OAI/Analysis/KadisonKastler/AEBoundaryDiagonal.lean
4 declarations, 0 contain sorry, 0 declared as axioms
Diagonal comparison from almost-everywhere cocycle data
A countable group has a common invariant conull set for the cocycle laws and approximation bounds. Outside that set the generating family is filled with one good value. This provides global bounds for the least-vector and polar constructions; covariance is required only on the conull set.
- theorem
OAI.KadisonKastler.exists_measurable_diagonal_unitary_on_setline 35Source documentation
Global boundedness suffices for the measurable least field. The cocycle laws need hold only on the set where covariance is asserted.
theorem exists_measurable_diagonal_unitary_on_set (J : Algebra M →ₗ[ℂ] E) (hJ : ∀ x, ‖J x‖ = traceTwoNorm τ x) (hτ : FiniteVectorTrace τ) {G D : Type*} [Group G] [Countable G] [MeasurableSpace D] {μ : Measure (D × D)} (S : Set D) (shift : G → D → D) (W : G → D → unitary (Algebra M)) (hW : ∀ g t x, x ∈ S → (W (g * t) x : Algebra M) = (W g x : Algebra M) * (W t (shift g x) : Algebra M)) (hWmeas : ∀ t, AEStronglyMeasurable (fun p : D × D => J ((W t p.1 : Algebra M) * star (W t p.2 : Algebra M))) μ) {r : ℝ} (hr0 : 0 ≤ r) (hr : r < 1) (hnear : ∀ t x y, ‖(W t x : Algebra M) * star (W t y : Algebra M) - 1‖ ≤ r) : ∃ a : D → D → unitary (Algebra M), …Mentions: OAI.KadisonKastler.Algebra, OAI.KadisonKastler.traceTwoNorm, OAI.KadisonKastler.FiniteVectorTrace
- theorem
OAI.KadisonKastler.norm_unitary_mul_star_sub_oneline 125Source documentation
The unitary-pair displacement equals the distance between the pair.
theorem norm_unitary_mul_star_sub_one (u v : unitary (Algebra M)) : ‖(u : Algebra M) * star (v : Algebra M) - 1‖ = ‖(u : Algebra M) - v‖ := by …Mentions: OAI.KadisonKastler.Algebra
- theorem
OAI.KadisonKastler.exists_ae_measurable_diagonal_unitary_comparisonline 135Source documentation
Countably many almost-everywhere laws give the diagonal comparison, with its explicit
4δdisplacement and almost-everywhere covariance.theorem exists_ae_measurable_diagonal_unitary_comparison (J : Algebra M →ₗ[ℂ] E) (hJ : ∀ x, ‖J x‖ = traceTwoNorm τ x) (hτ : FiniteVectorTrace τ) (α : NonsingularAction G D μ) (W : G → D → unitary (Algebra M)) (hW : ∀ g t, ∀ᵐ x ∂μ, (W (g * t) x : Algebra M) = (W g x : Algebra M) * (W t (α.toPerm g⁻¹ x) : Algebra M)) (hWmeas : ∀ t, AEStronglyMeasurable (fun p : D × D => J ((W t p.1 : Algebra M) * star (W t p.2 : Algebra M))) (μ.prod μ)) (U : G → unitary (H →L[ℂ] H)) {δ : ℝ} (hδ : 0 ≤ δ) (hsmall : 2 * δ < 1) (hclose : ∀ g, ∀ᵐ x ∂μ, ‖(W g x : Algebra M).val - (U g : H →L[ℂ] H)‖ ≤ δ) : ∃ a : D → D → unitary (Algebra M), AEStronglyMeasurable (fun p : D × D => J (a p.1 p.2 : Algebra M)) (μ.prod μ) ∧ …Mentions: OAI.KadisonKastler.Algebra, OAI.KadisonKastler.traceTwoNorm, OAI.KadisonKastler.FiniteVectorTrace, OAI.KadisonKastler.NonsingularAction
- theorem
OAI.KadisonKastler.StandardTracialPosition.exists_ae_diagonal_unitary_comparisonline 224Source documentation
The standard-position version needs only measurable operator evaluations of the original cocycle. Its diagonal unitary field is likewise measurable on every vector of the ambient Hilbert space.
theorem StandardTracialPosition.exists_ae_diagonal_unitary_comparison (p : StandardTracialPosition M) (α : NonsingularAction G D μ) (W : G → D → unitary (Algebra M)) (hW : ∀ g t, ∀ᵐ x ∂μ, (W (g * t) x : Algebra M) = (W g x : Algebra M) * (W t (α.toPerm g⁻¹ x) : Algebra M)) (hWmeas : ∀ g ξ, AEStronglyMeasurable (fun x => (W g x : Algebra M).val ξ) μ) (U : G → unitary (H →L[ℂ] H)) {δ : ℝ} (hδ : 0 ≤ δ) (hsmall : 2 * δ < 1) (hclose : ∀ g, ∀ᵐ x ∂μ, ‖(W g x : Algebra M).val - (U g : H →L[ℂ] H)‖ ≤ δ) : ∃ a : D → D → unitary (Algebra M), (∀ ξ, AEStronglyMeasurable (fun x : D × D => (a x.1 x.2 : Algebra M).val ξ) (μ.prod μ)) ∧ (∀ x y, ‖(a x y : Algebra M) - 1‖ ≤ 4 * δ) ∧ …Mentions: OAI.KadisonKastler.StandardTracialPosition, OAI.KadisonKastler.NonsingularAction, OAI.KadisonKastler.Algebra