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<channel>
	<title>scl &amp;laquo; WordPress.com Tag Feed</title>
	<link>http://en.wordpress.com/tag/scl/</link>
	<description>Feed of posts on WordPress.com tagged "scl"</description>
	<pubDate>Mon, 07 Dec 2009 20:25:35 +0000</pubDate>

	<generator>http://en.wordpress.com/tags/</generator>
	<language>en</language>

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<title><![CDATA[LAN Airlines (Chile) Airbus A318-121 CC-CVB (msn 3030) (80 Anos)]]></title>
<link>http://airlinersgallery.wordpress.com/2009/12/03/lan-airlines-chile-airbus-a318-121-cc-cvb-msn-3030-80-anos/</link>
<pubDate>Thu, 03 Dec 2009 18:58:47 +0000</pubDate>
<dc:creator>brucedrum</dc:creator>
<guid>http://airlinersgallery.wordpress.com/2009/12/03/lan-airlines-chile-airbus-a318-121-cc-cvb-msn-3030-80-anos/</guid>
<description><![CDATA[LAN Airlines (Chile) Airbus A318-121 CC-CVB (msn 3030) (80 Anos) SCL, originally uploaded by Airline]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><div style="text-align:left;padding:3px;"><a title="photo sharing" href="http://airlinersgallery.com/2/26bf22e/#/gallery/lan-airlines-chile/lan-chile-a318-100-cc-cvb-04-80-anos-tko-scl-ar-lr-904248/"><img style="border:solid 2px #000000;" src="http://farm3.static.flickr.com/2571/4156180902_5df779f2ac.jpg" alt="" width="500" height="333" /></a></p>
<p><span style="font-size:.8em;margin-top:0;"><a href="http://www.flickr.com/photos/40168621@N07/4156180902/">LAN Airlines (Chile) Airbus A318-121 CC-CVB (msn 3030) (80 Anos) SCL</a>, originally uploaded by <a href="http://www.flickr.com/people/40168621@N07/">Airliners Gallery</a>.</span></div>
<p>Copyright Photo: Alvaro Romero.</p>
<p>Please click on photo or link below for a full view, information, prints for sale and other photos:</p>
<p><a href="http://airlinersgallery.com/2/26bf22e/#/gallery/lan-airlines-chile/lan-chile-a318-100-cc-cvb-04-80-anos-tko-scl-ar-lr-904248/">http://airlinersgallery.com/2/26bf22e/#/gallery/lan-airlines-chile/lan-chile-a318-100-cc-cvb-04-80-anos-tko-scl-ar-lr-904248/</a></p>
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<title><![CDATA[PAL-Principal Airlines (Aerolinea Principal de Chile) Boeing 737-236 CC-CZO (msn 22030)]]></title>
<link>http://airlinersgallery.wordpress.com/2009/11/30/pal-principal-airlines-aerolinea-principal-de-chile-boeing-737-236-cc-czo-msn-22030/</link>
<pubDate>Mon, 30 Nov 2009 14:02:34 +0000</pubDate>
<dc:creator>brucedrum</dc:creator>
<guid>http://airlinersgallery.wordpress.com/2009/11/30/pal-principal-airlines-aerolinea-principal-de-chile-boeing-737-236-cc-czo-msn-22030/</guid>
<description><![CDATA[PAL-Principal Airlines (Aerolinea Principal de Chile) Boeing 737-236 CC-CZO (msn 22030) SCL, origina]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><div style="text-align:left;padding:3px;"><a title="photo sharing" href="http://airlinersgallery.com/2/269adff/#/gallery/pal-principal-airlines/pal-principal-737-200-cc-czo-09-tko-scl-ar-lr-904236/"><img style="border:solid 2px #000000;" src="http://farm3.static.flickr.com/2499/4147328386_70f9368d32.jpg" alt="" width="500" height="324" /></a></p>
<p><span style="font-size:.8em;margin-top:0;"><a href="http://www.flickr.com/photos/40168621@N07/4147328386/">PAL-Principal Airlines (Aerolinea Principal de Chile) Boeing 737-236 CC-CZO (msn 22030) SCL</a>, originally uploaded by <a href="http://www.flickr.com/people/40168621@N07/">Airliners Gallery</a>.</span></div>
<p>Copyright Photo: Alvaro Romero.</p>
<p>Please click on photo or link below for full view, information, prints for sale and other photos:</p>
<p><a href="http://airlinersgallery.com/2/269adff/#/gallery/pal-principal-airlines/pal-principal-737-200-cc-czo-09-tko-scl-ar-lr-904236/">http://airlinersgallery.com/2/269adff/#/gallery/pal-principal-airlines/pal-principal-737-200-cc-czo-09-tko-scl-ar-lr-904236/</a></p>
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<title><![CDATA[David signing CD at the Deseret Book, SLC 24 November 2009]]></title>
<link>http://huong4david.wordpress.com/2009/11/24/david-signing-cd-at-the-deseret-book-slc-24-november-2009/</link>
<pubDate>Tue, 24 Nov 2009 11:44:23 +0000</pubDate>
<dc:creator>davidforever18</dc:creator>
<guid>http://huong4david.wordpress.com/2009/11/24/david-signing-cd-at-the-deseret-book-slc-24-november-2009/</guid>
<description><![CDATA[Credit to Carrie, @annyo84, and Sbedwards and UtahArchieAngel]]></description>
<content:encoded><![CDATA[Credit to Carrie, @annyo84, and Sbedwards and UtahArchieAngel]]></content:encoded>
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<title><![CDATA[The AMCL c/o The SCL]]></title>
<link>http://craigeisaac.wordpress.com/2009/11/16/the-amcl-co-the-scl/</link>
<pubDate>Mon, 16 Nov 2009 18:49:11 +0000</pubDate>
<dc:creator>craigeisaac</dc:creator>
<guid>http://craigeisaac.wordpress.com/2009/11/16/the-amcl-co-the-scl/</guid>
<description><![CDATA[It was a pleasure to receive the following note from The Society of Composers and Lyricists (&#8216;]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p>It was a pleasure to receive the following note from The Society of Composers and Lyricists (&#8216;The SCL&#8217;):</p>
<p>&#8216;The SCL Board of Directors wishes to notify you of an informational meeting concerning possible union representation for composers and lyricists working in all forms of contemporary media. This event is being hosted by the Teamsters Local 399 which represents workers in the motion picture, television, commercials, and live theatrical production industries.</p>
<p>Composers and lyricists have not had a collective bargaining agreement with studios and producers since 1970. Over these last 39 years, the need for representation, protection, and guidance has become a critical concern for all of us.</p>
<p>For the past three years, an ad hoc committee of working composers and lyricists has explored the possibility of achieving a collective bargaining agreement with producers. Although composed of SCL members, the committee has worked totally independently of the Society to determine that the best opportunity for composers and lyricists to achieve an industry-wide labor contract is by partnering with the Teamsters. Such a partnership would provide negotiating leverage in bargaining with producers for basic agreements covering Health Benefits, Pension, Working Conditions, and Wages. This informational meeting is the culmination of those three years of exploration by the committee.</p>
<p>This notification should not be interpreted as an official SCL endorsement of an alliance with the Teamsters. Further, should such a relationship become a reality, the resulting labor entity would be a completely separate and distinct organization from the SCL, which would continue to function in the same way that it has for the past 25 years.</p>
<p>However, the SCL Board believes that it is in your individual and collective best interests to at least investigate the possibility of a partnership with the Teamsters. While there are no guarantees of success in this organizational effort, we urge all composers and lyricists to attend this meeting to learn about the possibilities for representation, the individual benefits to be gained, and the potential problems involved in unionizing.&#8217;</p>
<p>I look forward to attending this evening&#8217;s meeting to learn more.  Please drop me an email or comment if you would like the details.</p>
<p>In the interim, explore more at <a href="http://www.theamcl.org">The AMCL</a></p>
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<title><![CDATA[Polygonal words]]></title>
<link>http://lamington.wordpress.com/2009/11/15/polygonal-words/</link>
<pubDate>Sun, 15 Nov 2009 21:48:25 +0000</pubDate>
<dc:creator>Danny Calegari</dc:creator>
<guid>http://lamington.wordpress.com/2009/11/15/polygonal-words/</guid>
<description><![CDATA[Last Friday, Henry Wilton gave a talk at Caltech about his recent joint work with Sang-hyun Kim on p]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p>Last Friday, Henry Wilton gave a talk at Caltech about his recent <a href="http://arxiv.org/abs/0910.4709">joint work</a> with Sang-hyun Kim on polygonal words in free groups. Their work is motivated by the following well-known question of Gromov:</p>
<p><strong><a href="http://www.math.utah.edu/~bestvina/eprints/questions-updated.pdf">Question(Gromov):</a></strong> Let <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> be a one-ended word-hyperbolic group. Does <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> contain a subgroup isomorphic to the fundamental group of a closed hyperbolic surface?</p>
<p>Let me briefly say what &#8220;one-ended&#8221; and &#8220;word-hyperbolic&#8221; mean.</p>
<p>A group is said to be word-hyperbolic if it acts properly and cocompactly by isometries on a proper <img src='http://l.wordpress.com/latex.php?latex=%5Cdelta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\delta' title='\delta' class='latex' />-hyperbolic path metric space &#8212; i.e. a path metric space in which there is a constant <img src='http://l.wordpress.com/latex.php?latex=%5Cdelta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\delta' title='\delta' class='latex' /> so that geodesic triangles in the metric space have the property that each side of the triangle is contained in the <img src='http://l.wordpress.com/latex.php?latex=%5Cdelta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\delta' title='\delta' class='latex' />-neighborhood of the union of the other two sides (colloquially, triangles are <em>thin</em>). This condition distills the essence of negative curvature in the large, and was <a href="http://www.ams.org/mathscinet-getitem?mr=919829">shown</a> by Gromov to be equivalent to several other conditions (eg. that the group satisfies a linear isoperimetric inequality; that every ultralimit of the group is an <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbb%7BR%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbb{R}' title='\mathbb{R}' class='latex' />-tree). Free groups are hyperbolic; fundamental groups of closed manifolds with negative sectional curvature (eg surfaces with negative Euler characteristic) are word-hyperbolic; &#8220;random&#8221; groups are hyperbolic &#8212; and so on. In fact, it is an open question whether a group <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> that admits a finite <img src='http://l.wordpress.com/latex.php?latex=K%28G%2C1%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K(G,1)' title='K(G,1)' class='latex' /> is word hyperbolic if and only if it does not contain a copy of a Baumslag-Solitar group <img src='http://l.wordpress.com/latex.php?latex=BS%28m%2Cn%29%3A%3D%5Clangle+x%2Cy+%5C%3B+%26%23124%3B+%5C%3B+x%5E%7B-1%7Dy%5E%7Bm%7Dx+%3D+y%5En+%5Crangle&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='BS(m,n):=\langle x,y \; &#124; \; x^{-1}y^{m}x = y^n \rangle' title='BS(m,n):=\langle x,y \; &#124; \; x^{-1}y^{m}x = y^n \rangle' class='latex' /> for <img src='http://l.wordpress.com/latex.php?latex=m%2Cn+%5Cne+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='m,n \ne 0' title='m,n \ne 0' class='latex' /> (note that the group <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbb%7BZ%7D%5Coplus+%5Cmathbb%7BZ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbb{Z}\oplus \mathbb{Z}' title='\mathbb{Z}\oplus \mathbb{Z}' class='latex' /> is the special case <img src='http://l.wordpress.com/latex.php?latex=m%3Dn%3D1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='m=n=1' title='m=n=1' class='latex' />); in any case, this is a very good heuristic for identifying the word-hyperbolic groups one typically meets in examples.</p>
<p>If <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> is a finitely generated group, the <em>ends</em> of <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> really means the ends (as defined by <a href="http://www.ams.org/mathscinet-getitem?mr=6504">Freudenthal</a>) of the Cayley graph of <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> with respect to some finite generating set. Given a proper topological space <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' />, the set of compact subsets of <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' /> gives rise to an inverse system of inclusions, where <img src='http://l.wordpress.com/latex.php?latex=X-K%27&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X-K&#039;' title='X-K&#039;' class='latex' /> includes into <img src='http://l.wordpress.com/latex.php?latex=X-K&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X-K' title='X-K' class='latex' /> whenever <img src='http://l.wordpress.com/latex.php?latex=K&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K' title='K' class='latex' /> is a subset of <img src='http://l.wordpress.com/latex.php?latex=K%27&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K&#039;' title='K&#039;' class='latex' />. This inverse system defines an inverse system of maps of discrete spaces <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_0%28X-K%27%29+%5Cto+%5Cpi_0%28X-K%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_0(X-K&#039;) \to \pi_0(X-K)' title='\pi_0(X-K&#039;) \to \pi_0(X-K)' class='latex' />, and the inverse limit of this system is a compact, totally disconnected space <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BE%7D%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{E}(X)' title='\mathcal{E}(X)' class='latex' />, called the <em>space of ends</em> of <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' />. A proper topological space is canonically compactified by its set of ends; in fact, the compactification <img src='http://l.wordpress.com/latex.php?latex=X+%5Ccup+%5Cmathcal%7BE%7D%28X%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X \cup \mathcal{E}(X)' title='X \cup \mathcal{E}(X)' class='latex' /> is the &#8220;biggest&#8221; compactification of <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' /> by a totally disconnected space, in the sense that for any other compactification <img src='http://l.wordpress.com/latex.php?latex=X+%5Csubset+Y&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X \subset Y' title='X \subset Y' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=Y-X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Y-X' title='Y-X' class='latex' /> is zero dimensional, there is a continuous map <img src='http://l.wordpress.com/latex.php?latex=X+%5Ccup+%5Cmathcal%7BE%7D%28X%29+%5Cto+Y&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X \cup \mathcal{E}(X) \to Y' title='X \cup \mathcal{E}(X) \to Y' class='latex' /> which is the identity on <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' />.</p>
<p>For a word-hyperbolic group <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' />, the Cayley graph can be compactified by adding the <em>ideal boundary</em> <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial_%5Cinfty+G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial_\infty G' title='\partial_\infty G' class='latex' />, but this is typically not totally disconnected. In this case, the ends of <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> can be recovered as the components of <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial_%5Cinfty+G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial_\infty G' title='\partial_\infty G' class='latex' />.</p>
<p>A group <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> acts on its own ends <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BE%7D%28G%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{E}(G)' title='\mathcal{E}(G)' class='latex' />. An elementary argument shows that the cardinality of <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BE%7D%28G%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{E}(G)' title='\mathcal{E}(G)' class='latex' /> is one of <img src='http://l.wordpress.com/latex.php?latex=0%2C1%2C2%2C%5Cinfty&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='0,1,2,\infty' title='0,1,2,\infty' class='latex' /> (if a compact set <img src='http://l.wordpress.com/latex.php?latex=V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V' title='V' class='latex' /> disconnects <img src='http://l.wordpress.com/latex.php?latex=e_1%2Ce_2%2Ce_3&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='e_1,e_2,e_3' title='e_1,e_2,e_3' class='latex' /> then infinitely many translates of <img src='http://l.wordpress.com/latex.php?latex=V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V' title='V' class='latex' /> converging to <img src='http://l.wordpress.com/latex.php?latex=e_1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='e_1' title='e_1' class='latex' /> separate <img src='http://l.wordpress.com/latex.php?latex=e_3&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='e_3' title='e_3' class='latex' /> from infinitely many other ends accumulating on <img src='http://l.wordpress.com/latex.php?latex=e_1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='e_1' title='e_1' class='latex' />). A group has no ends if and only if it is finite. Stallings famously <a href="http://www.ams.org/mathscinet-getitem?mr=415622">showed</a> that a (finitely generated) group has at least <img src='http://l.wordpress.com/latex.php?latex=2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='2' title='2' class='latex' /> ends if and only if it admits a nontrivial description as an HNN extension or amalgamated free product over a finite group. One version of the argument proceeds more or less as follows, at least when <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> is finitely presented. Let <img src='http://l.wordpress.com/latex.php?latex=M&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='M' title='M' class='latex' /> be an <img src='http://l.wordpress.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n' title='n' class='latex' />-dimensional Riemannian manifold with fundamental group <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' />, and let <img src='http://l.wordpress.com/latex.php?latex=%5Ctilde%7BM%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tilde{M}' title='\tilde{M}' class='latex' /> denote the universal cover. We can identify the ends of <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> with the ends of <img src='http://l.wordpress.com/latex.php?latex=%5Ctilde%7BM%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tilde{M}' title='\tilde{M}' class='latex' />. Let <img src='http://l.wordpress.com/latex.php?latex=V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V' title='V' class='latex' /> be a least (<img src='http://l.wordpress.com/latex.php?latex=n-1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n-1' title='n-1' class='latex' />-dimensional) area hypersurface in <img src='http://l.wordpress.com/latex.php?latex=%5Ctilde%7BM%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tilde{M}' title='\tilde{M}' class='latex' /> amongst all hypersurfaces that separate some end from some other (here the hypothesis that <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> has at least two ends is used). Then every translate of <img src='http://l.wordpress.com/latex.php?latex=V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V' title='V' class='latex' /> by an element of <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> is either equal to <img src='http://l.wordpress.com/latex.php?latex=V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V' title='V' class='latex' /> or disjoint from it, or else one could use the Meeks-Yau &#8220;roundoff trick&#8221; to find a new <img src='http://l.wordpress.com/latex.php?latex=V%27&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V&#039;' title='V&#039;' class='latex' /> with strictly lower area than <img src='http://l.wordpress.com/latex.php?latex=V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V' title='V' class='latex' />. The translates of <img src='http://l.wordpress.com/latex.php?latex=V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V' title='V' class='latex' /> decompose <img src='http://l.wordpress.com/latex.php?latex=%5Ctilde%7BM%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tilde{M}' title='\tilde{M}' class='latex' /> into pieces, and one can build a tree <img src='http://l.wordpress.com/latex.php?latex=T&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='T' title='T' class='latex' /> whose vertices correspond to to components of <img src='http://l.wordpress.com/latex.php?latex=%5Ctilde%7BM%7D+-+G%5Ccdot+V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tilde{M} - G\cdot V' title='\tilde{M} - G\cdot V' class='latex' />, and whose edges correspond to the translates <img src='http://l.wordpress.com/latex.php?latex=G%5Ccdot+V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G\cdot V' title='G\cdot V' class='latex' />. The group <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> acts on this tree, with finite edge stabilizers (by the compactness of <img src='http://l.wordpress.com/latex.php?latex=V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V' title='V' class='latex' />), exhibiting <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> either as an HNN extension or an amalgamated product over the edge stabilizers. Note that the special case <img src='http://l.wordpress.com/latex.php?latex=%26%23124%3B%5Cmathcal%7BE%7D%28G%29%26%23124%3B%3D2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='&#124;\mathcal{E}(G)&#124;=2' title='&#124;\mathcal{E}(G)&#124;=2' class='latex' /> occurs if and only if <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> has a finite index subgroup which is isomorphic to <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbb%7BZ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbb{Z}' title='\mathbb{Z}' class='latex' />.</p>
