Low Dimensional Topology

March 5, 2012

Rethinking the basics

Filed under: Misc.,Quantum topology,Triangulations — dmoskovich @ 3:36 am

Some nights, one gazes up at the stars, and thinks about philosophy. Who are we? What is the meaning of life? What is reality? What are manifolds really?

This morning, I looked at Poincaré’s original definition in Papers on Topology: Analysis Situs and Its Five Supplements, translated by John Stillwell. His original definition was pretty-much that a manifold is a quotient of \mathbb{R}^n by a properly discontinuous group action, that group being his original fundamental group. Implicitly, his smooth, PL, and topological categories were all the same thing (indeed true for 1-manifolds, and for dimensions 2 and 3 PL and smooth categories still “coincide” in a sense that can be made fully precise); nowadays we understand that the situation is more subtle. But I’m still not sure that I understand what a manifold is- what it really is.

In some non-mathematical, philosophical (theological?) sense, I believe that both smooth and PL manifolds actually exist, in the sense that natural numbers exist, and tangles exist. Our clumsy formal definitions are attempts at describing something that is actually out there, as the Peano axioms describe the natural numbers. I also believe that Physics is a guide to Mathematics, because things that really exist might also be observed… so ideas from Physics (topological invariants defined by means of path integrals) ought to be taken very seriously, and it is my irrational belief that these will eventually turn out to be the most fundamental invariants in some precise mathematical sense.

It is fascinating to me, then, that input from physics seems to be leading towards a fundamental rethink of the basic definitions of smooth and PL manifolds. I feel like we had some sub-optimal definitions, which we worked with for sociological reasons (definitions are made by people, and people are not perfect), and maybe in the not too distant future there will be a chance to put more convenient definitions in place. Maybe the real world (physics) will force it on us. Let me tell you, then, about some of the papers I’ve been (casually) flicking through recently (the one I’m most excited about is Kirillov’s On piecewise linear cell decompositions).


Smooth manifolds

The definition of smooth manifolds has bothered me ever since these excellent slides from a talk by Oleg Viro did their job to make me feel uncomfortable.

The modern definition of differentiable manifolds appeared first in
The Foundations of Differential Geometry by Veblen and Whitehead, Cambridge University Press, 1932. It was inspired by a book on Riemann surfaces by Weyl. It’s an awful definition, really, in that it’s quite long, and it requires a choice of atlas, which plays no role in what follows and is ultimately done away with (in favour of a maximal atlas, perhaps). Worse still, the category of differentiable manifolds is not stable under basic set theoretical operations. This ought to especially bother quantum topologists, because the algebraic categories with which quantum invariants are defined do not reflect this instability. The image of a differentiable manifold under a differentiable map might not be a manifold. The space of maps between manifolds is not a manifold. If you slice up manifolds, as required to construct TQFT invariants, the pieces are not manifolds. Maybe worst of all (depending on your perspective), the most important functor in smooth topology, the tangent functor (which assigns tangent bundle TM to manifold M and map TM\to TN to map M\to N so that the obvious diagram commutes) is not a representable functor. I think that I believe Grothendieck’s assertion that useful functors should be representable, so this fact makes me most uncomfortable of all, in a strange sort of way.

The solution is surely to expand the category of manifolds which we consider. So a knot theorist perhaps thinks about tangles instead of knots, or maybe about virtual tangles (or even Dror’s w-knotted objects), and (in the world of manifolds) maybe we think about manifolds with corners, or, more ambitiously, stratified spaces. This lets us chop up manifolds, take quotients by group actions which we care about, contract loops to a point, and take covering spaces branched over graphs; which are all things I care about doing.

But what about spaces of diffeomorphisms between manifolds? Our category of smooth manifolds really ought to have exponential objects, in order to be a Cartesian closed category. I don’t understand enough to know why this would be useful concretely, but on the same fuzzy level with which I’ve been talking up until this point, diffeomorphism groups of manifolds are objects of obvious interest in geometric topology (the mapping class group is the group of connected components of the space of diffeomorphisms of the manifold, for example. Via Heegaard decompositions, a mapping class of a surface gives rise to a 3-manifold.) It would be nice to be able to discuss diffeomorphism groups on equal footing with smooth manifolds. Instead, they’re typically discussed in the context of tame Fréchet spaces, and the inverse function theorem gets generalized in a non-trivial way; it’s all a bit hard. I don’t know whether a larger category could make such theorems more convenient, or at least conceptually clarify what class of topological spaces we can expect them for, but it would be wonderful if it were so.

When we expand our category, perhaps we are throwing away “reality”… I don’t know. Natural numbers have some sort of metaphysical existence, I believe, and rational numbers sort-of still exist; but real numbers are an abstraction. In what sense can we claim that a number exists that we can never construct?

