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namespace OAI
noncomputable section
universe u_1 u_2 u_3 u_4 u_5 u_6 u_7 u_8 u_9 u_10 u_11 u_12
universe u_13 u_14 u_15 u_16 u_17 u_18 u_19 u_20 u_21 u_22 u_23 u_24
universe u_25
namespace FreeGroupFactorMain.Amplification
namespace OperatorSum
variable {E : Type u_5} [NormedAddCommGroup E] [InnerProductSpace ℂ E] [CompleteSpace E]
abbrev Operator (E : Type u_6) [NormedAddCommGroup E] [InnerProductSpace ℂ E] := E →L[ℂ] E
def IsPartial (U : Operator E) : Prop := U*star U*U=U
theorem initial_projection {U : Operator E} (h : IsPartial U) : IsStarProjection (star U*U) := by
constructor
· change (star U*U)*(star U*U)=star U*U
calc
_ = star U*(U*star U*U) := by noncomm_ring
_ = _ := by rw [h]
· simp only [IsSelfAdjoint,star_mul,star_star]
theorem partial_star {U : Operator E} (h : IsPartial U) : IsPartial (star U) := by
have hs := congrArg star h
simpa only [IsPartial,star_mul,star_star,mul_assoc] using hs
theorem partial_norm_le {U : Operator E} (h : IsPartial U) : ‖U‖ ≤ 1 := by
have hn := (initial_projection h).norm_le (star U*U)
rw [CStarRing.norm_star_mul_self] at hn
nlinarith [norm_nonneg U]
structure OrthogonalPartials {ι : Type u_7} (U : ι → Operator E) : Prop where
isPartial : ∀ i, IsPartial (U i)
initial : Pairwise (fun i j => star (U i)*U j=0)
final : Pairwise (fun i j => U i*star (U j)=0)
theorem OrthogonalPartials.adjoint {ι : Type u_8} {U : ι → Operator E} (h : OrthogonalPartials U) :
OrthogonalPartials (fun i => star (U i)) where
isPartial i := partial_star (h.isPartial i)
initial i j hij := by simpa only [star_star] using h.final hij
final i j hij := by simpa only [star_star] using h.initial hij
theorem OrthogonalPartials.finite_offdiag {ι : Type u_9} {U : ι → Operator E}
(h : OrthogonalPartials U) (s : Finset ι) :
star (∑ i ∈ s, U i)*(∑ i ∈ s, U i) = ∑ i ∈ s, star (U i)*U i := by
classical
simp only [star_sum,Finset.sum_mul,Finset.mul_sum]
apply Finset.sum_congr rfl
intro i hi
exact Finset.sum_eq_single_of_mem i hi (fun j _ hji => h.initial hji)
theorem OrthogonalPartials.finite_partial {ι : Type u_10} {U : ι → Operator E}
(h : OrthogonalPartials U) (s : Finset ι) : IsPartial (∑ i ∈ s, U i) := by
classical
change (∑i ∈ s,U i)*star (∑i ∈ s,U i)*(∑i ∈ s,U i) = _
have hs : (∑i ∈ s,U i)*star (∑i ∈ s,U i) = ∑i ∈ s,U i*star (U i) := by
simpa only [star_sum,star_star] using h.adjoint.finite_offdiag s
rw [hs,Finset.sum_mul]
apply Finset.sum_congr rfl
intro i hi
rw [Finset.mul_sum]
rw [Finset.sum_eq_single_of_mem i hi]
· exact h.isPartial i
· intro j _ hji
rw [mul_assoc,h.initial (Ne.symm hji),mul_zero]
theorem OrthogonalPartials.ranges {ι : Type u_11} {U : ι → Operator E}
(h : OrthogonalPartials U) :
OrthogonalFamily ℂ (fun i => U i |>.toLinearMap.range)
(fun i => (U i).toLinearMap.range.subtypeₗᵢ) := by
rintro i j hij ⟨_,x,rfl⟩ ⟨_,y,rfl⟩
change inner ℂ (U i x) (U j y) = 0
rw [← ContinuousLinearMap.adjoint_inner_right]
change inner ℂ x ((star (U i)*U j) y) = 0
rw [h.initial hij,zero_apply,inner_zero_right]
theorem OrthogonalPartials.apply_summable {ι : Type u_12} {U : ι → Operator E}
(h : OrthogonalPartials U) (x : E) : Summable (fun i => U i x) := by
let f : ∀ i, (U i).toLinearMap.range := fun i => ⟨U i x,LinearMap.mem_range_self _ x⟩
apply (h.ranges.summable_iff_norm_sq_summable f).mpr
apply summable_of_sum_le (fun i => sq_nonneg ‖f i‖) (c := ‖x‖^2)
