Lie Group Actions

Orbits, stabilizers, and homogeneous spaces

Orbits, Stabilizers, and Quotient Spaces

A Lie group action on a manifold is a smooth map that assigns to each group element a diffeomorphism of the manifold, compatible with the group operation. The orbit of a point is the set of all points reachable from it via the group action. The stabilizer (or isotropy group) is the subgroup that fixes the point.

The orbit-stabilizer theorem says dim(Orbit) + dim(Stabilizer) = dim(Group). This gives rise to homogeneous spaces: the sphere S² = SO(3)/SO(2) because SO(3) acts transitively on the sphere with SO(2) stabilizer at each point. Grassmannians, flag manifolds, and many other important spaces arise as quotients of Lie groups.

SO(3) Acting on S²

Pick a point on the sphere. The orbit under SO(3) fills the entire sphere in a color wave — the action is transitive, meaning any point can be rotated to any other. The stabilizer of a point is the set of rotations that fix it: rotations around the axis through that point, forming an SO(2) subgroup. The glowing ring with orbiting particles visualizes this stabilizer. Hence S² = SO(3)/SO(2).

Key insight: The sphere S² is a homogeneous space — it looks the same from every point. This is because SO(3) acts transitively: the orbit of any point is the entire sphere.

The Orbit-Stabilizer Theorem

dim(Orbit) + dim(Stabilizer) = dim(Group). This fundamental equation splits the dimension of the group into two complementary parts. Watch the bar animation divide dim(G) into colored segments representing the orbit and stabilizer dimensions. Explore multiple preset actions to see how the split varies.

Famous Homogeneous Spaces

Many important spaces in geometry arise as quotients of Lie groups: spheres Sⁿ = SO(n+1)/SO(n), real projective spaces ℝPⁿ = O(n+1)/(O(1) × O(n)), Grassmannians, and flag manifolds. Select a homogeneous space to see its structure and the animated group action that generates it.

Symmetry Breaking & Orbit Types

When a group acts on a space, different points can have different stabilizers — this is symmetry breaking. For SO(2) acting on ℝ², the origin has the full group as its stabilizer (it's a fixed point), while every other point has trivial stabilizer (its orbit is a full circle). The heatmap shows orbit dimension across the space, with animated particle flow along the circular orbits.

Key Takeaways

  • Orbits — the set of points reachable from a given point; transitive actions have a single orbit
  • Stabilizers — the subgroup fixing a point; complement orbits via dim(Orbit) + dim(Stab) = dim(G)
  • Homogeneous spaces — quotients G/H that “look the same everywhere”: spheres, projective spaces, Grassmannians
  • Symmetry breaking — different orbit types reveal the structure of the action and its fixed points