OAI/MathematicalPhysics/DefocusingNLS/Nonlinear/CutoffMovingPath.lean
4 declarations, 0 contain sorry, 0 declared as axioms
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.
- def
OAI.DefocusingNLS.sampledCutoffProfilePathline 19 - def
OAI.DefocusingNLS.sampledCutoffResidualPathline 29 - theorem
OAI.DefocusingNLS.expandingRadius_residual_powerline 41 - theorem
OAI.DefocusingNLS.exists_sampledCutoffResidualPath_boundline 50Source 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 …