OAI/MathematicalPhysics/DefocusingNLS/Nonlinear/GaussianRealization.lean

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11 declarations, 0 contain sorry, 0 declared as axioms

A measurable Hilbert-valued realization of the Fourier series

The weighted coefficients are realized in the standard ℓ² Hilbert model of the Sobolev norm. The realization is a measurable sum of coordinate vectors, and agrees almost surely with the prescribed coefficients.

  1. abbrev OAI.DefocusingNLS.FourierL2 line 22

    Also declared: ComparatorChallenges/DefocusingNLS.lean:58 (same declaration text).

  2. instance OAI.DefocusingNLS.(instance at line 26) line 26

    Source documentation

    Finite coordinate vectors have dense complex span, so this Hilbert model is separable.

    instance : SeparableSpace FourierL2 := by
    …

    Mentions: OAI.DefocusingNLS.FourierL2

  3. instance OAI.DefocusingNLS.(instance at line 46) line 46
  4. instance OAI.DefocusingNLS.(instance at line 47) line 47
  5. def OAI.DefocusingNLS.weightedGaussianVector line 50

    Source documentation

    Measurable Hilbert-valued sum of the weighted Gaussian coordinates.

    Also declared: ComparatorChallenges/DefocusingNLS.lean:63 (same declaration text).

    noncomputable def weightedGaussianVector (k α : ℝ)
        (g : frequencyLattice → ℂ) : FourierL2 :=
    …

    Mentions: OAI.DefocusingNLS.frequencyLattice, OAI.DefocusingNLS.FourierL2

  6. theorem OAI.DefocusingNLS.measurable_weightedGaussianVector line 54
  7. theorem OAI.DefocusingNLS.ae_weightedGaussianVector_coefficients line 64

    Source documentation

    In the summable range, the measurable realization has precisely the prescribed Fourier coefficients almost surely.

    theorem ae_weightedGaussianVector_coefficients (k α : ℝ) (hα : k + 6 < α) :
        ∀ᵐ g ∂fourierGaussianLaw, ∀ n,
          weightedGaussianVector k α g n = weightedGaussianCoefficient k α g n := by
    …

    Mentions: OAI.DefocusingNLS.fourierGaussianLaw, OAI.DefocusingNLS.weightedGaussianVector

  8. def OAI.DefocusingNLS.sobolevFourierCoefficient line 74

    Source documentation

    The unweighted Fourier coefficient of an element of the H^k model.

    Also declared: ComparatorChallenges/DefocusingNLS.lean:67 (same declaration text).

    noncomputable def sobolevFourierCoefficient (k : ℝ) (f : FourierL2)
        (n : frequencyLattice) : ℂ :=
    …

    Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.frequencyLattice

  9. theorem OAI.DefocusingNLS.ae_sobolevFourierCoefficient line 79

    Source documentation

    Undoing the Sobolev weight gives exactly gₙ / ⟨n⟩^α.

    theorem ae_sobolevFourierCoefficient (k α : ℝ) (hα : k + 6 < α) :
        ∀ᵐ g ∂fourierGaussianLaw, ∀ n,
          sobolevFourierCoefficient k (weightedGaussianVector k α g) n =
            (1 + ‖n‖ ^ 2) ^ (-α / 2) • g n := by
    …

    Mentions: OAI.DefocusingNLS.fourierGaussianLaw, OAI.DefocusingNLS.sobolevFourierCoefficient, OAI.DefocusingNLS.weightedGaussianVector

  10. def OAI.DefocusingNLS.weightedGaussianLaw line 91

    Source documentation

    The corresponding probability law in the Hilbert model.

    Distinct definitions of this name: ComparatorChallenges/DefocusingNLS.lean:71 (same statement text; different proof or body). Qualify references as OAI.DefocusingNLS.weightedGaussianLaw@path.

    noncomputable def weightedGaussianLaw (k α : ℝ) : Measure FourierL2 :=
    …

    Mentions: OAI.DefocusingNLS.FourierL2

  11. instance OAI.DefocusingNLS.(instance at line 94) line 94