Let GG act on MM by a .

For xMx\in M, the orbit map at xx is the

Φx:GM,Φx(g)=gx.\Phi^x: G \longrightarrow M,\qquad \Phi^x(g)=g\cdot x.
Image and stabilizer

Its image is the GxG\cdot x.

The fiber (Φx)1(x)(\Phi^x)^{-1}(x) is the GxG_x. The orbit map is constant on cosets gGxgG_x, because Φx(gh)=gx\Phi^x(gh)=g\cdot x for hGxh\in G_x, and hence factors through G/GxG/G_x.

Examples
  1. Left translation on GG. For the action of GG on itself by left multiplication and a fixed hGh\in G, the orbit map is gghg\mapsto gh.
  2. Rotations of a vector. For SO(2)R2SO(2)\curvearrowright \mathbb{R}^2 and x0x\neq 0, the orbit map parametrizes the circle of radius x\|x\|.
  3. Conjugation. For the conjugation action of GG on itself, the orbit map at hh is gghg1g\mapsto ghg^{-1}, whose image is the conjugacy class of hh.