OAI/MathematicalPhysics/DefocusingNLS/Linear/ExpandingDerivativeBounds.lean
4 declarations, 0 contain sorry, 0 declared as axioms
Scale-uniform derivatives of the actual expanding-torus nonlinearity
- theorem
OAI.DefocusingNLS.expanding_linear_two_jet_boundline 13 - theorem
OAI.DefocusingNLS.expanding_bilinear_two_jet_boundline 34 - theorem
OAI.DefocusingNLS.exists_expandingOddPower_two_jet_boundline 68Source documentation
Derivatives through order two are bounded uniformly for every
L ≥ 1.theorem exists_expandingOddPower_two_jet_bound (a k : ℝ) (ha : 0 < a) (ha1 : a < 1) (hk : 8 < k) (m : ℕ) (R : ℝ) (hR : 0 ≤ R) : ∃ C : ℝ, 0 ≤ C ∧ ∀ (L : ℝ) (hL : 1 ≤ L) (f : FourierL2), ‖f‖ ≤ R → ∀ n : ℕ, n ≤ 2 → ‖iteratedFDeriv ℝ n (expandingOddPower a k L ha ha1 hk hL m) f‖ ≤ C := by …Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.expandingOddPower
- theorem
OAI.DefocusingNLS.exists_expandingOddPower_derivative_lipschitzline 99Source documentation
The derivative is Lipschitz on each ball, uniformly in the torus radius.
theorem exists_expandingOddPower_derivative_lipschitz (a k : ℝ) (ha : 0 < a) (ha1 : a < 1) (hk : 8 < k) (m : ℕ) (R : ℝ) (hR : 0 ≤ R) : ∃ C : ℝ, 0 ≤ C ∧ ∀ (L : ℝ) (hL : 1 ≤ L) (f g : FourierL2), ‖f‖ ≤ R → ‖g‖ ≤ R → ‖fderiv ℝ (expandingOddPower a k L ha ha1 hk hL m) f - fderiv ℝ (expandingOddPower a k L ha ha1 hk hL m) g‖ ≤ C * ‖f - g‖ := by …Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.expandingOddPower