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UHF slicing and classification of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter) Mathematisches Institut Universit¨ at M¨ unster Workshop on C*-Algebras and Noncommutative Dynamics Sde Boker, Israel March 2013 Karen R. Strung (University of M¨ unster) UHF slicing March 14, 2013 1 / 18

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Page 1: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

UHF slicing and classification of nuclear C*-algebras

Karen R. Strung (joint work with Wilhelm Winter)

Mathematisches InstitutUniversitat Munster

Workshop on C*-Algebras andNoncommutative Dynamics

Sde Boker, IsraelMarch 2013

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 1 / 18

Page 2: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Let A be the class of separable nuclear unital simple C ∗-algebras satisfying

1 A ∈ A =⇒ A is locally recursive subhomogeneous (RSH) where theRSH algebras can be chosen so that projections can be lifted along an(F , η)-connected decomposition,

2 A ∈ A =⇒ T (A) has finitely many extreme points, each of whichinduce the same state on K0(A).

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 2 / 18

Page 3: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Let A be the class of separable nuclear unital simple C ∗-algebras satisfying

1 A ∈ A =⇒ A is locally recursive subhomogeneous (RSH) where theRSH algebras can be chosen so that projections can be lifted along an(F , η)-connected decomposition,

2 A ∈ A =⇒ T (A) has finitely many extreme points, each of whichinduce the same state on K0(A).

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 2 / 18

Page 4: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Let A be the class of separable nuclear unital simple C ∗-algebras satisfying

1 A ∈ A =⇒ A is locally recursive subhomogeneous (RSH) where theRSH algebras can be chosen so that projections can be lifted along an(F , η)-connected decomposition,

2 A ∈ A =⇒ T (A) has finitely many extreme points, each of whichinduce the same state on K0(A).

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 2 / 18

Page 5: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Theorem (S.–Winter)

Let A,B ∈ A. Then

A⊗Z ∼= B ⊗Z ⇐⇒ Ell(A⊗Z) ∼= Ell(B ⊗Z)

Corollary

Let A,B ∈ A and suppose that A and B have finite decomposition rank.Then

A ∼= B ⇐⇒ Ell(A) ∼= Ell(B)

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 3 / 18

Page 6: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Theorem (S.–Winter)

Let A,B ∈ A. Then

A⊗Z ∼= B ⊗Z ⇐⇒ Ell(A⊗Z) ∼= Ell(B ⊗Z)

Corollary

Let A,B ∈ A and suppose that A and B have finite decomposition rank.Then

A ∼= B ⇐⇒ Ell(A) ∼= Ell(B)

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 3 / 18

Page 7: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Key tools

1 Tensor with a UHF algebra to care of the lack of projections.UHF-stable classification can (often) be used to deduce Z-stableclassification (eg. Winter, Lin).

2 Tracial approximation for A⊗Q, for the universal UHF algebra Q(i.e. K0(Q) ∼= Q).

We will show that A ∈ A =⇒ A⊗Q is a tracially approximately intervalalgebra (TAI).

Then (Lin, 2009) =⇒ classification.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 4 / 18

Page 8: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Key tools

1 Tensor with a UHF algebra to care of the lack of projections.UHF-stable classification can (often) be used to deduce Z-stableclassification (eg. Winter, Lin).

2 Tracial approximation for A⊗Q, for the universal UHF algebra Q(i.e. K0(Q) ∼= Q).

We will show that A ∈ A =⇒ A⊗Q is a tracially approximately intervalalgebra (TAI).

Then (Lin, 2009) =⇒ classification.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 4 / 18

Page 9: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Key tools

1 Tensor with a UHF algebra to care of the lack of projections.UHF-stable classification can (often) be used to deduce Z-stableclassification (eg. Winter, Lin).

2 Tracial approximation for A⊗Q, for the universal UHF algebra Q(i.e. K0(Q) ∼= Q).

We will show that A ∈ A =⇒ A⊗Q is a tracially approximately intervalalgebra (TAI).

Then (Lin, 2009) =⇒ classification.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 4 / 18

Page 10: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Key tools

1 Tensor with a UHF algebra to care of the lack of projections.UHF-stable classification can (often) be used to deduce Z-stableclassification (eg. Winter, Lin).

