OAI/MathematicalPhysics/DefocusingNLS/Certificates/ForwardHermitianForm.lean
10 declarations, 0 contain sorry, 0 declared as axioms
The Hermitian matrix represented by a finite forward cone
- def
OAI.DefocusingNLS.forwardFormEntryline 11 - theorem
OAI.DefocusingNLS.star_eq_neg_of_re_zeroline 16 - theorem
OAI.DefocusingNLS.forwardFormEntry_hermitianline 19 - theorem
OAI.DefocusingNLS.forwardFormEntry_diagonalline 26 - theorem
OAI.DefocusingNLS.coneForm_as_hermitianline 36 - theorem
OAI.DefocusingNLS.hermitianPairForm_eq_quadraticline 43 - theorem
OAI.DefocusingNLS.forwardFormEntry_expansionline 52 - theorem
OAI.DefocusingNLS.forwardFormEntry_pairFormline 64Source documentation
The Hermitian quadratic form is twice the forward cone form.
theorem forwardFormEntry_pairForm (M : ℝ) (s : ℂ) (T : Matrix (Fin 2) (Fin 2) ℂ) (hs : s.re = 0) (u v : ℂ) : hermitianPairForm (forwardFormEntry M s T 0 0).re (forwardFormEntry M s T 1 1).re (forwardFormEntry M s T 0 1) u v = 2 * matrixCone M s T ![u, v] := by …Mentions: OAI.DefocusingNLS.hermitianPairForm, OAI.DefocusingNLS.forwardFormEntry, OAI.DefocusingNLS.matrixCone
- theorem
OAI.DefocusingNLS.hermitianPairForm_addline 74 - theorem
OAI.DefocusingNLS.positive_sum_matrixConeline 82Source documentation
Positive leading entry and determinant of the summed Hermitian matrix supply the positivity needed for exclusion of matching zeros.
theorem positive_sum_matrixCone (M : ℝ) (s₁ s₂ : ℂ) (T₁ T₂ : Matrix (Fin 2) (Fin 2) ℂ) (hs₁ : s₁.re = 0) (hs₂ : s₂.re = 0) (ha : 0 < (forwardFormEntry M s₁ T₁ 0 0).re + (forwardFormEntry M s₂ T₂ 0 0).re) (hdet : 0 < ((forwardFormEntry M s₁ T₁ 0 0).re + (forwardFormEntry M s₂ T₂ 0 0).re) * ((forwardFormEntry M s₁ T₁ 1 1).re + (forwardFormEntry M s₂ T₂ 1 1).re) - Complex.normSq (forwardFormEntry M s₁ T₁ 0 1 + forwardFormEntry M s₂ T₂ 0 1)) (w : Fin 2 → ℂ) (hw : w ≠ 0) : 0 < matrixCone M s₁ T₁ w + matrixCone M s₂ T₂ w := by …Mentions: OAI.DefocusingNLS.forwardFormEntry, OAI.DefocusingNLS.matrixCone