<?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[Groups with free subgroups (part&nbsp;2)]]></title><type><![CDATA[link]]></type><html><![CDATA[<p>In a previous post, I discussed some methods for showing that a given group contains a (nonabelian) free subgroup. The methods were analytic and/or dynamical, and phrased in terms of the existence (or nonexistence) of certain functions on <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" /> or on spaces derived from <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" />, or in terms of actions 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" /> on certain spaces. Dually, one can try to find a free group in <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" /> by finding a homomorphism <img src="https://s0.wp.com/latex.php?latex=%5Crho%3A+F+%5Cto+G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho: F &#92;to G" title="&#92;rho: F &#92;to G" class="latex" /> and looking for circumstances under which <img src="https://s0.wp.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho" title="&#92;rho" class="latex" /> is injective.</p>
<p>For concreteness, let <img src="https://s0.wp.com/latex.php?latex=G+%3D+%5Cpi_1%28X%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G = &#92;pi_1(X)" title="G = &#92;pi_1(X)" class="latex" /> for some (given) space <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" />. If <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" /> is a free group, a representation <img src="https://s0.wp.com/latex.php?latex=%5Crho%3AF+%5Cto+G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho:F &#92;to G" title="&#92;rho:F &#92;to G" class="latex" /> up to conjugation determines a homotopy class of map <img src="https://s0.wp.com/latex.php?latex=f%3A+S+%5Cto+X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="f: S &#92;to X" title="f: S &#92;to X" class="latex" /> where <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 <img src="https://s0.wp.com/latex.php?latex=K%28F%2C1%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="K(F,1)" title="K(F,1)" class="latex" />. The most natural <img src="https://s0.wp.com/latex.php?latex=K%28F%2C1%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="K(F,1)" title="K(F,1)" class="latex" />&#8216;s to consider are <em>graphs</em> and <em>surfaces</em> (with boundary). It is generally not easy to tell whether a map of a graph or a surface to a topological space is <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1" title="&#92;pi_1" class="latex" />-injective at the topological level, but might be easier if one can use some geometry.</p>
<p><strong>Example</strong>: Let <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> be a complete Riemannian manifold with sectional curvature bounded above by some negative constant <img src="https://s0.wp.com/latex.php?latex=K+%3C+0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="K &lt; 0" title="K &lt; 0" class="latex" />. Convexity of the distance function in a negatively curved space means that given any map of a graph <img src="https://s0.wp.com/latex.php?latex=f%3A%5CGamma+%5Cto+X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="f:&#92;Gamma &#92;to X" title="f:&#92;Gamma &#92;to X" class="latex" /> one can flow <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" /> by the negative gradient of total length until it undergoes some topology change (e.g. some edge shrinks to zero length) or it (asymptotically) achieves a local minimum (the adjective &#8220;asymptotically&#8221; here just means that the flow takes infinite time to reach the minimum, because the size of the gradient is small when the map is almost minimum; there are no analytic difficulties to overcome when taking the limit). A typical topological change might be some loop shrinking to a point, thereby certifying that a free summand of <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1%28%5CGamma%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1(&#92;Gamma)" title="&#92;pi_1(&#92;Gamma)" class="latex" /> mapped trivially to <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" /> and should have been discarded. Technically, one probably wants to choose <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" /> to be a trivalent graph, and when some interior edge collapses (so that four points come together) to let the <img src="https://s0.wp.com/latex.php?latex=4&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="4" title="4" class="latex" />-valent vertex resolve itself into a pair of <img src="https://s0.wp.com/latex.php?latex=3&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="3" title="3" class="latex" />-valent vertices in whichever of the three combinatorial possibilities is locally most efficient. The limiting graph, if nonempty, will be trivalent, with geodesic edges, and vertices at which the three edges are all (tangentially) coplanar and meet at angles of <img src="https://s0.wp.com/latex.php?latex=2%5Cpi%2F3&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="2&#92;pi/3" title="2&#92;pi/3" class="latex" />. Such a graph can be certified as <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1" title="&#92;pi_1" class="latex" />-injective provided the edges are sufficiently long (depending on the curvature <img src="https://s0.wp.com/latex.php?latex=K&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="K" title="K" class="latex" />). After rescaling the metric on <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> so that the supremum of the curvatures is <img src="https://s0.wp.com/latex.php?latex=-1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="-1" title="-1" class="latex" />, a trivalent geodesic graph with angles <img src="https://s0.wp.com/latex.php?latex=2%5Cpi%2F3&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="2&#92;pi/3" title="2&#92;pi/3" class="latex" /> at the vertices and edges at least <img src="https://s0.wp.com/latex.php?latex=2%5Ctanh%5E%7B-1%7D%281%2F2%29+%3D+1.0986%5Ccdots&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="2&#92;tanh^{-1}(1/2) = 1.0986&#92;cdots" title="2&#92;tanh^{-1}(1/2) = 1.0986&#92;cdots" class="latex" /> is <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1" title="&#92;pi_1" class="latex" />-injective. To see this, lift to maps between universal covers, i.e. consider an equivariant map from a tree <img src="https://s0.wp.com/latex.php?latex=%5Cwidetilde%7B%5CGamma%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;widetilde{&#92;Gamma}" title="&#92;widetilde{&#92;Gamma}" class="latex" /> to <img src="https://s0.wp.com/latex.php?latex=%5Cwidetilde%7BX%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;widetilde{X}" title="&#92;widetilde{X}" class="latex" />. Let <img src="https://s0.wp.com/latex.php?latex=%5Cell&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;ell" title="&#92;ell" class="latex" /> be an embedded arc in <img src="https://s0.wp.com/latex.php?latex=%5Cwidetilde%7B%5CGamma%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;widetilde{&#92;Gamma}" title="&#92;widetilde{&#92;Gamma}" class="latex" />, and consider the image in <img src="https://s0.wp.com/latex.php?latex=%5Cwidetilde%7BX%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;widetilde{X}" title="&#92;widetilde{X}" class="latex" />. Using Toponogov&#8217;s theorem, one can compare with a piecewise isometric map from <img src="https://s0.wp.com/latex.php?latex=%5Cell&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;ell" title="&#92;ell" class="latex" /> to <img src="https://s0.wp.com/latex.php?latex=%5Cmathbb%7BH%7D%5En&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathbb{H}^n" title="&#92;mathbb{H}^n" class="latex" />. The worst case is when all the edges are contained in a single <img src="https://s0.wp.com/latex.php?latex=%5Cmathbb%7BH%7D%5E2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathbb{H}^2" title="&#92;mathbb{H}^2" class="latex" />, and all corners &#8220;bend&#8221; the same way. Providing the image does not bend as much as a horocircle, the endpoints of the image of <img src="https://s0.wp.com/latex.php?latex=%5Cell&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;ell" title="&#92;ell" class="latex" /> stay far away in <img src="https://s0.wp.com/latex.php?latex=%5Cmathbb%7BH%7D%5E2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathbb{H}^2" title="&#92;mathbb{H}^2" class="latex" />. An infinite sided convex polygon in <img src="https://s0.wp.com/latex.php?latex=%5Cmathbb%7BH%7D%5E2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathbb{H}^2" title="&#92;mathbb{H}^2" class="latex" /> with all edges of length <img src="https://s0.wp.com/latex.php?latex=2%5Ctanh%5E%7B-1%7D%281%2F2%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="2&#92;tanh^{-1}(1/2)" title="2&#92;tanh^{-1}(1/2)" class="latex" /> and all angles <img src="https://s0.wp.com/latex.php?latex=2%5Cpi%2F3&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="2&#92;pi/3" title="2&#92;pi/3" class="latex" /> osculates a horocycle, so we are done.</p>
<p><strong>Remark</strong>: The fundamental group of a negatively curved manifold is word-hyperbolic, and therefore contains many nonabelian free groups, which may be certified by pingpong applied to the action of the group on its Gromov boundary. The point of the previous example is therefore to certify that a certain subgroup is free in terms of local geometric data, rather than global dynamical data (so to speak). Incidentally, I would not swear to the correctness of the constants above.</p>
<p><strong>Example</strong>: A given free group is the fundamental group of a surface with boundary in many different ways (this difference is one of the reasons that a group like <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BOut%7D%28F_n%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Out}(F_n)" title="&#92;text{Out}(F_n)" class="latex" /> is so much more complicated than the mapping class group of a surface). Pick a realization <img src="https://s0.wp.com/latex.php?latex=F+%3D+%5Cpi_1%28S%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="F = &#92;pi_1(S)" title="F = &#92;pi_1(S)" class="latex" />. Then a homomorphism <img src="https://s0.wp.com/latex.php?latex=%5Crho%3AF+%5Cto+G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho:F &#92;to G" title="&#92;rho:F &#92;to G" class="latex" /> up to conjugacy determines a homotopy class of map from <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 <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> as above. If <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> is negatively curved as before, each boundary loop is homotopic to a unique geodesic, and we may try to find a &#8220;good&#8221; map <img src="https://s0.wp.com/latex.php?latex=f%3AS+%5Cto+X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="f:S &#92;to X" title="f:S &#92;to X" class="latex" /> with boundary on these geodesics. There are many possible classes of good maps to consider:</p>
<ol>
<li>Fix a conformal structure on <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" /> and pick a harmonic map in the homotopy class of <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" />. Such a map exists since the target is nonpositively curved, by the famous theorem of <a href="http://www.ams.org/mathscinet-getitem?mr=0164306">Eells-Sampson</a>. The image is real analytic if <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> is, and is at least as negatively curved as the target, and therefore there is an <em>a priori</em> upper bound on the intrinsic curvature of the image; if the supremum of the curvature on <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> is normalized to be <img src="https://s0.wp.com/latex.php?latex=-1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="-1" title="-1" class="latex" />, then the image surface is <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BCAT%7D%28-1%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{CAT}(-1)" title="&#92;text{CAT}(-1)" class="latex" />, which just means that pointwise it is at least as negatively curved as hyperbolic space. By Gauss-Bonnet, one obtains an <em>a priori</em> bound on the area of the image 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" /> in terms of the Euler characteristic (which just depends on the rank of <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" />). On the other hand, this map depends on a choice of marked conformal structure on <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" />, and the space of such structures is noncompact.</li>
<li>Vary over all conformal structures on <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" /> and choose a harmonic map of least energy (if one exists) or find a sequence of maps that undergo a &#8220;neck pinch&#8221; as a sequence of conformal structures on <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" /> degenerates. Such a neck pinch exhibits a <em>simple</em> curve 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" /> that is essential 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" /> but whose image is inessential in <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" />; such a curve can be compressed, and the topology 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" /> simplified. Since each compression increases <img src="https://s0.wp.com/latex.php?latex=%5Cchi&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;chi" title="&#92;chi" class="latex" />, after finitely many steps the process terminates, and one obtains the desired map. This is <a href="http://www.ams.org/mathscinet-getitem?mr=0541332">Schoen-Yau</a>&#8216;s method to construct a stable minimal surface representative 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" />. When the target is <img src="https://s0.wp.com/latex.php?latex=3&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="3" title="3" class="latex" />-dimensional, the surface may be assumed to be unbranched, by a trick due to Osserman. </li>
<li>Following <a href="http://www.msri.org/communications/books/gt3m">Thurston</a>, pick an ideal triangulation 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" /> (i.e. a geodesic lamination 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" /> whose complementary regions are all ideal triangles); since <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" /> has boundary, we may choose such a lamination by first picking a triangulation (in the ordinary sense) with all vertices on <img src="https://s0.wp.com/latex.php?latex=%5Cpartial+S&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;partial S" title="&#92;partial S" class="latex" /> and then &#8220;spinning&#8221; the vertices to infinity. Unless <img src="https://s0.wp.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho" title="&#92;rho" class="latex" /> factors through a cyclic group, there is some choice of lamination so that the image of <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" /> can be straightened along the lamination, and then the image spanned with <img src="https://s0.wp.com/latex.php?latex=CAT%28-1%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="CAT(-1)" title="CAT(-1)" class="latex" /> ideal triangles to produce a <em>pleated surface</em> in <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> representing <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" /> (note: if <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> has constant negative curvature, these ideal triangles can be taken to be totally geodesic). The space of pleated surfaces in fixed (closed) <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> of given genus is compact, so this is a reasonable class of maps to work with.</li>
<li>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 merely a hyperbolic group, one can still construct pleated surfaces, not quite in <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" />, but equivariantly in <a href="http://arxiv.org/abs/math/0503274">Mineyev&#8217;s flow space</a> associated to <img src="https://s0.wp.com/latex.php?latex=%5Cwidetilde%7BX%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;widetilde{X}" title="&#92;widetilde{X}" class="latex" />. Here we are not really thinking of the triangles themselves, but the geodesic laminations they bound (which carry the same information). </li>
<li>If <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> is complete and <img src="https://s0.wp.com/latex.php?latex=3&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="3" title="3" class="latex" />-dimensional but noncompact, the space of pleated surfaces of given genus is generally not compact, and it is not always easy to find a pleated surface where you want it. This can sometimes be remedied by <em><a href="http://arxiv.org/abs/math/0407161">shrinkwrapping</a></em>; one looks for a minimal/pleated/harmonic surface subject to the constraint that it cannot pass through some prescribed set of geodesics in <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> (which act as &#8220;barriers&#8221; or &#8220;obstacles&#8221;, and force the resulting surface to end up roughly where one wants it to).</li>
</ol>
<p>Anyway, one way or another, one can usually find a map of a surface, or a space of maps of surfaces, representing a given homomorphism, with some kind of <em>a priori</em> control of the geometry. Usually, this control is <em>not</em> enough to certify that a given map is <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1" title="&#92;pi_1" class="latex" />-injective, but sometimes it might be. For instance, a totally geodesic (immersed) surface in a complete manifold of constant negative curvature is always <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1" title="&#92;pi_1" class="latex" />-injective, and any surface whose extrinsic curvature is small enough will also be <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1" title="&#92;pi_1" class="latex" />-injective.</p>
<p>Geometric methods to certify injectivity of free or surface groups are very useful and flexible, as far as they go. Unfortunately, I know of very few <em>topological</em> methods to certify injectivity. By far the most important exception is the following:</p>
<p><strong>Example</strong>: In <img src="https://s0.wp.com/latex.php?latex=3&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="3" title="3" class="latex" />-dimensions, one should look for <em>properly embedded</em> surfaces. If <img src="https://s0.wp.com/latex.php?latex=M&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="M" title="M" class="latex" /> is a <img src="https://s0.wp.com/latex.php?latex=3&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="3" title="3" class="latex" />-manifold (possibly with boundary), and <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 two-sided properly embedded surface, the famous <em>Dehn&#8217;s Lemma </em>(proved by <a href="http://www.ams.org/mathscinet-getitem?mr=0090053">Papakyriakopoulos</a>) implies that either <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 <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1" title="&#92;pi_1" class="latex" />-injective, or there is an <em>embedded</em> essential loop 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" /> that bounds an embedded disk in <img src="https://s0.wp.com/latex.php?latex=M&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="M" title="M" class="latex" /> on one side 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" />. Such a loop may be compressed (i.e. <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" /> may be cut open along the loop, and two copies of the compressing disk sewn in) preserving the property of embeddedness, but increasing <img src="https://s0.wp.com/latex.php?latex=%5Cchi&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;chi" title="&#92;chi" class="latex" />. After finitely many steps, either <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" /> compresses away entirely, or one obtains a <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1" title="&#92;pi_1" class="latex" />-injective surface. One way to ensure 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" /> does not compress away entirely is to start with a surface that is essential in (relative) homology; another way is to look for a surface dual to an action (of <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1%28M%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1(M)" title="&#92;pi_1(M)" class="latex" />) on a tree. In the latter case, one can often construct quite different free subgroups in <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1%28M%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1(M)" title="&#92;pi_1(M)" class="latex" /> by pingpong on the ends of the tree. Note by the way that this method produces <em>closed</em> surface subgroups as well as free subgroups. Note too that two-sidedness is essential to apply Dehn&#8217;s Lemma.</p>
<p><strong>Remark</strong>: Modern <img src="https://s0.wp.com/latex.php?latex=3&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="3" title="3" class="latex" />-manifold topologists are sometimes unreasonably indifferent to the power of Dehn&#8217;s Lemma (probably because this tool has been incorporated so fully into their subconscious?); it is worth reading Ralph Fox&#8217;s review of Papakyriakopoulos&#8217;s paper (linked above). Of this paper, he writes:</p>
<blockquote><p>. . . it has already led to renewed attack on the problem of classifying the 3-dimensional manifolds; significant results have been and are being obtained. A complete solution has suddenly become a definite possibility. </p></blockquote>
<p>Remember this was written more than 50 years ago &#8212; before the geometrization conjecture, before the JSJ decomposition, before the Scott core theorem, before Haken manifolds. The only reasonable reaction to this is: !!!</p>
<p><strong>Example</strong>: The construction of injective surfaces by Dehn&#8217;s Lemma may be abstracted in the following way. Given a target space <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" />, and a class of maps <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" /> of surfaces into <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> (in some category; e.g. homotopy classes of maps, pleated surfaces, <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BCAT%7D%28-1%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{CAT}(-1)" title="&#92;text{CAT}(-1)" class="latex" /> surfaces, etc.) suppose one can find a complexity <img src="https://s0.wp.com/latex.php?latex=c%3A%5Cmathcal%7BF%7D+%5Cto+%5Cmathcal%7BO%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="c:&#92;mathcal{F} &#92;to &#92;mathcal{O}" title="c:&#92;mathcal{F} &#92;to &#92;mathcal{O}" class="latex" /> with values in some ordered set, such that if <img src="https://s0.wp.com/latex.php?latex=f+%5Cin+%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="f &#92;in &#92;mathcal{F}" title="f &#92;in &#92;mathcal{F}" class="latex" /> is not injective, one can find <img src="https://s0.wp.com/latex.php?latex=f%27+%5Cin+%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="f&#039; &#92;in &#92;mathcal{F}" title="f&#039; &#92;in &#92;mathcal{F}" class="latex" /> of smaller complexity. Then if <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BO%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{O}" title="&#92;mathcal{O}" class="latex" /> is well-ordered, an injective surface may be found. If <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BO%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{O}" title="&#92;mathcal{O}" class="latex" /> is not well-ordered, one may ask at least that <img src="https://s0.wp.com/latex.php?latex=c&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="c" title="c" class="latex" /> is upper semi-continuous on <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" />, and hope to extend it upper semi-continuously to some suitable compactification of <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" />. Even if <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BO%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{O}" title="&#92;mathcal{O}" class="latex" /> is not well-ordered, one can at least <em>certify</em> that a map is injective, by showing that it minimizes <img src="https://s0.wp.com/latex.php?latex=c&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="c" title="c" class="latex" />. Here are some potential examples (none of them entirely satisfactory).</p>
<ol>
<li>Given a (homologically trivial) homotopy class of 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 <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" />, one can look at all maps of orientable surfaces <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 <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> with boundary factoring through <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" />. For such a surface, let <img src="https://s0.wp.com/latex.php?latex=n%28S%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n(S)" title="n(S)" class="latex" /> denote the degree with which the (possibly multiple) boundary (components) 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" /> wrap homologically around <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" />, and let <img src="https://s0.wp.com/latex.php?latex=-%5Cchi%5E-%28S%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="-&#92;chi^-(S)" title="-&#92;chi^-(S)" class="latex" /> denote the sum of Euler characteristics of non-disk and non-sphere components 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" />. For each 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" />, one considers the quantity <img src="https://s0.wp.com/latex.php?latex=-%5Cchi%5E-%28S%29%2F2n%28S%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="-&#92;chi^-(S)/2n(S)" title="-&#92;chi^-(S)/2n(S)" class="latex" /> (the factor of <img src="https://s0.wp.com/latex.php?latex=2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="2" title="2" class="latex" /> can be ignored if desired). The important feature of this quantity is that it does not change if <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 replaced by a finite cover. If <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1%28S%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1(S)" title="&#92;pi_1(S)" class="latex" /> is not injective, let <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" /> be an essential loop on <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" /> whose image in <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> is inessential. Peter Scott <a href="http://www.ams.org/mathscinet-getitem?mr=0494062">showed</a> that any essential loop on a surface lifts to an embedded loop in some finite cover. Hence, after passing to such a cover, <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" /> may be compressed, and the resulting surface <img src="https://s0.wp.com/latex.php?latex=S%27&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S&#039;" title="S&#039;" class="latex" /> satisfies <img src="https://s0.wp.com/latex.php?latex=-%5Cchi%5E-%28S%27%29%2F2n%28S%27%29+%3C+-%5Cchi%5E-%28S%29%2F2n%28S%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="-&#92;chi^-(S&#039;)/2n(S&#039;) &lt; -&#92;chi^-(S)/2n(S)" title="-&#92;chi^-(S&#039;)/2n(S&#039;) &lt; -&#92;chi^-(S)/2n(S)" class="latex" />. In other words, a global minimizer of this quantity is injective. Such a surface is called extremal. The problem is that extremal surfaces do not always exist; but this construction motivates one to look for them. </li>
<li>Given a <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BCAT%7D%28-1%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{CAT}(-1)" title="&#92;text{CAT}(-1)" class="latex" /> 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" /> with geodesic boundary in <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" />, one can retract <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 a geodesic spine, and encode the surface by the resulting fatgraph, with edges labelled by homotopy classes in <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" />. Since Euler characteristic is local, one does not really care precisely how the pieces of the fatgraph are assembled, but only how many pieces of what kinds are needed for a given boundary. So if only finitely many such pieces appear in some infinite family of surfaces, one can in fact construct an extremal surface as above, which is necessarily injective (more technically, one reduces the computation of Euler characteristic to a linear programming problem, finds a rational extremal solution (which corresponds to a weighted sum of pieces of fatgraph), and glues together the pieces to construct the extremal surface; one situation in which this scheme can be made to work is explained in this <a href="http://arxiv.org/abs/0802.1352">paper</a> of mine). Edges can be subdivided into a finite number of possibilities, so one just needs to ensure finiteness of the number of vertex types. One condition that ensures finiteness of vertex types is the existence of a uniform constant <img src="https://s0.wp.com/latex.php?latex=C%3E0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C&gt;0" title="C&gt;0" class="latex" /> so that for each 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" /> in the given family, and for each point <img src="https://s0.wp.com/latex.php?latex=p+%5Cin+S&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p &#92;in S" title="p &#92;in S" class="latex" />, there is an estimate <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7Bdist%7D%28p%2C%5Cpartial+S%29+%5Cle+C&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{dist}(p,&#92;partial S) &#92;le C" title="&#92;text{dist}(p,&#92;partial S) &#92;le C" class="latex" />. If this condition is violated, one finds pairs <img src="https://s0.wp.com/latex.php?latex=p_i%2CS_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p_i,S_i" title="p_i,S_i" class="latex" /> which converge in the geometric topology to a point in a <em>complete</em> (i.e. without boundary, but probably noncompact) surface.</li>
<li>Given <img src="https://s0.wp.com/latex.php?latex=S+%5Cto+X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S &#92;to X" title="S &#92;to X" class="latex" />, either compress an embedded essential loop, or realize <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" /> by a least area surface. If <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 not injective, pass to a cover, compress a loop, and realize the result by a least area surface. Repeat this process. One obtains in this way a sequence of least area surfaces in <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> (typically of bigger and bigger genus) and there is no reason to expect the process to terminate. If <img src="https://s0.wp.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X" title="X" class="latex" /> is a <img src="https://s0.wp.com/latex.php?latex=3&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="3" title="3" class="latex" />-manifold, the curvature of a least area surface admits two-sided curvature bounds away from the boundary, by a theorem of <a href="http://www.ams.org/mathscinet-getitem?mr=0795231">Schoen</a> (near the boundary, the negative curvature might blow up, but only in controlled ways &#8212; e.g. after rescaling about a sequence of points with the most negative curvature, one may obtain in the limit a helicoid). Away from the boundary, the family of surfaces one obtains vary precompactly in the <img src="https://s0.wp.com/latex.php?latex=C%5E%5Cinfty&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C^&#92;infty" title="C^&#92;infty" class="latex" /> topology, and one may obtain a complete locally least area lamination <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" /> in the limit. If <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1%28%5CLambda%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1(&#92;Lambda)" title="&#92;pi_1(&#92;Lambda)" class="latex" /> is not injective, one can continue to pass to covers (applying a version of Scott&#8217;s theorem for infinite surfaces) and compress, and by transfinite induction, eventually arrive at a locally least area lamination with injective <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1" title="&#92;pi_1" class="latex" />. Of course, such a limit might well be a lamination by planes. However, the lamination one obtains is not completely arbitrary: since it is a limit of limits of . . . compact surfaces, one can choose a limit that admits a nontrivial invariant transverse measure (one must be careful here, since the lamination will typically have boundary). Or, as in bullet 2. above, one may insist that this limit lamination is complete (i.e. without boundary). </li>
</ol>
<p>It is more tricky to find a limit lamination as in 3. without boundary and admitting an invariant transverse measure; in any case, this motivates the following:  </p>
<p><strong>Question</strong>: Is there a closed hyperbolic <img src="https://s0.wp.com/latex.php?latex=3&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="3" title="3" class="latex" />-manifold <img src="https://s0.wp.com/latex.php?latex=M&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="M" title="M" class="latex" /> which admits a locally least area transversely measured complete immersed lamination <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" />, all of whose leaves are disks? (note that the answer is negative if one asks for the lamination to be <em>embedded </em>(there are several easy proofs of this fact)).</p>
<p>Secretly, the function that assigns <img src="https://s0.wp.com/latex.php?latex=%5Cinf_S+-%5Cchi%5E-%28S%29%2F2n%28S%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;inf_S -&#92;chi^-(S)/2n(S)" title="&#92;inf_S -&#92;chi^-(S)/2n(S)" class="latex" /> to a homologically trivial 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" /> is the <em>stable commutator length</em> of the conjugacy class in <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1%28X%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1(X)" title="&#92;pi_1(X)" class="latex" /> represented by <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" />. Extremal surfaces can sometimes be certified by constructing certain functions on <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1%28X%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1(X)" title="&#92;pi_1(X)" class="latex" /> called <em>homogeneous quasimorphisms</em>, but a discussion of such functions will have to wait for another post.</p>
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