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		<summary type="html">&lt;p&gt;&lt;span class=&quot;autocomment&quot;&gt;Bibliography: &lt;/span&gt;Fix &lt;a href=&quot;/index.php?title=Help:CS1_errors&amp;amp;action=edit&amp;amp;redlink=1&quot; class=&quot;new&quot; title=&quot;Help:CS1 errors (page does not exist)&quot;&gt;CS1 deprecated date parameter errors&lt;/a&gt;&lt;/p&gt;
&lt;p&gt;&lt;b&gt;New page&lt;/b&gt;&lt;/p&gt;&lt;div&gt;In [[mathematics]], in particular in [[algebraic topology]], the Hopf invariant is a [[homotopy]] invariant of certain maps between [[sphere]]s.&lt;br /&gt;
__TOC__&lt;br /&gt;
== Motivation ==&lt;br /&gt;
In 1931 [[Heinz Hopf]] used [[Clifford parallel]]s to construct the &amp;#039;&amp;#039;[[Hopf map]]&amp;#039;&amp;#039; &lt;br /&gt;
:&amp;lt;math&amp;gt;\eta\colon S^3 \to S^2&amp;lt;/math&amp;gt;, &lt;br /&gt;
&lt;br /&gt;
and proved that &amp;lt;math&amp;gt;\eta&amp;lt;/math&amp;gt; is essential, i.e. not [[homotopic]] to the constant map, by using the linking number (=1) of the circles &lt;br /&gt;
:&amp;lt;math&amp;gt;\eta^{-1}(x),\eta^{-1}(y) \subset S^3&amp;lt;/math&amp;gt; for any &amp;lt;math&amp;gt;x \neq y \in S^2&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
It was later shown that the [[homotopy group]] &amp;lt;math&amp;gt;\pi_3(S^2)&amp;lt;/math&amp;gt; is the infinite [[cyclic group]] generated by &amp;lt;math&amp;gt;\eta&amp;lt;/math&amp;gt;. In 1951, [[Jean-Pierre Serre]] proved that the  [[rational homotopy]] groups &lt;br /&gt;
:&amp;lt;math&amp;gt;\pi_i(S^n) \otimes \mathbb{Q}&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
for an odd-dimensional sphere (&amp;lt;math&amp;gt;n&amp;lt;/math&amp;gt; odd) are zero unless &amp;#039;&amp;#039;i&amp;#039;&amp;#039; = 0 or &amp;#039;&amp;#039;n&amp;#039;&amp;#039;. However, for an even-dimensional sphere (&amp;#039;&amp;#039;n&amp;#039;&amp;#039; even), there is one more bit of infinite cyclic homotopy in degree &amp;lt;math&amp;gt;2n-1&amp;lt;/math&amp;gt;. There is an interesting way of seeing this:&lt;br /&gt;
&lt;br /&gt;
== Definition ==&lt;br /&gt;
Let &amp;lt;math&amp;gt;\phi \colon S^{2n-1} \to S^n&amp;lt;/math&amp;gt; be a [[continuous map]] (assume &amp;lt;math&amp;gt;n&amp;gt;1&amp;lt;/math&amp;gt;). Then we can form the [[cell complex]]&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt;C_\phi = S^n \cup_\phi D^{2n},&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
where &amp;lt;math&amp;gt;D^{2n}&amp;lt;/math&amp;gt; is a &amp;lt;math&amp;gt;2n&amp;lt;/math&amp;gt;-dimensional disc attached to &amp;lt;math&amp;gt;S^n&amp;lt;/math&amp;gt; via &amp;lt;math&amp;gt;\phi&amp;lt;/math&amp;gt;.&lt;br /&gt;
The cellular chain groups &amp;lt;math&amp;gt;C^*_\mathrm{cell}(C_\phi)&amp;lt;/math&amp;gt; are just freely generated on the &amp;lt;math&amp;gt;n&amp;lt;/math&amp;gt;-cells in degree &amp;lt;math&amp;gt;n&amp;lt;/math&amp;gt;, so they are &amp;lt;math&amp;gt;\mathbb{Z}&amp;lt;/math&amp;gt; in degree 0, &amp;lt;math&amp;gt;n&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;2n&amp;lt;/math&amp;gt; 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 &amp;lt;math&amp;gt;n&amp;gt;1&amp;lt;/math&amp;gt;), the cohomology is&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt;H^i_\mathrm{cell}(C_\phi) = \begin{cases} \mathbb{Z} &amp;amp; i=0,n,2n, \\ 0 &amp;amp; \mbox{otherwise}. \end{cases}&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
