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A few weeks ago, Ian Agol, Vlad Markovic, Ursula Hamenstadt and I organized a “hot topics” workshop at MSRI with the title Surface subgroups and cube complexes. The conference was pretty well attended, and (I believe) was a big success; the organizers clearly deserve a great deal of credit. The talks were excellent, and touched on a wide range of subjects, and to those of us who are mid-career or older it was a bit shocking to see how quickly the landscape of low-dimensional geometry/topology and geometric group theory has been transformed by the recent breakthrough work of (Kahn-Markovic-Haglund-Wise-Groves-Manning-etc.-) Agol. Incidentally, when I first started as a graduate student, I had a vague sense that I had somehow “missed the boat” — all the exciting developments in geometry due to Thurston, Sullivan, Gromov, Freedman, Donaldson, Eliashberg etc. had taken place 10-20 years earlier, and the subject now seemed to be a matter of fleshing out the consequences of these big breakthroughs. 20 years and several revolutions later, I no longer feel this way. (Another slightly shocking aspect of the workshop was for me to realize that I am older or about as old as 75% of the speakers . . .)
The rationale for the workshop (which I had some hand in drafting, and therefore feel comfortable quoting here) was the following:
Recently there has been substantial progress in our understanding of the related questions of which hyperbolic groups are cubulated on the one hand, and which contain a surface subgroup on the other. The most spectacular combination of these two ideas has been in 3-manifold topology, which has seen the resolution of many long-standing conjectures. In turn, the resolution of these conjectures has led to a new point of view in geometric group theory, and the introduction of powerful new tools and structures. The goal of this conference will be to explore the further potential of these new tools and perspectives, and to encourage communication between researchers working in various related fields.
I have blogged a bit about cubulated groups and surface subgroups previously, and I even began this blog (almost 4 years ago now) initially with the idea of chronicling my efforts to attack Gromov’s surface subgroup question. This question asks the following:
Gromov’s Surface Subgroup Question: Does every one-ended hyperbolic group contain a subgroup which is isomorphic to the fundamental group of a closed surface of genus at least 2?
The restriction to one-ended groups is just meant to rule out silly examples, like finite or virtually cyclic groups (i.e. “elementary” hyperbolic groups), or free products of simpler hyperbolic groups. Asking for the genus of the closed surface to be at least 2 rules out the sphere (whose fundamental group is trivial) and the torus (whose fundamental group cannot be a subgroup of a hyperbolic group). It is the purpose of this blog post to say that Alden Walker and I have managed to show that Gromov’s question has a positive answer for “most” hyperbolic groups; more precisely, we show that a random group (in the sense of Gromov) contains a surface subgroup (in fact, many surface subgroups) with probability going to 1 as a certain natural parameter (the “length”
of the random relators) goes to infinity. (update April 8: the preprint is available from the arXiv here.)
There is an old puzzle which starts by asking: what is the next number in the sequence 1,2,4,? We are supposed to recognize the start of the sequence and answer that the next number is surely 8, because the first three numbers are consecutive powers of 2, and so the next number should be the cube of 2 which is 8. The puzzler then explains (contrary to expectations) that the successive terms in the sequence are actually the number of regions into which the plane is divided by a collection of lines in general position (so that any two lines intersect, and no three lines intersect in a single point). Thus:
So the “correct” answer to the puzzle is 7 (and the sequence continues 11, 26, ). This is somehow meant to illustrate some profound point; I don’t quite see it myself. Anyway, I would like to suggest that there is a natural sense in which the “real” answer should actually be 8 after all, and it’s the point of this short blog post to describe some connections between this puzzle, the theory of cube complexes (which is at the heart of Agol’s recent proof of the Virtual Haken Conjecture), and the location of the missing 8th region.
Let be the free group on two generators, and let
be the endomorphism defined on generators by
and
. We define Sapir’s group
to be the ascending HNN extension
This group was studied by Crisp-Sageev-Sapir in the context of their work on right-angled Artin groups, and independently by Feighn (according to Mark Sapir); both sought (unsuccessfully) to determine whether contains a subgroup isomorphic to the fundamental group of a closed, oriented surface of genus at least 2. Sapir has conjectured in personal communication that
does not contain a surface subgroup, and explicitly posed this question as Problem 8.1 in his problem list.