<p>Free groups and virtually free groups do not contain closed surface subgroups; Gromov&#8217;s question more or less asks whether these are the only examples of word-hyperbolic groups with this property.</p>
<p>Kim and Wilton study Gromov&#8217;s question in a very, very concrete case, namely that case that <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> is the double of a free group <img src='http://l.wordpress.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F' title='F' class='latex' /> along a word <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' />; i.e. <img src='http://l.wordpress.com/latex.php?latex=G+%3D+F+%2A_%7B%5Clangle+w+%5Crangle+%7D+F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G = F *_{\langle w \rangle } F' title='G = F *_{\langle w \rangle } F' class='latex' /> (hereafter denoted <img src='http://l.wordpress.com/latex.php?latex=D%28w%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='D(w)' title='D(w)' class='latex' />). Such groups are known to be one-ended if and only if <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> is not contained in a proper free factor of <img src='http://l.wordpress.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F' title='F' class='latex' /> (it is clear that this condition is necessary), and to be hyperbolic if and only if <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> is not a proper power, by a <a href="http://www.ams.org/mathscinet-getitem?mr=1152226">result</a> of Bestvina-Feighn. To see that this condition is necessary, observe that the double <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbb%7BZ%7D+%2A_%7Bp%5Cmathbb%7BZ%7D%7D+%5Cmathbb%7BZ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbb{Z} *_{p\mathbb{Z}} \mathbb{Z}' title='\mathbb{Z} *_{p\mathbb{Z}} \mathbb{Z}' class='latex' /> is isomorphic to the fundamental group of a Seifert fiber space, with base space a disk with two orbifold points of order <img src='http://l.wordpress.com/latex.php?latex=p&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='p' title='p' class='latex' />; such a group contains a <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbb%7BZ%7D%5Coplus+%5Cmathbb%7BZ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbb{Z}\oplus \mathbb{Z}' title='\mathbb{Z}\oplus \mathbb{Z}' class='latex' />. One might think that such groups are too simple to give an insight into Gromov&#8217;s question. However, these groups (or perhaps the slightly larger class of graphs of free groups with cyclic edge groups) are a critical case for at least two reasons:</p>
<ol>
<li>The &#8220;smaller&#8221; a group is, the less room there is inside it for a surface group; thus the &#8220;simplest&#8221; groups should have the best chance of being a counterexample to Gromov&#8217;s question.</li>
<li>If <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> is word-hyperbolic and one-ended, one can try to find a surface subgroup by first looking for a graph of free groups <img src='http://l.wordpress.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H' title='H' class='latex' /> in <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' />, and then looking for a surface group in <img src='http://l.wordpress.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H' title='H' class='latex' />. Since a closed surface group is itself a graph of free groups, one cannot &#8220;miss&#8221; any surface groups this way.</li>
</ol>
<p>Not too long ago, I found an interesting construction of surface groups in certain graphs of free groups with cyclic edge groups. In fact, I <a href="http://www.ams.org/mathscinet-getitem?mr=2431013">showed</a> that every nontrivial element of <img src='http://l.wordpress.com/latex.php?latex=H_2%28G%3B%5Cmathbb%7BQ%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H_2(G;\mathbb{Q})' title='H_2(G;\mathbb{Q})' class='latex' /> in such a group is virtually represented by a sum of surface subgroups. Such surface subgroups are obtained by finding maps of surface groups into <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> which minimize the Gromov norm in their (projective) homology class. I think it is useful to extend Gromov&#8217;s question by making the following</p>
<p><strong>Conjecture:</strong> Let <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> be a word-hyperbolic group, and let <img src='http://l.wordpress.com/latex.php?latex=%5Calpha+%5Cin+H_2%28G%3B%5Cmathbb%7BQ%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha \in H_2(G;\mathbb{Q})' title='\alpha \in H_2(G;\mathbb{Q})' class='latex' /> be nonzero. Then some multiple of <img src='http://l.wordpress.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha' title='\alpha' class='latex' /> is represented by a norm-minimizing surface (which is necessarily <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_1' title='\pi_1' class='latex' />-injective).</p>
<p>Note that this conjecture does not generalize to wider classes of groups. There are even examples of <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7BCAT%7D%280%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{CAT}(0)' title='\text{CAT}(0)' class='latex' /> groups <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> with nonzero homology classes <img src='http://l.wordpress.com/latex.php?latex=%5Calpha+%5Cin+H_2%28G%3B%5Cmathbb%7BQ%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha \in H_2(G;\mathbb{Q})' title='\alpha \in H_2(G;\mathbb{Q})' class='latex' /> with positive, rational Gromov norm, for which there are no <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_1' title='\pi_1' class='latex' />-injective surfaces representing a multiple of <img src='http://l.wordpress.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha' title='\alpha' class='latex' /> at all.</p>
<p>It is time to define polygonal words in free groups.</p>
<p><strong>Definition:</strong> Let <img src='http://l.wordpress.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F' title='F' class='latex' /> be free. Let <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' /> be a wedge of circles whose edges are free generators for <img src='http://l.wordpress.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F' title='F' class='latex' />. A cyclically reduced word <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> in these generators is <em>polygonal</em> if there exists a van-Kampen graph <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> on a surface <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> such that:</p>
<ol>
<li>every complementary region is a disk whose boundary is a nontrivial (possibly negative) power of <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' />;</li>
<li>the (labelled) graph <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> immerses in <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' /> in a label preserving way;</li>
<li>the Euler characteristic of <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> is strictly less than the number of disks.</li>
</ol>
<p>The last condition rules out trivial examples; for example, the double of a single disk whose boundary is labeled by <img src='http://l.wordpress.com/latex.php?latex=w%5En&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w^n' title='w^n' class='latex' />. Notice that it is very important to allow both positive and negative powers of <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> as boundaries of complementary regions. In fact, if <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> is not in the commutator subgroup, then the sum of the powers over all complementary regions is necessarily zero (and if <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> is in the commutator subgroup, then <img src='http://l.wordpress.com/latex.php?latex=D%28w%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='D(w)' title='D(w)' class='latex' /> has nontrivial <img src='http://l.wordpress.com/latex.php?latex=H_2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H_2' title='H_2' class='latex' />, so one already knows that there is a surface subgroup).</p>
<p>Condition 2. means that at each vertex of <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' />, there is at most one oriented label corresponding to each generator of <img src='http://l.wordpress.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F' title='F' class='latex' /> or its inverse. This is really the crucial geometric property. If <img src='http://l.wordpress.com/latex.php?latex=%5CGamma%2CS&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma,S' title='\Gamma,S' class='latex' /> is a van-Kampen graph as above, then a theorem of Marshall Hall implies that there is a finite cover of <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' /> into which <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> embeds (in fact, this observation underlies Stallings&#8217;s <a href="http://www.ams.org/mathscinet-getitem?mr=695906">work</a> on foldings of graphs). If we build a <img src='http://l.wordpress.com/latex.php?latex=2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='2' title='2' class='latex' />-complex <img src='http://l.wordpress.com/latex.php?latex=Y&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Y' title='Y' class='latex' /> with <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_1%28Y%29%3DD%28w%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_1(Y)=D(w)' title='\pi_1(Y)=D(w)' class='latex' /> by attaching two ends of a cylinder to suitable loops in two copies of <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' />, then a tubular neighborhood of <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> in <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> (i.e. what is sometimes called a &#8220;fatgraph&#8221; ) embeds in a finite cover <img src='http://l.wordpress.com/latex.php?latex=%5Ctilde%7BY%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tilde{Y}' title='\tilde{Y}' class='latex' /> of <img src='http://l.wordpress.com/latex.php?latex=Y&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Y' title='Y' class='latex' />, and its double &#8212; a surface of strictly negative Euler characteristic &#8212; embeds as a closed surface in <img src='http://l.wordpress.com/latex.php?latex=%5Ctilde%7BY%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tilde{Y}' title='\tilde{Y}' class='latex' />, and is therefore <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_1' title='\pi_1' class='latex' />-injective. Hence if <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> is polygonal, <img src='http://l.wordpress.com/latex.php?latex=D%28w%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='D(w)' title='D(w)' class='latex' /> contains a surface subgroup.</p>
<p>Not every word is polygonal. Kim-Wilton discuss some interesting examples in their paper, including:</p>
<ol>
<li>suppose <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> is a cyclically reduced product of proper powers of the generators or their inverses (e.g a word like <img src='http://l.wordpress.com/latex.php?latex=a%5E3b%5E7a%5E%7B-2%7Dc%5E%7B13%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a^3b^7a^{-2}c^{13}' title='a^3b^7a^{-2}c^{13}' class='latex' /> but not a word like <img src='http://l.wordpress.com/latex.php?latex=a%5E3bc%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a^3bc^{-1}' title='a^3bc^{-1}' class='latex' />); then <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> is polygonal;</li>
<li>a word of the form <img src='http://l.wordpress.com/latex.php?latex=%5Cprod_i+a%5E%7Bp_%7B2i-1%7D%7D%28a%5E%7Bp_%7B2i%7D%7D%29%5Eb&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\prod_i a^{p_{2i-1}}(a^{p_{2i}})^b' title='\prod_i a^{p_{2i-1}}(a^{p_{2i}})^b' class='latex' /> is polygonal if <img src='http://l.wordpress.com/latex.php?latex=%26%23124%3Bp_i%26%23124%3B%26%2362%3B1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='&#124;p_i&#124;&gt;1' title='&#124;p_i&#124;&gt;1' class='latex' /> for each <img src='http://l.wordpress.com/latex.php?latex=i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='i' title='i' class='latex' />;</li>
<li>the word <img src='http://l.wordpress.com/latex.php?latex=abab%5E2ab%5E3&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='abab^2ab^3' title='abab^2ab^3' class='latex' /> is <em>not</em> polygonal.</li>
</ol>
<p>To see 3, suppose there were a van-Kampen diagram with more disks than Euler characteristic. Then there must be some vertex of valence at least <img src='http://l.wordpress.com/latex.php?latex=3&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='3' title='3' class='latex' />. Since <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> is positive, the complementary regions must have boundaries which alternate between positive and negative powers of <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' />, so the degree of the vertex must be even. On the other hand, since <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> must immerse in a wedge of two circles, the degree of every vertex must be at most <img src='http://l.wordpress.com/latex.php?latex=4&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='4' title='4' class='latex' />, so there is consequently some vertex of degree exactly <img src='http://l.wordpress.com/latex.php?latex=4&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='4' title='4' class='latex' />. Since each <img src='http://l.wordpress.com/latex.php?latex=a&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a' title='a' class='latex' /> is isolated, at least <img src='http://l.wordpress.com/latex.php?latex=2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='2' title='2' class='latex' /> edges must be labelled <img src='http://l.wordpress.com/latex.php?latex=b&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='b' title='b' class='latex' />; hence exactly two. Hence exactly two edges are labelled <img src='http://l.wordpress.com/latex.php?latex=a&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a' title='a' class='latex' />. But one of these must be incoming and one outgoing, and therefore these are adjacent, contrary to the fact that <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> does not contain a <img src='http://l.wordpress.com/latex.php?latex=a%5E%7B%5Cpm+2%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a^{\pm 2}' title='a^{\pm 2}' class='latex' />.</p>
<p>1 above is quite striking to me. When <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> is in the commutator subgroup, one can consider van-Kampen diagrams as above without the injectivity property, but with the property that every power of <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> on the boundary of a disk is <em>positive</em>; call such a van-Kampen diagram <em>monotone</em>. It turns out that monotone van-Kampen diagrams always exist when <img src='http://l.wordpress.com/latex.php?latex=w+%5Cin+%5BF%2CF%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w \in [F,F]' title='w \in [F,F]' class='latex' />, and in fact that norm-minimizing surfaces representing powers of the generator of <img src='http://l.wordpress.com/latex.php?latex=H_2%28D%28w%29%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H_2(D(w))' title='H_2(D(w))' class='latex' /> are associated to certain monotone diagrams. The construction of such surfaces is an important step in the argument that stable commutator length (a kind of relative Gromov norm) is rational in free groups. In my paper <a href="http://arxiv.org/abs/0907.3541">scl, sails and surgery</a> I showed that monomorphisms of free groups that send every generator to a power of that generator induce isometries of the <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}' title='\text{scl}' class='latex' /> norm; in other words, there is a natural correspondence between certain equivalence classes of monotone surfaces for an arbitrary word in <img src='http://l.wordpress.com/latex.php?latex=%5BF%2CF%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[F,F]' title='[F,F]' class='latex' /> and for a word of the kind that Kim-Wilton show is polygonal (Note: Henry Wilton tells me that Brady, Forester and Martinez-Pedroza have independently shown that <img src='http://l.wordpress.com/latex.php?latex=D%28w%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='D(w)' title='D(w)' class='latex' /> contains a surface group for such <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' />, but I have not seen their preprint (though I would be very grateful to get a copy!)).</p>
