<?xml version="1.0" encoding="UTF-8" standalone="yes"?><oembed><version><![CDATA[1.0]]></version><provider_name><![CDATA[Geometry and the imagination]]></provider_name><provider_url><![CDATA[https://lamington.wordpress.com]]></provider_url><author_name><![CDATA[Danny Calegari]]></author_name><author_url><![CDATA[https://lamington.wordpress.com/author/dannycaltech/]]></author_url><title><![CDATA[Random groups contain surface&nbsp;subgroups]]></title><type><![CDATA[link]]></type><html><![CDATA[<p>A few weeks ago, Ian Agol, Vlad Markovic, Ursula Hamenstadt and I organized a &#8220;hot topics&#8221; workshop at MSRI with the title <a href="http://www.msri.org/web/msri/scientific/show/-/event/Wm9922"><em>Surface subgroups and cube complexes</em></a>. 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 &#8220;missed the boat&#8221; &#8212; 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 . . .)</p>
<p>The rationale for the workshop (which I had some hand in drafting, and therefore feel comfortable quoting here) was the following:</p>
<blockquote><p>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.</p></blockquote>
<p>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&#8217;s surface subgroup question. This question asks the following:</p>
<p style="padding-left:30px;"><strong>Gromov&#8217;s Surface Subgroup Question:</strong> 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?</p>
<p>The restriction to one-ended groups is just meant to rule out silly examples, like finite or virtually cyclic groups (i.e. &#8220;elementary&#8221; 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 <img src="https://s0.wp.com/latex.php?latex=%5Cmathbb%7BZ%7D%5E2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathbb{Z}^2" title="&#92;mathbb{Z}^2" class="latex" /> 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&#8217;s question has a positive answer for &#8220;most&#8221; 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 &#8220;length&#8221; <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" /> of the random relators) goes to infinity. <strong>(update April 8:</strong> the preprint is available from the arXiv <a href="http://arxiv.org/abs/1304.2188">here</a>.<strong>)</strong></p>
<p><!--more--></p>
<p>First let&#8217;s start with the precise definition of a random group. There are actually two parameters in the definition &#8212; the <em>density</em> <img src="https://s0.wp.com/latex.php?latex=D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D" title="D" class="latex" /> and the <em>length</em> <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" />. A random group at density <img src="https://s0.wp.com/latex.php?latex=D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D" title="D" class="latex" /> and length <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" /> is obtained by fixing a finite generating set <img src="https://s0.wp.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S" title="S" class="latex" /> with at least 2 elements, and adding &#8220;random&#8221; reduced words <img src="https://s0.wp.com/latex.php?latex=R%3D%5Clbrace+r_i%5Crbrace&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="R=&#92;lbrace r_i&#92;rbrace" title="R=&#92;lbrace r_i&#92;rbrace" class="latex" /> of length <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" /> as relators, where the number of relators to add is governed by the density <img src="https://s0.wp.com/latex.php?latex=D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D" title="D" class="latex" />. Precisely, <img src="https://s0.wp.com/latex.php?latex=D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D" title="D" class="latex" /> is the <em>multiplicative density</em> of the relators. There are (approximately) <img src="https://s0.wp.com/latex.php?latex=%282k-1%29%5En&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="(2k-1)^n" title="(2k-1)^n" class="latex" /> cyclically reduced words of length <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" />, so we choose <img src="https://s0.wp.com/latex.php?latex=%282k-1%29%5E%7BDn%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="(2k-1)^{Dn}" title="(2k-1)^{Dn}" class="latex" /> subwords, independently and with the uniform measure, as our relators <img src="https://s0.wp.com/latex.php?latex=r_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r_i" title="r_i" class="latex" />, and then define <img src="https://s0.wp.com/latex.php?latex=G+%3D+%5Clangle+S+%5C%3B+%7C+%5C%3B+R%5Crangle&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G = &#92;langle S &#92;; | &#92;; R&#92;rangle" title="G = &#92;langle S &#92;; | &#92;; R&#92;rangle" class="latex" /> to be our &#8220;random group&#8221;.</p>
