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import OAI.Analysis.FactorGeneration.AmplificationEncoding
import OAI.Analysis.FactorGeneration.Correlation
import OAI.Analysis.FactorGeneration.MatrixGenerators
import OAI.Analysis.FactorGeneration.PerturbationBounds
import OAI.Analysis.FactorGeneration.RelativeGeneration
namespace OAI
noncomputable section
namespace Generator.Tracial
/-! Relative generation under represented-factor hypotheses: unitaries in a dense G-delta set satisfy W*(N,u)=M. -/
open Filter
open scoped Topology
section
open UltrapowerBridge
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 relative_generation_at_continuity (u : TraceUnitary τ)
(hcont : ∀ x : M.toStarSubalgebra,
ContinuousAt (fun v => projectionNorm (relativeTraceSpace (N := N) τ v) (baseVector τ x)) u) :
relativeGenerated (N := N) τ u=M := by
classical
by_contra hneq
let Q := relativeGenerated (N := N) τ u
have hQM : Q ≤ M := relativeGenerated_le τ hNM u
obtain ⟨z,hz⟩ := exists_unitary_outside hQM hneq
let xi := subalgebraResidual τ hQM (z : M.toStarSubalgebra)
let s : ℝ := τ.norm₂ xi
have hs : 0 < s := subalgebraResidual_norm_pos τ hQM _ hz
let α : ℝ := min (1/4) (s/32)/2
have hα : 0 < α := half_pos (lt_min (by norm_num) (by positivity))
have hq : α < 1/4 := by
have h := min_le_left (1/4 : ℝ) (s/32)
dsimp [α] at hα ⊢
linarith
have hsmall : α < s/32 := by
have h := min_le_right (1/4 : ℝ) (s/32)
dsimp [α] at hα ⊢
linarith
have hhalf : α < 1/2 := by linarith
let ω : Ultrafilter ℕ := Ultrafilter.of atTop
have hω : (ω : Filter ℕ) ≤ atTop := Ultrafilter.of_le atTop
have he (n : ℕ) := exists_represented_perturbation τ ω hNM hfactor hdiff hirr hsep hω
u.toUnitary z xi (n+1) (Nat.succ_pos _) α hα hhalf
choose v t hv ht using he
let V : ℕ → TraceUnitary τ := fun n => ⟨v n⟩
have hV : Tendsto V atTop (𝓝 u) := by
apply (TraceUnitary.tendsto_iff τ atTop V u).mpr
exact squeeze_zero (fun _ => norm_nonneg _) hv (perturbation_size_tendsto α)
let F : TraceUnitary τ → ℝ := fun v =>
projectionNorm (relativeTraceSpace (N := N) τ v) (baseVector τ xi)
have hFzero : F u=0 := by
change ‖(vectorOrbitClosure Q.toStarSubalgebra τ.vector).starProjection
(baseVector τ (subalgebraResidual τ hQM (z : M.toStarSubalgebra)))‖=0
rw [subalgebraResidual_projection,norm_zero]
let δ : ℕ → ℝ := fun n => 1/((n+1 : ℕ) : ℝ)
have hδ : Tendsto δ atTop (𝓝 0) :=
tendsto_one_div_atTop_nhds_zero_nat.comp (tendsto_add_atTop_nat 1)
let c : ℕ → ℂ := fun n => τ.trace (star xi*relativeUnitaryWord τ hNM (V n) (t n) (n+1))
have hc (n : ℕ) : ‖c n-((α*s^2/2 : ℝ) : ℂ)‖ ≤
s*(4*α^2/(1-2*α))+δ n := by
have hn := ht n
have hcorr : τ.trace (star xi*(z : M.toStarSubalgebra))=(s : ℂ)^2 :=
subalgebraResidual_correlation τ hQM (z : M.toStarSubalgebra)
rw [hcorr] at hn
have heq : ((α*s^2/2 : ℝ) : ℂ)=(α : ℂ)/2*(s : ℂ)^2 := by
push_cast
ring
rw [heq]
exact hn
have hproj (n : ℕ) : ‖c n‖ ≤ F (V n) :=
relativeUnitaryWord_correlation_le τ hNM (V n) (t n) (n+1) xi
