OAI/MathematicalPhysics/DefocusingNLS/Nonlinear/CutoffMovingPath.lean

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Actual cutoff profiles and residuals along the expanding radius

The sampled profile and its exact PDE residual are continuous histories on any finite time slab. The residual decay retains the starting-scale factor.

  1. def OAI.DefocusingNLS.sampledCutoffProfilePath line 19
  2. def OAI.DefocusingNLS.sampledCutoffResidualPath line 29
  3. theorem OAI.DefocusingNLS.expandingRadius_residual_power line 41
  4. theorem OAI.DefocusingNLS.exists_sampledCutoffResidualPath_bound line 50

    Source documentation

    The same constant controls every starting radius and every time slab.

    theorem exists_sampledCutoffResidualPath_bound (a k : ℝ)
        (ha : 0 < a) (ha1 : a < 1) (hk : 8 < k)
        (χ : 𝓢(E, ℝ)) (hχ : HasCompactSupport (χ : E → ℝ))
        (hχone : ∀ x : E, ‖x‖ < 1 / 2 → χ x = 1)
        (hχzero : ∀ x : E, 2 < ‖x‖ → χ x = 0) (m : ℕ) :
        ∃ N : ℕ, ∀ (Q : E → ℂ) (hQ : ContDiff ℝ ∞ Q) (D : ℝ), 0 ≤ D →
          (∀ n ≤ N, ∀ y : E, y ≠ 0 →
            ‖iteratedFDeriv ℝ n Q y‖ ≤ D * ‖y‖ ^ (-2 * a - (n : ℝ))) →
          ∃ C : ℝ, 0 ≤ C ∧ ∀ (L T : ℝ) (hL : 1 ≤ L) (t : Icc (0 : ℝ) T),
            ‖sampledCutoffResidualPath a k L T ha ha1 hk hL χ hχ hχone hχzero m Q hQ t‖ ≤
              C * L ^ (-2 - a) * Real.exp (-(2 + a) * (t : ℝ) / 2) := by
    …

    Mentions: OAI.DefocusingNLS.sampledCutoffResidualPath