Denote the generators of the cohomology groups by&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt;H^n(C_\phi) = \langle\alpha\rangle&amp;lt;/math&amp;gt; and &amp;lt;math&amp;gt;H^{2n}(C_\phi) = \langle\beta\rangle.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
For dimensional reasons, all cup-products between those classes must be trivial apart from &amp;lt;math&amp;gt;\alpha \smile \alpha&amp;lt;/math&amp;gt;. Thus, as a &amp;#039;&amp;#039;ring&amp;#039;&amp;#039;, the cohomology is&lt;br /&gt;
&lt;br /&gt;
: &amp;lt;math&amp;gt;H^*(C_\phi) = \mathbb{Z}[\alpha,\beta]/\langle \beta\smile\beta = \alpha\smile\beta = 0, \alpha\smile\alpha=h(\phi)\beta\rangle.&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
The integer &amp;lt;math&amp;gt;h(\phi)&amp;lt;/math&amp;gt; is the &amp;#039;&amp;#039;&amp;#039;Hopf invariant&amp;#039;&amp;#039;&amp;#039; of the map &amp;lt;math&amp;gt;\phi&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
== Properties ==&lt;br /&gt;
&amp;#039;&amp;#039;&amp;#039;Theorem&amp;#039;&amp;#039;&amp;#039;: &amp;lt;math&amp;gt;h\colon\pi_{2n-1}(S^n)\to\mathbb{Z}&amp;lt;/math&amp;gt; is a homomorphism. Moreover, if &amp;lt;math&amp;gt;n&amp;lt;/math&amp;gt; is even, &amp;lt;math&amp;gt;h&amp;lt;/math&amp;gt; maps onto &amp;lt;math&amp;gt;2\mathbb{Z}&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
The Hopf invariant is &amp;lt;math&amp;gt;1&amp;lt;/math&amp;gt; for the &amp;#039;&amp;#039;Hopf maps&amp;#039;&amp;#039; (where &amp;lt;math&amp;gt;n=1,2,4,8&amp;lt;/math&amp;gt;, corresponding to the real division algebras &amp;lt;math&amp;gt;\mathbb{A}=\mathbb{R},\mathbb{C},\mathbb{H},\mathbb{O}&amp;lt;/math&amp;gt;, respectively, and to the double cover &amp;lt;math&amp;gt;S(\mathbb{A}^2)\to\mathbb{PA}^1&amp;lt;/math&amp;gt; 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 [[topological K-theory]], that these are the only maps with Hopf invariant 1.&lt;br /&gt;
&lt;br /&gt;
== Generalisations for stable maps ==&lt;br /&gt;
&lt;br /&gt;
A very general notion of the Hopf invariant can be defined, but it requires a certain amount of homotopy theoretic groundwork:&lt;br /&gt;
&lt;br /&gt;
Let &amp;lt;math&amp;gt;V&amp;lt;/math&amp;gt; denote a vector space and &amp;lt;math&amp;gt;V^\infty&amp;lt;/math&amp;gt; its [[one-point compactification]], i.e. &amp;lt;math&amp;gt;V \cong \mathbb{R}^k&amp;lt;/math&amp;gt; and &lt;br /&gt;
:&amp;lt;math&amp;gt;V^\infty \cong S^k&amp;lt;/math&amp;gt; for some &amp;lt;math&amp;gt;k&amp;lt;/math&amp;gt;. &lt;br /&gt;
&lt;br /&gt;
If &amp;lt;math&amp;gt;(X,x_0)&amp;lt;/math&amp;gt; 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 &amp;lt;math&amp;gt;V^\infty&amp;lt;/math&amp;gt;, then we can form the wedge products &lt;br /&gt;
:&amp;lt;math&amp;gt;V^\infty \wedge X&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
Now let &lt;br /&gt;
:&amp;lt;math&amp;gt;F \colon V^\infty \wedge X \to V^\infty \wedge Y&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
be a stable map, i.e. stable under the [[reduced suspension]] functor. The &amp;#039;&amp;#039;(stable) geometric Hopf invariant&amp;#039;&amp;#039; of &amp;lt;math&amp;gt;F&amp;lt;/math&amp;gt; is&lt;br /&gt;
