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

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<math>\rho(a) = \begin{pmatrix} 0 & -1 \\ 1 & 0 \end{pmatrix}, \rho(x) = \begin{pmatrix} 1 & 0 \\ 0 & -1 \end{pmatrix}</math>.
<math>\rho(a) = \begin{pmatrix} 0 & -1 \\ 1 & 0 \end{pmatrix}, \rho(x) = \begin{pmatrix} 1 & 0 \\ 0 & -1 \end{pmatrix}</math>.


Calculating <math>S^2 \rho</math> gives a non-trivial one-dimensional representation of the group:
Calculating <math>S^2 \rho</math> gives a non-trivial three-dimensional representation of the group:


<math>S^2 \rho(a) =  \begin{pmatrix} 0 & 0 & 1 \\
<math>S^2 \rho(a) =  \begin{pmatrix} 0 & 0 & 1 \\
  0 & -1 & 0 \\ 1 & 0 & 0 \end{pmatrix}, S^2 \rho(x) = \begin{pmatrix} 1 & 0 & 0 \\
  0 & -1 & 0 \\ 1 & 0 & 0 \end{pmatrix}, S^2 \rho(x) = \begin{pmatrix} 1 & 0 & 0 \\
  0 & -1 & 0 \\ 0 & 0 & 1\end{pmatrix}</math>.
  0 & -1 & 0 \\ 0 & 0 & 1\end{pmatrix}</math>,
 
which is reducible.


Calculating <math>\Lambda^2 \rho</math> gives a non-trivial one-dimensional representation of the group:
Calculating <math>\Lambda^2 \rho</math> gives a non-trivial one-dimensional representation of the group:


<math>\Lambda^2 \rho(a) = \begin{pmatrix} 1 \end{pmatrix}, \Lambda^2 \rho(x) = \begin{pmatrix} -1 \end{pmatrix}</math>.
<math>\Lambda^2 \rho(a) = \begin{pmatrix} 1 \end{pmatrix}, \Lambda^2 \rho(x) = \begin{pmatrix} -1 \end{pmatrix}</math>.

Revision as of 19:32, 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 S2ρ gives a non-trivial three-dimensional representation of the group:

S2ρ(a)=(001010100),S2ρ(x)=(100010001),

which is reducible.

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

Λ2ρ(a)=(1),Λ2ρ(x)=(1).