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>. | ||
==Characters of the symmetric and alternating-squares== | |||
For a representation <math>\rho</math>, write <math>\chi_{\rho}</math> for its [[character of a representation|character]]. | |||
Then | |||
<math>\chi_{S^2 \rho} = \frac{1}{2} (\chi_{\rho}(g)^2 + \chi_{\rho}(g^2))</math>, and | |||
<math>\chi_{\Lambda^2 \rho} = \frac{1}{2} (\chi_{\rho}(g)^2 -\chi_{\rho}(g^2))</math>. | |||
Revision as of 19:20, 12 November 2023
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 respectively, that is,
for , for .
Characters of the symmetric and alternating-squares
For a representation , write for its character.
Then
, and
.