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namespace OAI
noncomputable section
namespace Generator.Tracial
/-! Complete each supported partial unitary by the identity on its orthogonal
complement. If the quotient support is one, the quotient value is unchanged. -/
section
open UltrapowerBridge Filter
variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]
variable {N M : VonNeumannAlgebra H}
def PartialUnitary.completed (v : PartialUnitary M) : M.toStarSubalgebra :=
v.val+(1-v.support.val)
theorem PartialUnitary.completed_unitary (v : PartialUnitary M) :
v.completed ∈ _root_.unitary M.toStarSubalgebra := by
have hp := v.support.property.isIdempotentElem.eq
have hs := v.support.property.isSelfAdjoint.star_eq
have hi := v.unitary.initial
have hf := v.unitary.final
have hleft := v.unitary.support_mul
have hright := v.unitary.mul_support
have hleft' := v.unitary.adjoint.support_mul
have hright' := v.unitary.adjoint.mul_support
dsimp only [CornerUnitary.adjoint] at hleft' hright'
constructor <;>
simp only [PartialUnitary.completed,star_add,star_sub,star_one,hs,add_mul,mul_add,
sub_mul,mul_sub,one_mul,mul_one,hi,hf,hleft,hright,hleft',hright',hp] <;> abel
theorem PartialUnitary.completed_mem (v : PartialUnitary M)
(hv : v.val.val ∈ N) : v.completed.val ∈ N := by
have hp : v.support.val.val ∈ N := by
rw [← v.unitary.initial]
have hstar : star v.val.val ∈ N := star_mem hv
exact N.mul_mem hstar hv
exact N.add_mem hv (N.sub_mem N.one_mem hp)
def boundedCompletedUnitary (u : ℕ → PartialUnitary M) : Bounded M :=
boundedPartialUnitary u+(1-boundedPartialSupport u)
@[simp] theorem boundedCompletedUnitary_apply (u : ℕ → PartialUnitary M) (j : ℕ) :
(boundedCompletedUnitary u).val j=(u j).completed := rfl
theorem boundedCompletedUnitary_unitary (u : ℕ → PartialUnitary M) (j : ℕ) :
(boundedCompletedUnitary u).val j ∈ _root_.unitary M.toStarSubalgebra :=
(u j).completed_unitary
theorem quotient_completed_eq (τ : TracialRepresentation M) (ω : Ultrafilter ℕ)
(u : ℕ → PartialUnitary M)
(hi : star (quotientMap τ (ω : Filter ℕ) (boundedPartialUnitary u))*
quotientMap τ (ω : Filter ℕ) (boundedPartialUnitary u)=1) :
quotientMap τ (ω : Filter ℕ) (boundedCompletedUnitary u)=
quotientMap τ (ω : Filter ℕ) (boundedPartialUnitary u) := by
have hp : quotientMap τ (ω : Filter ℕ) (boundedPartialSupport u)=1 := by
rw [← boundedPartialUnitary_initial,map_mul,quotientMap_star]
exact hi
let q := quotientMap τ (ω : Filter ℕ)
have hs : q (1-boundedPartialSupport u)=0 :=
(map_sub q 1 (boundedPartialSupport u)).trans
((congrArg₂ (fun a b => a-b) (map_one q) hp).trans (sub_self _))
exact (map_add q (boundedPartialUnitary u) (1-boundedPartialSupport u)).trans
((congrArg (fun b => q (boundedPartialUnitary u)+b) hs).trans (add_zero _))
theorem bounded_unitary_of_coordinates (a : Bounded M)
(ha : ∀ j,a.val j ∈ _root_.unitary M.toStarSubalgebra) : a ∈ _root_.unitary (Bounded M) := by
