adjoint representation
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Let be a Lie algebra. For every we define the, a.k.a. the adjoint action,
to be the linear transformation withaction
For any vector space , we use to denote the Lie algebraof determined by the commutator bracket. So as vector spaces, only the multiplications are different.
In this notation, treating as a vector space, the linear mapping with action
is called the adjoint representation of . The fact that defines a representation is a straight-forward consequence ofthe Jacobi identity
axiom. Indeed, let be given. Wewish to show that
where the bracket on the left is the multiplication structure, and the bracket on the right is thecommutator bracket. For all the left hand side maps to
while the right hand side maps to
Taking skew-symmetry of the bracket as agiven, the equality of these two expressions is logically equivalentto the Jacobi identity: