Hopf invariant
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In mathematics, in particular in algebraic topology, the Hopf invariant is a homotopy invariant of certain maps between spheres.
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[edit] Motivation
In 1931 Heinz Hopf used Clifford parallels to construct the Hopf map , and proved that η is essential, i.e. not homotopic to the constant map. It was later shown that η generates the homotopy group π3(S2). In 1951, Serre proved that the rational homotopy groups for an odd-dimensional sphere (n odd) are zero unless i = 0,n. However, for an even-dimensional sphere (n even), there is one more bit of infinite cyclic homotopy in degree 2n − 1. There is an interesting way of seeing this:
[edit] Definition
Let be a continuous map (and probably n > 1 for non-triviality). Then we can form the cell complex
where D2n is a 2n-dimensional disc attached to Sn via φ. The cellular chain groups are just freely generated on the n-cells in degree n, so they are in degree 0, n and 2n and zero everywhere else. Cellular (co-)homology is the (co-)homology of this chain complex, and since all boundary homomorphisms must be zero, the cohomology is
Denote the generators of the cohomology groups by
- and
For dimensional reasons, all cuppings between those classes must be trivial apart from . Thus, as a ring, the cohomology is
The number h(φ) is the Hopf invariant of the map φ.
[edit] Properties
Theorem: is a homomorphism. Moreover, if n is even, h maps onto .
The Hopf invariant is 1 for the Hopf maps (where n = 1,2,4,8, corresponding to the real division algebras , respectively, and to the double cover sending a direction on the sphere to the subspace it spans). It is a theorem, proved first by Frank Adams and subsequently by Michael Atiyah with methods of K-theory, that these are the only maps with Hopf invariant 1.
[edit] Generalisations for stable maps
A very general notion of the Hopf invariant can be defined, but it requires a certain amount of homotopy theoretic groundwork:
Let V denote a vector space and its one-point compactification, i.e. and for some k. If (X,x0) is any pointed space (as it is implicitly in the previous section), and if we take the point at infinity to be the basepoint of , then we can form the wedge products .
Now let be a stable map, i.e. stable under the reduced suspension functor. The (stable) geometric Hopf invariant of F is
,
an element of the stable -equivariant homotopy group of maps from X to . Here "stable" means "stable under suspension", i.e. the direct limit over V (or k, if you will) of the ordinary, equivariant homotopy groups; and the -action is the trivial action on X and the flipping of the two factors on . If we let denote the canonical diagonal map and I the identity, then the Hopf invariant is defined by the following:
This map is initially a map from to , but under the direct limit it becomes the advertised element of the stable homotopy -equivariant group of maps.
There exists also an unstable version of the Hopf invariant hV(F), for which one must keep track of the vector space V.
[edit] References
- H. Hopf (1931). "Über die Abbildungen der dreidimensionalen Sphäre auf die Kugeloberfläche". Math. Ann. 104: 637-665.
- J.F. Adams (1960). "On the non-existence of elements of Hopf invariant one". Ann. Math. 72: 20-104.
- J.F. Adams, M.F. Atiyah (1966). "K-Theory and the Hopf Invariant". The Quarterly Journal of Mathematics 17 (1): 31-38.
- M. Crabb, A. Ranicki (2006). "The geometric Hopf invariant". http://www.maths.ed.ac.uk/~aar/slides/hopfbeam.pdf.