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The Structure of Fusion Categories via Topological Quantum Field Theories Chris Schommer-Pries Department of Mathematics, MIT April 27 th , 2011 Joint with Christopher Douglas and Noah Snyder Chris Schommer-Pries (MIT) April 27 th , 2011 1 / 35

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Page 1: The Structure of Fusion Categories via Topological Quantum Field

The Structure of Fusion Categoriesvia Topological Quantum Field Theories

Chris Schommer-Pries

Department of Mathematics, MIT

April 27th, 2011

Joint with Christopher Douglas and Noah Snyder

Chris Schommer-Pries (MIT) April 27th, 2011 1 / 35

Page 2: The Structure of Fusion Categories via Topological Quantum Field

Duality: Adjoint Functors

D. Kan

Definition

An adjunction is a pair of functors

F : C � D : G

and a natural bijection

HomD(Fx , y) ∼= HomC (x ,Gy).

F is left adjoint to G .

Chris Schommer-Pries (MIT) April 27th, 2011 2 / 35

Page 3: The Structure of Fusion Categories via Topological Quantum Field

Equivalent Formulation

HomD(Fx ,Fx) ∼= HomC (x ,GFx) HomC (Gy ,Gy) ∼= HomD(FGy , y)

idFx 7→ (ηx : x → GFx) idGy 7→ (εy : FGy → y)

Natural transformations...

unit η : idC → GF counit ε : FG → idD

Satisfying equations...

F1∗η→ FGF

ε∗1→ F = Fid→ F

Gη∗1→ GFG

1∗ε→ G = Gid→ G

Chris Schommer-Pries (MIT) April 27th, 2011 3 / 35

Page 4: The Structure of Fusion Categories via Topological Quantum Field

Equivalent Formulation

HomD(Fx ,Fx) ∼= HomC (x ,GFx) HomC (Gy ,Gy) ∼= HomD(FGy , y)

idFx 7→ (ηx : x → GFx) idGy 7→ (εy : FGy → y)

Natural transformations...

unit η : idC → GF counit ε : FG → idD

Satisfying equations...

F1∗η→ FGF

ε∗1→ F = Fid→ F

Gη∗1→ GFG

1∗ε→ G = Gid→ G

Chris Schommer-Pries (MIT) April 27th, 2011 3 / 35

Page 5: The Structure of Fusion Categories via Topological Quantum Field

Duality in any bicategory

Definition

An adjunction is a pair of 1-morphisms

F : C � D : G

and 2-morphismsη : idC → GF ε : FG → idD

satisfying ‘Zig-Zag’ equations:

F1∗η→ FGF

ε∗1→ F = Fid→ F

Gη∗1→ GFG

1∗ε→ G = Gid→ G

Chris Schommer-Pries (MIT) April 27th, 2011 4 / 35

Page 6: The Structure of Fusion Categories via Topological Quantum Field

Higher Category Theory

Use the theory of (∞, n)-categories.

Generalizes both topological spacesand categories.

Hueristically:C. Barwick C. Rezk

Objects: a, b, c , . . . ,

1-morphisms f , g , h, . . . ,2-morphisms, 3-morphisms, etc. (invertible above n)compositions...

a b

f

g

⇓ c

f ′

g ′

h

Chris Schommer-Pries (MIT) April 27th, 2011 5 / 35

Page 7: The Structure of Fusion Categories via Topological Quantum Field

Higher Category Theory

Use the theory of (∞, n)-categories.

Generalizes both topological spacesand categories.

Hueristically:C. Barwick C. Rezk

Objects: a, b, c , . . . ,

1-morphisms f , g , h, . . . ,

2-morphisms, 3-morphisms, etc. (invertible above n)compositions...

a b

f

g

⇓ c

f ′

g ′

h

Chris Schommer-Pries (MIT) April 27th, 2011 5 / 35

Page 8: The Structure of Fusion Categories via Topological Quantum Field

Higher Category Theory

Use the theory of (∞, n)-categories.

Generalizes both topological spacesand categories.