2 Tracial approximation for A⊗Q, for the universal UHF algebra Q(i.e. K0(Q) ∼= Q).

We will show that A ∈ A =⇒ A⊗Q is a tracially approximately intervalalgebra (TAI).

Then (Lin, 2009) =⇒ classification.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 4 / 18

Page 11: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Tracial approximationA is tracially approximately S:

F ⊂ε

(1−p)A(1−p)

B

p = 1B , B ∈ S

x ∈ A then x ≈ pxp + (1− p)x(1− p)whereτ(1− p) < ε for every τ ∈ T (A)andpxp ∈ε B.

I = (⊕Kk=1C ([0, 1])⊗Mnk

)⊕ (⊕Ll=1Mnl

)

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 5 / 18

Page 12: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Tracial approximationA is tracially approximately S:

F ⊂ε

(1−p)A(1−p)

B

p = 1B , B ∈ S

x ∈ A then x ≈ pxp + (1− p)x(1− p)

whereτ(1− p) < ε for every τ ∈ T (A)andpxp ∈ε B.

I = (⊕Kk=1C ([0, 1])⊗Mnk

)⊕ (⊕Ll=1Mnl

)

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 5 / 18

Page 13: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Tracial approximationA is tracially approximately S:

F ⊂ε

(1−p)A(1−p)

B

p = 1B , B ∈ S

x ∈ A then x ≈ pxp + (1− p)x(1− p)whereτ(1− p) < ε for every τ ∈ T (A)

andpxp ∈ε B.

I = (⊕Kk=1C ([0, 1])⊗Mnk

)⊕ (⊕Ll=1Mnl

)

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 5 / 18

Page 14: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Tracial approximationA is tracially approximately S:

F ⊂ε

(1−p)A(1−p)

B

p = 1B , B ∈ S

x ∈ A then x ≈ pxp + (1− p)x(1− p)whereτ(1− p) < ε for every τ ∈ T (A)andpxp ∈ε B.

I = (⊕Kk=1C ([0, 1])⊗Mnk

)⊕ (⊕Ll=1Mnl

)

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 5 / 18

Page 15: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Tracial approximationA is tracially approximately S:

F ⊂ε

(1−p)A(1−p)

B

p = 1B , B ∈ S

x ∈ A then x ≈ pxp + (1− p)x(1− p)whereτ(1− p) < ε for every τ ∈ T (A)andpxp ∈ε B.

I = (⊕Kk=1C ([0, 1])⊗Mnk

)⊕ (⊕Ll=1Mnl

)

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 5 / 18

Page 16: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Main theorem

Theorem (S.–Winter)

Let A ∈ A. Then A⊗Q is TAI.

Recall: A is the class of separable nuclear unital simple C ∗-algebrassatisfying

1 A ∈ A =⇒ A is locally recursive subhomoeneous (RSH) where theRSH algebras can be chosen so that projections can be lifted along an(F , η)-connected decomposition,

2 A ∈ A =⇒ T (A) has finitely many extreme points, each of whichinduce the same state on K0(A).

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 6 / 18

Page 17: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Main theorem

Theorem (S.–Winter)

Let A ∈ A. Then A⊗Q is TAI.

Recall: A is the class of separable nuclear unital simple C ∗-algebrassatisfying

1 A ∈ A =⇒ A is locally recursive subhomoeneous (RSH) where theRSH algebras can be chosen so that projections can be lifted along an(F , η)-connected decomposition,

2 A ∈ A =⇒ T (A) has finitely many extreme points, each of whichinduce the same state on K0(A).

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 6 / 18

Page 18: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Recursive subhomogeneous C ∗-algebras

[Phillips 2001] B is RSH if it can be written as an iterated pullback

B =(. . .((

C0 ⊕C(0)1

C1

)⊕

C(0)2

C2

). . .)⊕

C(0)R

CR ,

whereCl = C (Xl)⊗Mnl

for some compact metrizable Xl and

C(0)l = C (Ωl)⊗Mnl

for a closed subset Ωl ⊂ Xl .

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 7 / 18

Page 19: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Recursive subhomogeneous C ∗-algebras

The l th stage Bl is given by

Bl = Bl−1 ⊕C(0)l

Cl = (b, c) ∈ Bl−1 ⊕ Cl | φ(b) = ρ(c)

whereφ : Bl−1 → C

(0)l

is a unital ∗-homomorphism, and

ρ : Cl → C(0)l

is the restriction map.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 8 / 18

Page 20: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

The decomposition is not unique, so we keep track of it:

[Bl ,Xl ,Ωl , nl , φl ]Rl=1.

