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		<title>Some Sylow arguments</title>
		<link>http://regularmaps.wordpress.com/2011/06/16/some-sylow-arguments/</link>
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		<pubDate>Thu, 16 Jun 2011 12:23:26 +0000</pubDate>
		<dc:creator>Nick Gill</dc:creator>
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		<description><![CDATA[I want to outline some arguments concerning Sylow groups that are based on results in this paper of Conder, Potočnik and Širán. My arguments will look slightly different from those of CPS because I will restrict myself to orientable surfaces, and will define the group which is associated with my regular map according to the [&#8230;]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=regularmaps.wordpress.com&#038;blog=22821215&#038;post=105&#038;subd=regularmaps&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p>I want to outline some arguments concerning Sylow groups that are based on results in <a href="http://www.ams.org/mathscinet-getitem?mr=2725192">this paper</a> of <a href="http://www.ams.org/mathscinet/search/publications.html?pg1=IID&amp;s1=50940">Conder</a>, <a href="http://www.ams.org/mathscinet/search/publications.html?pg1=IID&amp;s1=366771">Potočnik</a> and <a href="http://www.ams.org/mathscinet/search/publications.html?pg1=IID&amp;s1=163115">Širán</a>. My arguments will look slightly different from those of CPS because I will restrict myself to orientable surfaces, and will define the group <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' /> which is associated with my regular map according to the previous posts on this blog (the group in CPS is constructed differently &#8211; it is twice as large as ours).</p>
<p>For the purposes of this post all maps will be finite, hence (as <a href="http://regularmaps.wordpress.com/2011/05/18/finite-maps-equal-compact-surfaces/">we proved earlier</a>) the corresponding surface is compact and we can define the Euler characteristic <img src='http://s0.wp.com/latex.php?latex=%5Cchi&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;chi' title='&#92;chi' class='latex' />. Let <img src='http://s0.wp.com/latex.php?latex=%28G%2C+%5Cmathcal%7BV%7D%2C+%5Cmathcal%7BS%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(G, &#92;mathcal{V}, &#92;mathcal{S})' title='(G, &#92;mathcal{V}, &#92;mathcal{S})' class='latex' /> be a regular topological map of type <img src='http://s0.wp.com/latex.php?latex=%28m%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(m,n)' title='(m,n)' class='latex' /> (where these are <em>true orders</em>). Recall that, when the map is regular we can think of <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' /> as acting on the map via homeomorphisms of the surface (we can&#8217;t do this for non-regular maps), and this is how we will think of <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' /> in what follows..</p>
<p>Write <img src='http://s0.wp.com/latex.php?latex=V&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='V' title='V' class='latex' /> (resp. <img src='http://s0.wp.com/latex.php?latex=E&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='E' title='E' class='latex' />, <img src='http://s0.wp.com/latex.php?latex=F&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='F' title='F' class='latex' />) for the number of vertices (resp. edges, faces) in our map. I assert that the following follows immediately from the work of Jones &amp; Singerman that we have already discussed:</p>
<blockquote><p><img src='http://s0.wp.com/latex.php?latex=%5Cchi%3DV-E%2BF%3D%7CG%7C%28%5Cfrac1%7Bm%7D%2B%5Cfrac1%7Bn%7D%2B%5Cfrac12%29+%3D+-%7CG%7C%5Cfrac%7Bmn-2m-2n%7D%7B2mn%7D.&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;chi=V-E+F=|G|(&#92;frac1{m}+&#92;frac1{n}+&#92;frac12) = -|G|&#92;frac{mn-2m-2n}{2mn}.' title='&#92;chi=V-E+F=|G|(&#92;frac1{m}+&#92;frac1{n}+&#92;frac12) = -|G|&#92;frac{mn-2m-2n}{2mn}.' class='latex' /></p></blockquote>
<p>The first equality is the formula for the Euler characteristic, the second follows by regularity, the third by rearranging. Note that the second equality is based on the fact (which will be useful in its own right) that a vertex (resp. edge, resp. face) stabilizer is a cyclic subgroup of order <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> (resp. <img src='http://s0.wp.com/latex.php?latex=2%2C+n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='2, n' title='2, n' class='latex' />).</p>
<p>Now write <img src='http://s0.wp.com/latex.php?latex=%5Bm%2Cn%5D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='[m,n]' title='[m,n]' class='latex' /> (resp. <img src='http://s0.wp.com/latex.php?latex=%28m%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(m,n)' title='(m,n)' class='latex' />) for the lcm (resp. gcd) of <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' />. Then we can rearrange the above equation to obtain that</p>
<blockquote><p><img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%7CG%7C%7D%7B%5Bm%2Cn%5D%7D+%3D+%5Cfrac%7B-2%28m%2Cn%29%5Cchi%7D%7Bmn-2m-2n%7D+%3D+%5Cfrac%7B-2%5Cchi%7D%7B%5Bm%2Cn%5D-2%5Cfrac%7Bm%2Bn%7D%7B%28m%2Cn%29%7D%7D.&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{|G|}{[m,n]} = &#92;frac{-2(m,n)&#92;chi}{mn-2m-2n} = &#92;frac{-2&#92;chi}{[m,n]-2&#92;frac{m+n}{(m,n)}}.' title='&#92;frac{|G|}{[m,n]} = &#92;frac{-2(m,n)&#92;chi}{mn-2m-2n} = &#92;frac{-2&#92;chi}{[m,n]-2&#92;frac{m+n}{(m,n)}}.' class='latex' /></p></blockquote>
<p>The two equations displayed so far immediately yield some nice consequences. In what follows, if <img src='http://s0.wp.com/latex.php?latex=k&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='k' title='k' class='latex' /> is an integer, <img src='http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p' title='p' class='latex' /> a prime, write <img src='http://s0.wp.com/latex.php?latex=%7Ck%7C_p%3Dp%5Es&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|k|_p=p^s' title='|k|_p=p^s' class='latex' /> if <img src='http://s0.wp.com/latex.php?latex=p%5Es&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p^s' title='p^s' class='latex' /> is the highest power of <img src='http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p' title='p' class='latex' /> that divides <img src='http://s0.wp.com/latex.php?latex=k&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='k' title='k' class='latex' />.</p>
<p><span style="text-decoration:underline;">Proposition</span> 1: Let <img src='http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p' title='p' class='latex' /> be a prime dividing the order of <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' />. Either <img src='http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p' title='p' class='latex' /> divides <img src='http://s0.wp.com/latex.php?latex=%5Cchi&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;chi' title='&#92;chi' class='latex' /> or a Sylow <img src='http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p' title='p' class='latex' />-subgroup of <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' /> is cyclic.</p>
<p><span style="text-decoration:underline;">Proof</span>: All of the statements that we make depend only on the equations given above. Let <img src='http://s0.wp.com/latex.php?latex=P&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='P' title='P' class='latex' /> be a Sylow <img src='http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p' title='p' class='latex' />-subgroup of <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' />. Suppose that <img src='http://s0.wp.com/latex.php?latex=p%5Cnmid+%5Cchi&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p&#92;nmid &#92;chi' title='p&#92;nmid &#92;chi' class='latex' />. Then either <img src='http://s0.wp.com/latex.php?latex=p%5Cmid%5Bm%2Cn%5D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p&#92;mid[m,n]' title='p&#92;mid[m,n]' class='latex' /> or <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_p%3D2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_p=2' title='|G|_p=2' class='latex' />. But in the latter case <img src='http://s0.wp.com/latex.php?latex=P&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='P' title='P' class='latex' /> is cyclic and we&#8217;re done. So we assume from here on that <img src='http://s0.wp.com/latex.php?latex=p%5Cmid+%5Bm%2Cn%5D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p&#92;mid [m,n]' title='p&#92;mid [m,n]' class='latex' />.</p>
<p>Suppose that <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_p%3D%7C%5Bm%2Cn%5D%7C_p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_p=|[m,n]|_p' title='|G|_p=|[m,n]|_p' class='latex' />. In this case <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_p%3D%7Cm%7C_p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_p=|m|_p' title='|G|_p=|m|_p' class='latex' /> or <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_p%3D%7Cn%7C_p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_p=|n|_p' title='|G|_p=|n|_p' class='latex' />; suppose, without lost of generality that <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_p%3D%7Cm%7C_p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_p=|m|_p' title='|G|_p=|m|_p' class='latex' />. Since we know that <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' /> contains a cyclic group of order <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> (a vertex stabilizer) we conclude that <img src='http://s0.wp.com/latex.php?latex=P&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='P' title='P' class='latex' /> is cyclic as required.</p>
<p>Suppose that <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_p%5Cneq+%7C%5Bm%2Cn%5D%7C_p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_p&#92;neq |[m,n]|_p' title='|G|_p&#92;neq |[m,n]|_p' class='latex' />; then <img src='http://s0.wp.com/latex.php?latex=p%5Cmid+%5Cfrac%7B%7CG%7C%7D%7B%5Bm%2Cn%5D%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p&#92;mid &#92;frac{|G|}{[m,n]}' title='p&#92;mid &#92;frac{|G|}{[m,n]}' class='latex' />. Since <img src='http://s0.wp.com/latex.php?latex=p%5Cnmid%5Cchi&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p&#92;nmid&#92;chi' title='p&#92;nmid&#92;chi' class='latex' /> we conclude that <img src='http://s0.wp.com/latex.php?latex=p%3D2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p=2' title='p=2' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=%5Cchi&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;chi' title='&#92;chi' class='latex' /> is odd. But this implies that <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> are odd and so <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_2%3D2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_2=2' title='|G|_2=2' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=P&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='P' title='P' class='latex' /> is cyclic as required.</p>
<p style="text-align:right;">QED</p>
<p style="text-align:left;">Now it is well-known in group theory that any group with a cyclic Sylow <img src='http://s0.wp.com/latex.php?latex=2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='2' title='2' class='latex' />-subgroup is solvable. Thus Prop. 1 implies that any map on an orientable surface with odd Euler characteristic corresponds to a solvable group. Great!! Except that no orientable surfaces with odd Euler characteristic exist: in the orientable case <img src='http://s0.wp.com/latex.php?latex=%5Cchi%3D2-2g&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;chi=2-2g' title='&#92;chi=2-2g' class='latex' /> where <img src='http://s0.wp.com/latex.php?latex=g&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='g' title='g' class='latex' /> is the genus of the surface. (Incidentally I&#8217;d like a good explanation of that. I really don&#8217;t understand how <img src='http://s0.wp.com/latex.php?latex=%5Cchi&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;chi' title='&#92;chi' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=g&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='g' title='g' class='latex' /> work in the world of topology.)</p>
