Some notes on the structure theory of cocompact proper Lie groupoids. All Lie groupoids will be comprised of Hausdorff paracompact smooth manifolds.
A Lie groupoid is called proper if the map is proper.
Given a proper Lie groupoid the topological space , the coequaliser of , is Hausdorff and paracompact. In addition, the map is open.
The orbits of a proper Lie groupoid are closed embedded submanifolds of , and all isotropy groups are compact Lie groups.
A proper Lie groupoid is called cocompact if is compact.
Recall the definition of weak equivalence of Lie groupoids: an internal functor that is fully faithful and such that is a surjective submersion. We shall be interested in finding, for a given cocompact proper Lie groupoid, another Lie groupoid connected by a span of weak equivalences to the first and having a particular form. This requires the following simple result.
The properties of being proper and cocompact are invariant under weak equivalence.
The main technical result we shall use is the slice theorem for proper Lie groupoids, detailed expositions of which can be found in Crainic and Struchiner and Pflaum et al. To state the theorem we need to discuss the linearisation of a proper Lie groupoid.
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For a proper Lie groupoid , the space admits arbitrarily fine good open covers.
Thus the orbit space of a cocompact proper Lie groupoid admits arbitrarily fine finite good open covers.
A cocompact proper Lie groupoid admits an essentially surjective functor from a Lie groupoid of the form
where is a compact Lie group and is an invariant open ball in an orthogonal representation of , and each is a full embedding.
In fact any proper Lie groupoid admits such a functor where the coproduct isn’t necessarily finite, and this is essentially the content of the linearisation theorem. Compactness of the orbit space together with openness of the quotient map means finitely many balls map to an open cover of the orbit space, hence the saturations of those open balls form an open cover of the object manifold of the groupoid.
Call a Lie groupoid of the form as in the previous proposition a ball groupoid.
A cocompact proper Lie groupoid has only finitely many normal orbit types, and hence only finitely many weak orbit types.
The weak orbit type of a object is the isomorphism class of the Lie group of automorphisms of . The normal orbit type of is the isomorphism class of the slice representation at (see Pflaum et al, definition 5.6).
Given two ball groupoids , mapping to a Lie groupoid , it is of great interest to know what the pullback (in the appropriate Lie groupoid sense) is. One immediate result is that if, without loss of generality, , then it can be taken to be a full open subgroupoid of . Since this ball groupoid is the interior of the action groupoid , which is a cocompact proper Lie groupoid, it can itself (I believe!) be covered by finitely many ball groupoids, in the sense of the above proposition.
However, ideally the subgroupoid has as object space a contractible open set in . One way to get at this is to get estimates on a sort of ‘transverse convexity radius’. This will ultimately depend on the following result.
Every proper Lie groupoid admits a metric on that is transversally invariant and complete, and that is adapted to the singular Riemannian foliation given by connected components of the orbits of
A key property of a singular Riemannian foliation is that every geodesic that is perpendicular to a leaf at one point is perpendicular to every leaf it meets.
What if I consider the convexity radius for this metric?
We also can consider the injectivity radius (or a transverse version), which will tell us how large the ball groupoids can be. Actually the local structure theorem is a little stronger, in that one gets charts in the object manifold such that the induced groupoid is isomorphic to . Presumably if we take the geodesic radius of to be such that it arises from via exponential map and is geodesically convex, then since the decomposition is in some sense compatible with the geodesic flow, we should get transversally geodesically convex. Moreover, for any point the hope is that there is a global slice through for for any neighbourhood of such that (here is the orbit through ).
Cocompact proper Lie groupoids are compact objects in the (2,1)-category of Lie groupoids and anafunctors (equivalently the (2,1)-category of differentiable stacks).
This is complicated somewhat by differing notions of what ‘compact’ means in a higher topos. See differential cohomology in a cohesive topos, section 3.6.4.
Last revised on August 3, 2016 at 08:21:25. See the history of this page for a list of all contributions to it.