Symmetric and alternating-squares of linear representation: Difference between revisions
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<math>S^2 \rho(g) (v \otimes w) = \rho(g)(v) \otimes \rho(g) w</math> for <math>v \otimes w \in S^2 V</math>, <math>\Lambda^2 \rho(g) (v \otimes w) = \rho(g)(v) \otimes \rho(g) w</math> for <math>v \otimes w \in \Lambda^2 V</math>. | <math>S^2 \rho(g) (v \otimes w) = \rho(g)(v) \otimes \rho(g) w</math> for <math>v \otimes w \in S^2 V</math>, <math>\Lambda^2 \rho(g) (v \otimes w) = \rho(g)(v) \otimes \rho(g) w</math> for <math>v \otimes w \in \Lambda^2 V</math>. | ||
==Facts== | |||
* Even if <math>\rho</math> is [[irreducible representation|irreducible]], <math>S^2 \rho</math>, <math>\Lambda^2 \rho</math> need not be irreducible. See the example given in this article. | |||
==Characters of the symmetric and alternating-squares== | ==Characters of the symmetric and alternating-squares== | ||
Revision as of 19:33, 12 November 2023
This article gives a basic definition in the following area: linear representation theory
View other basic definitions in linear representation theory |View terms related to linear representation theory |View facts related to linear representation theory
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 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
.
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:
.