- Source: Groupoid
In mathematics, especially in category theory and homotopy theory, a groupoid (less often Brandt groupoid or virtual group) generalises the notion of group in several equivalent ways. A groupoid can be seen as a:
Group with a partial function replacing the binary operation;
Category in which every morphism is invertible. A category of this sort can be viewed as augmented with a unary operation on the morphisms, called inverse by analogy with group theory. A groupoid where there is only one object is a usual group.
In the presence of dependent typing, a category in general can be viewed as a typed monoid, and similarly, a groupoid can be viewed as simply a typed group. The morphisms take one from one object to another, and form a dependent family of types, thus morphisms might be typed
g
:
A
→
B
{\displaystyle g:A\rightarrow B}
,
h
:
B
→
C
{\displaystyle h:B\rightarrow C}
, say. Composition is then a total function:
∘
:
(
B
→
C
)
→
(
A
→
B
)
→
A
→
C
{\displaystyle \circ :(B\rightarrow C)\rightarrow (A\rightarrow B)\rightarrow A\rightarrow C}
, so that
h
∘
g
:
A
→
C
{\displaystyle h\circ g:A\rightarrow C}
.
Special cases include:
Setoids: sets that come with an equivalence relation,
G-sets: sets equipped with an action of a group
G
{\displaystyle G}
.
Groupoids are often used to reason about geometrical objects such as manifolds. Heinrich Brandt (1927) introduced groupoids implicitly via Brandt semigroups.
Definitions
= Algebraic
=A groupoid can be viewed as an algebraic structure consisting of a set with a binary partial function .
Precisely, it is a non-empty set
G
{\displaystyle G}
with a unary operation
−
1
:
G
→
G
,
{\displaystyle {}^{-1}:G\to G,}
and a partial function
∗
:
G
×
G
⇀
G
{\displaystyle *:G\times G\rightharpoonup G}
. Here * is not a binary operation because it is not necessarily defined for all pairs of elements of
G
{\displaystyle G}
. The precise conditions under which
∗
{\displaystyle *}
is defined are not articulated here and vary by situation.
The operations
∗
{\displaystyle \ast }
and −1 have the following axiomatic properties: For all
a
{\displaystyle a}
,
b
{\displaystyle b}
, and
c
{\displaystyle c}
in
G
{\displaystyle G}
,
Associativity: If
a
∗
b
{\displaystyle a*b}
and
b
∗
c
{\displaystyle b*c}
are defined, then
(
a
∗
b
)
∗
c
{\displaystyle (a*b)*c}
and
a
∗
(
b
∗
c
)
{\displaystyle a*(b*c)}
are defined and are equal. Conversely, if one of
(
a
∗
b
)
∗
c
{\displaystyle (a*b)*c}
or
a
∗
(
b
∗
c
)
{\displaystyle a*(b*c)}
is defined, then they are both defined (and they are equal to each other), and
a
∗
b
{\displaystyle a*b}
and
b
∗
c
{\displaystyle b*c}
are also defined.
Inverse:
a
−
1
∗
a
{\displaystyle a^{-1}*a}
and
a
∗
a
−
1
{\displaystyle a*{a^{-1}}}
are always defined.
Identity: If
a
∗
b
{\displaystyle a*b}
is defined, then
a
∗
b
∗
b
−
1
=
a
{\displaystyle a*b*{b^{-1}}=a}
, and
a
−
1
∗
a
∗
b
=
b
{\displaystyle {a^{-1}}*a*b=b}
. (The previous two axioms already show that these expressions are defined and unambiguous.)
Two easy and convenient properties follow from these axioms:
(
a
−
1
)
−
1
=
a
{\displaystyle (a^{-1})^{-1}=a}
,
If
a
∗
b
{\displaystyle a*b}
is defined, then
(
a
∗
b
)
−
1
=
b
−
1
∗
a
−
1
{\displaystyle (a*b)^{-1}=b^{-1}*a^{-1}}
.
= Category theoretic
=A groupoid is a small category in which every morphism is an isomorphism, i.e., invertible. More explicitly, a groupoid G is a set G0 of objects with
for each pair of objects x and y a (possibly empty) set G(x,y) of morphisms (or arrows) from x to y; we write f : x → y to indicate that f is an element of G(x,y);
for every object x a designated element
i
d
x
{\displaystyle \mathrm {id} _{x}}
of G(x,x);
for each triple of objects x, y, and z a function
c
o
m
p
x
,
y
,
z
:
G
(
y
,
z
)
×
G
(
x
,
y
)
→
G
(
x
,
z
)
:
(
g
,
f
)
↦
g
f
{\displaystyle \mathrm {comp} _{x,y,z}:G(y,z)\times G(x,y)\rightarrow G(x,z):(g,f)\mapsto gf}
;
for each pair of objects x, y a function
i
n
v
:
G
(
x
,
y
)
→
G
(
y
,
x
)
:
f
↦
f
−
1
{\displaystyle \mathrm {inv} :G(x,y)\rightarrow G(y,x):f\mapsto f^{-1}}
satisfying, for any f : x → y, g : y → z, and h : z → w:
f
i
d
x
=
f
{\displaystyle f\ \mathrm {id} _{x}=f}
and
i
d
y
f
=
f
{\displaystyle \mathrm {id} _{y}\ f=f}
;
(
h
g
)
f
=
h
(
g
f
)
{\displaystyle (hg)f=h(gf)}
;
f
f
−
1
=
i
d
y
{\displaystyle ff^{-1}=\mathrm {id} _{y}}
and
f
−
1
f
=
i
d
x
{\displaystyle f^{-1}f=\mathrm {id} _{x}}
.