We say that projections can be lifted along this decomposition if:

∀n ∈ N, ∀l = 1, . . . ,R − 1 and for every projection p ∈ Bl ⊗Mn, thereexists a projection p ∈ Bl+1 ⊗Mn lifting p.

Proposition

If dim(Xl) ≤ 1 for l = 2, . . . ,R then projections can be lifted along[Bl ,Xl ,Ωl , nl , φl ]

Rl=1.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 9 / 18

Page 21: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

The decomposition is not unique, so we keep track of it:

[Bl ,Xl ,Ωl , nl , φl ]Rl=1.

We say that projections can be lifted along this decomposition if:

∀n ∈ N, ∀l = 1, . . . ,R − 1 and for every projection p ∈ Bl ⊗Mn, thereexists a projection p ∈ Bl+1 ⊗Mn lifting p.

Proposition

If dim(Xl) ≤ 1 for l = 2, . . . ,R then projections can be lifted along[Bl ,Xl ,Ωl , nl , φl ]

Rl=1.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 9 / 18

Page 22: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

The decomposition is not unique, so we keep track of it:

[Bl ,Xl ,Ωl , nl , φl ]Rl=1.

We say that projections can be lifted along this decomposition if:

∀n ∈ N, ∀l = 1, . . . ,R − 1 and for every projection p ∈ Bl ⊗Mn, thereexists a projection p ∈ Bl+1 ⊗Mn lifting p.

Proposition

If dim(Xl) ≤ 1 for l = 2, . . . ,R then projections can be lifted along[Bl ,Xl ,Ωl , nl , φl ]

Rl=1.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 9 / 18

Page 23: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Idea of proof (A ∈ A =⇒ A TAI):

Given F ⊂⊂ A⊗Q, ε > 0, need C ∈ I with τ(1C ) bounded away from 0,∀τ ,

and 1C commutes up to ε with f ∈ F and that approximates 1C F 1C

up to ε.

Assume τ0, τ1 are the only extreme tracial states.

W.L.O.G., assume F = F0⊗1Q with F0 ⊂⊂ RSH algebra B.

Find a tracially large interval: Take a ∈ (A⊗Q)+ with τ0(a) ≈ 0 andτ(a) ≈ 1 (Brown–Toms 2007), then take C ∗(a, 1).

Must move this interval into position (w.r.t. F): model an interval inB ⊗Q, use strict comparison.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 10 / 18

Page 24: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Idea of proof (A ∈ A =⇒ A TAI):

Given F ⊂⊂ A⊗Q, ε > 0, need C ∈ I with τ(1C ) bounded away from 0,∀τ , and 1C commutes up to ε with f ∈ F

and that approximates 1C F 1C

up to ε.

Assume τ0, τ1 are the only extreme tracial states.

W.L.O.G., assume F = F0⊗1Q with F0 ⊂⊂ RSH algebra B.

Find a tracially large interval: Take a ∈ (A⊗Q)+ with τ0(a) ≈ 0 andτ(a) ≈ 1 (Brown–Toms 2007), then take C ∗(a, 1).

Must move this interval into position (w.r.t. F): model an interval inB ⊗Q, use strict comparison.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 10 / 18

Page 25: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Idea of proof (A ∈ A =⇒ A TAI):

Given F ⊂⊂ A⊗Q, ε > 0, need C ∈ I with τ(1C ) bounded away from 0,∀τ , and 1C commutes up to ε with f ∈ F and that approximates 1C F 1C

up to ε.

Assume τ0, τ1 are the only extreme tracial states.

W.L.O.G., assume F = F0⊗1Q with F0 ⊂⊂ RSH algebra B.

Find a tracially large interval: Take a ∈ (A⊗Q)+ with τ0(a) ≈ 0 andτ(a) ≈ 1 (Brown–Toms 2007), then take C ∗(a, 1).

Must move this interval into position (w.r.t. F): model an interval inB ⊗Q, use strict comparison.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 10 / 18

Page 26: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Idea of proof (A ∈ A =⇒ A TAI):

Given F ⊂⊂ A⊗Q, ε > 0, need C ∈ I with τ(1C ) bounded away from 0,∀τ , and 1C commutes up to ε with f ∈ F and that approximates 1C F 1C

up to ε.

Assume τ0, τ1 are the only extreme tracial states.

W.L.O.G., assume F = F0⊗1Q with F0 ⊂⊂ RSH algebra B.

Find a tracially large interval: Take a ∈ (A⊗Q)+ with τ0(a) ≈ 0 andτ(a) ≈ 1 (Brown–Toms 2007), then take C ∗(a, 1).

Must move this interval into position (w.r.t. F): model an interval inB ⊗Q, use strict comparison.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 10 / 18

Page 27: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Idea of proof (A ∈ A =⇒ A TAI):

Given F ⊂⊂ A⊗Q, ε > 0, need C ∈ I with τ(1C ) bounded away from 0,∀τ , and 1C commutes up to ε with f ∈ F and that approximates 1C F 1C

up to ε.

Assume τ0, τ1 are the only extreme tracial states.

W.L.O.G., assume F = F0⊗1Q with F0 ⊂⊂ RSH algebra B.

Find a tracially large interval: Take a ∈ (A⊗Q)+ with τ0(a) ≈ 0 andτ(a) ≈ 1 (Brown–Toms 2007), then take C ∗(a, 1).

Must move this interval into position (w.r.t. F): model an interval inB ⊗Q, use strict comparison.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 10 / 18

Page 28: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Idea of proof (A ∈ A =⇒ A TAI):

Given F ⊂⊂ A⊗Q, ε > 0, need C ∈ I with τ(1C ) bounded away from 0,∀τ , and 1C commutes up to ε with f ∈ F and that approximates 1C F 1C

up to ε.

Assume τ0, τ1 are the only extreme tracial states.

W.L.O.G., assume F = F0⊗1Q with F0 ⊂⊂ RSH algebra B.

Find a tracially large interval: Take a ∈ (A⊗Q)+ with τ0(a) ≈ 0 andτ(a) ≈ 1 (Brown–Toms 2007), then take C ∗(a, 1).

Must move this interval into position (w.r.t. F): model an interval inB ⊗Q, use strict comparison.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 10 / 18

Page 29: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Interval model: excisors and bridges

Definition

B unital RSH with decomposition [Bl ,Xl ,Ωl , nl , φl ], F ⊂⊂ B+1 , η > 0. An

(F , η)-excisor (E , ρ, σ, κ) consists of

1 a finite dimensional algebra E = ⊕Rl=1El ,

2 a unital ∗-homomorphism ρ = ⊕Rl=1ρl : B → ⊕R

l=1El

3 an isometric c.p. order zero map σ = ⊕Rl=1σl : ⊕R

l=1El → B ⊗Q suchthat

‖σ(1E )(b ⊗ 1Q) = σ ρ(b)‖ < η for all b ∈ F ,

4 a unital ∗-homomorphism κ : E → Q.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 11 / 18

Page 30: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Interval model: excisors and bridges

Definition

B unital RSH with decomposition [Bl ,Xl ,Ωl , nl , φl ], F ⊂⊂ B+1 , η > 0. An

(F , η)-excisor (E , ρ, σ, κ) consists of

1 a finite dimensional algebra E = ⊕Rl=1El ,

2 a unital ∗-homomorphism ρ = ⊕Rl=1ρl : B → ⊕R

l=1El

3 an isometric c.p. order zero map σ = ⊕Rl=1σl : ⊕R

l=1El → B ⊗Q suchthat

‖σ(1E )(b ⊗ 1Q) = σ ρ(b)‖ < η for all b ∈ F ,

4 a unital ∗-homomorphism κ : E → Q.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 11 / 18

Page 31: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Interval model: excisors and bridges

Definition

B unital RSH with decomposition [Bl ,Xl ,Ωl , nl , φl ], F ⊂⊂ B+1 , η > 0. An

(F , η)-excisor (E , ρ, σ, κ) consists of

1 a finite dimensional algebra E = ⊕Rl=1El ,

2 a unital ∗-homomorphism ρ = ⊕Rl=1ρl : B → ⊕R

l=1El

3 an isometric c.p. order zero map σ = ⊕Rl=1σl : ⊕R

l=1El → B ⊗Q suchthat

‖σ(1E )(b ⊗ 1Q) = σ ρ(b)‖ < η for all b ∈ F ,

4 a unital ∗-homomorphism κ : E → Q.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 11 / 18

