Tensor representation
Let
Weylβs construction
Let
Let
form an irreducible orthonormal basis under both
is a
is a
where
Proof of vanishing property
For
there exists some | π£ β© β π π ( πΌ ) s.t. π β πΏ π . Then | π£ β© = π | π£ πΌ π β© for π | π£ πΌ π β© = π π | π£ πΌ π β© β π π ( πΌ ) since π β π π , giving invariance. Clearly π π β πΏ π is a basis of { π π½ π | π£ πΌ π β© } π π π½ = 1 . We define a matrix representation π π ( πΌ ) by π· π π π π π π π = π π π π· π π π ( π ) with summation convention. Then
π π π π | π£ πΌ π β© = π π πΌ π· π π π ( π ) | π£ πΌ π β© = π π π | π£ πΌ π β© π· π π π ( π ) as required.
Proof
proof See 07 Tensor method for constructing irreps of GL(n) and subgroups for discussion.
Tensor representations of U ( π ) and S U ( π )
Every irrep of GLβ(β) is an irrep of U(n) and SU(n), so tensor irreps given above are also tensor irreps for these subgroups.
However, since each column of length
Properties
- Product of tensor representations
- Conjugate representations of
are given by completing every column to be of lengthS U ( π ) , and rotating the added shape 90Β°.π
Footnotes
-
In the sense that all such that all such subspaces are generated. β©