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3. A closed oriented manifold M of dimension n can be regarded as a bordism from the<br />

empty (n − 1)-manifold to itself, M : ∅ → ∅. Thus<br />

Z(M) : K ∼ = Z(∅) → Z(∅) ∼ = K<br />

and thus Z(M) ∈ Hom K (K, K) ∼ = K is a number: an invariant assigned to every closed<br />

oriented manifold of dimension n.<br />

Observation 4.1.7.<br />

Let Z be an n-dimensional topological field theory. For any closed oriented (n − 1)-dimensional<br />

manifold M, Z(M) is a vector space. The cylinder on M gives a bordism d M : M ∐ M → ∅<br />

which is a right evaluation. Similarly, we get a right coevaluation b M : ∅ → M ∐ M.<br />

Applying the functor Z, we get a vector space Z(M) together with another vector space<br />

Z(M) that is a right dual.<br />

We need two lemmas:<br />

Lemma 4.1.8.<br />

Let V be an object in a tensor category. Let (V ∨ , d V , b V ) and (Ṽ ∨ , ˜d V , ˜b V ) be two right duals.<br />

Then V ∨ and Ṽ ∨ are canonically isomorphic: there is a unique isomorphism ϕ : V ∨ → Ṽ ∨ , such<br />

that the two diagrams<br />

V ∨ ⊗ V<br />

<br />

ϕ⊗id V<br />

<br />

Ṽ ∨ ⊗ V<br />

V ⊗ V ∨<br />

<br />

id V ⊗ϕ<br />

V ⊗ Ṽ ∨<br />

d V<br />

˜d<br />

V<br />

I<br />

b V<br />

˜bV<br />

<br />

I<br />

<br />

commute.<br />

Proof.<br />

For simplicity, we assume that the tensor category is strict. The axioms of a duality imply that<br />

α : V ∨ id V ∨ ⊗˜b V<br />

−→<br />

V ∨ ⊗ V ⊗ Ṽ ∨ d V ⊗idṼ ∨<br />

−→<br />

Ṽ ∨<br />

and<br />

β : Ṽ ∨ id Ṽ ∨ ⊗b V<br />

−→<br />

are inverse to each other. Uniqueness is easy to see.<br />

Ṽ ∨ ⊗ V ⊗ V ∨ ˜d V ⊗id V ∨<br />

−→<br />

V ∨<br />

✷<br />

Lemma 4.1.9.<br />

A K-vector space V has a right dual, if and only if it is finite-dimensional.<br />

Proof.<br />

Consider the element<br />

b V (1) =<br />

N∑<br />

b i ⊗ β i with b i ∈ V and β i ∈ V ∗<br />

i=1<br />

which is necessarily a finite linear combination. Then by the axioms of a duality<br />

v = (id V ⊗ d V )(b V (1) ⊗ id V )(v) =<br />

N∑<br />

b i β i (v) .<br />

i=1<br />

86

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