exact no_continuous_correlated_sequence F (hcont xi) hFzero V hV δ hδ c
hs hα hq hsmall hc hproj
theorem represented_relative_generation :
∃ C : Set (TraceUnitary τ), IsGδ C ∧ Dense C ∧
∀ u ∈ C, wstar ((N : Set (H →L[ℂ] H)) ∪ {(u.algebra τ).val})=M.toStarSubalgebra := by
obtain ⟨C,hC,hd,hcont⟩ := common_relative_projection_continuity_algebra τ hNM hsep
refine ⟨C,hC,hd,fun u hu => ?_⟩
exact congrArg VonNeumannAlgebra.toStarSubalgebra
(relative_generation_at_continuity τ hNM hfactor hdiff hirr hsep u (hcont u hu))
end
/-! Four generators under a faithful normalized vector trace and trace-vector separability. -/
open scoped ComplexStarModule
section
open UltrapowerBridge
variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]
variable {M : VonNeumannAlgebra H}
theorem represented_four_selfAdjoint_generators (τ : TracialRepresentation M)
(hfactor : ∀ c : M.toStarSubalgebra,
(∀ a : M.toStarSubalgebra,a*c=c*a) → ∃ z : ℂ,c=z • (1 : M.toStarSubalgebra))
(hdiff : ∀ p : M.toStarSubalgebra,IsStarProjection p → p ≠ 0 →
∃ q : M.toStarSubalgebra,IsStarProjection q ∧ q ≠ 0 ∧ q ≠ p ∧ p*q=q ∧ q*p=q)
(hsep : TopologicalSpace.IsSeparable (Set.range (baseVector τ))) :
∃ a ∈ M,∃ b ∈ M,∃ c ∈ M,∃ d ∈ M,
IsSelfAdjoint a ∧ IsSelfAdjoint b ∧ IsSelfAdjoint c ∧ IsSelfAdjoint d ∧
wstar {a,b,c,d}=M.toStarSubalgebra := by
obtain ⟨P,hPM,hP,hscalar,a,ha,b,hb,hsa,hsb,hPgen⟩ :=
exists_irreducible_two_generated_subfactor τ le_rfl hfactor hdiff
(fun c hc => hfactor c hc) hsep
have hPfactor (c : P.toStarSubalgebra) (hc : ∀ a : P.toStarSubalgebra,a*c=c*a) :
∃ z : ℂ,c=z • (1 : P.toStarSubalgebra) := by
obtain ⟨z,hz⟩ := hP.factor c hc
exact ⟨z,by simpa only [Algebra.algebraMap_eq_smul_one] using hz⟩
have hirr (c : M.toStarSubalgebra)
(hc : ∀ a : P.toStarSubalgebra,coordinateInclusion hPM a*c=c*coordinateInclusion hPM a) :
∃ z : ℂ,c=z • (1 : M.toStarSubalgebra) :=
⟨τ.trace c,hscalar c (fun a => congrArg Subtype.val (hc a))⟩
obtain ⟨C,_,hC,hgen⟩ := represented_relative_generation τ hPM hPfactor hP.diffuse hirr hsep
let : Nonempty (TraceUnitary τ) := ⟨⟨1⟩⟩
obtain ⟨u,hu⟩ := hC.nonempty
let v : H →L[ℂ] H := (u.algebra τ).val
have hv : v ∈ M.toStarSubalgebra := (u.algebra τ).property
have hvgen : wstar ((P : Set (H →L[ℂ] H)) ∪ {v})=M.toStarSubalgebra := hgen u hu
refine ⟨a,hPM ha,b,hPM hb,ℜ v,realPart_mem _ hv,ℑ v,imaginaryPart_mem _ hv,
hsa,hsb,(ℜ v).property,(ℑ v).property,le_antisymm ?_ ?_⟩
· exact wstar_le (vonNeumann_wotClosed M)
(by rintro _ (rfl | rfl | rfl | rfl)
· exact hPM ha
· exact hPM hb
· exact realPart_mem _ hv
· exact imaginaryPart_mem _ hv)
· let Q := wstar {a,b,(ℜ v : H →L[ℂ] H),(ℑ v : H →L[ℂ] H)}
have hPQ : P.toStarSubalgebra ≤ Q := by
rw [← hPgen]
exact wstar_mono (by intro x hx; simp only [Set.mem_insert_iff,Set.mem_singleton_iff] at hx ⊢; tauto)
rw [← hvgen]
apply wstar_le (wstar_closed _)
rintro x (hx | rfl)
· exact hPQ hx
· apply (mem_iff_parts_mem Q v).mpr
exact ⟨subset_wstar _ (by simp),subset_wstar _ (by simp)⟩
