Geometric and Algebraic Topological Methods in Quantum Mechanics

10.2: Hopf Algebras

10.2 Hopf Algebras

In this Section, the relevant basics of Hopf algebras is summarized [98; 293].

Let be a complex unital algebra, i.e., a ?-ring. The tensor product of algebras is defined as that of vector spaces provided with the multiplication


Let us write the multiplication operation of the algebra as a ?-linear morphism


A coalgebra is defined as a vector space provided with the following linear morphisms:

  • a coassociative comultiplication ,

  • a counit ,

which obey the relations

(10.2.1)

As a shorthand, one writes

(10.2.2)

A comultiplication and a counit extend to tensor products pairwise, i.e.,


A bi-algebra ( , m, ?, ?) is defined as an associative algebra which is also a coalgebra so that


A Hopf algebra ( , m, ?, ?, S) is a bi-algebra endowed with a linear morphism , called the antipode, such that


It obeys the relations


where P : a ? b ? b ? a is the transposition operator. Let us note that, given a bi-algebra , there is a unique antipode, if any, such that becomes a Hopf algebra.

For the sake of brevity, we call ?, ? and S the co-operations of a Hopf algebra.

A Hopf algebra is said to be cocommutative if P ? ? = ?. If a Hopf algebra is commutative or cocommutative, then

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