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topology In mathematics, topology (from the Greek language, Greek words , and ) is concerned with the properties of a mathematical object, geometric object that are preserved under Continuous function, continuous Deformation theory, deformations, such ...
, a branch of mathematics, the clutching construction is a way of constructing fiber bundles, particularly vector bundles on spheres.


Definition

Consider the sphere S^n as the union of the upper and lower hemispheres D^n_+ and D^n_- along their intersection, the equator, an S^. Given trivialized
fiber bundle In mathematics, and particularly topology, a fiber bundle (or, in Commonwealth English: fibre bundle) is a space that is a product space, but may have a different topological structure. Specifically, the similarity between a space E and a p ...
s with fiber F and structure group G over the two hemispheres, then given a map f\colon S^ \to G (called the ''clutching map''), glue the two trivial bundles together via ''f''. Formally, it is the
coequalizer In category theory, a coequalizer (or coequaliser) is a generalization of a quotient by an equivalence relation to objects in an arbitrary category. It is the categorical construction dual to the equalizer. Definition A coequalizer is a co ...
of the inclusions S^ \times F \to D^n_+ \times F \coprod D^n_- \times F via (x,v) \mapsto (x,v) \in D^n_+ \times F and (x,v) \mapsto (x,f(x)(v)) \in D^n_- \times F: glue the two bundles together on the boundary, with a twist. Thus we have a map \pi_ G \to \text_F(S^n): clutching information on the equator yields a fiber bundle on the total space. In the case of vector bundles, this yields \pi_ O(k) \to \text_k(S^n), 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_\pm and S^n 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 \cap B gives a vector bundle on ''X''.


Classifying map construction

Let p \colon M \to N be a fibre bundle with fibre F. Let \mathcal U be a collection of pairs (U_i,q_i) such that q_i \colon p^(U_i) \to N \times F is a local trivialization of p over U_i \subset N. Moreover, we demand that the union of all the sets U_i is N (i.e. the collection is an atlas of trivializations \coprod_i U_i = N). Consider the space \coprod_i U_i\times F modulo the equivalence relation (u_i,f_i)\in U_i \times F is equivalent to (u_j,f_j)\in U_j \times F if and only if U_i \cap U_j \neq \phi and q_i \circ q_j^(u_j,f_j) = (u_i,f_i). By design, the local trivializations q_i give a fibrewise equivalence between this quotient space and the fibre bundle p. Consider the space \coprod_i U_i\times \operatorname(F) modulo the equivalence relation (u_i,h_i)\in U_i \times \operatorname(F) is equivalent to (u_j,h_j)\in U_j \times \operatorname(F) if and only if U_i \cap U_j \neq \phi and consider q_i \circ q_j^ to be a map q_i \circ q_j^ : U_i \cap U_j \to \operatorname(F) then we demand that q_i \circ q_j^(u_j)(h_j)=h_i. That is, in our re-construction of p we are replacing the fibre F by the topological group of homeomorphisms of the fibre, \operatorname(F). If the structure group of the bundle is known to reduce, you could replace \operatorname(F) with the reduced structure group. This is a bundle over N with fibre \operatorname(F) and is a principal bundle. Denote it by p \colon M_p \to N. The relation to the previous bundle is induced from the principal bundle: (M_p \times F)/\operatorname(F) = M. So we have a principal bundle \operatorname(F) \to M_p \to N. The theory of classifying spaces gives us an induced push-forward fibration M_p \to N \to B(\operatorname(F)) where B(Homeo(F)) is the classifying space of \operatorname(F). Here is an outline: Given a G-principal bundle G \to M_p \to N, consider the space M_p \times_ EG. This space is a fibration in two different ways: 1) Project onto the first factor: M_p \times_G EG \to M_p/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: M_p \times_G EG \to EG/G = BG. The fibre in this case is M_p. Thus we have a fibration M_p \to N \simeq M_p\times_G EG \to BG. This map is called the classifying map of the fibre bundle p \colon M \to N since 1) the principal bundle G \to M_p \to N is the pull-back of the bundle G \to EG \to 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 S^ \to S^: 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 S^ \to G: the gluing is trivial in the base, but not in the fibers.


Examples

The clutching construction is used to form the
chiral anomaly In theoretical physics, a chiral anomaly is the anomalous nonconservation of a chiral current. In everyday terms, it is equivalent to a sealed box that contained equal numbers of left and right-handed bolts, but when opened was found to have mor ...
, 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 \pi_3.) Similar constructions can be found for various
instanton An instanton (or pseudoparticle) is a notion appearing in theoretical and mathematical physics. An instanton is a classical solution to equations of motion with a finite, non-zero action, either in quantum mechanics or in quantum field theory. Mo ...
s, including the
Wess–Zumino–Witten model In theoretical physics and mathematics, a Wess–Zumino–Witten (WZW) model, also called a Wess–Zumino–Novikov–Witten model, is a type of two-dimensional conformal field theory named after Julius Wess, Bruno Zumino, Sergei Novikov and Edwa ...
.


See also

*
Alexander trick Alexander's trick, also known as the Alexander trick, is a basic result in geometric topology, named after J. W. Alexander. Statement Two homeomorphisms of the ''n''-dimensional ball D^n which agree on the boundary sphere S^ are isotopic. Mo ...


References

*
Allen Hatcher Allen, Allen's or Allens may refer to: Buildings * Allen Arena, an indoor arena at Lipscomb University in Nashville, Tennessee * Allen Center, a skyscraper complex in downtown Houston, Texas * Allen Fieldhouse, an indoor sports arena on the Univer ...
's book-in-progres
Vector Bundles & K-Theory
version 2.0, p. 22. {{DEFAULTSORT:Clutching Construction Topology Geometric topology Differential topology Differential structures