<p>In any case, if not every word is polygonal, all is not lost. To show that <img src='http://l.wordpress.com/latex.php?latex=D%28w%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='D(w)' title='D(w)' class='latex' /> contains a surface subgroup is suffices to show that <img src='http://l.wordpress.com/latex.php?latex=D%28w%27%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='D(w&#039;)' title='D(w&#039;)' class='latex' /> contains a surface subgroup, where <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=w%27&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w&#039;' title='w&#039;' class='latex' /> differ by an automorphism of <img src='http://l.wordpress.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F' title='F' class='latex' />. Kim-Wilton conjecture that one can always find an automorphism <img src='http://l.wordpress.com/latex.php?latex=%5Cphi&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi' title='\phi' class='latex' /> so that <img src='http://l.wordpress.com/latex.php?latex=%5Cphi%28w%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi(w)' title='\phi(w)' class='latex' /> is polygonal. In fact, they make the following:</p>
<p><strong>Conjecture (Kim-Wilton; tiling conjecture):</strong> A word <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> not contained in a proper free factor of shortest length (in a given generating set) in its orbit under <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7BAut%7D%28F%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{Aut}(F)' title='\text{Aut}(F)' class='latex' /> is polygonal.</p>
<p>If true, this would give a positive answer to Gromov&#8217;s question for groups of the form <img src='http://l.wordpress.com/latex.php?latex=D%28w%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='D(w)' title='D(w)' class='latex' />.</p>
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<title><![CDATA[Arduino²: Zwei Arduinos verbinden]]></title>
<link>http://netzwelten.wordpress.com/2009/11/14/arduino%c2%b2-zwei-arduinos-verbinden/</link>
<pubDate>Sat, 14 Nov 2009 12:21:28 +0000</pubDate>
<dc:creator>netzwelten</dc:creator>
<guid>http://netzwelten.wordpress.com/2009/11/14/arduino%c2%b2-zwei-arduinos-verbinden/</guid>
<description><![CDATA[Da ich ja mittlerweile zwei Arduinos besitze, einen Arduino Mega sowie den Arduino Duemilanove, lieg]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p>Da ich ja mittlerweile zwei Arduinos besitze, einen Arduino Mega sowie den Arduino Duemilanove, liegt es ja nahe, diese einmal miteinander zu verbinden und sie über <a href="http://de.wikipedia.org/wiki/I2C">I²C</a> miteinander kommunizieren zu lassen. Im Sketch wird dazu die <a href="http://www.arduino.cc/en/Reference/Wire">Wire.h library</a> benutzt: <cite>This library allows you to communicate with I2C / TWI devices. On most Arduino boards, SDA (data line) is on analog input pin 4, and SCL (clock line) is on analog input pin 5. On the Arduino Mega, SDA is digital pin 20 and SCL is 21.</cite></p>
<p>Aber zunächst müssen die beiden Arduinos miteinander vernetzt werden. Das geht wie folgt: Zuerst braucht man einen &#8220;Master&#8221; und einen &#8220;Slave&#8221;, d.h. ein Arduino ist das &#8220;Gehirn&#8221;, der andere der ausführende &#8220;Sklave&#8221; <img src='http://s.wordpress.com/wp-includes/images/smilies/icon_wink.gif' alt=';-)' class='wp-smiley' /> . Weil der <a href="http://arduino.cc/en/Main/ArduinoBoardMega">Arduino Mega</a> mit seinen 54 digitalen In- und Output Pins, seinen 128kb Speicher sowie sonst auch ziemlich aufgemotzt daherkommt, lassen wir diesen mal den Slave spielen. Er ist an meinem <a href="http://netzwelten.wordpress.com/tag/eee-pc/">eee PC</a> angeschlossen, während der <a href="http://netzwelten.wordpress.com/2009/03/21/experimentierboard-arduino-duemilanove/">Arduino Duemilanove</a> an meinem Desktop PC hängt.</p>
<p>Nun werden die beiden Arduinos gemäß diesem Schema miteinander verbunden:</p>
<p><a href="http://netzwelten.wordpress.com/files/2009/11/arduino-netzwerk-schema.gif"><img src="http://netzwelten.wordpress.com/files/2009/11/arduino-netzwerk-schema.gif" alt="arduino-netzwerk-schema" title="arduino-netzwerk-schema" width="388" height="306" class="aligncenter size-full wp-image-521" /></a></p>
<p>Es ist wichtig, dass die beiden Arduinos ihre Stromkreise teilen, deshalb verbindet man jeweils 5V sowie GND (Ground, Erde) miteinander und setzt zwei Widerstände dazwischen, sonst funktioniert die Kommunikation zwischen den Arduinos nicht. Dann verbindet man die beiden SDA und SCL Pins der Boards miteinander, d.h. Analog In 4 des Duemilanoves mit 20 des Megas sowie Pin 5 des Duamilanoves mit Pin 21 des Megas. Es ergibt sich folgendes Bild:</p>
<p><a href="http://netzwelten.wordpress.com/files/2009/11/arduino-netzwerk1.jpg"><img src="http://netzwelten.wordpress.com/files/2009/11/arduino-netzwerk1.jpg" alt="arduino-netzwerk1" title="arduino-netzwerk1" width="500" height="375" class="aligncenter size-full wp-image-522" /></a></p>
<p>Ziel des ganzen ist es, ein kleines Netzwerk zwischen den beiden Arduinos aufzubauen, wobei am Duemilanove ein Lichtsensor arbeitet und den jeweils ermittelten Sensorwert an den Arduino Mega sendet. Dieser soll je nach Höhe des Wertes eine LED unterschiedlich hell aufleuchten lassen. Die in die eine Richtung (Duemilanove, Master &#8211;&#62; Mega, Slave) übertragenen und vom Lichtsensor ermittelten Werte sollen außerdem im Serial-Fenster angezeigt werden. Die komplette Schaltung sieht dann so aus:</p>
<p><a href="http://netzwelten.wordpress.com/files/2009/11/arduino-netzwerk2.jpg"><img src="http://netzwelten.wordpress.com/files/2009/11/arduino-netzwerk2.jpg" alt="arduino-netzwerk2" title="arduino-netzwerk2" width="500" height="375" class="aligncenter size-full wp-image-523" /></a></p>
<p>Nun müssen noch zwei kleine Sketche für die beiden Arduinos geschrieben werden. Wie oben bereits erwähnt, bedient man sich dabei der Wire.h-Bibliothek. Zuerst der Master:</p>
<pre class="brush: cpp;">

#include &#60;Wire.h&#62;

void setup()
{
  Serial.begin(9600);
  Wire.begin(); // join i2c bus
}

int sensorPin = 0;
int sensorValue = 0;

void loop()
{
  sensorValue = analogRead(sensorPin);
  Serial.println(sensorValue);
  Wire.beginTransmission(4); // transmit to device #4
  Wire.send(sensorValue);
  Wire.endTransmission();
  delay(500);
}
</pre>
<p>Die Datenübertragung läuft über device #4. Dasselbe wird auch im Slave aufgesetzt:</p>
<pre class="brush: cpp;">

#include &#60;Wire.h&#62;

int led_status = 0;
int ledPin = 13;

void setup()
{
  Wire.begin(4);                // join i2c bus with address #4
  Wire.onReceive(receiveEvent); // register event
  Serial.begin(9600);
  pinMode(ledPin, OUTPUT);
}

void loop()
{
  analogWrite(ledPin, led_status);
  delay(500);
}

// function that executes whenever data is received from master
// this function is registered as an event, see setup()
void receiveEvent(int howMany)
{
  led_status = Wire.receive();
  Serial.println(led_status);
} 
</pre>
<p>Die Quellcodes der Sketche sind leicht zu verstehen: Im loop() des Masters wird am Analog-Input der helligkeitsabhängige Widerstand des Lichtsensors gemessen, im Serial-Fenster ausgegeben sowie über die Funktion send() der Wire-Bibliothek verschickt. Der Slave bekommt diesen Wert, gibt ihn ebenfalls aus und benutzt den Wert für die analogWrite-Funtkion an die LED.</p>
<p>Abschließend zeigt dieses kurze und wackelige Video, dass das auch tatsächlich funktioniert:</p>
<p><span style='text-align:center; display: block;'><object width='425' height='350'><param name='movie' value='http://www.youtube.com/v/OcRRWhURX5U&#038;rel=1&#038;fs=1&#038;showsearch=0&#038;hd=0' /><param name='allowfullscreen' value='true' /><param name='wmode' value='transparent' /><embed src='http://www.youtube.com/v/OcRRWhURX5U&#038;rel=1&#038;fs=1&#038;showsearch=0&#038;hd=0' type='application/x-shockwave-flash' allowfullscreen='true' width='425' height='350' wmode='transparent'></embed></object></span></p>
<ul><strong>Links</strong></p>
<li><a href="http://hacknmod.com/hack/how-to-connect-multiple-arduino-microcontrollers-using-i2c/">Connect multiple Arduino microcontrollers using I²C</a></li>
<li><a href="http://www.arduino.cc/playground/Learning/I2C">I2C / TWI (Two-Wire Interface)</a></li>
<li><a href="http://www.arduino.cc/en/Reference/Wire">Die Wire-Library</a></li>
<li><a href="http://www.neufeld.newton.ks.us/electronics/?p=241">Arduino I2C Expansion I/O</a></li>
</ul>
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<title><![CDATA[Walking the Walk]]></title>
<link>http://snowberrylife.wordpress.com/2009/11/09/walking-the-walk/</link>
<pubDate>Mon, 09 Nov 2009 19:52:38 +0000</pubDate>
<dc:creator>j</dc:creator>
<guid>http://snowberrylife.wordpress.com/2009/11/09/walking-the-walk/</guid>
<description><![CDATA[I&#8217;ve frequently encouraged/harassed people into visiting the Stuff Christians Like blog, and t]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p>I&#8217;ve frequently encouraged/harassed people into visiting the <a title="SCL" href="http://stuffchristianslike.net/">Stuff Christians Like</a> blog, and today, I&#8217;d like to do it once more.</p>
<p>Jon (the author of the blog) is proving that he can do more than write funny stories. Today, he&#8217;s connecting his readers with Samaritan&#8217;s Purse in an effort to build a school in Vietnam.</p>
<p>Go to his <a title="SCL- What if?" href="http://stuffchristianslike.net/2009/11/this-cant-be-real/">blog</a>. Read how his 6 year old daughter inspired this venture. Give a dollar or two and make an impact on the other side of the world.</p>
<p>Do you really have an excuse not to help?</p>
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<title><![CDATA[Exactrail HO Scale Gunderson 2420 Gondolas Now Available!]]></title>
<link>http://dccinstalled.wordpress.com/2009/11/03/exactrail-ho-scale-gunderson-2420-gondolas-now-available/</link>
<pubDate>Tue, 03 Nov 2009 04:40:04 +0000</pubDate>
<dc:creator>aealbright</dc:creator>
<guid>http://dccinstalled.wordpress.com/2009/11/03/exactrail-ho-scale-gunderson-2420-gondolas-now-available/</guid>
<description><![CDATA[HO Scale Gunderson 2420 Gondola Click Here to order now, only 15.99!]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p style="text-align:center;">HO Scale Gunderson 2420 Gondola</p>
<p style="text-align:center;"><img class="aligncenter size-full wp-image-525" title="ho-cr-gondola-01" src="http://dccinstalled.wordpress.com/files/2009/11/ho-cr-gondola-01.jpg" alt="ho-cr-gondola-01" width="450" height="300" /><a href="http://www.dccinstalled.com/HO_Gunderson_2420_Gondolas_s/2733.htm&#38;Click=14" target="_blank"><br />
Click Here</a> to order now, only <span style="color:#ff0000;">15.99</span>!</p>
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<title><![CDATA[PLUNA performs test flight in Chile]]></title>
<link>http://worldairlinenews.wordpress.com/2009/10/27/pluna-performs-test-flight-in-chile/</link>
<pubDate>Tue, 27 Oct 2009 16:21:00 +0000</pubDate>
<dc:creator>brucedrum</dc:creator>
<guid>http://worldairlinenews.wordpress.com/2009/10/27/pluna-performs-test-flight-in-chile/</guid>
<description><![CDATA[PLUNA Lineas Aereas Uruguayas Bombardier CRJ900 (CL-600-2D24) CX-CRD (msn 15180) SCL, originally upl]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><div style="text-align:left;padding:3px;"><a title="photo sharing" href="http://airlinersgallery.com/2/2526118/#/gallery/pluna/pluna-crj900-cx-crd-08-grd-scl-ar-lr-901660/"><img style="border:solid 2px #000000;" src="http://farm3.static.flickr.com/2501/4050411520_9e19be389e.jpg" alt="" width="500" height="333" /></a></p>
<p><span style="font-size:.8em;margin-top:0;"><a href="http://www.flickr.com/photos/40168621@N07/4050411520/">PLUNA Lineas Aereas Uruguayas Bombardier CRJ900 (CL-600-2D24) CX-CRD (msn 15180) SCL</a>, originally uploaded by <a href="http://www.flickr.com/people/40168621@N07/">Airliners Gallery</a>.</span></div>
<p>PLUNA Lineas Aereas Uruguayas (Montevideo) on October 23, 2009 performed its first test flight inside Chilean territory. The overnight flight linked Santiago de Chile (SCL) with Punta Arenas (PUQ) as flight PU 441 carrying freight (newspapers, magazines and documents) in a seat container configuration. The company used Bombardier CRJ900 (CL-600-2D24) CX-CRB. The cargo was flown on behalf of SKY Cargo (a subsidiary of SKY Airline) thanks to an agreement with that Chilean company. PLUNA is planning to operate passenger flights in Chile starting in December and will use the same aircraft on the route Punta Arenas -Santiago.</p>
<p>Copyright Photo: Alvaro Romero.</p>
<p>Sister ship CX-CRD (msn 15180) is seen at Santiago on a normal flight to and from Montevideo.</p>
<p>Please click on photo or link below for full view, information and other photos:</p>
<p><a href="http://airlinersgallery.com/2/2526118/#/gallery/pluna/pluna-crj900-cx-crd-08-grd-scl-ar-lr-901660/">http://airlinersgallery.com/2/2526118/#/gallery/pluna/pluna-crj900-cx-crd-08-grd-scl-ar-lr-901660/</a></p>
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<title><![CDATA[This guy is funny!]]></title>
<link>http://thesaltlick.tv/2009/10/26/this-guy-is-funny/</link>
<pubDate>Mon, 26 Oct 2009 13:56:05 +0000</pubDate>
<dc:creator>pgowesky</dc:creator>
<guid>http://thesaltlick.tv/2009/10/26/this-guy-is-funny/</guid>
<description><![CDATA[Seriously, just when you think that you are funny, someone else always shows up to the party that is]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p><a rel="attachment wp-att-1142" href="http://thesaltlick.tv/2009/10/26/this-guy-is-funny/jon-acuff-3/"><img class="alignleft size-full wp-image-1142" title="jon acuff" src="http://saltlick.wordpress.com/files/2009/10/jon-acuff2.jpg" alt="jon acuff" /></a>Seriously, just when you think that you are funny, someone else always shows up to the party that is infinitely funnier!  Totally ruins the mood!  So, whenever I look for a good dose of humor, I turn to non other than my friend Jon Acuff.  We&#8217;re facebook friends, that proves friendship right?  I mean, we all have deep and meaningful relationships with every single one of the 4.25 million people that we are &#8220;Friends&#8221; with.  So, then you could say that I am friends with Johnny as I like to call him.  (I can do that cause we&#8217;re <em>friends</em>&#8230;)</p>
<p>Today&#8217;s post was too funny not to share&#8230; Here is today&#8217;s <a href="http://stuffchristianslike.net/2009/10/deep-v-neck-syndrome-dvs/">post</a> from his blog, S<a href="http://stuffchristianslike.net/">tuff Christians Like</a>.  Check it out daily for a good dose of humor!</p>
<p>Today&#8217;s post is on the subject of: &#8220;The V neck&#8221;.  And as you know, I am a fan of the V.  So, head over <a href="http://stuffchristianslike.net/2009/10/deep-v-neck-syndrome-dvs/">here</a>&#8230; check it out, and enjoy!</p>
<p>~Peter</p>
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<title><![CDATA[Exactrail's Newest HO Scale Car, the Gunderson 2420 Gondola Announced!]]></title>
<link>http://dccinstalled.wordpress.com/2009/10/14/exactrails-newest-ho-scale-car-the-gunderson-2420-gondola-announced/</link>
<pubDate>Wed, 14 Oct 2009 14:22:59 +0000</pubDate>
<dc:creator>aealbright</dc:creator>
<guid>http://dccinstalled.wordpress.com/2009/10/14/exactrails-newest-ho-scale-car-the-gunderson-2420-gondola-announced/</guid>
<description><![CDATA[About the Gunderson 2420 Beginning in March of 1965, Gunderson built nine hundred 2,420 cu. ft. capa]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p><img class="aligncenter size-full wp-image-507" title="introducing_express" src="http://dccinstalled.wordpress.com/files/2009/10/introducing_express.jpg" alt="introducing_express" width="391" height="43" /></p>
<p><img class="aligncenter size-full wp-image-505" title="HO-sp-gondola-01" src="http://dccinstalled.wordpress.com/files/2009/10/ho-sp-gondola-01.jpg" alt="HO-sp-gondola-01" width="400" height="267" /><strong>About the Gunderson 2420</strong></p>
<p>Beginning in March of 1965, Gunderson built nine hundred 2,420 cu. ft. capacity gondolas for the Southern Pacific. With a straight, deep side sill, massive side stakes and a heavy duty top cord, these cars had a distinguished appearance without comparison. The Southern Pacific implemented rebuilding programs for these cars on two occasions, which kept them on the rails well into the nineties. ExactRail has precision captured the beautiful lines of these cars from the full flute side panels to the dreadnaught ends. Accurately decorated in Southern Pacific as well as classic period-era Heritage Decoration schemes, these classics are sure to please modelers from all corners of the hobby.</p>
<p>Retail $19.99     WRH $15.99</p>
<p>Available in the following road names:</p>
<p>SP, ATSF, ICG, GN, SCL, CR</p>
<p>Coming to <a href="http://www.dccinstalled.com/HO_Gunderson_2420_Gondolas_s/2733.htm" target="_blank">www.dccinstalled.com</a> November 2nd!</p>
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<title><![CDATA[Seattle City Lights Announces Data Feeds ]]></title>
<link>http://elliottlemenager.com/2009/10/08/seattle-city-lights-announces-data-feeds/</link>
<pubDate>Thu, 08 Oct 2009 05:13:43 +0000</pubDate>
<dc:creator>elemenager</dc:creator>
<guid>http://elliottlemenager.com/2009/10/08/seattle-city-lights-announces-data-feeds/</guid>
<description><![CDATA[Today Seattle City Light is the first utility to announce that it is offering customers the ability ]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p>Today Seattle City Light is the first utility to announce that it is offering  customers the ability to link their electricity consumption data with Microsoft Hohm.&#8221;Our customers understand that energy conservation means lower bills and less impact on our environment,” Superintendent Jorge Carrasco said. “We want to help them use less of our product by giving them the tools like Hohm to manage their energy use wisely.”</p>
<p>City Light was one of four launch partners when Microsoft Hohm debuted in Beta version in June and is the first utility to announce its customers can connect with a convenient, automatic data feed. Hohm users who do not have a data feed can enter their energy use information manually.</p>
<p>Nadia and I continued with our show to make the annoucement, give us some feedback on how we can improve the show.</p>
<p><span style='text-align:center; display: block;'><object width='425' height='350'><param name='movie' value='http://www.youtube.com/v/C7Ydtf9hqKs&#038;rel=1&#038;fs=1&#038;showsearch=0&#038;hd=0' /><param name='allowfullscreen' value='true' /><param name='wmode' value='transparent' /><embed src='http://www.youtube.com/v/C7Ydtf9hqKs&#038;rel=1&#038;fs=1&#038;showsearch=0&#038;hd=0' type='application/x-shockwave-flash' allowfullscreen='true' width='425' height='350' wmode='transparent'></embed></object></span></p>
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<title><![CDATA[Prezes SCL JE Sezer proponuje zmianę, która obejmie 3 dywizje]]></title>
<link>http://sultanat.wordpress.com/2009/09/28/prezes-scl-je-sezer-proponuje-zmiane-ktora-obejmie-3-dywizje/</link>
<pubDate>Mon, 28 Sep 2009 21:29:53 +0000</pubDate>
<dc:creator>sultanat</dc:creator>
<guid>http://sultanat.wordpress.com/2009/09/28/prezes-scl-je-sezer-proponuje-zmiane-ktora-obejmie-3-dywizje/</guid>
<description><![CDATA[Kraj / Sport: Prezes stowarzyszenia SAR Camel League [SCL] Ekscelencja Dżalal bin Sezer w krótkiej r]]></description>
<content:encoded><![CDATA[Kraj / Sport: Prezes stowarzyszenia SAR Camel League [SCL] Ekscelencja Dżalal bin Sezer w krótkiej r]]></content:encoded>
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<title><![CDATA[SCL Annual Conference: The impact of changing economic cycles on the practice of IT Law]]></title>
<link>http://chrisdale.wordpress.com/2009/08/11/scl-annual-conference-the-impact-of-changing-economic-cycles-on-the-practice-of-it-law/</link>
