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Course 7Book 7A: Topology and the Fundamental GroupChapter 9
The Poincaré Conjecture, Precisely
Every word of the statement, and why each hypothesis is needed.
This chapter is the guide's own; no textbook chapter matches it. John Morgan's survey "Recent progress on the Poincaré conjecture and the classification of 3-manifolds" (Bulletin of the AMS, 2005), section 1, and Milnor's essay "Towards the Poincaré conjecture and the classification of 3-manifolds" (Notices of the AMS, 2003) are good companions.
Everything in this book so far has been preparation for one sentence. Here it is, with every word defined.
Every closed, simply connected three-dimensional manifold is homeomorphic to the 3-sphere .
Henri Poincaré asked the question in 1904, at the end of the paper in which he found the homology sphere (7A.8 Homology in Brief). It resisted a century of attempts, became one of the seven Millennium Prize Problems of the Clay Mathematics Institute in 2000, and was proved by Grigori Perelman in three preprints posted in 2002 and 2003, using Richard Hamilton's Ricci flow. This chapter explains what the statement says, why each hypothesis is there, how it relates to the analogous statements in other dimensions, and why a theorem about topology could be proved by a method from differential geometry.
By the end of this chapter you will be able to:
- state the Poincaré conjecture and define every word in it, with a link to where it was built;
- give equivalent formulations, in terms of homotopy spheres;
- explain why each hypothesis is needed, with a counterexample for each;
- describe the analogous statements in other dimensions and who proved them;
- explain why topological and smooth three-manifolds are the same, so that Ricci flow can prove a topological theorem.
The shape of space
Space, on the largest scales, is modelled in cosmology as a three-dimensional manifold, and nothing in general relativity fixes its topology. It might be infinite, or it might be finite but without boundary, a closed three-manifold such as a torus or a quotient of the 3-sphere. If it is finite and smaller than the observable universe, light could reach us from the same region by different routes, and we would see repeated patterns. In the cosmic microwave background, the radiation from a sphere around us at the time it was emitted, a multiply connected space would show up as pairs of circles on the sky with matching temperature patterns, where the sphere of last scattering intersects its own translates under the deck group (7A.6 Covering Spaces). Neil Cornish, David Spergel and Glenn Starkman proposed this test in 1998.
The test has been applied with increasing precision. In 2003 Jean-Pierre Luminet and colleagues proposed that the Poincaré dodecahedral space, the homology sphere of 7A.8 Homology in Brief, could explain an observed weakness of large-angle correlations in the WMAP data (Nature, 2003). Searches for matched circles in the WMAP maps (Cornish, Spergel, Starkman and Komatsu, 2004, and later analyses) found none with radius larger than about , and the Planck collaboration's 2015 analysis found no evidence of non-trivial topology on scales smaller than roughly the distance to the last-scattering surface. So far, then, the observable universe looks simply connected, though space may still be a closed manifold too large for its topology to be seen. The candidates for its shape are exactly the three-manifolds this book and Book 10A describe.
Every word
| word | meaning | where |
|---|---|---|
| three-dimensional manifold | a Hausdorff, second countable space in which every point has a neighbourhood homeomorphic to | 7A.3 Manifolds and Surfaces |
| closed | compact, and without boundary | 7A.2 Compactness and Compactification, 7A.3 Manifolds and Surfaces |
| simply connected | path-connected, and every loop can be continuously shrunk to a point: | 7A.4 The Fundamental Group |
| homeomorphic | there is a continuous bijection with continuous inverse | 7A.1 Topological Spaces and Quotients |
| the 3-sphere | , equivalently , or the unit quaternions | 7A.2 Compactness and Compactification, 7A.6 Covering Spaces |
Equivalent forms. A closed three-manifold that is homotopy equivalent to is called a homotopy 3-sphere. A homotopy 3-sphere is simply connected, since is a homotopy invariant. Conversely, a closed simply connected three-manifold has and , generated by a map of degree (7A.8 Homology in Brief, last exercise), and Whitehead's theorem (a map between simply connected cell complexes inducing isomorphisms on all homology groups is a homotopy equivalence) shows that this map is a homotopy equivalence. So the conjecture can be stated as: every homotopy 3-sphere is homeomorphic to . It is also equivalent to: every closed three-manifold whose fundamental group is trivial is a sphere; or, using the results of Book 10A, every closed simply connected three-manifold admits a metric of constant positive curvature.