Hueristically:C. Barwick C. Rezk

Objects: a, b, c , . . . ,1-morphisms f , g , h, . . . ,

2-morphisms, 3-morphisms, etc. (invertible above n)compositions...

a b

f

g

⇓ c

f ′

g ′

h

Chris Schommer-Pries (MIT) April 27th, 2011 5 / 35

Page 9: The Structure of Fusion Categories via Topological Quantum Field

Higher Category Theory

Use the theory of (∞, n)-categories.

Generalizes both topological spacesand categories.

Hueristically:C. Barwick C. Rezk

Objects: a, b, c , . . . ,1-morphisms f , g , h, . . . ,2-morphisms, 3-morphisms, etc. (invertible above n)compositions...

a b

f

g

c

f ′

g ′

h

Chris Schommer-Pries (MIT) April 27th, 2011 5 / 35

Page 10: The Structure of Fusion Categories via Topological Quantum Field

Higher Category Theory

Use the theory of (∞, n)-categories.

Generalizes both topological spacesand categories.

Hueristically:C. Barwick C. Rezk

Objects: a, b, c , . . . ,1-morphisms f , g , h, . . . ,2-morphisms, 3-morphisms, etc. (invertible above n)compositions...

a b

f

g

c

f ′

g ′

h

Chris Schommer-Pries (MIT) April 27th, 2011 5 / 35

Page 11: The Structure of Fusion Categories via Topological Quantum Field

Higher Category Theory

Use the theory of (∞, n)-categories.

Generalizes both topological spacesand categories.

Hueristically:C. Barwick C. Rezk

Objects: a, b, c , . . . ,1-morphisms f , g , h, . . . ,2-morphisms, 3-morphisms, etc. (invertible above n)compositions...

a b

f

g

⇓ c

f ′

g ′

h

Chris Schommer-Pries (MIT) April 27th, 2011 5 / 35

Page 12: The Structure of Fusion Categories via Topological Quantum Field

Exmaples of (∞, n)-categories

Example

Cat the 2-category of small categories.More generally, any bicategory.

Example (Spaces = (∞, 0)-categories)

X a space

objects = points of X

1-morphisms = paths in X

2-morphisms = paths between paths

etc.

Chris Schommer-Pries (MIT) April 27th, 2011 6 / 35

Page 13: The Structure of Fusion Categories via Topological Quantum Field

Duality in any bicategory

Definition

An adjunction is a pair of 1-morphisms

F : C � D : G

and 2-morphismsη : idC → GF ε : FG → idD

satisfying ‘Zig-Zag’ equations:

F1∗η→ FGF

ε∗1→ F = Fid→ F

Gη∗1→ GFG

1∗ε→ G = Gid→ G

Chris Schommer-Pries (MIT) April 27th, 2011 7 / 35

Page 14: The Structure of Fusion Categories via Topological Quantum Field

Example

Monoidal Category (M,⊗) one object bicategory BM.

1-morphisms = objects of Mcomposition given by ⊗2-morphism = morphisms of M

Dual objects in M ↔ dual 1-morphisms in BM: x , x∗, and...

coevaluation η : 1→ x ⊗ x∗ evaluation ε : x∗ ⊗ x → 1

satisfying ‘Zig-Zag’ equations.

Example

M = Vect, a vector space x is dualizable ⇔ x is finite dimensional

Chris Schommer-Pries (MIT) April 27th, 2011 8 / 35

Page 15: The Structure of Fusion Categories via Topological Quantum Field

Example

Monoidal Category (M,⊗) one object bicategory BM.

1-morphisms = objects of Mcomposition given by ⊗2-morphism = morphisms of M

Dual objects in M ↔ dual 1-morphisms in BM: x , x∗, and...

coevaluation η : 1→ x ⊗ x∗ evaluation ε : x∗ ⊗ x → 1

satisfying ‘Zig-Zag’ equations.

Example

M = Vect, a vector space x is dualizable ⇔ x is finite dimensional

Chris Schommer-Pries (MIT) April 27th, 2011 8 / 35

Page 16: The Structure of Fusion Categories via Topological Quantum Field

Example

Monoidal Category (M,⊗) one object bicategory BM.

1-morphisms = objects of Mcomposition given by ⊗2-morphism = morphisms of M

Dual objects in M ↔ dual 1-morphisms in BM: x , x∗, and...

coevaluation η : 1→ x ⊗ x∗ evaluation ε : x∗ ⊗ x → 1

satisfying ‘Zig-Zag’ equations.

