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import OAI.Analysis.FactorGeneration.ProjectionEncoding
import OAI.Analysis.FactorGeneration.TensorRefinement
namespace OAI
noncomputable section
namespace Generator
/-! Diagonal projections and one full-support rank-one projection generate
every finite full matrix algebra, including matrices larger than size two. -/
namespace MatrixUnitSystem
open scoped BigOperators
variable {ι A : Type*} [Fintype ι] [DecidableEq ι]
variable [Ring A] [StarRing A] [Algebra ℂ A] [StarModule ℂ A]
variable (E : MatrixUnitSystem ι A)
def fullProjectionMatrix : Matrix ι ι ℂ := fun _ _ => (Fintype.card ι : ℂ)⁻¹
omit [DecidableEq ι] in
theorem fullProjectionMatrix_projection [Nonempty ι] :
IsStarProjection (fullProjectionMatrix (ι := ι)) := by
have hn : (Fintype.card ι : ℂ) ≠ 0 := by exact_mod_cast Fintype.card_ne_zero
constructor
· ext i j
simp only [Matrix.mul_apply,fullProjectionMatrix,Finset.sum_const,Finset.card_univ,
nsmul_eq_mul]
field_simp
· ext i j
simp [fullProjectionMatrix,Matrix.star_apply]
def fullProjection : A := E.hom (fullProjectionMatrix (ι := ι))
theorem fullProjection_projection [Nonempty ι] : IsStarProjection E.fullProjection :=
(fullProjectionMatrix_projection (ι := ι)).map E.hom
omit [StarModule ℂ A] in
theorem diagonal_commute (i j : ι) : Commute (E.entry i i) (E.entry j j) := by
show E.entry i i*E.entry j j=E.entry j j*E.entry i i
by_cases h : i=j
· subst j; rfl
· simp [E.mul_entry,h,Ne.symm h]
theorem cut_fullProjection (i j : ι) :
E.entry i i*E.fullProjection*E.entry j j=(Fintype.card ι : ℂ)⁻¹ • E.entry i j := by
simp only [fullProjection,hom_apply,fullProjectionMatrix,Finset.mul_sum,Finset.sum_mul,
mul_smul_comm,E.mul_entry,smul_ite,smul_zero]
simp [E.mul_entry,smul_ite]
theorem recover_entry [Nonempty ι] (i j : ι) :
(Fintype.card ι : ℂ) • (E.entry i i*E.fullProjection*E.entry j j)=E.entry i j := by
rw [E.cut_fullProjection,smul_smul,mul_inv_cancel₀,one_smul]
exact_mod_cast Fintype.card_ne_zero
theorem fullProjection_mem : E.fullProjection ∈ E.algebra := ⟨_,rfl⟩
theorem algebra_le_of_projection_mem [Nonempty ι] (S : StarSubalgebra ℂ A)
(hd : ∀ i,E.entry i i ∈ S) (hq : E.fullProjection ∈ S) : E.algebra ≤ S := by
apply (E.algebra_le_iff S).mpr
intro i j
rw [← E.recover_entry i j]
exact S.smul_mem (S.mul_mem (S.mul_mem (hd i) hq) (hd j)) _
theorem algebra_eq_adjoin_projections [Nonempty ι] :
E.algebra = StarAlgebra.adjoin ℂ (Set.range (fun i => E.entry i i) ∪ {E.fullProjection}) := by
apply le_antisymm
· apply E.algebra_le_of_projection_mem
· intro i; exact StarAlgebra.subset_adjoin ℂ _ (Or.inl ⟨i,rfl⟩)
· exact StarAlgebra.subset_adjoin ℂ _ (Or.inr rfl)
· apply StarAlgebra.adjoin_le
rintro x (⟨i,rfl⟩ | rfl)
· exact E.entry_mem i i
· exact E.fullProjection_mem
end MatrixUnitSystem
/-! Two actual self-adjoint generators for the weak closure of countably