If f is an element of G(x,y) then x is called the source of f, written s(f), and y is called the target of f, written t(f).
A groupoid G is sometimes denoted as
G
1
⇉
G
0
{\displaystyle G_{1}\rightrightarrows G_{0}}
, where
G
1
{\displaystyle G_{1}}
is the set of all morphisms, and the two arrows
G
1
→
G
0
{\displaystyle G_{1}\to G_{0}}
represent the source and the target.
More generally, one can consider a groupoid object in an arbitrary category admitting finite fiber products.
= Comparing the definitions
=The algebraic and category-theoretic definitions are equivalent, as we now show. Given a groupoid in the category-theoretic sense, let G be the disjoint union of all of the sets G(x,y) (i.e. the sets of morphisms from x to y). Then
c
o
m
p
{\displaystyle \mathrm {comp} }
and
i
n
v
{\displaystyle \mathrm {inv} }
become partial operations on G, and
i
n
v
{\displaystyle \mathrm {inv} }
will in fact be defined everywhere. We define ∗ to be
c
o
m
p
{\displaystyle \mathrm {comp} }
and −1 to be
i
n
v
{\displaystyle \mathrm {inv} }
, which gives a groupoid in the algebraic sense. Explicit reference to G0 (and hence to
i
d
{\displaystyle \mathrm {id} }
) can be dropped.
Conversely, given a groupoid G in the algebraic sense, define an equivalence relation
∼
{\displaystyle \sim }
on its elements by
a
∼
b
{\displaystyle a\sim b}
iff a ∗ a−1 = b ∗ b−1. Let G0 be the set of equivalence classes of
∼
{\displaystyle \sim }
, i.e.
G
0
:=
G
/
∼
{\displaystyle G_{0}:=G/\!\!\sim }
. Denote a ∗ a−1 by
1
x
{\displaystyle 1_{x}}
if
a
∈
G
{\displaystyle a\in G}
with
x
∈
G
0
{\displaystyle x\in G_{0}}
.
Now define
G
(
x
,
y
)
{\displaystyle G(x,y)}
as the set of all elements f such that
1
x
∗
f
∗
1
y
{\displaystyle 1_{x}*f*1_{y}}
exists. Given
f
∈
G
(
x
,
y
)
{\displaystyle f\in G(x,y)}
and
g
∈
G
(
y
,
z
)
,
{\displaystyle g\in G(y,z),}
their composite is defined as
g
f
:=
f
∗
g
∈
G
(
x
,
z
)
{\displaystyle gf:=f*g\in G(x,z)}
. To see that this is well defined, observe that since
(
1
x
∗
f
)
∗
1
y
{\displaystyle (1_{x}*f)*1_{y}}
and
1
y
∗
(
g
∗
1
z
)
{\displaystyle 1_{y}*(g*1_{z})}
exist, so does
(
1
x
∗
f
∗
1
y
)
∗
(
g
∗
1
z
)
=
f
∗
g
{\displaystyle (1_{x}*f*1_{y})*(g*1_{z})=f*g}
. The identity morphism on x is then
1
x
{\displaystyle 1_{x}}
, and the category-theoretic inverse of f is f−1.
Sets in the definitions above may be replaced with classes, as is generally the case in category theory.
= Vertex groups and orbits
=Given a groupoid G, the vertex groups or isotropy groups or object groups in G are the subsets of the form G(x,x), where x is any object of G. It follows easily from the axioms above that these are indeed groups, as every pair of elements is composable and inverses are in the same vertex group.
The orbit of a groupoid G at a point
x
∈
X
{\displaystyle x\in X}
is given by the set
s
(
t
−
1
(
x
)
)
⊆
X
{\displaystyle s(t^{-1}(x))\subseteq X}
containing every point that can be joined to x by a morphism in G. If two points
x
{\displaystyle x}
and
y
{\displaystyle y}
are in the same orbits, their vertex groups
G
(
x
)
{\displaystyle G(x)}
and
G
(
y
)
{\displaystyle G(y)}
are isomorphic: if
f
{\displaystyle f}
is any morphism from
x
{\displaystyle x}
to
y
{\displaystyle y}
, then the isomorphism is given by the mapping
g
→
f
g
f
−
1
{\displaystyle g\to fgf^{-1}}
.
Orbits form a partition of the set X, and a groupoid is called transitive if it has only one orbit (equivalently, if it is connected as a category). In that case, all the vertex groups are isomorphic (on the other hand, this is not a sufficient condition for transitivity; see the section below for counterexamples).
= Subgroupoids and morphisms
=A subgroupoid of
G
⇉
X
{\displaystyle G\rightrightarrows X}
is a subcategory
H
⇉
Y
{\displaystyle H\rightrightarrows Y}
that is itself a groupoid. It is called wide or full if it is wide or full as a subcategory, i.e., respectively, if
X
=
Y
{\displaystyle X=Y}
or
G
(
x
,
y
)
=
H
(
x
,
y
)
{\displaystyle G(x,y)=H(x,y)}
for every
x
,
y
∈
Y
{\displaystyle x,y\in Y}
.
