OAI/MathematicalPhysics/DefocusingNLS/Linear/ExpandingLinearization.lean
3 declarations, 0 contain sorry, 0 declared as axioms
Pointwise meaning of the uniform expanding-torus linearization
- theorem
OAI.DefocusingNLS.expandingOddPower_fderiv_pointwiseline 11Source documentation
At each torus point, the Sobolev derivative is the scalar real derivative.
theorem expandingOddPower_fderiv_pointwise (a k L : ℝ) (ha : 0 < a) (ha1 : a < 1) (hk : 8 < k) (hL : 1 ≤ L) (m : ℕ) (q v : FourierL2) (x : SchrodingerTorus) : expandingTorusFunction a k L (fderiv ℝ (expandingOddPower a k L ha ha1 hk hL m) q v) x = oddPowerDerivative m (expandingTorusFunction a k L q x) (expandingTorusFunction a k L v x) := by …Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.SchrodingerTorus, OAI.DefocusingNLS.expandingTorusFunction, OAI.DefocusingNLS.expandingOddPower, OAI.DefocusingNLS.oddPowerDerivative
- theorem
OAI.DefocusingNLS.expandingOddPower_fderiv_pointwise_explicitline 33Source documentation
The two circular components of the exact linearized odd-power operator.
theorem expandingOddPower_fderiv_pointwise_explicit (a k L : ℝ) (ha : 0 < a) (ha1 : a < 1) (hk : 8 < k) (hL : 1 ≤ L) (m : ℕ) (q v : FourierL2) (x : SchrodingerTorus) : expandingTorusFunction a k L (fderiv ℝ (expandingOddPower a k L ha ha1 hk hL m) q v) x = ((m + 1 : ℕ) : ℂ) * (expandingTorusFunction a k L q x) ^ m * star (expandingTorusFunction a k L q x) ^ m * expandingTorusFunction a k L v x + (m : ℂ) * (expandingTorusFunction a k L q x) ^ (m + 1) * star (expandingTorusFunction a k L q x) ^ (m - 1) * star (expandingTorusFunction a k L v x) := by …Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.SchrodingerTorus, OAI.DefocusingNLS.expandingTorusFunction, OAI.DefocusingNLS.expandingOddPower
- theorem
OAI.DefocusingNLS.expandingNonlinearRemainder_pointwiseline 44Source documentation
The abstract remainder evaluates to the actual scalar nonlinear Taylor remainder.
theorem expandingNonlinearRemainder_pointwise (a k L : ℝ) (ha : 0 < a) (ha1 : a < 1) (hk : 8 < k) (hL : 1 ≤ L) (m : ℕ) (q v : FourierL2) (x : SchrodingerTorus) : expandingTorusFunction a k L (expandingNonlinearRemainder a k L ha ha1 hk hL m q v) x = oddPowerNonlinearity m (expandingTorusFunction a k L q x + expandingTorusFunction a k L v x) - oddPowerNonlinearity m (expandingTorusFunction a k L q x) - oddPowerDerivative m (expandingTorusFunction a k L q x) (expandingTorusFunction a k L v x) := by …Mentions: OAI.DefocusingNLS.FourierL2, OAI.DefocusingNLS.SchrodingerTorus, OAI.DefocusingNLS.expandingTorusFunction, OAI.DefocusingNLS.expandingNonlinearRemainder, OAI.DefocusingNLS.oddPowerNonlinearity, OAI.DefocusingNLS.oddPowerDerivative