In the conditions of the previous definition, we call the -orbit of the set of points for .
For a subset and an element , the -translate is the set of points in of the form , for some .
The quotient set is the set of -orbits, and the map that sends to its -orbit is the quotient map.
If the action is transitive, then there is only one orbit, and for any , we have
where , the set of cosets. In this case, we say that is a homogeneous space.
Let be a topological space and a discrete group. A right action of on is continuous if, for each , the induced map is continuous (and therefore a homeomorphism).
The action is said to be properly discontinuous when it is continuous and each has a neighborhood such that the -translate intersects only for a finite number of elements of .
Free and properly discontinuous actions are important because, in Hausdorff spaces , each has at least one neighborhood disjoint from each for any (this needs to be proven).
Let be a Hausdorff topological space equipped with a free and properly discontinuous action by a group . There exists a unique topology on such that the quotient map is continuous and also a local homeomorphism. Moreover, this map is open.
In this topology, a set is open if and only if its preimage in is open. If a subset is an open set that is disjoint from for , then the restriction is a homeomorphism.
The space with this topology is locally Hausdorff in general. We can assert that it is Hausdorff in the following case:
Lemma
Under the conditions of the previous proposition, the space is Hausdorff if and only if the image of the map
is closed in .
We say that a group action is differentiable when the associated homeomorphisms are also diffeomorphisms.
Theorem (Quotient manifold theorem)
Suppose a Lie group acts smoothly, freely, and properly on a smooth manifold . Then the orbit space is a topological manifold of dimension , and has a unique smooth structure with the property that the quotient map is a smooth submersion.
See @lee2013smooth theorem 7.10 at page 153.
Lie group action
In case is a Lie group action on a manifold we have an injection
Indeed, is in some sense like a (infinite dimensional) Lie group, whose Lie algebra is . This is due to the flow theorem for vector fields.
Given a vector in the Lie algebra we can consider the fundamental vector field on . This corresponds to the differential of at the identity :