A groupoid morphism is simply a functor between two (category-theoretic) groupoids.
Particular kinds of morphisms of groupoids are of interest. A morphism
p
:
E
→
B
{\displaystyle p:E\to B}
of groupoids is called a fibration if for each object
x
{\displaystyle x}
of
E
{\displaystyle E}
and each morphism
b
{\displaystyle b}
of
B
{\displaystyle B}
starting at
p
(
x
)
{\displaystyle p(x)}
there is a morphism
e
{\displaystyle e}
of
E
{\displaystyle E}
starting at
x
{\displaystyle x}
such that
p
(
e
)
=
b
{\displaystyle p(e)=b}
. A fibration is called a covering morphism or covering of groupoids if further such an
e
{\displaystyle e}
is unique. The covering morphisms of groupoids are especially useful because they can be used to model covering maps of spaces.
It is also true that the category of covering morphisms of a given groupoid
B
{\displaystyle B}
is equivalent to the category of actions of the groupoid
B
{\displaystyle B}
on sets.
Examples
= Topology
=Given a topological space
X
{\displaystyle X}
, let
G
0
{\displaystyle G_{0}}
be the set
X
{\displaystyle X}
. The morphisms from the point
p
{\displaystyle p}
to the point
q
{\displaystyle q}
are equivalence classes of continuous paths from
p
{\displaystyle p}
to
q
{\displaystyle q}
, with two paths being equivalent if they are homotopic.
Two such morphisms are composed by first following the first path, then the second; the homotopy equivalence guarantees that this composition is associative. This groupoid is called the fundamental groupoid of
X
{\displaystyle X}
, denoted
π
1
(
X
)
{\displaystyle \pi _{1}(X)}
(or sometimes,
Π
1
(
X
)
{\displaystyle \Pi _{1}(X)}
). The usual fundamental group
π
1
(
X
,
x
)
{\displaystyle \pi _{1}(X,x)}
is then the vertex group for the point
x
{\displaystyle x}
.
The orbits of the fundamental groupoid
π
1
(
X
)
{\displaystyle \pi _{1}(X)}
are the path-connected components of
X
{\displaystyle X}
. Accordingly, the fundamental groupoid of a path-connected space is transitive, and we recover the known fact that the fundamental groups at any base point are isomorphic. Moreover, in this case, the fundamental groupoid and the fundamental groups are equivalent as categories (see the section below for the general theory).
An important extension of this idea is to consider the fundamental groupoid
π
1
(
X
,
A
)
{\displaystyle \pi _{1}(X,A)}
where
A
⊂
X
{\displaystyle A\subset X}
is a chosen set of "base points". Here
π
1
(
X
,
A
)
{\displaystyle \pi _{1}(X,A)}
is a (wide) subgroupoid of
π
1
(
X
)
{\displaystyle \pi _{1}(X)}
, where one considers only paths whose endpoints belong to
A
{\displaystyle A}
. The set
A
{\displaystyle A}
may be chosen according to the geometry of the situation at hand.
= Equivalence relation
=If
X
{\displaystyle X}
is a setoid, i.e. a set with an equivalence relation
∼
{\displaystyle \sim }
, then a groupoid "representing" this equivalence relation can be formed as follows:
The objects of the groupoid are the elements of
X
{\displaystyle X}
;
For any two elements
x
{\displaystyle x}
and
y
{\displaystyle y}
in
X
{\displaystyle X}
, there is a single morphism from
x
{\displaystyle x}
to
y
{\displaystyle y}
(denote by
(
y
,
x
)
{\displaystyle (y,x)}
) if and only if
x
∼
y
{\displaystyle x\sim y}
;
The composition of
(
z
,
y
)
{\displaystyle (z,y)}
and
(
y
,
x
)
{\displaystyle (y,x)}
is
(
z
,
x
)
{\displaystyle (z,x)}
.
The vertex groups of this groupoid are always trivial; moreover, this groupoid is in general not transitive and its orbits are precisely the equivalence classes. There are two extreme examples:
If every element of
X
{\displaystyle X}
is in relation with every other element of
X
{\displaystyle X}
, we obtain the pair groupoid of
X
{\displaystyle X}
, which has the entire
X
×
X
{\displaystyle X\times X}
as set of arrows, and which is transitive.
If every element of
X
{\displaystyle X}
is only in relation with itself, one obtains the unit groupoid, which has
X
{\displaystyle X}
as set of arrows,
s
=
t
=
i
d
X
{\displaystyle s=t=id_{X}}
, and which is completely intransitive (every singleton
{
x
}
{\displaystyle \{x\}}
is an orbit).
Examples
If
f
:
X
0
→
Y
{\displaystyle f:X_{0}\to Y}
is a smooth surjective submersion of smooth manifolds, then
X
0
×
Y
X
0
⊂
X
0
×
X
0
{\displaystyle X_{0}\times _{Y}X_{0}\subset X_{0}\times X_{0}}
is an equivalence relation since
Y
{\displaystyle Y}
has a topology isomorphic to the quotient topology of
X
0
{\displaystyle X_{0}}
under the surjective map of topological spaces. If we write,
X
1
=
X
0
×
Y
X
0
{\displaystyle X_{1}=X_{0}\times _{Y}X_{0}}
then we get a groupoid
X
1
⇉
X
0
{\displaystyle X_{1}\rightrightarrows X_{0}}
which is sometimes called the banal groupoid of a surjective submersion of smooth manifolds.
