Symmetric and alternating-squares of linear representation
This article gives a basic definition in the following area: linear representation theory
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Definition
Let be a linear representation of a group . Then we can define the linear representations and , the symmetric and alternating-squares of respectively, by restricting the representation of to the eigenspaces corresponding to the symmetric and alternating-squares of a vector space respectively, that is,
for , for .
Facts
- Even if is irreducible, , need not be irreducible. See the example given in this article.
Characters of the symmetric and alternating-squares
For a representation , write for its character.
Then
, and
.
Example
Dihedral group of order 8
Further information: linear representation theory of dihedral group:D8
Consider the dihedral group:D8 which has a two-dimensional faithful irreducible representation given by
.
(This specifies the whole representation as representations are group homomorphisms, which are specified by their action on generators of a group.)
Calculating gives a non-trivial three-dimensional representation of the group:
,
which is reducible.
Calculating gives a non-trivial one-dimensional representation of the group:
.
Applications
Character tables
When calculating the character table of a group, if some irreducible representations are unknown, we may find a (not necessarily irreducible) representation by taking the symmetric or alternating squares of found representations. Even if this is not irreducible, it can be decomposed into a direct sum of irreducible subrepresentations, some of which may be new, allowing for more rows in the character table to be filled.
An example of when this occurs is with the symmetric group:S4. A "natural/human" way to start is by writing down the trivial, sign and standard representations. The rest can be derived by tensor products and calculating alternating-squares. See linear representation theory of symmetric group:S4, Determination of character table of symmetric group:S4