<p style="text-align:left;">CPS have great success in using Prop. 1 to classify regular maps, with most of their attention focussed on non-orientable surfaces. But that story is for another day. For now let me do some bookwork and write down an extension of Prop. 1 that might come in handy to someone someday.</p>
<p style="text-align:left;"><span style="text-decoration:underline;">Proposition 2</span>: Let <img src='http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p' title='p' class='latex' /> be a prime dividing the order of <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' />. Either <img src='http://s0.wp.com/latex.php?latex=p%5E2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p^2' title='p^2' class='latex' /> divides <img src='http://s0.wp.com/latex.php?latex=%5Cchi&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;chi' title='&#92;chi' class='latex' /> or a Sylow <img src='http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p' title='p' class='latex' />-subgroup of <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' /> has a cyclic subgroup of index <img src='http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p' title='p' class='latex' />.</p>
<p style="text-align:left;"><span style="text-decoration:underline;">Proof</span>: Again all of the statements that we make depend only on the equations given above. Let <img src='http://s0.wp.com/latex.php?latex=P&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='P' title='P' class='latex' /> be a Sylow <img src='http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p' title='p' class='latex' />-subgroup of <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' />. Suppose that <img src='http://s0.wp.com/latex.php?latex=p%5E2%5Cnmid+%5Cchi&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p^2&#92;nmid &#92;chi' title='p^2&#92;nmid &#92;chi' class='latex' />; there are three possibilities: (a) <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_p%3Dp&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_p=p' title='|G|_p=p' class='latex' />; or (b) <img src='http://s0.wp.com/latex.php?latex=p%3D2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p=2' title='p=2' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_2%5Cleq+4&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_2&#92;leq 4' title='|G|_2&#92;leq 4' class='latex' />; or (c) <img src='http://s0.wp.com/latex.php?latex=p%5Cmid+%5Bm%2Cn%5D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p&#92;mid [m,n]' title='p&#92;mid [m,n]' class='latex' />. The first two cases yield the result immediately, hence we assume that (c) holds.</p>
<p style="text-align:left;">Suppose that <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_p%5Cleq+p+%5Ccdot+%7C%5Bm%2Cn%5D%7C_p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_p&#92;leq p &#92;cdot |[m,n]|_p' title='|G|_p&#92;leq p &#92;cdot |[m,n]|_p' class='latex' />. In this case, WLOG, <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_p%5Cleq+p%5Ccdot+%7Cm%7C_p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_p&#92;leq p&#92;cdot |m|_p' title='|G|_p&#92;leq p&#92;cdot |m|_p' class='latex' /> or <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_p%3D%7Cn%7C_p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_p=|n|_p' title='|G|_p=|n|_p' class='latex' />. Since we know that <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' /> contains a cyclic group of order <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> (a vertex stabilizer) the result follows.</p>
<p style="text-align:left;">Finally suppose that <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_p+%3E+p+%5Ccdot+%7C%5Bm%2Cn%5D%7C_p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_p &gt; p &#92;cdot |[m,n]|_p' title='|G|_p &gt; p &#92;cdot |[m,n]|_p' class='latex' />. Then <img src='http://s0.wp.com/latex.php?latex=p%3D2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p=2' title='p=2' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=%5Cchi%3D2a&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;chi=2a' title='&#92;chi=2a' class='latex' /> for some odd integer <img src='http://s0.wp.com/latex.php?latex=a&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='a' title='a' class='latex' />. But now if either <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> or <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> are even, then <img src='http://s0.wp.com/latex.php?latex=%5Bm%2Cn%5D-2%5Cfrac%7Bm%2Bn%7D%7B%28m%2Cn%29%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='[m,n]-2&#92;frac{m+n}{(m,n)}' title='[m,n]-2&#92;frac{m+n}{(m,n)}' class='latex' /> is even and we conclude that <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_2%3D2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_2=2' title='|G|_2=2' class='latex' /> and the result follows. On the other hand if <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> are both odd, then <img src='http://s0.wp.com/latex.php?latex=%7CG%7C_2%3D2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|G|_2=2' title='|G|_2=2' class='latex' /> and the result follows.</p>
<p style="text-align:right;">QED</p>
<p style="text-align:left;">I am most interested in applying Prop. 2 in the case <img src='http://s0.wp.com/latex.php?latex=p%3D2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p=2' title='p=2' class='latex' />. In this situation we know explicitly what the group <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' /> looks like (see for instance <a href="http://www.ams.org/mathscinet-getitem?mr=160816">this paper</a>, and the papers it cites). I wanted to write a load more stuff on this but I&#8217;m out of time for now. More anon.</p>
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		<title>From algebraic maps to Riemannian maps</title>
		<link>http://regularmaps.wordpress.com/2011/05/26/from-algebraic-maps-to-riemannian-maps/</link>
		<comments>http://regularmaps.wordpress.com/2011/05/26/from-algebraic-maps-to-riemannian-maps/#comments</comments>
		<pubDate>Thu, 26 May 2011 10:23:44 +0000</pubDate>
		<dc:creator>Nick Gill</dc:creator>
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		<description><![CDATA[In the earlier post What is a regular map? we stated that the three categories AM, TM and RM were equivalent, but we did not complete the proof. The main task that we left open was to demonstrate how, if given an element of AM, we can construct (in a natural way) an element of [&#8230;]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=regularmaps.wordpress.com&#038;blog=22821215&#038;post=82&#038;subd=regularmaps&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p>In the earlier post <a href="http://regularmaps.wordpress.com/2011/05/10/what-is-a-regular-map/">What is a regular map?</a> we stated that the three categories <strong>AM</strong>, <strong>TM</strong> and <strong>RM</strong> were equivalent, but we did not complete the proof. The main task that we left open was to demonstrate how, if given an element of <strong>AM</strong>, we can construct (in a natural way) an element of <strong>RM</strong>. This construction is the topic of today&#8217;s post.</p>
<p>Before we get going, a caveat: to properly prove the stated categorical equivalences I really need to ensure that morphisms behave properly. As it is I&#8217;m going to content myself with an inspection of the objects in each category (go the <a href="http://www.ams.org/mathscinet-getitem?mr=505721">original paper of Jones and Singerman</a> for a full treatment).</p>
<p>Let <img src='http://s0.wp.com/latex.php?latex=%28G%2C+%5COmega%2C+x%2C+y%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(G, &#92;Omega, x, y)' title='(G, &#92;Omega, x, y)' class='latex' /> be an element of <strong>AM(m,n)</strong> and assume that <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> are the <em>true orders</em> of the elements <img src='http://s0.wp.com/latex.php?latex=y&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='y' title='y' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=z%3Dy%5E%7B-1%7Dx&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='z=y^{-1}x' title='z=y^{-1}x' class='latex' />. Recall that <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' /> is a quotient of the group</p>
<blockquote><p><img src='http://s0.wp.com/latex.php?latex=%5CGamma+%3D+%5CGamma%28m%2Cn%29%3D%5Clangle+x%2C+y%2Cz+%5C%2C+%5Cmid+%5C%2C+x%5E2%3Dy%5Em%3Dz%5En%3Dxyz%3D1%5Crangle.&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma = &#92;Gamma(m,n)=&#92;langle x, y,z &#92;, &#92;mid &#92;, x^2=y^m=z^n=xyz=1&#92;rangle.' title='&#92;Gamma = &#92;Gamma(m,n)=&#92;langle x, y,z &#92;, &#92;mid &#92;, x^2=y^m=z^n=xyz=1&#92;rangle.' class='latex' /></p></blockquote>
<h2>Some Riemannian geometry</h2>
<p>Let us consider the group</p>
<blockquote><p><img src='http://s0.wp.com/latex.php?latex=%5CGamma+%3D+%5CGamma%28l%2Cm%2Cn%29%3D%5Clangle+x%2C+y%2Cz+%5C%2C+%5Cmid+%5C%2C+x%5El%3Dy%5Em%3Dz%5En%3Dxyz%3D1%5Crangle.&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma = &#92;Gamma(l,m,n)=&#92;langle x, y,z &#92;, &#92;mid &#92;, x^l=y^m=z^n=xyz=1&#92;rangle.' title='&#92;Gamma = &#92;Gamma(l,m,n)=&#92;langle x, y,z &#92;, &#92;mid &#92;, x^l=y^m=z^n=xyz=1&#92;rangle.' class='latex' /></p></blockquote>
<p>where we assume, without loss of generality, that <img src='http://s0.wp.com/latex.php?latex=l%5Cleq+m+%5Cleq+n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='l&#92;leq m &#92;leq n' title='l&#92;leq m &#92;leq n' class='latex' />. The group <img src='http://s0.wp.com/latex.php?latex=%5CGamma&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma' title='&#92;Gamma' class='latex' /> is well known in Riemannian geometry: it is the <em><img src='http://s0.wp.com/latex.php?latex=%28l%2Cm%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(l,m,n)' title='(l,m,n)' class='latex' />-triangle group.</em> It has a natural action on a simply connected Riemann surface, preserving a tessellation of that surface by isometric geodesic triangles with angles of size <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7Dl%2C+%5Cfrac%7B%5Cpi%7Dm&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}l, &#92;frac{&#92;pi}m' title='&#92;frac{&#92;pi}l, &#92;frac{&#92;pi}m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7Dn&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}n' title='&#92;frac{&#92;pi}n' class='latex' />. (I will not define terms like <em>tesselation</em> or <em>geodesic triangle</em> here; your intuition is likely to be good enough to understand what is going on.) J&amp;S allow for the possibility that <img src='http://s0.wp.com/latex.php?latex=l%2C+m%2C+n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='l, m, n' title='l, m, n' class='latex' /> are not all finite, but I won&#8217;t bother with that generality here.</p>
<p>The classical <em>Uniformization theorem of Poincaré</em> states that there are precisely three simply connected Riemann surfaces and, what is more, that they can only be tessellated by triangles of a certain form. The breakdown is as follows:</p>
<p><strong>1. The unit sphere</strong> <img src='http://s0.wp.com/latex.php?latex=S%5E2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='S^2' title='S^2' class='latex' /> in <img src='http://s0.wp.com/latex.php?latex=%5Cmathbb%7BR%7D%5E3&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathbb{R}^3' title='&#92;mathbb{R}^3' class='latex' /> (a surface of positive constant curvature with the Euclidean metric): this can be tessellated by isometric triangles with angles <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7Dl%2C+%5Cfrac%7B%5Cpi%7Dm&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}l, &#92;frac{&#92;pi}m' title='&#92;frac{&#92;pi}l, &#92;frac{&#92;pi}m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7Dn&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}n' title='&#92;frac{&#92;pi}n' class='latex' /> if and only if <img src='http://s0.wp.com/latex.php?latex=%5Cfrac1%7Bl%7D+%2B+%5Cfrac1%7Bm%7D+%2B+%5Cfrac1%7Bn%7D+%3E1&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac1{l} + &#92;frac1{m} + &#92;frac1{n} &gt;1' title='&#92;frac1{l} + &#92;frac1{m} + &#92;frac1{n} &gt;1' class='latex' />. This condition allows us to explicitly list all possible tesselations; in all cases the associated group <img src='http://s0.wp.com/latex.php?latex=%5CGamma&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma' title='&#92;Gamma' class='latex' /> is finite:</p>
