OAI/MathematicalPhysics/DefocusingNLS/Nonlinear/MaximalStrongSolution.lean
3 declarations, 0 contain sorry, 0 declared as axioms
Maximality among strong Sobolev Schrödinger solutions
- theorem
OAI.DefocusingNLS.continuousOn_maximalSobolevSchrodingerFlowline 13 - theorem
OAI.DefocusingNLS.strongSobolevSchrodingerSolution_restricts_maximalline 22Source documentation
Every strong solution through the initial datum is a restriction of the maximal flow.
theorem strongSobolevSchrodingerSolution_restricts_maximal (k : ℝ) (hk : 6 < k) (m : ℕ) (f₀ : FourierL2) (u : ℝ → FourierL2) (a b : ℝ) (ha : a < 0) (hb : 0 < b) (hu₀ : u 0 = f₀) (huc : ContinuousOn u (Ioo a b)) (hu : ∀ t ∈ Ioo a b, HasDerivAt (fun s => lowerSobolevInclusion (u s)) (lowerSobolevGenerator (u t) - Complex.I • lowerSobolevInclusion (sobolevOddPower k hk m (u t))) t) : Ioo a b ⊆ maximalSobolevInteractionDomain k hk m f₀ ∧ EqOn u (maximalSobolevSchrodingerFlow k hk m f₀) (Ioo a b) := by …Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.lowerSobolevInclusion, OAI.DefocusingNLS.maximalSobolevInteractionDomain
- theorem
OAI.DefocusingNLS.maximalSobolev_lifespan_of_positive_rescaled_observationline 48Source documentation
A positive rescaled observation fixes the finite endpoint of the maximal strong solution. The observation may be evaluation at any point of the twelve-dimensional torus.
theorem maximalSobolev_lifespan_of_positive_rescaled_observation {F : Type*} [NormedAddCommGroup F] (k : ℝ) (hk : 6 < k) (m : ℕ) (f₀ : FourierL2) (u : ℝ → FourierL2) (a T β c : ℝ) (ha : a < 0) (hT : 0 < T) (hβ : 0 < β) (hc : 0 < c) (hu₀ : u 0 = f₀) (huc : ContinuousOn u (Ioo a T)) (hu : ∀ t ∈ Ioo a T, HasDerivAt (fun s => lowerSobolevInclusion (u s)) (lowerSobolevGenerator (u t) - Complex.I • lowerSobolevInclusion (sobolevOddPower k hk m (u t))) t) (observe : FourierL2 → F) (hobs : Continuous observe) (hblowup : Tendsto (fun t => (T - t) ^ β * ‖observe (u t)‖) (𝓝[<] T) (𝓝 c)) : …Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.lowerSobolevInclusion