constructor
· apply Subtype.ext; funext j; exact (ha j).1
· apply Subtype.ext; funext j; exact (ha j).2
theorem quotient_unitary_of_coordinates (τ : TracialRepresentation M) (ω : Ultrafilter ℕ)
(a : Bounded M) (ha : ∀ j,a.val j ∈ _root_.unitary M.toStarSubalgebra) :
quotientMap τ (ω : Filter ℕ) a ∈ _root_.unitary (Q τ ω) := by
have hu := bounded_unitary_of_coordinates a ha
constructor
· rw [← quotientMap_star,← map_mul,hu.1,map_one]
· rw [← quotientMap_star,← map_mul,hu.2,map_one]
theorem bounded_coordinate_unitaries_inclusion (hNM : N ≤ M) (a : Bounded M)
(ha : ∀ j,a.val j ∈ _root_.unitary M.toStarSubalgebra ∧ (a.val j).val ∈ N) :
∃ b : Bounded N,(∀ j,b.val j ∈ _root_.unitary N.toStarSubalgebra) ∧ boundedInclusion hNM b=a := by
let b : Bounded N := ⟨fun j => ⟨(a.val j).val,(ha j).2⟩,a.property⟩
refine ⟨b,?_,rfl⟩
intro j
constructor
· apply Subtype.ext
change star (a.val j).val*(a.val j).val=1
exact congrArg (fun x : M.toStarSubalgebra => x.val) (ha j).1.1
· apply Subtype.ext
change (a.val j).val*star (a.val j).val=1
exact congrArg (fun x : M.toStarSubalgebra => x.val) (ha j).1.2
end
/-! Ordered independence with actual coordinate unitaries in the included
algebra, obtained by completing the constructed partial-unitary coordinates. -/
section
open UltrapowerBridge Filter
variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]
variable {N M : VonNeumannAlgebra H} (τ : TracialRepresentation M)
variable (hNM : N ≤ M)
variable (hfactor : ∀ c : N.toStarSubalgebra,
(∀ a : N.toStarSubalgebra,a*c=c*a) → ∃ z : ℂ,c=z • (1 : N.toStarSubalgebra))
variable (hdiff : ∀ r : N.toStarSubalgebra,IsStarProjection r → r ≠ 0 →
∃ q : N.toStarSubalgebra,IsStarProjection q ∧ q ≠ 0 ∧ q ≠ r ∧ r*q=q ∧ q*r=q)
variable (hirr : ∀ c : M.toStarSubalgebra,
(∀ a : N.toStarSubalgebra,coordinateInclusion hNM a*c=c*coordinateInclusion hNM a) →
∃ z : ℂ,c=z • (1 : M.toStarSubalgebra))
variable (hsep : TopologicalSpace.IsSeparable (Set.range (baseVector τ)))
include hfactor hdiff hirr hsep
theorem exists_coordinate_ordered_unitary
(ω : Ultrafilter ℕ) (hω : (ω : Filter ℕ) ≤ atTop)
(x : ℕ → Q τ ω) (hx : ∀ i,quotientTrace τ ω (x i)=0) :
∃ b : Bounded M,
(∀ j,b.val j ∈ unitary M.toStarSubalgebra ∧ (b.val j).val ∈ N) ∧
ExactOrderedMoments τ ω (quotientMap τ (ω : Filter ℕ) b) x := by
obtain ⟨u,hu,hi,hf,hm⟩ := exists_full_support_ordered_independence τ hNM
hfactor hdiff hirr hsep ω hω x hx
refine ⟨boundedCompletedUnitary u,?_,?_⟩
· intro j
exact ⟨boundedCompletedUnitary_unitary u j,(u j).completed_mem (hu j)⟩
· rwa [quotient_completed_eq τ ω u hi]
end
/-! Two coordinate-unitary witnesses produce the reduced-moment Haar precursor
while retaining actual unitary coordinates in the included algebra. -/
section
open UltrapowerBridge Filter
variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]