<ul>
<li><img src='http://s0.wp.com/latex.php?latex=%28l%2Cm%2Cn%29%3D%282%2C2%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(l,m,n)=(2,2,n)' title='(l,m,n)=(2,2,n)' class='latex' />. The tesselation looks like a ring of <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> vertices around the equator of the sphere; with vertices at each pole. The group <img src='http://s0.wp.com/latex.php?latex=%5CGamma%5Ccong+D_n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma&#92;cong D_n' title='&#92;Gamma&#92;cong D_n' class='latex' /> the dihedral group of order <img src='http://s0.wp.com/latex.php?latex=2n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='2n' title='2n' class='latex' />.</li>
<li><img src='http://s0.wp.com/latex.php?latex=%28l%2Cm%2Cn%29%3D%282%2C3%2C3%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(l,m,n)=(2,3,3)' title='(l,m,n)=(2,3,3)' class='latex' />. The tesselation is identical to the tetrahedron, and <img src='http://s0.wp.com/latex.php?latex=%5CGamma%5Ccong+A_4&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma&#92;cong A_4' title='&#92;Gamma&#92;cong A_4' class='latex' />.</li>
<li><img src='http://s0.wp.com/latex.php?latex=%28l%2Cm%2Cn%29%3D%282%2C3%2C4%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(l,m,n)=(2,3,4)' title='(l,m,n)=(2,3,4)' class='latex' />. The tesselation is identical to the octahedron, and <img src='http://s0.wp.com/latex.php?latex=%5CGamma%5Ccong+S_4&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma&#92;cong S_4' title='&#92;Gamma&#92;cong S_4' class='latex' />.</li>
<li><img src='http://s0.wp.com/latex.php?latex=%28l%2Cm%2Cn%29%3D%282%2C3%2C5%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(l,m,n)=(2,3,5)' title='(l,m,n)=(2,3,5)' class='latex' />. The tesselation is identical to the icosahedron, and <img src='http://s0.wp.com/latex.php?latex=%5CGamma%5Ccong+A_5&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma&#92;cong A_5' title='&#92;Gamma&#92;cong A_5' class='latex' />.</li>
</ul>
<p><strong>2. The Euclidean plane </strong><img src='http://s0.wp.com/latex.php?latex=%5Cmathbb%7BR%7D%5E2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathbb{R}^2' title='&#92;mathbb{R}^2' class='latex' /> (a surface of zero constant curvature with the Euclidean metric): this can be tessellated by isometric triangles with angles <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7Dl%2C+%5Cfrac%7B%5Cpi%7Dm&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}l, &#92;frac{&#92;pi}m' title='&#92;frac{&#92;pi}l, &#92;frac{&#92;pi}m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7Dn&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}n' title='&#92;frac{&#92;pi}n' class='latex' /> if and only if <img src='http://s0.wp.com/latex.php?latex=%5Cfrac1%7Bl%7D+%2B+%5Cfrac1%7Bm%7D+%2B+%5Cfrac1%7Bn%7D%3D+1&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac1{l} + &#92;frac1{m} + &#92;frac1{n}= 1' title='&#92;frac1{l} + &#92;frac1{m} + &#92;frac1{n}= 1' class='latex' />. Once again we can explicitly list all possible tesselations.</p>
<ul>
<li><img src='http://s0.wp.com/latex.php?latex=%28l%2Cm%2Cn%29%3D%283%2C3%2C3%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(l,m,n)=(3,3,3)' title='(l,m,n)=(3,3,3)' class='latex' />. The tesselation looks like the standard honeycomb of equilateral triangles; the group <img src='http://s0.wp.com/latex.php?latex=%5CGamma%5Ccong+%28%5Cmathbb%7BZ%7D%5Ctimes+%5Cmathbb%7BZ%7D%29%5Crtimes+C_3&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma&#92;cong (&#92;mathbb{Z}&#92;times &#92;mathbb{Z})&#92;rtimes C_3' title='&#92;Gamma&#92;cong (&#92;mathbb{Z}&#92;times &#92;mathbb{Z})&#92;rtimes C_3' class='latex' />.</li>
<li><img src='http://s0.wp.com/latex.php?latex=%28l%2Cm%2Cn%29%3D%282%2C4%2C4%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(l,m,n)=(2,4,4)' title='(l,m,n)=(2,4,4)' class='latex' />. This looks like the standard tesselation by squares, with each square split into two; here <img src='http://s0.wp.com/latex.php?latex=%5CGamma%5Ccong+%28%5Cmathbb%7BZ%7D%5Ctimes+%5Cmathbb%7BZ%7D%29%5Crtimes+C_4&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma&#92;cong (&#92;mathbb{Z}&#92;times &#92;mathbb{Z})&#92;rtimes C_4' title='&#92;Gamma&#92;cong (&#92;mathbb{Z}&#92;times &#92;mathbb{Z})&#92;rtimes C_4' class='latex' /></li>
<li><img src='http://s0.wp.com/latex.php?latex=%28l%2Cm%2Cn%29%3D%282%2C3%2C6%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(l,m,n)=(2,3,6)' title='(l,m,n)=(2,3,6)' class='latex' />. this looks like the honeycomb of equilater triangles with each triangle split into two; here <img src='http://s0.wp.com/latex.php?latex=%5CGamma%5Ccong+S_6&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma&#92;cong S_6' title='&#92;Gamma&#92;cong S_6' class='latex' />.</li>
</ul>
<p><strong>3. The Hyperbolic plane </strong><img src='http://s0.wp.com/latex.php?latex=%5Cmathbb%7BH%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathbb{H}' title='&#92;mathbb{H}' class='latex' /> (a surface of negative constant curvature with a hyperbolic metric): this can be tessellated by isometric triangles with angles <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7Dl%2C+%5Cfrac%7B%5Cpi%7Dm&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}l, &#92;frac{&#92;pi}m' title='&#92;frac{&#92;pi}l, &#92;frac{&#92;pi}m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7Dn&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}n' title='&#92;frac{&#92;pi}n' class='latex' /> if and only if <img src='http://s0.wp.com/latex.php?latex=%5Cfrac1%7Bl%7D+%2B+%5Cfrac1%7Bm%7D+%2B+%5Cfrac1%7Bn%7D%3D+1&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac1{l} + &#92;frac1{m} + &#92;frac1{n}= 1' title='&#92;frac1{l} + &#92;frac1{m} + &#92;frac1{n}= 1' class='latex' />. In this case there are an infinite number of possibilities &#8211; this is where things get interesting! The smallest triple <img src='http://s0.wp.com/latex.php?latex=%28l%2Cm%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(l,m,n)' title='(l,m,n)' class='latex' /> where we lie in the hyperbolic plane is <img src='http://s0.wp.com/latex.php?latex=%282%2C3%2C7%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(2,3,7)' title='(2,3,7)' class='latex' />; the associated group <img src='http://s0.wp.com/latex.php?latex=%5CGamma&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma' title='&#92;Gamma' class='latex' /> and its quotients are known as <em>Hurwitz groups</em>; they have a <a href="http://www.ams.org/mathscinet-getitem?mr=1041434">huge literature</a>.</p>
<p>In each case the group <img src='http://s0.wp.com/latex.php?latex=%5CGamma&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma' title='&#92;Gamma' class='latex' /> acts by <em>isometries</em> on the simply connected Riemann surface (i.e. it preserves the associated metric); what is more <img src='http://s0.wp.com/latex.php?latex=%5CGamma&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma' title='&#92;Gamma' class='latex' /> acts <em>conformally</em> (angles are also preserved) and <em>totally discontinuously</em> (every group element moves every point of the surface &#8220;a good distance&#8221;).</p>
<h2>Making a Universal Riemann map</h2>
<p>Let us first construct a Riemann map for the <em>universal</em> algebraic map in <strong>AM(m,n)</strong>. Take the group <img src='http://s0.wp.com/latex.php?latex=%5CGamma+%3D+%5CGamma%282%2Cm%2Cn%29%3D%5CGamma%28m%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma = &#92;Gamma(2,m,n)=&#92;Gamma(m,n)' title='&#92;Gamma = &#92;Gamma(2,m,n)=&#92;Gamma(m,n)' class='latex' />.  (Beware: in the algebraic maps context we are not allowed to assume that <img src='http://s0.wp.com/latex.php?latex=m%5Cleq+n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m&#92;leq n' title='m&#92;leq n' class='latex' /> as the distinguished element <img src='http://s0.wp.com/latex.php?latex=y&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='y' title='y' class='latex' /> is of order <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' />. Of course <img src='http://s0.wp.com/latex.php?latex=%5CGamma%28m%2Cn%29%5Ccong+%5CGamma%28n%2Cm%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma(m,n)&#92;cong &#92;Gamma(n,m)' title='&#92;Gamma(m,n)&#92;cong &#92;Gamma(n,m)' class='latex' /> so the discussion of the previous section still applies.)</p>
<p>We have just seen that <img src='http://s0.wp.com/latex.php?latex=%5CGamma%28m%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma(m,n)' title='&#92;Gamma(m,n)' class='latex' /> preserves a tesselation of triangles with angles <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7D2%2C+%5Cfrac%7B%5Cpi%7Dm&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}2, &#92;frac{&#92;pi}m' title='&#92;frac{&#92;pi}2, &#92;frac{&#92;pi}m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7Dn&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}n' title='&#92;frac{&#92;pi}n' class='latex' /> on <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BU%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{U}' title='&#92;mathcal{U}' class='latex' />, the corresponding simply connected Riemann surface. Here is a little piece of the tesselation (taken from J&amp;S), with the actions of <img src='http://s0.wp.com/latex.php?latex=x%2Cy&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='x,y' title='x,y' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=z&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='z' title='z' class='latex' /> inscribed:</p>
<p style="text-align:center;"><a href="http://regularmaps.files.wordpress.com/2011/05/triangletesselation.jpg"><img class="alignnone size-full wp-image-90" title="triangletesselation" src="http://regularmaps.files.wordpress.com/2011/05/triangletesselation.jpg?w=600" alt=""   /></a></p>
<p style="text-align:left;">One can imagine the rest of the surface being covered by repeated copies of  this diamond such that every tesselation-vertex is surrounded either by angles of size <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7D%7Bn%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}{n}' title='&#92;frac{&#92;pi}{n}' class='latex' /> or by angles of size <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7D%7Bm%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}{m}' title='&#92;frac{&#92;pi}{m}' class='latex' />.</p>
<p style="text-align:left;">We construct a Riemann map on the simply connected surface <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BU%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{U}' title='&#92;mathcal{U}' class='latex' /> as follows: The vertices are those tesselation-vertices which are surrounded by angles <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7Dm&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}m' title='&#92;frac{&#92;pi}m' class='latex' /> (in the figure <img src='http://s0.wp.com/latex.php?latex=b&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='b' title='b' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=bx&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='bx' title='bx' class='latex' /> are two such); the edges are simply unions of those lines in the tesselation that join them (in the figure the vertical line segment is one such).</p>
<p style="text-align:left;">The edges of the map we have constructed are all geodesics; they all meet at vertices at angles of <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7D%7Bm%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}{m}' title='&#92;frac{&#92;pi}{m}' class='latex' />, faces are regular <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' />-gons; in other words we have a a Riemann map of type <img src='http://s0.wp.com/latex.php?latex=%28m%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(m,n)' title='(m,n)' class='latex' />. This map is known as the <em>universal</em> Riemann map of type <img src='http://s0.wp.com/latex.php?latex=%28m%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(m,n)' title='(m,n)' class='latex' /> (clearly it corresponds to the universal algebraic map).</p>
