Group algebra
The finite-support group ring R[G], called the group algebra when R is a field.
Let be a group and a commutative ring with identity. The group ring is the free -module with basis and multiplication determined by
extended -bilinearly. Thus every element has a unique expression
with only finitely many nonzero coefficients, and multiplication is
The identity is , where is the identity of . When is a field, is called the group algebra (also written ). Neither construction requires to be finite.
Representations as modules
Over a field , a (finite-dimensional) group representation on a -vector space extends uniquely to a unital -algebra homomorphism
Equivalently, giving a representation of is the same as giving a unital left -module structure on extending its scalar action. In this correspondence:
- subrepresentations are exactly -submodules,
- irreducible representations are exactly simple modules over ,
- for finite , Maschke’s theorem describes when is semisimple and its representations are completely reducible.
Integral orders
For finite , is a -order in : its basis has elements, it spans , and its multiplication has integer structure constants. For infinite , it is not a finite-rank order in this sense.
Examples
Example 1: Cyclic groups
Let . Then
via . This realizes as a commutative -algebra.
Example 2: The order-2 group
Here with . So
If , the elements
satisfy and , giving a decomposition . (This is a concrete instance of semisimplicity in characteristic not dividing .)
Example 3: and class sums
For , is -dimensional with basis . The center is spanned by sums over conjugacy classes:
Over an algebraically closed field, these class sums act as scalars in any finite-dimensional irreducible representation (compare Schur’s lemma).