Exotic spheres

From Manifold Atlas
Jump to: navigation, search

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

Contents

[edit] 1 Introduction

By a homotopy sphere \Sigma^n we mean a closed smooth oriented 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. An important subgroup of \Theta_n is bP_{n+1} which consists of those homotopy spheres which bound parallelisable manifolds.

[edit] 2 Construction and examples

The first exotic spheres discovered were certain 3-sphere bundles over the 4-sphere, [Milnor1956]. Following this discovery there was a rapid development of techniques which construct exotic spheres. We review four such constructions: plumbing, Brieskorn varieties, sphere-bundles and twisting.

[edit] 2.1 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}\}) =: \Sigma_M, the Milnor sphere, generates bP_{4k}, k>1.
  • \Sigma^{4k+1}(\tau_{2k+1}, \tau_{2k+1}) =: \Sigma_K, 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(\gamma_3^5, \eta_3\gamma'_3), generates \Theta_8 = \Zz_2.
  • \Sigma^{16}(\gamma_{7}^9, \eta_7\gamma'_7), generates \Theta_{16} = \Zz_2.

[edit] 2.2 Brieskorn varieties

Let z = (z_0, \dots , z_n) be a point in \Cc^{n+1} and let a = (a_0, \dots, a_n) be a string of n+1 positive integers. Given the complex variety V(a) : = \{z \, | \, z_0^{a_0} + \dots + z_n^{a_n} =0 \} and the \epsilon-sphere S^{2n+1}_\epsilon : = \{ z \, | \, \Sigma_{i=0}^n z_i\bar z_i = \epsilon \} for small \epsilon, following [Milnor1968] we define the closed smooth oriented (n-2)-connected (2n-1)-manifold

\displaystyle  W^{2n-1}(a) : = V(a) \cap S^{2n+1}_\epsilon.

The manifolds W^{2n-1}(a) are often called Brieskorn varieties. By construction, every W^{2n-1}(a) lies in S^{2n+1} and so bounds a parallelisable manifold. In [Brieskorn1966, Korollar 2] (see also [Brieskorn1966a] and [Hirzebruch&Mayer1968]), it is shown that all homotopy spheres in bP_{4k} and bP_{4k-2} can be realised as W(a) for some a. Let 2, \dots, 2 be a string of 2k-1 2's in a row with k \geq 2, then there are diffeomorphisms

\displaystyle   W^{4k-1}(3, 6r+1, 2, \dots , 2) \cong r \cdot \Sigma_M \in bP_{4k},
\displaystyle   W^{4k-3}(3, 2, \dots, 2) \cong \Sigma_K \in bP_{4k-2}.

[edit] 2.3 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, 2} is not diffeomorphic to S^7. A little later Kervaire and Milnor [Kervaire&Milnor1963] proved that \Theta_7 \cong \Zz_{28} and Eells and Kuiper [Eells&Kuiper1962] defined a refinement of the \lambda-invariant, now called the Eells-Kuiper \mu-invariant, which in particular gives

\displaystyle  \Sigma^7_{m, 1} = -(m(m-1)/2)\cdot \Sigma_M \in bP_8 \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. Results of [Wall1962a] and [Eells&Kuiper1962] combine to show that

\displaystyle  \Sigma^{15}_{m, 1} = -(m(m-1)/2)\cdot \Sigma_M  \in 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.

[edit] 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, p.583, The group of diffeomorphisms of S^n].

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 diffeomorphism 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 for k=1, 2 we see that \sigma(\gamma_{4k-1}', \gamma_{4k-1}') \cong -\Sigma_M generates bP_{4k}.

[edit] 3 Invariants

Finding invariants of exotic sphere \Sigma which distinguish it from the standard sphere is rather a subtle undertaking. Moreover such invariants are often defined via a manifold W with \partial W \cong \Sigma. In this case finding an intrinsic definition and or computation of the relevant invariant can also be subtle.

We begin by listing some invariants which are equal for all exotic spheres.

Proposition 3.1. Let \Sigma be a closed smooth manifold homeomorphic to the n-sphere. Then

  1. there is an isomorphism of tangent bundles T\Sigma \cong TS^n,
  2. the signature of \Sigma vanishes,
  3. the Kervaire invariant of (\Sigma, F) is zero for every framing of \Sigma.

(To make sense of the first statement remember that the topological space underlying every exotic sphere is homeomorphic to S^n.)

Remark 3.2. The analogue of the first statement for the stable tangent bundle was proven in [Kervaire&Milnor1963, Theorem 3.1]. A proof of the unstable statement is given in [Ray&Pedersen1980, Lemma 1.1]. The next two statements are obvious since both the signature and Kervaire invariant are defined to be zero if n = 2k+1 and via a symmetric or quadratic form on H_k(\Sigma; \Zz) = 0 if n = 2k.