<p style="text-align:left;">The dual map &#8211; of type <img src='http://s0.wp.com/latex.php?latex=%28n%2Cm%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(n,m)' title='(n,m)' class='latex' /> &#8211; can be constructed by taking vertices to be the tesselation-vertices which are surrounded by angles <img src='http://s0.wp.com/latex.php?latex=%5Cfrac%7B%5Cpi%7D%7Bn%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;frac{&#92;pi}{n}' title='&#92;frac{&#92;pi}{n}' class='latex' /> and so on.</p>
<h2 style="text-align:left;">The general Riemann map</h2>
<p>Recall that an algebraic map of type <img src='http://s0.wp.com/latex.php?latex=%28m%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(m,n)' title='(m,n)' class='latex' /> is completely determined by an associated <em>mapping subgroup</em> <img src='http://s0.wp.com/latex.php?latex=M&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='M' title='M' class='latex' /> &#8211; any subgroup of <img src='http://s0.wp.com/latex.php?latex=%5CGamma%28m%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma(m,n)' title='&#92;Gamma(m,n)' class='latex' />. The group <img src='http://s0.wp.com/latex.php?latex=M&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='M' title='M' class='latex' /> preserves the tesselation described above and it acts totally discontinuously on the simply connected Riemann surface <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BU%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{U}' title='&#92;mathcal{U}' class='latex' />; we can, therefore construct the quotient Riemann surface <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BS%7D%3D%5Cmathcal%7BU%7D%2FM&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{S}=&#92;mathcal{U}/M' title='&#92;mathcal{S}=&#92;mathcal{U}/M' class='latex' /> on which will be preserved the quotient tesselation.</p>
<p>Now we construct a Riemann map on the surface <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BS%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{S}' title='&#92;mathcal{S}' class='latex' /> in precisely the same way as the previous section. Job done.</p>
<h2>Equivalence of categories</h2>
<p>The fact that the categories <strong>AM</strong>, <strong>TM</strong> and <strong>RM</strong> are equivalent is demonstrated by Prop. 5.3 of J&amp;S. Start with a topological map <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M}' title='&#92;mathcal{M}' class='latex' />; we described in an earlier post how to construct an algebraic map <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BA%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{A}' title='&#92;mathcal{A}' class='latex' /> from <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M}' title='&#92;mathcal{M}' class='latex' />; we now know how to construct a Riemann map <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%27%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M&#039;}' title='&#92;mathcal{M&#039;}' class='latex' /> from <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BA%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{A}' title='&#92;mathcal{A}' class='latex' />. The key point is that the two maps <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M}' title='&#92;mathcal{M}' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%27%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M&#039;}' title='&#92;mathcal{M&#039;}' class='latex' /> are isomorphic (where we view both of them as objects in the category <strong>TM</strong>).</p>
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		<title>Finite maps equal compact surfaces</title>
		<link>http://regularmaps.wordpress.com/2011/05/18/finite-maps-equal-compact-surfaces/</link>
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		<pubDate>Wed, 18 May 2011 15:10:39 +0000</pubDate>
		<dc:creator>Nick Gill</dc:creator>
				<category><![CDATA[Uncategorized]]></category>

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		<description><![CDATA[In the earlier post What is a regular map? we stated a side result without proving it. Let&#8217;s do that now. Prop. A topological map is finite if and only if the surface is compact. Proof. Suppose that the surface is compact and the map is infinite; in other words is infinite. Since the valency [&#8230;]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=regularmaps.wordpress.com&#038;blog=22821215&#038;post=65&#038;subd=regularmaps&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p>In the earlier post <a href="http://regularmaps.wordpress.com/2011/05/10/what-is-a-regular-map/"><em>What is a regular map?</em></a> we stated a side result without proving it. Let&#8217;s do that now.</p>
<p><span style="text-decoration:underline;">Prop.</span> A topological map <img src='http://s0.wp.com/latex.php?latex=%28%5Cmathcal%7BG%7D%2C+%5Cmathcal%7BV%7D%2C+%5Cmathcal%7BS%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(&#92;mathcal{G}, &#92;mathcal{V}, &#92;mathcal{S})' title='(&#92;mathcal{G}, &#92;mathcal{V}, &#92;mathcal{S})' class='latex' /> is finite if and only if the surface <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BS%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{S}' title='&#92;mathcal{S}' class='latex' /> is compact.</p>
<p><span style="text-decoration:underline;">Proof.</span> Suppose that the surface <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BS%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{S}' title='&#92;mathcal{S}' class='latex' /> is compact and the map is infinite; in other words <img src='http://s0.wp.com/latex.php?latex=%5COmega&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Omega' title='&#92;Omega' class='latex' /> is infinite. Since the valency of all the vertices is finite (AG3) we conclude that <img src='http://s0.wp.com/latex.php?latex=%7C%5Cmathcal%7BV%7D%7C&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|&#92;mathcal{V}|' title='|&#92;mathcal{V}|' class='latex' /> is infinite. This implies that there is an accumulation point on <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BS%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{S}' title='&#92;mathcal{S}' class='latex' /> for the set <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BV%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{V}' title='&#92;mathcal{V}' class='latex' />. Let <img src='http://s0.wp.com/latex.php?latex=v_1%2C+v_2%2C+%5Cdots&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='v_1, v_2, &#92;dots' title='v_1, v_2, &#92;dots' class='latex' /> be a converging sequence of vertices; (TM1) implies that for <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> large enough,  these vertices must all be joined to each other and, what is more, they must all have valency 2 (think of the edges between them forming a single line on which they all lie). Then, for <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> large enough every <img src='http://s0.wp.com/latex.php?latex=v_n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='v_n' title='v_n' class='latex' /> lies on two darts <img src='http://s0.wp.com/latex.php?latex=%5Calpha_n%2C+%5Cbeta_n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;alpha_n, &#92;beta_n' title='&#92;alpha_n, &#92;beta_n' class='latex' /> and (provided we label darts appropriately) it is clear that <img src='http://s0.wp.com/latex.php?latex=face%28%5Calpha_n%29+%3D+face%28%5Calpha_m%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='face(&#92;alpha_n) = face(&#92;alpha_m)' title='face(&#92;alpha_n) = face(&#92;alpha_m)' class='latex' /> for <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> large enough. This is a contradiction of (TM4).</p>
<p>Now for the converse; we suppose that the map is finite. Let <img src='http://s0.wp.com/latex.php?latex=f&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='f' title='f' class='latex' /> be a face of the map; (TM4) implies that there are a finite number of darts <img src='http://s0.wp.com/latex.php?latex=%5Calpha&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;alpha' title='&#92;alpha' class='latex' /> for which <img src='http://s0.wp.com/latex.php?latex=f%3Dface%28%5Calpha%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='f=face(&#92;alpha)' title='f=face(&#92;alpha)' class='latex' />. We list these darts:<img src='http://s0.wp.com/latex.php?latex=%5Calpha_1%3D%28v_1%2C+e_1%29%2C+%5Cdots%2C+%5Calpha_n%3D%28v_n%2C+e_n%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;alpha_1=(v_1, e_1), &#92;dots, &#92;alpha_n=(v_n, e_n)' title='&#92;alpha_1=(v_1, e_1), &#92;dots, &#92;alpha_n=(v_n, e_n)' class='latex' />. Now (TM3) implies that <img src='http://s0.wp.com/latex.php?latex=f&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='f' title='f' class='latex' /> is homeomorphic to an open disc; it is clearly sufficient to show that <img src='http://s0.wp.com/latex.php?latex=f%5Ccup+e_1+%5Ccup+%5Ccdots+%5Ccup+e_n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='f&#92;cup e_1 &#92;cup &#92;cdots &#92;cup e_n' title='f&#92;cup e_1 &#92;cup &#92;cdots &#92;cup e_n' class='latex' /> is homeomorphic to a closed disc (since then the surface <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BS%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{S}' title='&#92;mathcal{S}' class='latex' /> is homeomorphic to a finite union of compact surfaces and so is itself compact).</p>
<p>Now why is <img src='http://s0.wp.com/latex.php?latex=f%5Ccup+e_1+%5Ccup+%5Ccdots+%5Ccup+e_n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='f&#92;cup e_1 &#92;cup &#92;cdots &#92;cup e_n' title='f&#92;cup e_1 &#92;cup &#92;cdots &#92;cup e_n' class='latex' /> is homeomorphic to a closed disc? First of all, there is the possibility that <img src='http://s0.wp.com/latex.php?latex=n%3D1&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n=1' title='n=1' class='latex' /> and the edge <img src='http://s0.wp.com/latex.php?latex=e_1&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e_1' title='e_1' class='latex' /> is a loop. In this case the result is clear. Suppose this is not the case &#8211; then all edges are segments or free-edges. With a little thought it should be clear that the edges <img src='http://s0.wp.com/latex.php?latex=e_i&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e_i' title='e_i' class='latex' /> which are segments form a closed loop; the free-edges can be thought of as spikes coming off this closed loop, &#8220;poking into&#8221; the face <img src='http://s0.wp.com/latex.php?latex=f&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='f' title='f' class='latex' />. This union of segments clearly forms the boundary of <img src='http://s0.wp.com/latex.php?latex=f%5Ccup+e_1+%5Ccup+%5Ccdots+%5Ccup+e_n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='f&#92;cup e_1 &#92;cup &#92;cdots &#92;cup e_n' title='f&#92;cup e_1 &#92;cup &#92;cdots &#92;cup e_n' class='latex' />; the required homeomorphism can then be obtained by &#8220;pinching&#8221; the face round each of the free-edges, and extending it smoothly to the union of segments. Hopefully the principle is clear.</p>
<p style="text-align:right;"><strong>QED</strong></p>
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		<title>What is a regular map?</title>
		<link>http://regularmaps.wordpress.com/2011/05/10/what-is-a-regular-map/</link>
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		<pubDate>Tue, 10 May 2011 10:10:05 +0000</pubDate>
		<dc:creator>Nick Gill</dc:creator>
				<category><![CDATA[algebraic map]]></category>
		<category><![CDATA[definitions]]></category>
		<category><![CDATA[topological map]]></category>

		<guid isPermaLink="false">http://regularmaps.wordpress.com/?p=17</guid>
