import Mathlib.Analysis.CStarAlgebra.Unitary.Span import OAI.Analysis.FactorGeneration.CornerTrace namespace OAI noncomputable section namespace Generator.Tracial /-! The least-norm unitary-orbit point is scalar when the coordinate inclusion has scalar commutant. -/ section open scoped Topology open UltrapowerBridge variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] variable {M : VonNeumannAlgebra H} (τ : TracialRepresentation M) def subalgebraUnitaries (P : StarSubalgebra ℂ M.toStarSubalgebra) : Subgroup (unitary M.toStarSubalgebra) where carrier := {u | (u : M.toStarSubalgebra) ∈ P} one_mem' := P.one_mem mul_mem' hu hv := P.mul_mem hu hv inv_mem' hu := by change star _ ∈ P exact star_mem hu def ambientUnitary (P : StarSubalgebra ℂ M.toStarSubalgebra) (u : unitary P) : subalgebraUnitaries P := ⟨Unitary.map { toFun := P.subtype, map_one' := map_one _, map_mul' := map_mul _, map_star' := map_star _ } u, u.val.property⟩ theorem commutes_of_fixed_unitaries (P : StarSubalgebra ℂ M.toStarSubalgebra) [CompleteSpace P] (c : M.toStarSubalgebra) (hc : ∀ u : subalgebraUnitaries P, conjugateLinear u.val c = c) : ∀ a : P, (a : M.toStarSubalgebra)*c = c*(a : M.toStarSubalgebra) := by let : CStarAlgebra P := {} intro a obtain ⟨u, s, ha, _⟩ := CStarAlgebra.exists_sum_four_unitary a have hu (i : Fin 4) : ((u i).val : M.toStarSubalgebra)*c = c*((u i).val : M.toStarSubalgebra) := by have h := congrArg (fun z : M.toStarSubalgebra => z * ((u i).val : M.toStarSubalgebra)) (hc (ambientUnitary P (u i))) change (((u i).val : M.toStarSubalgebra)*c*star ((u i).val : M.toStarSubalgebra))*((u i).val : M.toStarSubalgebra) = _ at h have he : star ((u i).val : M.toStarSubalgebra)*((u i).val : M.toStarSubalgebra) = 1 := congrArg Subtype.val (u i).property.1 simpa only [mul_assoc, he, mul_one] using h change P.subtype a*c = c*P.subtype a rw [ha, map_sum, Finset.sum_mul, Finset.mul_sum] apply Finset.sum_congr rfl intro i _ simp only [map_smul, smul_mul_assoc, mul_smul_comm] exact congrArg (fun z : M.toStarSubalgebra => s i • z) (hu i) /-- Irreducibility is exactly the coordinate relative-commutant hypothesis. Completeness of P is automatic for a von Neumann subalgebra, and is used only to express its elements as sums of four unitaries. -/ theorem scalar_mem_traceOrbitHull (P : StarSubalgebra ℂ M.toStarSubalgebra) [CompleteSpace P] (hirr : ∀ c : M.toStarSubalgebra, (∀ a : P, (a : M.toStarSubalgebra)*c = c*(a : M.toStarSubalgebra)) → ∃ z : ℂ, c = z • (1 : M.toStarSubalgebra)) (b : M.toStarSubalgebra) : baseVector τ (τ.trace b • (1 : M.toStarSubalgebra)) ∈ traceOrbitHull τ (subalgebraUnitaries P) b := by obtain ⟨c, _, hc, _, hfixed⟩ := traceOrbitHull_minimum τ (subalgebraUnitaries P) b obtain ⟨z, rfl⟩ := hirr c (commutes_of_fixed_unitaries P c hfixed) have hz := traceOrbitHull_trace τ (subalgebraUnitaries P) b hc have he : z = τ.trace b := by change inner ℂ τ.vector (z • τ.vector) = _ at hz rw [inner_smul_right, inner_self_eq_norm_sq_to_K, τ.norm_vector] at hz simpa using hz simpa only [he] using hc theorem trace_distance_le_unitary_displacement (P : StarSubalgebra ℂ M.toStarSubalgebra) [CompleteSpace P] (hirr : ∀ c : M.toStarSubalgebra, (∀ a : P, (a : M.toStarSubalgebra)*c = c*(a : M.toStarSubalgebra)) → ∃ z : ℂ, c = z • (1 : M.toStarSubalgebra)) (b : M.toStarSubalgebra) (δ : ℝ) (hδ : ∀ u : subalgebraUnitaries P, τ.norm₂ (conjugateLinear u.val b-b) ≤ δ) : τ.norm₂ (b-τ.trace b • (1 : M.toStarSubalgebra)) ≤ δ := by have h := traceOrbitHull_distance τ (subalgebraUnitaries P) b δ hδ (scalar_mem_traceOrbitHull τ P hirr b) rw [norm_sub_rev] at h exact h end /-! Irreducibility excludes disconnected nonzero ambient projections. This gives the projection part of irreducibility in every nonzero corner. -/ open scoped Topology open UltrapowerBridge variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] variable {M : VonNeumannAlgebra H} (τ : TracialRepresentation