If we relax the reflexivity requirement and consider partial equivalence relations, then it becomes possible to consider semidecidable notions of equivalence on computable realisers for sets. This allows groupoids to be used as a computable approximation to set theory, called PER models. Considered as a category, PER models are a cartesian closed category with natural numbers object and subobject classifier, giving rise to the effective topos introduced by Martin Hyland.
= Čech groupoid
=A Čech groupoidp. 5 is a special kind of groupoid associated to an equivalence relation given by an open cover
U
=
{
U
i
}
i
∈
I
{\displaystyle {\mathcal {U}}=\{U_{i}\}_{i\in I}}
of some manifold
X
{\displaystyle X}
. Its objects are given by the disjoint union
G
0
=
∐
U
i
{\displaystyle {\mathcal {G}}_{0}=\coprod U_{i}}
,
and its arrows are the intersections
G
1
=
∐
U
i
j
{\displaystyle {\mathcal {G}}_{1}=\coprod U_{ij}}
.
The source and target maps are then given by the induced maps
s
=
ϕ
j
:
U
i
j
→
U
j
t
=
ϕ
i
:
U
i
j
→
U
i
{\displaystyle {\begin{aligned}s=\phi _{j}:U_{ij}\to U_{j}\\t=\phi _{i}:U_{ij}\to U_{i}\end{aligned}}}
and the inclusion map
ε
:
U
i
→
U
i
i
{\displaystyle \varepsilon :U_{i}\to U_{ii}}
giving the structure of a groupoid. In fact, this can be further extended by setting
G
n
=
G
1
×
G
0
⋯
×
G
0
G
1
{\displaystyle {\mathcal {G}}_{n}={\mathcal {G}}_{1}\times _{{\mathcal {G}}_{0}}\cdots \times _{{\mathcal {G}}_{0}}{\mathcal {G}}_{1}}
as the
n
{\displaystyle n}
-iterated fiber product where the
G
n
{\displaystyle {\mathcal {G}}_{n}}
represents
n
{\displaystyle n}
-tuples of composable arrows. The structure map of the fiber product is implicitly the target map, since
U
i
j
k
→
U
i
j
↓
↓
U
i
k
→
U
i
{\displaystyle {\begin{matrix}U_{ijk}&\to &U_{ij}\\\downarrow &&\downarrow \\U_{ik}&\to &U_{i}\end{matrix}}}
is a cartesian diagram where the maps to
U
i
{\displaystyle U_{i}}
are the target maps. This construction can be seen as a model for some ∞-groupoids. Also, another artifact of this construction is k-cocycles
[
σ
]
∈
H
ˇ
k
(
U
,
A
_
)
{\displaystyle [\sigma ]\in {\check {H}}^{k}({\mathcal {U}},{\underline {A}})}
for some constant sheaf of abelian groups can be represented as a function
σ
:
∐
U
i
1
⋯
i
k
→
A
{\displaystyle \sigma :\coprod U_{i_{1}\cdots i_{k}}\to A}
giving an explicit representation of cohomology classes.
= Group action
=If the group
G
{\displaystyle G}
acts on the set
X
{\displaystyle X}
, then we can form the action groupoid (or transformation groupoid) representing this group action as follows:
The objects are the elements of
X
{\displaystyle X}
;
For any two elements
x
{\displaystyle x}
and
y
{\displaystyle y}
in
X
{\displaystyle X}
, the morphisms from
x
{\displaystyle x}
to
y
{\displaystyle y}
correspond to the elements
g
{\displaystyle g}
of
G
{\displaystyle G}
such that
g
x
=
y
{\displaystyle gx=y}
;
Composition of morphisms interprets the binary operation of
G
{\displaystyle G}
.
More explicitly, the action groupoid is a small category with
o
b
(
C
)
=
X
{\displaystyle \mathrm {ob} (C)=X}
and
h
o
m
(
C
)
=
G
×
X
{\displaystyle \mathrm {hom} (C)=G\times X}
and with source and target maps
s
(
g
,
x
)
=
x
{\displaystyle s(g,x)=x}
and
t
(
g
,
x
)
=
g
x
{\displaystyle t(g,x)=gx}
. It is often denoted
G
⋉
X
{\displaystyle G\ltimes X}
(or
X
⋊
G
{\displaystyle X\rtimes G}
for a right action). Multiplication (or composition) in the groupoid is then
(
h
,
y
)
(
g
,
x
)
=
(
h
g
,
x
)
{\displaystyle (h,y)(g,x)=(hg,x)}
which is defined provided
y
=
g
x
{\displaystyle y=gx}
.
For
x
{\displaystyle x}
in
X
{\displaystyle X}
, the vertex group consists of those
(
g
,
x
)
{\displaystyle (g,x)}
with
g
x
=
x
{\displaystyle gx=x}
, which is just the isotropy subgroup at
x
{\displaystyle x}
for the given action (which is why vertex groups are also called isotropy groups). Similarly, the orbits of the action groupoid are the orbit of the group action, and the groupoid is transitive if and only if the group action is transitive.
