<?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[Orderability, and groups of homeomorphisms of the&nbsp;disk]]></title><type><![CDATA[link]]></type><html><![CDATA[<p>I have struggled for a long time (and I continue to struggle) with the following question:</p>
<p><strong>Question: </strong>Is the group of self-homeomorphisms of the unit disk (in the plane) that fix the boundary pointwise a left-orderable group?</p>
<p>Recall that a group <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 left-orderable if there is a total order <img src="https://s0.wp.com/latex.php?latex=%3C&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&lt;" title="&lt;" class="latex" /> on the elements satisfying <img src="https://s0.wp.com/latex.php?latex=g%3Ch&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="g&lt;h" title="g&lt;h" class="latex" /> if and only if <img src="https://s0.wp.com/latex.php?latex=fg+%3C+fh&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="fg &lt; fh" title="fg &lt; fh" class="latex" /> for all <img src="https://s0.wp.com/latex.php?latex=f%2Cg%2Ch+%5Cin+G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="f,g,h &#92;in G" title="f,g,h &#92;in G" class="latex" />. For a countable group, the property of being left orderable is equivalent to the property that the group admits a faithful action on the interval by orientation-preserving homeomorphisms; however, this equivalence is not &#8220;natural&#8221; in the sense that there is no natural way to extract an ordering from an action, or vice-versa. This formulation of the question suggests that one is trying to embed the group of homeomorphisms of the disk into the group of homeomorphisms of the interval, an unlikely proposition, made even more unlikely by the following famous theorem of <a href="http://www.ams.org/mathscinet-getitem?mr=0693972">Filipkiewicz</a>:</p>
<p><strong>Theorem:</strong> (Filipkiewicz) Let <img src="https://s0.wp.com/latex.php?latex=M_1%2CM_2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="M_1,M_2" title="M_1,M_2" class="latex" /> be two compact manifolds, and <img src="https://s0.wp.com/latex.php?latex=r_1%2Cr_2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r_1,r_2" title="r_1,r_2" class="latex" /> two non-negative integers or infinity. Suppose the connected components of the identity of <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BDiff%7D%5E%7Br_1%7D%28M_1%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Diff}^{r_1}(M_1)" title="&#92;text{Diff}^{r_1}(M_1)" class="latex" /> and <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BDiff%7D%5E%7Br_2%7D%28M_2%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Diff}^{r_2}(M_2)" title="&#92;text{Diff}^{r_2}(M_2)" class="latex" /> are isomorphic as abstract groups. Then <img src="https://s0.wp.com/latex.php?latex=r_1%3Dr_2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="r_1=r_2" title="r_1=r_2" class="latex" /> and the isomorphism is induced by some diffeomorphism.</p>
<p>The hard(est?) part of the argument is to identify a subgroup stabilizing a point in purely algebraic terms. It is a fundamental and well-studied problem, in some ways a natural outgrowth of Klein&#8217;s Erlanger programme, to perceive the geometric structure on a space in terms of algebraic properties of its automorphism group. The <a href="http://www.ams.org/mathscinet-getitem?mr=1445290">book by Banyaga</a> is the best reference I know for this material, in the context of &#8220;flexible&#8221; geometric structures, with big transformation groups (it is furthermore the only math book I know with a pink cover).</p>
<p>Left orderability is inherited under extensions. I.e. if <img src="https://s0.wp.com/latex.php?latex=K+%5Cto+G+%5Cto+H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="K &#92;to G &#92;to H" title="K &#92;to G &#92;to H" class="latex" /> is a short exact sequence, and both <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" /> and <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> are left orderable, then so is <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" />. Furthermore, it is a simple but useful theorem of <a href="http://www.ams.org/mathscinet-getitem?mr=0310046">Burns and Hale</a> that a group <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 left orderable if and only if for every finitely generated subgroup <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> there is a left orderable group <img src="https://s0.wp.com/latex.php?latex=H%27&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H&#039;" title="H&#039;" class="latex" /> and a surjective homomorphism <img src="https://s0.wp.com/latex.php?latex=H+%5Cto+H%27&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H &#92;to H&#039;" title="H &#92;to H&#039;" class="latex" />. The necessity of this condition is obvious: a subgroup of a left orderable group is left orderable (by restricting the order), so one can take <img src="https://s0.wp.com/latex.php?latex=H%27&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H&#039;" title="H&#039;" class="latex" /> to be <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> and the surjection to be the identity. One can exploit this strategy to show that certain transformation groups are left orderable, as follows:</p>