		<description><![CDATA[In this post we use the seminal paper of Jones and Singerman to define a regular map; in particular we will give a number of equivalent definitions of a map and then we will focus our attention on the regular maps at the end. It is important to note that, for the purposes of this [&#8230;]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=regularmaps.wordpress.com&#038;blog=22821215&#038;post=17&#038;subd=regularmaps&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p>In this post we use <a href="http://www.ams.org/mathscinet-getitem?mr=505721">the seminal paper of Jones and Singerman</a> to define a regular map; in particular we will give a number of equivalent definitions of a <em>map</em> and then we will focus our attention on the regular maps at the end. It is important to note that, for the purposes of this post, we restrict our attention to <em>orientable surfaces; i</em>n a later post we will extend the definition to non-orientable surfaces.</p>
<p>(Note: after you&#8217;ve read this post I heartily recommend you go and read the original Jones-Singerman paper  &#8211; it&#8217;s a cracking bit of mathematical exposition.)</p>
<h2>The naive idea</h2>
<p>In what follows think of a map as being a graph <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BG%7D%3D%28%5Cmathcal%7BV%7D%2C+%5Cmathcal%7BE%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{G}=(&#92;mathcal{V}, &#92;mathcal{E})' title='&#92;mathcal{G}=(&#92;mathcal{V}, &#92;mathcal{E})' class='latex' /> drawn on some surface <img src='http://s0.wp.com/latex.php?latex=S&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='S' title='S' class='latex' />. For instance a triangulation of the plane will do, or a couple of loops on a torus, with vertices at the intersections. The key point is that edges are <strong>not</strong> allowed to cross; this implies, for instance, that when the surface <img src='http://s0.wp.com/latex.php?latex=S&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='S' title='S' class='latex' /> is the plane, a map is the same thing as a <em>planar graph</em>.</p>
<h2>Topological maps</h2>
<p>Let&#8217;s translate the naive idea into the topological setting. Let <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BE%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{E}' title='&#92;mathcal{E}' class='latex' /> be a collection of topological spaces each of which is homeomorphic to <img src='http://s0.wp.com/latex.php?latex=%5B0%2C1%5D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='[0,1]' title='[0,1]' class='latex' /> or <img src='http://s0.wp.com/latex.php?latex=S%5E1&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='S^1' title='S^1' class='latex' /> &#8211; these are the edges. Let <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BV%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{V}' title='&#92;mathcal{V}' class='latex' /> be a subset of <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BG%7D+%3D+%5Ccup_%7Be%5Cin%5Cmathcal%7BE%7D%7D+e&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{G} = &#92;cup_{e&#92;in&#92;mathcal{E}} e' title='&#92;mathcal{G} = &#92;cup_{e&#92;in&#92;mathcal{E}} e' class='latex' /> &#8211; these are the vertices. For <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BG%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{G}' title='&#92;mathcal{G}' class='latex' /> to be map we need some conditions on <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BE%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{E}' title='&#92;mathcal{E}' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BV%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{V}' title='&#92;mathcal{V}' class='latex' /> as follows. For a given <img src='http://s0.wp.com/latex.php?latex=e%5Cin%5Cmathcal%7BE%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e&#92;in&#92;mathcal{E}' title='e&#92;in&#92;mathcal{E}' class='latex' /> define <img src='http://s0.wp.com/latex.php?latex=%5CDelta+e+%3D+e%5Ccap+%5Cmathcal%7BV%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Delta e = e&#92;cap &#92;mathcal{V}' title='&#92;Delta e = e&#92;cap &#92;mathcal{V}' class='latex' />, and <img src='http://s0.wp.com/latex.php?latex=e%5E%5C%23+%3D+e%5Csetminus%5CDelta+e&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e^&#92;# = e&#92;setminus&#92;Delta e' title='e^&#92;# = e&#92;setminus&#92;Delta e' class='latex' />. Then we require that</p>
<ul>
<li>(AG1) if <img src='http://s0.wp.com/latex.php?latex=e&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e' title='e' class='latex' /> is homeomorphic to <img src='http://s0.wp.com/latex.php?latex=S%5E1&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='S^1' title='S^1' class='latex' /> then <img src='http://s0.wp.com/latex.php?latex=%7C%5CDelta+e%7C+%3D+1&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='|&#92;Delta e| = 1' title='|&#92;Delta e| = 1' class='latex' /> (and <img src='http://s0.wp.com/latex.php?latex=e&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e' title='e' class='latex' /> is a<em> loop</em>);</li>
<li>(AG1&#8242;) if <img src='http://s0.wp.com/latex.php?latex=e&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e' title='e' class='latex' /> is homeomorphic to <img src='http://s0.wp.com/latex.php?latex=%5B0%2C1%5D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='[0,1]' title='[0,1]' class='latex' /> then <img src='http://s0.wp.com/latex.php?latex=%5CDelta+e&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Delta e' title='&#92;Delta e' class='latex' /> contains either one or both of the end-points of <img src='http://s0.wp.com/latex.php?latex=e&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e' title='e' class='latex' /> (and <img src='http://s0.wp.com/latex.php?latex=e&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e' title='e' class='latex' /> is a <em>free edge</em> or a <em>segment</em> respectively);</li>
<li>(AG2) for all distinct <img src='http://s0.wp.com/latex.php?latex=e_1%2C+e_2%5Cin%5Cmathcal%7BE%7D%2C+e_1%5E%7B%5C%23%7D+%5Ccap+e_2%5E%7B%5C%23%7D%3D%5Cemptyset&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e_1, e_2&#92;in&#92;mathcal{E}, e_1^{&#92;#} &#92;cap e_2^{&#92;#}=&#92;emptyset' title='e_1, e_2&#92;in&#92;mathcal{E}, e_1^{&#92;#} &#92;cap e_2^{&#92;#}=&#92;emptyset' class='latex' />;</li>
<li>(AG3) for any <img src='http://s0.wp.com/latex.php?latex=v%5Cin+%5Cmathcal%7BV%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='v&#92;in &#92;mathcal{V}' title='v&#92;in &#92;mathcal{V}' class='latex' />, at most finitely many <img src='http://s0.wp.com/latex.php?latex=e%5Cin%5Cmathcal%7BE%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e&#92;in&#92;mathcal{E}' title='e&#92;in&#92;mathcal{E}' class='latex' /> satisfy <img src='http://s0.wp.com/latex.php?latex=v%5Cin%5CDelta+e&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='v&#92;in&#92;Delta e' title='v&#92;in&#92;Delta e' class='latex' />.</li>
</ul>
<p>A pair <img src='http://s0.wp.com/latex.php?latex=%28%5Cmathcal%7BG%7D%2C+%5Cmathcal%7BV%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(&#92;mathcal{G}, &#92;mathcal{V})' title='(&#92;mathcal{G}, &#92;mathcal{V})' class='latex' /> satisfying these axioms is known as an <em>allowed graph</em>. We need some more axioms before we can declare that the pair is a <em>topological map</em>.</p>
<p>Before we give the extra axioms, a little note: when we come to consider regular maps, the notions of free edge and loop become entirely uninteresting (as soon as we have a free edge or a loop, any connected regular map must have at most one vertex) however for the categorical equivalences that we wish to consider for general maps, free edges are a required concept.</p>
<p>Now for the extra axioms. Suppose that <img src='http://s0.wp.com/latex.php?latex=%28%5Cmathcal%7BG%7D%2C+%5Cmathcal%7BV%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(&#92;mathcal{G}, &#92;mathcal{V})' title='(&#92;mathcal{G}, &#92;mathcal{V})' class='latex' /> is an allowed graph, that <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BS%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{S}' title='&#92;mathcal{S}' class='latex' /> is a connected, oriented surface without boundary, and there is a homeomorphism of <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BG%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{G}' title='&#92;mathcal{G}' class='latex' /> with a subspace of <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BS%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{S}' title='&#92;mathcal{S}' class='latex' />. We identify <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BG%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{G}' title='&#92;mathcal{G}' class='latex' /> with its image in <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BS%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{S}' title='&#92;mathcal{S}' class='latex' /> and make a couple of definitions:</p>
<ul>
<li>define <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{F}' title='&#92;mathcal{F}' class='latex' /> to be the set of connected components of <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BG%7D%5Csetminus%5Cmathcal%7BS%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{G}&#92;setminus&#92;mathcal{S}' title='&#92;mathcal{G}&#92;setminus&#92;mathcal{S}' class='latex' /> (these are the <em>faces</em> of the map)</li>
<li>we define the <em>valency</em> of a point <img src='http://s0.wp.com/latex.php?latex=p%5Cin+%5Cmathcal%7BV%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p&#92;in &#92;mathcal{V}' title='p&#92;in &#92;mathcal{V}' class='latex' /> to equal<br />
<img src='http://s0.wp.com/latex.php?latex=2%7C%5C%7Be%5Cin%5Cmathcal%7BE%7D+%7C+e+%5Ctextrm%7B+is+a+loop+and+%7Dp%5Cin%5CDelta+e%5C%7D%7C%2B%7C%5C%7Be%5Cin%5Cmathcal%7BE%7D+%7C+e+%5Ctextrm%7B+is+a+segment+and+%7Dp%5Cin%5CDelta+e%5C%7D%7C%3B&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='2|&#92;{e&#92;in&#92;mathcal{E} | e &#92;textrm{ is a loop and }p&#92;in&#92;Delta e&#92;}|+|&#92;{e&#92;in&#92;mathcal{E} | e &#92;textrm{ is a segment and }p&#92;in&#92;Delta e&#92;}|;' title='2|&#92;{e&#92;in&#92;mathcal{E} | e &#92;textrm{ is a loop and }p&#92;in&#92;Delta e&#92;}|+|&#92;{e&#92;in&#92;mathcal{E} | e &#92;textrm{ is a segment and }p&#92;in&#92;Delta e&#92;}|;' class='latex' /><br />
define the valency of a point <img src='http://s0.wp.com/latex.php?latex=p%5Cin%5Cmathcal%7BG%7D%5Csetminus%5Cmathcal%7BV%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p&#92;in&#92;mathcal{G}&#92;setminus&#92;mathcal{V}' title='p&#92;in&#92;mathcal{G}&#92;setminus&#92;mathcal{V}' class='latex' /> to equal <img src='http://s0.wp.com/latex.php?latex=1&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='1' title='1' class='latex' /> whenever <img src='http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p' title='p' class='latex' /> is the end-point of a free edge <img src='http://s0.wp.com/latex.php?latex=e&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e' title='e' class='latex' />, and to equal <img src='http://s0.wp.com/latex.php?latex=2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='2' title='2' class='latex' /> otherwise.</li>
</ul>
<p>We can now proceed to define three of our four extra axioms.</p>
<ul>
<li>(TM1) whenever <img src='http://s0.wp.com/latex.php?latex=p%5Cin%5Cmathcal%7BG%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p&#92;in&#92;mathcal{G}' title='p&#92;in&#92;mathcal{G}' class='latex' /> has valency <img src='http://s0.wp.com/latex.php?latex=k&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='k' title='k' class='latex' />, there is a neighbourhood <img src='http://s0.wp.com/latex.php?latex=N_p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='N_p' title='N_p' class='latex' /> of <img src='http://s0.wp.com/latex.php?latex=p&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='p' title='p' class='latex' /> in <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BS%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{S}' title='&#92;mathcal{S}' class='latex' /> and a homeomorphism <img src='http://s0.wp.com/latex.php?latex=%5Cphi_p%3A+N_p%5Cto+D+%3D+%5C%7Bz%5Cin%5Cmathbb%7BC%7D+%5C%2C+%5Cmid+%5C%2C+%7CZ%7C%3C1%5C%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;phi_p: N_p&#92;to D = &#92;{z&#92;in&#92;mathbb{C} &#92;, &#92;mid &#92;, |Z|&lt;1&#92;}' title='&#92;phi_p: N_p&#92;to D = &#92;{z&#92;in&#92;mathbb{C} &#92;, &#92;mid &#92;, |Z|&lt;1&#92;}' class='latex' /> such that <img src='http://s0.wp.com/latex.php?latex=%5Cphi_p%28p%29%3D0&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;phi_p(p)=0' title='&#92;phi_p(p)=0' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=%5Cphi_p%28N_p%5Ccap+%5Cmathcal%7BG%7D%29%3D%5C%7Bz%5Cin%5Cmathbb%7BC%7D+%5C%2C+%5Cmid+%5C%2C+z%5Ek%5Cin%5B0%2C1%29%5Csubseteq+%5Cmathbb%7BR%7D%5C%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;phi_p(N_p&#92;cap &#92;mathcal{G})=&#92;{z&#92;in&#92;mathbb{C} &#92;, &#92;mid &#92;, z^k&#92;in[0,1)&#92;subseteq &#92;mathbb{R}&#92;}' title='&#92;phi_p(N_p&#92;cap &#92;mathcal{G})=&#92;{z&#92;in&#92;mathbb{C} &#92;, &#92;mid &#92;, z^k&#92;in[0,1)&#92;subseteq &#92;mathbb{R}&#92;}' class='latex' />;</li>