intro s
rw [← h.ranges.norm_sum f s]
have hn : ‖∑i ∈ s, U i x‖ ≤ ‖x‖ := by
have hb := (∑i ∈ s, U i).le_opNorm x
have ho := partial_norm_le (h.finite_partial s)
calc
_ = ‖(∑i ∈ s,U i) x‖ := by simp only [sum_apply]
_ ≤ ‖∑i ∈ s,U i‖*‖x‖ := hb
_ ≤ 1*‖x‖ := mul_le_mul_of_nonneg_right ho (norm_nonneg _)
_ = _ := one_mul _
change ‖∑i ∈ s,U i x‖^2 ≤ ‖x‖^2
simpa only [pow_two] using mul_self_le_mul_self (norm_nonneg _) hn
theorem OrthogonalPartials.tsum_bound {ι : Type u_13} {U : ι → Operator E}
(h : OrthogonalPartials U) (x : E) : ‖∑'i, U i x‖ ≤ ‖x‖ := by
apply le_of_tendsto ((h.apply_summable x).hasSum.norm)
apply Filter.Eventually.of_forall
intro s
calc
_ = ‖(∑i ∈ s,U i) x‖ := by simp only [sum_apply]
_ ≤ ‖∑i ∈ s,U i‖*‖x‖ := (∑i ∈ s,U i).le_opNorm x
_ ≤ 1*‖x‖ := mul_le_mul_of_nonneg_right (partial_norm_le (h.finite_partial s)) (norm_nonneg _)
_ = _ := one_mul _
def OrthogonalPartials.sum {ι : Type u_14} {U : ι → Operator E} (h : OrthogonalPartials U) : Operator E :=
LinearMap.mkContinuous
{ toFun := fun x => ∑'i,U i x
map_add' := fun x y => by
simp only [map_add]
exact (h.apply_summable x).tsum_add (h.apply_summable y)
map_smul' := fun c x => by
simp only [map_smul,RingHom.id_apply]
exact (h.apply_summable x).tsum_const_smul c }
1 (fun x => by
change ‖∑' i, U i x‖ ≤ 1 * ‖x‖
rw [one_mul]
exact h.tsum_bound x)
theorem OrthogonalPartials.sum_apply {ι : Type u_15} {U : ι → Operator E}
(h : OrthogonalPartials U) (x : E) : h.sum x = ∑'i,U i x := rfl
end OperatorSum
end FreeGroupFactorMain.Amplification
namespace FreeGroupFactorMain.Amplification.OperatorSum
section
variable {E : Type u_16} [NormedAddCommGroup E] [InnerProductSpace ℂ E] [CompleteSpace E]
variable {ι : Type u_17} {U : ι → Operator E}
theorem OrthogonalPartials.sum_star (h : OrthogonalPartials U) :
h.adjoint.sum = star h.sum := by
apply ContinuousLinearMap.ext
intro x
apply ext_inner_left ℂ
intro y
rw [ContinuousLinearMap.star_eq_adjoint,ContinuousLinearMap.adjoint_inner_right]
rw [h.adjoint.sum_apply,h.sum_apply]
change (innerSL ℂ y) (∑' i, star (U i) x) = ((innerSL ℂ).flip x) (∑' i, U i y)
rw [(innerSL ℂ y).map_tsum (h.adjoint.apply_summable x)]
have hr := ((innerSL ℂ).flip x).map_tsum (h.apply_summable y)
rw [hr]
apply tsum_congr
intro i
exact ContinuousLinearMap.adjoint_inner_right (U i) y x
theorem OrthogonalPartials.star_single_mul_sum (h : OrthogonalPartials U) (i : ι) :
star (U i)*h.sum = star (U i)*U i := by
classical
apply ContinuousLinearMap.ext
intro x
rw [mul_apply_eq_comp,h.sum_apply,(star (U i)).map_tsum (h.apply_summable x)]
rw [tsum_eq_single i]
· rfl
· intro j hji
change (star (U i)*U j) x = 0
rw [h.initial hji.symm,zero_apply]
theorem OrthogonalPartials.star_sum_mul_single (h : OrthogonalPartials U) (i : ι) :
star h.sum*U i = star (U i)*U i := by
have he := congrArg star (h.star_single_mul_sum i)
simpa only [star_mul,star_star] using he
theorem OrthogonalPartials.sum_mul_star_single (h : OrthogonalPartials U) (i : ι) :
h.sum*star (U i) = U i*star (U i) := by
have he := h.adjoint.star_sum_mul_single i
simpa only [h.sum_star,star_star] using he
theorem OrthogonalPartials.sum_partial (h : OrthogonalPartials U) : IsPartial h.sum := by
apply ContinuousLinearMap.ext
intro x
change (h.sum*star h.sum) (h.sum x) = h.sum x
rw [h.sum_apply,(h.sum*star h.sum).map_tsum (h.apply_summable x)]
