Representation theory of finite symmetric groups
Symmetrizer and antisymmetrizer elements
The symmetrizer and antisymmetrizer are essential idempotents of the complex group ring
The symmetrizer
Proof
For the symmetrizer see Trivial irrep carrying ideal of the group ring. For the antisymmetrizer note
π 2 = β π , π β π π s g n β‘ ( π ) πΏ π β s g n β‘ ( π ) πΏ π = β π , π β π π s g n β‘ ( π π ) πΏ π π = π ! β π β π π s g n β‘ ( π ) πΏ π = π ! π and for any
and π β π π π β β [ π π ] Ξ ( π ) π β π = β π₯ , π¦ β π π π ( π₯ ) s g n β‘ ( π¦ ) πΏ π π₯ π¦ = β π₯ , π§ β π π π ( π₯ ) s g n β‘ ( π₯ β 1 π β 1 π₯ π§ ) πΏ π₯ π§ = s g n β‘ ( π ) β π₯ , π§ β π π π ( π₯ ) s g n β‘ ( π§ ) πΏ π₯ π§ = s g n β‘ ( π ) π β π where we used
s g n β‘ π₯ β 1 π β 1 π₯ π§ = s g n β‘ π₯ β 1 s g n β‘ π β 1 s g n β‘ π₯ s g n β‘ π§ = s g n β‘ π₯ s g n β‘ π s g n β‘ π₯ s g n β‘ π§ = ( s g n β‘ π₯ β Β± 1 ) 2 s g n β‘ π s g n β‘ π§ = s g n β‘ π s g n β‘ π§ Thus
generates the minimal ideΓ€l carrying π . The nonequivalence of these irreps may also be shown using the Equivalence of irreps on left ideals criterion: For any π π , π β β [ πΊ ] π° β π β π = π° β π = β π , π β π π s g n β‘ ( π ) πΏ π π = β π β π π s g n β‘ ( π ) β π β π π s g n β‘ ( π π ) πΏ π π = β π β π π s g n β‘ ( π ) π = 0 since there exist equal even and odd permutations.
The symmetrizer and antisymmetrizer elements fall into the more general category of Young operators, the former corresponding to the one-row diagram and the latter to the one-column diagram.