Symmetric and alternating-squares of linear representation: Difference between revisions

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(→‎Definition: Added section on the characters of the representations.)
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<math>\chi_{\Lambda^2 \rho} = \frac{1}{2} (\chi_{\rho}(g)^2 -\chi_{\rho}(g^2))</math>.
<math>\chi_{\Lambda^2 \rho} = \frac{1}{2} (\chi_{\rho}(g)^2 -\chi_{\rho}(g^2))</math>.
==Example==
===Dihedral group of order 8===
{{further|[[linear representation theory of dihedral group:D8]]}}
Consider the [[dihedral group:D8]] <math>\langle x,a| a^4 = x^2 = e, xax^{-1} = a^{-1}\rangle</math> which has a two-dimensional faithful [[irreducible representation|irreducible]] representation given by
<math>\rho(a) = \begin{pmatrix} 0 & -1 \\ 1 & 0 \end{pmatrix}, \rho(x) = \begin{pmatrix} 1 & 0 \\ 0 & -1 \end{pmatrix}</math>.
Calculating <math>\Lambda^2 \rho</math> gives a non-trivial one-dimensional representation of the group:
<math>\rho(a) = \begin{pmatrix} 1 \end{pmatrix}, \rho(x) = \begin{pmatrix} -1 \end{pmatrix}</math>.

Revision as of 19:27, 12 November 2023

This article gives a basic definition in the following area: linear representation theory
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Definition

Let (ρ,V) be a linear representation of a group G. Then we can define the linear representations (S2ρ,S2V) and (Λ2ρ,Λ2V), the symmetric and alternating-squares of (ρ,V) respectively, by restricting the representation (ρρ,VV) of G to the eigenspaces corresponding to the symmetric and alternating-squares respectively, that is,

S2ρ(g)(vw)=ρ(g)(v)ρ(g)w for vwS2V, Λ2ρ(g)(vw)=ρ(g)(v)ρ(g)w for vwΛ2V.

Characters of the symmetric and alternating-squares

For a representation ρ, write χρ for its character.

Then

χS2ρ=12(χρ(g)2+χρ(g2)), and

χΛ2ρ=12(χρ(g)2χρ(g2)).

Example

Dihedral group of order 8

Further information: linear representation theory of dihedral group:D8

Consider the dihedral group:D8 x,a|a4=x2=e,xax1=a1 which has a two-dimensional faithful irreducible representation given by

ρ(a)=(0110),ρ(x)=(1001).

Calculating Λ2ρ gives a non-trivial one-dimensional representation of the group:

ρ(a)=(1),ρ(x)=(1).