Page 32: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Interval model: excisors and bridges

Definition

B unital RSH with decomposition [Bl ,Xl ,Ωl , nl , φl ], F ⊂⊂ B+1 , η > 0. An

(F , η)-excisor (E , ρ, σ, κ) consists of

1 a finite dimensional algebra E = ⊕Rl=1El ,

2 a unital ∗-homomorphism ρ = ⊕Rl=1ρl : B → ⊕R

l=1El

3 an isometric c.p. order zero map σ = ⊕Rl=1σl : ⊕R

l=1El → B ⊗Q

suchthat

‖σ(1E )(b ⊗ 1Q) = σ ρ(b)‖ < η for all b ∈ F ,

4 a unital ∗-homomorphism κ : E → Q.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 11 / 18

Page 33: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Interval model: excisors and bridges

Definition

B unital RSH with decomposition [Bl ,Xl ,Ωl , nl , φl ], F ⊂⊂ B+1 , η > 0. An

(F , η)-excisor (E , ρ, σ, κ) consists of

1 a finite dimensional algebra E = ⊕Rl=1El ,

2 a unital ∗-homomorphism ρ = ⊕Rl=1ρl : B → ⊕R

l=1El

3 an isometric c.p. order zero map σ = ⊕Rl=1σl : ⊕R

l=1El → B ⊗Q suchthat

‖σ(1E )(b ⊗ 1Q) = σ ρ(b)‖ < η for all b ∈ F ,

4 a unital ∗-homomorphism κ : E → Q.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 11 / 18

Page 34: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Interval model: excisors and bridges

Definition

B unital RSH with decomposition [Bl ,Xl ,Ωl , nl , φl ], F ⊂⊂ B+1 , η > 0. An

(F , η)-excisor (E , ρ, σ, κ) consists of

1 a finite dimensional algebra E = ⊕Rl=1El ,

2 a unital ∗-homomorphism ρ = ⊕Rl=1ρl : B → ⊕R

l=1El

3 an isometric c.p. order zero map σ = ⊕Rl=1σl : ⊕R

l=1El → B ⊗Q suchthat

‖σ(1E )(b ⊗ 1Q) = σ ρ(b)‖ < η for all b ∈ F ,

4 a unital ∗-homomorphism κ : E → Q.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 11 / 18

Page 35: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Interval model: excisors and bridges

We say that (E , ρ, σ, κ) is compatible with the RSH decomposition if eachρl factorizes through

B

ψl

ρl // El

Blψl // C(Xl)⊗Mrl

ρl

OO

for some compact Xl ⊂ Xl \ Ωl .

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 12 / 18

Page 36: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Interval model: excisors and bridges

Definition

An (F , η)-bridge between (E0, ρ0, σ0, κ0) and (E1, ρ1, σ1, κ1) consists ofK ∈ N and (F , η)-excisors (Ej/K , ρj/K , σj/K , κj/K ), j = 1, . . . ,K − 1satisfying

‖κj/K ρj/K (b)− κ(j+1)/K ρ(j+1)/K (b)‖ < η

for all b ∈ F and j = 0, . . . ,K − 1.

In this case, write (E0, ρ0, σ0, κ0) ∼(F ,η) (E1, ρ1, σ1, κ1).

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 13 / 18

Page 37: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Interval model: excisors and bridges

Definition

An (F , η)-bridge between (E0, ρ0, σ0, κ0) and (E1, ρ1, σ1, κ1) consists ofK ∈ N and (F , η)-excisors (Ej/K , ρj/K , σj/K , κj/K ), j = 1, . . . ,K − 1satisfying

‖κj/K ρj/K (b)− κ(j+1)/K ρ(j+1)/K (b)‖ < η

for all b ∈ F and j = 0, . . . ,K − 1.

In this case, write (E0, ρ0, σ0, κ0) ∼(F ,η) (E1, ρ1, σ1, κ1).

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 13 / 18

Page 38: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

(F , η)-connected decomposition

[Bl ,Xl ,Ωl , nl , φl ]Rl=1 the RSH decomposition.

For every l = 1, . . . ,R and every x ∈ Xl we can define an (F , η)-excisor.