<pubDate>Tue, 11 Aug 2009 01:36:02 +0000</pubDate>
<dc:creator>Editor</dc:creator>
<guid>http://chrisdale.wordpress.com/2009/08/11/scl-annual-conference-the-impact-of-changing-economic-cycles-on-the-practice-of-it-law/</guid>
<description><![CDATA[I promised in an earlier post to follow up on a reference to the Society for Computers and Law Annua]]></description>
<content:encoded><![CDATA[I promised in an earlier post to follow up on a reference to the Society for Computers and Law Annua]]></content:encoded>
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<title><![CDATA[Faces of the scl norm ball]]></title>
<link>http://lamington.wordpress.com/2009/08/04/faces-of-the-scl-norm-ball/</link>
<pubDate>Tue, 04 Aug 2009 13:01:58 +0000</pubDate>
<dc:creator>Danny Calegari</dc:creator>
<guid>http://lamington.wordpress.com/2009/08/04/faces-of-the-scl-norm-ball/</guid>
<description><![CDATA[I am in Melbourne at the moment, in the middle of giving a lecture series, as part of the 2009 Clay-]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p>I am in Melbourne at the moment, in the middle of giving a lecture series, as part of the 2009 <a href="http://www.austms.org.au/tiki-read_article.php?articleId=61">Clay-Mahler lectures</a> (also see <a href="http://www.claymath.org/programs/claylecturesmath/2010CLM/">here</a>). Yesterday I gave a lecture with the title &#8220;faces of the scl norm ball&#8221;, and I thought I would try to give a sense of what it was all about. This also gives me an excuse to fiddle around with images in wordpress.</p>
<p>One starts with a basic question: given an immersion of a circle in the plane, when is there an immersion of the disk in the plane that bounds the given immersion of a circle? I.e., given a immersion <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma%3AS%5E1+%5Cto+%5Cbf%7BR%7D%5E2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma:S^1 \to \bf{R}^2' title='\gamma:S^1 \to \bf{R}^2' class='latex' />, when is there an immersion <img src='http://l.wordpress.com/latex.php?latex=f%3AD%5E2+%5Cto+%5Cbf%7BR%7D%5E2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f:D^2 \to \bf{R}^2' title='f:D^2 \to \bf{R}^2' class='latex' /> for which <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+f&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial f' title='\partial f' class='latex' /> factors through <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' />? Obviously this depends on <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' />. Consider the following examples:</p>
<p><img class="aligncenter size-full wp-image-429" title="immersed_circles" src="http://lamington.wordpress.com/files/2009/08/immersed_circles.jpg" alt="immersed_circles" width="380" height="120" />The first immersed circle obviously bounds an immersed disk; in fact, an embedded disk.</p>
<p>The second circle does not bound such a disk. One way to see this is to use the Gauss map, i.e. the map <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma%27%2F%26%23124%3B%5Cgamma%27%26%23124%3B%3AS%5E1+%5Cto+S%5E1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma&#039;/&#124;\gamma&#039;&#124;:S^1 \to S^1' title='\gamma&#039;/&#124;\gamma&#039;&#124;:S^1 \to S^1' class='latex' /> that takes each point on the circle to the unit tangent to its image under the immersion. The degree of the Gauss map for an embedded circle is <img src='http://l.wordpress.com/latex.php?latex=%5Cpm+1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pm 1' title='\pm 1' class='latex' /> (depending on a choice of orientation). If an immersed circle bounds an immersed disk, one can use this immersed disk to define a 1-parameter family of immersions, connecting the initial immersed circle to an embedded immersed circle; hence the degree of the Gauss map is aso <img src='http://l.wordpress.com/latex.php?latex=%5Cpm+1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pm 1' title='\pm 1' class='latex' /> for an immersed circle bounding an immersed disk; this rules out the second example.</p>
<p>The third example maps under the Gauss map with degree 1, and yet it does not bound an immersed disk. One must use a slightly more sophisticated invariant to see this. The immersed circle divides the plane up into regions. For each bounded region <img src='http://l.wordpress.com/latex.php?latex=R&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='R' title='R' class='latex' />, let <img src='http://l.wordpress.com/latex.php?latex=%5Calpha%3A%5B0%2C1%5D+%5Cto+%5Cbf%7BR%7D%5E2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha:[0,1] \to \bf{R}^2' title='\alpha:[0,1] \to \bf{R}^2' class='latex' /> be an embedded arc, transverse to <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' />, that starts in the region <img src='http://l.wordpress.com/latex.php?latex=R&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='R' title='R' class='latex' /> and ends up &#8220;far away&#8221; (ideally &#8220;at infinity&#8221;). The arc <img src='http://l.wordpress.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha' title='\alpha' class='latex' /> determines a homological intersection number that we denote <img src='http://l.wordpress.com/latex.php?latex=%5Calpha+%5Ccap+%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha \cap \gamma' title='\alpha \cap \gamma' class='latex' />, where each point of intersection contributes <img src='http://l.wordpress.com/latex.php?latex=%5Cpm+1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pm 1' title='\pm 1' class='latex' /> depending on orientations. In this example, there are three bounded regions, which get the numbers <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />, <img src='http://l.wordpress.com/latex.php?latex=-1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-1' title='-1' class='latex' />, <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' /> respectively:</p>
<p><img class="aligncenter size-full wp-image-430" title="immersions2" src="http://lamington.wordpress.com/files/2009/08/immersions2.jpg" alt="immersions2" width="300" height="120" />If <img src='http://l.wordpress.com/latex.php?latex=f%3AS+%5Cto+%5Cbf%7BR%7D%5E2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f:S \to \bf{R}^2' title='f:S \to \bf{R}^2' class='latex' /> is any map of any oriented surface with one boundary component whose boundary factors through <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' />, then the (homological) degree with which <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> maps over each region complementary to the image of <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' /> is the number we have just defined. Hence if <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' /> bounds an immersed disk, these numbers must all be positive (or all negative, if we reverse orientation). This rules out the third example.</p>
<p>The complete answer of which immersed circles in the plane bound immersed disks was given by S. Blank, in his Ph.D. thesis at Brandeis in 1967 (unfortunately, this does not appear to be available online). The answer is in the form of an algorithm to decide the question. One such algorithm (not Blank&#8217;s, but related to it) is as follows. The image of <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' /> cuts up the plane into regions <img src='http://l.wordpress.com/latex.php?latex=R_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='R_i' title='R_i' class='latex' />, and each region <img src='http://l.wordpress.com/latex.php?latex=R_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='R_i' title='R_i' class='latex' /> gets an integer <img src='http://l.wordpress.com/latex.php?latex=n_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n_i' title='n_i' class='latex' />. Take <img src='http://l.wordpress.com/latex.php?latex=n_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n_i' title='n_i' class='latex' /> &#8220;copies&#8221; of each region <img src='http://l.wordpress.com/latex.php?latex=R_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='R_i' title='R_i' class='latex' />, and think of these as pieces of a jigsaw puzzle. Try to glue them together along their edges so that they fit together nicely along <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' /> and make a disk with smooth boundary. If you are successful, you have constructed an immersion. If you are not successful (after trying all possible ways of gluing the puzzle pieces together), no such immersion exists. This answer is a bit unsatisfying, since in the first place it does not give any insight into which loops bound and which don&#8217;t, and in the second place the algorithm is quite slow and impractial.</p>
<p>As usual, more insight can be gained by generalizing the question. Fix a compact oriented surface <img src='http://l.wordpress.com/latex.php?latex=%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Sigma' title='\Sigma' class='latex' /> and consider an immersed <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />-manifold <img src='http://l.wordpress.com/latex.php?latex=%5CGamma%3A+%5Ccoprod_i+S%5E1+%5Cto+%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma: \coprod_i S^1 \to \Sigma' title='\Gamma: \coprod_i S^1 \to \Sigma' class='latex' />. One would like to know which such <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />-manifolds bound an immersion of a surface. One piece of subtlety is the fact that there are examples where <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> itself does not bound, but a finite cover of <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> (e.g. two copies of <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' />) does bound. It is also useful to restrict the class of <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />-manifolds that one considers. For the sake of concreteness then, let <img src='http://l.wordpress.com/latex.php?latex=%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Sigma' title='\Sigma' class='latex' /> be a hyperbolic surface with geodesic boundary, and let <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> be an oriented immersed geodesic <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />-manifold in <img src='http://l.wordpress.com/latex.php?latex=%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Sigma' title='\Sigma' class='latex' />. An immersion <img src='http://l.wordpress.com/latex.php?latex=f%3AS+%5Cto+%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f:S \to \Sigma' title='f:S \to \Sigma' class='latex' /> is said to <em>virtually bound</em> <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> if the map <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+f&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial f' title='\partial f' class='latex' /> factors as a composition <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+S+%5Cto+%5Ccoprod_i+S%5E1+%5Cto+%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial S \to \coprod_i S^1 \to \Sigma' title='\partial S \to \coprod_i S^1 \to \Sigma' class='latex' /> where the second map is <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' />, and where the first map is a covering map with some degree <img src='http://l.wordpress.com/latex.php?latex=n%28S%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n(S)' title='n(S)' class='latex' />. The fundamental question, then is:</p>
<p><strong>Question:</strong> Which immersed geodesic <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />-manifolds <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> in <img src='http://l.wordpress.com/latex.php?latex=%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Sigma' title='\Sigma' class='latex' /> are virtually bounded by an immersed surface?</p>
<p>It turns out that this question is unexpectedly connected to stable commutator length, symplectic rigidity, and several other geometric issues; I hope to explain how in the remainder of this post.</p>
<p>First, recall that if <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> is any group and <img src='http://l.wordpress.com/latex.php?latex=g+%5Cin+%5BG%2CG%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g \in [G,G]' title='g \in [G,G]' class='latex' />, the <em>commutator length</em> of <img src='http://l.wordpress.com/latex.php?latex=g&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g' title='g' class='latex' />, denoted <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bcl%7D%28g%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{cl}(g)' title='\text{cl}(g)' class='latex' />, is the smallest number of commutators in <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> whose product is equal to <img src='http://l.wordpress.com/latex.php?latex=g&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g' title='g' class='latex' />, and the <em>stable commutator length</em> <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D%28g%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}(g)' title='\text{scl}(g)' class='latex' /> is the limit <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D%28g%29+%3D+%5Clim_%7Bn+%5Cto+%5Cinfty%7D+%5Ctext%7Bcl%7D%28g%5En%29%2Fn&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}(g) = \lim_{n \to \infty} \text{cl}(g^n)/n' title='\text{scl}(g) = \lim_{n \to \infty} \text{cl}(g^n)/n' class='latex' />. One can geometrize this definition as follows. Let <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' /> be a space with <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_1%28X%29+%3D+G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_1(X) = G' title='\pi_1(X) = G' class='latex' />, and let <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma%3AS%5E1+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma:S^1 \to X' title='\gamma:S^1 \to X' class='latex' /> be a homotopy class of loop representing the conjugacy class of <img src='http://l.wordpress.com/latex.php?latex=g&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g' title='g' class='latex' />. Then <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D%28g%29+%3D+%5Cinf_S+-%5Cchi%5E-%28S%29%2F2n%28S%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}(g) = \inf_S -\chi^-(S)/2n(S)' title='\text{scl}(g) = \inf_S -\chi^-(S)/2n(S)' class='latex' /> over all surfaces <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> (possibly with multiple boundary components) mapping to <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' /> whose boundary wraps a total of <img src='http://l.wordpress.com/latex.php?latex=n%28S%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n(S)' title='n(S)' class='latex' /> times around <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' />. One can extend this definition to <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />-manifolds <img src='http://l.wordpress.com/latex.php?latex=%5CGamma%3A%5Ccoprod_i+S%5E1+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma:\coprod_i S^1 \to X' title='\Gamma:\coprod_i S^1 \to X' class='latex' /> in the obvious way, and one gets a definition of stable commutator length for formal sums of elements in <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> which represent <img src='http://l.wordpress.com/latex.php?latex=0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='0' title='0' class='latex' /> in homology. Let <img src='http://l.wordpress.com/latex.php?latex=B_1%28G%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='B_1(G)' title='B_1(G)' class='latex' /> denote the vector space of real finite linear combinations of elements in <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> whose sum represents zero in (real group) homology (i.e. in the abelianization of <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' />, tensored with <img src='http://l.wordpress.com/latex.php?latex=%5Cbf%7BR%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\bf{R}' title='\bf{R}' class='latex' />). Let <img src='http://l.wordpress.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H' title='H' class='latex' /> be the subspace spanned by chains of the form <img src='http://l.wordpress.com/latex.php?latex=g%5En+-+ng&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g^n - ng' title='g^n - ng' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=g+-+hgh%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g - hgh^{-1}' title='g - hgh^{-1}' class='latex' />. Then <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}' title='\text{scl}' class='latex' /> descends to a (pseudo)-norm on the quotient <img src='http://l.wordpress.com/latex.php?latex=B_1%28G%29%2FH&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='B_1(G)/H' title='B_1(G)/H' class='latex' /> which we denote hereafter by <img src='http://l.wordpress.com/latex.php?latex=B_1%5EH%28G%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='B_1^H(G)' title='B_1^H(G)' class='latex' /> (<img src='http://l.wordpress.com/latex.php?latex=H&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H' title='H' class='latex' /> for homogeneous).</p>
<p>There is a dual definition of this norm, in terms of <em>quasimorphisms</em>.</p>
<p><strong>Definition:</strong> Let <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> be a group. A function <img src='http://l.wordpress.com/latex.php?latex=%5Cphi%3AG+%5Cto+%5Cbf%7BR%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi:G \to \bf{R}' title='\phi:G \to \bf{R}' class='latex' /> is a <em>homogeneous quasimorphism</em> if there is a least non-negative real number <img src='http://l.wordpress.com/latex.php?latex=D%28%5Cphi%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='D(\phi)' title='D(\phi)' class='latex' /> (called the <em>defect</em>) so that for all <img src='http://l.wordpress.com/latex.php?latex=g%2Ch+%5Cin+G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g,h \in G' title='g,h \in G' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=n+%5Cin+%5Cbf%7BZ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n \in \bf{Z}' title='n \in \bf{Z}' class='latex' /> one has</p>
<ol>
<li><img src='http://l.wordpress.com/latex.php?latex=%5Cphi%28g%5En%29+%3D+n%5Cphi%28g%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi(g^n) = n\phi(g)' title='\phi(g^n) = n\phi(g)' class='latex' /> (homogeneity)</li>
<li><img src='http://l.wordpress.com/latex.php?latex=%26%23124%3B%5Cphi%28gh%29+-+%5Cphi%28g%29+-+%5Cphi%28h%29%26%23124%3B+%5Cle+D%28%5Cphi%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='&#124;\phi(gh) - \phi(g) - \phi(h)&#124; \le D(\phi)' title='&#124;\phi(gh) - \phi(g) - \phi(h)&#124; \le D(\phi)' class='latex' /> (quasimorphism)</li>
</ol>
