adjoint representation
\\DeclareMathOperator\\ad
ad\\DeclareMathOperator\\EndEnd
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: