Clutching construction

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Short description: Topological construct

In topology, a branch of mathematics, the clutching construction is a way of constructing fiber bundles, particularly vector bundles on spheres.

Definition

Consider the sphere Sn as the union of the upper and lower hemispheres D+n and D−n along their intersection, the equator, an Sn−1.

Given trivialized fiber bundles with fiber F and structure group G over the two hemispheres, then given a map f:Sn−1→G (called the clutching map), glue the two trivial bundles together via f.

Formally, it is the coequalizer of the inclusions Sn−1×F→D+n×F∐D−n×F via (x,v)↦(x,v)∈D+n×F and (x,v)↦(x,f(x)(v))∈D−n×F: glue the two bundles together on the boundary, with a twist.

Thus we have a map πn−1G→FibF(Sn): clutching information on the equator yields a fiber bundle on the total space.

In the case of vector bundles, this yields πn−1O(k)→Vectk(Sn), and indeed this map is an isomorphism (under connect sum of spheres on the right).

Generalization

The above can be generalized by replacing D±n and Sn with any closed triad (X;A,B), that is, a space X, together with two closed subsets A and B whose union is X. Then a clutching map on A∩B gives a vector bundle on X.

Classifying map construction

Let p:M→N be a fibre bundle with fibre F. Let 𝒰 be a collection of pairs (Ui,qi) such that qi:p−1(Ui)→N×F is a local trivialization of p over Ui⊂N. Moreover, we demand that the union of all the sets Ui is N (i.e. the collection is an atlas of trivializations ∐iUi=N).

Consider the space ∐iUi×F modulo the equivalence relation (ui,fi)∈Ui×F is equivalent to (uj,fj)∈Uj×F if and only if Ui∩Uj≠∅ and qi∘qj−1(uj,fj)=(ui,fi). By design, the local trivializations qi give a fibrewise equivalence between this quotient space and the fibre bundle p.

Consider the space ∐iUi×Homeo⁡(F) modulo the equivalence relation (ui,hi)∈Ui×Homeo⁡(F) is equivalent to (uj,hj)∈Uj×Homeo⁡(F) if and only if Ui∩Uj≠∅ and consider qi∘qj−1 to be a map qi∘qj−1:Ui∩Uj→Homeo⁡(F) then we demand that qi∘qj−1(uj)(hj)=hi. That is, in our re-construction of p we are replacing the fibre F by the topological group of homeomorphisms of the fibre, Homeo⁡(F). If the structure group of the bundle is known to reduce, you could replace Homeo⁡(F) with the reduced structure group. This is a bundle over N with fibre Homeo⁡(F) and is a principal bundle. Denote it by p:Mp→N. The relation to the previous bundle is induced from the principal bundle: (Mp×F)/Homeo⁡(F)=M.

So we have a principal bundle Homeo⁡(F)→Mp→N. The theory of classifying spaces gives us an induced push-forward fibration Mp→N→B(Homeo⁡(F)) where B(Homeo⁡(F)) is the classifying space of Homeo⁡(F). Here is an outline:

Given a G-principal bundle G→Mp→N, consider the space Mp×GEG. This space is a fibration in two different ways:

1) Project onto the first factor: Mp×GEG→Mp/G=N. The fibre in this case is EG, which is a contractible space by the definition of a classifying space.

2) Project onto the second factor: Mp×GEG→EG/G=BG. The fibre in this case is Mp.

Thus we have a fibration Mp→N≃Mp×GEG→BG. This map is called the classifying map of the fibre bundle p:M→N since 1) the principal bundle G→Mp→N is the pull-back of the bundle G→EG→BG along the classifying map and 2) The bundle p is induced from the principal bundle as above.

Contrast with twisted spheres

Twisted spheres are sometimes referred to as a "clutching-type" construction, but this is misleading: the clutching construction is properly about fiber bundles.

  • In twisted spheres, you glue two halves along their boundary. The halves are a priori identified (with the standard ball), and points on the boundary sphere do not in general go to their corresponding points on the other boundary sphere. This is a map Sn−1→Sn−1: the gluing is non-trivial in the base.
  • In the clutching construction, you glue two bundles together over the boundary of their base hemispheres. The boundary spheres are glued together via the standard identification: each point goes to the corresponding one, but each fiber has a twist. This is a map Sn−1→G: the gluing is trivial in the base, but not in the fibers.

Examples

The clutching construction is used to form the chiral anomaly, by gluing together a pair of self-dual curvature forms. Such forms are locally exact on each hemisphere, as they are differentials of the Chern–Simons 3-form; by gluing them together, the curvature form is no longer globally exact (and so has a non-trivial homotopy group π3.)

Similar constructions can be found for various instantons, including the Wess–Zumino–Witten model.[1]

See also

  • Alexander trick

References

  1. ↑ Yao, Yuan; Hsieh, Chang-Tse; Oshikawa, Masaki (2019). "Anomaly Matching and Symmetry-Protected Critical Phases in SU(N) Spin Systems in 1+1 Dimensions". Physical Review Letters 123 (18). doi:10.1103/PhysRevLett.123.180201. PMID 31763914. 
  • clutching construction on nLab