In mathematics, a Lie groupoid is a groupoid where the set
O
b
of objects and the set
M
o
r
of morphisms are both manifolds, the source and target operations
s
,
t
:
M
o
r
→
O
b
are submersions, and all the category operations (source and target, composition, and identity-assigning map) are smooth.
A Lie groupoid can thus be thought of as a "many-object generalization" of a Lie group, just as a groupoid is a many-object generalization of a group. Just as every Lie group has a Lie algebra, every Lie groupoid has a Lie algebroid.
Any Lie group gives a Lie groupoid with one object, and conversely. So, the theory of Lie groupoids includes the theory of Lie groups.
Given any manifold
M
, there is a Lie groupoid called the pair groupoid, with
M
as the manifold of objects, and precisely one morphism from any object to any other. In this Lie groupoid the manifold of morphisms is thus
M
×
M
.
Given a Lie group
G
acting on a manifold
M
, there is a Lie groupoid called the translation groupoid with one morphism for each triple
g
∈
G
,
x
,
y
∈
M
with
g
x
=
y
.
Any foliation gives a Lie groupoid.
Any principal bundle
P
→
M
with structure group G gives a groupoid, namely
P
×
P
/
G
over M, where G acts on the pairs componentwise. Composition is defined via compatible representatives as in the pair groupoid.
Morita Morphisms and Smooth Stacks
Beside isomorphism of groupoids there is a more coarse notation of equivalence, the so-called Morita equivalence. A quite general example is the Morita-morphism of the Čech groupoid which goes as follows. Let M be a smooth manifold and
{
U
α
}
an open cover of M. Define
G
0
:=
⨆
α
U
α
the disjoint union with the obvious submersion
p
:
G
0
→
M
. In order to encode the structure of the manifold M define the set of morphisms
G
1
:=
⨆
α
,
β
U
α
β
where
U
α
β
=
U
α
∩
U
β
⊂
M
. The source and target map are defined as the embeddings
s
:
U
α
β
→
U
α
and
t
:
U
α
β
→
U
β
. And multiplication is the obvious one if we read the
U
α
β
as subsets of M (compatible points in
U
α
β
and
U
β
γ
actually are the same in M and also lie in
U
α
γ
).
This Čech groupoid is in fact the pullback groupoid of
M
⇒
M
, i.e. the trivial groupoid over M, under p. That is what makes it Morita-morphism.
In order to get the notion of an equivalence relation we need to make the construction symmetric and show that it is also transitive. In this sense we say that 2 groupoids
G
1
⇒
G
0
and
H
1
⇒
H
0
are Morita equivalent iff there exists a third groupoid
K
1
⇒
K
0
together with 2 Morita morphisms from G to K and H to K. Transitivity is an interesting construction in the category of groupoid principal bundles and left to the reader.
It arises the question of what is preserved under the Morita equivalence. There are 2 obvious things, one the coarse quotient/ orbit space of the groupoid
G
0
/
G
1
=
H
0
/
H
1
and secondly the stabilizer groups
G
p
≅
H
q
for corresponding points
p
∈
G
0
and
q
∈
H
0
.
The further question of what is the structure of the coarse quotient space leads to the notion of a smooth stack. We can expect the coarse quotient to be a smooth manifold if for example the stabilizer groups are trivial (as in the example of the Čech groupoid). But if the stabilizer groups change we cannot expect a smooth manifold any longer. The solution is to revert the problem and to define:
A smooth stack is a Morita-equivalence class of Lie groupoids. The natural geometric objects living on the stack are the geometric objects on Lie groupoids invariant under Morita-equivalence. As an example consider the Lie groupoid cohomology.
The notion of smooth stack is quite general, obviously all smooth manifolds are smooth stacks.
But also orbifolds are smooth stacks, namely (equivalence classes of) étale groupoids.
Orbit spaces of foliations are another class of examples