Example

M = Vect, a vector space x is dualizable ⇔ x is finite dimensional

Chris Schommer-Pries (MIT) April 27th, 2011 8 / 35

Page 17: The Structure of Fusion Categories via Topological Quantum Field

Fusion Categories

Definition

A Fusion Category is a monoidal semi-simple k-linear category, with

finitely many isom. classes of simples,

End(1) ∼= k,

left and right duals for all objects.

For simplicity, k = C.Sources of Fusion Categories:

Quantum Groups

Operator Algebras

Conformal Field Theory

Representations of Loop Groups

Chris Schommer-Pries (MIT) April 27th, 2011 9 / 35

Page 18: The Structure of Fusion Categories via Topological Quantum Field

P. Etingof D. Nikshych

V. Ostrik

Theorem (Etingof-Nikshych-Ostrik)

In any Fusion category, the functor

X 7→ X ∗∗∗∗

is canonically monoidally equivalent to id.

Why?

Chris Schommer-Pries (MIT) April 27th, 2011 10 / 35

Page 19: The Structure of Fusion Categories via Topological Quantum Field

P. Etingof D. Nikshych

V. Ostrik

Theorem (Etingof-Nikshych-Ostrik)

In any Fusion category, the functor

X 7→ X ∗∗∗∗

is canonically monoidally equivalent to id.

Why?

Chris Schommer-Pries (MIT) April 27th, 2011 10 / 35

Page 20: The Structure of Fusion Categories via Topological Quantum Field

Definition

A fusion category is pivotal if it admits a pivotal structure, i.e. a naturalmonoidal isomorphism X ∼= X ∗∗.

Definition

A fusion category is spherical if it admits a pivotal structure compatiblewith canonical X ∼= X ∗∗∗∗.

Conjecture (ENO)

All fusion categories are pivotal.

Conjecture

All pivotal categories are spherical.

Still Open

Chris Schommer-Pries (MIT) April 27th, 2011 11 / 35

Page 21: The Structure of Fusion Categories via Topological Quantum Field

Definition

A fusion category is pivotal if it admits a pivotal structure, i.e. a naturalmonoidal isomorphism X ∼= X ∗∗.

Definition

A fusion category is spherical if it admits a pivotal structure compatiblewith canonical X ∼= X ∗∗∗∗.

Conjecture (ENO)

All fusion categories are pivotal.

Conjecture

All pivotal categories are spherical.

Still Open

Chris Schommer-Pries (MIT) April 27th, 2011 11 / 35

Page 22: The Structure of Fusion Categories via Topological Quantum Field

Definition

A fusion category is pivotal if it admits a pivotal structure, i.e. a naturalmonoidal isomorphism X ∼= X ∗∗.

Definition

A fusion category is spherical if it admits a pivotal structure compatiblewith canonical X ∼= X ∗∗∗∗.

Conjecture (ENO)

All fusion categories are pivotal.

Conjecture

All pivotal categories are spherical.

Still Open

Chris Schommer-Pries (MIT) April 27th, 2011 11 / 35

Page 23: The Structure of Fusion Categories via Topological Quantum Field

Chris Schommer-Pries (MIT) April 27th, 2011 12 / 35

Page 24: The Structure of Fusion Categories via Topological Quantum Field

Manifold Invariants

ZW

ZW1 ZW2

Locality of manifold invariants:

Reconstruct ZW from ZW1 and ZW2?

ZW = 〈ZW1 ,ZW2〉

Chris Schommer-Pries (MIT) April 27th, 2011 13 / 35

Page 25: The Structure of Fusion Categories via Topological Quantum Field

Manifold Invariants

ZW

ZW1 ZW2

Locality of manifold invariants:

Reconstruct ZW from ZW1 and ZW2?

ZW = 〈ZW1 ,ZW2〉

Chris Schommer-Pries (MIT) April 27th, 2011 13 / 35

Page 26: The Structure of Fusion Categories via Topological Quantum Field

Manifold Invariants

ZW

ZW1 ZW2

Locality of manifold invariants:

Reconstruct ZW from ZW1 and ZW2?