<p>A function satisfying the second condition but not the first is an (ordinary) quasimorphism. The vector space of quasimorphisms on <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> is denoted <img src='http://l.wordpress.com/latex.php?latex=%5Cwidehat%7BQ%7D%28G%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\widehat{Q}(G)' title='\widehat{Q}(G)' class='latex' />, and the vector subspace of homogeneous quasimorphisms is denoted <img src='http://l.wordpress.com/latex.php?latex=Q%28G%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Q(G)' title='Q(G)' class='latex' />. Given <img src='http://l.wordpress.com/latex.php?latex=%5Cphi+%5Cin+%5Cwidehat%7BQ%7D%28G%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi \in \widehat{Q}(G)' title='\phi \in \widehat{Q}(G)' class='latex' />, one can homogenize it, by defining <img src='http://l.wordpress.com/latex.php?latex=%5Coverline%7B%5Cphi%7D%28g%29+%3D+%5Clim_%7Bn+%5Cto+%5Cinfty%7D+%5Cphi%28g%5En%29%2Fn&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\overline{\phi}(g) = \lim_{n \to \infty} \phi(g^n)/n' title='\overline{\phi}(g) = \lim_{n \to \infty} \phi(g^n)/n' class='latex' />. Then <img src='http://l.wordpress.com/latex.php?latex=%5Coverline%7B%5Cphi%7D+%5Cin+Q%28G%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\overline{\phi} \in Q(G)' title='\overline{\phi} \in Q(G)' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=D%28%5Coverline%7B%5Cphi%7D%29+%5Cle+2D%28%5Cphi%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='D(\overline{\phi}) \le 2D(\phi)' title='D(\overline{\phi}) \le 2D(\phi)' class='latex' />. A quasimorphism has defect zero if and only if it is a homomorphism (i.e. an element of <img src='http://l.wordpress.com/latex.php?latex=H%5E1%28G%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H^1(G)' title='H^1(G)' class='latex' />) and <img src='http://l.wordpress.com/latex.php?latex=D%28%5Ccdot%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='D(\cdot)' title='D(\cdot)' class='latex' /> makes the quotient <img src='http://l.wordpress.com/latex.php?latex=Q%2FH%5E1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Q/H^1' title='Q/H^1' class='latex' /> into a Banach space.</p>
<p>Examples of quasimorphisms include the following:</p>
<ol>
<li>Let <img src='http://l.wordpress.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F' title='F' class='latex' /> be a free group on a generating set <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' />. Let <img src='http://l.wordpress.com/latex.php?latex=%5Csigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sigma' title='\sigma' class='latex' /> be a reduced word in <img src='http://l.wordpress.com/latex.php?latex=S%5E%2A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S^*' title='S^*' class='latex' /> and for each reduced word <img src='http://l.wordpress.com/latex.php?latex=w+%5Cin+S%5E%2A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w \in S^*' title='w \in S^*' class='latex' />, define <img src='http://l.wordpress.com/latex.php?latex=C_%5Csigma%28w%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C_\sigma(w)' title='C_\sigma(w)' class='latex' /> to be the number of copies of <img src='http://l.wordpress.com/latex.php?latex=%5Csigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sigma' title='\sigma' class='latex' /> in <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' />. If <img src='http://l.wordpress.com/latex.php?latex=%5Coverline%7Bw%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\overline{w}' title='\overline{w}' class='latex' /> denotes the corresponding element of <img src='http://l.wordpress.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F' title='F' class='latex' />, define <img src='http://l.wordpress.com/latex.php?latex=C_%5Csigma%28%5Coverline%7Bw%7D%29+%3D+C_%5Csigma%28w%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C_\sigma(\overline{w}) = C_\sigma(w)' title='C_\sigma(\overline{w}) = C_\sigma(w)' class='latex' /> (note this is well-defined, since each element of a free group has a unique reduced representative). Then define <img src='http://l.wordpress.com/latex.php?latex=H_%5Csigma+%3D+C_%5Csigma+-+C_%7B%5Csigma%5E%7B-1%7D%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H_\sigma = C_\sigma - C_{\sigma^{-1}}' title='H_\sigma = C_\sigma - C_{\sigma^{-1}}' class='latex' />. This quasimorphism is not yet homogeneous, but can be homogenized as above (this example is due to <a href="http://www.ams.org/mathscinet-getitem?mr=0624804">Brooks</a>).</li>
<li>Let <img src='http://l.wordpress.com/latex.php?latex=M&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='M' title='M' class='latex' /> be a closed hyperbolic manifold, and let <img src='http://l.wordpress.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha' title='\alpha' class='latex' /> be a <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />-form. For each <img src='http://l.wordpress.com/latex.php?latex=g+%5Cin+%5Cpi_1%28M%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g \in \pi_1(M)' title='g \in \pi_1(M)' class='latex' /> let <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma_g&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma_g' title='\gamma_g' class='latex' /> be the geodesic representative in the free homotopy class of <img src='http://l.wordpress.com/latex.php?latex=g&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g' title='g' class='latex' />. Then define <img src='http://l.wordpress.com/latex.php?latex=%5Cphi_%5Calpha%28g%29+%3D+%5Cint_%7B%5Cgamma_g%7D+%5Calpha&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi_\alpha(g) = \int_{\gamma_g} \alpha' title='\phi_\alpha(g) = \int_{\gamma_g} \alpha' class='latex' />. By Stokes&#8217; theorem, and some basic hyperbolic geometry, <img src='http://l.wordpress.com/latex.php?latex=%5Cphi_%5Calpha&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi_\alpha' title='\phi_\alpha' class='latex' /> is a homogeneous quasimorphism with defect at most <img src='http://l.wordpress.com/latex.php?latex=2%5Cpi+%5C%26%23124%3Bd%5Calpha%5C%26%23124%3B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='2\pi \&#124;d\alpha\&#124;' title='2\pi \&#124;d\alpha\&#124;' class='latex' />.</li>
<li>Let <img src='http://l.wordpress.com/latex.php?latex=%5Crho%3A+G+%5Cto+%5Ctext%7BHomeo%7D%5E%2B%28S%5E1%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\rho: G \to \text{Homeo}^+(S^1)' title='\rho: G \to \text{Homeo}^+(S^1)' class='latex' /> be an orientation-preserving action of <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> on a circle. The group of homeomorphisms of the circle has a natural central extension <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7BHomeo%7D%5E%2B%28%5Cbf%7BR%7D%29%5E%7B%5Cbf%7BZ%7D%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{Homeo}^+(\bf{R})^{\bf{Z}}' title='\text{Homeo}^+(\bf{R})^{\bf{Z}}' class='latex' />, the group of homeomorphisms of <img src='http://l.wordpress.com/latex.php?latex=%5Cbf%7BR%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\bf{R}' title='\bf{R}' class='latex' /> that commute with integer translation. The preimage of <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> in this extension is an extension <img src='http://l.wordpress.com/latex.php?latex=%5Cwidehat%7BG%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\widehat{G}' title='\widehat{G}' class='latex' />. Given <img src='http://l.wordpress.com/latex.php?latex=g+%5Cin+%5Ctext%7BHomeo%7D%5E%2B%28%5Cbf%7BR%7D%29%5E%7B%5Cbf%7BZ%7D%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g \in \text{Homeo}^+(\bf{R})^{\bf{Z}}' title='g \in \text{Homeo}^+(\bf{R})^{\bf{Z}}' class='latex' />, define <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Brot%7D%28g%29+%3D+%5Clim_%7Bn+%5Cto+%5Cinfty%7D+%28g%5En%280%29+-+0%29%2Fn&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{rot}(g) = \lim_{n \to \infty} (g^n(0) - 0)/n' title='\text{rot}(g) = \lim_{n \to \infty} (g^n(0) - 0)/n' class='latex' />; this descends to a <img src='http://l.wordpress.com/latex.php?latex=%5Cbf%7BR%7D%2F%5Cbf%7BZ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\bf{R}/\bf{Z}' title='\bf{R}/\bf{Z}' class='latex' />-valued function on <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7BHomeo%7D%5E%2B%28S%5E1%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{Homeo}^+(S^1)' title='\text{Homeo}^+(S^1)' class='latex' />, Poincare&#8217;s so-called rotation number. But on <img src='http://l.wordpress.com/latex.php?latex=%5Cwidehat%7BG%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\widehat{G}' title='\widehat{G}' class='latex' />, this function is a homogeneous quasimorphism, typically with defect <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />.</li>
<li>Similarly, the group <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7BSp%7D%282n%2C%5Cbf%7BR%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{Sp}(2n,\bf{R})' title='\text{Sp}(2n,\bf{R})' class='latex' /> has a universal cover <img src='http://l.wordpress.com/latex.php?latex=%5Cwidetilde%7B%5Ctext%7BSp%7D%7D%282n%2C%5Cbf%7BR%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\widetilde{\text{Sp}}(2n,\bf{R})' title='\widetilde{\text{Sp}}(2n,\bf{R})' class='latex' /> with deck group <img src='http://l.wordpress.com/latex.php?latex=%5Cbf%7BZ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\bf{Z}' title='\bf{Z}' class='latex' />. The symplectic group acts on the space <img src='http://l.wordpress.com/latex.php?latex=%5CLambda_n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Lambda_n' title='\Lambda_n' class='latex' /> of Lagrangian subspaces in <img src='http://l.wordpress.com/latex.php?latex=%5Cbf%7BR%7D%5E%7B2n%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\bf{R}^{2n}' title='\bf{R}^{2n}' class='latex' />. This is equal to the coset space <img src='http://l.wordpress.com/latex.php?latex=%5CLambda_n+%3D+U%28n%29%2FO%28n%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Lambda_n = U(n)/O(n)' title='\Lambda_n = U(n)/O(n)' class='latex' />, and we can therefore define a function <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bdet%7D%5E2%3A%5CLambda_n+%5Cto+S%5E1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{det}^2:\Lambda_n \to S^1' title='\text{det}^2:\Lambda_n \to S^1' class='latex' />. After picking a basepoint, one obtains an <img src='http://l.wordpress.com/latex.php?latex=S%5E1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S^1' title='S^1' class='latex' />-valued function on the symplectic group, which lifts to a real-valued function on its universal cover. This function is a quasimorphism on the covering group, whose homogenization is sometimes called the <em>symplectic rotation number</em>; see e.g. <a href="http://www.ams.org/mathscinet-getitem?mr=1183404">Barge-Ghys</a>.</li>
</ol>
<p>Quasimorphisms and stable commutator length are related by Bavard Duality:</p>
<p><strong>Theorem (Bavard duality):</strong> Let <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> be a group, and let <img src='http://l.wordpress.com/latex.php?latex=%5Csum+t_i+g_i+%5Cin+B_1%5EH%28G%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sum t_i g_i \in B_1^H(G)' title='\sum t_i g_i \in B_1^H(G)' class='latex' />. Then there is an equality <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D%28%5Csum+t_i+g_i%29+%3D+%5Csup_%5Cphi+%5Csum+t_i+%5Cphi%28g_i%29%2F2D%28%5Cphi%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}(\sum t_i g_i) = \sup_\phi \sum t_i \phi(g_i)/2D(\phi)' title='\text{scl}(\sum t_i g_i) = \sup_\phi \sum t_i \phi(g_i)/2D(\phi)' class='latex' /> where the supremum is taken over all homogeneous quasimorphisms.</p>
<p>This duality theorem shows that <img src='http://l.wordpress.com/latex.php?latex=Q%2FH%5E1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Q/H^1' title='Q/H^1' class='latex' /> with the defect norm is the dual of <img src='http://l.wordpress.com/latex.php?latex=B_1%5EH&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='B_1^H' title='B_1^H' class='latex' /> with the <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}' title='\text{scl}' class='latex' /> norm. (this theorem is proved for elements <img src='http://l.wordpress.com/latex.php?latex=g+%5Cin+%5BG%2CG%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g \in [G,G]' title='g \in [G,G]' class='latex' /> by <a href="http://www.ams.org/mathscinet-getitem?mr=1115747">Bavard</a>, and in generality in <a href="http://www.its.caltech.edu/~dannyc/scl/toc.html">my monograph</a>, which is a reference for the content of this post.)</p>
<p>What does this have to do with rigidity (or, for that matter, immersions)? Well, one sees from the examples (and many others) that homogeneous quasimorphisms arise from geometry &#8212; specifically, from <em>hyperbolic geometry</em> (negative curvature) and <em>symplectic geometry</em> (causal structures). One expects to find rigidity in extremal circumstances, and therefore one wants to understand, for a given chain <img src='http://l.wordpress.com/latex.php?latex=C+%5Cin+B_1%5EH%28G%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C \in B_1^H(G)' title='C \in B_1^H(G)' class='latex' />, the set of extremal quasimorphisms for <img src='http://l.wordpress.com/latex.php?latex=C&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C' title='C' class='latex' />, i.e. those homogeneous quasimorphisms <img src='http://l.wordpress.com/latex.php?latex=%5Cphi&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi' title='\phi' class='latex' /> satisfying <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D%28C%29+%3D+%5Cphi%28C%29%2F2D%28%5Cphi%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}(C) = \phi(C)/2D(\phi)' title='\text{scl}(C) = \phi(C)/2D(\phi)' class='latex' />. By the duality theorem, the space of such extremal quasimorphisms are a nonempty closed convex cone, dual to the set of hyperplanes in <img src='http://l.wordpress.com/latex.php?latex=B_1%5EH&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='B_1^H' title='B_1^H' class='latex' /> that contain <img src='http://l.wordpress.com/latex.php?latex=C%2F%26%23124%3BC%26%23124%3B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C/&#124;C&#124;' title='C/&#124;C&#124;' class='latex' /> and support the unit ball of the <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}' title='\text{scl}' class='latex' /> norm. The fewer supporting hyperplanes, the smaller the set of extremal quasimorphisms for <img src='http://l.wordpress.com/latex.php?latex=C&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C' title='C' class='latex' />, and the more rigid such extremal quasimorphisms will be.</p>
<p>When <img src='http://l.wordpress.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F' title='F' class='latex' /> is a free group, the unit ball in the <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}' title='\text{scl}' class='latex' /> norm in <img src='http://l.wordpress.com/latex.php?latex=B_1%5EH%28F%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='B_1^H(F)' title='B_1^H(F)' class='latex' /> is a rational polyhedron. Every nonzero chain <img src='http://l.wordpress.com/latex.php?latex=C+%5Cin+B_1%5EH%28F%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C \in B_1^H(F)' title='C \in B_1^H(F)' class='latex' /> has a nonzero multiple <img src='http://l.wordpress.com/latex.php?latex=C%2F%26%23124%3BC%26%23124%3B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C/&#124;C&#124;' title='C/&#124;C&#124;' class='latex' /> contained in the boundary of this polyhedron; let <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_C&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_C' title='\pi_C' class='latex' /> denote the face of the polyhedron containing this multiple in its interior. The smaller the codimension of <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_C&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_C' title='\pi_C' class='latex' />, the smaller the dimension of the cone of extremal quasimorphisms for <img src='http://l.wordpress.com/latex.php?latex=C&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C' title='C' class='latex' />, and the more rigidity we will see. The best circumstance is when <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_C&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_C' title='\pi_C' class='latex' /> has codimension one, and an extremal quasimorphism for <img src='http://l.wordpress.com/latex.php?latex=C&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C' title='C' class='latex' /> is unique, up to scale, and elements of <img src='http://l.wordpress.com/latex.php?latex=H%5E1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H^1' title='H^1' class='latex' />.</p>
<p>An infinite dimensional polyhedron need not necessarily have any top dimensional faces; thus it is natural to ask: does the unit ball in <img src='http://l.wordpress.com/latex.php?latex=B_1%5EH%28F%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='B_1^H(F)' title='B_1^H(F)' class='latex' /> have any top dimensional faces? and can one say anything about their geometric meaning? We have now done enough to motivate the following, which is the main theorem from my paper &#8220;<a href="http://arxiv.org/abs/0807.0395">Faces of the scl norm ball</a>&#8221;:</p>
<p><strong>Theorem:</strong> Let <img src='http://l.wordpress.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F' title='F' class='latex' /> be a free group. For every isomorphism <img src='http://l.wordpress.com/latex.php?latex=F+%5Cto+%5Cpi_1%28%5CSigma%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F \to \pi_1(\Sigma)' title='F \to \pi_1(\Sigma)' class='latex' /> (up to conjugacy) where <img src='http://l.wordpress.com/latex.php?latex=%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Sigma' title='\Sigma' class='latex' /> is a compact oriented surface, there is a well-defined chain <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+%5CSigma+%5Cin+B_1%5EH%28F%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial \Sigma \in B_1^H(F)' title='\partial \Sigma \in B_1^H(F)' class='latex' />. This satisfies the following properties:</p>
<ol>
<li>The projective class of <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial \Sigma' title='\partial \Sigma' class='latex' /> intersects the interior of a codimension one face <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_\Sigma' title='\pi_\Sigma' class='latex' /> of the <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}' title='\text{scl}' class='latex' /> norm ball</li>
<li>The unique extremal quasimorphism dual to <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_\Sigma' title='\pi_\Sigma' class='latex' /> (up to scale and elements of <img src='http://l.wordpress.com/latex.php?latex=H%5E1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H^1' title='H^1' class='latex' />) is the rotation quasimorphism <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Brot%7D_%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{rot}_\Sigma' title='\text{rot}_\Sigma' class='latex' /> (to be defined below) associated to any complete hyperbolic structure on <img src='http://l.wordpress.com/latex.php?latex=%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Sigma' title='\Sigma' class='latex' /></li>
<li>A homologically trivial geodesic <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />-manifold <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> in <img src='http://l.wordpress.com/latex.php?latex=%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Sigma' title='\Sigma' class='latex' /> is virtually bounded by an immersed surface <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> in <img src='http://l.wordpress.com/latex.php?latex=%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Sigma' title='\Sigma' class='latex' /> if and only if the projective class of <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> (thought of as an element of <img src='http://l.wordpress.com/latex.php?latex=B_1%5EH%28F%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='B_1^H(F)' title='B_1^H(F)' class='latex' />) intersects <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_\Sigma' title='\pi_\Sigma' class='latex' />. Equivalently, if and only if <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Brot%7D_%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{rot}_\Sigma' title='\text{rot}_\Sigma' class='latex' /> is extremal for <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' />. Equivalently, if and only if <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D%28%5CGamma%29+%3D+%5Ctext%7Brot%7D_%5CSigma%28%5CGamma%29%2F2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}(\Gamma) = \text{rot}_\Sigma(\Gamma)/2' title='\text{scl}(\Gamma) = \text{rot}_\Sigma(\Gamma)/2' class='latex' />.</li>
