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Remarks 4.1.2.<br />

1. Graphically, we represent the braiding by overcrossings and its inverse by undercrossings.<br />

Overcrossings and undercrossings have to be distinguished.<br />

2. The flip map<br />

τ : V ⊗ W → W ⊗ V<br />

v ⊗ w ↦→ w ⊗ v<br />

defines a symmetric braiding on the monoidal category vect(K) of K-vector spaces. It also<br />

induces a symmetric braiding on the category K[G]-mod of K-linear representations of a<br />

group. More generally, flip maps give a symmetric braiding on the category H−mod for<br />

any cocommutative Hopf algebra. Since the universal enveloping algebra U(g) of a Lie<br />

algebra g is cocommutative, the category of K-linear representations of g is symmetric,<br />

as well.<br />

3. There are tensor categories that do not admit a braiding. For example, for G a non-abelian<br />

group, the category vect(G) of G-graded vector spaces does not admit a braiding since<br />

are not isomorphic, if gh ≠ hg.<br />

K g ⊗ K h<br />

∼ = Kgh and K h ⊗ K g<br />

∼ = Khg<br />

4. The category vect(G) admits the flip as a braiding, if the group G is abelian. In the<br />

case of G = Z 2 , objects are Z 2 -graded vector spaces V 0 ⊕ V 1 . We can introduce another<br />

symmetric braiding c: on homogeneous vector spaces, it equals the flip, except for<br />

c : V 1 ⊗ W 1 → W 1 ⊗ V 1<br />

v 1 ⊗ w 1 ↦→ −w 1 ⊗ v 1<br />

This category is called the category of super vector spaces. In particular, a tensor category<br />

can admit inequivalent braidings.<br />

5. The monoidal category of cobordisms has disjoint union as the tensor product. It admits<br />

the morphism represented by the bordism of two cylinders exchanging the order of the<br />

two tensorands M 1<br />

∐<br />

M2 → M 2<br />

∐<br />

M1 as a symmetric braiding.<br />

Remarks 4.1.3.<br />

1. As in any tensor category, we can consider algebras and coalgebras in a braided tensor<br />

category (C, ⊗, c). Now, we have the notion of a commutative associative unital algebra<br />

(A, μ, η): here the product is required to obey μ ◦ c A,A = μ. We also have the opposed<br />

algebra with multiplication μ opp := μ◦c A,A . Similarly, we have the notion of the coopposed<br />

coalgebra with coproduct Δ copp := c C,C ◦Δ, and the notion of a cocommative coassociative<br />

counital coalgebra with coproduct obeying c C,C ◦ Δ = Δ.<br />

2. Another construction that uses the braiding is the following: Suppose that we have two<br />

associative unital algebras (A, μ, η) and (A ′ , μ ′ , η ′ ) in a braided tensor category C. Then<br />

the tensor product A ⊗ A ′ can be endowed with the structure of an associative algebra<br />

with product<br />

A ⊗ A ′ ⊗ A ⊗ A ′ id A⊗c A,A ′ ⊗id A ′<br />

−→<br />

A ⊗ A ⊗ A ′ ⊗ A ′ μ⊗μ′<br />

−→ A ⊗ A ′ .<br />

A unit is then η ⊗ η ′ .<br />

Dually, also the tensor product of two counital coassociative coalgebras can be endowed<br />

with the structure of a coalgebra.<br />

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