Geometric and Algebraic Topological Methods in Quantum Mechanics

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