ZW = 〈ZW1 ,ZW2〉

Chris Schommer-Pries (MIT) April 27th, 2011 13 / 35

Page 27: The Structure of Fusion Categories via Topological Quantum Field

The Cobordism Category

Objects are closed compact(d − 1)-manifolds Ywith germ of d-manifold

Morphisms are compact d-manifolds W ,with ∂W = Y1 t Y2

up to equivalence.

variants:

extra structures: orientations, spin structures, etc

higher categories of cobordisms

Chris Schommer-Pries (MIT) April 27th, 2011 14 / 35

Page 28: The Structure of Fusion Categories via Topological Quantum Field

The Cobordism Category

Objects are closed compact(d − 1)-manifolds Ywith germ of d-manifold

Morphisms are compact d-manifolds W ,with ∂W = Y1 t Y2

up to equivalence.

variants:

extra structures: orientations, spin structures, etc

higher categories of cobordisms

Chris Schommer-Pries (MIT) April 27th, 2011 14 / 35

Page 29: The Structure of Fusion Categories via Topological Quantum Field

The Cobordism Category

Objects are closed compact(d − 1)-manifolds Ywith germ of d-manifold

Morphisms are compact d-manifolds W ,with ∂W = Y1 t Y2

up to equivalence.

variants:

extra structures: orientations, spin structures, etc

higher categories of cobordisms

Chris Schommer-Pries (MIT) April 27th, 2011 14 / 35

Page 30: The Structure of Fusion Categories via Topological Quantum Field

Topological Quantum Field Theories

Definition

A TQFT is a symmetricmonoidal functor:

Bord︸︷︷︸Cobordism Category

→ C︸︷︷︸Target Category

∅ ∈ Bord 7→ 1 ∈ C

M closed 7→ (1ZM→ 1)

M. Atiyah

G. Segal

Chris Schommer-Pries (MIT) April 27th, 2011 15 / 35

Page 31: The Structure of Fusion Categories via Topological Quantum Field

Topological Quantum Field Theories

Definition

A TQFT is a symmetricmonoidal functor:

Bord︸︷︷︸Cobordism Category

→ C︸︷︷︸Target Category

∅ ∈ Bord 7→ 1 ∈ C

M closed 7→ (1ZM→ 1)

M. Atiyah

G. Segal

Chris Schommer-Pries (MIT) April 27th, 2011 15 / 35

Page 32: The Structure of Fusion Categories via Topological Quantum Field

Distinguishing Manifolds?

0D, 1D, and 2D TFTs distinguish manifolds.

4D (unitary) TFTs cannot detect smooth structures.[Freedman-Kitaev-Nayak-Slingerland-Walker-Wang]

5D (unitary) TFTs can detect, if π1 = 0. [Kreck-Teichner]

≥ 6D (unitary) TFTs cannot detect homotopy type. [Kreck-Teichner]

Open Problem: Can 3D TFTs distinguish 3-manifolds?Evidence suggest “yes?”. [Calegari-Freedman-Walker]

Chris Schommer-Pries (MIT) April 27th, 2011 16 / 35

Page 33: The Structure of Fusion Categories via Topological Quantum Field

Distinguishing Manifolds?

0D, 1D, and 2D TFTs distinguish manifolds.

4D (unitary) TFTs cannot detect smooth structures.[Freedman-Kitaev-Nayak-Slingerland-Walker-Wang]

5D (unitary) TFTs can detect, if π1 = 0. [Kreck-Teichner]

≥ 6D (unitary) TFTs cannot detect homotopy type. [Kreck-Teichner]

Open Problem: Can 3D TFTs distinguish 3-manifolds?Evidence suggest “yes?”. [Calegari-Freedman-Walker]

Chris Schommer-Pries (MIT) April 27th, 2011 16 / 35

Page 34: The Structure of Fusion Categories via Topological Quantum Field

Distinguishing Manifolds?

0D, 1D, and 2D TFTs distinguish manifolds.