many pairwise commuting finite full matrix factors. -/
section
variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]
theorem countable_projection_generator {ι : Type*} [Countable ι] [Nonempty ι]
(e : ι → (H →L[ℂ] H)) (hp : ∀ i,IsStarProjection (e i))
(hc : ∀ i j,Commute (e i) (e j)) :
∃ b : H →L[ℂ] H,IsSelfAdjoint b ∧ ‖b‖ ≤ 1 ∧ wstar {b}=wstar (Set.range e) := by
obtain ⟨f,hf⟩ := exists_surjective_nat ι
obtain ⟨b,hb,hn,hgen⟩ := CommutingProjectionEncoding.exists_selfAdjoint_generator
(fun n => e (f n)) (fun n => hp (f n)) (fun n m => hc (f n) (f m))
refine ⟨b,hb,hn,hgen.trans ?_⟩
congr 1
ext x
constructor
· rintro ⟨n,rfl⟩; exact ⟨f n,rfl⟩
· rintro ⟨i,rfl⟩
obtain ⟨n,rfl⟩ := hf i
exact ⟨n,rfl⟩
namespace MatrixUnitSystem
variable {ι κ A : Type*} [Fintype ι] [DecidableEq ι] [Fintype κ] [DecidableEq κ]
variable [Ring A] [StarRing A] [Algebra ℂ A] [StarModule ℂ A]
theorem fullProjection_commute (E : MatrixUnitSystem ι A) (F : MatrixUnitSystem κ A)
(hc : ∀ i j k l,Commute (E.entry i j) (F.entry k l)) :
Commute E.fullProjection F.fullProjection := by
apply (E.commute_algebra_iff _).mpr _ _ E.fullProjection_mem
intro i j
exact ((F.commute_algebra_iff _).mpr (fun k l => (hc i j k l).symm) _
F.fullProjection_mem).symm
end MatrixUnitSystem
namespace FiniteMatrixStage
variable {N : VonNeumannAlgebra H}
theorem two_generators_of_commuting_factors (F : ℕ → FiniteMatrixStage N)
(hc : ∀ n m,n ≠ m → ∀ i j k l,
Commute ((F n).units.entry i j) ((F m).units.entry k l)) :
∃ a ∈ generated F,∃ b ∈ generated F,
IsSelfAdjoint a ∧ IsSelfAdjoint b ∧ wstar {a,b}=generated F := by
classical
let I := (n : ℕ) × Fin (F n).size
let : Nonempty I := ⟨⟨0,⟨0,(F 0).positive⟩⟩⟩
let (n : ℕ) : Nonempty (Fin (F n).size) := ⟨⟨0,(F n).positive⟩⟩
let d : I → (H →L[ℂ] H) := fun i => ((F i.1).units.entry i.2 i.2).val
let q : ℕ → (H →L[ℂ] H) := fun n => (F n).units.fullProjection.val
have hdproj (i : I) : IsStarProjection (d i) :=
((F i.1).units.diagonal_projection i.2).map N.toStarSubalgebra.subtype
have hqproj (n : ℕ) : IsStarProjection (q n) :=
(F n).units.fullProjection_projection.map N.toStarSubalgebra.subtype
have hdcomm (i j : I) : Commute (d i) (d j) := by
obtain ⟨n,i⟩ := i
obtain ⟨m,j⟩ := j
by_cases h : n=m
· subst m
exact congrArg Subtype.val ((F n).units.diagonal_commute i j).eq
· exact congrArg Subtype.val (hc n m h i i j j).eq
have hqcomm (n m : ℕ) : Commute (q n) (q m) := by
by_cases h : n=m
· subst m; exact Commute.refl _
· exact congrArg Subtype.val ((F n).units.fullProjection_commute (F m).units (hc n m h)).eq
obtain ⟨a,ha,_,hagen⟩ := countable_projection_generator d hdproj hdcomm
obtain ⟨b,hb,_,hbgen⟩ := countable_projection_generator q hqproj hqcomm
have hdmem (i : I) : d i ∈ generated F :=
stage_le_generated F i.1 (((F i.1).units.mem_concreteAlgebra _).mpr
((F i.1).units.entry_mem i.2 i.2))
have hqmem (n : ℕ) : q n ∈ generated F :=
