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Hopf invariant

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[edit] Motivation

The rational homotopy

\pi_i(S^n) \otimes \mathbb{Q}

of an odd sphere (n odd) is zero unless i = 0,n. However, for an even 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 \phi \colon S^{2n-1} \to S^n be a continuous map (and probably n > 1 for non-triviality). Then we can form the cell complex

C_\phi = S^n \cup_\phi D^{2n},

where D2n is a 2n-dimensional disc attached to Sn via φ. The cellular chain groups C^*_\mathrm{cell}(C_\phi) are just freely generated on the n-cells in degree n, so they are \mathbb{Z} 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

H^i_\mathrm{cell}(C_\phi) = \begin{cases} \mathbb{Z} & i=0,n,2n, \\ 0 & \mbox{otherwise}. \end{cases}

Denote the generators of the cohomology groups by

H^n(C_\phi) = \langle\alpha\rangle and H^{2n}(C_\phi) = \langle\beta\rangle.

For dimensional reasons, all cuppings between those classes must be trivial apart from \alpha \smile \alpha. Thus, as a ring, the cohomology is

H^*(C_\phi) = \mathbb{Z}[\alpha,\beta]/\langle \beta\smile\beta = \alpha\smile\beta = 0, \alpha\smile\alpha=h(\phi)\beta\rangle.

The number h(φ) is the Hopf invariant of the map φ.

[edit] Properties

Theorem: h\colon\pi_{2n-1}(S^n)\to\mathbb{Z} is a homomorphism. Moreover, if n is even, h maps onto 2\mathbb{Z}.

The Hopf invariant is 1 for the Hopf maps (where n = 1,2,4,8, corresponding to the real division algebras \mathbb{A}=\mathbb{R},\mathbb{C},\mathbb{H},\mathbb{O}, respectively, and to the double cover S(\mathbb{A}^2)\to\mathbb{PA}^1 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 V^\infty its one-point compactification, i.e. V \cong \mathbb{R}^k and V^\infty \cong S^k 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 V^\infty, then we can form the wedge products V^\infty \wedge X.

Now let F \colon V^\infty \wedge X \to V^\infty \wedge Y be a stable map, i.e. stable under the reduced suspension functor. The (stable) geometric Hopf invariant of F is

h(F) \in \{X, Y \wedge Y\}_{\mathbb{Z}_2},

an element of the stable, \mathbb{Z}_2-equivariant homotopy group of maps from X to Y \wedge Y. 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 \mathbb{Z}_2-action is the trivial action on X and the flipping of the two factors on Y \wedge Y. If we let \Delta_X \colon X \to X \wedge X denote the canonnical diagonal map and I the identity, then the Hopf invariant is defined by the following:

h(F) := (F \wedge F) (I \wedge \Delta_X) - (I \wedge \Delta_Y) (I \wedge F)

This map is initially a map from V^\infty \wedge V^\infty \wedge X to V^\infty \wedge V^\infty \wedge Y \wedge Y, but under the direct limit it becomes the advertised element of the stable homotopy 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

  • 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.
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