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 with action
For any vector space![]()
, we use to denote the Lie algebra
of 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 of
the Jacobi identity
![]()
axiom. Indeed, let be given. We
wish to show that
where the bracket on the left is the
multiplication structure![]()
, and the bracket on the right is the
commutator bracket. For all the left hand side maps to
while the right hand side maps to
Taking skew-symmetry of the bracket as a given, the equality of these two expressions is logically equivalent to the Jacobi identity:
| 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 |