The decomposition is (F , η)-connected if, for any l = 1, . . . ,R and anyx , y ∈ Xl , we can always find an (F , η)-bridge between their corresponding(F , η)-excisors.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 14 / 18

Page 39: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

(F , η)-connected decomposition

[Bl ,Xl ,Ωl , nl , φl ]Rl=1 the RSH decomposition.

For every l = 1, . . . ,R and every x ∈ Xl we can define an (F , η)-excisor.

The decomposition is (F , η)-connected if, for any l = 1, . . . ,R and anyx , y ∈ Xl , we can always find an (F , η)-bridge between their corresponding(F , η)-excisors.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 14 / 18

Page 40: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Interval model: large trace

With a suitable calculus for (F , η)-excisors, we can find (E0, ρ0, σ0, κ0) and(E1, ρ0, σ0, κ0) with τi (σ(1Ei

)) large and τi (σj(1Ej)) small, i 6= j ∈ 0, 1.

It remains to find an (F , η)-bridge through the decomposition.

To do this, we use linear algebra based on equations which we can read offthe RSH decomposition.

This is where we require that projections can be lifted and that eachtracial state induces the same state on K0.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 15 / 18

Page 41: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Interval model: large trace

With a suitable calculus for (F , η)-excisors, we can find (E0, ρ0, σ0, κ0) and(E1, ρ0, σ0, κ0) with τi (σ(1Ei

)) large and τi (σj(1Ej)) small, i 6= j ∈ 0, 1.

It remains to find an (F , η)-bridge through the decomposition.

To do this, we use linear algebra based on equations which we can read offthe RSH decomposition.

This is where we require that projections can be lifted and that eachtracial state induces the same state on K0.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 15 / 18

Page 42: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Interval model: large trace

With a suitable calculus for (F , η)-excisors, we can find (E0, ρ0, σ0, κ0) and(E1, ρ0, σ0, κ0) with τi (σ(1Ei

)) large and τi (σj(1Ej)) small, i 6= j ∈ 0, 1.

It remains to find an (F , η)-bridge through the decomposition.

To do this, we use linear algebra based on equations which we can read offthe RSH decomposition.

This is where we require that projections can be lifted and that eachtracial state induces the same state on K0.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 15 / 18

Page 43: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Interval model: large trace

With a suitable calculus for (F , η)-excisors, we can find (E0, ρ0, σ0, κ0) and(E1, ρ0, σ0, κ0) with τi (σ(1Ei

)) large and τi (σj(1Ej)) small, i 6= j ∈ 0, 1.

It remains to find an (F , η)-bridge through the decomposition.

To do this, we use linear algebra based on equations which we can read offthe RSH decomposition.

This is where we require that projections can be lifted and that eachtracial state induces the same state on K0.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 15 / 18

Page 44: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

What we get...

With two extreme tracial states τ0, τ1, we find (F , η)-excisors

(E0, ρ0, σ0, κ0) ∼(F ,η) (E1, ρ1, σ1, κ)

such that(τi ⊗ τQ)(σi (1Ei

)) ≥ 1/3.

Now use strict comparison to move the elements in a partition of unity ofthe actual interval under this model.This will be an interval which is large in trace, and the condition

‖σ(1E )(b ⊗ 1Q) = σ ρ(b)‖ < η for all b ∈ F ,

for (F , η)-excisors allows us to properly approximate elements in the finitesubset.

A⊗Q is TAI.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 16 / 18

Page 45: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

What we get...

With two extreme tracial states τ0, τ1, we find (F , η)-excisors

(E0, ρ0, σ0, κ0) ∼(F ,η) (E1, ρ1, σ1, κ)

such that(τi ⊗ τQ)(σi (1Ei

)) ≥ 1/3.

Now use strict comparison to move the elements in a partition of unity ofthe actual interval under this model.This will be an interval which is large in trace, and the condition

‖σ(1E )(b ⊗ 1Q) = σ ρ(b)‖ < η for all b ∈ F ,

for (F , η)-excisors allows us to properly approximate elements in the finitesubset.

A⊗Q is TAI.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 16 / 18

Page 46: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

What we get...

With two extreme tracial states τ0, τ1, we find (F , η)-excisors

(E0, ρ0, σ0, κ0) ∼(F ,η) (E1, ρ1, σ1, κ)

such that(τi ⊗ τQ)(σi (1Ei

)) ≥ 1/3.

