In topology, a branch of mathematics, the clutching construction is a way of constructing fiber bundles, particularly vector bundles on spheres.
Consider the sphere
Sn
n | |
D | |
+ |
n | |
D | |
- |
Sn-1
Given trivialized fiber bundles with fiber
F
G
f\colonSn-1\toG
Formally, it is the coequalizer of the inclusions
Sn-1 x F\to
n | |
D | |
+ |
x F\coprod
n | |
D | |
- |
x F
(x,v)\mapsto(x,v)\in
n | |
D | |
+ |
x F
(x,v)\mapsto(x,f(x)(v))\in
n | |
D | |
- |
x F
Thus we have a map
\pin-1G\to
n) | |
Fib | |
F(S |
In the case of vector bundles, this yields
\pin-1O(k)\to
n) | |
Vect | |
k(S |
The above can be generalized by replacing
n | |
D | |
\pm |
Sn
(X;A,B)
A\capB
Let
p\colonM\toN
F
lU
(Ui,qi)
qi\colonp-1(Ui)\toN x F
p
Ui\subsetN
Ui
N
\coprodiUi=N
Consider the space
\coprodiUi x F
(ui,fi)\inUi x F
(uj,fj)\inUj x F
Ui\capUj ≠ \phi
qi\circ
-1 | |
q | |
j |
(uj,fj)=(ui,fi)
qi
p
Consider the space
\coprodiUi x \operatorname{Homeo}(F)
(ui,hi)\inUi x \operatorname{Homeo}(F)
(uj,hj)\inUj x \operatorname{Homeo}(F)
Ui\capUj ≠ \phi
qi\circ
-1 | |
q | |
j |
qi\circ
-1 | |
q | |
j |
:Ui\capUj\to\operatorname{Homeo}(F)
qi\circ
-1 | |
q | |
j |
(uj)(hj)=hi
p
F
\operatorname{Homeo}(F)
\operatorname{Homeo}(F)
N
\operatorname{Homeo}(F)
p\colonMp\toN
(Mp x F)/\operatorname{Homeo}(F)=M
So we have a principal bundle
\operatorname{Homeo}(F)\toMp\toN
Mp\toN\toB(\operatorname{Homeo}(F))
B(\operatorname{Homeo}(F))
\operatorname{Homeo}(F)
Given a
G
G\toMp\toN
Mp x GEG
1) Project onto the first factor:
Mp x GEG\toMp/G=N
EG
2) Project onto the second factor:
Mp x GEG\toEG/G=BG
Mp
Thus we have a fibration
Mp\toN\simeqMp x GEG\toBG
p\colonM\toN
G\toMp\toN
G\toEG\toBG
p
See also: Twisted sphere. Twisted spheres are sometimes referred to as a "clutching-type" construction, but this is misleading: the clutching construction is properly about fiber bundles.
Sn-1\toSn-1
Sn-1\toG
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
\pi3.
Similar constructions can be found for various instantons, including the Wess–Zumino–Witten model.