<p>Gromov introduced random groups and established some of their basic properties. One talks about a random group <em>at density</em> <img src="https://s0.wp.com/latex.php?latex=D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D" title="D" class="latex" />, and says that it has a certain property <em>with overwhelming probability</em>. What this means is that with fixed <img src="https://s0.wp.com/latex.php?latex=D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D" title="D" class="latex" />, the probability that the property holds goes to 1 as <img src="https://s0.wp.com/latex.php?latex=n+%5Cto+%5Cinfty&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n &#92;to &#92;infty" title="n &#92;to &#92;infty" class="latex" />. Gromov showed that there is a remarkable phase transition in this definition. Explicitly, he showed:</p>
<p style="padding-left:30px;"><strong>Theorem (Gromov):</strong> A random group has the following properties with overwhelming probability:</p>
<p style="padding-left:60px;">1. At <img src="https://s0.wp.com/latex.php?latex=D%3E1%2F2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D&gt;1/2" title="D&gt;1/2" class="latex" /> the group is either trivial or isomorphic to <img src="https://s0.wp.com/latex.php?latex=%5Cmathbb%7BZ%7D%2F2%5Cmathbb%7BZ%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathbb{Z}/2&#92;mathbb{Z}" title="&#92;mathbb{Z}/2&#92;mathbb{Z}" class="latex" />;</p>
<p style="padding-left:60px;">2. At <img src="https://s0.wp.com/latex.php?latex=D%3C1%2F2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D&lt;1/2" title="D&lt;1/2" class="latex" /> the group is infinite, hyperbolic, and 2-dimensional; and</p>
<p style="padding-left:60px;">3. At <img src="https://s0.wp.com/latex.php?latex=D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D" title="D" class="latex" /> the group satisfies the small cancellation condition <img src="https://s0.wp.com/latex.php?latex=C%27%282D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C&#039;(2D)" title="C&#039;(2D)" class="latex" />.</p>
<p>The story at density <img src="https://s0.wp.com/latex.php?latex=D%3D1%2F2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D=1/2" title="D=1/2" class="latex" /> is more subtle, and it is not so clear what happens, as far as I know. <strong>(</strong><strong>update April 6: </strong>Piotr Przytycki points out that the one-endedness of random groups is actually due to Dahmani-Guirardel-Przytycki. Thanks Piotr!<strong>)</strong></p>
<p>With this definition, the main theorem Alden and I prove is the following:</p>
<p style="padding-left:30px;"><strong>Theorem (Calegari-Walker):</strong> A random group at density <img src="https://s0.wp.com/latex.php?latex=D%3C1%2F2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D&lt;1/2" title="D&lt;1/2" class="latex" /> contains many quasiconvex surface subgroups, with probability <img src="https://s0.wp.com/latex.php?latex=1-O%28e%5E%7B-n%5Ec%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="1-O(e^{-n^c})" title="1-O(e^{-n^c})" class="latex" />.</p>
<p>In particular, they contain surface subgroups with overwhelming probability. In fact, at the MSRI conference I gave a partial announcement of this theorem, saying only that we could prove the existence of surface subgroups at &#8220;some positive density&#8221;; I was worried about the fact that at density <img src="https://s0.wp.com/latex.php?latex=D%3E1%2F12&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D&gt;1/12" title="D&gt;1/12" class="latex" /> the group is no longer <img src="https://s0.wp.com/latex.php?latex=C%27%281%2F6%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C&#039;(1/6)" title="C&#039;(1/6)" class="latex" /> and therefore not a small cancellation group in the classical sense. However, it turns out that Yann Ollivier <a href="http://www.yann-ollivier.org/rech/publs/dehnrandom.pdf">developed</a> enough elements of a kind of small cancellation theory for random groups at any <img src="https://s0.wp.com/latex.php?latex=D%3C1%2F2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D&lt;1/2" title="D&lt;1/2" class="latex" /> that the argument can be pushed all the way.</p>
<p>The proof contains some technical details, but I believe that some of the main ideas of the proof can be given in a blog post. But before I do so, I think it is worth discussing (very) briefly why one might be interested in finding surface subgroups.</p>
<p>For certain classes of hyperbolic groups &#8212; for example, fundamental groups of hyperbolic 3-manifolds &#8212; finding a surface subgroup was always known to be an important question to give insight into the virtual Haken conjecture. In fact, the Kahn-Markovic construction of such subgroups turned out to be one of the key steps in the eventual proof of that conjecture by Agol. But even beyond 3-manifolds per se, surface subgroups play an important role. At the MSRI conference Vlad Markovic talked about an <a href="http://arxiv.org/abs/1205.5747">approach</a> he has to Cannon&#8217;s Conjecture &#8212; which says if <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> is a hyperbolic group whose boundary is homeomorphic to a 2-sphere, then <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> is virtually isomorphic to a (hyperbolic) 3-manifold group &#8212; and his approach depends on being able to find &#8220;enough&#8221; (quasiconvex) surface subgroups of <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" />. I asked Gromov (by email) what had motivated him to pose this question; I don&#8217;t think he would mind if I shared his reply, which was:</p>