4D (unitary) TFTs cannot detect smooth structures.[Freedman-Kitaev-Nayak-Slingerland-Walker-Wang]

5D (unitary) TFTs can detect, if π1 = 0. [Kreck-Teichner]

≥ 6D (unitary) TFTs cannot detect homotopy type. [Kreck-Teichner]

Open Problem: Can 3D TFTs distinguish 3-manifolds?Evidence suggest “yes?”. [Calegari-Freedman-Walker]

Chris Schommer-Pries (MIT) April 27th, 2011 16 / 35

Page 35: The Structure of Fusion Categories via Topological Quantum Field

Distinguishing Manifolds?

0D, 1D, and 2D TFTs distinguish manifolds.

4D (unitary) TFTs cannot detect smooth structures.[Freedman-Kitaev-Nayak-Slingerland-Walker-Wang]

5D (unitary) TFTs can detect, if π1 = 0. [Kreck-Teichner]

≥ 6D (unitary) TFTs cannot detect homotopy type. [Kreck-Teichner]

Open Problem: Can 3D TFTs distinguish 3-manifolds?Evidence suggest “yes?”. [Calegari-Freedman-Walker]

Chris Schommer-Pries (MIT) April 27th, 2011 16 / 35

Page 36: The Structure of Fusion Categories via Topological Quantum Field

Turaev-Viro-Barrett-Westbury Construction: a 3D TQFT

Input:C a Spherical Category

triangulate your 3-manifold

Label using data from C

Weighted average over all labelings gives invariant.

In 2010...

Theorem (Turaev-Virelizier, Balsam-Kirillov)

This gives a tqft which is local down to 1-manifolds.

Chris Schommer-Pries (MIT) April 27th, 2011 17 / 35

Page 37: The Structure of Fusion Categories via Topological Quantum Field

Turaev-Viro-Barrett-Westbury Construction: a 3D TQFT

Input:C a Spherical Category

triangulate your 3-manifold

Label using data from C

Weighted average over all labelings gives invariant.

In 2010...

Theorem (Turaev-Virelizier, Balsam-Kirillov)

This gives a tqft which is local down to 1-manifolds.

Chris Schommer-Pries (MIT) April 27th, 2011 17 / 35

Page 38: The Structure of Fusion Categories via Topological Quantum Field

Theorem (Douglas-SP-Snyder)

Fusion, Pivotal, and Spherical Categories all give rise to fully localextended 3D TQFTs.

Moreover the structure of the TQFTs reflects the structure of fusioncategories.

Chris Schommer-Pries (MIT) April 27th, 2011 18 / 35

Page 39: The Structure of Fusion Categories via Topological Quantum Field

Tangential Structures on Manifolds

a manifold M has a tangent bundle τclassified by a map

G → O(n)

M BO(n)

BG

τ

G = SO(n) Orientation

G = Spin(n) (universal cover of SO(n)) Spin structure

G = 1 framing

etc

Chris Schommer-Pries (MIT) April 27th, 2011 19 / 35

Page 40: The Structure of Fusion Categories via Topological Quantum Field

Tangential Structures on Manifolds

a manifold M has a tangent bundle τclassified by a mapG → O(n)

M BO(n)

BG

τ

G = SO(n) Orientation

G = Spin(n) (universal cover of SO(n)) Spin structure

G = 1 framing

etc

Chris Schommer-Pries (MIT) April 27th, 2011 19 / 35

Page 41: The Structure of Fusion Categories via Topological Quantum Field

different sorts of fusion categories give different tqfts.

Theorem (Douglas-SP-Snyder)

G name of structure kind of category

SO(3)† Orientation Spherical

SO(2) Combing Pivotal

1 = SO(1) Framing Fusion

† This group might change slightly.

Chris Schommer-Pries (MIT) April 27th, 2011 20 / 35

Page 42: The Structure of Fusion Categories via Topological Quantum Field

2D (non-local) TQFTs

Theorem (Folklore)

The category of (non-local) oriented 2D tqfts in C is equivalent tocategory of commutative Frobenius algebras in C .

