Clutching construction

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Template:Short description 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 Dn along their intersection, the equator, an Sn1.

Given trivialized fiber bundles with fiber F and structure group G over the two hemispheres, then given a map f:Sn1G (called the clutching map), glue the two trivial bundles together via f.

Formally, it is the coequalizer of the inclusions Sn1×FD+n×FDn×F via (x,v)(x,v)D+n×F and (x,v)(x,f(x)(v))Dn×F: glue the two bundles together on the boundary, with a twist.

Thus we have a map πn1GFibF(Sn): clutching information on the equator yields a fiber bundle on the total space.

In the case of vector bundles, this yields πn1O(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 AB gives a vector bundle on X.

Classifying map construction

Let p:MN be a fibre bundle with fibre F. Let 𝒰 be a collection of pairs (Ui,qi) such that qi:p1(Ui)N×F is a local trivialization of p over UiN. 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 UiUjϕ and qiqj1(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 UiUjϕ and consider qiqj1 to be a map qiqj1:UiUjHomeo(F) then we demand that qiqj1(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:MpN. 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)MpN. The theory of classifying spaces gives us an induced push-forward fibration MpNB(Homeo(F)) where B(Homeo(F)) is the classifying space of Homeo(F). Here is an outline:

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

1) Project onto the first factor: Mp×GEGMp/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×GEGEG/G=BG. The fibre in this case is Mp.

Thus we have a fibration MpNMp×GEGBG. This map is called the classifying map of the fibre bundle p:MN since 1) the principal bundle GMpN is the pull-back of the bundle GEGBG along the classifying map and 2) The bundle p is induced from the principal bundle as above.

Contrast with twisted spheres

Template:See also 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 Sn1Sn1: 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 Sn1G: 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.

See also

References