Consider a collection of diagonal matrices , which span
a subspace
. Then the
th eigenvalue, i.e., the
th entry along the diagonal, is a linear
functional on
,
and is called a weight.
The general setting for weights occurs in a Lie algebra representation of a semisimple Lie
algebra, in which case the Cartan subalgebra is Abelian
and can be put into diagonal form. For example, consider the standard representation
of the special linear Lie algebra
on
. Then
(1)
|
and
(2)
|
span the Cartan subalgebra . There are three weights,
(3)
|
(4)
|
and
(5)
|
corresponding to the decomposition of
(6)
|
into its eigenspaces. Note that , because the matrices have zero matrix trace. The eigenvectors
are called weight vectors,
and the corresponding eigenspaces are called weight spaces.
In the important special case of the adjoint representation of a semisimple Lie algebra,
the weights are called Lie algebra roots and the
weight space is called the root
space. The roots generate a discrete lattice,
called the root lattice, in the dual
vector space .
The set of all possible weights forms a weight lattice,
which contains the root lattice. The Lie
Algebra representations of
can be classified using the weight
lattice.