The fundamental groupoid of a space is a groupoid whose objects are the points of and whose morphisms are paths in , identified up to endpoint-preserving homotopy.
In parts of the literature the fundamental groupoid, and more generally the fundamental ∞-groupoid, is called the Poincaré groupoid.
The fundamental groupoid of a topological space is the groupoid whose set of objects is and whose morphisms from to are the equivalence classes of homotopy of homotopy relative to of continuous maps whose endpoints map to and (which the homotopies are required to fix). Composition is by concatenation (and reparametrization) of representative maps. Under the homotopy-equivalence relation this becomes an associative and unital composition with respect to which every morphism has an inverse; hence is a groupoid.
The use of the fundamental groupoid of a manifold for describing the monodromy principle on the extension of local morphisms is discussed in the paper by Brown/Mucuk listed below.
For any in the first homotopy group of based at arises as the automorphism group of in :
So the fundamental groupoid gets rid of the choice of basepoint for the fundamental group, and this is valuable for some applications. The set of connected components of is precisely the set of path-components of . (This is not to be confused with the set of connected components of , sometimes denoted by the same symbol. Of course they are the same when is locally path-connected.)
The fundamental groupoid can be made into a topological groupoid (i.e. a groupoid internal to Top) when is path-connected, locally path-connected and semi-locally simply connected. This is a special case of (Brown 06, 10.5.8). This construction is closely linked with the construction of a universal covering space for a path-connected pointed space. The object space of this groupoid is just the space .
When is not semi-locally simply connected, the set of arrows of the fundamental groupoid inherits the quotient topology from the path space such that the fibres of are not discrete, which is an obstruction to the above-mentioned source fibre's being a covering space. However the composition is no longer continuous. When is not locally path-connected, also inherits a non-discrete topology (the quotient topology of by the relation of path connections).
In circumstances like these more sophisticated methods are appropriate, such as shape theory. This is also related to the fundamental group of a topos, which is in general a progroup or a localic group rather than an ordinary group.
An improvement on the fundamental group and the total fundamental groupoid relevant to the van Kampen theorem for computing the fundamental group or groupoid is to use , defined for a set to be the full subgroupoid of on the set , thus giving a set of base points which can be chosen according to the geometry at hand. Thus if is the union of two open sets with intersection then we can take large enough to meet each path-component of ; note that by the above definition we can write , etc. If has an action of a group then acts on if is a union of orbits of the action. Thus can represent some symmetry of a given situation.
The notion of was introduced in 1967 by Ronnie Brown to give a version of the Seifert-van Kampen Theorem which allowed the determination of the fundamental group of a connected space which is the union of connected subspaces with nonconnected intersection, such as the circle, a space which is, after all, THE basic example in topology.
Grothendieck writes in his 1984 Esquisse d'un Programme? (English translation):
“ ..,people still obstinately persist, when calculating with fundamental groups, in fixing a single base point, instead of cleverly choosing a whole packet of points which is invariant under the symmetries of the situation, which thus get lost on the way. In certain situations (such as descent theorems for fundamental groups `a la van Kampen) it is much more elegant, even indispensable for understanding something, to work with fundamental groupoids with respect to a suitable packet of base points,..”.
Notice that recovers the full fundamental groupoid, while is simply the fundamental group .
Basically, allows for the computation of homotopy 1-types; the theory was developed in Elements of Modern Topology (1968), now available as Topology and Groupoids (2006). These accounts show the use of the algebra of groupoids in 1-dimensional homotopy theory, for example for covering spaces, and, in the later edition, for orbit spaces. spring
See simplicial fundamental groupoid.
A detailed treatment is available in
Monograph:
Review and Exposition:
Jesper Møller, The fundamental group and covering spaces (2011) [arXiv:1106.5650, pdf, pdf]
Alberto Santini, Topological groupoids (2011) [pdf, pdf]
(about groupoids in topology, notably fundamental groupoids – not about topological groupoids)
See also:
R. Brown, Groupoids and Van Kampen’s theorem, Proc. London Math. Soc. (3) 17 (1967) 385-401.
R. Brown and G. Danesh-Naruie, The fundamental groupoid as a topological groupoid, Proc. Edinburgh Math. Soc. 19 (1975) 237-244.
R. Brown and O. Mucuk, The monodromy groupoid of a Lie groupoid, Cah. Top. G'eom. Diff. Cat. 36 (1995) 345-369.
Ronnie Brown, Topology and Groupoids, Booksurge (2006). (See particularly 10.5.8, using lifted topologies to topologise where is a normal, totally disconnected subgroupoid of , and admits a universal cover). (more info)
Discussion from the point of view of Galois theory is in
Luis Javier Hernández-Paricio, Fundamental pro-groupoids and covering projections, Fund. Math. (1998), (pdf)
The use of many base points is discussed at this (mathoverflow page).
Discussion of the fundamental groupoid (for good topological spaces and for noetherian schemes) as the costack? (via the Seifert-van Kampen theorem) characterized as being 2-terminal is in
Ilia Pirashvili, The fundamental groupoid as a terminal costack (arXiv:1406.4419)
Ilia Pirashvili, The Étale Fundamental Groupoid as a Terminal Costack (arXiv:1412.5473)
Discussion in the context of dynamical systems:
Last revised on November 18, 2023 at 05:19:02. See the history of this page for a list of all contributions to it.