</ol>
<p>It remains to give a definition of <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Brot%7D_%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{rot}_\Sigma' title='\text{rot}_\Sigma' class='latex' />. In fact, we give two definitions.</p>
<p>First, a hyperbolic structure on <img src='http://l.wordpress.com/latex.php?latex=%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Sigma' title='\Sigma' class='latex' /> and the isomorphism <img src='http://l.wordpress.com/latex.php?latex=F%5Cto+%5Cpi_1%28%5CSigma%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F\to \pi_1(\Sigma)' title='F\to \pi_1(\Sigma)' class='latex' /> determines a representation <img src='http://l.wordpress.com/latex.php?latex=F+%5Cto+%5Ctext%7BPSL%7D%282%2C%5Cbf%7BR%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F \to \text{PSL}(2,\bf{R})' title='F \to \text{PSL}(2,\bf{R})' class='latex' />. This lifts to <img src='http://l.wordpress.com/latex.php?latex=%5Cwidetilde%7B%5Ctext%7BSL%7D%7D%282%2C%5Cbf%7BR%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\widetilde{\text{SL}}(2,\bf{R})' title='\widetilde{\text{SL}}(2,\bf{R})' class='latex' />, since <img src='http://l.wordpress.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F' title='F' class='latex' /> is free. The composition with rotation number is a homogeneous quasimorphism on <img src='http://l.wordpress.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F' title='F' class='latex' />, well-defined up to <img src='http://l.wordpress.com/latex.php?latex=H%5E1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H^1' title='H^1' class='latex' />. Note that because the image in <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7BPSL%7D%282%2C%5Cbf%7BR%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{PSL}(2,\bf{R})' title='\text{PSL}(2,\bf{R})' class='latex' /> is discrete and torsion-free, this quasimorphism is integer valued (and has defect <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />). This quasimorphism is <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Brot%7D_%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{rot}_\Sigma' title='\text{rot}_\Sigma' class='latex' />.</p>
<p>Second, a geodesic <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />-manifold <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> in <img src='http://l.wordpress.com/latex.php?latex=%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Sigma' title='\Sigma' class='latex' /> cuts the surface up into regions <img src='http://l.wordpress.com/latex.php?latex=R_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='R_i' title='R_i' class='latex' />. For each such region, let <img src='http://l.wordpress.com/latex.php?latex=%5Calpha_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha_i' title='\alpha_i' class='latex' /> be an arc transverse to <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' />, joining <img src='http://l.wordpress.com/latex.php?latex=R_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='R_i' title='R_i' class='latex' /> to <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial \Sigma' title='\partial \Sigma' class='latex' />. Let <img src='http://l.wordpress.com/latex.php?latex=%28%5Calpha_i+%5Ccap+%5CGamma%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(\alpha_i \cap \Gamma)' title='(\alpha_i \cap \Gamma)' class='latex' /> denote the homological (signed) intersection number. Then define <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Brot%7D_%5CSigma%28%5CGamma%29+%3D+1%2F2%5Cpi+%5Csum_i+%28%5Calpha_i+%5Ccap+%5CGamma%29+%5Ctext%7Barea%7D%28R_i%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{rot}_\Sigma(\Gamma) = 1/2\pi \sum_i (\alpha_i \cap \Gamma) \text{area}(R_i)' title='\text{rot}_\Sigma(\Gamma) = 1/2\pi \sum_i (\alpha_i \cap \Gamma) \text{area}(R_i)' class='latex' />.</p>
<p>We now show how 3 follows. Given <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' />, we compute <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D%28%5CGamma%29+%3D+%5Cinf_S+-%5Cchi%5E-%28S%29%2F2n%28S%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}(\Gamma) = \inf_S -\chi^-(S)/2n(S)' title='\text{scl}(\Gamma) = \inf_S -\chi^-(S)/2n(S)' class='latex' /> as above. Let <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> be such a surface, mapping to <img src='http://l.wordpress.com/latex.php?latex=%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Sigma' title='\Sigma' class='latex' />. We adjust the map by a homotopy so that it is <em>pleated</em>; i.e. so that <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> is itself a hyperbolic surface, decomposed into ideal triangles, in such a way that the map is a (possibly orientation-reversing) isometry on each ideal triangle. By Gauss-Bonnet, we can calculate <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Barea%7D%28S%29+%3D+-2%5Cpi+%5Cchi%5E-%28S%29+%3D+%5Cpi+%5Csum_%5CDelta+1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{area}(S) = -2\pi \chi^-(S) = \pi \sum_\Delta 1' title='\text{area}(S) = -2\pi \chi^-(S) = \pi \sum_\Delta 1' class='latex' />. On the other hand, <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial S' title='\partial S' class='latex' /> wraps <img src='http://l.wordpress.com/latex.php?latex=n%28S%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n(S)' title='n(S)' class='latex' /> times around <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> (homologically) so <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Brot%7D_%5CSigma%28%5CGamma%29+%3D+%5Cpi%2F2%5Cpi+n%28S%29+%5Csum_%5CDelta+%5Cpm+1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{rot}_\Sigma(\Gamma) = \pi/2\pi n(S) \sum_\Delta \pm 1' title='\text{rot}_\Sigma(\Gamma) = \pi/2\pi n(S) \sum_\Delta \pm 1' class='latex' /> where the sign in each case depends on whether the ideal triangle <img src='http://l.wordpress.com/latex.php?latex=%5CDelta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Delta' title='\Delta' class='latex' /> is mapped in with positive or negative orientation. Consequently <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Brot%7D_%5CSigma%28%5CGamma%29%2F2+%5Cle+-%5Cchi%5E-%28S%29%2F2n%28S%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{rot}_\Sigma(\Gamma)/2 \le -\chi^-(S)/2n(S)' title='\text{rot}_\Sigma(\Gamma)/2 \le -\chi^-(S)/2n(S)' class='latex' /> with equality if and only if the sign of every triangle is <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />. This holds if and only if the map <img src='http://l.wordpress.com/latex.php?latex=S+%5Cto+%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S \to \Sigma' title='S \to \Sigma' class='latex' /> is an immersion; on the other hand, equality holds if and only if <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Brot%7D_%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{rot}_\Sigma' title='\text{rot}_\Sigma' class='latex' /> is extremal for <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' />. This proves part 3 of the theorem above.</p>
<p>Incidentally, this fact gives a fast algorithm to determine whether <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> is the virtual boundary of an immersed surface. Stable commutator length in free groups can be computed in polynomial time in word length; likewise, the value of <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Brot%7D_%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{rot}_\Sigma' title='\text{rot}_\Sigma' class='latex' /> can be computed in polynomial time (see section 4.2 of my monograph for details). So one can determine whether <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> projectively intersects <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_\Sigma' title='\pi_\Sigma' class='latex' />, and therefore whether it is the virtual boundary of an immersed surface. In fact, these algorithms are quite practical, and run quickly (in a matter of seconds) on words of length 60 and longer in <img src='http://l.wordpress.com/latex.php?latex=F_2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F_2' title='F_2' class='latex' />.</p>
<p>One application to rigidity is a new proof of the following theorem:</p>
<p><strong>Corollary (Goldman, <a href="http://arxiv.org/abs/math/0605656">Burger-Iozzi-Wienhard</a>):</strong> Let <img src='http://l.wordpress.com/latex.php?latex=%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Sigma' title='\Sigma' class='latex' /> be a closed oriented surface of positive genus, and <img src='http://l.wordpress.com/latex.php?latex=%5Crho%3A%5Cpi_1%28%5CSigma%29+%5Cto+%5Ctext%7BSp%7D%282n%2C%5Cbf%7BR%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\rho:\pi_1(\Sigma) \to \text{Sp}(2n,\bf{R})' title='\rho:\pi_1(\Sigma) \to \text{Sp}(2n,\bf{R})' class='latex' /> a Zariski dense representation. Let <img src='http://l.wordpress.com/latex.php?latex=e_%5Crho+%5Cin+H%5E2%28%5CSigma%3B%5Cmathbb%7BZ%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='e_\rho \in H^2(\Sigma;\mathbb{Z})' title='e_\rho \in H^2(\Sigma;\mathbb{Z})' class='latex' /> be the Euler class associated to the action. Suppose that <img src='http://l.wordpress.com/latex.php?latex=%26%23124%3Be_%5Crho%28%5B%5CSigma%5D%29%26%23124%3B+%3D+-n%5Cchi%28%5CSigma%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='&#124;e_\rho([\Sigma])&#124; = -n\chi(\Sigma)' title='&#124;e_\rho([\Sigma])&#124; = -n\chi(\Sigma)' class='latex' /> (note: by a theorem of <a href="http://www.ams.org/mathscinet-getitem?mr=0875338">Domic and Toledo</a>, one always has <img src='http://l.wordpress.com/latex.php?latex=%26%23124%3Be_%5Crho%28%5B%5CSigma%5D%29%26%23124%3B+%5Cle+-n%5Cchi%28%5CSigma%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='&#124;e_\rho([\Sigma])&#124; \le -n\chi(\Sigma)' title='&#124;e_\rho([\Sigma])&#124; \le -n\chi(\Sigma)' class='latex' />). Then <img src='http://l.wordpress.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\rho' title='\rho' class='latex' /> is discrete.</p>
<p>Here <img src='http://l.wordpress.com/latex.php?latex=e_%5Crho&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='e_\rho' title='e_\rho' class='latex' /> is the first Chern class of the bundle associated to <img src='http://l.wordpress.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\rho' title='\rho' class='latex' />. The proof is as follows: cut <img src='http://l.wordpress.com/latex.php?latex=%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Sigma' title='\Sigma' class='latex' /> along an essential loop <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' /> into two subsurfaces <img src='http://l.wordpress.com/latex.php?latex=%5CSigma_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Sigma_i' title='\Sigma_i' class='latex' />. One obtains homogeneous quasimorphisms on each group <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_1%28%5CSigma_i%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_1(\Sigma_i)' title='\pi_1(\Sigma_i)' class='latex' /> (i.e. the symplectic rotation number associated to <img src='http://l.wordpress.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\rho' title='\rho' class='latex' />), and the hypothesis of the theorem easily implies that they are extremal for <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+%5CSigma_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial \Sigma_i' title='\partial \Sigma_i' class='latex' />. Consequently the symplectic rotation number is equal to <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Brot%7D_%7B%5CSigma_i%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{rot}_{\Sigma_i}' title='\text{rot}_{\Sigma_i}' class='latex' />, at least on the commutator subgroup. But this latter quasimorphism takes only integral values; it follows that each element in <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_1%28%5CSigma_i%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_1(\Sigma_i)' title='\pi_1(\Sigma_i)' class='latex' /> fixes a Lagrangian subspace under <img src='http://l.wordpress.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\rho' title='\rho' class='latex' />. But this implies that <img src='http://l.wordpress.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\rho' title='\rho' class='latex' /> is not dense, and since it is Zariski dense, it is discrete. (Notes: there are a couple of details under the rug here, but not many; furthermore, the hypothesis that <img src='http://l.wordpress.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\rho' title='\rho' class='latex' /> is Zariski dense is not necessary (but can be derived as a conclusion with more work), and one can just as easily treat representations of compact surface groups as closed ones; finally, Burger-Iozzi-Wienhard prove more than just this statement; for instance, they show that the space of maximal representations is always real semialgebraic, and describe it in some detail).</p>
<p>More abstractly, we have shown that <em>extremal quasimorphisms on</em> <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+%5CSigma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial \Sigma' title='\partial \Sigma' class='latex' /> <em>are unique</em>. In other words, by prescribing the value of a quasimorphism on a single group element, one determines its values on the entire commutator subgroup. If such a quasimorphism arises from some geometric or dynamical context, this can be interpreted as a kind of rigidity theorem, of which the Corollary above is an example.</p>
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<title><![CDATA[scl, sails and surgery]]></title>
<link>http://lamington.wordpress.com/2009/07/23/scl-sails-and-surgery/</link>
<pubDate>Thu, 23 Jul 2009 23:10:32 +0000</pubDate>
<dc:creator>Danny Calegari</dc:creator>
<guid>http://lamington.wordpress.com/2009/07/23/scl-sails-and-surgery/</guid>
<description><![CDATA[I have just uploaded a paper to the arXiv, entitled &#8220;Scl, sails and surgery&#8221;. The paper ]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p>I have just uploaded a paper to the arXiv, entitled &#8220;<a href="http://arxiv.org/abs/0907.3541">Scl, sails and surgery</a>&#8221;. The paper discusses a connection between stable commutator length in free groups and the geometry of sails. This is an interesting example of what sometimes happens in geometry, where a complicated topological problem in low dimensions can be translated into a &#8220;simple&#8221; geometric problem in high dimensions. Other examples include the Veronese embedding in Algebraic geometry (i.e. the embedding of one projective space into another taking a point with homogeneous co-ordinates <img src='http://l.wordpress.com/latex.php?latex=x_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='x_i' title='x_i' class='latex' /> to the point whose homogeneous co-ordinates are the monomials of some fixed degree in the <img src='http://l.wordpress.com/latex.php?latex=x_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='x_i' title='x_i' class='latex' />), which lets one exhibit any projective variety as an intersection of a Veronese variety (whose geometry is understood very well) with a linear subspace.</p>
<p>In my paper, the fundamental problem is to compute stable commutator length in free groups, and more generally in free products of Abelian groups. Let&#8217;s focus on the case of a group <img src='http://l.wordpress.com/latex.php?latex=G+%3D+A%2AB&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G = A*B' title='G = A*B' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=A%2CB&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='A,B' title='A,B' class='latex' /> are free abelian of finite rank. A <img src='http://l.wordpress.com/latex.php?latex=K%28G%2C1%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K(G,1)' title='K(G,1)' class='latex' /> is just a wedge <img src='http://l.wordpress.com/latex.php?latex=X%3A%3DK_A+%5Cvee+K_B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X:=K_A \vee K_B' title='X:=K_A \vee K_B' class='latex' /> of tori of dimension equal to the ranks of <img src='http://l.wordpress.com/latex.php?latex=A%2CB&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='A,B' title='A,B' class='latex' />. Let <img src='http://l.wordpress.com/latex.php?latex=%5CGamma%3A+%5Ccoprod_i+S%5E1+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma: \coprod_i S^1 \to X' title='\Gamma: \coprod_i S^1 \to X' class='latex' /> be a free homotopy class of <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />-manifold in <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' />, which is homologically trivial. Formally, we can think of <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> as a chain <img src='http://l.wordpress.com/latex.php?latex=%5Csum_i+g_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sum_i g_i' title='\sum_i g_i' class='latex' /> in <img src='http://l.wordpress.com/latex.php?latex=B_1%5EH%28G%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='B_1^H(G)' title='B_1^H(G)' class='latex' />, the vector space of group <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />-boundaries, modulo homogenization; i.e. quotiented by the subspace spanned by chains of the form <img src='http://l.wordpress.com/latex.php?latex=g%5En+-+ng&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g^n - ng' title='g^n - ng' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=g-hgh%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g-hgh^{-1}' title='g-hgh^{-1}' class='latex' />. One wants to find the simplest surface <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> mapping to <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' /> that rationally bounds <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' />. I.e. we want to find a map <img src='http://l.wordpress.com/latex.php?latex=f%3AS+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f:S \to X' title='f:S \to X' class='latex' /> such that <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+f%3A%5Cpartial+S+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial f:\partial S \to X' title='\partial f:\partial S \to X' class='latex' /> factors through <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' />, and so that the boundary <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial S' title='\partial S' class='latex' /> wraps homologically <img src='http://l.wordpress.com/latex.php?latex=n%28S%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n(S)' title='n(S)' class='latex' /> times around each loop of <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' />, in such a way as to infimize <img src='http://l.wordpress.com/latex.php?latex=-%5Cchi%28S%29%2F2n%28S%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-\chi(S)/2n(S)' title='-\chi(S)/2n(S)' class='latex' />. This infimum, over all maps of all surfaces <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> of all possible genus, is the <em>stable commutator length</em> of the chain <img src='http://l.wordpress.com/latex.php?latex=%5Csum_i+g_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sum_i g_i' title='\sum_i g_i' class='latex' />. Computing this quantity for all such finite chains is tantamount to understanding the bounded cohomology of a free group in dimension <img src='http://l.wordpress.com/latex.php?latex=2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='2' title='2' class='latex' />.</p>
