There is an obvious functor
which sends every Lie group to its Lie algebra and every homomorphism of Lie groups to the corresponding homomorphism of Lie algebras.
Lie’s three theorems establish the following properties of this functor.
1. Lie’s first theorem is today regarded as lacking a good notion of differentiable manifold;
2. Lie II If and are Lie groups with Lie algebras and ; such that is simply connected; and if is a morphism of Lie algebras; then there is a unique morphism of Lie groups lifting , i.e. such that .
3. Lie III is surjective on objects: to every Lie algebra there is a Lie group such that . Moreover, there exists such which is simply connected.
Let be the full subcategory of on simply connected Lie groups. Then the above implies that restricted to the functor becomes a surjective equivalence of categories
The horizontal categorification of Lie’s theorems for Lie groups leads to analogous statements for Lie groupoids: in this case becomes the differentiation functor from Lie groupoids to Lie algebroids
In the case of Lie groupoids, the condition of a group being simply connected which plays an important role in the above statements is generalized to the condition that source fibers of the Lie groupoid (the preimages of the source map at every object of the Lie groupoid ) are simply connected. One says
Lie II for Lie groupoids now reads exactly as Lie II for Lie groups, with “simply connected” replaced by “source simply connected”.
Lie II for Lie groupoids was proven in
and
Lie III for Lie groupoids does not hold in direct generalization:
by the general mechanism of Lie integration the space of morphisms of the source simply-connected topological groupoid integrating a Lie algebroid is a quotient space. This quotient may fail to be a manifold due to singularities.
The precise conditions under which Lie algebroids do have Lie groupoids integrating them were found in
A comprehensive review is in
A review of Lie theory of Lie groupoids in on pages 3-5 of
and in the introduction of
This failure of Lie III for Lie groupoids, i.e. for internal groupoids in Diff seems to suggest that the category of manifolds is not the natural home for general Lie theory. More concretely, it seems to suggest that Lie theory ought to be practiced internal to some category of generalized smooth spaces.
One such choice is given by replacing manifolds by differentiable stacks.
The generalization of Lie’s theorems from Lie groups to to stacky Lie groupoids is discussed in