<li>(TM2) <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BG%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{G}' title='&#92;mathcal{G}' class='latex' /> is connected (this isn&#8217;t necessary, but it makes life a lot easier and there is effectively no loss of generality);</li>
<li>(TM3) each face <img src='http://s0.wp.com/latex.php?latex=f&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='f' title='f' class='latex' /> is homeomorphic to the open disc;</li>
</ul>
<p>Two more definitions:</p>
<ul>
<li>We need the concept of a <em>dart</em> (sometimes called a <em>half-edge</em>). I&#8217;m only going to define these for allowed graphs satisfying TM1 to TM3 (as opposed to for allowed graphs), so I can give a more naive definition than that of Jones and Singerman. For me a <em>dart</em> is an edge-vertex incident pair. Specifically the set of darts is:  <img src='http://s0.wp.com/latex.php?latex=%5COmega%3D%5C%7B%28e%2Cv%29%5Cin+%28%5Cmathcal%7BE%7D%2C%5Cmathcal%7BV%7D%29+%5C%2C+%5Cmid+%5C%2C+v%5Cin%5CDelta+e%5C%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Omega=&#92;{(e,v)&#92;in (&#92;mathcal{E},&#92;mathcal{V}) &#92;, &#92;mid &#92;, v&#92;in&#92;Delta e&#92;}' title='&#92;Omega=&#92;{(e,v)&#92;in (&#92;mathcal{E},&#92;mathcal{V}) &#92;, &#92;mid &#92;, v&#92;in&#92;Delta e&#92;}' class='latex' />. Think of a dart <img src='http://s0.wp.com/latex.php?latex=%28e%2Cv%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(e,v)' title='(e,v)' class='latex' /> as being an arrow running along the edge <img src='http://s0.wp.com/latex.php?latex=e&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e' title='e' class='latex' /> with its head at <img src='http://s0.wp.com/latex.php?latex=v&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='v' title='v' class='latex' />.</li>
<li><em></em>For <img src='http://s0.wp.com/latex.php?latex=v%5Cin%5Cmathcal%7BV%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='v&#92;in&#92;mathcal{V}' title='v&#92;in&#92;mathcal{V}' class='latex' /> let <img src='http://s0.wp.com/latex.php?latex=N_v&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='N_v' title='N_v' class='latex' /> be the neighbourhood mentioned in TM1. For a dart <img src='http://s0.wp.com/latex.php?latex=%5Calpha%3D%28e%2Cv%29%5Cin%5COmega&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;alpha=(e,v)&#92;in&#92;Omega' title='&#92;alpha=(e,v)&#92;in&#92;Omega' class='latex' /> consider a circular arc in <img src='http://s0.wp.com/latex.php?latex=N_v&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='N_v' title='N_v' class='latex' /> which starts on <img src='http://s0.wp.com/latex.php?latex=e&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e' title='e' class='latex' />, follows orientation, and ends on the next edge incident with <img src='http://s0.wp.com/latex.php?latex=v&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='v' title='v' class='latex' />. This arc lies in a unique face of <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BG%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{G}' title='&#92;mathcal{G}' class='latex' />; this face is called <img src='http://s0.wp.com/latex.php?latex=face%28%5Calpha%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='face(&#92;alpha)' title='face(&#92;alpha)' class='latex' />. Now for <img src='http://s0.wp.com/latex.php?latex=f%5Cin%5Cmathcal%7BF%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='f&#92;in&#92;mathcal{F}' title='f&#92;in&#92;mathcal{F}' class='latex' /> define the <em>valency</em> of <img src='http://s0.wp.com/latex.php?latex=f&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='f' title='f' class='latex' /> to be <img src='http://s0.wp.com/latex.php?latex=val%28f%29%3D%5C%7B%5Calpha%5Cin%5COmega+%5C%2C+%5Cmid+%5C%2C+f%3Dface%28%5Calpha%29%5C%7D.&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='val(f)=&#92;{&#92;alpha&#92;in&#92;Omega &#92;, &#92;mid &#92;, f=face(&#92;alpha)&#92;}.' title='val(f)=&#92;{&#92;alpha&#92;in&#92;Omega &#92;, &#92;mid &#92;, f=face(&#92;alpha)&#92;}.' class='latex' /></li>
</ul>
<p>Finally, our last axiom.</p>
<ul>
<li>(TM4) For all <img src='http://s0.wp.com/latex.php?latex=f%5Cin%5Cmathcal%7BF%7D%2C+1%5Cleq+val%28f%29%3C%5Cinfty&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='f&#92;in&#92;mathcal{F}, 1&#92;leq val(f)&lt;&#92;infty' title='f&#92;in&#92;mathcal{F}, 1&#92;leq val(f)&lt;&#92;infty' class='latex' />.</li>
</ul>
<p>A triple <img src='http://s0.wp.com/latex.php?latex=%28%5Cmathcal%7BG%7D%2C+%5Cmathcal%7BV%7D%2C+%5Cmathcal%7BS%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(&#92;mathcal{G}, &#92;mathcal{V}, &#92;mathcal{S})' title='(&#92;mathcal{G}, &#92;mathcal{V}, &#92;mathcal{S})' class='latex' /> satisfying AG1 to AG3 and TM1 to TM4 is called a <em>topological map</em>. Define the <em>type</em> of the map to be <img src='http://s0.wp.com/latex.php?latex=%28m%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(m,n)' title='(m,n)' class='latex' /> where <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> is the l.c.m of <img src='http://s0.wp.com/latex.php?latex=val%28v%29+%28+v%5Cin%5Cmathcal%7BV%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='val(v) ( v&#92;in&#92;mathcal{V})' title='val(v) ( v&#92;in&#92;mathcal{V})' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> is the l.c.m of <img src='http://s0.wp.com/latex.php?latex=val%28f%29+%28+v%5Cin%5Cmathcal%7BF%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='val(f) ( v&#92;in&#92;mathcal{F})' title='val(f) ( v&#92;in&#92;mathcal{F})' class='latex' />; we allow <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> and/or <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> to be infinite when the l.c.m. does not exist. The map is said to have <em>finite type</em> if <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> are finite; the map is said to be <em>finite</em> if <img src='http://s0.wp.com/latex.php?latex=%5COmega&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Omega' title='&#92;Omega' class='latex' /> is finite (J&amp;S state that a map is finite exactly when <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BS%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{S}' title='&#92;mathcal{S}' class='latex' /> is compact; I&#8217;d like a proof of that).</p>
<p>Some examples: regular tesselations of the plane <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BS%7D%3D%5Cmathbb%7BR%7D%5E2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{S}=&#92;mathbb{R}^2' title='&#92;mathcal{S}=&#92;mathbb{R}^2' class='latex' /> by triangles, squares, and hexagons give infinite maps of type <img src='http://s0.wp.com/latex.php?latex=%286%2C3%29%2C+%284%2C4%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(6,3), (4,4)' title='(6,3), (4,4)' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=%283%2C6%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(3,6)' title='(3,6)' class='latex' /> respectively. Platonic solids give finite maps on the sphere. And so on and so on.</p>
<p>We define morphisms of maps <img src='http://s0.wp.com/latex.php?latex=%28%5Cmathcal%7BG%7D_i%2C+%5Cmathcal%7BV%7D_i%2C+%5Cmathcal%7BS%7D_i%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(&#92;mathcal{G}_i, &#92;mathcal{V}_i, &#92;mathcal{S}_i)' title='(&#92;mathcal{G}_i, &#92;mathcal{V}_i, &#92;mathcal{S}_i)' class='latex' />  just as one would expect. Note, in particular, that all branch-points of the associated covering <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BS%7D_1%5Cto%5Cmathcal%7BS%7D_2&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{S}_1&#92;to&#92;mathcal{S}_2' title='&#92;mathcal{S}_1&#92;to&#92;mathcal{S}_2' class='latex' />  have finite order. We then have a category <strong>TM</strong> of topological maps; define <strong>TM(m,n)</strong> to be the subcategory of all maps of type <img src='http://s0.wp.com/latex.php?latex=%28r%2Cs%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(r,s)' title='(r,s)' class='latex' /> where <img src='http://s0.wp.com/latex.php?latex=r%5Cmid+m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='r&#92;mid m' title='r&#92;mid m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=s%5Cmid+n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='s&#92;mid n' title='s&#92;mid n' class='latex' />.</p>
<h2>Algebraic maps</h2>
<p>We can define algebraic maps much more easily; they are a quadruple <img src='http://s0.wp.com/latex.php?latex=%28G%2C%5COmega%2C+x%2Cy%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(G,&#92;Omega, x,y)' title='(G,&#92;Omega, x,y)' class='latex' /> where <img src='http://s0.wp.com/latex.php?latex=%5COmega&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Omega' title='&#92;Omega' class='latex' /> is a set and <img src='http://s0.wp.com/latex.php?latex=x%2Cy%5Cin+G+%3CSym%28%5COmega%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='x,y&#92;in G &lt;Sym(&#92;Omega)' title='x,y&#92;in G &lt;Sym(&#92;Omega)' class='latex' /> such that</p>
<ul>
<li>(AG1) <img src='http://s0.wp.com/latex.php?latex=x%5E2%3D1&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='x^2=1' title='x^2=1' class='latex' />;</li>
<li>(AG2) <img src='http://s0.wp.com/latex.php?latex=G%3D%5Clangle+x%2C+y%5Crangle&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G=&#92;langle x, y&#92;rangle' title='G=&#92;langle x, y&#92;rangle' class='latex' /> is transitive on <img src='http://s0.wp.com/latex.php?latex=%5COmega&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Omega' title='&#92;Omega' class='latex' />;</li>
</ul>
<p>We define the <em>type</em> of an algebraic map <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BA%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{A}' title='&#92;mathcal{A}' class='latex' /> to be<img src='http://s0.wp.com/latex.php?latex=%28m%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(m,n)' title='(m,n)' class='latex' /> where <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> is the order of <img src='http://s0.wp.com/latex.php?latex=y&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='y' title='y' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> is the order of <img src='http://s0.wp.com/latex.php?latex=z%3Dy%5E%7B-1%7Dx&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='z=y^{-1}x' title='z=y^{-1}x' class='latex' />. Similarly to before the map is said to have <em>finite type</em> if <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> are finite; the map is said to be <em>finite</em> if <img src='http://s0.wp.com/latex.php?latex=%5COmega&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Omega' title='&#92;Omega' class='latex' /> is finite.</p>
<p>We define morphisms in the obvious way &#8211; they are permutation group morphisms mapping the distinguished elements <img src='http://s0.wp.com/latex.php?latex=x&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='x' title='x' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=y&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='y' title='y' class='latex' /> to the corresponding distinguished elements. Thus we have a category <strong>AM</strong> of all algebraic maps and, just as before, a subcategory <strong>AM(m,n) </strong>to be the subcategory of all maps of type <img src='http://s0.wp.com/latex.php?latex=%28r%2Cs%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(r,s)' title='(r,s)' class='latex' /> where <img src='http://s0.wp.com/latex.php?latex=r%5Cmid+m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='r&#92;mid m' title='r&#92;mid m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=s%5Cmid+n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='s&#92;mid n' title='s&#92;mid n' class='latex' />.</p>