[R. Dijkgraaf, L. Abrams, S. Sawin, B. Dubrovin, Moore-Segal, . . . ]

unit multiplication comultiplication counit

Chris Schommer-Pries (MIT) April 27th, 2011 21 / 35

Page 43: The Structure of Fusion Categories via Topological Quantum Field

1D TQFTs

Theorem (1D Cobordism Hypothesis)

The category of 1D oriented tqfts in C is equivalent to the groupoid ofdualizable objects of C , denoted k(C fd)

coevaluation-

+ evaluation+

-

Zig-Zag equations:

= =

F1∗η→ FGF

ε∗1→ F = Fid→ F

Gη∗1→ GFG

1∗ε→ G = Gid→ G

Chris Schommer-Pries (MIT) April 27th, 2011 22 / 35

Page 44: The Structure of Fusion Categories via Topological Quantum Field

2D Local TQFTs

Like 1D tqfts, but with 2D bordisms too.

Objects (0-manifolds) have duals

1-morphisms (1-manifolds)also have duals

F ◦ G⇓ ε

id

id⇓ η

G ◦ F

Zig-Zag Equation: =

Chris Schommer-Pries (MIT) April 27th, 2011 23 / 35

Page 45: The Structure of Fusion Categories via Topological Quantum Field

2D Local TQFTs

Like 1D tqfts, but with 2D bordisms too.

Objects (0-manifolds) have duals

1-morphisms (1-manifolds)also have duals

F ◦ G⇓ ε

id

id⇓ η

G ◦ F

Zig-Zag Equation: =

Chris Schommer-Pries (MIT) April 27th, 2011 23 / 35

Page 46: The Structure of Fusion Categories via Topological Quantum Field

Layers of dualizability

3-Cat

monoidal3-Cat

dual 2-mor

dual 1-mordual 1-mor

dual objects

Chris Schommer-Pries (MIT) April 27th, 2011 24 / 35

Page 47: The Structure of Fusion Categories via Topological Quantum Field

Layers of dualizability

3-Cat

monoidal3-Cat

dual 2-mor

dual 1-mordual 1-mor

dual objects

Chris Schommer-Pries (MIT) April 27th, 2011 24 / 35

Page 48: The Structure of Fusion Categories via Topological Quantum Field

Layers of dualizability

3-Cat

monoidal3-Cat

dual 2-mor

dual 1-mor

dual 1-mor

dual objects

Chris Schommer-Pries (MIT) April 27th, 2011 24 / 35

Page 49: The Structure of Fusion Categories via Topological Quantum Field

Layers of dualizability

3-Cat

monoidal3-Cat

dual 2-mor

dual 1-mor

dual 1-mor

dual objects

Chris Schommer-Pries (MIT) April 27th, 2011 24 / 35

Page 50: The Structure of Fusion Categories via Topological Quantum Field

Fully-dualizable

Fully-dualizable is dualizable on all levels:

Definition

If C is a symmetric monoidal n-category, there is a filtration

C fd = C0 ⊆ C1 ⊆ · · · ⊆ Cn−1 ⊆ C

where Ci = the maximal sub-n-category where j-morphisms have bothduals if i ≤ j ≤ n − 1.

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Page 51: The Structure of Fusion Categories via Topological Quantum Field

Baez-Dolan Cobordism Hypothesis

J. Baez

J. Dolan

“Bordn is the free symmetricmonoidal n-category withduality”

Theorem (Hopkins-Lurie)

Fun(Bordfrn ,C) ' k(Cfd)

M. Hopkins

J. Lurie

Chris Schommer-Pries (MIT) April 27th, 2011 26 / 35

Page 52: The Structure of Fusion Categories via Topological Quantum Field

Theorem (Douglas-SP-Snyder)

Fusion categories are fully-dualizable objects in the symmetric monoidal3-category TC. (Tensor Categories)

Corollary

Fusion categories give rise to fully-local extended 3D tqfts.

What is TC?

Chris Schommer-Pries (MIT) April 27th, 2011 27 / 35

Page 53: The Structure of Fusion Categories via Topological Quantum Field

Theorem (Douglas-SP-Snyder)

Fusion categories are fully-dualizable objects in the symmetric monoidal3-category TC. (Tensor Categories)

Corollary

Fusion categories give rise to fully-local extended 3D tqfts.

What is TC?

