OAI/MathematicalPhysics/DefocusingNLS/Linear/SchwartzLocalizationKernel.lean
5 declarations, 0 contain sorry, 0 declared as axioms
Schwartz kernels in the mixed Fourier localization estimate
The actual localization kernel is the Fourier transform of a smooth cutoff. Its Bessel-weighted versions remain Schwartz, so the lattice-to-continuum bound applies at both Sobolev orders used in the manuscript.
- def
OAI.DefocusingNLS.weightedSchwartzKernelline 19Source documentation
Applying any real Bessel weight preserves the Schwartz localization kernel.
noncomputable def weightedSchwartzKernel (s : ā) (K : š¢(EuclideanSpace ā (Fin 12), ā)) : š¢(EuclideanSpace ā (Fin 12), ā) := ⦠- theorem
OAI.DefocusingNLS.weightedSchwartzKernel_applyline 24 - theorem
OAI.DefocusingNLS.weightedSchwartzKernel_normline 30 - theorem
OAI.DefocusingNLS.exists_schwartz_mixedFourier_boundline 37Source documentation
A concrete Schwartz kernel has a finite mixed L² operator bound.
theorem exists_schwartz_mixedFourier_bound (K : š¢(EuclideanSpace ā (Fin 12), ā)) : ā C : ā, 0 ⤠C ā§ ā (S : Finset frequencyLattice) (v : frequencyLattice ā ā), Integrable (fun x => āā n ā S, v n * K (x - n)ā ^ 2) ā§ (ā« x, āā n ā S, v n * K (x - n)ā ^ 2) ⤠C * ā n ā S, āv nā ^ 2 := by ā¦Mentions: OAI.DefocusingNLS.frequencyLattice
- theorem
OAI.DefocusingNLS.exists_weightedSchwartz_mixedFourier_boundline 48Source documentation
The same estimate applies to every real Sobolev weight of the cutoff kernel.
theorem exists_weightedSchwartz_mixedFourier_bound (s : ā) (K : š¢(EuclideanSpace ā (Fin 12), ā)) : ā C : ā, 0 ⤠C ā§ ā (S : Finset frequencyLattice) (v : frequencyLattice ā ā), Integrable (fun x => āā n ā S, v n * weightedSchwartzKernel s K (x - n)ā ^ 2) ā§ (ā« x, āā n ā S, v n * weightedSchwartzKernel s K (x - n)ā ^ 2) ⤠C * ā n ā S, āv nā ^ 2 := ā¦Mentions: OAI.DefocusingNLS.frequencyLattice, OAI.DefocusingNLS.weightedSchwartzKernel