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and trivial coaction<br />

K → A ⊗ K<br />

λ ↦→ 1 A ⊗ λ<br />

is trivially a Yetter-Drinfeld module and is a tensor unit for the tensor product.<br />

Proposition 4.5.3.<br />

Let A be a bialgebra. Then the category of Yetter-Drinfeld modules has a natural structure of<br />

a tensor category.<br />

Proof.<br />

Let V, W be Yetter-Drinfeld modules. We only have to show that the vector space V ⊗ W<br />

with action and coaction defined above obeys the Yetter-Drinfeld condition. This is done<br />

graphically.<br />

✷<br />

Proposition 4.5.4.<br />

Let H be a Hopf algebra. Then the category of Yetter-Drinfeld modules has a natural structure<br />

of a braided tensor category with the braiding of two Yetter-Drinfeld modules V, W ∈ H H YD<br />

given by<br />

c V,W : V ⊗ W → W ⊗ V<br />

v ⊗ w ↦→ v (−1) .w ⊗ v (0)<br />

Proof.<br />

The following statements are shown graphically:<br />

• The linear map c V,W is a morphism of modules and comodules and thus a morphism of<br />

Yetter-Drinfeld modules.<br />

• The morphisms c V,W obey the hexagon axioms.<br />

• Based on lemma 2.5.7, we show that the morphisms c V,W have inverses.<br />

We define as in proposition 2.5.13 the right dual action of H on V ∗ = Hom K (V, K) as<br />

the pullback along S of the transpose of the action on V and the left dual action as the<br />

pullback of the transpose along S −1 . The right dual coaction maps β ∈ V ∗ to the linear map<br />

Δ ∨ V (β) ∈ H ⊗ V ∗ ∼ = HomK (V, H)<br />

while the left dual coaction maps to<br />

Δ ∨ V (β) : V ↦→ H<br />

v ↦→ S −1 (v (−1) )β(v (0) )<br />

∨ Δ V (β) : V ↦→ H<br />

v ↦→ S(v (−1) )β(v (0) )<br />

Proposition 4.5.5.<br />

Let H be a Hopf algebra. Then the category of finite-dimensional Yetter-Drinfeld modules H H YD<br />

is rigid.<br />

✷<br />

107

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