Why each hypothesis is needed
| drop | counterexample | why it fails |
|---|---|---|
| closed (allow non-compact) | simply connected and a three-manifold, but not compact, so not | |
| closed (allow boundary) | the closed ball | compact, simply connected, but it has a boundary |
| simply connected | , | closed, but has a non-contractible loop (7A.4 The Fundamental Group) |
| simply connected | lens spaces , | closed, with finite non-trivial (7A.6 Covering Spaces) |
| simply connected, replaced by homology | the Poincaré sphere | same homology as , but of order (7A.8 Homology in Brief) |
| dimension 3 (dimension 2) | none: true, by classification | the only closed simply connected surface is (7A.5 Computing π₁) |
The table shows which conditions do real work. Non-compact simply connected three-manifolds can be very strange: John Henry Constant Whitehead found in 1935 an open subset of , contractible but not homeomorphic to (the Whitehead manifold), while trying to prove the conjecture. Simple connectivity cannot be weakened to "has the homology of a sphere", by Poincaré's own example. Finite fundamental group is not enough either: the spherical space forms are all closed with finite , and Perelman's theorem includes the statement that they are the only ones (the elliptization conjecture, 10A.5 Thurston’s Eight Geometries).
Other dimensions
The generalized Poincaré conjecture asks, in each dimension , whether every closed manifold homotopy equivalent to is homeomorphic to . (For , simply connected is not enough, as shows, so the statement uses homotopy equivalence.)
- : true, by the classification of curves and surfaces (7A.3 Manifolds and Surfaces).
- : true. Stephen Smale proved it in 1961 (with John Stallings and Christopher Zeeman independently proving cases by other methods), using handle decompositions (7A.10 Morse Theory); there is so much room in high dimensions that handles can be cancelled. Smale received the Fields Medal in 1966.
- : true. Michael Freedman proved it in 1982, with entirely different, topological methods; Fields Medal 1986.
- : true. Perelman, 2002–03.
Smooth versus topological. In some dimensions the smooth version, "homeomorphic" replaced by "diffeomorphic", fails: John Milnor found in 1956 smooth manifolds homeomorphic but not diffeomorphic to , the exotic spheres. In dimension the smooth Poincaré conjecture is open: no one knows whether there is a smooth manifold homeomorphic but not diffeomorphic to . In dimension the question does not arise, as the next section explains. So dimension three was the last case of the topological conjecture to be settled, and in an important sense the hardest: the high dimensions have room for handle-cancelling tricks, dimension four allows Freedman's infinite constructions, and dimension three has neither (Figure 9.1).
Topological and smooth three-manifolds
The Ricci flow is a smooth tool: it differentiates a Riemannian metric, which requires a smooth structure on the manifold (8A.1 Smooth Structures, 9A.1 Riemannian Metrics and Model Spaces). The Poincaré conjecture is a topological statement. The bridge is a theorem special to low dimensions:
Every topological three-manifold has a smooth structure, unique up to diffeomorphism. Consequently, two smooth three-manifolds are homeomorphic if and only if they are diffeomorphic.
Edwin Moise proved in 1952 that every three-manifold can be triangulated, uniquely up to subdivision, and results of James Munkres and J. H. C. Whitehead (around 1960) convert triangulations into smooth structures and back (8A.1 Smooth Structures). So a closed simply connected topological three-manifold can be given a smooth structure, then a Riemannian metric (by a partition of unity, 8A.2 Partitions of Unity), and then the Ricci flow can be run. If the flow shows the smooth manifold is diffeomorphic to , it is in particular homeomorphic to . In dimension this bridge fails, which is one reason the smooth four-dimensional case is so different.
The proof, in outline, which the rest of the guide fills in: put a metric on and run the Ricci flow (11A.1 The Equation and Its First Solutions). It exists for a short time (11A.3 Short-Time Existence and Uniqueness) and may form singularities, where the curvature blows up (11B.4 Singularities). Perelman's entropy and noncollapsing estimates (12A.3 The 𝓦-Entropy, 12A.4 κ-Noncollapsing) show that near a singularity the flow looks like one of a short list of models: necks and caps (12B.1 κ-Solutions–12B.3 The Canonical Neighbourhood Theorem). Cut along the necks and glue in caps, surgery (12B.4 Surgery), and continue the flow (12B.5 Ricci Flow with Surgery for All Time). Because is simply connected, the flow with surgery becomes extinct in finite time (12C.2 Finite Extinction), and tracing the surgeries back shows that was a connected sum of spherical space forms and copies of ; simple connectivity leaves only (12C.1 Reading Off the Topology, 12C.3 The Poincaré Conjecture, Assembled).