Chris Schommer-Pries (MIT) April 27th, 2011 27 / 35

Page 54: The Structure of Fusion Categories via Topological Quantum Field

The 3-category of Tensor Categories

Example

Algebras, Bimodules, Bimodule maps = a (monoidal) 2-category

Definition

TC =

objects: Tensor Categories (monoidal k-linear)

1-morphisms: Bimodule Categories

2-morphisms and 3-morphisms: Bimodule Functors and BimoduleNatural Transformations

Monoidal for Deligne tensor product.

Proposition (Douglas-SP-Snyder)

TC is a symmetric monoidal (∞, 3)-category.

Chris Schommer-Pries (MIT) April 27th, 2011 28 / 35

Page 55: The Structure of Fusion Categories via Topological Quantum Field

The 3-category of Tensor Categories

Example

Algebras, Bimodules, Bimodule maps = a (monoidal) 2-category

Definition

TC =

objects: Tensor Categories (monoidal k-linear)

1-morphisms: Bimodule Categories

2-morphisms and 3-morphisms: Bimodule Functors and BimoduleNatural Transformations

Monoidal for Deligne tensor product.

Proposition (Douglas-SP-Snyder)

TC is a symmetric monoidal (∞, 3)-category.

Chris Schommer-Pries (MIT) April 27th, 2011 28 / 35

Page 56: The Structure of Fusion Categories via Topological Quantum Field

A Basic Principle

and a Theorem

If G acts on B, then G acts on Map(B,C ).

O(3) acts on Bordfr3 by change of framing.

O(3)→ Aut(k(Cfd))

Theorem (Hopkins-Lurie)

Fun(BordGn ,C) ' [k(Cfd)]hG .

Chris Schommer-Pries (MIT) April 27th, 2011 29 / 35

Page 57: The Structure of Fusion Categories via Topological Quantum Field

A Basic Principle

and a Theorem

If G acts on B, then G acts on Map(B,C ).

O(3) acts on Bordfr3 by change of framing.

O(3)→ Aut(k(Cfd))

Theorem (Hopkins-Lurie)

Fun(BordGn ,C) ' [k(Cfd)]hG .

Chris Schommer-Pries (MIT) April 27th, 2011 29 / 35

Page 58: The Structure of Fusion Categories via Topological Quantum Field

A Basic Principle and a Theorem

If G acts on B, then G acts on Map(B,C ).

O(3) acts on Bordfr3 by change of framing.

O(3)→ Aut(k(Cfd))

Theorem (Hopkins-Lurie)

Fun(BordGn ,C) ' [k(Cfd)]hG .

Chris Schommer-Pries (MIT) April 27th, 2011 29 / 35

Page 59: The Structure of Fusion Categories via Topological Quantum Field

So O(3) acts on the “space” of fusion categories.What is the action?

points in O(3) self-equivalences k(Cfd)→ k(Cfd)

paths in O(3) natural isomorphisms

paths between paths in O(3) natural 2-isomorphism

etc

Chris Schommer-Pries (MIT) April 27th, 2011 30 / 35

Page 60: The Structure of Fusion Categories via Topological Quantum Field

So O(3) acts on the “space” of fusion categories.What is the action?

points in O(3) self-equivalences k(Cfd)→ k(Cfd)

paths in O(3) natural isomorphisms

paths between paths in O(3) natural 2-isomorphism

etc

Chris Schommer-Pries (MIT) April 27th, 2011 30 / 35

Page 61: The Structure of Fusion Categories via Topological Quantum Field

So O(3) acts on the “space” of fusion categories.What is the action?

points in O(3) self-equivalences k(Cfd)→ k(Cfd)

paths in O(3) natural isomorphisms

paths between paths in O(3) natural 2-isomorphism

etc

Chris Schommer-Pries (MIT) April 27th, 2011 30 / 35

Page 62: The Structure of Fusion Categories via Topological Quantum Field

In more detail...

π0O(3) = Z/2, non-trivial element: (F ,⊗) 7→ (F ,⊗op).

π1O(3) gives the Serre automorphism (natural automorphism ofidentity functor)

in componentsSF : F → F

is an invertible F -F -bimodule category.

π2O(3) = 0

π3O(3) = Z gives the anomaly. aF ∈ C×

No other data since TC is just a 3-category.