<p><strong>Example:</strong> Suppose <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 group of homeomorphisms of some 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" />, with a nonempty fixed point set. If <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> is a finitely generated subgroup 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" />, then there is a point <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 the frontier of <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7Bfix%7D%28H%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{fix}(H)" title="&#92;text{fix}(H)" class="latex" /> so that <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> has a nontrivial image in the group of germs of homeomorphisms of <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" /> at <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" />. If this group of germs is left-orderable for all <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" />, then so is <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 Burns-Hale.</p>
<p><strong>Example:</strong> (Rolfsen-Wiest) Let <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" /> be the group of PL homeomorphisms of the unit disk (thought of as a PL square in the plane) fixed on the boundary. If <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> is a finitely generated subgroup, there is a point <img src="https://s0.wp.com/latex.php?latex=p&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p" title="p" class="latex" /> in the frontier of <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7Bfix%7D%28H%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{fix}(H)" title="&#92;text{fix}(H)" class="latex" />. Note that <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> has a nontrivial image in the group of piecewise linear homeomorphisms of the projective space of lines through <img src="https://s0.wp.com/latex.php?latex=p&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p" title="p" class="latex" />. Since the fixed point set of a finitely generated subgroup is equal to the intersection of the fixed point sets of a finite generating set, it is itself a polyhedron. Hence <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> fixes some line through <img src="https://s0.wp.com/latex.php?latex=p&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p" title="p" class="latex" />, and therefore has a nontrivial image in the group of homeomorphisms of an interval. By Burns-Hale, <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 left orderable.</p>
<p><strong>Example:</strong> Let <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" /> be the group of diffeomorphisms of the unit disk, fixed on the boundary. If <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> is a finitely generated subgroup, then at a non-isolated point <img src="https://s0.wp.com/latex.php?latex=p&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p" title="p" class="latex" /> in <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7Bfix%7D%28H%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{fix}(H)" title="&#92;text{fix}(H)" class="latex" /> the group <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> fixes some tangent vector to <img src="https://s0.wp.com/latex.php?latex=p&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p" title="p" class="latex" /> (a limit of short straight lines from <img src="https://s0.wp.com/latex.php?latex=p&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p" title="p" class="latex" /> to nearby fixed points). Consequently the image of <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> in <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BGL%7D%28T_p%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{GL}(T_p)" title="&#92;text{GL}(T_p)" class="latex" /> is reducible, and is conjugate into an affine subgroup, which is left orderable. If the image is nontrivial, we are done by Burns-Hale. If it is trivial, then the linear part of <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> at <img src="https://s0.wp.com/latex.php?latex=p&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p" title="p" class="latex" /> is trivial, and therefore by the <a href="http://www.ams.org/mathscinet-getitem?mr=0356087">Thurston stability theorem</a>, there is a nontrivial homomorphism from <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> to the (orderable) group of translations of the plane. By Burns-Hale, we conclude that <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 left orderable.</p>
<p>The second example does not require infinite differentiability, just <img src="https://s0.wp.com/latex.php?latex=C%5E1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C^1" title="C^1" class="latex" />, the necessary hypothesis to apply the Thurston stability theorem. This is such a beautiful and powerful theorem that it is worth making an aside to discuss it. Thurston&#8217;s theorem says that if <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> is a finitely generated group of germs of diffeomorphisms of a manifold fixing a common point, then a suitable limit of rescaled actions of the group near the fixed point converge to a nontrivial action by translations. One way to think of this is in terms of power series: if <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" /> is a group of real analytic diffeomorphisms of the line, fixing the point <img src="https://s0.wp.com/latex.php?latex=0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="0" title="0" class="latex" />, then every <img src="https://s0.wp.com/latex.php?latex=h+%5Cin+H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="h &#92;in