History
Poincaré posed the question in 1904. Over the twentieth century many proofs were announced and withdrawn; Whitehead's 1935 attempt produced the Whitehead manifold, and the search drove much of three-manifold topology, from Dehn's lemma (proved by Christos Papakyriakopoulos in 1957) to Thurston's geometrization conjecture (1982), which contains the Poincaré conjecture (10A.5 Thurston’s Eight Geometries). Hamilton introduced the Ricci flow in 1982 and proposed it as a route to geometrization. Perelman posted his three preprints on the arXiv in November 2002, March 2003 and July 2003. Detailed expositions by Bruce Kleiner and John Lott, by John Morgan and Gang Tian, and by Huai-Dong Cao and Xi-Ping Zhu appeared in 2006–08. Perelman was awarded the Fields Medal in 2006 and the Clay Millennium Prize in 2010, and declined both.
The Poincaré conjecture: every closed, simply connected three-manifold is homeomorphic to ; equivalently, every homotopy 3-sphere is . Each hypothesis is needed: and are simply connected but not closed, and lens spaces are closed but not simply connected, and the Poincaré homology sphere shows homology is not enough. The analogous statements were proved in dimensions by Smale (1961), in dimension by Freedman (1982), and in dimension by Perelman (2002–03); the smooth four-dimensional case is open. In dimension three topological and smooth manifolds coincide (Moise), so the Ricci flow can prove the theorem. 7A.10 Morse Theory, optional, introduces Morse theory, the source of handle decompositions and Heegaard splittings.
Exercises
For each of , , , , and the Poincaré homology sphere, say which hypothesis of the conjecture fails, with a reference to the result that shows it.
Solution
and (7A.2 Compactness and Compactification): not compact. : (7A.4 The Fundamental Group). : (7A.6 Covering Spaces). : . Poincaré sphere: , order (7A.6 Covering Spaces, 7A.8 Homology in Brief).
(a) Show that a closed three-manifold homotopy equivalent to is simply connected. (b) Show that is a closed simply connected four-manifold that is not homotopy equivalent to (compare ). Why does the generalized conjecture in dimension use homotopy equivalence instead of simple connectivity?
Solution
(a) is a homotopy invariant and . (b) , but while . In dimension and above, simple connectivity doesn't control the middle homology, so the right hypothesis is that looks like a sphere to all homotopy invariants. In dimension , Poincaré duality and Hurewicz make simple connectivity enough (7A.8 Homology in Brief).
Write out the proof that a closed simply connected surface is homeomorphic to , citing 7A.3 Manifolds and Surfaces and 7A.5 Computing π₁. Why does no such list-and-check proof work in dimension three?
Suppose space is a flat 3-torus with smaller than twice the radius of the sphere of last scattering. Explain why the sphere of radius about the observer intersects its translate by in a circle, and why the temperature pattern along that circle is seen twice, in two opposite directions on the sky. What is the angular radius of each circle, in terms of ?
Solution
Two spheres of radius whose centres are apart meet in a circle, in the plane halfway between them; the points on it are seen from the observer along two different directions (one directly, one as the image of the translated copy), so the same physical points appear on two circles on the sky. The circle is at distance from the observer's centre along the axis, so its angular radius satisfies .
Suppose a closed three-manifold carries a Riemannian metric of constant curvature . Accept that its universal cover, with the pulled-back metric, is isometric to the round (a complete simply connected manifold of constant curvature is the round sphere, 9A.7 Jacobi Fields and Curvature versus Topology). (a) Show that , where acts on by isometries, freely (7A.6 Covering Spaces). (b) Conclude that if is simply connected, it is isometric, hence homeomorphic, to . Hamilton's 1982 theorem produces such a metric when has positive Ricci curvature (11A.6 Hamilton’s 1982 Theorem), and Perelman's proof reduces the general simply connected case to pieces of this kind (12C.3 The Poincaré Conjecture, Assembled).
Solution
(a) The deck group of the universal cover is (7A.6 Covering Spaces), it acts freely, and since the covering map is a local isometry the deck transformations are isometries of . (b) If , the covering has one sheet, so it is an isometry.
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