:&amp;lt;math&amp;gt;h(F) \in \{X, Y \wedge Y\}_{\mathbb{Z}_2}&amp;lt;/math&amp;gt;,&lt;br /&gt;
&lt;br /&gt;
an element of the stable &amp;lt;math&amp;gt;\mathbb{Z}_2&amp;lt;/math&amp;gt;-equivariant homotopy group of maps from &amp;lt;math&amp;gt;X&amp;lt;/math&amp;gt; to &amp;lt;math&amp;gt;Y \wedge Y&amp;lt;/math&amp;gt;. Here &amp;quot;stable&amp;quot; means &amp;quot;stable under suspension&amp;quot;, i.e. the direct limit over &amp;lt;math&amp;gt;V&amp;lt;/math&amp;gt; (or &amp;lt;math&amp;gt;k&amp;lt;/math&amp;gt;, if you will) of the ordinary, equivariant homotopy groups; and the &amp;lt;math&amp;gt;\mathbb{Z}_2&amp;lt;/math&amp;gt;-action is the trivial action on &amp;lt;math&amp;gt;X&amp;lt;/math&amp;gt; and the flipping of the two factors on &amp;lt;math&amp;gt;Y \wedge Y&amp;lt;/math&amp;gt;. If we let &lt;br /&gt;
:&amp;lt;math&amp;gt;\Delta_X \colon X \to X \wedge X&amp;lt;/math&amp;gt; &lt;br /&gt;
&lt;br /&gt;
denote the canonical diagonal map and &amp;lt;math&amp;gt;I&amp;lt;/math&amp;gt; the identity, then the Hopf invariant is defined by the following:&lt;br /&gt;
:&amp;lt;math&amp;gt;h(F) := (F \wedge F) (I \wedge \Delta_X) - (I \wedge \Delta_Y) (I \wedge F).&amp;lt;/math&amp;gt;&lt;br /&gt;
&lt;br /&gt;
This map is initially a map from &lt;br /&gt;
:&amp;lt;math&amp;gt;V^\infty \wedge V^\infty \wedge X&amp;lt;/math&amp;gt; to &amp;lt;math&amp;gt;V^\infty \wedge V^\infty \wedge Y \wedge Y&amp;lt;/math&amp;gt;, &lt;br /&gt;
&lt;br /&gt;
but under the direct limit it becomes the advertised element of the stable homotopy &amp;lt;math&amp;gt;\mathbb{Z}_2&amp;lt;/math&amp;gt;-equivariant group of maps.&lt;br /&gt;
There exists also an unstable version of the Hopf invariant &amp;lt;math&amp;gt;h_V(F)&amp;lt;/math&amp;gt;, for which one must keep track of the vector space &amp;lt;math&amp;gt;V&amp;lt;/math&amp;gt;.&lt;br /&gt;
&lt;br /&gt;
==References==&lt;br /&gt;
* {{citation&lt;br /&gt;
    | first = J.F.|last= Adams&lt;br /&gt;
    | year = 1960&lt;br /&gt;
    | title = On the non-existence of elements of Hopf invariant one&lt;br /&gt;
    | journal = Ann. Math.&lt;br /&gt;
    | volume = 72&lt;br /&gt;
    | pages = 20–104&lt;br /&gt;
    | doi = 10.2307/1970147&lt;br /&gt;
    | issue = 1&lt;br /&gt;
    | publisher = The Annals of Mathematics, Vol. 72, No. 1&lt;br /&gt;
    | jstor = 1970147&lt;br /&gt;
}}&lt;br /&gt;
* {{citation&lt;br /&gt;
    | first = J.F.|last= Adams&lt;br /&gt;
    | first2 = M.F.&lt;br /&gt;
    | year = 1966&lt;br /&gt;
    | title = K-Theory and the Hopf Invariant&lt;br /&gt;
    | journal = The Quarterly Journal of Mathematics&lt;br /&gt;
    | volume = 17&lt;br /&gt;
    | issue = 1&lt;br /&gt;
    | pages = 31–38|last2=Atiyah&lt;br /&gt;
    | doi = 10.1093/qmath/17.1.31&lt;br /&gt;
}}&lt;br /&gt;
&lt;br /&gt;
* {{citation&lt;br /&gt;
    | first = M.|last= Crabb&lt;br /&gt;
    | first2=A. |last2= Ranicki&lt;br /&gt;
    | year = 2006&lt;br /&gt;
    | title = The geometric Hopf invariant&lt;br /&gt;
    | url = http://www.maths.ed.ac.uk/~aar/slides/hopfbeam.pdf&lt;br /&gt;
    &lt;br /&gt;
}}&lt;br /&gt;
* {{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}}&lt;br /&gt;
*{{springer|first=A.V. |last=Shokurov|title=Hopf invariant|id=h/h048000}}&lt;br /&gt;
&lt;br /&gt;
[[Category:Homotopy theory]]&lt;/div&gt;</summary>
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