<p>Now, a trivial observation: the group <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' /> has a presentation of the following form: <img src='http://s0.wp.com/latex.php?latex=%5Clangle+x%2C+y%2C+z+%5C%2C+%5Cmid+%5C%2C+x%5E2%3Dy%5Em%3Dz%5Em%3Dxyz%3D%5Ccdots+%3D+1+%5Crangle&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;langle x, y, z &#92;, &#92;mid &#92;, x^2=y^m=z^m=xyz=&#92;cdots = 1 &#92;rangle' title='&#92;langle x, y, z &#92;, &#92;mid &#92;, x^2=y^m=z^m=xyz=&#92;cdots = 1 &#92;rangle' class='latex' />. Let us define the following &#8220;universal group&#8221;: <img src='http://s0.wp.com/latex.php?latex=%5CGamma%3D%5CGamma%28m%2Cn%29%3D+%5Clangle+x%2C+y%2C+z+%5C%2C+%5Cmid+%5C%2C+x%5E2%3Dy%5Em%3Dz%5Em%3Dxyz%3D+1+%5Crangle&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma=&#92;Gamma(m,n)= &#92;langle x, y, z &#92;, &#92;mid &#92;, x^2=y^m=z^m=xyz= 1 &#92;rangle' title='&#92;Gamma=&#92;Gamma(m,n)= &#92;langle x, y, z &#92;, &#92;mid &#92;, x^2=y^m=z^m=xyz= 1 &#92;rangle' class='latex' />; then <img src='http://s0.wp.com/latex.php?latex=G%3D%5CGamma%2F+N&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G=&#92;Gamma/ N' title='G=&#92;Gamma/ N' class='latex' /> for some normal subgroup <img src='http://s0.wp.com/latex.php?latex=N%5Cunlhd+%5CGamma&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='N&#92;unlhd &#92;Gamma' title='N&#92;unlhd &#92;Gamma' class='latex' />.</p>
<p>In fact, we can define the concept of a <em>universal algebraic map of type <img src='http://s0.wp.com/latex.php?latex=%28m%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(m,n)' title='(m,n)' class='latex' /></em>: it is the algebraic map <img src='http://s0.wp.com/latex.php?latex=%28%5CGamma%2C+%5CGamma%2C+x%2C+y%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(&#92;Gamma, &#92;Gamma, x, y)' title='(&#92;Gamma, &#92;Gamma, x, y)' class='latex' /> &#8211; here the set <img src='http://s0.wp.com/latex.php?latex=%5COmega%3D%5CGamma&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Omega=&#92;Gamma' title='&#92;Omega=&#92;Gamma' class='latex' /> where we simply ignore the group operation. Note that we allow one or both of <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> to be equal to <img src='http://s0.wp.com/latex.php?latex=%5Cinfty&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;infty' title='&#92;infty' class='latex' />. Now one can see immediately that any algebraic map in <strong>AM(m,n)</strong> has the following form: <img src='http://s0.wp.com/latex.php?latex=%28%5CGamma%2F+M%5E%2A%2C+%5CGamma%2F+M%2C+xM%5E%2A%2C+yM%5E%2A%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(&#92;Gamma/ M^*, &#92;Gamma/ M, xM^*, yM^*)' title='(&#92;Gamma/ M^*, &#92;Gamma/ M, xM^*, yM^*)' class='latex' />. We must clarify our notation: here <img src='http://s0.wp.com/latex.php?latex=M&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='M' title='M' class='latex' /> is any subgroup of <img src='http://s0.wp.com/latex.php?latex=%5CGamma&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma' title='&#92;Gamma' class='latex' />, and <img src='http://s0.wp.com/latex.php?latex=M%5E%2A&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='M^*' title='M^*' class='latex' /> is the <em>core</em> of <img src='http://s0.wp.com/latex.php?latex=M&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='M' title='M' class='latex' />; that is, it is the intersection of all conjugates of <img src='http://s0.wp.com/latex.php?latex=M&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='M' title='M' class='latex' />.</p>
<p>A consequence of the preceding paragraph is that every algebraic map in <strong>AM(m,n)</strong> is prescribed by (the conjugacy class of) the subgroup <img src='http://s0.wp.com/latex.php?latex=M&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='M' title='M' class='latex' />; we call <img src='http://s0.wp.com/latex.php?latex=M&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='M' title='M' class='latex' /> the <em>map subgroup</em>; observe that <img src='http://s0.wp.com/latex.php?latex=M%2FM%5E%2A+%3C+G%3D%5CGamma%2FM%5E%2A&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='M/M^* &lt; G=&#92;Gamma/M^*' title='M/M^* &lt; G=&#92;Gamma/M^*' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=M&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='M' title='M' class='latex' /> acts as a stabilizer in the action on <img src='http://s0.wp.com/latex.php?latex=%5COmega&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Omega' title='&#92;Omega' class='latex' />.</p>
<h2>Connecting topological maps and algebraic maps</h2>
<p>It turns out that the category <strong>TM(m,n)</strong> and the category <strong>AM(m,n)</strong> are equivalent. For now we will show how, given an element of <strong>TM(m,n)</strong>, one can construct an element of <strong>AM(m,n)</strong>.</p>
<p>Suppose, then, that we have a topological map <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%7D%3D%28%5Cmathcal%7BG%7D%2C+%5Cmathcal%7BV%7D%2C+%5Cmathcal%7BS%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M}=(&#92;mathcal{G}, &#92;mathcal{V}, &#92;mathcal{S})' title='&#92;mathcal{M}=(&#92;mathcal{G}, &#92;mathcal{V}, &#92;mathcal{S})' class='latex' />. We will define our algebraic map in terms of a permutation group acting on <img src='http://s0.wp.com/latex.php?latex=%5COmega&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Omega' title='&#92;Omega' class='latex' />, the set of darts.</p>
<p>Define the element <img src='http://s0.wp.com/latex.php?latex=x&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='x' title='x' class='latex' /> as the element that maps a dart <img src='http://s0.wp.com/latex.php?latex=%28e%2Cv%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(e,v)' title='(e,v)' class='latex' /> to <img src='http://s0.wp.com/latex.php?latex=%28e%2Cv%27%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(e,v&#039;)' title='(e,v&#039;)' class='latex' /> where, if <img src='http://s0.wp.com/latex.php?latex=e&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e' title='e' class='latex' /> is a segment or a loop, then <img src='http://s0.wp.com/latex.php?latex=v%27%5Cneq+v&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='v&#039;&#92;neq v' title='v&#039;&#92;neq v' class='latex' /> while, if <img src='http://s0.wp.com/latex.php?latex=e&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e' title='e' class='latex' /> is a free edge, then <img src='http://s0.wp.com/latex.php?latex=v%27%3Dv&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='v&#039;=v' title='v&#039;=v' class='latex' />. (We think of <img src='http://s0.wp.com/latex.php?latex=x&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='x' title='x' class='latex' /> as the element which maps each dart to its &#8220;opposite&#8221;.) Clearly <img src='http://s0.wp.com/latex.php?latex=x%5E2%3D1&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='x^2=1' title='x^2=1' class='latex' />.</p>
<p>Now the  the element <img src='http://s0.wp.com/latex.php?latex=y&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='y' title='y' class='latex' /> is the element that maps a dart <img src='http://s0.wp.com/latex.php?latex=%28e%2Cv%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(e,v)' title='(e,v)' class='latex' /> to <img src='http://s0.wp.com/latex.php?latex=%28e%27%2Cv%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(e&#039;,v)' title='(e&#039;,v)' class='latex' /> where <img src='http://s0.wp.com/latex.php?latex=e%27&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='e&#039;' title='e&#039;' class='latex' /> is the &#8220;next&#8221; edge incident with <img src='http://s0.wp.com/latex.php?latex=v&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='v' title='v' class='latex' /> as one follows a circular path around the vertex <img src='http://s0.wp.com/latex.php?latex=v&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='v' title='v' class='latex' /> following orientation. Clearly <img src='http://s0.wp.com/latex.php?latex=y&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='y' title='y' class='latex' /> has order <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> where <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> is the l.c.m. of <img src='http://s0.wp.com/latex.php?latex=val%28v%29+%28+v%5Cin%5Cmathcal%7BV%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='val(v) ( v&#92;in&#92;mathcal{V})' title='val(v) ( v&#92;in&#92;mathcal{V})' class='latex' /> (as required).</p>
<p>Now define <img src='http://s0.wp.com/latex.php?latex=z%3Dy%5E%7B-1%7Dx&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='z=y^{-1}x' title='z=y^{-1}x' class='latex' />; with a little thought (and some diagram drawing) it is not too hard to work out that the action of <img src='http://s0.wp.com/latex.php?latex=z&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='z' title='z' class='latex' /> is to fix the faces, while mapping a dart onto the &#8220;next&#8221; dart as one proceeds round the face following orientation. One sees immediately that the order of <img src='http://s0.wp.com/latex.php?latex=z&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='z' title='z' class='latex' /> is  <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' />, the l.c.m of <img src='http://s0.wp.com/latex.php?latex=val%28f%29+%28+v%5Cin%5Cmathcal%7BF%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='val(f) ( v&#92;in&#92;mathcal{F})' title='val(f) ( v&#92;in&#92;mathcal{F})' class='latex' /> (as required).</p>
<p>We have constructed our algebraic map, as promised; we will refer to it from here on as <img src='http://s0.wp.com/latex.php?latex=Alg%28%5Cmathcal%7BM%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='Alg(&#92;mathcal{M})' title='Alg(&#92;mathcal{M})' class='latex' />. One thing should be made clear: the group that we have described is most certainly <strong>not</strong> an automorphism group for the underlying topological map since the given dart permutations cannot, in general, be chosen to act as homeomorphisms of the underlying surface.</p>
<h2>Riemann maps</h2>
<p>Consider the subcategory <strong>RM(m,n)</strong> of <strong>TM(m,n)</strong> consisting of all elements for which the underlying surface is a Riemann surface, for which the edges of the graph are all geodesics in the corresponding metric, and where the angle between edges at a given vertex is constant. It is a surprising and hugely important result that, in fact, <strong>RM(m,n)</strong> and <strong>TM(m,n)</strong> are equivalent. In other words, in considering a topological map we are allowed to assume this extra structure.</p>
<p>The proof can be found in J&amp;S; I&#8217;ll give a brief outline here, but won&#8217;t go into details (maybe in a future post&#8230;) Note, first, that in the previous section we showed that <strong>TM(m,n)</strong> embeds into <strong>AM(m,n)</strong>. We&#8217;ve noted (it is a triviality) that <strong>RM(m,n)</strong> embeds into <strong>TM(m,n)</strong>. To prove that <strong>RM(m,n)</strong> and <strong>TM(m,n)</strong> are equivalent, then, it is sufficent to prove that <strong>AM(m,n)</strong> embeds into <strong>RM(m,n)</strong>.</p>
