Exotic spheres

(Difference between revisions)
Jump to: navigation, search
(Sphere bundles)
(Sphere bundles)
Line 28: Line 28:
=== Sphere bundles ===
=== Sphere bundles ===
<wikitex>;
<wikitex>;
The first known examples of exotic spheres were discovered by Milnor in {{cite|Milnor1956}}. They are the total spaces of certain 3-[[Wikipedia:Sphere_bundle#Sphere_bundles|sphere bundles]] over the 4-sphere as we now explain: the group $\pi_3(SO(4)) \cong \Zz \oplus \Zz$ parametrises linear $3$-sphere bundles over $S^4$ where a pair $(m, n)$ gives rise to a bundle with Euler number $n$ and first Pontrjagin class $2(n+2m)$: here we orient $S^4$ and so identify $H^4(S^4; \Zz) = \Zz$. If we set $n = 1$ then the long exact homotopy sequence of a fibration and Poincare duality ensure that the manifold $\Sigma_{m, 1}$, the total space of the bundle $(m, 1)$ is a homotopy sphere. Milnor first used a $\Zz/7$-invariant, called the $\lambda$-invariant, to show, e.g. that $\Sigma_{1, 1}$ is not diffeomorphic to $S^7$. A little later Kervaire and Milnor {{cite|Kervaire&Milnor1963}} show that $\Theta_7 \cong \Zz/28$ and Eells and Kuiper {{cite|Eells&Kuiper1962}} showed that
+
*The first known examples of exotic spheres were discovered by Milnor in {{cite|Milnor1956}}. They are the total spaces of certain 3-[[Wikipedia:Sphere_bundle#Sphere_bundles|sphere bundles]] over the 4-sphere as we now explain: the group $\pi_3(SO(4)) \cong \Zz \oplus \Zz$ parametrises linear $3$-sphere bundles over $S^4$ where a pair $(m, n)$ gives rise to a bundle with Euler number $n$ and first Pontrjagin class $2(n+2m)$: here we orient $S^4$ and so identify $H^4(S^4; \Zz) = \Zz$. If we set $n = 1$ then the long exact homotopy sequence of a fibration and Poincare duality ensure that the manifold $\Sigma^7_{m, 1}$, the total space of the bundle $(m, 1)$, is a homotopy sphere. Milnor first used a $\Zz_7$-invariant, called the $\lambda$-invariant, to show, e.g. that $\Sigma^7_{1, 1}$ is not diffeomorphic to $S^7$. A little later Kervaire and Milnor {{cite|Kervaire&Milnor1963}} show that $\Theta_7 \cong \Zz_{28}$ and Eells and Kuiper {{cite|Eells&Kuiper1962}} showed that
$$ \Sigma_{m, 1} = \frac{m(m-1)}{56} \in \Zz/28 \cong \Theta_7.$$
+
$$ \Sigma^7_{m, 1} = \frac{m(m-1)}{56} \in \Zz/28 \cong \Theta_7.$$
Shimada {{cite|Shimada1957}} used similar techniques to show that the total spaces of certain 7-sphere bundles over the 8-sphere are exotic 15-spheres.
+
*Shimada {{cite|Shimada1957}} used similar techniques to show that the total spaces of certain 7-sphere bundles over the 8-sphere are exotic 15-spheres. In this case $\pi_7(SO(8)) \cong \Zz \oplus \Zz$ and the bundle $(m, n)$ has Euler number $n$ and second Pontrjagin class $6(n+2m)$. Moreover $\Theta_{15} \cong \Zz_{8,128} \oplus \Zz_2$ where the $\Zz_{8,128}$-summand is $bP_{16}$ as explained below and results of {{cite|Wall1962}} and {{cite|Eells&Kuiper1962}} combine to show that
+
$$ \Sigma^{15}_{m, 1} = \frac{m(m-1)}{8,128} \in \Zz_{8,128} \cong bP_{16} \subset \Theta_{15}.$$
By Adams' solution of the [[Wikipedia:Hopf_invariant| Hopf-invariant]] 1 problem, {{cite|Adams1958}} and {{cite|Adams1960}}, the dimensions n = 3, 7 and 15 are the only dimensions where an n-sphere can be fibre over an m-sphere for 0 < m < n.
+
+
*By Adams' solution of the [[Wikipedia:Hopf_invariant| Hopf-invariant]] 1 problem, {{cite|Adams1958}} and {{cite|Adams1960}}, the dimensions n = 3, 7 and 15 are the only dimensions in which a topological n-sphere can be fibre over an m-sphere for 0 < m < n.
</wikitex>
</wikitex>

Revision as of 16:51, 5 January 2010


This page has not been refereed. The information given here might be incomplete or provisional.