<p>Given such a surface <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' />, one can cut it up into simpler pieces, along the preimage of the basepoint <img src='http://l.wordpress.com/latex.php?latex=K_A+%5Ccap+K_B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K_A \cap K_B' title='K_A \cap K_B' class='latex' />. Since <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> is a surface with boundary, these simpler pieces are surfaces with <em>corners</em>. In general, understanding how a surface can be assembled from an abstract collection of surfaces with corners is a hopeless task. When one tries to glue the pieces back together, one runs into trouble at the corners &#8212; how does one decide when a collection of surfaces &#8220;closes up&#8221; around a corner? The wrong decision leads to branch points; moreover, a decision made at one corner will propogate along an edge and lead to constraints on the choices one can make at other corners. This problem arises again and again in low-dimensional topology, and has several different (and not always equivalent) formulations and guises, including -</p>
<ul>
<li>Given an abstract branched surface and a weight on that surface, when is there an unbranched surface carried by the abstract branched surface and realizing the weight?</li>
<li>Given a triangulation of a <img src='http://l.wordpress.com/latex.php?latex=3&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='3' title='3' class='latex' />-manifold and a collection of normal surface types in each simplex satisfying the gluing constraints but *not*  necessarily satisfying the quadrilateral condition (i.e. there might be more than one quadrilateral type per simplex), when is there an immersed unbranched normal surface in the manifold realizing the weight?</li>
<li>Given an immersed curve in the plane, when is there an immersion from the disk to the plane whose boundary is the given curve?</li>
<li>Given a polyhedral surface (arising e.g. in computer graphics), how can one choose smooth approximations of the polygonal faces that mesh smoothly at the vertices?</li>
</ul>
<p>I think of all these problems as examples of what I like to call the <em>holonomy problem</em>, since all of them can be reduced, in one way or another, to studying representations of fundamental groups of punctured surfaces into finite groups. The fortunate &#8220;accident&#8221; in this case is that every corner arises by intersecting a cut with a boundary edge of <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' />. Consequently, one never wants to glue more than two pieces up at any corner, and the holonomy problem does not arise. Hence in principle, to understand the surface <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> one just needs to understand the pieces of <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> that can arise by cutting, and the ways in which they can be reassembled.</p>
<p>This is still not a complete solution of the problem, since infinitely many kinds of pieces can arise by cutting complicated surfaces <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' />. The <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />-manifold <img src='http://l.wordpress.com/latex.php?latex=%5CGamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\Gamma' title='\Gamma' class='latex' /> decomposes into a collection of arcs in the tori <img src='http://l.wordpress.com/latex.php?latex=K_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K_A' title='K_A' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=K_B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K_B' title='K_B' class='latex' /> which we denote <img src='http://l.wordpress.com/latex.php?latex=%5Ctau_A%2C%5Ctau_B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tau_A,\tau_B' title='\tau_A,\tau_B' class='latex' /> respectively, and the surface <img src='http://l.wordpress.com/latex.php?latex=S+%5Ccap+K_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S \cap K_A' title='S \cap K_A' class='latex' /> (hereafter abbreviated to <img src='http://l.wordpress.com/latex.php?latex=S_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S_A' title='S_A' class='latex' />) has edges that alternate between elements of <img src='http://l.wordpress.com/latex.php?latex=%5Ctau_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tau_A' title='\tau_A' class='latex' />, and edges mapping to <img src='http://l.wordpress.com/latex.php?latex=K_A+%5Ccap+K_B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K_A \cap K_B' title='K_A \cap K_B' class='latex' />. Since <img src='http://l.wordpress.com/latex.php?latex=K_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K_A' title='K_A' class='latex' /> is a torus, handles of <img src='http://l.wordpress.com/latex.php?latex=S_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S_A' title='S_A' class='latex' /> mapping to <img src='http://l.wordpress.com/latex.php?latex=K_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K_A' title='K_A' class='latex' /> can be compressed, reducing the complexity of <img src='http://l.wordpress.com/latex.php?latex=S_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S_A' title='S_A' class='latex' />, and thereby <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' />, so one need only consider <em>planar</em> surfaces <img src='http://l.wordpress.com/latex.php?latex=S_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S_A' title='S_A' class='latex' />.</p>
<p>Let <img src='http://l.wordpress.com/latex.php?latex=C_2%28A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C_2(A)' title='C_2(A)' class='latex' /> denote the real vector space with basis the set of ordered pairs <img src='http://l.wordpress.com/latex.php?latex=%28t%2Ct%27%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(t,t&#039;)' title='(t,t&#039;)' class='latex' /> of elements of <img src='http://l.wordpress.com/latex.php?latex=%5Ctau_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tau_A' title='\tau_A' class='latex' /> (not necessarily distinct), and <img src='http://l.wordpress.com/latex.php?latex=C_1%28A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C_1(A)' title='C_1(A)' class='latex' /> the real vector space with basis the elements of <img src='http://l.wordpress.com/latex.php?latex=%5Ctau_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\tau_A' title='\tau_A' class='latex' />. A surface <img src='http://l.wordpress.com/latex.php?latex=S_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S_A' title='S_A' class='latex' /> determines a non-negative integral vector <img src='http://l.wordpress.com/latex.php?latex=v%28S_A%29+%5Cin+C_2%28A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v(S_A) \in C_2(A)' title='v(S_A) \in C_2(A)' class='latex' />, by counting the number of times a given pair of edges <img src='http://l.wordpress.com/latex.php?latex=%28t%2Ct%27%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(t,t&#039;)' title='(t,t&#039;)' class='latex' /> appear in succession on one of the (oriented) boundary components of <img src='http://l.wordpress.com/latex.php?latex=S_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S_A' title='S_A' class='latex' />. The vector <img src='http://l.wordpress.com/latex.php?latex=v%28S_A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v(S_A)' title='v(S_A)' class='latex' /> satisfies two linear constraints. First, there is a map <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial%3A+C_2%28A%29+%5Cto+C_1%28A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial: C_2(A) \to C_1(A)' title='\partial: C_2(A) \to C_1(A)' class='latex' /> defined on a basis vector by <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial%28t%2Ct%27%29+%3D+t+-+t%27&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial(t,t&#039;) = t - t&#039;' title='\partial(t,t&#039;) = t - t&#039;' class='latex' />. The vector <img src='http://l.wordpress.com/latex.php?latex=v%28S_A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v(S_A)' title='v(S_A)' class='latex' /> satisfies <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+v%28S_A%29+%3D+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial v(S_A) = 0' title='\partial v(S_A) = 0' class='latex' />. Second, each element <img src='http://l.wordpress.com/latex.php?latex=t+%5Cin+%5Ctau_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='t \in \tau_A' title='t \in \tau_A' class='latex' /> is a based loop in <img src='http://l.wordpress.com/latex.php?latex=K_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K_A' title='K_A' class='latex' />, and therefore corresponds to an element in the free abelian group <img src='http://l.wordpress.com/latex.php?latex=A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='A' title='A' class='latex' />. Define <img src='http://l.wordpress.com/latex.php?latex=h%3AC_2%28A%29+%5Cto+A+%5Cotimes+%5Cmathbb%7BR%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='h:C_2(A) \to A \otimes \mathbb{R}' title='h:C_2(A) \to A \otimes \mathbb{R}' class='latex' /> on a basis vector by <img src='http://l.wordpress.com/latex.php?latex=h%28t%2Ct%27%29+%3D+t%2Bt%27&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='h(t,t&#039;) = t+t&#039;' title='h(t,t&#039;) = t+t&#039;' class='latex' /> (warning: the notation obscures the fact that <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial' title='\partial' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=h&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='h' title='h' class='latex' /> map to quite different vector spaces). Then <img src='http://l.wordpress.com/latex.php?latex=h+v%28S_A%29%3D0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='h v(S_A)=0' title='h v(S_A)=0' class='latex' />; moreover, a non-negative rational vector <img src='http://l.wordpress.com/latex.php?latex=v+%5Cin+C_2%28A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v \in C_2(A)' title='v \in C_2(A)' class='latex' /> satisfying <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+v+%3D+h+v+%3D+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial v = h v = 0' title='\partial v = h v = 0' class='latex' /> has a multiple of the form <img src='http://l.wordpress.com/latex.php?latex=v%28S_A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v(S_A)' title='v(S_A)' class='latex' /> for some <img src='http://l.wordpress.com/latex.php?latex=S_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S_A' title='S_A' class='latex' /> as above. Denote the subspace of <img src='http://l.wordpress.com/latex.php?latex=C_2%28A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C_2(A)' title='C_2(A)' class='latex' /> consisting of non-negative vectors in the kernel of <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial' title='\partial' class='latex' /> and <img src='http://l.wordpress.com/latex.php?latex=h&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='h' title='h' class='latex' /> by <img src='http://l.wordpress.com/latex.php?latex=V_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V_A' title='V_A' class='latex' />. This is a rational polyhedral cone &#8212; i.e. a cone with finitely many extremal rays, each spanned by a rational vector.</p>
<p>Although every integral <img src='http://l.wordpress.com/latex.php?latex=v+%5Cin+V_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v \in V_A' title='v \in V_A' class='latex' /> is equal to <img src='http://l.wordpress.com/latex.php?latex=v%28S_A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v(S_A)' title='v(S_A)' class='latex' /> for some <img src='http://l.wordpress.com/latex.php?latex=S_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S_A' title='S_A' class='latex' />, many different <img src='http://l.wordpress.com/latex.php?latex=S_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S_A' title='S_A' class='latex' /> correspond to a given <img src='http://l.wordpress.com/latex.php?latex=v&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v' title='v' class='latex' />. Moreover, if we are allowed to consider formal weighted sums of surfaces, then even more possibilities. In order to compute stable commutator length, we must determine, for a given vector <img src='http://l.wordpress.com/latex.php?latex=v+%5Cin+V_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v \in V_A' title='v \in V_A' class='latex' />, an expression <img src='http://l.wordpress.com/latex.php?latex=v+%3D+%5Csum+t_i+v%28S_i%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v = \sum t_i v(S_i)' title='v = \sum t_i v(S_i)' class='latex' /> where the <img src='http://l.wordpress.com/latex.php?latex=t_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='t_i' title='t_i' class='latex' /> are positive real numbers, which minimizes <img src='http://l.wordpress.com/latex.php?latex=%5Csum+-t_i+%5Cchi_o%28S_i%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\sum -t_i \chi_o(S_i)' title='\sum -t_i \chi_o(S_i)' class='latex' />. Here <img src='http://l.wordpress.com/latex.php?latex=%5Cchi_o%28%5Ccdot%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\chi_o(\cdot)' title='\chi_o(\cdot)' class='latex' /> denotes <em>orbifold</em> Euler characteristic of a surface with corners; each corner contributes <img src='http://l.wordpress.com/latex.php?latex=-1%2F4&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-1/4' title='-1/4' class='latex' /> to <img src='http://l.wordpress.com/latex.php?latex=%5Cchi_o&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\chi_o' title='\chi_o' class='latex' />. The reason one counts complexity using this modified definition is that the result is additive: <img src='http://l.wordpress.com/latex.php?latex=%5Cchi%28S%29+%3D+%5Cchi_o%28S_A%29+%2B+%5Cchi_o%28S_B%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\chi(S) = \chi_o(S_A) + \chi_o(S_B)' title='\chi(S) = \chi_o(S_A) + \chi_o(S_B)' class='latex' />. The contribution to <img src='http://l.wordpress.com/latex.php?latex=%5Cchi_o&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\chi_o' title='\chi_o' class='latex' /> from corners is a linear function on <img src='http://l.wordpress.com/latex.php?latex=V_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V_A' title='V_A' class='latex' />. Moreover, a component <img src='http://l.wordpress.com/latex.php?latex=S_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S_i' title='S_i' class='latex' /> with <img src='http://l.wordpress.com/latex.php?latex=%5Cchi%28S_i%29+%5Cle+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\chi(S_i) \le 0' title='\chi(S_i) \le 0' class='latex' /> can be covered by a surface of high genus and compressed (increasing <img src='http://l.wordpress.com/latex.php?latex=%5Cchi&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\chi' title='\chi' class='latex' />); so such a term can always be replaced by a formal sum <img src='http://l.wordpress.com/latex.php?latex=1%2Fn+S_i%27&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1/n S_i&#039;' title='1/n S_i&#039;' class='latex' /> for which <img src='http://l.wordpress.com/latex.php?latex=%5Cchi%28S_i%27%29+%3D+%5Cchi%28S_i%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\chi(S_i&#039;) = \chi(S_i)' title='\chi(S_i&#039;) = \chi(S_i)' class='latex' />. Thus the only nonlinear contribution to <img src='http://l.wordpress.com/latex.php?latex=%5Cchi_o&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\chi_o' title='\chi_o' class='latex' /> comes from the surfaces <img src='http://l.wordpress.com/latex.php?latex=S_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S_i' title='S_i' class='latex' /> whose underlying topological surface is a <em>disk</em>.</p>
<p>Call a vector <img src='http://l.wordpress.com/latex.php?latex=v+%5Cin+V_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v \in V_A' title='v \in V_A' class='latex' /> a <em>disk vector</em> if <img src='http://l.wordpress.com/latex.php?latex=v+%3D+v%28S_A%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v = v(S_A)' title='v = v(S_A)' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=S_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S_A' title='S_A' class='latex' /> is topologically a disk (with corners). It turns out that the set of disk vectors <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BD%7D_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{D}_A' title='\mathcal{D}_A' class='latex' /> has the following simple form: it is equal to the union of the integer lattice points contained in certain of the open faces of <img src='http://l.wordpress.com/latex.php?latex=V_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V_A' title='V_A' class='latex' /> (those satisfying a combinatorial criterion). Define the <em>sail</em> of <img src='http://l.wordpress.com/latex.php?latex=V_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V_A' title='V_A' class='latex' /> to be equal to the boundary of the convex hull of the polyhedron <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BD%7D_A+%2B+V_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{D}_A + V_A' title='\mathcal{D}_A + V_A' class='latex' /> (where <img src='http://l.wordpress.com/latex.php?latex=%2B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='+' title='+' class='latex' /> here denotes Minkowski sum). The <em>Klein function</em> <img src='http://l.wordpress.com/latex.php?latex=%5Ckappa&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\kappa' title='\kappa' class='latex' /> is the unique continuous function on <img src='http://l.wordpress.com/latex.php?latex=V_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V_A' title='V_A' class='latex' />, linear on rays, that is equal to <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' /> exactly on the sail. Then <img src='http://l.wordpress.com/latex.php?latex=%5Cchi_o%28v%29%3A%3D+%5Cmax+%5Csum+t_i%5Cchi_o%28S_i%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\chi_o(v):= \max \sum t_i\chi_o(S_i)' title='\chi_o(v):= \max \sum t_i\chi_o(S_i)' class='latex' /> over expressions <img src='http://l.wordpress.com/latex.php?latex=v+%3D+%5Csum+t_i+v%28S_i%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v = \sum t_i v(S_i)' title='v = \sum t_i v(S_i)' class='latex' /> satisfies <img src='http://l.wordpress.com/latex.php?latex=%5Cchi_o%28v%29+%3D+%5Ckappa%28v%29+-+%26%23124%3Bv%26%23124%3B%2F2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\chi_o(v) = \kappa(v) - &#124;v&#124;/2' title='\chi_o(v) = \kappa(v) - &#124;v&#124;/2' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=%26%23124%3B%5Ccdot%26%23124%3B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='&#124;\cdot&#124;' title='&#124;\cdot&#124;' class='latex' /> denotes <img src='http://l.wordpress.com/latex.php?latex=L%5E1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='L^1' title='L^1' class='latex' /> norm. To calculate stable commutator length, one minimizes <img src='http://l.wordpress.com/latex.php?latex=-%5Cchi_o%28v%29+-+%5Cchi_o%28v%27%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-\chi_o(v) - \chi_o(v&#039;)' title='-\chi_o(v) - \chi_o(v&#039;)' class='latex' /> over <img src='http://l.wordpress.com/latex.php?latex=%28v%2Cv%27%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='(v,v&#039;)' title='(v,v&#039;)' class='latex' /> contained in a certain rational polyhedron in <img src='http://l.wordpress.com/latex.php?latex=V_A+%5Ctimes+V_B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V_A \times V_B' title='V_A \times V_B' class='latex' />.</p>
