OAI/MathematicalPhysics/DefocusingNLS/Linear/SobolevRestartExtension.lean

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2 declarations, 0 contain sorry, 0 declared as axioms

Extending a maximal trajectory through a later local solution

  1. theorem OAI.DefocusingNLS.maximalSobolevInteractionFlow_restart_extension line 13

    Source documentation

    A classical interaction solution through a later point extends the original maximal trajectory to the right. This is a gluing theorem, with no assumed continuation principle.

    theorem maximalSobolevInteractionFlow_restart_extension
        (k : ℝ) (hk : 6 < k) (m : ℕ) (f₀ : FourierL2) (s δ : ℝ)
        (hs : s ∈ maximalSobolevInteractionDomain k hk m f₀) (hs₀ : 0 ≤ s) (hδ : 0 < δ)
        (w : ℝ → FourierL2)
        (hw : ∀ t ∈ Ioo (s - δ) (s + δ),
          HasDerivAt w (schrodingerInteractionField k hk m t (w t)) t)
        (hw₀ : w s = maximalSobolevInteractionFlow k hk m f₀ s) :
        ∀ t ∈ Ico s (s + δ),
          t ∈ maximalSobolevInteractionDomain k hk m f₀ ∧
            maximalSobolevInteractionFlow k hk m f₀ t = w t := by
    …

    Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.maximalSobolevInteractionDomain

  2. theorem OAI.DefocusingNLS.maximalSobolevSchrodingerFlow_restart_extension line 81

    Source documentation

    A local physical solution through a later state extends the original maximal physical solution. The derivative is taken in the lower Sobolev space, as in the Cauchy problem.

    theorem maximalSobolevSchrodingerFlow_restart_extension
        (k : ℝ) (hk : 6 < k) (m : ℕ) (f₀ : FourierL2) (s δ : ℝ)
        (hs : s ∈ maximalSobolevInteractionDomain k hk m f₀) (hs₀ : 0 ≤ s) (hδ : 0 < δ)
        (w : ℝ → FourierL2) (hw₀ : w 0 = maximalSobolevSchrodingerFlow k hk m f₀ s)
        (hwc : ContinuousOn w (Ioo (-δ) δ))
        (hw : ∀ t ∈ Ioo (-δ) δ, HasDerivAt (fun r => lowerSobolevInclusion (w r))
          (lowerSobolevGenerator (w t) -
            Complex.I • lowerSobolevInclusion (sobolevOddPower k hk m (w t))) t) :
        ∀ t ∈ Ico 0 δ,
          s + t ∈ maximalSobolevInteractionDomain k hk m f₀ ∧
            maximalSobolevSchrodingerFlow k hk m f₀ (s + t) = w t := by
    …

    Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.maximalSobolevInteractionDomain, OAI.DefocusingNLS.lowerSobolevInclusion