Lie’s third theorem

Every finite-dimensional Lie algebra is the Lie algebra of a connected, simply connected Lie group.
Lie’s third theorem

Let g\mathfrak g be a finite-dimensional over R\Bbb R (or C\Bbb C).

Theorem (existence and uniqueness up to simply connected cover)

There exists a connected, GG such that

Lie(G)g \operatorname{Lie}(G)\cong \mathfrak g

as Lie algebras (via a ).

Moreover, if G1G_1 and G2G_2 are connected simply connected Lie groups with Lie algebras isomorphic to g\mathfrak g, then G1G_1 and G2G_2 are isomorphic as . In other words, the simply connected integration of g\mathfrak g is unique up to Lie group isomorphism.

Context

Combined with the fact that every connected Lie group has a which is again a Lie group (see ), Lie’s third theorem explains why Lie algebras control the local—and, up to discrete central quotients, the global—structure of connected Lie groups (compare ).

It also underlies the : Lie subalgebras integrate to connected (immersed) Lie subgroups inside a given Lie group.