One interesting attempt to expand the category of smooth spaces to a cartesian closed category is Frölicher spaces. This approach, and the category of diffeologies, which is another good idea which is more general, are extensively discussed by experts at the n-Category Cafe. Philosophically, I don’t know whether or not these smooth spaces “exist” in any Platonic metaphysical sense; but cartesian closedness might be worth a bit of abstraction.

But what about representability of the tangent functor? Here’s where another mesmerizingly beautiful idea comes into play. Synthetic differential geometry. I’d love to talk about it, and I really should (especially if there are genuine links to proper low dimensional topology, which one can exploit); in a nutshell of a nutshell, or “on one leg” as we say in Hebrew, you trade sets for topoi to get a version of smooth topology (and differential geometry) in which infinitesmals in the Liebnitz sense exist, and you have \epsilon\neq 0 for which \epsilon^2=0. Words like “topos” sound complicated, but actually the core idea meshes well with our naive intuition as humans (although not with our mathematical training)- is it really such a stretch to imagine a circle intersecting its “tangent line” along an infinitesmal line rather than a point? Or to have an infinitesmally small n-manifold for each n?

Synthetic differential geometry makes the tangent functor representable. So what is the ultimately real higher-realm Platonic category of smooth spaces? Perhaps some sort of category of synthetic Frölicher spaces? Or maybe even synthetic diffeologies?

It turns out that people are thinking hard about such questions, and my imagination soars as a read the preprints of Hirokazu Nishimura on the topic. And surely, Andrew Stacey is working on similar things, and perhaps many others. Perhaps the true smooth world will reveal itself to mankind soon- and if so, how I would delight to lay eyes on it!


PL manifolds

In the previous section, I revealed my discomfort with the definition of smooth manifolds. Do I find PL manifolds to be any better?

Let’s briefly recall the definition. An n-simplex \Delta_n is the convex hull of n+1 points in \mathbb{R}^n which do not all lie on a common hyperplace. We say that K\subset \mathbb{R}^n is a polyhedron if, for each point x\in K, there exist a finite number of simplexes whose union contains a neighbourhood of x. Polyhedron M is said to be a PL manifold if, for every point x\in M, there exists a neighbourhood U\subset M of x and a PL homeomorphism U\simeq \mathbb{R}^n. So a PL manifold is one which can be chopped up into simplices (higher dimensional generalizations of triangles), which makes the category of PL manifolds really discrete and combinatorial.

Any PL manifold has a triangulation (a decomposition into simplices); actually it has infinitely many of them, because any simplex can be chopped up into smaller simplices (a refinement of the triangulation). The Hauptvermutung, which for n-manifolds is true for n\leq 3 and false for n\geq 4, states that any two triangulations of a PL manifold share a common refinement. PL manifolds with a common refinement are said to be combinatorially equivalent.

Recall that the star S_\Delta of simplex \Delta is the union of all (closed) simplices containing \Delta. Given a triangulation, you can replace star S_\Delta by the cone over the boundary of S_\Delta centred at a point p\in \Delta. Such a move is called a stellar move. Alexander’s theorem says that any two combinatorially equivalent triangulations of a PL manifold are related by a sequence of stellar moves and their inverses. Actually, each stellar move can be realized as a sequence of simpler “bistellar” or Pachner moves by a fundamental theorem of Pachner.

A PL manifold isn’t trying to be abstract- it’s a lego structure built up block by block, where the lego blocks are simplices. Alexander’s Theorem, and Pachner’s Theorem, then give us a framework in which to relate manifolds, and their invariants, which were constructed simplex by simplex.

This looks nice, but from the point of view of this post this is horrible- triangulations aren’t preserved under anything! Consider the product of two triangulated manifolds- say, the product of two line segments [0,1]\times [0,1], each divided into subsegments [0,\frac{1}{2}]\cup_{\{\frac{1}{2}\}} [\frac{1}{2},1]\simeq [0,1]. The square that is their product isn’t triangulated- instead, it’s partitioned into four smaller squares. Worse, the dual complex (0-simplex for n-simplex, 1-simplex between 0-simplices if corresponding n-simplices share an (n-1)-face \ldots) for an n-manifold with boundary isn’t a triangulation. For Poincaré duality you need this complex, so obviously something is philosophically wrong.

So, along comes Whitehead, and he defines CW complexes, which are what we use when we teach courses on this stuff. Now, you’re gluing together closed balls B^n\subset \mathbb{R}^n instead of simplices. The maps f\colon\, B^n\to M are required to satisfy:

  • The restriction of f to the interior of B^n is a homeomorphism onto its image.
  • The image under f of \partial B^n is contained in the union of a finite number of elements of the partition, each having cell dimension less than n.