variable {N M : VonNeumannAlgebra H} (τ : TracialRepresentation M)
variable (hNM : N ≤ M)
variable (hfactor : ∀ c : N.toStarSubalgebra,
(∀ a : N.toStarSubalgebra,a*c=c*a) → ∃ z : ℂ,c=z • (1 : N.toStarSubalgebra))
variable (hdiff : ∀ r : N.toStarSubalgebra,IsStarProjection r → r ≠ 0 →
∃ q : N.toStarSubalgebra,IsStarProjection q ∧ q ≠ 0 ∧ q ≠ r ∧ r*q=q ∧ q*r=q)
variable (hirr : ∀ c : M.toStarSubalgebra,
(∀ a : N.toStarSubalgebra,coordinateInclusion hNM a*c=c*coordinateInclusion hNM a) →
∃ z : ℂ,c=z • (1 : M.toStarSubalgebra))
variable (hsep : TopologicalSpace.IsSeparable (Set.range (baseVector τ)))
include hfactor hdiff hirr hsep
theorem exists_coordinate_reduced_unitary
(ω : Ultrafilter ℕ) (hω : (ω : Filter ℕ) ≤ atTop)
(x : ℕ → Q τ ω) (hx : ∀ i,quotientTrace τ ω (x i)=0) :
∃ a : Bounded M,
(∀ j,a.val j ∈ unitary M.toStarSubalgebra ∧ (a.val j).val ∈ N) ∧
ReducedOrderedMoments τ ω (quotientMap τ (ω : Filter ℕ) a) x := by
obtain ⟨a,ha,ham⟩ := exists_coordinate_ordered_unitary τ hNM hfactor hdiff hirr hsep ω hω x hx
let u := quotientMap τ (ω : Filter ℕ) a
have hu : u ∈ unitary (Q τ ω) := quotient_unitary_of_coordinates τ ω a (fun j => (ha j).1)
obtain ⟨b,hb,hbm⟩ := exists_coordinate_ordered_unitary τ hNM hfactor hdiff hirr hsep ω hω
(productCenteredFamily τ ω u x) (productCenteredFamily_centered τ ω u x hu.2 hx ham)
refine ⟨a*b,?_,?_⟩
· intro j
exact ⟨(unitary M.toStarSubalgebra).mul_mem (ha j).1 (hb j).1,N.mul_mem (ha j).2 (hb j).2⟩
· rw [map_mul]
intro c d sign xs hxs
exact product_reduced_moment τ ω u (quotientMap τ (ω : Filter ℕ) b) x hbm c d sign xs hxs
end
/-! Full integer endpoint moments and an actual included coordinate-unitary
Haar witness, before imposing an operator topology on generated algebras. -/
open UltrapowerBridge Filter
variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]
variable {N M : VonNeumannAlgebra H} (τ : TracialRepresentation M) (ω : Ultrafilter ℕ)
variable (hNM : N ≤ M)
variable (hfactor : ∀ c : N.toStarSubalgebra,
(∀ a : N.toStarSubalgebra,a*c=c*a) → ∃ z : ℂ,c=z • (1 : N.toStarSubalgebra))
variable (hdiff : ∀ r : N.toStarSubalgebra,IsStarProjection r → r ≠ 0 →
∃ q : N.toStarSubalgebra,IsStarProjection q ∧ q ≠ 0 ∧ q ≠ r ∧ r*q=q ∧ q*r=q)
variable (hirr : ∀ c : M.toStarSubalgebra,
(∀ a : N.toStarSubalgebra,coordinateInclusion hNM a*c=c*coordinateInclusion hNM a) →
∃ z : ℂ,c=z • (1 : M.toStarSubalgebra))
variable (hsep : TopologicalSpace.IsSeparable (Set.range (baseVector τ)))
include hfactor hdiff hirr hsep
omit hfactor hdiff hirr hsep in
private theorem coordinate_haar_endpoints_of_coordinates
(D : Subalgebra ℂ (Q τ ω)) (x : ℕ → Q τ ω)
(hdense : ∀ d ∈ D,quotientTrace τ ω d=0 → d ∈ closure (Set.range x))
(a : Bounded M)
(ha : ∀ j,a.val j ∈ unitary M.toStarSubalgebra ∧ (a.val j).val ∈ N)
(hm : ReducedOrderedMoments τ ω (quotientMap τ (ω : Filter ℕ) a) x) :
∃ t : unitary (Q τ ω),
