OAI/MathematicalPhysics/DefocusingNLS/Linear/SobolevLinearization.lean

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Pointwise meaning of the Sobolev linearization

Bounded torus observation commutes with the real Fréchet derivative. Thus the operator used in the perturbation equation is exactly the scalar linearization, including its conjugate component.

  1. theorem OAI.DefocusingNLS.sobolevOddPower_fderiv_pointwise line 15

    Source documentation

    At each torus point, the Sobolev derivative is the scalar real derivative.

    theorem sobolevOddPower_fderiv_pointwise (k : ℝ) (hk : 6 < k) (m : ℕ)
        (q v : FourierL2) (x : SchrodingerTorus) :
        sobolevTorusFunction k (fderiv ℝ (sobolevOddPower k hk m) q v) x =
          oddPowerDerivative m (sobolevTorusFunction k q x) (sobolevTorusFunction k v x) := by
    …

    Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.SchrodingerTorus, OAI.DefocusingNLS.oddPowerDerivative

  2. theorem OAI.DefocusingNLS.sobolevOddPower_fderiv_pointwise_explicit line 37

    Source documentation

    The two circular components of the exact linearized odd-power operator.

    theorem sobolevOddPower_fderiv_pointwise_explicit (k : ℝ) (hk : 6 < k) (m : ℕ)
        (q v : FourierL2) (x : SchrodingerTorus) :
        sobolevTorusFunction k (fderiv ℝ (sobolevOddPower k hk m) q v) x =
          ((m + 1 : ℕ) : ℂ) * (sobolevTorusFunction k q x) ^ m *
            star (sobolevTorusFunction k q x) ^ m * sobolevTorusFunction k v x +
          (m : ℂ) * (sobolevTorusFunction k q x) ^ (m + 1) *
            star (sobolevTorusFunction k q x) ^ (m - 1) * star (sobolevTorusFunction k v x) := by
    …

    Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.SchrodingerTorus

  3. theorem OAI.DefocusingNLS.sobolevNonlinearRemainder_pointwise line 48

    Source documentation

    The abstract remainder evaluates to the actual scalar nonlinear Taylor remainder.

    theorem sobolevNonlinearRemainder_pointwise (k : ℝ) (hk : 6 < k) (m : ℕ)
        (q v : FourierL2) (x : SchrodingerTorus) :
        sobolevTorusFunction k (sobolevNonlinearRemainder k hk m q v) x =
          oddPowerNonlinearity m (sobolevTorusFunction k q x + sobolevTorusFunction k v x) -
            oddPowerNonlinearity m (sobolevTorusFunction k q x) -
              oddPowerDerivative m (sobolevTorusFunction k q x) (sobolevTorusFunction k v x) := by
    …

    Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.SchrodingerTorus, OAI.DefocusingNLS.sobolevNonlinearRemainder, OAI.DefocusingNLS.oddPowerNonlinearity, OAI.DefocusingNLS.oddPowerDerivative