Another way to describe
G
{\displaystyle G}
-sets is the functor category
[
G
r
,
S
e
t
]
{\displaystyle [\mathrm {Gr} ,\mathrm {Set} ]}
, where
G
r
{\displaystyle \mathrm {Gr} }
is the groupoid (category) with one element and isomorphic to the group
G
{\displaystyle G}
. Indeed, every functor
F
{\displaystyle F}
of this category defines a set
X
=
F
(
G
r
)
{\displaystyle X=F(\mathrm {Gr} )}
and for every
g
{\displaystyle g}
in
G
{\displaystyle G}
(i.e. for every morphism in
G
r
{\displaystyle \mathrm {Gr} }
) induces a bijection
F
g
{\displaystyle F_{g}}
:
X
→
X
{\displaystyle X\to X}
. The categorical structure of the functor
F
{\displaystyle F}
assures us that
F
{\displaystyle F}
defines a
G
{\displaystyle G}
-action on the set
G
{\displaystyle G}
. The (unique) representable functor
F
{\displaystyle F}
:
G
r
→
S
e
t
{\displaystyle \mathrm {Gr} \to \mathrm {Set} }
is the Cayley representation of
G
{\displaystyle G}
. In fact, this functor is isomorphic to
H
o
m
(
G
r
,
−
)
{\displaystyle \mathrm {Hom} (\mathrm {Gr} ,-)}
and so sends
o
b
(
G
r
)
{\displaystyle \mathrm {ob} (\mathrm {Gr} )}
to the set
H
o
m
(
G
r
,
G
r
)
{\displaystyle \mathrm {Hom} (\mathrm {Gr} ,\mathrm {Gr} )}
which is by definition the "set"
G
{\displaystyle G}
and the morphism
g
{\displaystyle g}
of
G
r
{\displaystyle \mathrm {Gr} }
(i.e. the element
g
{\displaystyle g}
of
G
{\displaystyle G}
) to the permutation
F
g
{\displaystyle F_{g}}
of the set
G
{\displaystyle G}
. We deduce from the Yoneda embedding that the group
G
{\displaystyle G}
is isomorphic to the group
{
F
g
∣
g
∈
G
}
{\displaystyle \{F_{g}\mid g\in G\}}
, a subgroup of the group of permutations of
G
{\displaystyle G}
.
Finite set
Consider the group action of
Z
/
2
{\displaystyle \mathbb {Z} /2}
on the finite set
X
=
{
−
2
,
−
1
,
0
,
1
,
2
}
{\displaystyle X=\{-2,-1,0,1,2\}}
which takes each number to its negative, so
−
2
↦
2
{\displaystyle -2\mapsto 2}
and
1
↦
−
1
{\displaystyle 1\mapsto -1}
. The quotient groupoid
[
X
/
G
]
{\displaystyle [X/G]}
is the set of equivalence classes from this group action
{
[
0
]
,
[
1
]
,
[
2
]
}
{\displaystyle \{[0],[1],[2]\}}
, and
[
0
]
{\displaystyle [0]}
has a group action of
Z
/
2
{\displaystyle \mathbb {Z} /2}
on it.
Quotient variety
Any finite group
G
{\displaystyle G}
that maps to
G
L
(
n
)
{\displaystyle GL(n)}
gives a group action on the affine space
A
n
{\displaystyle \mathbb {A} ^{n}}
(since this is the group of automorphisms). Then, a quotient groupoid can be of the form
[
A
n
/
G
]
{\displaystyle [\mathbb {A} ^{n}/G]}
, which has one point with stabilizer
G
{\displaystyle G}
at the origin. Examples like these form the basis for the theory of orbifolds. Another commonly studied family of orbifolds are weighted projective spaces
P
(
n
1
,
…
,
n
k
)
{\displaystyle \mathbb {P} (n_{1},\ldots ,n_{k})}
and subspaces of them, such as Calabi–Yau orbifolds.
= Fiber product of groupoids
=Given a diagram of groupoids with groupoid morphisms
X
↓
Y
→
Z
{\displaystyle {\begin{aligned}&&X\\&&\downarrow \\Y&\rightarrow &Z\end{aligned}}}
where
f
:
X
→
Z
{\displaystyle f:X\to Z}
and
g
:
Y
→
Z
{\displaystyle g:Y\to Z}
, we can form the groupoid
X
×
Z
Y
{\displaystyle X\times _{Z}Y}
whose objects are triples
(
x
,
ϕ
,
y
)
{\displaystyle (x,\phi ,y)}
, where
x
∈
Ob
(
X
)
{\displaystyle x\in {\text{Ob}}(X)}
,
y
∈
Ob
(
Y
)
{\displaystyle y\in {\text{Ob}}(Y)}
, and
ϕ
:
f
(
x
)
→
g
(
y
)
{\displaystyle \phi :f(x)\to g(y)}
in
Z
{\displaystyle Z}
. Morphisms can be defined as a pair of morphisms
(
α
,
β
)
{\displaystyle (\alpha ,\beta )}
where
α
:
x
→
x
′
{\displaystyle \alpha :x\to x'}
and
β
:
y
→
y
′
{\displaystyle \beta :y\to y'}
such that for triples
(
x
,
ϕ
,
y
)
,
(
x
′
,
ϕ
′
,
y
′
)
{\displaystyle (x,\phi ,y),(x',\phi ',y')}
, there is a commutative diagram in
Z
{\displaystyle Z}
of
f
(
α
)
:
f
(
x
)
→
f
(
x
′
)
{\displaystyle f(\alpha ):f(x)\to f(x')}
,
g
(
β
)
:
g
(
y
)
→
g
(
y
′
)
{\displaystyle g(\beta ):g(y)\to g(y')}
and the
ϕ
,
ϕ
′
{\displaystyle \phi ,\phi '}
.