H" title="h &#92;in H" class="latex" /> can be expanded as a power series: <img src="https://s0.wp.com/latex.php?latex=h%28x%29+%3D+c_1%28h%29x+%2B+c_2%28h%29x%5E2+%2B+%5Ccdots&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="h(x) = c_1(h)x + c_2(h)x^2 + &#92;cdots" title="h(x) = c_1(h)x + c_2(h)x^2 + &#92;cdots" class="latex" />. The function <img src="https://s0.wp.com/latex.php?latex=h+%5Cto+c_1%28h%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="h &#92;to c_1(h)" title="h &#92;to c_1(h)" class="latex" /> is a multiplicative homomorphism; however, if the logarithm of <img src="https://s0.wp.com/latex.php?latex=c_1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="c_1" title="c_1" class="latex" /> is identically zero, then if <img src="https://s0.wp.com/latex.php?latex=i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="i" title="i" class="latex" /> is the first index for which some <img src="https://s0.wp.com/latex.php?latex=c_i%28h%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="c_i(h)" title="c_i(h)" class="latex" /> is nonzero, then <img src="https://s0.wp.com/latex.php?latex=h+%5Cto+c_i%28h%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="h &#92;to c_i(h)" title="h &#92;to c_i(h)" class="latex" /> is an <em>additive</em> homomorphism. The choice of coefficient <img src="https://s0.wp.com/latex.php?latex=i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="i" title="i" class="latex" /> is a &#8220;gauge&#8221;, adapted to <img src="https://s0.wp.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H" title="H" class="latex" />, that sees the most significant nontrivial part; this leading term is a character (i.e. a homomorphism to an abelian group), since the nonabelian corrections have strictly higher degree. Thurston&#8217;s insight was to realize that for a <em>finitely generated</em> group of germs of <img src="https://s0.wp.com/latex.php?latex=C%5E1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C^1" title="C^1" class="latex" /> diffeomorphisms with trivial linear part, one can find some gauge that sees the most significant nontrivial part of the action of the group, and at this gauge, the action looks abelian. There is a subtlety, that one must restrict attention to <em>finitely generated</em> groups of homeomorphisms: on each scale of a sequence of finer and finer scales, one of a finite generating set differs the most from the identity; one must pass to a subsequence of scales for which this one element is constant (this is where the finite generation is used). The necessity of this condition is demonstrated by a theorem of <a href="http://www.ams.org/mathscinet-getitem?mr=0474327">Sergeraert</a>: the group of germs of (<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" />) diffeomorphisms of the unit interval, infinitely tangent to the identity at both endpoints (i.e. with trivial power series at each endpoint) is perfect, and therefore admits no nontrivial homomorphism to an abelian group.</p>
<p>Let us now return to the original question. The examples above suggest that it might be possible to find a left ordering on the group of homeomorphisms of the disk, fixed on the boundary. However, I think this is misleading. The construction of a left ordering in either category (PL or smooth) was ad hoc, and depended on locality in two different ways: the locality of the property of left orderability (i.e. Burns-Hale) and the tameness of groups of PL or smooth homeomorphisms blown up near a common fixed point. Rescaling an arbitrary homeomorphism about a fixed point does not make things any less complicated. Burns-Hale and Filipkiewicz together suggest that one should look for a structural dissimilarity between the group of homeomorphisms of the disk and of the interval that persists in finitely generated subgroups. The simplest way to distinguish between the two spaces algebraically is in terms of their lattices of closed (or equivalently, open) subsets. To a topological 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" />, one can associate the lattice <img src="https://s0.wp.com/latex.php?latex=%5CLambda%28X%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;Lambda(X)" title="&#92;Lambda(X)" class="latex" /> of (nonempty, for the sake of argument) closed subsets of <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" />, ordered by inclusion. One can reconstruct the 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" /> from this lattice, since points 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" /> correspond to minimal elements. However, any surjective map <img src="https://s0.wp.com/latex.php?latex=X+%5Cto+Y&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X &#92;to Y" title="X &#92;to Y" class="latex" /> defines an embedding <img src="https://s0.wp.com/latex.php?latex=%5CLambda%28Y%29+%5Cto+%5CLambda%28X%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;Lambda(Y) &#92;to &#92;Lambda(X)" title="&#92;Lambda(Y) &#92;to &#92;Lambda(X)" class="latex" />, so there are many structure-preserving morphisms between such lattices. The lattice <img src="https://s0.wp.com/latex.php?latex=%5CLambda%28X%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;Lambda(X)" title="&#92;Lambda(X)" class="latex" /> is an <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BAut%7D%28X%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Aut}(X)" title="&#92;text{Aut}(X)" class="latex" />-space in an obvious way, and one can study algebraic maps <img