adjoint representation
\DeclareMathOperator\ad
ad \DeclareMathOperator\EndEnd
Let \mathfrakg be a Lie algebra. For every a∈\mathfrakg we define the
, a.k.a. the adjoint action,
\ad(a):\mathfrakg→\mathfrakg |
to be the linear transformation with action
\ad(a):b↦[a,b],b∈\mathfrakg. |
For any vector space V, we use \mathfrakgl(V) to denote the Lie algebra
of \EndV determined by the commutator bracket. So
\mathfrakgl(V)=\EndV as vector spaces, only the multiplications are different.
In this notation, treating \mathfrakg as a vector space, the linear mapping \ad:\mathfrakg→\mathfrakgl(\mathfrakg) with action
a↦\ad(a),a∈\mathfrakg |
is called the adjoint representation of \mathfrakg. The fact that
\ad defines a representation is a straight-forward consequence of
the Jacobi identity
axiom. Indeed, let a,b∈\mathfrakg be given. We
wish to show that
\ad([a,b])=[\ad(a),\ad(b)], |
where the bracket on the left is the
\mathfrakg multiplication structure, and the bracket on the right is the
commutator bracket. For all c∈\mathfrakg 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 |