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Hopf algebra
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==Representation theory== {{Main|Representation theory of Hopf algebras}} Let ''A'' be a Hopf algebra, and let ''M'' and ''N'' be ''A''-modules. Then, ''M'' β ''N'' is also an ''A''-module, with :<math>a(m\otimes n):=\Delta(a)(m \otimes n)=(a_1\otimes a_2)(m\otimes n)=(a_1 m \otimes a_2 n)</math> for ''m'' β ''M'', ''n'' β ''N'' and Ξ(''a'') = (''a''<sub>1</sub>, ''a''<sub>2</sub>). Furthermore, we can define the trivial representation as the base field ''K'' with :<math>a(m):=\epsilon(a)m</math> for ''m'' β ''K''. Finally, the dual representation of ''A'' can be defined: if ''M'' is an ''A''-module and ''M*'' is its dual space, then :<math>(af)(m):=f(S(a)m)</math> where ''f'' β ''M*'' and ''m'' β ''M''. The relationship between Ξ, Ξ΅, and ''S'' ensure that certain natural homomorphisms of vector spaces are indeed homomorphisms of ''A''-modules. For instance, the natural isomorphisms of vector spaces ''M'' β ''M'' β ''K'' and ''M'' β ''K'' β ''M'' are also isomorphisms of ''A''-modules. Also, the map of vector spaces ''M*'' β ''M'' β ''K'' with ''f'' β ''m'' β ''f''(''m'') is also a homomorphism of ''A''-modules. However, the map ''M'' β ''M*'' β ''K'' is not necessarily a homomorphism of ''A''-modules.
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