src="https://s0.wp.com/latex.php?latex=%5CLambda%28Y%29+%5Cto+%5CLambda%28X%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;Lambda(Y) &#92;to &#92;Lambda(X)" title="&#92;Lambda(Y) &#92;to &#92;Lambda(X)" class="latex" /> together with homomorphisms <img src="https://s0.wp.com/latex.php?latex=%5Crho%3A%5Ctext%7BAut%7D%28Y%29+%5Cto+%5Ctext%7BAut%7D%28X%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho:&#92;text{Aut}(Y) &#92;to &#92;text{Aut}(X)" title="&#92;rho:&#92;text{Aut}(Y) &#92;to &#92;text{Aut}(X)" class="latex" /> for which the algebraic maps respect the induced <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BAut%7D%28Y%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Aut}(Y)" title="&#92;text{Aut}(Y)" class="latex" />-structures. A weaker &#8220;localization&#8221; of this condition asks merely that for points (i.e. minimal elements) <img src="https://s0.wp.com/latex.php?latex=p%2Cp%27+%5Cin+%5CLambda%28Y%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p,p&#039; &#92;in &#92;Lambda(Y)" title="p,p&#039; &#92;in &#92;Lambda(Y)" class="latex" /> in the same <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BAut%7D%28Y%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Aut}(Y)" title="&#92;text{Aut}(Y)" class="latex" />-orbit, their images in <img src="https://s0.wp.com/latex.php?latex=%5CLambda%28X%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;Lambda(X)" title="&#92;Lambda(X)" class="latex" /> are in the same <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BAut%7D%28X%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Aut}(X)" title="&#92;text{Aut}(X)" class="latex" />-orbit. This motivates the following:</p>
<p><strong>Proposition:</strong> There is a surjective map from the unit interval to the unit disk so that the preimages of any two points are homeomorphic.</p>
<p><em>Sketch of Proof:</em> This proposition follows from two simpler propositions. The first is that there is a surjective map from the unit interval to itself so that every point preimage is a Cantor set. The second is that there is a surjective map from the unit interval to the unit disk so that the preimage of any point is finite. A composition of these two maps gives the desired map, since a finite union of Cantor sets is itself a Cantor set.</p>
<p>There are many surjective maps from the unit interval to the unit disk so that the preimage of any point is finite. For example, 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 hyperbolic three-manifold fibering over the circle with fiber <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" />, then the universal cover of a fiber <img src="https://s0.wp.com/latex.php?latex=%5Cwidetilde%7BS%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;widetilde{S}" title="&#92;widetilde{S}" class="latex" /> is properly embedded in 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" />-space, and its ideal boundary (a circle) maps surjectively and finitely-to-one to the sphere at infinity of 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" />-space. Restricting to a suitable subinterval gives the desired map.</p>
<p>To obtain the first proposition, one builds a surjective map from the interval to itself inductively; there are many possible ways to do this, and details are left to the reader. qed.</p>
<p>It is not clear how much insight such a construction gives.</p>
<p>Another approach to the original question involves trying to construct an explicit (finitely generated) subgroup of the group of homeomorphisms of the disk that is not left orderable. There is a &#8220;cheap&#8221; method to produce finitely presented groups with no left-orderable quotients. Let <img src="https://s0.wp.com/latex.php?latex=G+%3D+%5Clangle+x%2Cy+%5C%3B+%7C+%5C%3B+w_1%2C+w_2+%5Crangle&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G = &#92;langle x,y &#92;; | &#92;; w_1, w_2 &#92;rangle" title="G = &#92;langle x,y &#92;; | &#92;; w_1, w_2 &#92;rangle" class="latex" /> be a group defined by a presentation, where <img src="https://s0.wp.com/latex.php?latex=w_1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="w_1" title="w_1" class="latex" /> is a word in the letters <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 <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" />, and <img src="https://s0.wp.com/latex.php?latex=w_2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="w_2" title="w_2" class="latex" /> is a word in the letters <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 <img src="https://s0.wp.com/latex.php?latex=y%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="y^{-1}" title="y^{-1}" class="latex" />. In any left-orderable quotient in which both <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 <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" /> are nontrivial, after reversing the orientation if necessary, we can assume that <img src="https://s0.wp.com/latex.php?latex=x+%3E+%5Ctext%7Bid%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="x &gt; &#92;text{id}" title="x &gt; &#92;text{id}" class="latex" />. If further <img src="https://s0.wp.com/latex.php?latex=y%3E%5Ctext%7Bid%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="y&gt;&#92;text{id}" title="y&gt;&#92;text{id}" class="latex" /> then <img src="https://s0.wp.com/latex.php?latex=w_1+%3E%5Ctext%7Bid%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="w_1 &gt;&#92;text{id}" title="w_1 &gt;&#92;text{id}" class="latex" />, contrary to the fact that <img