<p>To do this we start with an element of <strong>AM(m,n)</strong>; observe first that the corresponding group is isomorphic to <img src='http://s0.wp.com/latex.php?latex=%5CGamma%28m%2Cn%29%2FN&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma(m,n)/N' title='&#92;Gamma(m,n)/N' class='latex' /> for some normal group <img src='http://s0.wp.com/latex.php?latex=N&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='N' title='N' class='latex' />. Now observe that <img src='http://s0.wp.com/latex.php?latex=%5CGamma%28m%2Cn%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma(m,n)' title='&#92;Gamma(m,n)' class='latex' /> preserves a tesselation of the hyperbolic plane (provide <img src='http://s0.wp.com/latex.php?latex=m&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='m' title='m' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=n&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='n' title='n' class='latex' /> are not too small, in which case we have a tesselation of the plane or the sphere); the quotient <img src='http://s0.wp.com/latex.php?latex=%5CGamma%28m%2Cn%29%2FN&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma(m,n)/N' title='&#92;Gamma(m,n)/N' class='latex' /> therefore, preserves a tesselation on a quotient space, i.e. a tesselation on a particular Riemann surface. This tesselation is precisely equivalent to a graph inscribed upon the Riemann surface; thus, given an element of <strong>AM(m,n)</strong> we can construct an element of <strong>RM(m,n)</strong> as required.</p>
<h2>Automorphism groups</h2>
<p>We were a little vague about morphisms earlier, so let us firm things up: an automorphism of a topological map (i.e. of an element of <strong>TM</strong>) is a homeomorphism of the surface <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BS%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{S}' title='&#92;mathcal{S}' class='latex' /> which restricts to a graph automorphism of <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BG%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{G}' title='&#92;mathcal{G}' class='latex' />. If we are assuming that our element in fact lies in <strong>RM</strong> (as we can), then we can assume that the action on the surface is by isometry with respect to the Riemannian metric. An automorphism of an algebraic map (i.e. of an element of <strong>AM</strong>) is just a permutation group automorphism which fixes the distinguished elements <img src='http://s0.wp.com/latex.php?latex=x&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='x' title='x' class='latex' /> and <img src='http://s0.wp.com/latex.php?latex=y&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='y' title='y' class='latex' />.</p>
<p>For <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M}' title='&#92;mathcal{M}' class='latex' /> in <strong>TM</strong>, write <img src='http://s0.wp.com/latex.php?latex=TAut%28%5Cmathcal%7BM%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='TAut(&#92;mathcal{M})' title='TAut(&#92;mathcal{M})' class='latex' /> for the automorphism group of <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M}' title='&#92;mathcal{M}' class='latex' /> and write <img src='http://s0.wp.com/latex.php?latex=Aut%28%5Cmathcal%7BM%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='Aut(&#92;mathcal{M})' title='Aut(&#92;mathcal{M})' class='latex' /> for the automorphism group of <img src='http://s0.wp.com/latex.php?latex=Alg%28%5Cmathcal%7BM%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='Alg(&#92;mathcal{M})' title='Alg(&#92;mathcal{M})' class='latex' />, the corresponding algebraic map. It is easy to see that <img src='http://s0.wp.com/latex.php?latex=Aut%28%5Cmathcal%7BM%7D%29+%5Ccong+TAut%28%5Cmathcal%7BM%7D%29%2FK&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='Aut(&#92;mathcal{M}) &#92;cong TAut(&#92;mathcal{M})/K' title='Aut(&#92;mathcal{M}) &#92;cong TAut(&#92;mathcal{M})/K' class='latex' /> where <img src='http://s0.wp.com/latex.php?latex=K&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='K' title='K' class='latex' /> is the set of all elements of <img src='http://s0.wp.com/latex.php?latex=TAut%28%5Cmathcal%7BM%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='TAut(&#92;mathcal{M})' title='TAut(&#92;mathcal{M})' class='latex' /> which fix every dart. Now the key result concerning automorphisms is the following (the proof of which takes a paragraph, so we leave it as an exercise):</p>
<p><span style="text-decoration:underline;">Prop.</span> 1 Let <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M}' title='&#92;mathcal{M}' class='latex' /> be a topological map, with <img src='http://s0.wp.com/latex.php?latex=Alg%28%5Cmathcal%7BM%7D%29%3D%28G%2C%5COmega%2C+x%2Cy%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='Alg(&#92;mathcal{M})=(G,&#92;Omega, x,y)' title='Alg(&#92;mathcal{M})=(G,&#92;Omega, x,y)' class='latex' />, or let <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%7D%3D%28G%2C%5COmega%2C+x%2Cy%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M}=(G,&#92;Omega, x,y)' title='&#92;mathcal{M}=(G,&#92;Omega, x,y)' class='latex' /> be an algebraic map. Then</p>
<ol>
<li><img src='http://s0.wp.com/latex.php?latex=Aut%28%5Cmathcal%7BM%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='Aut(&#92;mathcal{M})' title='Aut(&#92;mathcal{M})' class='latex' /> acts faithfully on <img src='http://s0.wp.com/latex.php?latex=%5COmega&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Omega' title='&#92;Omega' class='latex' /> as the centralizer of <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' /> in <img src='http://s0.wp.com/latex.php?latex=Sym%28%5COmega%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='Sym(&#92;Omega)' title='Sym(&#92;Omega)' class='latex' />;</li>
<li><img src='http://s0.wp.com/latex.php?latex=Aut%28%5Cmathcal%7BM%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='Aut(&#92;mathcal{M})' title='Aut(&#92;mathcal{M})' class='latex' /> acts semi-regularly on <img src='http://s0.wp.com/latex.php?latex=%5COmega&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Omega' title='&#92;Omega' class='latex' />, i.e. the stabilizer of every point of <img src='http://s0.wp.com/latex.php?latex=%5COmega&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Omega' title='&#92;Omega' class='latex' /> is trivial.</li>
</ol>
<p>In the case of algebraic maps, one can come at these things from a different angle; it turns out that for <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M}' title='&#92;mathcal{M}' class='latex' /> in <strong>AM</strong>(m,n), we have <img src='http://s0.wp.com/latex.php?latex=Aut%28%5Cmathcal%7BM%7D%29+%5Ccong+N_%5CGamma%28M%29%2FM&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='Aut(&#92;mathcal{M}) &#92;cong N_&#92;Gamma(M)/M' title='Aut(&#92;mathcal{M}) &#92;cong N_&#92;Gamma(M)/M' class='latex' /> where <img src='http://s0.wp.com/latex.php?latex=M&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='M' title='M' class='latex' /> is the map subgroup of <img src='http://s0.wp.com/latex.php?latex=%5CGamma&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma' title='&#92;Gamma' class='latex' />, the universal group.</p>
<h2>Regularity</h2>
<p>Call an algebraic map <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M}' title='&#92;mathcal{M}' class='latex' /> <em>regular</em> if <img src='http://s0.wp.com/latex.php?latex=Aut%28%5Cmathcal%7BM%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='Aut(&#92;mathcal{M})' title='Aut(&#92;mathcal{M})' class='latex' /> acts transitively on <img src='http://s0.wp.com/latex.php?latex=%5COmega&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Omega' title='&#92;Omega' class='latex' />. Now the following are equivalent:</p>
<ol>
<li><img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M}' title='&#92;mathcal{M}' class='latex' /> is regular;</li>
<li>the mapping subgroup <img src='http://s0.wp.com/latex.php?latex=M&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='M' title='M' class='latex' /> is normal in <img src='http://s0.wp.com/latex.php?latex=%5CGamma&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Gamma' title='&#92;Gamma' class='latex' />;</li>
<li><img src='http://s0.wp.com/latex.php?latex=%28G%2C%5COmega%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='(G,&#92;Omega)' title='(G,&#92;Omega)' class='latex' /> is a regular permutation group (i.e. <img src='http://s0.wp.com/latex.php?latex=G&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='G' title='G' class='latex' /> is transitive on <img src='http://s0.wp.com/latex.php?latex=%5COmega&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;Omega' title='&#92;Omega' class='latex' />, and every stabilizer is trivial).</li>
</ol>
<p>The first two equivalences are clear. The third follows from Prop. 1 and the group theory fact  that the centralizer of a regular subgroup of <img src='http://s0.wp.com/latex.php?latex=Sym%28%5COmega%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='Sym(&#92;Omega)' title='Sym(&#92;Omega)' class='latex' /> is semi-regular. (Indeed to prove Prop. 1 one uses a more general fact: namely that the centralizer of a transitive subgroup of <img src='http://s0.wp.com/latex.php?latex=Sym%28%5COmega%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='Sym(&#92;Omega)' title='Sym(&#92;Omega)' class='latex' /> is semi-regular.)</p>
<p>Now suppose that <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M}' title='&#92;mathcal{M}' class='latex' /> is a topological map. If <img src='http://s0.wp.com/latex.php?latex=Alg%28%5Cmathcal%7BM%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='Alg(&#92;mathcal{M})' title='Alg(&#92;mathcal{M})' class='latex' /> is regular, then the discussion of the previous section implies that <img src='http://s0.wp.com/latex.php?latex=Aut%28%5Cmathcal%7BM%7D%29&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='Aut(&#92;mathcal{M})' title='Aut(&#92;mathcal{M})' class='latex' /> acts regularly on the darts of <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M}' title='&#92;mathcal{M}' class='latex' /> and, in this case, we say that <img src='http://s0.wp.com/latex.php?latex=%5Cmathcal%7BM%7D&amp;bg=ffffff&amp;fg=333333&amp;s=0' alt='&#92;mathcal{M}' title='&#92;mathcal{M}' class='latex' /> is regular.</p>
<p>All that remains is to classify the regular maps (he says with a smile)&#8230; Once one has got a handle on the category <strong>RM</strong> it becomes clear that this is a question in hyperbolic geometry. But that will have to wait for another day.</p>
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		<title>Introduction</title>
		<link>http://regularmaps.wordpress.com/2011/05/05/hello-world/</link>
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		<pubDate>Thu, 05 May 2011 13:00:52 +0000</pubDate>
		<dc:creator>Nick Gill</dc:creator>
				<category><![CDATA[Blog admin]]></category>

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		<description><![CDATA[This blog is intended to document the progress we make in understanding the concept of a regular map. If we&#8217;re lucky, it might lead to a paper. In the short term, most of our posts will discuss results already in the literature; as time goes by, we may discuss possible avenues for new research. The [&#8230;]<img alt="" border="0" src="http://stats.wordpress.com/b.gif?host=regularmaps.wordpress.com&#038;blog=22821215&#038;post=1&#038;subd=regularmaps&#038;ref=&#038;feed=1" width="1" height="1" />]]></description>
				<content:encoded><![CDATA[<p>This blog is intended to document the progress we make in understanding the concept of a <em>regular map</em>. If we&#8217;re lucky, it might lead to a paper. In the short term, most of our posts will discuss results already in the literature; as time goes by, we may discuss possible avenues for new research.</p>
<p>The great thing about regular maps (and it&#8217;s one of the reasons why we decided to investigate them together, despite our disparate mathematical backgrounds) is that <em></em>one can approach them from a number of different avenues: via (for instance) algebraic topology, combinatorial and algebraic graph theory, hyperbolic geometry, surface groups and Riemann surfaces, or geometric group theory. None of us are experts in all of these areas so we may well intersperse posts on regular maps with posts discussing useful background concepts.</p>
<p>Anyone should feel free to comment on what we write; we&#8217;d be very glad if regular-map-experts were to visit this blog occasionally and tell us when we&#8217;re talking nonsense. If you would like to write a post on any subject relating to regular maps, then that would be splendid. You can email us as follows:</p>
<p>Our usernames: <em>n.gill; ian.short; r.brignall</em>;</p>
<p>Followed by: <em> [at] open [dot] ac [dot] uk.</em></p>
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