Hopf invariant#Properties

{{Short description|Homotopy invariant of maps between n-spheres}}

In mathematics, in particular in algebraic topology, the Hopf invariant is a homotopy invariant of certain maps between n-spheres.

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Motivation

In 1931 Heinz Hopf used Clifford parallels to construct the Hopf map

:\eta\colon S^3 \to S^2,

and proved that \eta is essential, i.e., not homotopic to the constant map, by using the fact that the linking number of the circles

:\eta^{-1}(x),\eta^{-1}(y) \subset S^3

is equal to 1, for any x \neq y \in S^2.

It was later shown that the homotopy group \pi_3(S^2) is the infinite cyclic group generated by \eta. In 1951, Jean-Pierre Serre proved that the rational homotopy groups {{cite journal |last1=Serre |first1=Jean-Pierre |title=Groupes D'Homotopie Et Classes De Groupes Abeliens |journal=The Annals of Mathematics |date=September 1953 |volume=58 |issue=2 |pages=258–294 |doi=10.2307/1969789|jstor=1969789 }}

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

for an odd-dimensional sphere (n odd) are zero unless i is equal to 0 or n. However, for an even-dimensional sphere (n even), there is one more bit of infinite cyclic homotopy in degree 2n-1.

Definition

Let \varphi \colon S^{2n-1} \to S^n be a continuous map (assume n>1). Then we can form the cell complex

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

where D^{2n} is a 2n-dimensional disc attached to S^n via \varphi.

The cellular chain groups C^*_\mathrm{cell}(C_\varphi) are just freely generated on the i-cells in degree i, 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 (recall that n>1), the cohomology is

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

Denote the generators of the cohomology groups by

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

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

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

The integer h(\varphi) is the Hopf invariant of the map \varphi.

Properties

Theorem: The map h\colon\pi_{2n-1}(S^n)\to\mathbb{Z} is a homomorphism.

If n is odd, h is trivial (since \pi_{2n-1}(S^n) is torsion).

If n is even, the image of h contains 2\mathbb{Z}. Moreover, the image of the Whitehead product of identity maps equals 2, i. e. h([i_n, i_n])=2, where i_n \colon S^n \to S^n is the identity map and [\,\cdot\,,\,\cdot\,] is the Whitehead product.

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 fibration 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 Adams and Michael Atiyah with methods of topological K-theory, that these are the only maps with Hopf invariant 1.

Whitehead integral formula

J. H. C. Whitehead has proposed the following integral formula for the Hopf invariant.{{cite journal |last1=Whitehead |first1=J. H. C. |title=An Expression of Hopf's Invariant as an Integral |journal=Proceedings of the National Academy of Sciences |date=1 May 1947 |volume=33 |issue=5 |pages=117–123 |doi=10.1073/pnas.33.5.117|pmid=16578254 |doi-access=free |pmc=1079004 |bibcode=1947PNAS...33..117W }}{{cite book |last1=Bott |first1=Raoul |last2=Tu |first2=Loring W |title=Differential forms in algebraic topology |date=1982 |location=New York |isbn=9780387906133}}{{rp|prop. 17.22}}

Given a map \varphi \colon S^{2n-1} \to S^n, one considers a volume form \omega_n on S^n such that \int_{S^n}\omega_n = 1.

Since d\omega_n = 0, the pullback \varphi^* \omega_n is a closed differential form: d(\varphi^* \omega_n) = \varphi^* (d\omega_n) = \varphi^* 0 = 0.

By Poincaré's lemma it is an exact differential form: there exists an (n - 1)-form \eta on S^{2n - 1} such that d\eta = \varphi^* \omega_n. The Hopf invariant is then given by

:

\int_{S^{2n - 1}} \eta \wedge d \eta.

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,x_0) 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 canonical 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 \mathbb{Z}_2-equivariant group of maps.

There exists also an unstable version of the Hopf invariant h_V(F), for which one must keep track of the vector space V.

References

{{Reflist}}

  • {{citation

| first = J. Frank|last= Adams|authorlink=Frank Adams

| year = 1960

| title = On the non-existence of elements of Hopf invariant one

| journal = Annals of Mathematics

| volume = 72

| pages = 20–104

| doi = 10.2307/1970147

| issue = 1

| jstor = 1970147

| mr=0141119

|citeseerx= 10.1.1.299.4490}}

  • {{citation

| first1 = J. Frank|last1= Adams| author1-link=Frank Adams

| first2 = Michael F.|last2=Atiyah| author2-link=Michael Atiyah

| year = 1966

| title = K-Theory and the Hopf Invariant

| journal = Quarterly Journal of Mathematics

| volume = 17

| issue = 1

| pages = 31–38

| doi = 10.1093/qmath/17.1.31

| mr=0198460

}}

  • {{cite web

| first1 = Michael|last1= Crabb

| first2=Andrew |last2= Ranicki|author2-link=Andrew Ranicki

| year = 2006

| title = The geometric Hopf invariant

| url = http://www.maths.ed.ac.uk/~aar/slides/hopfbeam.pdf

}}

  • {{Citation | last1=Hopf | first1=Heinz | title=Über die Abbildungen der dreidimensionalen Sphäre auf die Kugelfläche | year=1931 | journal=Mathematische Annalen | issn=0025-5831 | volume=104 | pages=637–665 | doi=10.1007/BF01457962}}
  • {{springer|first=A.V. |last=Shokurov|title=Hopf invariant|id=h/h048000}}

Category:Homotopy theory