the common (2π)^12 normalization.
theorem exists_localizedFourierPolynomial_energy_bound (a k : ℝ) (ha : 0 < a) (ha1 : a < 1) (hk : 8 < k) (χ : 𝓢(E, ℂ)) : ∃ C : ℝ, 0 ≤ C ∧ ∀ (L : ℝ), 1 ≤ L → ∀ (S : Finset frequencyLattice) (v : frequencyLattice → ℂ), homogeneousFourierEnergy (6 - a) (localizedFourierPolynomial L χ S v) + homogeneousFourierEnergy k (localizedFourierPolynomial L χ S v) ≤ C * ∑ n ∈ S, expandingSobolevWeightSq a k L n * ‖v n‖ ^ 2 := by …Mentions: OAI.DefocusingNLS.frequencyLattice, OAI.DefocusingNLS.homogeneousFourierEnergy, OAI.DefocusingNLS.localizedFourierPolynomial, OAI.DefocusingNLS.expandingSobolevWeightSq