stage_le_generated F n (((F n).units.mem_concreteAlgebra _).mpr (F n).units.fullProjection_mem)
have hamem : a ∈ generated F := by
have hle : wstar {a} ≤ generated F := by
rw [hagen]
exact wstar_le (generated_closed F) (by rintro _ ⟨i,rfl⟩; exact hdmem i)
exact hle (subset_wstar _ rfl)
have hbmem : b ∈ generated F := by
have hle : wstar {b} ≤ generated F := by
rw [hbgen]
exact wstar_le (generated_closed F) (by rintro _ ⟨n,rfl⟩; exact hqmem n)
exact hle (subset_wstar _ rfl)
refine ⟨a,hamem,b,hbmem,ha,hb,le_antisymm ?_ ?_⟩
· exact wstar_le (generated_closed F) (by rintro _ (rfl | rfl) <;> assumption)
· apply generated_minimal F _ (wstar_closed _)
intro n x hx
let y : N.toStarSubalgebra := ⟨x,(F n).units.concreteAlgebra_le hx⟩
let S := (wstar {a,b}).comap N.toStarSubalgebra.subtype
have hdS (i : Fin (F n).size) : (F n).units.entry i i ∈ S := by
change d ⟨n,i⟩ ∈ wstar {a,b}
apply (wstar_mono (s := {a}) (t := {a,b}) (by simp))
rw [hagen]
exact subset_wstar (Set.range d) (Set.mem_range_self (⟨n,i⟩ : I))
have hqS : (F n).units.fullProjection ∈ S := by
change q n ∈ wstar {a,b}
apply (wstar_mono (s := {b}) (t := {a,b}) (by simp))
rw [hbgen]
exact subset_wstar _ (Set.mem_range_self n)
exact (F n).units.algebra_le_of_projection_mem S hdS hqS
(((F n).units.mem_concreteAlgebra y).mp hx)
end FiniteMatrixStage
end
/-! The retained tensor extensions supply commuting factors generating
exactly the original matrix-union weak closure. -/
namespace FiniteMatrixStage
variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]
variable {N : VonNeumannAlgebra H}
theorem concrete_le_iff (E : FiniteMatrixStage N) (S : StarSubalgebra ℂ (H →L[ℂ] H)) :
E.units.concreteAlgebra ≤ S ↔ E.units.algebra ≤ S.comap N.toStarSubalgebra.subtype := by
constructor
· intro h x hx
exact h ((E.units.mem_concreteAlgebra x).mpr hx)
· intro h x hx
let y : N.toStarSubalgebra := ⟨x,E.units.concreteAlgebra_le hx⟩
exact h ((E.units.mem_concreteAlgebra y).mp hx)
theorem exists_commuting_factors_of_tensor_extensions (A : ℕ → FiniteMatrixStage N)
(hzero : A 0=scalarStage N) (hstep : ∀ n,TensorExtension (A n) (A (n+1))) :
∃ F : ℕ → FiniteMatrixStage N,
(∀ n m,n ≠ m → ∀ i j k l,Commute ((F n).units.entry i j) ((F m).units.entry k l)) ∧
generated F=generated A := by
have hm : Monotone (fun n => (A n).units.algebra) :=
monotone_nat_of_le_succ (fun n => (hstep n).algebra_le)
choose F hc he using hstep
have hFA (n : ℕ) : (F n).units.algebra ≤ (A (n+1)).units.algebra := by
rw [he n]; exact le_sup_right
have hcomm_lt (n m : ℕ) (hnm : n < m) (i j : Fin (F n).size) (k l : Fin (F m).size) :
Commute ((F n).units.entry i j) ((F m).units.entry k l) := by
exact ((A m).units.commute_algebra_iff _).mpr (fun a b => hc m a b k l) _
(hm (Nat.succ_le_of_lt hnm) (hFA n ((F n).units.entry_mem i j)))
refine ⟨F,?_,le_antisymm ?_ ?_⟩
· intro n m hnm i j k l