In particular, you can connect blocks by some crazy continuous function (rather than just slotting together simplexes by the identity), and you can build all sorts of monstousities as CW complexes. From our perspective, though, the more serious problem is that there is no known analogue to Alexander’s Theorem, meaning that the CW decomposition is, in one sense, annoying extra data which we don’t really care about, and that if we use it to construct an invariant, we cannot then prove that the invariant is independent of the cellular decomposition.

People have realized that there is something amiss about this state of affairs at least since the 1950′s (Gugenheim). But, through inertia I suppose, it has never been rectified. One can get away with such things for quite a long time. Take products, then triangulate. Build as CW complexes, then triangulate. But in quantum topology, you are constructing invariants simplex by simplex, one simplex at a time, and having to work with huge numbers of simplexes and retriangulate every 5 seconds is seriously annoying. It’s actually even worse than that. If you want to construct extended TQFT, some of the most fundamental cells to consider are digons.

A paper I’m looking at, and which I’m currently quite excited about, is On piecewise linear cell decompositions by Alexander Kirillov. Motivated by (tremendously interesting) work with his student Benjamin Balsam (a must read paper, by the way), Kirillov defines a more modest generalization of simplicial decomposition, which he calls PLCW decomposition (I suggest PW decomposition as shorter, hence better). He defines a regular map as a PL map f\colon\, C\to \mathbb{R}^n from convex compact polyhedron C (a cell), such that the restriction of f to the interior of C is injective. In particular, f can glue pieces of the boundary of C together.

A PLCW complex is now defined inductively by starting with an (n-1)-dimensional PLCW skeleton, and attaching n-cells, such that the restriction to their boundary is a regular map. This is a simple and a natural enough condition that I can well-believe that such structures exist in some metaphysical sense. A product of PLCW decompositions is again a PLCW decomposition, and we have all of the cells that we want.

Another suggestion that PLCW is the way to go is the version of Alexander’s Theorem that is proven in the paper (I casually wonder about a Pachner Theorem). Stellar moves have natural analogues for PLCW complexes, and any two combinatorially equivalent PW (PLCW) decompositions are related by these moves.

The paper really is a joy to read, because it’s written so clearly, and the objects it considers are so intuitively natural. Why was it not written 70 years ago? I don’t know. But better late than never. The idea of PLCW decompositions is really cool, and I would love for it to enter into the topological mainstream!

11 Comments »

  1. I’m pretty sure the idea of PL CW complexes is an idea that goes back to near the beginning of CW complexes. When I have time I’ll look it up, but I’m pretty sure I’ve cited some references on PL CW complexes in either my first or 2nd paper, and they were quite old references at the time.

    Yes, here is a reference from Cohen-Metzler-Sauermann 1985 on PLCW’s: Contemporary Mathematics 85 page 6 “Collapses of KxI and group presentations”. I suspect PLCWs are older than this reference, though.

    Comment by Ryan Budney — March 5, 2012 @ 3:50 pm | Reply

    • That is wonderful!! I’ll have a look at the paper.

      It’s not unusual for good ideas to be forgotten and rediscovered, perhaps many times… certainly the idea of a PLCW complex is so natural that it would be strange if nobody had thought about them earlier. It makes me happy that this turns out to indeed have been the case. I think that the way that they are now arising, as a cell decomposition of a manifold dictated by an extended TQFT, guarantees that they are here to stay.

      Added: It turns out that PLCW complexes in the sense of the Cohen-Metzler-Sauermann paper (called a “membrane complex” by Whitehead) is not the same as a PLCW complex in the sense of Kirillov. Their PLCW complexes (membrane complexes) are just CW complexes in the PL category- in particular, you can’t glue together different faces of a cell, which you can do in PLCW complexes. The membrane complex definition is of a CW complex, with the condition that the attaching map \phi makes the closure of the cell homeomorphic rel boundary to D^n\cup_{\partial D^n}C(\phi) where C(\phi) is the PL mapping cylinder of \phi. For Kirillov’s complexes, the requirement is instead that the attaching map be regular, which rules out strange CW attaching maps, but allows faces of the same cell to be glued to one another. Perhaps I can feed this into my confirmation bias that Kirillov’s PLCW complexes should be called PW complexes, if only to avoid this confusion of terminology.

      Comment by dmoskovich — March 5, 2012 @ 6:37 pm | Reply

  2. Hi Daniel,

    Are you sure about that? I think RP^2 with its standard cell structure (one cell in each dimension) is a PLCW in the Cohen-Metzler-Sauermann sense, which in effect means you’re taking a 2-cell and modding out by the antipodal map on the boundary. I’d call that gluing faces of a cell.