Contents

1 Introduction

A homotopy sphere \Sigma^n is a closed, smooth n-manifold homotopy equivalent to S^n. The manifold \Sigma^n is called an exotic sphere if it is not diffeomorphic to S^n. By the Generalised Poincaré Conjecture proven by Smale, every homotopy sphere in dimension n \geq 5 is homeomorphic to S^n: this statement holds in dimension 2 by the classification of surfaces and was famously proven in dimension 4 in [Freedman1982] and in dimension 3 by Perelman. We define

\displaystyle \Theta_{n} := \{[\Sigma^n] | \Sigma^n \simeq S^n \}

to be the set of oriented diffeomorphism classes of homotopy spheres. Connected sum makes \Theta_n into an abelian group with inverse given by reversing orientation.

2 Construction and examples

Exotic spheres may be constructed in a variety of ways.

2.1 Brieskorn varieties

2.2 Sphere bundles

  • The first known examples of exotic spheres were discovered by Milnor in [Milnor1956]. They are the total spaces of certain 3-sphere bundles over the 4-sphere as we now explain: the group \pi_3(SO(4)) \cong \Zz \oplus \Zz parametrises linear 3-sphere bundles over S^4 where a pair (m, n) gives rise to a bundle with Euler number n and first Pontrjagin class 2(n+2m): here we orient S^4 and so identify H^4(S^4; \Zz) = \Zz. If we set n = 1 then the long exact homotopy sequence of a fibration and Poincare duality ensure that the manifold \Sigma^7_{m, 1}, the total space of the bundle (m, 1), is a homotopy sphere. Milnor first used a \Zz_7-invariant, called the \lambda-invariant, to show, e.g. that \Sigma^7_{1, 1} is not diffeomorphic to S^7. A little later Kervaire and Milnor [Kervaire&Milnor1963] show that \Theta_7 \cong \Zz_{28} and Eells and Kuiper [Eells&Kuiper1962] showed that
\displaystyle  \Sigma^7_{m, 1} = \frac{m(m-1)}{56} \in \Zz/28 \cong \Theta_7.
  • Shimada [Shimada1957] used similar techniques to show that the total spaces of certain 7-sphere bundles over the 8-sphere are exotic 15-spheres. In this case \pi_7(SO(8)) \cong \Zz \oplus \Zz and the bundle (m, n) has Euler number n and second Pontrjagin class 6(n+2m). Moreover \Theta_{15} \cong \Zz_{8,128} \oplus \Zz_2 where the \Zz_{8,128}-summand is bP_{16} as explained below and results of [Wall1962] and [Eells&Kuiper1962] combine to show that
\displaystyle  \Sigma^{15}_{m, 1} = \frac{m(m-1)}{8,128} \in \Zz_{8,128} \cong bP_{16} \subset \Theta_{15}.


  • By Adams' solution of the Hopf-invariant 1 problem, [Adams1958] and [Adams1960], the dimensions n = 3, 7 and 15 are the only dimensions in which a topological n-sphere can be fibre over an m-sphere for 0 < m < n.

2.3 Plumbing

As special case of the following construction goes back at least to [Milnor1959].

Let i \in  \{1,  \dots, n\}, let (p_i, q_i) be pairs of positive integers such that p_i + q_i + 2 = n and let \alpha_i \in \pi_{p_i}(SO(q_i+1)) be the clutching functions of D^{q_i+1}-bundles over S^{p_i + 1}

\displaystyle  D^{q_i+1} \to D(\alpha_i) \to S^{p_i+1}.

Let G be a graph with vertices \{v_1, \dots, v_n\} such that the edge set between v_i and v_j, is non-empty only if p_i = q_j. We form the manifold W = W(G;\{\alpha_i\}) from the disjoint union of the D(\alpha_i) by identifying D^{p_i+1} \times D^{q_i+1} and D^{q_j+1} \times D^{p_j+1} for each edge in G. If G is simply connected then

\displaystyle \Sigma(G, \{\alpha_i \}) : = \partial W

is often a homotopy sphere. We establish some notation for graphs, bundles and define

  • let T denote the graph with two vertices and one edge connecting them and define \Sigma(\alpha, \beta) : = \Sigma(T; \{\alpha, \beta\}),
  • let E_8 denote the E_8-graph,
  • let \tau_{n} \in \pi_{n-1}(SO(n)) denote the tangent bundle of the n-sphere,
  • let \gamma_{4s-1}^k \in \pi_{4s-1}(SO(k)) \cong \Zz, k > 4s, denote a generator,
  • let \gamma_{4s-1}' \in \pi_{4s-1}(SO(4s-1)) \cong \Zz, denote a generator:
  • let S : \pi_k(SO(j)) \to \pi_k(SO(j+1)) be the suspension homomorphism,
    • S^2(\gamma'_{4k-1}) = \pm 2 \gamma_{4k-1}^{4k+1} for k = 1, 2 and S^2 (\gamma'_{4k-1}) = \pm \gamma_{4k-1}^{4k+1} for k > 2,
  • let \eta_n : S^{n+1} \to S^n be essential.