After three years of thinking about this question on and off, Alden Walker and I have recently succeeded in finding a surface subgroup of , and it is the purpose of this blog post to describe this surface, how it was found, and some related observations. By pushing the technique further, Alden and I managed to prove that for a fixed free group
of finite rank, and for a random endomorphism
of length
(i.e. one taking the generators to random words of length
), the associated HNN extension contains a closed surface subgroup with probability going to 1 as
. This result is part of a larger project which we expect to post to the arXiv soon.
Ian gave his second and third talks this afternoon, completing his (quite detailed) sketch of the proof of the Virtual Haken Theorem. Recall that after work of Kahn-Markovic, Wise, Haglund-Wise and Bergeron-Wise, the proof reduces to showing the following:
Theorem (Agol): Let G be a hyperbolic group acting properly discontinuously and cocompactly on a CAT(0) cube complex X. Then there is a finite index subgroup G’ so that X/G’ is special; in other words, G is virtually special.
Today Jason Manning gave a talk on a vital ingredient in the proof of Agol’s theorem, which is a result in geometric group theory. The theorem is a joint project of Agol-Groves-Manning, and generalizes some earlier work they did a few years ago. Jason referred to the main theorem during his talk as the “Goal Theorem” (I guess it was the goal of his lecture), but I’m going to call it the Weak Separation Theorem, since that is a somewhat more descriptive name. The statement of the theorem is as follows.
Weak Separation Theorem (Agol-Groves-Manning): Let G be a hyperbolic group, let H be a subgroup of G which is quasiconvex, and isomorphic to the fundamental group of a virtually special NPC cube complex, and let g be an element of G which is not contained in H. Then there is a surjection so that
is hyperbolic;
is finite; and
is not contained in
.
In the remainder of this post I will try to explain the proof of this theorem, to the extent that I understand it. Basically, this amounts to my summarizing Manning’s talk (or the part of it that I managed to get down in my notes); again, any errors, foolishness, silly blog post titles etc. are due to me.
I am in Paris attending a workshop at the IHP where Ian Agol has just given the first of three talks outlining his proof of the Virtual Haken Conjecture and Virtual Fibration Conjecture in 3-manifold topology (hat tip to Henry Wilton at the Low Dimensional Topology blog from whom I first learned about Ian’s announcement last week). I think it is no under overstatement to say that this marks the end of an era in 3-manifold topology, since the proof ties up just about every loose end left over on the list of problems in 3-manifold topology from Thurston’s famous Bulletin article (with the exception of problem 23 — to show that volumes of closed hyperbolic 3-manifolds are not rationally related — which is very close to some famous open problems in number theory). The purpose of this blog post is to say what the Virtual Haken Conjecture is, and some of the background that goes into Ian’s argument. I hope to follow this up with more details in another post (after Agol gives talks 2 and 3 this coming Wednesday). Needless to say this post has been written in a bit of a hurry, and I have probably messed up some crucial details; but if that caveat is not enough to dissuade you, then read on.
The purpose of this blog post is to try to give some insight into the “meaning” of the Hall-Witt identity in group theory. This identity can look quite mysterious in its algebraic form, but there are several ways of describing it geometrically which are more natural and easier to understand.
If is a group, and
are elements of
, the commutator of
and
(denoted
) is the expression
(note: algebraists tend to use the convention that
instead). Commutators (as their name suggests) measure the failure of a pair of elements to commute, in the sense that
. Since
, the property of being a commutator is invariant under conjugation (here the superscript
means conjugation by
; i.e.
; again, the algebraists use the opposite convention).
1. Mostow Rigidity
For hyperbolic surfaces, Moduli space is quite large and complicated. However, in three dimensions Moduli space is trivial:
Theorem 1 If
is a homotopy equivalence of closed hyperbolic
manifolds with
, then
is homotopic to an isometry.
In other words, Moduli space is a single point.
This post will go through the proof of Mostow rigidity. Unfortunately, the proof just doesn’t work as well on paper as it does in person, especially in the later sections.