    Unfortunately I’m pretty swamped right now, but in the next week I’ll try and sit-down and compare the two definitions.

    Comment by Ryan Budney — March 5, 2012 @ 9:53 pm | Reply

  3. I had a closer look at Kirillov’s paper. His definition appears to be essentially equivalent to Cohen-Metzler-Sauermann. Or am I missing something?

    Comment by Ryan Budney — March 5, 2012 @ 11:53 pm | Reply

    • I should admit I was not familiar with the Cohen-Metzler-Sauermann paper when writing thsi note – thanks for bringing it to my attention. I’ll try to figure out what the relation between our definitions is. However, for me the most important part is the analog of Alexander’s theorem, on moves allowing to get from one PLCW decomposition to another – did they have an analog of this?

      Alexander Kirillov

      Comment by Alexander Kirillov — March 12, 2012 @ 11:05 am | Reply

  4. I never understand the objection that

    The space of maps between manifolds is not a manifold.

    The space of homomorphisms between groups is almost never itself a group. Does this mean that the definition of a group is somehow inadequate?

    Comment by Henry Wilton — March 6, 2012 @ 7:25 am | Reply

    • Does this mean that the definition of a group is somehow inadequate?

      Perhaps yes. There is an argument to be made that what in-fact occurs in nature is the category of groupoids, not groups (fundamental groupoids, Lie groupoids, and so on). The category of groupoids is cartesian closed. The argument continues that groups are merely a computationally simple subcategory which we have gotten used to using, and which many groupoid problems can be reduced to by arbitrarily fixing a basepoint.

      Comment by dmoskovich — March 6, 2012 @ 9:46 am | Reply

      • The category of groupoids will do? That’s not too bad! Though I’ll probably stick to groups for now, pace Ronnie Brown.

        Comment by Henry Wilton — March 6, 2012 @ 10:06 am

  5. I view these objections to the foundations of manifold theory as not terribly relevant to manifold theory itself. These objections come from the perspective that somehow category theory, and generally more combinatorial manipulations are what one wants (in Viro’s talk, due to the nature of the invariants he likes to work with). But that kind of ignores the whole spirit and point of the definition of manifolds. Manifolds are designed to be homogeneous objects, so by design any kind of combinatorial framework on them is an imposition and to some extent unnatural. The manifold idea is designed to be something that’s awkward and tricky to get one’s hands on, in a sense manifolds were meant to be an archetypal example of something mathematics has a hard time dealing with. In that regard I don’t think there’s anything wrong with the foundations of manifold theory. I feel a little like VIro’s talk and this thread is more representative of the general angst one gets when one tries to deal with an issue that by its very nature refuses to sit convieniently in the formal frameworks one might prefer to think in. People in more applied subjects tend to be more at ease with this kind of awkwardness. IMO this is a healthy way to live as a mathematician.

    Comment by Ryan Budney — March 9, 2012 @ 5:07 pm | Reply

    • As you say, whether or not the foundations of manifold theory are optimal seems to depend on one’s perspective. In quantum topology, invariants are obtained as maps from cobordism categories to algebraic categories. The algebraic categories admit certain structures (ribbon Hopf algebras, for example), but it’s not clear a-priori why the cobordism categories should admit corresponding combinatorial structures. If one believes that physics is a guiding light for mathematics, then this implies that we should reformulate the construction of the cobordism categories so that they do admit these extra structures… find a collection of basic building blocks, and relations between different ways of gluing them together, which parallel the objects and relations in the algebraic category (as has already been done in the case of surfaces). Certainly you’d need manifolds with corners, and you’d want to equip them with some extra structure to make the gluing work as you want it to.

      How any of this would mesh with existing 3-manifold theory looks completely mysterious to me, most fundamentally because I don’t know what the optimal cobordism category for 3-dimensional quantum topology would look like. The philosophical belief that “when physics contradicts mathematics, it is mathematics that should change”, though, gives me blind faith that the combinatorial picture, with its gluing of blocks, will eventually be linked in with geometrization and other classical topics, in which the algebraic structures in play look quite different.

      Comment by dmoskovich — March 10, 2012 @ 11:00 pm | Reply

  6. I’d agree physics is one of *many* guiding lights for mathematics, but the frequency with which that light is used really depends on the mathematics and in this case, the physics as well. In particular, physics (like mathematics) does not speak with one voice so singling-out one message from physics as “the message” is hard for me to swallow. Mathematics is by and large guided by all the sciences. Biology seems to be flaring up as the go-to influence nowadays and in the near future. I think much of manifold theory developed largely independently of physics — many of the key contributors were certainly aware of physics but the degree of influence depends on the person.

    Comment by Ryan Budney — March 11, 2012 @ 9:28 pm | Reply


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