(∃ b : Bounded N,(∀ j,b.val j ∈ unitary N.toStarSubalgebra) ∧
quotientInclusion τ hNM (ω : Filter ℕ)
(quotientMap (restrictedTrace τ hNM) (ω : Filter ℕ) b)=(t : Q τ ω)) ∧
(∀ n : ℤ,n ≠ 0 → quotientTrace τ ω (↑(t^n) : Q τ ω)=0) ∧
∀ c ∈ D,∀ d ∈ D,∀ n : ℤ,n ≠ 0 → ∀ xs : List (Q τ ω × ℤ),
(∀ z ∈ xs,z.1 ∈ D ∧ quotientTrace τ ω z.1=0 ∧ z.2 ≠ 0) →
quotientTrace τ ω (c*integerValueWord τ ω t n xs d)=0 := by
let t : unitary (Q τ ω) := ⟨quotientMap τ (ω : Filter ℕ) a,
quotient_unitary_of_coordinates τ ω a (fun j => (ha j).1)⟩
obtain ⟨b,hb⟩ := bounded_coordinate_unitaries_inclusion hNM a ha
have hhaar := reducedOrderedMoments_haar τ ω t x hm
refine ⟨t,⟨b,hb.1,?_⟩,hhaar,?_⟩
· change quotientMap τ (ω : Filter ℕ) (boundedInclusion hNM b)=quotientMap τ (ω : Filter ℕ) a
exact congrArg (quotientMap τ (ω : Filter ℕ)) hb.2
· intro c hc d hd n hn xs hxs
apply reduced_integer_moment_closedSpan τ ω t x hm c d
(subalgebra_mem_centered_closedSpan τ ω D x hdense c hc)
(subalgebra_mem_centered_closedSpan τ ω D x hdense d hd) n hn xs
intro z hz
exact ⟨Submodule.closure_subset_topologicalClosure_span _
(hdense z.1 (hxs z hz).1 (hxs z hz).2.1),(hxs z hz).2.2⟩
private theorem coordinate_haar_endpoints_of_dense_family (hω : (ω : Filter ℕ) ≤ atTop)
(D : Subalgebra ℂ (Q τ ω)) (x : ℕ → Q τ ω)
(hx : ∀ i,x i ∈ D ∧ quotientTrace τ ω (x i)=0)
(hdense : ∀ d ∈ D,quotientTrace τ ω d=0 → d ∈ closure (Set.range x)) :
∃ t : unitary (Q τ ω),
(∃ b : Bounded N,(∀ j,b.val j ∈ unitary N.toStarSubalgebra) ∧
quotientInclusion τ hNM (ω : Filter ℕ)
(quotientMap (restrictedTrace τ hNM) (ω : Filter ℕ) b)=(t : Q τ ω)) ∧
(∀ n : ℤ,n ≠ 0 → quotientTrace τ ω (↑(t^n) : Q τ ω)=0) ∧
∀ c ∈ D,∀ d ∈ D,∀ n : ℤ,n ≠ 0 → ∀ xs : List (Q τ ω × ℤ),
(∀ z ∈ xs,z.1 ∈ D ∧ quotientTrace τ ω z.1=0 ∧ z.2 ≠ 0) →
quotientTrace τ ω (c*integerValueWord τ ω t n xs d)=0 := by
obtain ⟨a,ha⟩ := exists_coordinate_reduced_unitary (H := H) (N := N) (M := M) τ hNM hfactor hdiff hirr hsep
ω hω x (fun i => (hx i).2)
exact coordinate_haar_endpoints_of_coordinates τ ω hNM D x hdense a ha.1 ha.2
theorem exists_coordinate_haar_endpoints (hω : (ω : Filter ℕ) ≤ atTop)
(D : Subalgebra ℂ (Q τ ω)) (hD : TopologicalSpace.IsSeparable (D : Set (Q τ ω))) :
∃ t : unitary (Q τ ω),
(∃ b : Bounded N,(∀ j,b.val j ∈ unitary N.toStarSubalgebra) ∧
quotientInclusion τ hNM (ω : Filter ℕ)
(quotientMap (restrictedTrace τ hNM) (ω : Filter ℕ) b)=(t : Q τ ω)) ∧
(∀ n : ℤ,n ≠ 0 → quotientTrace τ ω (↑(t^n) : Q τ ω)=0) ∧
∀ c ∈ D,∀ d ∈ D,∀ n : ℤ,n ≠ 0 → ∀ xs : List (Q τ ω × ℤ),
(∀ z ∈ xs,z.1 ∈ D ∧ quotientTrace τ ω z.1=0 ∧ z.2 ≠ 0) →
quotientTrace τ ω (c*integerValueWord τ ω t n xs d)=0 := by
obtain ⟨x,hx⟩ := exists_centered_dense_quotient_family (H := H) (M := M) τ ω D hD
exact coordinate_haar_endpoints_of_dense_family τ ω hNM hfactor hdiff hirr hsep
hω D x hx.1 hx.2
end Generator.Tracial
end
end OAI
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