OAI/MathematicalPhysics/DefocusingNLS/Linear/ExpandingStrongEquation.lean
3 declarations, 0 contain sorry, 0 declared as axioms
Strong derivatives for the moving-torus equation
The time-dependent Laplacian loses two Sobolev orders. After this loss, continuity of the candidate derivative upgrades the Fourier-mode equation to a strong Hilbert-space equation.
- def
OAI.DefocusingNLS.expandingReducedFieldline 17 - theorem
OAI.DefocusingNLS.continuousOn_expandingReducedFieldline 22 - theorem
OAI.DefocusingNLS.hasDerivAt_expandingReducedFieldline 34Source documentation
A continuous Fourier solution of the exact mode equations is a strong solution in the space with two fewer Sobolev derivatives.
theorem hasDerivAt_expandingReducedField (a b L A B : ℝ) (u r : ℝ → FourierL2) (hu : ContinuousOn u (Ioo A B)) (hr : ContinuousOn r (Ioo A B)) (hmode : ∀ t ∈ Ioo A B, ∀ n : frequencyLattice, HasDerivAt (fun s => u s n) (expandingModeRate a b L t n * u t n + r t n) t) (t : ℝ) (ht : t ∈ Ioo A B) : HasDerivAt (fun s => lowerSobolevInclusion (u s)) (expandingReducedField a b L u r t) t := by …Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.frequencyLattice, OAI.DefocusingNLS.expandingModeRate, OAI.DefocusingNLS.lowerSobolevInclusion, OAI.DefocusingNLS.expandingReducedField