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