M) variable (P : StarSubalgebra ℂ M.toStarSubalgebra) [CompleteSpace P] variable (hirr : ∀ c : M.toStarSubalgebra, (∀ a : P, (a : M.toStarSubalgebra)*c=c*(a : M.toStarSubalgebra)) → ∃ z : ℂ, c=z • (1 : M.toStarSubalgebra)) theorem baseVector_inner_eq_trace (a b : M.toStarSubalgebra) : inner ℂ (baseVector τ a) (baseVector τ b)=τ.trace (star a*b) := by change _ = inner ℂ τ.vector (star (a : H →L[ℂ] H) ((b : H →L[ℂ] H) τ.vector)) rw [ContinuousLinearMap.star_eq_adjoint,ContinuousLinearMap.adjoint_inner_right] rfl /-- A continuous trace test vanishing on an orbit vanishes on its closed convex hull. -/ theorem orbitHull_trace_test_zero (G : Subgroup (unitary M.toStarSubalgebra)) (b d : M.toStarSubalgebra) (hd : ∀ u : G, τ.trace (star d * conjugateLinear u.val b)=0) {ξ : H} (hξ : ξ ∈ traceOrbitHull τ G b) : inner ℂ (baseVector τ d) ξ=0 := by let K : Set H := {ξ | inner ℂ (baseVector τ d) ξ=0} have hc : IsClosed K := isClosed_eq (continuous_const.inner continuous_id) continuous_const have hv : Convex ℝ K := by intro x hx y hy s t hs ht hst change inner ℂ (baseVector τ d) (s • x+t • y)=0 rw [inner_add_right,inner_smul_right_eq_smul,inner_smul_right_eq_smul] change s • inner ℂ (baseVector τ d) x+t • inner ℂ (baseVector τ d) y=0 rw [show inner ℂ (baseVector τ d) x=0 from hx, show inner ℂ (baseVector τ d) y=0 from hy,smul_zero,smul_zero,add_zero] apply (closure_minimal (convexHull_min ?_ hv) hc) hξ rintro _ ⟨a,⟨u,rfl⟩,rfl⟩ exact (baseVector_inner_eq_trace τ d (conjugateLinear u.val b)).trans (hd u) include τ hirr in /-- Nonzero ambient projections cannot have all their P matrix coefficients zero in an irreducible inclusion. No comparison theorem is assumed. -/ theorem projection_eq_zero_or_eq_zero_of_no_links (r s : AlgebraProjection M) (hlink : ∀ a : P, s.val*(a : M.toStarSubalgebra)*r.val=0) : r.val=0 ∨ s.val=0 := by have htest : ∀ u : subalgebraUnitaries P, τ.trace (star s.val*conjugateLinear u.val r.val)=0 := by intro u change τ.trace (star s.val*((u.val : M.toStarSubalgebra)*r.val* star (u.val : M.toStarSubalgebra)))=0 rw [s.property.isSelfAdjoint.star_eq,← mul_assoc,← mul_assoc, hlink ⟨u.val.val,u.property⟩,zero_mul] exact inner_zero_right _ have hz := orbitHull_trace_test_zero τ (subalgebraUnitaries P) r.val s.val htest (scalar_mem_traceOrbitHull τ P hirr r.val) rw [map_smul,inner_smul_right,baseVector_inner_eq_trace, s.property.isSelfAdjoint.star_eq,mul_one] at hz rcases mul_eq_zero.mp hz with hr | hs · left by_contra hn have hp := projection_trace_pos τ r.val r.property hn rw [hr,Complex.zero_re] at hp exact (lt_irrefl 0 hp) · right by_contra hn have hp := projection_trace_pos τ s.val s.property hn rw [hs,Complex.zero_re] at hp exact (lt_irrefl 0 hp) include τ hirr in /-- Every projection commuting with pPp inside pMp is either zero or p. -/ theorem corner_commutant_projection_trivial (p r : AlgebraProjection M) (hrp : r ≤ p) (hr : ∀ a : P, Commute r.val (p.val*(a : M.toStarSubalgebra)*p.val)) : r.val=0 ∨ r.val=p.val := by let s : AlgebraProjection M := ⟨p.val-r.val,r.property.sub_of_mul_eq_right p.property hrp⟩ have hlink (a : P) : s.val*(a : M.toStarSubalgebra)*r.val=0 := by have hl : p.val*r.val=r.val := hrp have hright := projection_mul_of_le hrp have he := congrArg (fun z : M.toStarSubalgebra => z*r.val) (hr a).eq simp only [mul_assoc,hl,r.property.isIdempotentElem.eq] at he have he' : r.val*((p.val*(a : M.toStarSubalgebra))*r.val)= (p.val*(a : M.toStarSubalgebra))*r.val := by simpa only [mul_assoc,hl,r.property.isIdempotentElem.eq] using he have he'' : r.val*(a : M.toStarSubalgebra)*r.val= p.val*(a : M.toStarSubalgebra)*r.val := by simpa only [← mul_assoc,hright] using he' change (p.val-r.val)*(a : M.toStarSubalgebra)*r.val=0 rw [sub_mul,sub_mul,he'',sub_self] rcases projection_eq_zero_or_eq_zero_of_no_links τ P hirr r s hlink with h | h · exact Or.inl h · exact Or.inr (sub_eq_zero.mp h).symm end Generator.Tracial end end OAI