<p style="padding-left:30px;">I do not remember exactly my motivations and heuristic evidence in favor of the existence of &#8220;many surface groups in many hyperbolic groups&#8221; except for connectedness arguments at the boundaries, but I had  (and am having) a feeling that these are essential structural components of hyperbolic groups.</p>
<p>My own view, and my main interest in this question, is stimulated by a belief that surface groups (not necessarily closed, and possibly with boundary) can act as a sort of &#8220;bridge&#8221; between hyperbolic geometry and symplectic geometry (through their connection to causal structures, quasimorphisms, stable commutator length, etc). Surface groups are the &#8220;simplest&#8221; kind of hyperbolic groups after free groups, and surfaces themselves are the &#8220;simplest&#8221; class of symplectic manifold; any route between the two kinds of geometry must surely say a lot about surfaces. In this vein, I should remark that in the world of 3-manifold topology (where these issues are infinitely better understood), surfaces again play the premier role in both worlds: minimal/pleated/shrinkwrapped surfaces in the hyperbolic world, norm minimizing/pseudoholomorphic/convex in the contact/symplectic world. It is worth remarking that for the longest time <em>embedded</em> surfaces played a preeminent role in both theories, but that recent breakthroughs (on the hyperbolic side) have depended on developing a deep understanding of <em>immersed</em> surfaces. I wonder whether there is an important role for immersed surfaces on the symplectic side (in <img src="https://s0.wp.com/latex.php?latex=3%5Cpm+1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="3&#92;pm 1" title="3&#92;pm 1" class="latex" />-manifold topology)? Maybe a reader who is an expert on Heegaard Floer homology can offer an opinion.</p>
<p>OK, let&#8217;s move on to the proof of the Random Group Surface Subgroup Theorem. The first step of the proof builds on a construction in our paper <a href="http://arxiv.org/abs/1212.2618">Surface subgroups from Linear Programming</a>, where we show that a sufficiently random homologically trivial collection of cyclic words in a free groups can be taken to bound a certain kind of combinatorial object called a <em>Folded Fatgraph</em> (this result also underpins the main theorem in my recent related paper <a href="http://arxiv.org/abs/1303.2700">Random graphs of free groups contain surface subgroups</a>, joint with Henry Wilton). A fatgraph is just an ordinary graph together with a choice of cyclic ordering on the edges incident to each vertex. Such a graph can be canonically fattened to a compact surface (with boundary) in which it lies as a spine. Stallings famously observed that an immersion (i.e. a locally injective simplicial map) between graphs is injective on fundamental groups; such a map of graphs is said to be<em> folded</em>. Thus a folded fatgraph gives an injective surface (with boundary!) subgroup of a free group with prescribed boundary.</p>
<p>The first step in our paper is to make this result more quantitative. A trivalent fatgraph with reduced boundary words is necessarily folded. Our first main result is the following</p>
<p style="padding-left:30px;"> <strong>Thin Fatgraph Theorem:</strong> If <img src="https://s0.wp.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;Gamma" title="&#92;Gamma" class="latex" /> is a sufficiently random homologically trivial collection of cyclically reduced words in a free group <img src="https://s0.wp.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="F" title="F" class="latex" />, then for any <img src="https://s0.wp.com/latex.php?latex=L&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="L" title="L" class="latex" /> there is some <img src="https://s0.wp.com/latex.php?latex=N&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="N" title="N" class="latex" /> depending only on <img src="https://s0.wp.com/latex.php?latex=L&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="L" title="L" class="latex" /> so that <img src="https://s0.wp.com/latex.php?latex=N&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="N" title="N" class="latex" /> copies of <img src="https://s0.wp.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;Gamma" title="&#92;Gamma" class="latex" /> bounds a trivalent fatgraph in which every edge has length at least <img src="https://s0.wp.com/latex.php?latex=L&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="L" title="L" class="latex" />.</p>