1.1. Part 1
First we need a definition familiar to geometric group theorists: a map between metric spaces (not necessarily Riemannian manifolds) is a
quasi-isometry if for all
, we have
Without the term,
would be called bilipschitz.
First, we observe that if is a homotopy equivalence, then
lifts to a map
in the sense that
is equivariant with respect to
(thought of as the desk groups of
and
, so for all
, we have
.
Now suppose that and
are hyperbolic. Then we can lift the Riemannian metric to the covers, so
and
are specific discrete subgroups in
, and
maps
equivariantly with respect to
and
.
Lemma 2
is a quasi-isometry.
Proof: Since is a homotopy equivalence, there is a
such that
. Perturbing slightly, we may assume that
and
are smooth, and as
and
are compact, there exists a constant
such that
and
. In other words, paths in
and
are stretched by a factor of at most
: for any path
,
. The same is true for
going in the other direction, and because we can lift the metric, the same is true for the universal covers: for any path
,
, and similarly for
.
Thus, for any in the universal cover
,
and
We see, then, that is Lipschitz in one direction. We only need the
for the other side.
Since , we lift it to get an equivariant lift
For any point
, the homotopy between
gives a path between
and
. Since this is a lift of the homotopy downstairs, this path must have bounded length, which we will call
. Thus,
Putting these facts together, for any in
,
And
By the triangle inequality,
This is the left half of the quasi-isometry definition, so we have shown that is a quasi-isometry.
Notice that the above proof didn’t use anything hyperbolic—all we needed was that and
are Lipschitz.
Our next step is to prove that a quasi-isometry of hyperbolic space extends to a continuous map on the boundary. The boundary of hyperbolic space is best thought of as the boundary of the disk in the Poincare model.
Lemma 3 A
quasi-isometry
extends to a continuous map on the boundary
.
The basic idea is that given a geodesic, it maps under to a path that is uniformly close to a geodesic, so we map the endpoints of the first geodesic to the endpoints of the second. We first need a sublemma:
Lemma 4 Take a geodesic and two points
and
a distance
apart on it. Draw two perpendicular geodesic segments of length
from
and
. Draw a line
between the endpoints of these segments such that
has constant distance from the geodesic. Then the length of
is linear in
and exponential in
.
Proof: Here is a representative picture:

So we see that . By Gauss-Bonnet,
Where the on the left is the sum of the turning angles, and
is the geodesic curvature of the segment
. What is this geodesic curvature
? If we imagine increasing
, then the derivative of the length
with respect to
is the geodesic curvature
times the length
, i.e.
So . Therefore, by the Gauss-Bonnet equality,
so . Therefore,
, which proves the lemma
With this lemma in hand, we move on the next sublemma:
Lemma 5 If
is a
quasi-isometry, there is a constant
depending only on
and
such that for all
on the geodesic from
to
in
,
is distance less than
from any geodesic from
to
.
Proof: Fix some , and suppose the image
of the geodesic
from
to
goes outside a
neighborhood of the geodesic
from
to
. That is, there is some segment
on
between the points
and
such that
maps completely outside the
neighborhood.

Let’s look at the nearest point projection from
to
. By the above lemma,
. Thus means that
On the other hand, because is a quasi-isometry,
and
So we have
Which implies that
That is, the length of the offending path is uniformly bounded. Thus, increase
by
times this length plus
, and every offending path will now be inside the new
neighborhood of
.
The last lemma says that the image under of a geodesic segment is uniformly close to an actual geodesic. Now suppose that we have an infinite geodesic in
. Take geodesic segments with endpoints going off to infinity. There is a subsequence of the endpoints converging to a pair on the boundary. This is because the visual distance between successive pairs of endspoints goes to zero. That is, we have extended
to a map
, where
is the diagonal
. This map is actually continuous, since by the same argument geodesics with endpoints visually close map (uniformly close) to geodesics with visually close endpoints.
1.2. Part 2
Now we know that a quasi-isometry extends continuously to the boundary of hyperbolic space. We will end up showing that
is conformal, which will give us the theorem.
We now introduce the Gromov norm. if is a topological space, then singular chain complex
is a real vector space with basis the continuous maps
. We define a norm on
as the
norm:
This defines a pseudonorm (the Gromov norm) on by:
This (pseudo) norm has some nice properties:
Lemma 6 If
is continuous, and
, then
.