[edit] 3.1 Bordism classes

As every homotopy sphere is stably parallelisable, homotopy spheres admit B-structures for any B. If B is such that [S^n, F] \mapsto 0 \in \Omega_n^B for any stable framing F of S^n, then we obtain a well-defined homomorphism

\displaystyle  \eta^B : \Theta_n \longrightarrow \Omega_n^B, ~~~\Sigma \longmapsto [\Sigma, F].
  • If B = BO\langle k \rangle for [n/2] + 1 < k < n+2 then \Omega_n^B is isomorphic to almost framed bordism and the homomorphism \eta^B is the same thing as the \eta: \Theta_n \to \pi_n(G/O) in Theorem 4.1.
  • Perhaps surprisingly \eta_n^{\Spin} \neq 0 for all n = 8k+1, 8k+2, as explained in the next subsection.
  • In general determining \eta^B is a hard and interesting problem.
  • B-coboundaries for elements of Ker(\eta^B_n) are often used to define invariants of B-null bordant homotopy spheres.

[edit] 3.2 The α-invariant

In dimensions n > 1, every exotic sphere \Sigma has a unique Spin structure and from above we have the homomorphism \eta_n^{\Spin} : \Theta_n \to \Omega_n^{\Spin}. Recall the \alpha-invariant homomorphism \alpha : \Omega_*^{\Spin} \to KO^{-*} and that there are isomorphisms KO^{-8k-1} \cong KO^{-8k-2} \cong \Zz/2 for all k \geq 1.

Theorem 3.3 [Anderson&Brown&Peterson1967]. We have \eta_n^{\Spin}(\Sigma) = 0 if and only if \alpha \circ \eta_n^{\Spin}(\Sigma) = 0 and \eta_n^{\Spin} \neq 0 if and only if n = 8k+1 or 8k+2.

Remark 3.4. Exotic spheres \Sigma with \alpha(\Sigma) \neq 0 are often called Hitchin spheres, after [Hitchin1974]: see the discussion of curvature below.

[edit] 3.3 The Eells-Kuiper invariant

[edit] 3.4 The s-invariant

[edit] 4 Classification

For n =1, 2 and 3, \Theta_n = \{ S^n \}. For n = 4, \Theta_4 is unknown. We therefore concentrate on higher dimensions.

For n \geq 5, the group of exotic n-spheres \Theta_n fits into the following long exact sequence, first discovered in [Kervaire&Milnor1963] (more details can also be found in [Levine1983] and [Lück2001]):

\displaystyle  \dots \stackrel{\eta_{n+1}}{\longrightarrow} \pi_{n+1}(G/O) \stackrel{\sigma_{n+1}}{\longrightarrow} L_{n+1}(e) \stackrel{\omega_{n+1}}{\longrightarrow} \Theta_n \stackrel{\eta_n}{\longrightarrow} \pi_n(G/O) \stackrel{\sigma_n}{\longrightarrow} L_n(e) \to \dots~.

Here L_n(e) is the n-th L-group of the the trivial group: L_n(e) = \Zz, 0, \Zz/2, 0 as n = 0, 1, 2 or 3 modulo 4 and the sequence ends at L_5(e) = 0. Also O is the stable orthogonal group and G is the stable group of homtopy self-equivalences of the sphere. There is a fibration O \to G \to G/O and the groups \pi_n(G/O) fit into the homtopy long exact sequence

\displaystyle  \dots \to \pi_n(O) \to \pi_n(G) \to \pi_n(G/O) \to \pi_{n-1}(O) \to \pi_{n-1}(G) \to \dots

of this fibration. The homomorphism J_n: \pi_n(O) \to \pi_n^S \cong \pi_n(G) is the stable J-homomorphism. In particular, by [Serre1951] the groups \pi_i(G) are finite and by [Bott1959], [Adams1966] and [Quillen1971] the domain, image and kernel of J_n have been completely determined. An important result in [Kervaire&Milnor1963] is that the homomorphism \sigma_{4k} is nonzero. The above sequence then gives

Theorem 4.1 [Kervaire&Milnor1963]. For n \geq 5, the group \Theta_n is finite. Moreover there is an exact sequence

\displaystyle  0 \longrightarrow bP_{n+1} \longrightarrow \Theta_{n} \longrightarrow Coker(J_n) \stackrel{K_n}{\longrightarrow} C_n \longrightarrow 0

where bP_{n+1} := {Im}(\omega_{n+1}), the group of homotopy spheres bounding paralellisable manifolds, is a finite cyclic group which vanishes if n is even. Moreover C_n = 0 unless n = 4k+2 when it is 0 or \Zz/2.

The groups Coker(J_n) are known for n up to approximately 62. In general their determination is a very hard problem. Modulo this problem we see two remaining problems in the determination of \Theta_n: an extension problem and the comptutation of the order of the groups bP_{n+1} and C_n. We discuss these in turn.

Theorem 4.2 [Brumfiel1968], [Brumfiel1969], [Brumfiel1970]. If n \neq 2^{j} - 3 the Kervaire-Milnor extension splits:

\displaystyle \Theta_n \cong bP_{n+1} \oplus Ker(K_n).