apply tsum_congr
intro i
change (h.sum*star h.sum*U i) x = U i x
rw [mul_assoc,h.star_sum_mul_single,← mul_assoc,h.sum_mul_star_single,h.isPartial]
theorem OrthogonalPartials.sum_mem_centralizer (h : OrthogonalPartials U)
(s : Set (Operator E)) (hU : ∀ i, U i ∈ StarSubalgebra.centralizer ℂ s) :
h.sum ∈ StarSubalgebra.centralizer ℂ s := by
rw [StarSubalgebra.mem_centralizer_iff]
intro S hS
have hc (i) := (StarSubalgebra.mem_centralizer_iff ℂ).mp (hU i) S hS
constructor
· apply ContinuousLinearMap.ext
intro x
change S (h.sum x) = h.sum (S x)
rw [h.sum_apply,h.sum_apply,S.map_tsum (h.apply_summable x)]
apply tsum_congr
intro i
exact DFunLike.congr_fun (hc i).1 x
· apply ContinuousLinearMap.ext
intro x
change star S (h.sum x) = h.sum (star S x)
rw [h.sum_apply,h.sum_apply,(star S).map_tsum (h.apply_summable x)]
apply tsum_congr
intro i
exact DFunLike.congr_fun (hc i).2 x
theorem OrthogonalPartials.sum_left_support (h : OrthogonalPartials U)
(q : Operator E) (hq : ∀ i, q*U i=U i) : q*h.sum=h.sum := by
apply ContinuousLinearMap.ext
intro x
rw [mul_apply_eq_comp,h.sum_apply,q.map_tsum (h.apply_summable x)]
apply tsum_congr
intro i
exact DFunLike.congr_fun (hq i) x
theorem OrthogonalPartials.sum_right_support (h : OrthogonalPartials U)
(p : Operator E) (hp : ∀ i, U i*p=U i) : h.sum*p=h.sum := by
apply ContinuousLinearMap.ext
intro x
rw [mul_apply_eq_comp,h.sum_apply,h.sum_apply]
apply tsum_congr
intro i
exact DFunLike.congr_fun (hp i) x
end
variable {E : Type u_18} [NormedAddCommGroup E] [InnerProductSpace ℂ E] [CompleteSpace E]
theorem residual_projection {p e : Operator E} (hp : IsStarProjection p)
(he : IsStarProjection e) (hep : e*p=e) : IsStarProjection (p-e) := by
have hpe : p*e=e := by
have h := congrArg star hep
simpa only [star_mul,hp.isSelfAdjoint.star_eq,he.isSelfAdjoint.star_eq] using h
exact ⟨he.isIdempotentElem.sub hp.isIdempotentElem hep hpe,hp.isSelfAdjoint.sub he.isSelfAdjoint⟩
theorem OrthogonalPartials.sum_final_mul_single {ι : Type u_19} {U : ι → Operator E}
(h : OrthogonalPartials U) (i : ι) : h.sum*star h.sum*U i=U i := by
rw [mul_assoc,h.star_sum_mul_single,← mul_assoc,h.sum_mul_star_single,h.isPartial]
theorem OrthogonalPartials.single_mul_sum_initial {ι : Type u_20} {U : ι → Operator E}
(h : OrthogonalPartials U) (i : ι) : U i*star h.sum*h.sum=U i := by
have he := congrArg star (h.adjoint.sum_final_mul_single i)
simpa only [h.sum_star,star_mul,star_star,mul_assoc] using he
theorem IsPartial.initial_zero {U : Operator E} (h : star U*U=0) : U=0 := by
have hn := congrArg norm h
rw [CStarRing.norm_star_mul_self,norm_zero] at hn
exact norm_eq_zero.mp (by nlinarith [norm_nonneg U])
def PartialFamily (s : Set (Operator E)) (p q : Operator E) (F : Set (Operator E)) : Prop :=
(∀ U ∈ F, U ≠ 0 ∧ U ∈ StarSubalgebra.centralizer ℂ s ∧ IsPartial U ∧ q*U=U ∧ U*p=U) ∧
F.Pairwise (fun U V => star U*V=0 ∧ U*star V=0)
theorem maximal_partial_family (s : Set (Operator E)) (p q : Operator E) :
∃ F, Maximal (PartialFamily s p q) F := by
apply zorn_subset {F | PartialFamily s p q F}
intro c hc hchain
refine ⟨⋃₀ c,⟨?_,?_⟩,fun S hS => Set.subset_sUnion_of_mem hS⟩
· intro U hU
obtain ⟨F,hF,hUF⟩ := Set.mem_sUnion.mp hU
exact (hc hF).1 U hUF
· intro U hU V hV hne
obtain ⟨F,hF,hUF⟩ := Set.mem_sUnion.mp hU
obtain ⟨G,hG,hVG⟩ := Set.mem_sUnion.mp hV
rcases hchain.total hF hG with hFG|hGF
