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

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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.
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.
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]].

Revision as of 10:48, 18 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 (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 of a vector space 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.

Facts

  • Even if ρ is irreducible, S2ρ, Λ2ρ need not be irreducible. See the example given in this article.

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).

(This specifies the whole representation as representations are group homomorphisms, which are specified by their action on generators of a group.)

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).

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.