Outer tensor product of linear representations

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Definition

Suppose G1,G2 are groups and K is a field. Suppose ρ1:G1GL(V1) and ρ2:G2GL(V2) are linear representations of G1,G2 respectively over K. The outer tensor product, denoted ρ1ρ2, is a linear representation of G1×G2 on the tensor product of vector spaces V1KV2 defined in the following equivalent ways.

Direct definition in terms of tensor product of vector spaces

The outer tensor product representation is defined as follows:

(ρ1ρ2)(g1,g2)=ρ1(g1)ρ2(g2)

The on the right is the natural homomorphism:

GL(V1)×GL(V2)GL(V1V2)

Definition in terms of tensor product of linear representations

Let π1:G1×G2G1 and π2:G1×G2G2 be the projection maps onto the direct factors. Let φ1=ρ1π1 and φ2=ρ2π2. Then, both φ1 and φ2 are linear representations of G1×G2. The outer tensor product of ρ1 and ρ2 is defined as the tensor product of linear representations φ1φ2.