The map K_{4k+2} : Coker(J_{4k+2}) \to \Zz/2 is the Kervaire invariant and by definition C_{4k+2} = Im(K_{4k+2}). By the long exact sequence above we have

Theorem 4.3 [Kervaire&Milnor1963, Section 8]. The group bP_{4k+2} is either \Zz/2 or 0. Moreover the following are equivalent:

  • bP_{4k+2} = 0,
  • the Kervaire sphere \Sigma^{4k+1}_K is diffeomorphic to the standard sphere,
  • there is a framed manifold with Kervaire invariant 1: C_{4k+2} \cong \Zz/2.

Conversely the following are equivalent:

  • bP_{4k+2} = \Zz/2,
  • the Kervaire sphere \Sigma^{4k+1}_K is not diffeomorphic to the standard sphere,
  • there is no framed manifold with Kervaire invariant 1: C_{4k+2} \cong 0.

[edit] 4.1 The order of bP4k

The group bP_{4k} is a cyclic group whose order can be determined using the Hirzebruch's signature theorem if one knows the order of Im(J_{4k-1}) \subset \pi_{4k-1}(G). Adams determined the latter group up to a factor of two which was settled by Quillen with a positive solution to the Adams conjecture.

Theorem 4.4. Let a_k = (3-(-1)^k)/2, let B_k be the k-th Bernoulli number (topologist indexing) and for x \in \Qq let Num(x) denote the numerator of x expressed in lowest form. Then for k \geq 2, the order of bP_{4k} is

\displaystyle  t_k = a_k \cdot 2^{2k-2}\cdot (2^{2k-1}-1) \cdot Num(B_k/4k).

Remark 4.5. Note that Num(B_k/4k) is odd so the 2-primary order of bP_{4k} is a_k \cdot 2^{2k-2} while the odd part is (2^{2k-1}-1) \cdot Num(B_k/4k). Modulo the Adams conjecture the proof appeared in [Kervaire&Milnor1963, Section 7]. Detailed treatments can also be found in [Levine1983, Section 3] and [Lück2001, Chapter 6].

The following table lists factorisations of |bP_{4k}| for k = 2, \dots, 8.

4k 8 12 16 20 24 28 32
order bP4k 22.7 25.31 26.127 29.511 210.2047.691 213.8191 214.16384.3617


[edit] 4.2 The order of bP4k+2

The situation for bP_{4k+2} which is now almost completely understood as well. References for the theorem are given in the remark which follows it.

Theorem 4.6. The group bP_{4k+2} is given as follows:

  • bP_{6} = bP_{14} = bP_{30} = bP_{62} = 0,
  • bP_{126} = 0 or \Zz/2,
  • bP_{4k+2} = \Zz/2 else.

Remark 4.7. The following is a chronological list of determinations of bP_{4k+2}:

[edit] 5 Further discussion

[edit] 5.1 Curvature on exotic spheres

Gromoll-Meyer proved that a certain exotic 7-sphere can be realized as a biquotient of the compact Lie group Sp(2) and thus by the O'Neill formula has a Riemannian metric of nonnegative sectional curvature. It is not known whether there exist exotic spheres with Riemannian metrics of positive sectional curvature. For a recent review of which exotic spheres admit metrics of various sorts of positive curvature see [Joachim&Wraith2008].

[edit] 5.2 The Kervaire-Milnor braid

\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  \Theta_n \ar[dr] \ar@/u\curv/[rr] && \pi_{n-1}(O) \ar[dr] \ar@/u\curv/[rr] && \pi_{n-1}^S \\  & \Omega^{alm} \ar[dr] \ar[ur] && \Theta_{n-1}^{fr} \ar[dr] \ar[ur] \\  \pi_n^S \ar[ur] \ar@/d\curv/[rr] && L_n(\Z) \ar[ur] \ar@/d\curv/[rr] && \Theta_{n-1}  }
\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)  }

[edit] 6 Topological manifolds admitting no smooth structure

Let W^{2n} be a plumbing manifold as described above. By a simple version of the Alexander trick, there is a homemorphism f \colon \partial W \cong S^{2n-1} and so we can form the closed topological manifold

\displaystyle  \bar W : = W \cup_f D^{2n}.

If \partial W is exotic then it turns out that \bar W is a topological manifold which admits no smooth structure.

[Kervaire1960a] shows that \bar W^{10} is non-smoothable and the arugments there work for all odd n so long as the Kervaire sphere is exotic.

When n is even the proof is more complicated: one first need's Novikov's theorem that the rational Pontrjagin classes of a topological manifold are homeomorphism invariants [Novikov1965b]. Prior to Novikov's theorem, some weaker statements were known. For example, when n=4 and W is the total space of a D^4-bundle over S^4 as above and if \partial W = \Sigma_{m, 1} then by [Tamura1961] \bar W is smoothable if and only if m(m-1)/2 \equiv 0 mod 4. [1]; Applying Novikov's theorem we now know that \bar W is smoothable if and only if m(m-1)/2 \equiv 0 mod 56.

[edit] 7 Footnotes

  1. Note that Tamura uses a different identification \pi_3(SO(4)) \cong \Zz \oplus \Zz from the one used above.

[edit] 8 References

[edit] 9 External links

Personal tools
Namespaces
Variants
Actions
Navigation
Interaction
Toolbox