src="https://s0.wp.com/latex.php?latex=w_1+%3D+%5Ctext%7Bid%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="w_1 = &#92;text{id}" title="w_1 = &#92;text{id}" class="latex" />. If <img src="https://s0.wp.com/latex.php?latex=y%5E%7B-1%7D+%3E%5Ctext%7Bid%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="y^{-1} &gt;&#92;text{id}" title="y^{-1} &gt;&#92;text{id}" class="latex" />, then <img src="https://s0.wp.com/latex.php?latex=w_2+%3E%5Ctext%7Bid%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="w_2 &gt;&#92;text{id}" title="w_2 &gt;&#92;text{id}" class="latex" />, contrary to the fact that <img src="https://s0.wp.com/latex.php?latex=w_2%3D%5Ctext%7Bid%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="w_2=&#92;text{id}" title="w_2=&#92;text{id}" class="latex" />. In either case we get a contradiction. One can try to build by hand nontrivial homeomorphisms <img src="https://s0.wp.com/latex.php?latex=x%2Cy&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="x,y" title="x,y" class="latex" /> of the unit disk, fixed on the boundary, that satisfy <img src="https://s0.wp.com/latex.php?latex=w_1%2Cw_2+%3D%5Ctext%7Bid%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="w_1,w_2 =&#92;text{id}" title="w_1,w_2 =&#92;text{id}" class="latex" />. Some evidence that this will be hard to do comes from the fact that the group of smooth and PL homeomorphisms of the disk are in fact left-orderable: any such <img src="https://s0.wp.com/latex.php?latex=x%2Cy&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="x,y" title="x,y" class="latex" /> can be arbitrarily well-approximated by smooth <img src="https://s0.wp.com/latex.php?latex=x%27%2Cy%27&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="x&#039;,y&#039;" title="x&#039;,y&#039;" class="latex" />; nevertheless at least one of the words <img src="https://s0.wp.com/latex.php?latex=w_1%2Cw_2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="w_1,w_2" title="w_1,w_2" class="latex" /> evaluated on any smooth <img src="https://s0.wp.com/latex.php?latex=x%27%2Cy%27&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="x&#039;,y&#039;" title="x&#039;,y&#039;" class="latex" /> will be nontrivial. Other examples of finitely presented groups that are not left orderable include higher <strong>Q</strong>-rank lattices (e.g. subgroups of finite index in <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BSL%7D%28n%2C%5Cmathbb%7BZ%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{SL}(n,&#92;mathbb{Z})" title="&#92;text{SL}(n,&#92;mathbb{Z})" class="latex" /> when <img src="https://s0.wp.com/latex.php?latex=n%5Cge+3&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n&#92;ge 3" title="n&#92;ge 3" class="latex" />), by a <a href="http://www.ams.org/mathscinet-getitem?mr=1198459">result</a> of Dave Witte-Morris. Suppose such a group admits a faithful action by homeomorphisms on some closed surface of genus at least <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" />. Since such groups do not admit homogeneous quasimorphisms, their image in the mapping class group of the surface is finite, so after passing to a subgroup of finite index, one obtains a (lifted) action on the universal cover. If the genus of the surface is at least <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" />, this action can be compactified to an action by homeomorphisms on the unit disk (thought of as the universal cover of a hyperbolic surface) fixed pointwise on the boundary. Fortunately or unfortunately, it is already known by <a href="http://www.ams.org/mathscinet-getitem?mr=2026546">Franks-Handel</a> (see also <a href="http://www.ams.org/mathscinet-getitem?mr=1946555">Polterovich</a>) that such groups admit no area-preserving actions on closed oriented surfaces (other than those factoring through a finite group), and it is consistent with the so-called &#8220;Zimmer program&#8221; that they should admit no actions even without the area-preserving hypothesis when the genus is positive (of course, <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BSL%7D%283%2C%5Cmathbb%7BR%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{SL}(3,&#92;mathbb{R})" title="&#92;text{SL}(3,&#92;mathbb{R})" class="latex" /> admits a projective action on <img src="https://s0.wp.com/latex.php?latex=S%5E2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S^2" title="S^2" class="latex" />). Actually, higher rank lattices are very fragile, because of Margulis&#8217; normal subgroup theorem. Every normal subgroup of such a lattice is either finite or finite index, so to prove the results of Franks-Handel and Polterovich, it suffices to find a single element in the group of infinite order that acts trivially. Unipotent elements are exponentially distorted in the word metric (i.e. the cyclic subgroups they generate are not quasi-isometrically embedded), so one &#8220;just&#8221; needs to show that groups of area-preserving diffeomorphisms of closed surfaces (of genus at least <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" />) do not contain such distorted elements. Some naturally occurring non-left orderable groups include some (rare) 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 groups, amenable but not locally indicable groups, and a few others. It is hard to construct actions of such groups on a disk, although certain flows on <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" />-manifolds give rise to actions of the fundamental group on a plane.</p>
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