· exact (hc hG).2 (hFG hUF) hVG hne
· exact (hc hF).2 hUF (hGF hVG) hne
theorem PartialFamily.orthogonal {s : Set (Operator E)} {p q : Operator E}
{F : Set (Operator E)} (h : PartialFamily s p q F) :
OrthogonalPartials (fun U : F => (U : Operator E)) where
isPartial U := (h.1 U U.property).2.2.1
initial := by
intro U V hne
exact (h.2 U.property V.property (fun he => hne (Subtype.ext he))).1
final := by
intro U V hne
exact (h.2 U.property V.property (fun he => hne (Subtype.ext he))).2
theorem commutant_maximal_partial (s : Set (Operator E)) (p q : Operator E)
(hp : IsStarProjection p) (hq : IsStarProjection q)
(hpm : p ∈ StarSubalgebra.centralizer ℂ s) (hqm : q ∈ StarSubalgebra.centralizer ℂ s) :
∃ V ∈ StarSubalgebra.centralizer ℂ s, IsPartial V ∧ q*V=V ∧ V*p=V ∧
∀ T ∈ StarSubalgebra.centralizer ℂ s, (q-V*star V)*T*(p-star V*V)=0 := by
classical
obtain ⟨F,hF⟩ := maximal_partial_family s p q
let h := hF.1.orthogonal
let V := h.sum
have hV : V ∈ StarSubalgebra.centralizer ℂ s :=
h.sum_mem_centralizer s (fun U => (hF.1.1 U U.property).2.1)
have hVp : V*p=V := h.sum_right_support p (fun U => (hF.1.1 U U.property).2.2.2.2)
have hqV : q*V=V := h.sum_left_support q (fun U => (hF.1.1 U U.property).2.2.2.1)
refine ⟨V,hV,h.sum_partial,hqV,hVp,?_⟩
intro T hT
let pr := p-star V*V
let qr := q-V*star V
have hpr : IsStarProjection pr := residual_projection hp (initial_projection h.sum_partial) (by rw [mul_assoc,hVp])
have hqr : IsStarProjection qr := residual_projection hq (by simpa only [star_star] using initial_projection (partial_star h.sum_partial)) (by
have he := congrArg star hqV
simp only [star_mul,hq.isSelfAdjoint.star_eq] at he
rw [mul_assoc,he])
have hprm : pr ∈ StarSubalgebra.centralizer ℂ s := sub_mem hpm (mul_mem (star_mem hV) hV)
have hqrm : qr ∈ StarSubalgebra.centralizer ℂ s := sub_mem hqm (mul_mem hV (star_mem hV))
have hq_qr : q*qr=qr := by
dsimp [qr]
rw [mul_sub,hq.isIdempotentElem,← mul_assoc,hqV]
have hpr_p : pr*p=pr := by
dsimp [pr]
rw [sub_mul,hp.isIdempotentElem,mul_assoc,hVp]
by_contra hne
let W := Polar.partialIsometry (qr*T*pr)
have hWne : W ≠ 0 := Polar.partialIsometry_nonzero hne
have hWm : W ∈ StarSubalgebra.centralizer ℂ s :=
Polar.partialIsometry_mem_centralizer s (mul_mem (mul_mem hqrm hT) hprm)
have hWp : W*pr=W := Polar.partialIsometry_right_support hpr.isSelfAdjoint (by rw [mul_assoc,hpr.isIdempotentElem])
have hqW : qr*W=W := Polar.partialIsometry_left_support (by rw [← mul_assoc,← mul_assoc,hqr.isIdempotentElem])
have hWpartial : IsPartial W := Polar.partialIsometry_partial _
have hWp' : W*p=W := by rw [← hWp,mul_assoc,hpr_p]
have hqW' : q*W=W := by rw [← hqW,← mul_assoc,hq_qr]
have hqrU (U : F) : qr*U=0 := by
change (q-V*star V)*(U : Operator E)=0
rw [sub_mul,(hF.1.1 U U.property).2.2.2.1,h.sum_final_mul_single]
exact sub_self _
have hUpr (U : F) : (U : Operator E)*pr=0 := by
change (U : Operator E)*(p-star V*V)=0
rw [mul_sub,(hF.1.1 U U.property).2.2.2.2,← mul_assoc,h.single_mul_sum_initial]
exact sub_self _
have hUW (U : F) : star (U : Operator E)*W=0 ∧ (U : Operator E)*star W=0 := by
have he := congrArg star (hqrU U)
simp only [star_mul,hqr.isSelfAdjoint.star_eq,star_zero (Operator E)] at he
have hw := congrArg star hWp
simp only [star_mul,hpr.isSelfAdjoint.star_eq] at hw
constructor
· rw [← hqW,← mul_assoc,he,zero_mul]
· rw [← hw,← mul_assoc,hUpr,zero_mul]
