Structure of connected abelian Lie groups

Every connected abelian Lie group is isomorphic to R^n × T^m.
Structure of connected abelian Lie groups

Let GG be a that is , and let g\mathfrak{g} be its .

Theorem (classification). There exist integers n,m0n,m\ge 0 such that

GRn×Tmas Lie groups, G \cong \mathbb{R}^n \times \mathbb{T}^m \quad\text{as Lie groups},

where Tm\mathbb{T}^m is an mm-torus (isomorphic to (S1)m(S^1)^m). In particular, GG is determined up to isomorphism by the pair (n,m)(n,m) with dimG=n+m\dim G = n+m.

Idea of proof (covering + lattice).

  • Since GG is connected and abelian, its universal cover G~\widetilde{G} is a connected simply connected abelian Lie group. Such a group is isomorphic to the additive group of its Lie algebra, so G~(g,+)Rn+m\widetilde{G}\cong (\mathfrak{g},+) \cong \mathbb{R}^{n+m}; compare .
  • The covering map G~G\widetilde{G}\to G has kernel a of G~\widetilde{G}, hence a lattice in Rn+m\mathbb{R}^{n+m} up to linear change of coordinates.
  • Splitting Rn+m\mathbb{R}^{n+m} into directions along the lattice and transverse directions produces Rn×(Rm/Zm)\mathbb{R}^n\times (\mathbb{R}^m/\mathbb{Z}^m).

Context. This result explains why the basic connected abelian examples are Rn\mathbb{R}^n, circles, and tori; see and . It also matches the infinitesimal picture: g\mathfrak{g} is an , so the is a local group isomorphism whose global kernel records the lattice.