<p>These fatgraphs have very long edges and are trivalent; hence are &#8220;thin&#8221;. Let me not say anything about the proof except that the first part of it closely models the proof of Thm 8.9 from our SSLP paper linked above, but the last step (which was done by computer in the SSLP paper) depends on an elementary but complicated combinatorial argument (which takes up almost half the paper!). (It is worth remarking that this last combinatorial step has something morally in common with the Kahn-Markovic proof of the <a href="http://arxiv.org/abs/1101.1330">Ehrenpreis conjecture</a> via the theory of &#8220;good pants homology&#8221;, in that we want to cancel some collection of &#8220;superfluous&#8221; short loops which can be thought of as random excitations on the surface of a (Dirac) sea of perfectly equidistributed loops. I should also remark that some version of this theory &#8212; &#8220;pants homology&#8221; if you will &#8212; was earlier developed by me in my paper <a href="http://arxiv.org/abs/0807.0395">Faces of the scl norm ball</a>, in which I showed that every homologically trivial immersed collection of geodesics on a hyperbolic surface virtually cobounds an immersed subsurface with a sufficiently large multiple of the boundary.)</p>
<p>By the way, it is natural to wonder just how &#8220;random&#8221; the collection <img src="https://s0.wp.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;Gamma" title="&#92;Gamma" class="latex" /> needs to be for the conclusion of the theorem to hold (technically, we work with a deterministic property called &#8220;pseudorandomness&#8221; which is a kind of controlled equidistribution at certain scales). One can ask how long a random cyclically reduced (homologically trivial) word needs to be before it bounds a trivalent fatgraph (with, for the sake of concreteness, no constraint on the length of edges). This is a question that can be addressed experimentally by computer. The results are very interesting. For rank 3, we looked at between 100000 and 400000 such words of each even length from 10 to 120. The proportion of such words that bound trivalent fatgraphs is plotted below:</p>
<p style="text-align:center;"><a href="https://lamington.files.wordpress.com/2013/04/trivalent_graph.jpg"><img data-attachment-id="1989" data-permalink="https://lamington.wordpress.com/2013/04/03/random-groups-contain-surface-subgroups/trivalent_graph/" data-orig-file="https://lamington.files.wordpress.com/2013/04/trivalent_graph.jpg" data-orig-size="709,446" data-comments-opened="1" data-image-meta="{&quot;aperture&quot;:&quot;0&quot;,&quot;credit&quot;:&quot;&quot;,&quot;camera&quot;:&quot;&quot;,&quot;caption&quot;:&quot;&quot;,&quot;created_timestamp&quot;:&quot;0&quot;,&quot;copyright&quot;:&quot;&quot;,&quot;focal_length&quot;:&quot;0&quot;,&quot;iso&quot;:&quot;0&quot;,&quot;shutter_speed&quot;:&quot;0&quot;,&quot;title&quot;:&quot;&quot;}" data-image-title="trivalent_graph" data-image-description="" data-medium-file="https://lamington.files.wordpress.com/2013/04/trivalent_graph.jpg?w=300" data-large-file="https://lamington.files.wordpress.com/2013/04/trivalent_graph.jpg?w=709" class="alignnone size-large wp-image-1989" alt="trivalent_graph" src="https://lamington.files.wordpress.com/2013/04/trivalent_graph.jpg?w=1024&#038;h=644" srcset="https://lamington.files.wordpress.com/2013/04/trivalent_graph.jpg 709w, https://lamington.files.wordpress.com/2013/04/trivalent_graph.jpg?w=150&amp;h=94 150w, https://lamington.files.wordpress.com/2013/04/trivalent_graph.jpg?w=300&amp;h=189 300w" sizes="(max-width: 709px) 100vw, 709px"   /></a></p>
<p style="text-align:left;">The first time we did this experiment, we only looked at words up to length 50 or so; needless to say, this gives a somewhat misleading idea of the asymptotic picture!</p>
<p>How can one use thin fatgraphs to build surface subgroups? Before tackling a random group, let&#8217;s consider a one-relator group with a single (long, random) relator <img src="https://s0.wp.com/latex.php?latex=r&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r" title="r" class="latex" />. We can imagine building a (polygonal) surface <img src="https://s0.wp.