have hWU (U : F) : star W*(U : Operator E)=0 ∧ W*star (U : Operator E)=0 := by
constructor
· simpa only [star_mul,star_star,star_zero (Operator E)] using congrArg star (hUW U).1
· simpa only [star_mul,star_star,star_zero (Operator E)] using congrArg star (hUW U).2
have hinsert : PartialFamily s p q (insert W F) := by
constructor
· intro U hU
rcases Set.mem_insert_iff.mp hU with rfl|hU
· exact ⟨hWne,hWm,hWpartial,hqW',hWp'⟩
· exact hF.1.1 U hU
· apply hF.1.2.insert
intro U hU _
exact ⟨hWU ⟨U,hU⟩,hUW ⟨U,hU⟩⟩
have hWF : W ∈ F := hF.2 hinsert (Set.subset_insert _ _) (Set.mem_insert _ _)
exact hWne (IsPartial.initial_zero (hUW ⟨W,hWF⟩).1)
end FreeGroupFactorMain.Amplification.OperatorSum
namespace FreeGroupFactorMain.Amplification.Polar
variable {E : Type u_21} [NormedAddCommGroup E] [InnerProductSpace ℂ E] [CompleteSpace E]
def centralSupportSpace (A : StarSubalgebra ℂ (Operator E)) (p : Operator E) : Submodule ℂ E :=
(Submodule.span ℂ {x | ∃ T ∈ A, ∃ y, x=T (p y)}).topologicalClosure
instance centralSupportSpace_complete (A : StarSubalgebra ℂ (Operator E)) (p : Operator E) :
CompleteSpace (centralSupportSpace A p) :=
(Submodule.isClosed_topologicalClosure _).isComplete.completeSpace_coe
theorem centralSupportSpace_invariant (A : StarSubalgebra ℂ (Operator E)) (p S : Operator E)
(h : ∀ T ∈ A, ∀ y, ∃ U ∈ A, ∃ z, S (T (p y))=U (p z)) :
∀ x ∈ centralSupportSpace A p, S x ∈ centralSupportSpace A p := by
let K := Submodule.span ℂ {x | ∃ T ∈ A, ∃ y, x=T (p y)}
have hi : K ∈ Module.End.invtSubmodule S := by
rw [Module.End.mem_invtSubmodule_iff_map_le,Submodule.map_le_iff_le_comap]
apply Submodule.span_le.mpr
rintro x ⟨T,hT,y,rfl⟩
change S (T (p y)) ∈ K
obtain ⟨U,hU,z,he⟩ := h T hT y
exact Submodule.subset_span ⟨U,hU,z,he⟩
exact Submodule.topologicalClosure_mem_invtSubmodule hi
theorem centralSupport_commutes (A : StarSubalgebra ℂ (Operator E)) (p S : Operator E)
(hS : S ∈ A) : Commute (centralSupportSpace A p).starProjection S := by
apply starProjection_commute
· apply centralSupportSpace_invariant
intro T hT y
exact ⟨S*T,mul_mem hS hT,y,rfl⟩
· apply centralSupportSpace_invariant
intro T hT y
exact ⟨star S*T,mul_mem (star_mem hS) hT,y,rfl⟩
theorem centralSupport_mem_centralizer (s : Set (Operator E)) (p : Operator E)
(hp : p ∈ StarSubalgebra.centralizer ℂ s) :
(centralSupportSpace (StarSubalgebra.centralizer ℂ s) p).starProjection ∈
StarSubalgebra.centralizer ℂ s := by
rw [StarSubalgebra.mem_centralizer_iff]
intro S hS
have hinv (S' : Operator E) (he : ∀ T ∈ StarSubalgebra.centralizer ℂ s, S'*T=T*S') :
∀ x ∈ centralSupportSpace (StarSubalgebra.centralizer ℂ s) p,
S' x ∈ centralSupportSpace (StarSubalgebra.centralizer ℂ s) p := by
apply centralSupportSpace_invariant
intro T hT y
refine ⟨T,hT,S' y,?_⟩
change (S'*T*p) y=(T*p*S') y
rw [he T hT,mul_assoc,he p hp,← mul_assoc]
have h₁ : ∀ T ∈ StarSubalgebra.centralizer ℂ s, S*T=T*S :=
fun T hT => ((StarSubalgebra.mem_centralizer_iff ℂ).mp hT S hS).1
have h₂ : ∀ T ∈ StarSubalgebra.centralizer ℂ s, star S*T=T*star S :=
fun T hT => ((StarSubalgebra.mem_centralizer_iff ℂ).mp hT S hS).2
have hc := starProjection_commute _ S (hinv S h₁) (hinv (star S) h₂)
have hcs := starProjection_commute _ (star S) (hinv (star S) h₂) (by simpa only [star_star] using hinv S h₁)
exact ⟨hc.eq.symm,hcs.eq.symm⟩
theorem centralSupport_fixes (A : StarSubalgebra ℂ (Operator E)) (p : Operator E) :
(centralSupportSpace A p).starProjection*p=p := by
apply ContinuousLinearMap.ext
intro x
apply Submodule.starProjection_eq_self_iff.mpr
apply Submodule.le_topologicalClosure
exact Submodule.subset_span ⟨1,one_mem A,x,by simp⟩
theorem centralSupport_annihilated (A : StarSubalgebra ℂ (Operator E)) (p q : Operator E)
(h : ∀ T ∈ A, q*T*p=0) : q*(centralSupportSpace A p).starProjection=0 := by
have hK : centralSupportSpace A p ≤ q.ker := by
apply Submodule.topologicalClosure_minimal
· apply Submodule.span_le.mpr
rintro x ⟨T,hT,y,rfl⟩
change (q*T*p) y=0
rw [h T hT,zero_apply]
· exact q.isClosed_ker
apply ContinuousLinearMap.ext
intro x
exact hK (Submodule.starProjection_apply_mem _ x)
theorem cross_corner_nonzero (s : Set (Operator E))
(hfactor : ∀ P ∈ StarSubalgebra.centralizer ℂ s, IsStarProjection P →
(∀ S ∈ StarSubalgebra.centralizer ℂ s, Commute P S) → P=0 ∨ P=1)
(p q : Operator E) (hp : p ∈ StarSubalgebra.centralizer ℂ s) (hpne : p ≠ 0) (hqne : q ≠ 0) :
∃ T ∈ StarSubalgebra.centralizer ℂ s, q*T*p ≠ 0 := by
by_contra! h
let A := StarSubalgebra.centralizer ℂ s
let P := (centralSupportSpace A p).starProjection
have hm : P ∈ A := centralSupport_mem_centralizer s p hp
have hf : P*p=p := centralSupport_fixes A p
rcases hfactor P hm isStarProjection_starProjection (fun S hS => centralSupport_commutes A p S hS) with hP|hP
· apply hpne
rw [hP,zero_mul] at hf
exact hf.symm
· apply hqne
have hh := centralSupport_annihilated A p q h
change q*P=0 at hh
simpa only [hP,mul_one] using hh
end FreeGroupFactorMain.Amplification.Polar
namespace FreeGroupFactorMain.Amplification.OperatorSum
variable {E : Type u_22} [NormedAddCommGroup E] [InnerProductSpace ℂ E] [CompleteSpace E]
theorem factor_partial_comparison (s : Set (Operator E))
(hfactor : ∀ P ∈ StarSubalgebra.centralizer ℂ s, IsStarProjection P →
(∀ S ∈ StarSubalgebra.centralizer ℂ s, Commute P S) → P=0 ∨ P=1)
(p q : Operator E) (hp : IsStarProjection p) (hq : IsStarProjection q)
(hpm : p ∈ StarSubalgebra.centralizer ℂ s) (hqm : q ∈ StarSubalgebra.centralizer ℂ s) :
∃ V ∈ StarSubalgebra.centralizer ℂ s, IsPartial V ∧ q*V=V ∧ V*p=V ∧
(star V*V=p ∨ V*star V=q) := by
obtain ⟨V,hV,hpart,hqV,hVp,hcross⟩ := commutant_maximal_partial s p q hp hq hpm hqm
refine ⟨V,hV,hpart,hqV,hVp,?_⟩
by_cases h : p-star V*V=0
· exact Or.inl (sub_eq_zero.mp h).symm
· by_cases h' : q-V*star V=0
· exact Or.inr (sub_eq_zero.mp h').symm
· obtain ⟨T,hT,hne⟩ := Polar.cross_corner_nonzero s hfactor (p-star V*V) (q-V*star V)
(sub_mem hpm (mul_mem (star_mem hV) hV)) h h'
exact (hne (hcross T hT)).elim
end FreeGroupFactorMain.Amplification.OperatorSum
namespace FreeGroupFactorMain.Amplification
section
open scoped ENNReal
open OperatorSum
variable {E : Type u_23} [NormedAddCommGroup E] [InnerProductSpace ℂ E] [CompleteSpace E]
theorem projection_inner (p : E →L[ℂ] E) (hp : IsStarProjection p) (x : E) :
inner ℂ x (p x)=(‖p x‖^2 : ℂ) := by
have he := ContinuousLinearMap.adjoint_inner_right p x (p x)
rw [← ContinuousLinearMap.star_eq_adjoint,hp.isSelfAdjoint.star_eq] at he
have hh : p (p x)=p x := congrArg (fun T : E →L[ℂ] E => T x) hp.isIdempotentElem.eq
rw [hh] at he
exact he.trans (inner_self_eq_norm_sq_to_K (p x))
theorem partial_initial_norm_sq (V : E →L[ℂ] E) (hV : IsPartial V) (x : E) :
‖(star V*V) x‖^2=‖V x‖^2 := by
have he : (‖(star V*V) x‖ : ℂ)^2=(‖V x‖ : ℂ)^2 := by