= Homological algebra
=A two term complex
C
1
→
d
C
0
{\displaystyle C_{1}{\overset {d}{\rightarrow }}C_{0}}
of objects in a concrete Abelian category can be used to form a groupoid. It has as objects the set
C
0
{\displaystyle C_{0}}
and as arrows the set
C
1
⊕
C
0
{\displaystyle C_{1}\oplus C_{0}}
; the source morphism is just the projection onto
C
0
{\displaystyle C_{0}}
while the target morphism is the addition of projection onto
C
1
{\displaystyle C_{1}}
composed with
d
{\displaystyle d}
and projection onto
C
0
{\displaystyle C_{0}}
. That is, given
c
1
+
c
0
∈
C
1
⊕
C
0
{\displaystyle c_{1}+c_{0}\in C_{1}\oplus C_{0}}
, we have
t
(
c
1
+
c
0
)
=
d
(
c
1
)
+
c
0
.
{\displaystyle t(c_{1}+c_{0})=d(c_{1})+c_{0}.}
Of course, if the abelian category is the category of coherent sheaves on a scheme, then this construction can be used to form a presheaf of groupoids.
= Puzzles
=While puzzles such as the Rubik's Cube can be modeled using group theory (see Rubik's Cube group), certain puzzles are better modeled as groupoids.
The transformations of the fifteen puzzle form a groupoid (not a group, as not all moves can be composed). This groupoid acts on configurations.
= Mathieu groupoid
=The Mathieu groupoid is a groupoid introduced by John Horton Conway acting on 13 points such that the elements fixing a point form a copy of the Mathieu group M12.
Relation to groups
If a groupoid has only one object, then the set of its morphisms forms a group. Using the algebraic definition, such a groupoid is literally just a group. Many concepts of group theory generalize to groupoids, with the notion of functor replacing that of group homomorphism.
Every transitive/connected groupoid - that is, as explained above, one in which any two objects are connected by at least one morphism - is isomorphic to an action groupoid (as defined above)
(
G
,
X
)
{\displaystyle (G,X)}
. By transitivity, there will only be one orbit under the action.
Note that the isomorphism just mentioned is not unique, and there is no natural choice. Choosing such an isomorphism for a transitive groupoid essentially amounts to picking one object
x
0
{\displaystyle x_{0}}
, a group isomorphism
h
{\displaystyle h}
from
G
(
x
0
)
{\displaystyle G(x_{0})}
to
G
{\displaystyle G}
, and for each
x
{\displaystyle x}
other than
x
0
{\displaystyle x_{0}}
, a morphism in
G
{\displaystyle G}
from
x
0
{\displaystyle x_{0}}
to
x
{\displaystyle x}
.
If a groupoid is not transitive, then it is isomorphic to a disjoint union of groupoids of the above type, also called its connected components (possibly with different groups
G
{\displaystyle G}
and sets
X
{\displaystyle X}
for each connected component).
In category-theoretic terms, each connected component of a groupoid is equivalent (but not isomorphic) to a groupoid with a single object, that is, a single group. Thus any groupoid is equivalent to a multiset of unrelated groups. In other words, for equivalence instead of isomorphism, one does not need to specify the sets
X
{\displaystyle X}
, but only the groups
G
.
{\displaystyle G.}
For example,
The fundamental groupoid of
X
{\displaystyle X}
is equivalent to the collection of the fundamental groups of each path-connected component of
X
{\displaystyle X}
, but an isomorphism requires specifying the set of points in each component;
The set
X
{\displaystyle X}
with the equivalence relation
∼
{\displaystyle \sim }
is equivalent (as a groupoid) to one copy of the trivial group for each equivalence class, but an isomorphism requires specifying what each equivalence class is:
The set
X
{\displaystyle X}
equipped with an action of the group
G
{\displaystyle G}
is equivalent (as a groupoid) to one copy of
G
{\displaystyle G}
for each orbit of the action, but an isomorphism requires specifying what set each orbit is.
The collapse of a groupoid into a mere collection of groups loses some information, even from a category-theoretic point of view, because it is not natural. Thus when groupoids arise in terms of other structures, as in the above examples, it can be helpful to maintain the entire groupoid. Otherwise, one must choose a way to view each
G
(
x
)
{\displaystyle G(x)}
in terms of a single group, and this choice can be arbitrary. In the example from topology, one would have to make a coherent choice of paths (or equivalence classes of paths) from each point
p
{\displaystyle p}
to each point
q
{\displaystyle q}
in the same path-connected component.
