adjoint representation


\DeclareMathOperator\ad

ad \DeclareMathOperator\EndEnd

Let \mathfrak⁢g be a Lie algebraMathworldPlanetmath. For every a∈\mathfrak⁢g we define the , a.k.a. the adjoint action,

\ad⁢(a):\mathfrak⁢g→\mathfrak⁢g

to be the linear transformation with action

\ad⁢(a):b↦[a,b],b∈\mathfrak⁢g.

For any vector spaceMathworldPlanetmath V, we use \mathfrak⁢g⁢l⁢(V) to denote the Lie algebra of \End⁢V determined by the commutator bracket. So \mathfrak⁢g⁢l⁢(V)=\End⁢V as vector spaces, only the multiplications are different.

In this notation, treating \mathfrak⁢g as a vector space, the linear mapping \ad:\mathfrak⁢g→\mathfrak⁢g⁢l⁢(\mathfrak⁢g) with action

a↦\ad⁢(a),a∈\mathfrak⁢g

is called the adjoint representation of \mathfrak⁢g. The fact that \ad defines a representationPlanetmathPlanetmath is a straight-forward consequence of the Jacobi identityMathworldPlanetmath axiom. Indeed, let a,b∈\mathfrak⁢g be given. We wish to show that

\ad⁢([a,b])=[\ad⁢(a),\ad⁢(b)],

where the bracket on the left is the \mathfrak⁢g multiplication structureMathworldPlanetmath, and the bracket on the right is the commutator bracket. For all c∈\mathfrak⁢g the left hand side maps c to

[[a,b],c],

while the right hand side maps c to

[a,[b,c]]+[b,[a,c]].

Taking skew-symmetry of the bracket as a given, the equality of these two expressions is logically equivalent to the Jacobi identity:

[a,[b,c]]+[b,[c,a]]+[c,[a,b]]=0.
Title adjoint representation
Canonical name AdjointRepresentation
Date of creation 2015-10-05 17:38:19
Last modified on 2015-10-05 17:38:19
Owner rmilson (146)
Last modified by rmilson (146)
Numerical id 9
Author rmilson (146)
Entry type Definition
Classification msc 17B10
Related topic IsotropyRepresentation
Defines adjoint action
Defines gl
Defines general linear Lie algebra