import Mathlib.Analysis.SpecialFunctions.Complex.CircleAddChar import Mathlib.LinearAlgebra.Matrix.Trace import OAI.Analysis.FactorGeneration.MatrixUnits import OAI.Analysis.FactorGeneration.ProjectionComparison import OAI.Analysis.FactorGeneration.SpectralApproximation namespace OAI noncomputable section namespace Generator /-! Equal-trace finite partitions extend to actual matrix units in the same factor. The theorem also retains a prescribed corner as the sum of diagonals. -/ open scoped BigOperators namespace Tracial open UltrapowerBridge variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] variable {M : VonNeumannAlgebra H} (τ : TracialRepresentation M) variable (hfactor : ∀ c : M.toStarSubalgebra, (∀ a : M.toStarSubalgebra, a*c=c*a) → ∃ z : ℂ, c=z • (1 : M.toStarSubalgebra)) include hfactor in theorem exists_matrixUnits_for_partition {p : AlgebraProjection M} (Q : CornerPartition p) (hn : 0 < Q.size) (ht : ∀ i j, τ.trace (Q.piece i).val=τ.trace (Q.piece j).val) : ∃ E : Fin Q.size → Fin Q.size → M.toStarSubalgebra, (∀ i, E i i=(Q.piece i).val) ∧ (∀ i j, star (E i j)=E j i) ∧ (∀ i j k l, E i j*E k l=if j=k then E i l else 0) ∧ (∑ i, E i i)=p.val := by classical let o : Fin Q.size := ⟨0,hn⟩ have hv : ∀ i, ∃ v : M.toStarSubalgebra, star v*v=(Q.piece o).val ∧ v*star v=(Q.piece i).val := fun i => exists_partialIsometry_of_trace_eq τ hfactor (Q.piece o) (Q.piece i) (ht o i) choose v hvi hvf using hv let V (i : Fin Q.size) : PartialIsometry M := ⟨Q.piece o,v i,hvi i⟩ have htarget (i : Fin Q.size) : (V i).target=Q.piece i := Subtype.ext (hvf i) have hcross (i j : Fin Q.size) (hij : i≠j) : star (v i)*v j=0 := by exact (V i).adjoint.mul_eq_zero (V j) (by change (V i).target.val*(V j).target.val=0 rw [htarget,htarget] exact Q.orthogonal i j hij) let E (i j : Fin Q.size) := v i*star (v j) refine ⟨E,hvf,?_,?_,?_⟩ · intro i j simp only [E,star_mul,star_star] · intro i j k l by_cases hjk : j=k · subst k rw [ite_eq_left rfl] change (v i*star (v j))*(v j*star (v l))=v i*star (v l) calc _ = (v i*(star (v j)*v j))*star (v l) := by simp only [mul_assoc] _ = v i*star (v l) := by rw [hvi,show v i*(Q.piece o).val=v i from (V i).mul_support] · rw [ite_eq_right hjk] change (v i*star (v j))*(v k*star (v l))=0 calc _ = (v i*(star (v j)*v k))*star (v l) := by simp only [mul_assoc] _ = 0 := by rw [hcross j k hjk,mul_zero,zero_mul] · simpa only [E,hvf] using Q.total end Tracial /-! The matrix-unit image in the original represented algebra, with its finite dimensionality and weak-operator closedness proved. -/ open scoped BigOperators section open UltrapowerBridge variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] variable {M : VonNeumannAlgebra H} {ι : Type*} [Fintype ι] [DecidableEq ι] namespace MatrixUnitSystem variable (E : Generator.MatrixUnitSystem ι M.toStarSubalgebra) def concreteHom : Matrix ι ι ℂ →⋆ₐ[ℂ] (H →L[ℂ] H) := M.toStarSubalgebra.subtype.comp E.hom def concreteAlgebra : StarSubalgebra ℂ (H →L[ℂ] H) := E.concreteHom.range theorem concreteAlgebra_le : E.concreteAlgebra ≤ M.toStarSubalgebra := by rintro x ⟨a,rfl⟩ exact (E.hom a).property theorem mem_concreteAlgebra (x : M.toStarSubalgebra) : x.val ∈ E.concreteAlgebra ↔ x ∈ E.algebra := by constructor · rintro ⟨a,ha⟩ exact ⟨a,Subtype.ext ha⟩ · rintro ⟨a,ha⟩ exact ⟨a,congrArg Subtype.val ha⟩ instance concrete_finiteDimensional : FiniteDimensional ℂ E.concreteAlgebra := by change FiniteDimensional ℂ E.concreteHom.toAlgHom.range exact FiniteDimensional.of_surjective E.concreteHom.toAlgHom.rangeRestrict.toLinearMap E.concreteHom.toAlgHom.rangeRestrict_surjective def wotLinearMap : Matrix ι ι ℂ →ₗ[ℂ] (H →WOT[ℂ] H) := (ContinuousLinearMap.WOTofCLM.toLinearMap).comp E.concreteHom.toAlgHom.toLinearMap theorem concreteAlgebra_wotClosed : WOTClosed E.concreteAlgebra := by have heq : {T : H →WOT[ℂ] H | T.toCLM ∈ E.concreteAlgebra} = (E.wotLinearMap.range : Set (H →WOT[ℂ] H)) := by ext T constructor · rintro ⟨a,ha⟩ exact ⟨a, congrArg ContinuousLinearMapWOT.ofCLM ha⟩ · rintro ⟨a,ha⟩ exact ⟨a,congrArg ContinuousLinearMapWOT.toCLM ha⟩ unfold WOTClosed rw [heq] exact E.wotLinearMap.range.closed_of_finiteDimensional theorem concreteHom_injective (o : ι) (ho : E.entry o o ≠ 0) : Function.Injective E.concreteHom := Subtype.val_injective.comp (E.hom_injective o ho) end MatrixUnitSystem namespace Tracial theorem exists_matrixAlgebra_for_unit_partition (τ : TracialRepresentation M) (hfactor : ∀ c : M.toStarSubalgebra, (∀ a : M.toStarSubalgebra, a*c=c*a) → ∃ z : ℂ, c=z • (1 : M.toStarSubalgebra)) (Q : CornerPartition (identityProjection M)) (hn : 0 < Q.size) (ht : ∀ i j, τ.trace (Q.piece i).val=τ.trace (Q.piece j).val) : ∃ E : Generator.MatrixUnitSystem (Fin Q.size) M.toStarSubalgebra, (∀ i, E.entry i i=(Q.piece i).val) ∧ Function.Injective E.hom ∧ E.concreteAlgebra ≤ M.toStarSubalgebra ∧ WOTClosed E.concreteAlgebra := by obtain ⟨e,hd,hs,hm,hu⟩ := exists_matrixUnits_for_partition τ hfactor Q hn ht let E : Generator.MatrixUnitSystem (Fin Q.size) M.toStarSubalgebra := ⟨e,hs,hm,hu⟩ have : Nontrivial M.toStarSubalgebra := by apply nontrivial_of_ne (0 : M.toStarSubalgebra) 1 intro h have ht := congrArg τ.trace h have hz : τ.trace 0=0 := by simp [TracialRepresentation.trace] rw [hz,τ.trace_one] at ht exact zero_ne_one ht have : Nonempty (Fin Q.size) := ⟨⟨0,hn⟩⟩ exact ⟨E,hd,E.injective,E.concreteAlgebra_le,E.concreteAlgebra_wotClosed⟩ end Tracial end /-! The actual relative commutant in M is a diffuse scalar-center von Neumann algebra, with the restricted faithful trace available from M. -/ namespace MatrixUnitSystem section open UltrapowerBridge variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] variable {M : VonNeumannAlgebra H} {ι : Type*} [Fintype ι] [DecidableEq ι] variable (E : MatrixUnitSystem ι M.toStarSubalgebra) def relativeStar : StarSubalgebra ℂ (H →L[ℂ] H) where carrier := {x | ∃ a : E.commutant, a.val.val=x} zero_mem' := ⟨0,rfl⟩ one_mem' := ⟨1,rfl⟩ add_mem' := by rintro x y ⟨a,rfl⟩ ⟨b,rfl⟩; exact ⟨a+b,rfl⟩ mul_mem' := by rintro x y ⟨a,rfl⟩ ⟨b,rfl⟩; exact ⟨a*b,rfl⟩ algebraMap_mem' z := ⟨algebraMap ℂ E.commutant z,rfl⟩ star_mem' := by rintro x ⟨a,rfl⟩; exact ⟨star a,rfl⟩ theorem relativeStar_mem (x : H →L[ℂ] H) : x ∈ E.relativeStar ↔ x ∈ M ∧ ∀ i j, (E.entry i j).val*x=x*(E.entry i j).val := by constructor · rintro ⟨a,rfl⟩ exact ⟨a.val.property,fun i j => congrArg Subtype.val (a.property i j).eq⟩ · rintro ⟨hx,hc⟩ exact ⟨⟨⟨x,hx⟩,fun i j => Subtype.ext (hc i j)⟩,rfl⟩ theorem relativeStar_bicommutant : Set.centralizer (Set.centralizer (E.relativeStar : Set (H →L[ℂ] H))) = (E.relativeStar : Set (H →L[ℂ] H)) := by apply Set.Subset.antisymm · intro a ha apply (E.relativeStar_mem a).mpr constructor · rw [← SetLike.mem_coe,← M.centralizer_centralizer] exact fun b hb => ha b (fun c hc => hb c ((E.relativeStar_mem c).mp hc).1) · intro i j exact ha (E.entry i j).val (fun b hb => (((E.relativeStar_mem b).mp hb).2 i j).symm) · intro a ha b hb exact (hb a ha).symm def relativeVonNeumann : VonNeumannAlgebra H where toStarSubalgebra := E.relativeStar centralizer_centralizer' := E.relativeStar_bicommutant theorem relativeVonNeumann_le : E.relativeVonNeumann ≤ M := by intro x hx exact ((E.relativeStar_mem x).mp hx).1 def relativeEquiv : E.commutant ≃⋆ₐ[ℂ] E.relativeVonNeumann.toStarSubalgebra where toFun a := ⟨a.val.val,⟨a,rfl⟩⟩ invFun a := ⟨⟨a.val,((E.relativeStar_mem a.val).mp a.property).1⟩, fun i j => Subtype.ext (((E.relativeStar_mem a.val).mp a.property).2 i j)⟩ left_inv _ := rfl right_inv _ := rfl map_mul' _ _ := rfl map_add' _ _ := rfl map_smul' _ _ := rfl map_star' _ := rfl theorem relative_scalar_center (o : ι) (hfactor : ∀ c : M.toStarSubalgebra, (∀ a : M.toStarSubalgebra,a*c=c*a) → ∃ z : ℂ,c=z • (1 : M.toStarSubalgebra)) (c : E.relativeVonNeumann.toStarSubalgebra) (hc : ∀ a : E.relativeVonNeumann.toStarSubalgebra,a*c=c*a) : ∃ z : ℂ,c=z • (1 : E.relativeVonNeumann.toStarSubalgebra) := by obtain ⟨z,hz⟩ := E.commutant_scalar_center o hfactor (E.relativeEquiv.symm c) (by intro a apply E.relativeEquiv.injective change E.relativeEquiv (a*E.relativeEquiv.symm c)= E.relativeEquiv (E.relativeEquiv.symm c*a) rw [map_mul,map_mul,E.relativeEquiv.apply_symm_apply] exact hc (E.relativeEquiv a)) refine ⟨z,?_⟩ have h := congrArg E.relativeEquiv hz simpa only [StarAlgEquiv.apply_symm_apply,map_smul,map_one] using h theorem relative_diffuse (o : ι) (hdiff : ∀ p : M.toStarSubalgebra,IsStarProjection p → p ≠ 0 → ∃ q : M.toStarSubalgebra,IsStarProjection q ∧ q ≠ 0 ∧ q ≠ p ∧ p*q=q ∧ q*p=q) (p : E.relativeVonNeumann.toStarSubalgebra) (hp : IsStarProjection p) (hp0 : p ≠ 0) : ∃ q : E.relativeVonNeumann.toStarSubalgebra, IsStarProjection q ∧ q ≠ 0 ∧ q ≠ p ∧ p*q=q ∧ q*p=q := by obtain ⟨q,hq,hq0,hqp,hpq,hqp'⟩ := E.commutant_diffuse o hdiff (E.relativeEquiv.symm p) (hp.map E.relativeEquiv.symm) (by intro h apply hp0 simpa using congrArg E.relativeEquiv h) refine ⟨E.relativeEquiv q,?_,?_,?_,?_,?_⟩ · exact hq.map E.relativeEquiv.toStarAlgHom · intro h apply hq0 exact E.relativeEquiv.injective (h.trans (map_zero E.relativeEquiv).symm) · intro h apply hqp exact E.relativeEquiv.injective (h.trans (E.relativeEquiv.apply_symm_apply p).symm) · simpa only [map_mul,StarAlgEquiv.apply_symm_apply] using congrArg E.relativeEquiv hpq · simpa only [map_mul,StarAlgEquiv.apply_symm_apply] using congrArg E.relativeEquiv hqp' end /-! Passing an irreducible inclusion through a common finite matrix algebra preserves irreducibility of the actual relative commutants. -/ variable {ι A B : Type*} [Fintype ι] [DecidableEq ι] variable [Ring A] [StarRing A] [Algebra ℂ A] [StarModule ℂ A] variable [Ring B] [StarRing B] [Algebra ℂ B] [StarModule ℂ B] omit [StarModule ℂ A] [StarModule ℂ B] in theorem commute_mapped_of_amplify (E : MatrixUnitSystem ι A) (o : ι) (f : A →⋆ₐ[ℂ] B) (y : B) (hE : ∀ i j,Commute (f (E.entry i j)) y) (hamp : ∀ a : A,Commute (f (E.amplify o a)) y) (x : A) : Commute (f x) y := by rw [← E.reconstruct o x,map_sum] apply Commute.sum_left intro i hi rw [map_sum] apply Commute.sum_left intro j hj rw [map_mul,map_mul] exact ((hE i o).mul_left (hamp _)).mul_left (hE o j) open UltrapowerBridge Tracial variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] variable {N M : VonNeumannAlgebra H} variable (E : MatrixUnitSystem ι N.toStarSubalgebra) (hNM : N ≤ M) theorem relative_inclusion : E.relativeVonNeumann ≤ (E.map (coordinateInclusion hNM)).relativeVonNeumann := by intro x hx have h := (E.relativeStar_mem x).mp hx apply ((E.map (coordinateInclusion hNM)).relativeStar_mem x).mpr exact ⟨hNM h.1,h.2⟩ theorem relative_irreducible (o : ι) (hirr : ∀ c : M.toStarSubalgebra, (∀ a : N.toStarSubalgebra,coordinateInclusion hNM a*c=c*coordinateInclusion hNM a) → ∃ z : ℂ,c=z • (1 : M.toStarSubalgebra)) (c : (E.map (coordinateInclusion hNM)).relativeVonNeumann.toStarSubalgebra) (hc : ∀ a : E.relativeVonNeumann.toStarSubalgebra, coordinateInclusion (E.relative_inclusion hNM) a*c= c*coordinateInclusion (E.relative_inclusion hNM) a) : ∃ z : ℂ,c=z • (1 : (E.map (coordinateInclusion hNM)).relativeVonNeumann.toStarSubalgebra) := by let F := E.map (coordinateInclusion hNM) let cM := coordinateInclusion F.relativeVonNeumann_le c have hentries : ∀ i j,Commute (coordinateInclusion hNM (E.entry i j)) cM := by intro i j apply Subtype.ext exact ((F.relativeStar_mem c.val).mp c.property).2 i j have hamp (a : N.toStarSubalgebra) : Commute (coordinateInclusion hNM (E.amplify o a)) cM := by let b : E.relativeVonNeumann.toStarSubalgebra := E.relativeEquiv ⟨E.amplify o a,E.amplify_mem o a⟩ apply Subtype.ext exact congrArg (fun t : F.relativeVonNeumann.toStarSubalgebra => t.val) (hc b) obtain ⟨z,hz⟩ := hirr cM (fun x => E.commute_mapped_of_amplify o (coordinateInclusion hNM) cM hentries hamp x) exact ⟨z,Subtype.ext (congrArg (fun t : M.toStarSubalgebra => t.val) hz)⟩ end MatrixUnitSystem /-! Explicit Bell projections in two equal finite matrix factors. -/ open scoped BigOperators namespace Bell variable {n : ℕ} [NeZero n] theorem char_sum (t : ZMod n) : (∑ i : ZMod n, ZMod.stdAddChar (t*i)) = if t=0 then (n : ℂ) else 0 := by split_ifs with h · simp [h] · exact AddChar.sum_eq_zero_of_ne_one (ZMod.isPrimitive_stdAddChar n h) theorem char_star (t : ZMod n) : star (ZMod.stdAddChar t) = ZMod.stdAddChar (-t) := by simp only [ZMod.stdAddChar_apply, AddChar.map_neg_eq_inv] exact (Circle.coe_inv_eq_conj (ZMod.toCircle t)).symm def projection (s f : ZMod n) : Matrix (ZMod n × ZMod n) (ZMod n × ZMod n) ℂ := fun a b => if a.2=a.1+s ∧ b.2=b.1+s then (n : ℂ)⁻¹ * ZMod.stdAddChar (f*(a.1-b.1)) else 0 theorem projection_star (s f : ZMod n) : star (projection s f) = projection s f := by ext a b change star (projection s f b a)=projection s f a b simp only [projection, apply_ite star, star_mul, char_star, star_zero] rw [show -(f*(b.1-a.1))=f*(a.1-b.1) by ring] simp [and_comm, mul_comm] theorem projection_mul (s f t g : ZMod n) : projection s f * projection t g = if s=t ∧ f=g then projection s f else 0 := by ext a b simp only [Matrix.mul_apply, Fintype.sum_prod_type, projection] have hterm (i j : ZMod n) : (if a.2=a.1+s ∧ j=i+s then (n : ℂ)⁻¹*ZMod.stdAddChar (f*(a.1-i)) else 0) * (if j=i+t ∧ b.2=b.1+t then (n : ℂ)⁻¹*ZMod.stdAddChar (g*(i-b.1)) else 0) = if a.2=a.1+s ∧ b.2=b.1+t ∧ s=t then if j=i+s then (n : ℂ)⁻¹^2 * ZMod.stdAddChar (f*a.1-g*b.1) * ZMod.stdAddChar ((g-f)*i) else 0 else 0 := by by_cases ha : a.2=a.1+s · by_cases hb : b.2=b.1+t · by_cases hs : s=t · subst t by_cases hj : j=i+s · simp only [ha,hb,hj,and_self,ite_true] calc _ = (n : ℂ)⁻¹^2 * (ZMod.stdAddChar (f*(a.1-i)) * ZMod.stdAddChar (g*(i-b.1))) := by ring _ = _ := by rw [← AddChar.map_add_eq_mul, show f*(a.1-i)+g*(i-b.1)=(f*a.1-g*b.1)+(g-f)*i by ring, AddChar.map_add_eq_mul] ring · simp [ha,hb,hj] · by_cases hj : j=i+s · simp [ha,hb,hs,hj] · simp [ha,hb,hs,hj] · simp [hb] · simp [ha] simp_rw [hterm] by_cases hs : s=t · subst t by_cases ha : a.2=a.1+s ∧ b.2=b.1+s · simp only [ha.1,ha.2,and_self,ite_true,Finset.sum_ite_eq',Finset.mem_univ] rw [← Finset.mul_sum, char_sum] by_cases hf : f=g · subst g simp only [sub_self,ite_true,Matrix.ite_apply,Matrix.zero_apply, and_self, projection, ha, ite_true] rw [show f*a.1-f*b.1=f*(a.1-b.1) by ring] field_simp · simp [sub_eq_zero,Ne.symm hf,hf] · simp [ha,Matrix.ite_apply,projection] · simp [hs] theorem projection_total : (∑ s : ZMod n, ∑ f : ZMod n, projection