As a more illuminating example, the classification of groupoids with one endomorphism does not reduce to purely group theoretic considerations. This is analogous to the fact that the classification of vector spaces with one endomorphism is nontrivial.
Morphisms of groupoids come in more kinds than those of groups: we have, for example, fibrations, covering morphisms, universal morphisms, and quotient morphisms. Thus a subgroup
H
{\displaystyle H}
of a group
G
{\displaystyle G}
yields an action of
G
{\displaystyle G}
on the set of cosets of
H
{\displaystyle H}
in
G
{\displaystyle G}
and hence a covering morphism
p
{\displaystyle p}
from, say,
K
{\displaystyle K}
to
G
{\displaystyle G}
, where
K
{\displaystyle K}
is a groupoid with vertex groups isomorphic to
H
{\displaystyle H}
. In this way, presentations of the group
G
{\displaystyle G}
can be "lifted" to presentations of the groupoid
K
{\displaystyle K}
, and this is a useful way of obtaining information about presentations of the subgroup
H
{\displaystyle H}
. For further information, see the books by Higgins and by Brown in the References.
Category of groupoids
The category whose objects are groupoids and whose morphisms are groupoid morphisms is called the groupoid category, or the category of groupoids, and is denoted by Grpd.
The category Grpd is, like the category of small categories, Cartesian closed: for any groupoids
H
,
K
{\displaystyle H,K}
we can construct a groupoid
GPD
(
H
,
K
)
{\displaystyle \operatorname {GPD} (H,K)}
whose objects are the morphisms
H
→
K
{\displaystyle H\to K}
and whose arrows are the natural equivalences of morphisms. Thus if
H
,
K
{\displaystyle H,K}
are just groups, then such arrows are the conjugacies of morphisms. The main result is that for any groupoids
G
,
H
,
K
{\displaystyle G,H,K}
there is a natural bijection
Grpd
(
G
×
H
,
K
)
≅
Grpd
(
G
,
GPD
(
H
,
K
)
)
.
{\displaystyle \operatorname {Grpd} (G\times H,K)\cong \operatorname {Grpd} (G,\operatorname {GPD} (H,K)).}
This result is of interest even if all the groupoids
G
,
H
,
K
{\displaystyle G,H,K}
are just groups.
Another important property of Grpd is that it is both complete and cocomplete.
= Relation to Cat
=The inclusion
i
:
G
r
p
d
→
C
a
t
{\displaystyle i:\mathbf {Grpd} \to \mathbf {Cat} }
has both a left and a right adjoint:
hom
G
r
p
d
(
C
[
C
−
1
]
,
G
)
≅
hom
C
a
t
(
C
,
i
(
G
)
)
{\displaystyle \hom _{\mathbf {Grpd} }(C[C^{-1}],G)\cong \hom _{\mathbf {Cat} }(C,i(G))}
hom
C
a
t
(
i
(
G
)
,
C
)
≅
hom
G
r
p
d
(
G
,
C
o
r
e
(
C
)
)
{\displaystyle \hom _{\mathbf {Cat} }(i(G),C)\cong \hom _{\mathbf {Grpd} }(G,\mathrm {Core} (C))}
Here,
C
[
C
−
1
]
{\displaystyle C[C^{-1}]}
denotes the localization of a category that inverts every morphism, and
C
o
r
e
(
C
)
{\displaystyle \mathrm {Core} (C)}
denotes the subcategory of all isomorphisms.
= Relation to sSet
=The nerve functor
N
:
G
r
p
d
→
s
S
e
t
{\displaystyle N:\mathbf {Grpd} \to \mathbf {sSet} }
embeds Grpd as a full subcategory of the category of simplicial sets. The nerve of a groupoid is always a Kan complex.
The nerve has a left adjoint
hom
G
r
p
d
(
π
1
(
X
)
,
G
)
≅
hom
s
S
e
t
(
X
,
N
(
G
)
)
{\displaystyle \hom _{\mathbf {Grpd} }(\pi _{1}(X),G)\cong \hom _{\mathbf {sSet} }(X,N(G))}
Here,
π
1
(
X
)
{\displaystyle \pi _{1}(X)}
denotes the fundamental groupoid of the simplicial set X.
= Groupoids in Grpd
=There is an additional structure which can be derived from groupoids internal to the category of groupoids, double-groupoids. Because Grpd is a 2-category, these objects form a 2-category instead of a 1-category since there is extra structure. Essentially, these are groupoids
G
1
,
G
0
{\displaystyle {\mathcal {G}}_{1},{\mathcal {G}}_{0}}
with functors
s
,
t
:
G
1
→
G
0
{\displaystyle s,t:{\mathcal {G}}_{1}\to {\mathcal {G}}_{0}}
and an embedding given by an identity functor
i
:
G
0
→
G
1
{\displaystyle i:{\mathcal {G}}_{0}\to {\mathcal {G}}_{1}}
One way to think about these 2-groupoids is they contain objects, morphisms, and squares which can compose together vertically and horizontally. For example, given squares
∙
→
∙
↓
↓
∙
→
a
∙
{\displaystyle {\begin{matrix}\bullet &\to &\bullet \\\downarrow &&\downarrow \\\bullet &\xrightarrow {a} &\bullet \end{matrix}}}
and
∙
→
a
∙
↓
↓
∙
→
∙
{\displaystyle {\begin{matrix}\bullet &\xrightarrow {a} &\bullet \\\downarrow &&\downarrow \\\bullet &\to &\bullet \end{matrix}}}
with
a
{\displaystyle a}
the same morphism, they can be vertically conjoined giving a diagram
∙
→
∙
↓
↓
∙
→
a
∙
↓
↓
∙
→
∙
{\displaystyle {\begin{matrix}\bullet &\to &\bullet \\\downarrow &&\downarrow \\\bullet &\xrightarrow {a} &\bullet \\\downarrow &&\downarrow \\\bullet &\to &\bullet \end{matrix}}}
which can be converted into another square by composing the vertical arrows. There is a similar composition law for horizontal attachments of squares.