Proof: If represents
, then
represents
.
Thus, we see that if is a homotopy equivalence, then
.
If is a closed orientable manifold, then we define the Gromov norm of
to be the Gromov norm
.
Here is an example: if admits a self map of degree
, then
. This is because we can let
represent
, so
, so
represents
. Thus
. Notice that we can repeat the composition with
to get that
is as small as we’d like, so it must be zero.
Theorem 7 (Gromov) Let
be a closed oriented hyperbolic
-manifold. Then
. Where
is a constant depending only on
.
We now go through the proof of this theorem. First, we need to know how to straighten chains:
Lemma 8 There is a map
(the second complex is totally geodesic simplices) which is
-equivariant and
– equivariantly homotopic to
.
Proof: In the hyperboloid model, we imagine a simplex mapping in to . In
, we can connect its vertices with straight lines, faces, etc. These project to being totally geodesics in the hyperboloid. We can move the original simplex to this straightened one via linear homotopy in
; now project this homotopy to
.
Now, if represents
, then we can straighten the simplices, so
represents
, and
, so when finding the Gromov norm
it suffices to consider geodesic simplices. Notice that every point has finitely many preimages, and total degree is 1, so for any point
,
.
Next, we observe:
Lemma 9 If given a chain
, there is a collection
such that
and
is a cycle homologous to
.
Proof: We are looking at a real vector space of coefficients, and the equations defining what it means to be a cycle are rational. Rational points are therefore dense in it.
By the lemma, there is an integral cycle , where
is some constant. We create a simplicial complex by gluing these simplices together, and this complex comes together with a map to
. Make it smooth. Now by the fact above,
, so
. Then
on the one hand, and on the other hand,
The volume on the right is at most , the volume of an ideal
simplex, so we have that
i.e.
This gives the lower bound in the theorem. To get an upper bound, we need to exhibit a chain representing with all the simplices mapping with degree 1, such that the volume of each image simplex is at least
.
We now go through the construction of this chain. Set , and fix a fundamental domain
for
, so
is tiled by translates of
. Let
be the set of all simplices with side lengths
with vertices in a particular
-tuple of fundamental domains
. Pick
to be a geodesic simplex with vertices
, and let
be the image of
under the projection. This only depends on
up to the deck group of
.
Now define the chain:
With the to make it orientation-preserving, and where
is an
-invariant measure on the space of regular simplices of side length
. If the diameter of
is
every simplex with
has edge length in
, so:
- The volume of each simplex is
if
is large enough.
is finite — fix a fundamental domain; then there are only finitely many other fundamental domains in
.
Therefore, we just need to know that is a cycle representing
: to see this, observe that every for every face of every simplex, there is an equal weight assigned to a collection of simplices on the front and back of the face, so the boundary is zero.
By the equality above, then,
Taking to zero, we get the theorem.
1.3. Part 3 (Finishing the proof of Mostow Rigidity
We know that for all , there is a cycle
representing
such that every simplex is geodesic with side lengths in
, and the simplices are almost equi-distributed. Now, if
, and
represents
, then
represents
, as
is a homotopy equivalence.
We know that extends to a map
. Suppose that there is an
tuple in
which is the vertices of an ideal regular simplex. The map
takes (almost) regular simplices arbitrarily close to this regular ideal simplex to other almost regular simplices close to an ideal regular simplex. That is,
takes regular ideal simplices to regular ideal simplices. Visualizing in the upper half space model for dimension 3, pick a regular ideal simplex with one vertex at infinity. Its vertices form an equilateral triangle in the plane, and
takes this triangle to another equilateral triangle. We can translate this simplex around by the set of reflections in its faces, and this gives us a dense set of equilateral triangles being sent to equilateral triangles. This implies that
is conformal on the boundary. This argument works as long as the boundary sphere is at least 2 dimensional, so this works as long as
is 3-dimensional.
Now, as is conformal on the boundary, it is a conformal map on the disk, and thus it is an isometry. Translating, this means that the map conjugating the deck group
to
is an isometry of
, so
is actually an isometry, as desired. The proof is now complete.


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