Lie algebras MOC

Tensor product of Lie algebra representations

Let 𝜋𝑖 :𝔤 𝔤𝔩(𝑉𝑖) be representations of a Lie algebra 𝔤 for 𝑖 =1,2. The tensor product 𝜋1 𝜋2 :𝔤 𝔤𝔩(𝑉1 𝑉2) is a representation defined by

(𝜋1𝜋2)(𝑥)=𝜋1(𝑥)1+1𝜋2(𝑥)

The corresponding module over a Lie algebra is denoted 𝑉1 𝕂𝑉2.

Proof of representation

Clearly each summand defines a representation, furthermore these representations commute. Thus by Sum of commuting Lie algebra representations the above defines a representation.

Properties


#state/tidy | #lang/en | #SemBr