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
:
and proved that is essential, i.e., not homotopic to the constant map, by using the fact that the linking number of the circles
:
is equal to 1, for any .
It was later shown that the homotopy group is the infinite cyclic group generated by . 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 }}
:
for an odd-dimensional sphere ( odd) are zero unless 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 .
Definition
Let be a continuous map (assume ). Then we can form the cell complex
:
where is a -dimensional disc attached to via .
The cellular chain groups are just freely generated on the -cells in degree , so they are in degree 0, and 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 ), the cohomology is
:
Denote the generators of the cohomology groups by
: and
For dimensional reasons, all cup-products between those classes must be trivial apart from . Thus, as a ring, the cohomology is
:
The integer is the Hopf invariant of the map .
Properties
Theorem: The map is a homomorphism.
If is odd, is trivial (since is torsion).
If is even, the image of contains . Moreover, the image of the Whitehead product of identity maps equals 2, i. e. , where is the identity map and is the Whitehead product.
The Hopf invariant is for the Hopf maps, where , corresponding to the real division algebras , respectively, and to the fibration 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 , one considers a volume form on such that .
Since , the pullback is a closed differential form: .
By Poincaré's lemma it is an exact differential form: there exists an -form on such that . 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 denote a vector space and its one-point compactification, i.e. and
: for some .
If 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 is
:
an element of the stable -equivariant homotopy group of maps from to . Here "stable" means "stable under suspension", i.e. the direct limit over (or , if you will) of the ordinary, equivariant homotopy groups; and the -action is the trivial action on and the flipping of the two factors on . If we let
:
denote the canonical diagonal map and 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 , for which one must keep track of the vector space .
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}}