Tensor product of linear representations

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

Suppose G is a group and ρ1:GGL(V1) and ρ2:GGL(V2) are linear representations of G over a field K. The tensor product of the representations, denoted ρ1Kρ2 is a linear representation ρ1ρ2:GGL(V1V2) on the tensor product of the vector spaces V1KV2 defined in the following equivalent ways.

Definition using tensor product of linear maps

as follows: for gG, (ρ1ρ2)(g)=ρ1(g)ρ2(g). Here, ρ1(g)ρ2(g) is the image of the pair (ρ1(g),ρ2(g)) in the natural homomorphism GL(V1)GL(V2)GL(V1V2).

Conceptually, the mapping:

GL(V1)GL(V2)GL(V1V2)

is described as follows: we know that V1,V2 up to isomorphism determine V1V2 up to isomorphism. This means that any choice of automorphism of V1 along with automorphism of V2 induces an automorphism of V1V2. The mapping describes how.

Definition using outer tensor product

The tensor product ρ1ρ2 can be defined as the composite of the outer tensor product of linear representations of ρ1 and ρ2 (which gives a linear representation of G×G) with the diagonal inclusion map g(g,g), a homomorphism from G to G×G.

Definition in terms of symmetric bimonoidal category

The tensor product of linear representations over a field K can be defined as the tensor product of representations over a symmetric bimonoidal category where the category is the category of K-vector spaces, the additive operation is direct sum of vector spaces, and the multiplicative operation is tensor product of vector spaces.

Explicit definition in terms of block matrices

This definition works for finite-dimensional linear representations, though it also has infinite-dimensional analogues if we use infinitary matrices.

We use the same notation as in the previous definition, but assume further that V1=Km and V2=Kn. Then V1V2 can be identified with Kmn where the first m coordinates represent one copy of Km, the next m copies represent the next copy of Km, and so on. The explicit definition is now given as follows: for gG, first write the n×n matrix for ρ2(g). Then, replace each cell of the matrix by a n×n matrix that equals the cell value times ρ1(g). Overall, we get a mn×mn matrix.

Definition over a commutative unital ring

Suppose G is a group and ρ1:GGL(V1) and ρ2:GGL(V2) are linear representations of G over a commutative unital ring R. The tensor product of the representations, denoted ρ1Rρ2 is a linear representation ρ1ρ2:GGL(V1V2) on the tensor product of the modules V1RV2 defined as follows: for gG, (ρ1ρ2)(g)=ρ1(g)ρ2(g). Here, ρ1(g)ρ2(g) is the image of the pair (ρ1(g),ρ2(g)) in the natural homomorphism GL(V1)GL(V2)GL(V1V2).

Conceptually, the mapping:

GL(V)GL(W)GL(VW)

is described as follows: we know that V,W up to isomorphism determine VW up to isomorphism. This means that any choice of automorphism of V along with automorphism of W induces an automorphism of VW. The mapping describes how.

Note that the explicit matrix description of tensor product is available only if the modules V and W are free modules of finite rank over R.

Related notions

Facts