s f) = 1 := by ext a b simp only [Matrix.sum_apply, Matrix.one_apply] have hf (s : ZMod n) : (∑ f : ZMod n, projection s f a b) = if a.2=a.1+s ∧ b.2=b.1+s ∧ a.1=b.1 then 1 else 0 := by simp only [projection] by_cases h : a.2=a.1+s ∧ b.2=b.1+s · simp only [h.1,h.2,and_self,true_and,ite_true] rw [← Finset.mul_sum] simp_rw [mul_comm _ (a.1-b.1)] rw [char_sum] by_cases hab : a.1=b.1 · simp [hab] · simp [hab,sub_eq_zero] · simp [h,show ¬(a.2=a.1+s ∧ b.2=b.1+s ∧ a.1=b.1) by tauto] simp_rw [hf] by_cases hab : a.1=b.1 · have hs (s : ZMod n) : a.2=a.1+s ↔ s=a.2-a.1 := by constructor · intro h; rw [h]; simp · intro h; rw [h]; abel simp_rw [hs] simp only [hab, and_true] simp_rw [ite_and] simp [Prod.ext_iff,hab,eq_comm] · simp [hab,show a≠b by exact fun h => hab (congrArg Prod.fst h)] /-- The matrix unit in the first tensor factor, with identity on the second. -/ def leftEntry (i j : ZMod n) : Matrix (ZMod n × ZMod n) (ZMod n × ZMod n) ℂ := fun a b => if a.1=i ∧ b.1=j ∧ a.2=b.2 then 1 else 0 theorem mul_leftEntry (X : Matrix (ZMod n × ZMod n) (ZMod n × ZMod n) ℂ) (i j : ZMod n) (a b : ZMod n × ZMod n) : (X * leftEntry i j) a b = if b.1=j then X a (i,b.2) else 0 := by simp only [Matrix.mul_apply,Fintype.sum_prod_type,leftEntry,mul_ite,mul_one,mul_zero] by_cases h : b.1=j · simp [h,ite_and] · simp [h] theorem projection_sandwich (s f i j : ZMod n) : projection s f * leftEntry i j * projection s f = if i=j then (n : ℂ)⁻¹ • projection s f else 0 := by apply Matrix.ext intro a b have hr : (if i=j then (n : ℂ)⁻¹ • projection s f else 0) a b = if i=j then (n : ℂ)⁻¹ * projection s f a b else 0 := by split_ifs <;> rfl rw [hr] rw [Matrix.mul_apply] simp only [mul_leftEntry,Fintype.sum_prod_type,ite_mul,zero_mul] simp only [Finset.sum_ite_irrel, Finset.sum_const_zero] simp only [Finset.sum_ite_eq',Finset.mem_univ,ite_true] have hterm (k : ZMod n) : projection s f a (i,k)*projection s f (j,k) b = if a.2=a.1+s ∧ b.2=b.1+s ∧ i=j then if k=i+s then (n : ℂ)⁻¹^2 * ZMod.stdAddChar (f*(a.1-b.1)) else 0 else 0 := by by_cases ha : a.2=a.1+s · by_cases hb : b.2=b.1+s · by_cases hij : i=j · subst j by_cases hk : k=i+s · simp only [projection,ha,hb,hk,and_self,ite_true] calc _ = (n : ℂ)⁻¹^2 * (ZMod.stdAddChar (f*(a.1-i)) * ZMod.stdAddChar (f*(i-b.1))) := by ring _ = _ := by rw [← AddChar.map_add_eq_mul, show f*(a.1-i)+f*(i-b.1)=f*(a.1-b.1) by ring] · simp [projection,ha,hb,hk] · by_cases hk : k=i+s · simp [projection,ha,hb,hij,hk] · simp [projection,ha,hb,hij,hk] · simp [projection,hb] · simp [projection,ha] simp_rw [hterm] by_cases hij : i=j <;> by_cases h : a.2=a.1+s ∧ b.2=b.1+s <;> simp [hij,h,projection,pow_two,mul_assoc] end Bell /-! Exact normalized traces of constructed matrix algebras and all their commuting product refinements. -/ open scoped BigOperators namespace MatrixUnitSystem section open UltrapowerBridge Tracial variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] variable {M : VonNeumannAlgebra H} {ι : Type*} [Fintype ι] [DecidableEq ι] variable (E : MatrixUnitSystem ι M.toStarSubalgebra) (τ : TracialRepresentation M) theorem trace_diagonal_eq (i j : ι) : τ.trace (E.entry i i)=τ.trace (E.entry j j) := by have h := τ.trace_mul_comm (E.entry i j) (E.entry j i) simpa only [E.mul_entry,ite_true] using h theorem trace_off_diagonal (i j : ι) (hij : i ≠ j) : τ.trace (E.entry i j)=0 := by have h := τ.trace_mul_comm (E.entry i i) (E.entry i j) simpa [E.mul_entry,hij,Ne.symm hij,TracialRepresentation.trace] using h theorem trace_diagonal (o : ι) : τ.trace (E.entry o o)=(Fintype.card ι : ℂ)⁻¹ := by have h : (Fintype.card ι : ℂ)*τ.trace (E.entry o o)=1 := by calc _ = ∑ i, τ.trace (E.entry i i) := by simp only [E.trace_diagonal_eq τ _ o,Finset.sum_const,Finset.card_univ,nsmul_eq_mul] _ = τ.trace (∑ i,E.entry i i) := by let t : M.toStarSubalgebra →+ ℂ := { toFun := τ.trace, map_zero' := by simp [TracialRepresentation.trace], map_add' := τ.trace_add } exact (map_sum t _ _).symm _ = 1 := by rw [E.total,τ.trace_one] exact eq_inv_of_mul_eq_one_right h theorem trace_hom (_ : ι) (a : Matrix ι ι ℂ) : τ.trace (E.hom a)=(Fintype.card ι : ℂ)⁻¹*Matrix.trace a := by have hsum (b : ι → M.toStarSubalgebra) : τ.trace (∑ i,b i)=∑ i,τ.trace (b i) := by let t : M.toStarSubalgebra →+ ℂ := { toFun := τ.trace, map_zero' := by simp [TracialRepresentation.trace], map_add' := τ.trace_add } exact map_sum t _ _ rw [E.hom_apply,hsum] simp only [hsum,τ.trace_smul] have hentry (i j : ι) : τ.trace (E.entry i j)= if i=j then (Fintype.card ι : ℂ)⁻¹ else 0 := by split · next h => subst j; exact E.trace_diagonal τ i · next h => exact E.trace_off_diagonal τ i j h simp only [hentry,mul_ite,mul_zero,Finset.sum_ite_eq,Finset.mem_univ,ite_true] rw [Matrix.trace,Finset.mul_sum] exact Finset.sum_congr rfl fun i _ => mul_comm _ _ end open UltrapowerBridge Tracial variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H] variable {M : VonNeumannAlgebra H} {n : ℕ} [NeZero n] variable (E F : MatrixUnitSystem (ZMod n) M.toStarSubalgebra) variable (hc : ∀ i j k l,Commute (E.entry i j) (F.entry k l)) theorem product_hom_leftEntry (i j : ZMod n) : (E.product F hc).hom (Bell.leftEntry i j) = E.entry i j := by simp only [hom_apply,Fintype.sum_prod_type,Bell.leftEntry,ite_smul,one_smul,zero_smul] simp only [ite_and,Finset.sum_ite_irrel,Finset.sum_const_zero,Finset.sum_ite_eq',Finset.mem_univ,ite_true] rw [← E.product_sum_left F hc i j] apply Finset.sum_congr rfl intro k hk rw [Finset.sum_eq_single j] · simp · intro l hl hlj simp [hlj] · simp def bellPiece (s f : ZMod n) : AlgebraProjection M := ⟨(E.product F hc).hom (Bell.projection s f),by constructor · show (E.product F hc).hom (Bell.projection s f) * (E.product F hc).hom (Bell.projection s f) = _ rw [← map_mul,Bell.projection_mul,ite_eq_left ⟨rfl,rfl⟩] · show star ((E.product F hc).hom (Bell.projection s f)) = _ rw [← map_star,Bell.projection_star]⟩ theorem bellPiece_orthogonal (a b : ZMod n × ZMod n) (h : a≠b) : (E.bellPiece F hc a.1 a.2).val * (E.bellPiece F hc b.1 b.2).val = 0 := by change (E.product F hc).hom _ * (E.product F hc).hom _ = 0 rw [← map_mul,Bell.projection_mul,ite_eq_right (fun he => h (Prod.ext he.1 he.2)),map_zero] theorem bellPiece_total : (∑ a : ZMod n × ZMod n,(E.bellPiece F hc a.1 a.2).val) = 1 := by change (∑ a : ZMod n × ZMod n,(E.product F hc).hom (Bell.projection a.1 a.2))=1 rw [← map_sum,Fintype.sum_prod_type,Bell.projection_total,map_one] def bellPartition : CornerPartition (identityProjection M) where size := Fintype.card (ZMod n × ZMod n) piece i := let a := (Fintype.equivFin (ZMod n × ZMod n)).symm i E.bellPiece F hc a.1 a.2 orthogonal _ _ h := E.bellPiece_orthogonal F hc _ _ (fun he => h ((Fintype.equivFin (ZMod n × ZMod n)).symm.injective he)) total := ((Fintype.equivFin (ZMod n × ZMod n)).symm.sum_comp (fun a => (E.bellPiece F hc a.1 a.2).val)).trans (E.bellPiece_total F hc) theorem bellPiece_sandwich_entry (s f i j : ZMod n) : (E.bellPiece F hc s f).val * E.entry i j * (E.bellPiece F hc s f).val = if i=j then (n : ℂ)⁻¹ • (E.bellPiece F hc s f).val else 0 := by rw [← E.product_hom_leftEntry F hc i j] change ((E.product F hc).hom _ * (E.product F hc).hom _) * (E.product F hc).hom _ = _ rw [← map_mul,← map_mul,Bell.projection_sandwich] split <;> simp [bellPiece,map_smul] theorem bellPartition_pinch_entry (i j : ZMod n) : (E.bellPartition F hc).pinch (E.entry i j) = if i=j then (n : ℂ)⁻¹ • (1 : M.toStarSubalgebra) else 0 := by have hpiece (a : Fin (E.bellPartition F hc).size) : ((E.bellPartition F hc).piece a).val * E.entry i j * ((E.bellPartition F hc).piece a).val = if i=j then (n : ℂ)⁻¹ • ((E.bellPartition F hc).piece a).val else 0 := E.bellPiece_sandwich_entry F hc _ _ i j unfold CornerPartition.pinch simp_rw [hpiece] split · simp only [← Finset.smul_sum,(E.bellPartition F hc).total] rfl · simp theorem bellPartition_pinch_algebra (τ : TracialRepresentation M) (x : M.toStarSubalgebra) (hx : x ∈ E.algebra) : (E.bellPartition F hc).pinch x = τ.trace x • (1 : M.toStarSubalgebra) := by obtain ⟨a,rfl⟩ := hx change (E.bellPartition F hc).pinch (E.hom a)=τ.trace (E.hom a) • 1 rw [E.trace_hom τ 0] have hsum (y : ZMod n → M.toStarSubalgebra) : (E.bellPartition F hc).pinch (∑ i,y i) = ∑ i,(E.bellPartition F hc).pinch (y i) := by simp only [CornerPartition.pinch,Finset.mul_sum,Finset.sum_mul] exact Finset.sum_comm simp only [hom_apply,hsum,CornerPartition.pinch_smul,E.bellPartition_pinch_entry F hc, smul_ite,smul_zero,Finset.sum_ite_eq,Finset.mem_univ,ite_true,smul_smul] rw [← Finset.sum_smul,Matrix.trace,Finset.mul_sum] congr 1 simp [ZMod.card,mul_comm] end MatrixUnitSystem end Generator end end OAI