Now use strict comparison to move the elements in a partition of unity ofthe actual interval under this model.

This will be an interval which is large in trace, and the condition

‖σ(1E )(b ⊗ 1Q) = σ ρ(b)‖ < η for all b ∈ F ,

for (F , η)-excisors allows us to properly approximate elements in the finitesubset.

A⊗Q is TAI.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 16 / 18

Page 47: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

What we get...

With two extreme tracial states τ0, τ1, we find (F , η)-excisors

(E0, ρ0, σ0, κ0) ∼(F ,η) (E1, ρ1, σ1, κ)

such that(τi ⊗ τQ)(σi (1Ei

)) ≥ 1/3.

Now use strict comparison to move the elements in a partition of unity ofthe actual interval under this model.This will be an interval which is large in trace, and the condition

‖σ(1E )(b ⊗ 1Q) = σ ρ(b)‖ < η for all b ∈ F ,

for (F , η)-excisors allows us to properly approximate elements in the finitesubset.

A⊗Q is TAI.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 16 / 18

Page 48: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

What we get...

With two extreme tracial states τ0, τ1, we find (F , η)-excisors

(E0, ρ0, σ0, κ0) ∼(F ,η) (E1, ρ1, σ1, κ)

such that(τi ⊗ τQ)(σi (1Ei

)) ≥ 1/3.

Now use strict comparison to move the elements in a partition of unity ofthe actual interval under this model.This will be an interval which is large in trace, and the condition

‖σ(1E )(b ⊗ 1Q) = σ ρ(b)‖ < η for all b ∈ F ,

for (F , η)-excisors allows us to properly approximate elements in the finitesubset.

A⊗Q is TAI.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 16 / 18

Page 49: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Main theorem

Theorem (S.–Winter)

Let A,B ∈ A. Then

A⊗Z ∼= B ⊗Z ⇐⇒ Ell(A⊗Z) ∼= Ell(B ⊗Z).

Where A is the class of separable nuclear unital simple C ∗-algebrassatisfying

1 A ∈ A =⇒ A is locally recursive subhomoeneous (RSH) where theRSH algebras can be chosen so that projections can be lifted along an(F , η)-connected decomposition,

2 A ∈ A =⇒ T (A) has finitely many extreme points, each of whichinduce the same state on K0(A).

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 17 / 18

Page 50: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Main theorem

Theorem (S.–Winter)

Let A,B ∈ A. Then

A⊗Z ∼= B ⊗Z ⇐⇒ Ell(A⊗Z) ∼= Ell(B ⊗Z).

Where A is the class of separable nuclear unital simple C ∗-algebrassatisfying

1 A ∈ A =⇒ A is locally recursive subhomoeneous (RSH) where theRSH algebras can be chosen so that projections can be lifted along an(F , η)-connected decomposition,

2 A ∈ A =⇒ T (A) has finitely many extreme points, each of whichinduce the same state on K0(A).

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 17 / 18

Page 51: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Some consequences

1. Elliott 1996 – Simple approximately SH algebras constructed byattaching 1-dimensional spaces to the circle. Theorem =⇒ classificationwhen restricted to finitely many extreme tracial states, each inducing sameK0-state.

2. Lin–Matui 2005 – A := C (X × T) o Z. Restricting to finitely manytraces each inducing same state on K0, theorem =⇒ Ax ⊗Q is TAI,then (S.-Winter 2010) =⇒ A⊗Q TAI =⇒ classification.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 18 / 18

Page 52: UHF slicing and classification of nuclear C*-algebrascstar/workshop/slides/strung.pdfUHF slicing and classi cation of nuclear C*-algebras Karen R. Strung (joint work with Wilhelm Winter)

Some consequences

1. Elliott 1996 – Simple approximately SH algebras constructed byattaching 1-dimensional spaces to the circle. Theorem =⇒ classificationwhen restricted to finitely many extreme tracial states, each inducing sameK0-state.

2. Lin–Matui 2005 – A := C (X × T) o Z. Restricting to finitely manytraces each inducing same state on K0, theorem =⇒ Ax ⊗Q is TAI,then (S.-Winter 2010) =⇒ A⊗Q TAI =⇒ classification.

Karen R. Strung (University of Munster) UHF slicing March 14, 2013 18 / 18