Let GG and MM be given.

A smooth left action of GG on MM is a

Φ:G×M⟶M\Phi: G\times M \longrightarrow M

such that, writing g⋅x:=Φ(g,x)g\cdot x:=\Phi(g,x), the following hold for all g,h∈Gg,h\in G and x∈Mx\in M:

  1. (Identity) e⋅x=xe\cdot x = x.
  2. (Compatibility) (gh)⋅x=g⋅(h⋅x)(gh)\cdot x = g\cdot(h\cdot x).

A smooth right action is defined similarly, using a smooth map M×G→MM\times G\to M, (x,g)↦x⋅g(x,g)\mapsto x\cdot g, with x⋅e=xx\cdot e=x and (x⋅g)⋅h=x⋅(gh)(x\cdot g)\cdot h = x\cdot(gh).

Time-independent action maps

For each g∈Gg\in G, the map Φg:M→M\Phi_g:M\to M, Φg(x)=g⋅x\Phi_g(x)=g\cdot x, is a with inverse Φg−1\Phi_{g^{-1}}.

Examples
  1. Left translation on the group. GG acts on itself by g⋅h:=ghg\cdot h := gh.
  2. Rotations of the plane. SO(2)SO(2) acts on R2\mathbb{R}^2 by matrix multiplication.
  3. Change of frame. The general linear group GL(n,R)GL(n,\mathbb{R}) acts on the frame bundle of a manifold by u⋅g=u∘gu\cdot g=u\circ g for a frame u:Rn→TxMu:\mathbb R^n\to T_xM (precomposition of the frame by gg, a right action).