Then we have the following exotic spheres.

  • \Sigma^{4k-1}(E_8; \{\tau_{2k}, \dots \tau_{2k}\}), the Milnor sphere, generates bP_{4k}, k>1.
  • \Sigma^{4k+1}(T; \{\tau_{2k+1}, \tau_{2k+1}\}), the Kervaire sphere, generates bP_{4k+2}.
  • \Sigma^{4k-1}(S\gamma_{4k-1}', S\gamma_{4k-1}') is the inverse of the Milnor sphere for k = 1, 2.
    • For general k, \Sigma^{4k-1}(S\gamma_{4k-1}', S\gamma_{4k-1}') is exotic.
  • \Sigma^8(T; \{\gamma_3^5, \eta_3\tau_4\}), generates \Theta_8 = \Zz_2.
  • \Sigma^{16}(T; \{\gamma_{7}^9, \eta_7\tau_8\}), generates \Theta_{16} = \Zz_2.

2.4 Twisting

By [Cerf1970] and [Smale1962a] there is an isomorphism \Theta_{n+1} \cong \Gamma_{n+1} for n \geq 5 where \Gamma_{n+1} = \pi_0(\Diff_+(S^n)) is the group of isotopy classes of orientation preserving diffeomorphisms of S^n. The map is given by

\displaystyle  \Gamma_{n+1} \to \Theta_{n+1}, ~~~~~[f] \longmapsto \Sigma_{f} := D^{n+1} \cup_f (-D^{n+1}).

Hence one may construct exotic (n+1)-spheres by describing diffeomorphisms of S^n which are not isotopic to the identity. We give such a construction which probably goes back to Milnor: so far the earliest reference found is the problem list of the 1963 Seattle topology conference [Lashof1965].

Represent \alpha \in \pi_p(SO(q)) and \beta \in \pi_q(SO(p)) by smooth compactly supported functions \alpha : \Rr^p \to SO(q) and \beta : \Rr^q \to SO(p) and define the following self-diffeomorphisms of \Rr^p \times \Rr^q

\displaystyle  F_\alpha : \Rr^p \times \Rr^q \cong \Rr^p \times \Rr^q, ~~~~(x, y) \longmapsto (x, \alpha(x)y),
\displaystyle  F_\beta : \Rr^p \times \Rr^q \cong \Rr^p \times \Rr^q, ~~~~(x, y) \longmapsto (\beta(y)x,y),
\displaystyle s(\alpha, \beta) := F_\alpha F_\beta F_\alpha^{-1}F_\beta^{-1}.

If follows that s(\alpha, \beta) is compactly supported and so extends uniquely to a diffeomrphism of S^{p+q}. In this way we obtain a bilinear pairing

\displaystyle  \sigma : \pi_q(SO(q)) \otimes \pi_q(SO(p)) \longrightarrow \Theta_{p+q+1}, ~~~~(\alpha, \beta) \longmapsto \Sigma_{s(\alpha, \beta)}

such that

\displaystyle  \sigma(\alpha, \beta) \equiv \Sigma(S\alpha, S\beta).

In particular \sigma(\gamma_{4k-1}', \gamma_{4k-1}') generates bP_{4k} for k = 1, 2.

3 Invariants

Signature, Kervaire invariant, \alpha-invariant, Eels-Kuiper invariant, s-invariant.

4 Classification

For n \geq 5, group of exotic spheres \Theta_n fits into the following long exact sequence which stops at L_5(e) = 0:

\displaystyle  \dots \to \pi_{n+1}(G/O) \to L_{n+1}(e) \to \Theta_n \to \pi_n(G/O) \to L_n(e) \to \dots .

The existence of the above sequence was proven in [Kervaire&Milnor1963]. More details can also be found in [Levine1983].

5 Further discussion

\displaystyle   \def\curv{1.5pc}% Adjust the curvature of the curved arrows here  \xymatrix@!R@!C@!0@R=2.5pc@C=4pc{% Adjust the spacing here  \pi_n(\Top/O) \ar[dr] \ar@/u\curv/[rr] && \pi_{n-1}(O) \ar[dr] \ar@/u\curv/[rr] && \pi_{n-1}(G) \\  & \pi_n(G/O) \ar[dr] \ar[ur] && \pi_{n-1}(\Top) \ar[dr] \ar[ur] \\  \pi_n(G) \ar[ur] \ar@/d\curv/[rr] && \pi_n(G/\Top) \ar[ur] \ar@/d\curv/[rr] && \pi_{n-1}(\Top/O)  }

6 External references

7 References

Personal tools
Namespaces
Variants
Actions
Navigation
Interaction
Toolbox