rw [← projection_inner _ (initial_projection hV)]
exact (ContinuousLinearMap.adjoint_inner_right V x (V x)).trans (inner_self_eq_norm_sq_to_K (V x))
exact_mod_cast he
theorem orthogonal_projection_norm_sq (p q : E →L[ℂ] E)
(hp : IsSelfAdjoint p) (hpq : p*q=0) (x : E) :
‖(p+q) x‖^2=‖p x‖^2+‖q x‖^2 := by
change ‖p x+q x‖^2=_
rw [sq,sq,sq]
apply norm_add_sq_eq_norm_sq_add_norm_sq_of_inner_eq_zero (𝕜 := ℂ)
have he := ContinuousLinearMap.adjoint_inner_right p x (q x)
rw [← ContinuousLinearMap.star_eq_adjoint,hp.star_eq] at he
have hz : p (q x)=0 := congrArg (fun T : E →L[ℂ] E => T x) hpq
rw [hz,inner_zero_right] at he
exact he.symm
variable {G : Type u_24} [Group G]
theorem stabilizedProjectionTrace_faithful (T : stabilization G)
(h : stabilizedProjectionTrace T=0) : T=0 := by
classical
have hdelta (j : ℕ) : (T : GroupOperator (ℕ × G)) (lp.single 2 (j,1) (1 : ℂ))=0 := by
have hh := (ENNReal.tsum_eq_zero.mp h) j
have hzero : ‖(T : GroupOperator (ℕ × G)) (lp.single 2 (j,1) (1 : ℂ))‖^2=0 :=
le_antisymm (ENNReal.ofReal_eq_zero.mp hh) (sq_nonneg _)
exact norm_eq_zero.mp (sq_eq_zero_iff.mp hzero)
apply Subtype.ext
apply matrixEntry_ext
intro i j
have hm := (mem_stabilization_iff_matrix _).mp T.property i j
have hz : matrixEntry (T : GroupOperator (ℕ × G)) i j (lp.single 2 (1 : G) (1 : ℂ))=0 := by
ext g
rw [matrixEntry_apply,productSingle_single,hdelta]
rfl
have he := groupVN_separating ⟨_,hm⟩ hz
calc
matrixEntry (T : GroupOperator (ℕ × G)) i j=0 := congrArg (fun A : groupVonNeumann G => (A : GroupOperator G)) he
_ = matrixEntry (0 : GroupOperator (ℕ × G)) i j := by
apply ContinuousLinearMap.ext
intro ξ
ext g
rw [matrixEntry_apply]
rfl
theorem stabilizedProjectionTrace_initial (V : stabilization G)
(hV : IsPartial (V : GroupOperator (ℕ × G))) :
stabilizedProjectionTrace (star V*V)=stabilizedProjectionTrace V := by
classical
apply tsum_congr
intro j
congr 1
exact partial_initial_norm_sq (V : GroupOperator (ℕ × G)) hV _
theorem stabilizedProjectionTrace_initial_final (V : stabilization G)
(hV : IsPartial (V : GroupOperator (ℕ × G))) :
stabilizedProjectionTrace (star V*V)=stabilizedProjectionTrace (V*star V) := by
classical
rw [stabilizedProjectionTrace_initial V hV]
have he := stabilizedProjectionTrace_initial (star V) (partial_star hV)
rw [star_star,stabilizedProjectionTrace_star] at he
exact he.symm
theorem stabilizedProjectionTrace_orthogonal_add (p q : stabilization G)
(hp : IsSelfAdjoint p) (hpq : p*q=0) :
stabilizedProjectionTrace (p+q)=stabilizedProjectionTrace p+stabilizedProjectionTrace q := by
classical
rw [stabilizedProjectionTrace,stabilizedProjectionTrace,stabilizedProjectionTrace,← ENNReal.tsum_add]
apply tsum_congr
intro j
change ENNReal.ofReal (‖((p : GroupOperator (ℕ × G))+(q : GroupOperator (ℕ × G))) (lp.single 2 (j,1) (1 : ℂ))‖^2)=_
rw [orthogonal_projection_norm_sq (p : GroupOperator (ℕ × G)) q
(show IsSelfAdjoint (p : GroupOperator (ℕ × G)) from congrArg Subtype.val hp)
(congrArg Subtype.val hpq),ENNReal.ofReal_add (sq_nonneg _) (sq_nonneg _)]
theorem finite_trace_equal_projection_of_le (p e : stabilization G)
(_hp : IsStarProjection p) (he : IsStarProjection e) (hep : e*p=e)
(htrace : stabilizedProjectionTrace p=stabilizedProjectionTrace e)
(hfinite : stabilizedProjectionTrace p ≠ ⊤) : p=e := by
have he' : e*(p-e)=0 := by rw [mul_sub,hep,he.isIdempotentElem,sub_self]
have hs := stabilizedProjectionTrace_orthogonal_add e (p-e) he.isSelfAdjoint he'
rw [add_sub_cancel,htrace] at hs
have hzero : stabilizedProjectionTrace (p-e)=0 := by
have hf : stabilizedProjectionTrace e ≠ ⊤ := htrace ▸ hfinite
exact (ENNReal.add_right_inj hf).mp (by simpa only [add_zero] using hs.symm)
exact sub_eq_zero.mp (stabilizedProjectionTrace_faithful (p-e) hzero)
end
open scoped ENNReal
open OperatorSum
theorem equal_finite_trace_equivalence {G : Type u_25} [Group G]
(hbase : ∀ T : groupVonNeumann G, (∀ S : groupVonNeumann G, Commute T S) →
∃ c : ℂ, T=c • (1 : groupVonNeumann G))
(p q : stabilization G) (hp : IsStarProjection p) (hq : IsStarProjection q)
(htrace : stabilizedProjectionTrace p=stabilizedProjectionTrace q)
(hfinite : stabilizedProjectionTrace p ≠ ⊤) :
∃ V : stabilization G, star V*V=p ∧ V*star V=q := by
have hfac := stabilization_center_projection hbase
have hp' : IsStarProjection (p : GroupOperator (ℕ × G)) := hp.map (stabilization G).subtype
have hq' : IsStarProjection (q : GroupOperator (ℕ × G)) := hq.map (stabilization G).subtype
obtain ⟨V,hV,hpart,hqV,hVp,hside⟩ := factor_partial_comparison (stabilizedRightTranslations G)
hfac p q hp' hq' p.property q.property
let U : stabilization G := ⟨V,hV⟩
have hpart' : IsPartial (U : GroupOperator (ℕ × G)) := hpart
have hi : IsStarProjection (star U*U) := by
constructor
· apply Subtype.ext
exact (initial_projection hpart).isIdempotentElem
· apply Subtype.ext
exact (initial_projection hpart).isSelfAdjoint
have hf : IsStarProjection (U*star U) := by
constructor
· apply Subtype.ext
change (V*star V)*(V*star V)=V*star V
simpa only [star_star] using (initial_projection (partial_star hpart)).isIdempotentElem.eq
· apply Subtype.ext
change star (V*star V)=V*star V
simpa only [star_star] using (initial_projection (partial_star hpart)).isSelfAdjoint.star_eq
have hitrace := stabilizedProjectionTrace_initial_final U hpart'
refine ⟨U,?_⟩
rcases hside with he|he
· have hu : star U*U=p := Subtype.ext he
have hle : (U*star U)*q=U*star U := by
apply Subtype.ext
have he' := congrArg star hqV
simp only [star_mul,hq'.isSelfAdjoint.star_eq] at he'
change (V*star V)*(q : GroupOperator (ℕ × G))=V*star V
rw [mul_assoc,he']
rw [hu] at hitrace
have ht : stabilizedProjectionTrace q=stabilizedProjectionTrace (U*star U) := htrace.symm.trans hitrace
exact ⟨hu,(finite_trace_equal_projection_of_le q (U*star U) hq hf hle ht (htrace ▸ hfinite)).symm⟩
· have hu : U*star U=q := Subtype.ext he
have hle : (star U*U)*p=star U*U := by
apply Subtype.ext
change (star V*V)*(p : GroupOperator (ℕ × G))=star V*V
rw [mul_assoc,hVp]
rw [hu] at hitrace
have ht : stabilizedProjectionTrace p=stabilizedProjectionTrace (star U*U) := htrace.trans hitrace.symm
exact ⟨(finite_trace_equal_projection_of_le p (star U*U) hp hi hle ht hfinite).symm,hu⟩
theorem infinite_equal_finite_trace_equivalence
(p q : stabilization (FreeGroup ℕ)) (hp : IsStarProjection p) (hq : IsStarProjection q)
(htrace : stabilizedProjectionTrace p=stabilizedProjectionTrace q)
(hfinite : stabilizedProjectionTrace p ≠ ⊤) :
∃ V : stabilization (FreeGroup ℕ), star V*V=p ∧ V*star V=q :=
equal_finite_trace_equivalence
(fun T hT => ⟨canonicalTrace T,infinite_free_group_center_scalar T hT⟩) p q hp hq htrace hfinite
end FreeGroupFactorMain.Amplification
end
end OAI
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