end
/-! Single generation for the explicit faithful normalized vector-trace
representation with separable trace-vector range. -/
open UltrapowerBridge
variable {H : Type*} [NormedAddCommGroup H] [InnerProductSpace ℂ H] [CompleteSpace H]
variable {M : VonNeumannAlgebra H}
theorem represented_two_selfAdjoint_generators (τ : TracialRepresentation M)
(hfactor : ∀ c : M.toStarSubalgebra,
(∀ a : M.toStarSubalgebra,a*c=c*a) → ∃ z : ℂ,c=z • (1 : M.toStarSubalgebra))
(hdiff : ∀ p : M.toStarSubalgebra,IsStarProjection p → p ≠ 0 →
∃ q : M.toStarSubalgebra,IsStarProjection q ∧ q ≠ 0 ∧ q ≠ p ∧ p*q=q ∧ q*p=q)
(hsep : TopologicalSpace.IsSeparable (Set.range (baseVector τ))) :
∃ a ∈ M,∃ b ∈ M,IsSelfAdjoint a ∧ IsSelfAdjoint b ∧ wstar {a,b}=M.toStarSubalgebra := by
obtain ⟨E,_,_,_,_,_⟩ := exists_commuting_matrix_extension τ
(FiniteMatrixStage.scalarStage M).units ⟨0,(FiniteMatrixStage.scalarStage M).positive⟩ hfactor hdiff 2 (by norm_num)
let N := E.relativeVonNeumann
let τN := restrictedTrace τ E.relativeVonNeumann_le
have hsepN : TopologicalSpace.IsSeparable (Set.range (baseVector τN)) := by
apply hsep.mono
rintro y ⟨a,rfl⟩
exact ⟨coordinateInclusion E.relativeVonNeumann_le a,rfl⟩
obtain ⟨a,ha,b,hb,c,hc,d,hd,hsa,hsb,hsc,hsd,hgen⟩ := represented_four_selfAdjoint_generators
τN (E.relative_scalar_center 0 hfactor) (E.relative_diffuse 0 hdiff) hsepN
let a' : E.commutant := E.relativeEquiv.symm ⟨a,ha⟩
let b' : E.commutant := E.relativeEquiv.symm ⟨b,hb⟩
let c' : E.commutant := E.relativeEquiv.symm ⟨c,hc⟩
let d' : E.commutant := E.relativeEquiv.symm ⟨d,hd⟩
have hs (x : H →L[ℂ] H) (hx : x ∈ N) (h : IsSelfAdjoint x) :
IsSelfAdjoint (E.relativeEquiv.symm ⟨x,hx⟩) :=
(show IsSelfAdjoint (⟨x,hx⟩ : N.toStarSubalgebra) from Subtype.ext h.star_eq).map E.relativeEquiv.symm
exact E.two_generators_of_four_commutant_generators a' b' c' d'
(hs a ha hsa) (hs b hb hsb) (hs c hc hsc) (hs d hd hsd) hgen
theorem represented_single_generator (τ : TracialRepresentation M)
(hfactor : ∀ c : M.toStarSubalgebra,
(∀ a : M.toStarSubalgebra,a*c=c*a) → ∃ z : ℂ,c=z • (1 : M.toStarSubalgebra))
(hdiff : ∀ p : M.toStarSubalgebra,IsStarProjection p → p ≠ 0 →
∃ q : M.toStarSubalgebra,IsStarProjection q ∧ q ≠ 0 ∧ q ≠ p ∧ p*q=q ∧ q*p=q)
(hsep : TopologicalSpace.IsSeparable (Set.range (baseVector τ))) :
SinglyGenerated M.toStarSubalgebra := by
obtain ⟨a,ha,b,hb,hsa,hsb,hgen⟩ := represented_two_selfAdjoint_generators τ hfactor hdiff hsep
exact ⟨a+Complex.I • b,M.add_mem ha (M.smul_mem hb _),(wstar_pack hsa hsb).trans hgen⟩
theorem singlyGenerated_of_tracialRepresentation (hM : IsII1Factor M.toStarSubalgebra)
(τ : TracialRepresentation M)
(hsep : TopologicalSpace.IsSeparable (Set.range (baseVector τ))) :
SinglyGenerated M.toStarSubalgebra := by
apply represented_single_generator τ _ hM.diffuse hsep
intro c hc
obtain ⟨z,hz⟩ := hM.factor c hc
exact ⟨z,by simpa only [Algebra.algebraMap_eq_smul_one] using hz⟩
end Generator.Tracial
end
end OAI