General linear Lie algebra

The Lie algebra gl(V) of all endomorphisms with commutator bracket.
General linear Lie algebra

Let VV be a finite-dimensional real or complex vector space.

Definition (General linear Lie algebra).
The general linear Lie algebra is the vector space

gl(V)=End(V) \mathfrak{gl}(V)=\mathrm{End}(V)

equipped with the commutator

[X,Y]=XYYX. [X,Y]=XY-YX.

After choosing a basis, gl(V)gln(F)=Mn(F)\mathfrak{gl}(V)\cong \mathfrak{gl}_n(\mathbb F)=M_n(\mathbb F) with the same bracket.

Relation to the group GL(V)\mathrm{GL}(V).
If G=GL(V)G=\mathrm{GL}(V) is the , then gl(V)\mathfrak{gl}(V) is naturally the , identified with TIGT_I G; under this identification, the Lie bracket on g\mathfrak g agrees with the commutator bracket.

Useful subalgebras.
The trace map tr:gln(F)F\mathrm{tr}:\mathfrak{gl}_n(\mathbb F)\to\mathbb F is a Lie algebra homomorphism to the abelian Lie algebra (F,0)(\mathbb F,0), and its kernel is . The center is the scalar matrices, matching description Z(gln)=FIZ(\mathfrak{gl}_n)=\mathbb F\cdot I.

Context.
Representations of Lie groups and Lie algebras are, by definition, maps into some gl(V)\mathfrak{gl}(V) (see and ).