rcases lt_or_gt_of_ne hnm with h | h
· exact hcomm_lt n m h i j k l
· exact (hcomm_lt m n h k l i j).symm
· apply generated_minimal F _ (generated_closed A)
intro n
apply ((F n).concrete_le_iff _).mpr
exact (hFA n).trans (((A (n+1)).concrete_le_iff _).mp (stage_le_generated A (n+1)))
· apply generated_minimal A _ (generated_closed F)
intro n
apply ((A n).concrete_le_iff _).mpr
induction n with
| zero =>
rw [hzero]
apply ((scalarStage N).units.algebra_le_iff _).mpr
intro i j
exact (generated F).one_mem
| succ n ih =>
rw [he n]
exact sup_le ih (((F n).concrete_le_iff _).mp (stage_le_generated F n))
theorem two_generators_of_tensor_extensions (A : ℕ → FiniteMatrixStage N)
(hzero : A 0=scalarStage N) (hstep : ∀ n,TensorExtension (A n) (A (n+1))) :
∃ a ∈ generated A,∃ b ∈ generated A,
IsSelfAdjoint a ∧ IsSelfAdjoint b ∧ wstar {a,b}=generated A := by
obtain ⟨F,hF,hgen⟩ := exists_commuting_factors_of_tensor_extensions A hzero hstep
rw [← hgen]
exact two_generators_of_commuting_factors F hF
end FiniteMatrixStage
/-! The represented irreducible matrix subfactor can be constructed together
with two self-adjoint generators, without hyperfinite uniqueness. -/
namespace Tracial
open UltrapowerBridge FiniteMatrixStage
variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]
variable {N M : VonNeumannAlgebra H}
theorem exists_irreducible_two_generated_subfactor
(τ : TracialRepresentation M) (hNM : N ≤ M)
(hfactor : ∀ c : N.toStarSubalgebra,
(∀ a : N.toStarSubalgebra,a*c=c*a) → ∃ z : ℂ,c=z • (1 : N.toStarSubalgebra))
(hdiff : ∀ p : N.toStarSubalgebra,IsStarProjection p → p ≠ 0 →
∃ q : N.toStarSubalgebra,IsStarProjection q ∧ q ≠ 0 ∧ q ≠ p ∧ p*q=q ∧ q*p=q)
(hirr : ∀ c : M.toStarSubalgebra,
(∀ a : N.toStarSubalgebra,coordinateInclusion hNM a*c=c*coordinateInclusion hNM a) →
∃ z : ℂ,c=z • (1 : M.toStarSubalgebra))
(hsep : TopologicalSpace.IsSeparable (Set.range (baseVector τ))) :
∃ P : VonNeumannAlgebra H,P ≤ N ∧ IsII1Factor P.toStarSubalgebra ∧
(∀ c : M.toStarSubalgebra,(∀ a : P.toStarSubalgebra,a.val*c.val=c.val*a.val) →
c=τ.trace c • (1 : M.toStarSubalgebra)) ∧
∃ a ∈ P,∃ b ∈ P,IsSelfAdjoint a ∧ IsSelfAdjoint b ∧ wstar {a,b}=P.toStarSubalgebra := by
let S : Set M.toStarSubalgebra := {b | τ.trace b=0}
obtain ⟨x,hx,hdense⟩ := exists_countable_norm₂_dense τ S
⟨0,by change τ.trace 0=0; simp [TracialRepresentation.trace]⟩
(hsep.mono (Set.image_subset_range _ _))
obtain ⟨A,hA,hstep,_,_,hlim⟩ := exists_countable_tensor_refinement τ hNM
hfactor hdiff hirr x hx (scalarStage N)
have hscalar := generated_relative_scalar A τ hNM
(scalar_common_commutant_of_dense_energy_decay τ hNM A x hdense hlim)
obtain ⟨a,ha,b,hb,hsa,hsb,hgen⟩ := two_generators_of_tensor_extensions A hA hstep
exact ⟨generatedVonNeumann A,generatedVonNeumann_le A,
generated_isII1 A τ hNM hdiff hscalar,hscalar,a,ha,b,hb,hsa,hsb,hgen⟩
end Tracial
end Generator
end
end OAI