OAI/MathematicalPhysics/DefocusingNLS/Linear/SobolevContinuation.lean

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5 declarations, 0 contain sorry, 0 declared as axioms

Uniform local lifespans and continuation of Sobolev interaction solutions

  1. theorem OAI.DefocusingNLS.exists_uniform_sobolevInteraction_time line 12

    Source documentation

    Every bounded set of initial data has one common positive local lifespan, at every time.

    theorem exists_uniform_sobolevInteraction_time (k : ℝ) (hk : 6 < k) (m : ℕ)
        (R : ℝ) (hR : 0 ≤ R) :
        ∃ δ : ℝ, 0 < δ ∧ ∀ (t₀ : ℝ) (f₀ : FourierL2), ‖f₀‖ ≤ R →
          ∃ v : ℝ → FourierL2, v t₀ = f₀ ∧
            ∀ t ∈ Ioo (t₀ - δ) (t₀ + δ),
              HasDerivAt v (schrodingerInteractionField k hk m t (v t)) t := by
    …

    Mentions: OAI.DefocusingNLS.FourierL2

  2. def OAI.DefocusingNLS.HasSobolevInteractionContinuation line 72

    Source documentation

    A right continuation is a classical solution across the endpoint agreeing on a left neighborhood.

    def HasSobolevInteractionContinuation (k : ℝ) (hk : 6 < k) (m : ℕ)
        (v : ℝ → FourierL2) (T : ℝ) : Prop :=
    …

    Mentions: OAI.DefocusingNLS.FourierL2

  3. theorem OAI.DefocusingNLS.sobolevInteraction_continuation_from_overlap line 80

    Source documentation

    A local solution started before the endpoint and lasting beyond it continues the original one.

    theorem sobolevInteraction_continuation_from_overlap
        (k : ℝ) (hk : 6 < k) (m : ℕ) (v w : ℝ → FourierL2)
        (a T t₀ δ : ℝ) (ht₀ : t₀ ∈ Ioo a T) (hT : T < t₀ + δ)
        (hv : ∀ t ∈ Ioo a T, HasDerivAt v (schrodingerInteractionField k hk m t (v t)) t)
        (hw : ∀ t ∈ Ioo (t₀ - δ) (t₀ + δ),
          HasDerivAt w (schrodingerInteractionField k hk m t (w t)) t)
        (heq : v t₀ = w t₀) : HasSobolevInteractionContinuation k hk m v T := by
    …

    Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.HasSobolevInteractionContinuation

  4. theorem OAI.DefocusingNLS.sobolevInteraction_continuation_of_bounded line 116

    Source documentation

    A finite right endpoint with bounded Sobolev norm is extendible.

    theorem sobolevInteraction_continuation_of_bounded
        (k : ℝ) (hk : 6 < k) (m : ℕ) (v : ℝ → FourierL2)
        (a T R : ℝ) (haT : a < T) (hR : 0 ≤ R)
        (hv : ∀ t ∈ Ioo a T, HasDerivAt v (schrodingerInteractionField k hk m t (v t)) t)
        (hb : ∀ t ∈ Ioo a T, ‖v t‖ ≤ R) : HasSobolevInteractionContinuation k hk m v T := by
    …

    Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.HasSobolevInteractionContinuation

  5. theorem OAI.DefocusingNLS.sobolevInteraction_norm_tendsto_atTop line 139

    Source documentation

    A nonextendible finite endpoint forces the Sobolev norm to diverge.

    theorem sobolevInteraction_norm_tendsto_atTop
        (k : ℝ) (hk : 6 < k) (m : ℕ) (v : ℝ → FourierL2)
        (a T : ℝ) (haT : a < T)
        (hv : ∀ t ∈ Ioo a T, HasDerivAt v (schrodingerInteractionField k hk m t (v t)) t)
        (hmax : ¬ HasSobolevInteractionContinuation k hk m v T) :
        Tendsto (fun t => ‖v t‖) (𝓝[<] T) atTop := by
    …

    Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.HasSobolevInteractionContinuation