Lie Group Actions

Def: A smooth manifold M endowed with an smooth action from a Lie group G is called a smooth G-space.

Prop: Suppose E and M are smooth manifolds with or without boundary, and π:N→M is a smooth covering map. With the discrete topology, the covering group Autπ(N) is a zero dimensional Lie group acting smoothly, freely and properly on N.

Suppose G is a Lie group, and M and N are both smooth manifolds endowed with a left or right G-actions. A map F:M→N is said to be equivariant with respect to the given G-actions if for each g∈G, $$\begin{align*} F(g \cdot p) &= g\cdot F(p) \quad \text{for left actions} \ F(p \cdot g) &= F(p)\cdot g \quad \text{for right actions} \end{align*}$$

Equivaraint Rank Theorem: Let M and N be smooth manifolds and let G be a Lie group. Suppose F:M→N is a smooth map that is equivariant with respect to a transitive smooth G-action on M and any smooth action on N. Then F has constant rank. Thus, if F is surjective, it is a smooth submersion, if it is injective it is a smooth immersion; and if it is bijective it is a diffeomorphism.

Suppose G is a Lie group, M is a smooth manifold, and θ:G×M→M is a smooth left action. For each p∈M, we define a map θ(p):G→M by $$\theta^{(p)}(g) = g\cdot p. $$This is often called the orbit map, because its image is the orbit G⋅p. We see that θ(p){p} is just the stabiliser group Gp.

Properties of the Orbit Map: Suppose θ is a smooth left action of a Lie group G on A smooth manifold M. For each p∈M, the orbit map θ(p):G→M is smooth and has constant rank, so the stabiliser group Gp is a properly embedded Lie subgroup of G. If Gp={e}, then θ(p) is an injective smooth immersion, so that G⋅p is an immersed submanifold of M.

Def: If G is a Lie group smoothly on a smooth manifold E, we say that the action is an orientation presering action if for each g∈G, the diffeomorphism x↦g⋅x is orientation preserving.

Semidirect Products

Suppose H and N are Lie groups and θ:H×N→N is a smooth left action of H on N. If is said to be an action by automorphism if for each h∈H, the map θh:N→N is a group automorphism of N. Given such an action, we define a new Lie group N⋊θH, called the semidirect product of H and N, as follows. As a smooth manifold N⋊θH is just the Cartesian product N×H by the group operation is defined by $$(n, h)(n', h') = (n\theta_h(n'), hh').$$
Sometimes, if the action of H on N is understood or irrelevant, the semidirect product is denoted simply by N⋊H.

Example: We see that the Euclidean Group is actually just the semidirect product of Rn⋊O(n), where O(n) is the Orthogonal Group.

Prop: Suppose N and H are Lie groups, and θ is a smooth action of H on N by automorphism. Let G=N⋊θH.

Characterisation of Semidirect Products: Suppose G is a Lie group, and N,H≤G are closed Lie subgroups such that N is normal N∩H={e}, and NH)G. Then the map (n,h)↦nh is a Lie group isomorphism between N⋊θH and G, where θ:H×N→N is the action by conjugation: θh(n)=hnh−1.

Under the hypothesis of the theorem above, we say that G is the internal semidirect product of N and H.

We see that this is just the natural extension of the Semidirect Product of Groups applied to Lie groups.

Prop: Suppose G, N, and H are Lie groups. Then G is isomorphic to a semidirect product N⋊H iff there are Lie group homomorphism φ:G→H and ψ:H→G such that φ∘ψ=idH and ker⁡φ≅N.

Representations

Def: If G is a Lie group, a (finite-dimensional) representation of G is a Lie group homomorphism ρ:G→GL(V) for some finite dimensional real or complex vector space V.

Obs: Any representation ρ yields a smooth left action of G on V, defined by $$g \cdot v := \rho(g) v, \qquad \text{for }g \in G, v \in V$$
Def: If G is a Lie group, an action G on a finite dimensional vector space V is said to be linear if for each g∈G, the map from V to itself given by v↦g⋅v is linear:

Prop: Let G be a Lie group and let V be a finite-dimensional vector space. A smooth action of G on V is linear iff it is of the form g⋅v=ρ(g)v for some representation ρ of G.

Def: If a representation ρ:G→GL(V) is injective, it is said to be a faithful representation.

Obs: By choosing a basis of V, we obtain a Lie group isomorphism GL(V)≅GL(n,R) or GL(n,C), and the image of a representation ρ:G→Gl(V) is a Lie subgroup of GL(V). Meaning, a Lie group admits a faithful representation iff it is isomorphic to a Lie subgroup of GL(n,R) or GL(n,C).

Def: If G is a Lie subgroup of GL(n,R), the inclusion map G↪GL(n,R) is a faithful representation, called the defining representation of G.

Let G be a Lie group. For any g∈G, the conjugation map Cg:G→G given y Cg(h)=ghg−1 is a Lie group homomorphism. We let Ad(g)=(Cg)∗:g→g denote its induced Lie algebra homomorphism. Because conjugation is an action of the Lie group onto itself, we get that Ad(g1g2)=Ad(g1)∘Ad(g2), and Ad(g) is invertible with Ad(g−1). We can show that Ad:G→GL(g) is smooth, it follows that it is a representation, called the adjoint representation of G.

Def: If g os a finite-dimensional Lie algebra, a (finite-dimensional) representation of g is a Lie algebra homomorphism ϕ:g→gl(V) for some finite-dimensional vector space V. If ϕ is injective, it is said to be a faithful representation, in which case g is isomorphic to the Lie subalgebra ϕ(g)⊆gl(V)≅gl(n,R).

Obs: If ρ:G→GL(V) is any representation of the Lie group G, then ρ∗:g→gl(V) is easily seen to be a representation of g.

(∗) Ado's Theorem: Every finite-dimensional Lie algebra admits a faithful finite-dimensional representation.

Quotients of Manifolds by Group Actions

Prop: Any continuous action by a compact Lie group on manifold is proper.

Quotient Manifold Theorem: Suppose a Lie group G acts smoothly, freely, and properly on a smooth manifold M. Then the orbit space M/G is a topological manifold of dimension equal to dim⁡M−dim⁡G, and has a unique smooth structure with the property that the quotient map π:M→M/G is a smooth submersion.

Prop: Suppose a Lie group acts smoothly on a manifold M. Each orbit is an immersed submanifold of M.

Prop: Suppose a connected Lie group G acts smoothly on a discrete space K. Then this action is trivial.

Cor: If G is a connected Lie group, then every discrete normal subgroup of G is central.

Prop: Given that π:G~→G is a universal covering map, then the covering group Cπ(G~) is isomorphic to π1(G,e). Then we can prove that the fundamental group of a connected Lie group is abelian.

Th: Suppose M is a connected smooth manifold, and Γ is a discrete group acting smoothly, freely and properly on M. Then the quotient space M/Γ is a topological manifold and has a unique smooth structure such that π:M→M/Γ is a smooth normal covering map.

Cor: Let π:N→M be a smooth normal covering map, then M is diffeomorphic to the quotient manifold N/Cπ(N).

Prop: Let M be a smooth manifold, and let π:E→M be a smooth vector bundle over M. Suppose Γ is a discrete group acting smoothly, freely and properly on both E and M. Suppose further that π is Γ-equivariant, and each p∈M and each g∈Γ, the map Ep to Eg⋅p is given by v↦g⋅v is linear. Then E/Γ can be given the structure of a smooth vector bundle over M/Γ un such a way that the following diagram commutes:

\usepackage{tikz-cd}
\begin{document}
\begin{tikzcd}[row sep=2cm, column sep=2cm]
E \arrow{r}\arrow{d}& E/\Gamma \arrow{d} \\
M \arrow{r}& M/\Gamma
\end{tikzcd}
\end{document}

Actions on Riemannian Manifolds

Let (M,g) be a connected Riemannian manifold, and let Γ be a Lie group, and let θ:Γ×M→M be a group action. We say that Γ acts by isometries if for each g∈Γ, the map θg:M→M is Riemannian isometry. Γ acts discontinuously if no Γ-orbit has a limit point in M.

Acting by isometry can be also be understood as there being an group homomorphism θ:Γ→Iso(M), The action being free and acting by isometry would imply that the group homomorphism is injective.

Prop: If Γ acts, freely, smoothly, and discontinuously on M by isometries, then the quotient map M→M/Γ is a smooth covering map.

Prop: Let Γ be a discrete group acting smoothly, freely, and properly on a connected smooth manifold M~, and let M=M~/Γ. If a Riemannian metric g~ on M~ is a pullback of a metric on M by the quotient map π:M~→M iff Γ acts by isometry.