Chris Schommer-Pries (MIT) April 27th, 2011 31 / 35

Page 63: The Structure of Fusion Categories via Topological Quantum Field

In more detail...

π0O(3) = Z/2, non-trivial element: (F ,⊗) 7→ (F ,⊗op).

π1O(3) gives the Serre automorphism (natural automorphism ofidentity functor)in components

SF : F → F

is an invertible F -F -bimodule category.

π2O(3) = 0

π3O(3) = Z gives the anomaly. aF ∈ C×

No other data since TC is just a 3-category.

Chris Schommer-Pries (MIT) April 27th, 2011 31 / 35

Page 64: The Structure of Fusion Categories via Topological Quantum Field

In more detail...

π0O(3) = Z/2, non-trivial element: (F ,⊗) 7→ (F ,⊗op).

π1O(3) gives the Serre automorphism (natural automorphism ofidentity functor)in components

SF : F → F

is an invertible F -F -bimodule category.

π2O(3) = 0

π3O(3) = Z gives the anomaly. aF ∈ C×

No other data since TC is just a 3-category.

Chris Schommer-Pries (MIT) April 27th, 2011 31 / 35

Page 65: The Structure of Fusion Categories via Topological Quantum Field

evL ev

Theorem (Douglas-SP-Snyder)

The Serre Automorphism of a fusion category F is the bimodulification of

(F ,⊗)→ (F ,⊗)

x 7→ x∗∗

π1O(3) ∼= Z/2⇒ square of the Serre is trivial!

Corollary

The bimodulification of x 7→ x∗∗∗∗ is trivial.

Chris Schommer-Pries (MIT) April 27th, 2011 32 / 35

Page 66: The Structure of Fusion Categories via Topological Quantum Field

Some 3D structure groups

1

Spin(3)

Spinc(3)

SO(2)

Orpo

SO(3)

O(3)

[framing]

[combing]

[Atiyah 2-framing]

kill w1

kill p1kill βw2

kill w2

fusion

pivotal

spherical

if ourTQFTagrees withTuraev-Viro

Conjecture:anomalyvanishes

Chris Schommer-Pries (MIT) April 27th, 2011 33 / 35

Page 67: The Structure of Fusion Categories via Topological Quantum Field

Some 3D structure groups

1

Spin(3)

Spinc(3)

SO(2)

Orpo

SO(3)

O(3)

[framing]

[combing]

[Atiyah 2-framing]

kill w1

kill p1kill βw2

kill w2

fusion

pivotal

spherical

if ourTQFTagrees withTuraev-Viro

Conjecture:anomalyvanishes

Chris Schommer-Pries (MIT) April 27th, 2011 33 / 35

Page 68: The Structure of Fusion Categories via Topological Quantum Field

Some 3D structure groups

1

Spin(3)

Spinc(3)

SO(2)

Orpo

SO(3)

O(3)

[framing]

[combing]

[Atiyah 2-framing]

kill w1

kill p1kill βw2

kill w2

fusion

pivotal

spherical

if ourTQFTagrees withTuraev-Viro

Conjecture:anomalyvanishes

Chris Schommer-Pries (MIT) April 27th, 2011 33 / 35

Page 69: The Structure of Fusion Categories via Topological Quantum Field

Some 3D structure groups

1

Spin(3)

Spinc(3)

SO(2)

Orpo

SO(3)

O(3)

[framing]

[combing]

[Atiyah 2-framing]

kill w1

kill p1kill βw2

kill w2

fusion

pivotal

spherical

if ourTQFTagrees withTuraev-Viro

Conjecture:anomalyvanishes

Chris Schommer-Pries (MIT) April 27th, 2011 33 / 35

Page 70: The Structure of Fusion Categories via Topological Quantum Field

A new version of ENO conjecture

Conjecture

All framed extended 3D tqfts in TC can be extended to oriented tqfts.

Evidence one dimension lower...

Theorem

All framed extended 2D tqfts in Alg can be extended to oriented tqfts.

Chris Schommer-Pries (MIT) April 27th, 2011 34 / 35

Page 71: The Structure of Fusion Categories via Topological Quantum Field

The End

Chris Schommer-Pries (MIT) April 27th, 2011 35 / 35