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S" title="S" class="latex" /> out of disks, each of which has either <img src="https://s0.wp.com/latex.php?latex=r&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r" title="r" class="latex" /> or <img src="https://s0.wp.com/latex.php?latex=r%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r^{-1}" title="r^{-1}" class="latex" /> on its boundary, where the disks are glued to each other along mutually inverse subwords of the boundary words. Since a random word will probably not be homologically trivial, we build a surface out of <img src="https://s0.wp.com/latex.php?latex=N&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="N" title="N" class="latex" /> disks labeled <img src="https://s0.wp.com/latex.php?latex=r&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r" title="r" class="latex" /> and <img src="https://s0.wp.com/latex.php?latex=N&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="N" title="N" class="latex" /> disks labeled <img src="https://s0.wp.com/latex.php?latex=r%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r^{-1}" title="r^{-1}" class="latex" />, where <img src="https://s0.wp.com/latex.php?latex=N&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="N" title="N" class="latex" /> is as in the Thin Fatgraph Theorem. The 1-skeleton <img src="https://s0.wp.com/latex.php?latex=Y&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="Y" title="Y" class="latex" /> of <img src="https://s0.wp.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S" title="S" class="latex" /> is a graph, and the way in which it sits in <img src="https://s0.wp.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S" title="S" class="latex" /> gives it a fatgraph structure.</p>
<p>The first thing one might think therefore is that one should just apply the Thin Fatgraph Theorem to build a fatgraph bounding <img src="https://s0.wp.com/latex.php?latex=Nr+%2B+Nr%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="Nr + Nr^{-1}" title="Nr + Nr^{-1}" class="latex" />. One can do this, but why should one expect the resulting surface to be injective? In order for the surface <img src="https://s0.wp.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S" title="S" class="latex" /> to fail to be injective there must be some essential loop <img src="https://s0.wp.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;gamma" title="&#92;gamma" class="latex" /> in the 1-skeleton <img src="https://s0.wp.com/latex.php?latex=Y&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="Y" title="Y" class="latex" /> which bounds a van Kampen disk <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BD%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{D}" title="&#92;mathcal{D}" class="latex" /> in the group. Without loss of generality, we can assume that this disk has a minimal number of faces; note that each face has either <img src="https://s0.wp.com/latex.php?latex=r&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r" title="r" class="latex" /> or <img src="https://s0.wp.com/latex.php?latex=r%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r^{-1}" title="r^{-1}" class="latex" /> on its boundary. A (random) 1-relator group is hyperbolic; in fact, it is <img src="https://s0.wp.com/latex.php?latex=C%27%28%5Clambda%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C&#039;(&#92;lambda)" title="C&#039;(&#92;lambda)" class="latex" /> for any <img src="https://s0.wp.com/latex.php?latex=%5Clambda&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;lambda" title="&#92;lambda" class="latex" /> with overwhelming probability, when the length <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" /> of the relator gets long. So in such a van Kampen diagram there must be very long subwords (of length <img src="https://s0.wp.com/latex.php?latex=O%28n%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="O(n)" title="O(n)" class="latex" />) in <img src="https://s0.wp.com/latex.php?latex=r&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r" title="r" class="latex" /> or <img src="https://s0.wp.com/latex.php?latex=r%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r^{-1}" title="r^{-1}" class="latex" /> which are subwords of <img src="https://s0.wp.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;gamma" title="&#92;gamma" class="latex" />. Of course, <img src="https://s0.wp.com/latex.php?latex=Y&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="Y" title="Y" class="latex" /> does contain long subwords of <img src="https://s0.wp.com/latex.php?latex=r&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r" title="r" class="latex" /> and <img src="https://s0.wp.com/latex.php?latex=r%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r^{-1}" title="r^{-1}" class="latex" />; the boundary of the fattening of <img src="https://s0.wp.com/latex.php?latex=Y&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="Y" title="Y" class="latex" /> consists entirely of such words! But in a minimal van Kampen diagram such &#8220;boundary&#8221; subwords must not occur, and the question is whether <img src="https://s0.wp.com/latex.php?latex=Y&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="Y" title="Y" class="latex" /> contains long subwords in common with <img src="https://s0.wp.com/latex.php?latex=r&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r" title="r" class="latex" /> or <img src="https://s0.wp.com/latex.php?latex=r%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r^{-1}" title="r^{-1}" class="latex" /> that are not boundary-parallel.</p>
<p>A counting estimate gives the following heuristic answer. By the defining property of a Thin Fatgraph, for any <img src="https://s0.wp.com/latex.php?latex=T&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="T" title="T" class="latex" /> there are <img src="https://s0.wp.com/latex.php?latex=O%282%5E%7BT%2FL%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="O(2^{T/L})" title="O(2^{T/L})" class="latex" /> paths in <img src="https://s0.wp.com/latex.php?latex=Y&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="Y" title="Y" class="latex" /> of length <img src="https://s0.wp.com/latex.php?latex=T&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="T" title="T" class="latex" /> starting at any point, and only <img src="https://s0.wp.com/latex.php?latex=%7CY%7C%3DO%28n%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="|Y|=O(n)" title="|Y|=O(n)" class="latex" /> starting points. On the other hand, there are <img src="https://s0.wp.com/latex.php?latex=%282k-1%29%5ET&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="(2k-1)^T" title="(2k-1)^T" class="latex" /> random reduced words of length <img src="https://s0.wp.com/latex.php?latex=T&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="T" title="T" class="latex" />, and the relator <img src="https://s0.wp.com/latex.php?latex=r&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r" title="r" class="latex" /> contains at most <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" /> of them. The difficulty in making this argument rigorous is that the fatgraph <img src="https://s0.wp.com/latex.php?latex=Y&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="Y" title="Y" class="latex" /> is not independent of <img src="https://s0.wp.com/latex.php?latex=r&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r" title="r" class="latex" />; in fact it is constructed &#8220;from&#8221; <img src="https://s0.wp.com/latex.php?latex=r&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r" title="r" class="latex" /> in a direct sense! So the trick is to break up <img src="https://s0.wp.com/latex.php?latex=r&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r" title="r" class="latex" /> into small subwords, and build thin fatgraphs bounding each subword, and then each small thin fatgraph will be independent of the other subwords.</p>
<p>Explicitly, we find what we call a <em>Bead Decomposition</em> of <img src="https://s0.wp.com/latex.php?latex=r&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r" title="r" class="latex" />; this is a decomposition of <img src="https://s0.wp.com/latex.php?latex=r&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r" title="r" class="latex" /> into subwords <img src="https://s0.wp.com/latex.php?latex=r_i%5E%5Cpm&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r_i^&#92;pm" title="r_i^&#92;pm" class="latex" /> of length <img src="https://s0.wp.com/latex.php?latex=O%28n%5E%7B1-%5Cdelta%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="O(n^{1-&#92;delta})" title="O(n^{1-&#92;delta})" class="latex" /> which start and end with mutually inverse subwords of length <img src="https://s0.wp.com/latex.php?latex=C%5Clog%28n%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C&#92;log(n)" title="C&#92;log(n)" class="latex" />. The inverse subwords at the start of each <img src="https://s0.wp.com/latex.php?latex=r_i%5E%5Cpm&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r_i^&#92;pm" title="r_i^&#92;pm" class="latex" /> are paired, to produce a collection of <em>beads</em> of size <img src="https://s0.wp.com/latex.php?latex=O%28n%5E%7B1-%5Cdelta%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="O(n^{1-&#92;delta})" title="O(n^{1-&#92;delta})" class="latex" />, separated by intervals of length <img src="https://s0.wp.com/latex.php?latex=C%5Clog%28n%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C&#92;log(n)" title="C&#92;log(n)" class="latex" /> called <em>necks</em>. Each bead on its own will probably be homologically essential, but we can perform a bead decomposition at &#8220;the same&#8221; locations in the word <img src="https://s0.wp.com/latex.php?latex=r%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r^{-1}" title="r^{-1}" class="latex" /> to get a collection of pairs of inverse beads <img src="https://s0.wp.com/latex.php?latex=B_i%2C+B_i%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B_i, B_i^{-1}" title="B_i, B_i^{-1}" class="latex" /> of length <img src="https://s0.wp.com/latex.php?latex=O%28n%5E%7B1-%5Cdelta%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="O(n^{1-&#92;delta})" title="O(n^{1-&#92;delta})" class="latex" />. Taking <img src="https://s0.wp.com/latex.php?latex=N&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="N" title="N" class="latex" /> copies of each pair of beads, we can build a thin fatgraph that bounds it, and then these thin fatgraphs are joined one to the next along necks. By construction, the subwords contained in the spine of the fatgraph bounding a bead <img src="https://s0.wp.com/latex.php?latex=B_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B_i" title="B_i" class="latex" /> are independent of the subwords in <img src="https://s0.wp.com/latex.php?latex=B_j&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B_j" title="B_j" class="latex" /> for <img src="https://s0.wp.com/latex.php?latex=i+%5Cne+j&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="i &#92;ne j" title="i &#92;ne j" class="latex" />, so with overwhelming probability, they have no long subwords in common. The necks are sufficiently long that whenever a subword passes over a neck, another copy of that subword cannot appear within distance <img src="https://s0.wp.com/latex.php?latex=n%5E%7B%5Cepsilon%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n^{&#92;epsilon}" title="n^{&#92;epsilon}" class="latex" /> for some <img src="https://s0.wp.com/latex.php?latex=0+%3C%5Cepsilon+%3C+%5Cdelta&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="0 &lt;&#92;epsilon &lt; &#92;delta" title="0 &lt;&#92;epsilon &lt; &#92;delta" class="latex" /> (with high probability). But the existence of a van Kampen diagram would give rise to a long string of such coincidences, and therefore we deduce that no van Kampen diagram exists, and the surface is injective.</p>
<p>We now throw in an additional <img src="https://s0.wp.com/latex.php?latex=%282k-1%29%5E%7BnD%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="(2k-1)^{nD}" title="(2k-1)^{nD}" class="latex" /> random relators of length <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" /> independently, and with the uniform measure. Now the naive counting argument above is rigorous, and each additional relator <img src="https://s0.wp.com/latex.php?latex=r%27&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r&#039;" title="r&#039;" class="latex" /> is unlikely to have a long segment in common with a subpath in the spine <img src="https://s0.wp.com/latex.php?latex=Y&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="Y" title="Y" class="latex" />. In fact, what can be shown is that for each <img src="https://s0.wp.com/latex.php?latex=E%3CD&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="E&lt;D" title="E&lt;D" class="latex" /> there are of order <img src="https://s0.wp.com/latex.php?latex=%282k-1%29%5E%7Bn%28D-E%29%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="(2k-1)^{n(D-E)}" title="(2k-1)^{n(D-E)}" class="latex" /> relators that have <img src="https://s0.wp.com/latex.php?latex=En&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="En" title="En" class="latex" /> of their boundary in common with a subpath of <img src="https://s0.wp.com/latex.php?latex=Y&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="Y" title="Y" class="latex" /> (this common part does not need to be consecutive, but we do need to bound the number of connected components by some constant independent of <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" />; this is where Ollivier&#8217;s small cancellation work comes in to bootstrap such &#8220;local&#8221; small cancellation estimates to &#8220;global&#8221; ones). From this argument, and some elementary reasoning with van Kampen diagrams, the result follows.</p>
<p>One subtlety is that it is necessary to control the size of the van Kampen diagrams we consider independently of <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" />. A path in a hyperbolic group which is not quasigeodesic can be shortened on a segment of size <img src="https://s0.wp.com/latex.php?latex=8%5Cdelta&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="8&#92;delta" title="8&#92;delta" class="latex" />, where <img src="https://s0.wp.com/latex.php?latex=%5Cdelta&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;delta" title="&#92;delta" class="latex" /> is the constant of hyperbolicity. Ollivier shows that <img src="https://s0.wp.com/latex.php?latex=%5Cdelta&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;delta" title="&#92;delta" class="latex" /> is <em>linear</em> in <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" />, for fixed <img src="https://s0.wp.com/latex.php?latex=D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D" title="D" class="latex" />, and therefore we can obtain estimates on the probability that <img src="https://s0.wp.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S" title="S" class="latex" /> fails to be injective by considering van Kampen diagrams containing a <em>bounded</em> number of disks.</p>
]]></html><thumbnail_url><![CDATA[https://lamington.files.wordpress.com/2013/04/trivalent_graph.jpg?w=490&fit=440%2C330]]></thumbnail_url><thumbnail_width><![CDATA[440]]></thumbnail_width><thumbnail_height><![CDATA[277]]></thumbnail_height></oembed>