Groupoids with geometric structures
When studying geometrical objects, the arising groupoids often carry a topology, turning them into topological groupoids, or even some differentiable structure, turning them into Lie groupoids. These last objects can be also studied in terms of their associated Lie algebroids, in analogy to the relation between Lie groups and Lie algebras.
Groupoids arising from geometry often possess further structures which interact with the groupoid multiplication. For instance, in Poisson geometry one has the notion of a symplectic groupoid, which is a Lie groupoid endowed with a compatible symplectic form. Similarly, one can have groupoids with a compatible Riemannian metric, or complex structure, etc.
See also
∞-groupoid
2-group
Homotopy type theory
Inverse category
Groupoid algebra (not to be confused with algebraic groupoid)
R-algebroid
Notes
References
Brandt, H (1927), "Über eine Verallgemeinerung des Gruppenbegriffes", Mathematische Annalen, 96 (1): 360–366, doi:10.1007/BF01209171, S2CID 119597988
Brown, Ronald, 1987, "From groups to groupoids: a brief survey," Bull. London Math. Soc. 19: 113–34. Reviews the history of groupoids up to 1987, starting with the work of Brandt on quadratic forms. The downloadable version updates the many references.
—, 2006. Topology and groupoids. Booksurge. Revised and extended edition of a book previously published in 1968 and 1988. Groupoids are introduced in the context of their topological application.
—, Higher dimensional group theory. Explains how the groupoid concept has led to higher-dimensional homotopy groupoids, having applications in homotopy theory and in group cohomology. Many references.
Dicks, Warren; Ventura, Enric (1996), The group fixed by a family of injective endomorphisms of a free group, Mathematical Surveys and Monographs, vol. 195, AMS Bookstore, ISBN 978-0-8218-0564-0
Dokuchaev, M.; Exel, R.; Piccione, P. (2000). "Partial Representations and Partial Group Algebras". Journal of Algebra. 226. Elsevier: 505–532. arXiv:math/9903129. doi:10.1006/jabr.1999.8204. ISSN 0021-8693. S2CID 14622598.
F. Borceux, G. Janelidze, 2001, Galois theories. Cambridge Univ. Press. Shows how generalisations of Galois theory lead to Galois groupoids.
Cannas da Silva, A., and A. Weinstein, Geometric Models for Noncommutative Algebras. Especially Part VI.
Golubitsky, M., Ian Stewart, 2006, "Nonlinear dynamics of networks: the groupoid formalism", Bull. Amer. Math. Soc. 43: 305–64
"Groupoid", Encyclopedia of Mathematics, EMS Press, 2001 [1994]
Higgins, P. J., "The fundamental groupoid of a graph of groups", J. London Math. Soc. (2) 13 (1976) 145–149.
Higgins, P. J. and Taylor, J., "The fundamental groupoid and the homotopy crossed complex of an orbit space", in Category theory (Gummersbach, 1981), Lecture Notes in Math., Volume 962. Springer, Berlin (1982), 115–122.
Higgins, P. J., 1971. Categories and groupoids. Van Nostrand Notes in Mathematics. Republished in Reprints in Theory and Applications of Categories, No. 7 (2005) pp. 1–195; freely downloadable. Substantial introduction to category theory with special emphasis on groupoids. Presents applications of groupoids in group theory, for example to a generalisation of Grushko's theorem, and in topology, e.g. fundamental groupoid.
Mackenzie, K. C. H., 2005. General theory of Lie groupoids and Lie algebroids. Cambridge Univ. Press.
Weinstein, Alan, "Groupoids: unifying internal and external symmetry — A tour through some examples." Also available in Postscript., Notices of the AMS, July 1996, pp. 744–752.
Weinstein, Alan, "The Geometry of Momentum" (2002)
R.T. Zivaljevic. "Groupoids in combinatorics—applications of a theory of local symmetries". In Algebraic and geometric combinatorics, volume 423 of Contemp. Math., 305–324. Amer. Math. Soc., Providence, RI (2006)
fundamental groupoid at the nLab
core at the nLab
Kata Kunci Pencarian:
- Simetri
- Grupoid
- Magma (aljabar)
- Teori grup
- Kategori (matematika)
- Grup automorfisme
- Grup bebas
- Grup dasar
- Tindakan grup (matematika)
- Groupoid
- Lie groupoid
- ∞-groupoid
- Fundamental groupoid
- Magma (algebra)
- Double groupoid
- Partial groupoid
- Lie algebroid
- Central groupoid
- Mathieu groupoid