<p>Sails are considered elsewhere by several authors; usually, people take <img src='http://l.wordpress.com/latex.php?latex=%5Cmathcal%7BD%7D_A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathcal{D}_A' title='\mathcal{D}_A' class='latex' /> to be the set of all integer vectors except the vertex of the cone, and the sail is therefore the boundary of the convex hull of this (simpler) set. Klein introduced sails as a higher-dimensional generalization of continued fractions: if <img src='http://l.wordpress.com/latex.php?latex=V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V' title='V' class='latex' /> is a polyhedral cone in two dimensions (i.e. a sector in the plane, normalized so that one edge is the horizontal axis, say), the vertices of the sail are the continued fraction approximations of the boundary slope. Arnold has <a href="http://www.ams.org/mathscinet-getitem?mr=1704965">revived</a> the study of such objects in recent years. They arise in many different interesting contexts, such as numerical analysis (especially diophantine approximation) and algebraic number theory. For example, let <img src='http://l.wordpress.com/latex.php?latex=A+%5Cin+%5Ctext%7BSL%7D%28n%2C%5Cmathbb%7BZ%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='A \in \text{SL}(n,\mathbb{Z})' title='A \in \text{SL}(n,\mathbb{Z})' class='latex' /> be a matrix with irreducible characteristic equation, and all eigenvalues real and positive. There is a basis for <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbb%7BR%7D%5En&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbb{R}^n' title='\mathbb{R}^n' class='latex' /> consisting of eigenvalues, spanning a convex cone <img src='http://l.wordpress.com/latex.php?latex=V&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V' title='V' class='latex' />. The cone &#8212; and therefore its sail &#8212; is invariant under <img src='http://l.wordpress.com/latex.php?latex=A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='A' title='A' class='latex' />; moreover, there is a <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbb%7BZ%7D%5E%7Bn-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbb{Z}^{n-1}' title='\mathbb{Z}^{n-1}' class='latex' /> subgroup of <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7BSL%7D%28n%2C%5Cmathbb%7BZ%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{SL}(n,\mathbb{Z})' title='\text{SL}(n,\mathbb{Z})' class='latex' /> consisting of matrices with the same set of eigenvectors; this observation follows from Dirichlet&#8217;s theorem on the units in a number field, and is due to <a href="http://www.ams.org/mathscinet-getitem?mr=0721966">Tsuchihashi</a>. This abelian group acts freely on the sail with quotient a (topological) torus of dimension <img src='http://l.wordpress.com/latex.php?latex=n-1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n-1' title='n-1' class='latex' />, together with a &#8220;canonical&#8221; cell decomposition. This connection between number theory and combinatorics is quite mysterious; for example, Arnold asks: which cell decompositions can arise? This is unknown even in the case <img src='http://l.wordpress.com/latex.php?latex=n%3D3&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n=3' title='n=3' class='latex' />.</p>
<p>The most interesting aspect of this correspondence, between stable commutator length and sails, is that it allows one to introduce <em>parameters</em>. An element in a free group <img src='http://l.wordpress.com/latex.php?latex=F_2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F_2' title='F_2' class='latex' /> can be expressed as a word in letters <img src='http://l.wordpress.com/latex.php?latex=a%2Cb%2Ca%5E%7B-1%7D%2Cb%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a,b,a^{-1},b^{-1}' title='a,b,a^{-1},b^{-1}' class='latex' />, e.g. <img src='http://l.wordpress.com/latex.php?latex=aab%5E%7B-1%7Db%5E%7B-1%7Da%5E%7B-1%7Da%5E%7B-1%7Da%5E%7B-1%7Dbbbbab%5E%7B-1%7Db%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='aab^{-1}b^{-1}a^{-1}a^{-1}a^{-1}bbbbab^{-1}b^{-1}' title='aab^{-1}b^{-1}a^{-1}a^{-1}a^{-1}bbbbab^{-1}b^{-1}' class='latex' />, which is usually abbreviated with exponential notation, e.g. <img src='http://l.wordpress.com/latex.php?latex=a%5E2b%5E%7B-2%7Da%5E%7B-3%7Db%5E4ab%5E%7B-2%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a^2b^{-2}a^{-3}b^4ab^{-2}' title='a^2b^{-2}a^{-3}b^4ab^{-2}' class='latex' />. Having introduced this notation, one can think of the exponents as parameters, and study stable commutator length in families of words, e.g. <img src='http://l.wordpress.com/latex.php?latex=a%5E%7B2%2Bp%7Db%5E%7B-2%2Bq%7Da%5E%7B-3-p%7Db%5E%7B4-q%7Dab%5E%7B-2%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a^{2+p}b^{-2+q}a^{-3-p}b^{4-q}ab^{-2}' title='a^{2+p}b^{-2+q}a^{-3-p}b^{4-q}ab^{-2}' class='latex' />. Under the correspondence above, the parameters only affect the coefficients of the linear map <img src='http://l.wordpress.com/latex.php?latex=h&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='h' title='h' class='latex' />, and therefore one obtains families of polyhedral cones <img src='http://l.wordpress.com/latex.php?latex=V_A%28p%2Cq%2C%5Ccdots%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='V_A(p,q,\cdots)' title='V_A(p,q,\cdots)' class='latex' /> whose extremal rays depend linearly on the exponent parameters. This lets one prove many facts about the stable commutator length spectrum in a free group, including:</p>
<p><strong>Theorem: </strong>The image of a nonabelian free group of rank at least <img src='http://l.wordpress.com/latex.php?latex=4&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='4' title='4' class='latex' /> under scl in <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbb%7BR%7D%2F%5Cmathbb%7BZ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbb{R}/\mathbb{Z}' title='\mathbb{R}/\mathbb{Z}' class='latex' /> is precisely <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbb%7BQ%7D%2F%5Cmathbb%7BZ%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbb{Q}/\mathbb{Z}' title='\mathbb{Q}/\mathbb{Z}' class='latex' />.</p>
<p>and</p>
<p><strong>Theorem:</strong> For each <img src='http://l.wordpress.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n' title='n' class='latex' />, the image of the free group <img src='http://l.wordpress.com/latex.php?latex=F_n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F_n' title='F_n' class='latex' /> under scl contains a well-ordered sequence of values with ordinal type <img src='http://l.wordpress.com/latex.php?latex=%5Comega%5E%7B%5Clfloor+n%2F4+%5Crfloor%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\omega^{\lfloor n/4 \rfloor}' title='\omega^{\lfloor n/4 \rfloor}' class='latex' />. The image of <img src='http://l.wordpress.com/latex.php?latex=F_%5Cinfty&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F_\infty' title='F_\infty' class='latex' /> contains a well-ordered sequence of values with ordinal type <img src='http://l.wordpress.com/latex.php?latex=%5Comega%5E%5Comega&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\omega^\omega' title='\omega^\omega' class='latex' />.</p>
<p>One can also say things about the precise dependence of scl on parameters in particular families. More conjecturally, one would like to use this correspondence to say something about the <em>statistical</em> distribution of scl in free groups. Experimentally, this distribution appears to obey power laws, in the sense that a given (reduced) fraction <img src='http://l.wordpress.com/latex.php?latex=p%2Fq&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='p/q' title='p/q' class='latex' /> appears in certain infinite families of elements with frequency proportional to <img src='http://l.wordpress.com/latex.php?latex=q%5E%7B-%5Cdelta%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='q^{-\delta}' title='q^{-\delta}' class='latex' /> for some power <img src='http://l.wordpress.com/latex.php?latex=%5Cdelta&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\delta' title='\delta' class='latex' /> (which unfortunately depends in a rather opaque way on the family). Such power laws are reminiscent of Arnold tongues in dynamics, one of the best-known examples of <em>phase locking</em> of coupled nonlinear oscillators. Heuristically one expects such power laws to appear in the geometry of &#8220;random&#8221; sails &#8212; this is explained by the fact that the (affine) geometry of a sail depends only on its <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7BSL%7D%28n%2C%5Cmathbb%7BZ%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{SL}(n,\mathbb{Z})' title='\text{SL}(n,\mathbb{Z})' class='latex' /> orbit, and the existence of invariant measures on a natural moduli space; see e.g. <a href="http://www.ams.org/mathscinet-getitem?mr=1733869">Kontsevich and Suhov</a>. The simplest example concerns the (<img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />-dimensional) cone spanned by a random integral vector in <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbb%7BZ%7D%5E2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbb{Z}^2' title='\mathbb{Z}^2' class='latex' />. The <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7BSL%7D%282%2C%5Cmathbb%7BZ%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{SL}(2,\mathbb{Z})' title='\text{SL}(2,\mathbb{Z})' class='latex' /> orbit of such a vector depends only on the gcd of the two co-ordinates. As is easy to see, the probability distribution of the gcd of a random pair of integers <img src='http://l.wordpress.com/latex.php?latex=p%2Cq&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='p,q' title='p,q' class='latex' /> obeys a power law: <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bgcd%7D%28p%2Cq%29+%3D+n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{gcd}(p,q) = n' title='\text{gcd}(p,q) = n' class='latex' /> with probability <img src='http://l.wordpress.com/latex.php?latex=%5Czeta%282%29%5E%7B-1%7D%2Fn%5E2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\zeta(2)^{-1}/n^2' title='\zeta(2)^{-1}/n^2' class='latex' />. The rigorous justification of the power laws observed in the scl spectrum of free groups remains the focus of current research by myself and my students.</p>
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<title><![CDATA[van Kampen soup and thermodynamics of DNA]]></title>
<link>http://lamington.wordpress.com/2009/07/16/van-kampen-soup-and-thermodynamics-of-dna/</link>
<pubDate>Thu, 16 Jul 2009 08:32:34 +0000</pubDate>
<dc:creator>Danny Calegari</dc:creator>
<guid>http://lamington.wordpress.com/2009/07/16/van-kampen-soup-and-thermodynamics-of-dna/</guid>
<description><![CDATA[The development and scope of modern biology is often held out as a fantastic opportunity for mathema]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p>The development and scope of modern biology is often held out as a fantastic opportunity for mathematicians. The accumulation of vast amounts of biological data, and the development of new tools for the manipulation of biological organisms at microscopic levels and with unprecedented accuracy, invites the development of new mathematical tools for their analysis and exploitation. I know of several examples of mathematicians who have dipped a toe, or sometimes some more substantial organ, into the water. But it has struck me that I know (personally) few mathematicians who believe they have something substantial to learn from the biologists, despite the existence of several famous historical examples.  This strikes me as odd; my instinctive feeling has always been that intellectual ruts develop so easily, so deeply, and so invisibly, that continual cross-fertilization of ideas is essential to escape ossification (if I may mix biological metaphors . . .)</p>
<p>It is not necessarily easy to come up with profound examples of biological ideas or principles that can be easily translated into mathematical ones, but it is sometimes possible to come up with suggestive ones. Let me try to give a tentative example.</p>
<p>Deoxiribonucleic acid (DNA) is a nucleic acid that contains the genetic blueprint for all known living things. This blueprint takes the form of a code &#8212; a molecule of DNA is a long polymer strand composed of simple units called <em>nucleotides</em>; such a molecule is typically imagined as a string in a four character alphabet <img src='http://l.wordpress.com/latex.php?latex=%5Clbrace+A%2CT%2CG%2CC+%5Crbrace&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\lbrace A,T,G,C \rbrace' title='\lbrace A,T,G,C \rbrace' class='latex' />, which stand for the nucleotides Adenine, Thymine, Guanine, and Cytosine. These molecular strands like to arrange themselves in tightly bound oppositely aligned pairs, matching up nucleotides in one string with complementary nucleotides in the other, so that <img src='http://l.wordpress.com/latex.php?latex=A&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='A' title='A' class='latex' /> matches with <img src='http://l.wordpress.com/latex.php?latex=T&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='T' title='T' class='latex' />, and <img src='http://l.wordpress.com/latex.php?latex=C&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='C' title='C' class='latex' /> with <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' />.</p>
<p>The geometry of a strand of DNA is very complicated &#8212; strands can be tangled, knotted, linked in complicated ways, and the fundamental interactions between strands (e.g. transcription, recombination) are facilitated or obstructed by mechanical processes depending on this geometry. Topology, especially knot theory, <a href="http://www.ams.org/notices/199505/sumners.pdf">has been used</a> in the study of some of these processes; the value of topological methods in this context include their robustness (fault-tolerance) and the discreteness of their invariants (similar virtues motivate some efforts to build <a href="http://stationq.cnsi.ucsb.edu/~freedman/Publications/96.pdf">topological quantum computers</a>). A complete mathematical description of the salient biochemistry, mechanics, and semantic content of a configuration of DNA in a single cell is an unrealistic goal for the foreseeable future, and therefore attempts to model such systems depends on ignoring, or treating statistically, certain features of the system. One such framework ignores the ambient geometry entirely, and treats the system using symbolic, or combinatorial methods which have some of the flavor of geometric group theory.</p>
<p>One interesting approach is to consider a mapping from the alphabet of nucleotides to a standard generating set for <img src='http://l.wordpress.com/latex.php?latex=F_2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F_2' title='F_2' class='latex' />, the free group on two generators; for example, one can take the mapping <img src='http://l.wordpress.com/latex.php?latex=T+%5Cto+a%2C+A+%5Cto+A%2C+C+%5Cto+b%2C+G+%5Cto+B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='T \to a, A \to A, C \to b, G \to B' title='T \to a, A \to A, C \to b, G \to B' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=a%2Cb&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='a,b' title='a,b' class='latex' /> are free generators for <img src='http://l.wordpress.com/latex.php?latex=F_2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F_2' title='F_2' class='latex' />, and <img src='http://l.wordpress.com/latex.php?latex=%7B%7DA%2CB&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='{}A,B' title='{}A,B' class='latex' /> denote their inverses. Then a pair of oppositely aligned strands of DNA translates into an edge of a van Kampen diagram &#8212; the &#8220;words&#8221; obtained by reading the letters along an edge on either side are inverse in <img src='http://l.wordpress.com/latex.php?latex=F_2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F_2' title='F_2' class='latex' />.</p>
<p>Strands of DNA in a configuration are <em>not</em> always paired along their lengths; sometimes junctions of three or more strands can form; certain mobile four-strand junctions, so-called &#8220;<a href="http://en.wikipedia.org/wiki/Holliday_junction">Holliday junctions</a>&#8221;, perform important functions in the process of genetic recombination, and are found in a wide variety of organisms. A configuration of several strands with junctions of varying valences corresponds in the language of van Kampen diagrams to a <em>fatgraph</em> &#8212; i.e. a graph together with a choice of cyclic ordering of edges at each vertex &#8212; with edges labeled by inverse pairs of words in <img src='http://l.wordpress.com/latex.php?latex=F_2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F_2' title='F_2' class='latex' /> (note that this is quite different from the <a href="http://arxiv.org/abs/0902.1025">fatgraph model of proteins</a> developed by Penner-Knudsen-Wiuf-Andersen). The energy landscape for branch migration (i.e. the process by which DNA strands separate or join along some segment) is very complicated, and it is challenging to model it thermodynamically. It is therefore not easy to predict in advance what kinds of fatgraphs are more or less likely to arise spontaneously in a prepared &#8220;soup&#8221; of free DNA strands.</p>
<p>As a thought experiment, consider the following &#8220;toy&#8221; model, which I do not suggest is physically realistic. We make the assumption that the energy cost of forming a junction of valence <img src='http://l.wordpress.com/latex.php?latex=v&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='v' title='v' class='latex' /> is <img src='http://l.wordpress.com/latex.php?latex=c%28v-2%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='c(v-2)' title='c(v-2)' class='latex' /> for some fixed constant <img src='http://l.wordpress.com/latex.php?latex=c&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='c' title='c' class='latex' />. Consequently, the energy of a configuration is proportional to <img src='http://l.wordpress.com/latex.php?latex=-%5Cchi&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-\chi' title='-\chi' class='latex' />, i.e. the negative of Euler characteristic of the underlying graph. Let <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> be a reduced word, representing an element of <img src='http://l.wordpress.com/latex.php?latex=F_2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F_2' title='F_2' class='latex' />, and imagine a soup containing some large number of copies of the strand of DNA corresponding to the string <img src='http://l.wordpress.com/latex.php?latex=%5Cdot%7Bw%7D%3A%3D%5Ccdots+www+%5Ccdots&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\dot{w}:=\cdots www \cdots' title='\dot{w}:=\cdots www \cdots' class='latex' />. In thermodynamic equilibrium, the partition function has the form <img src='http://l.wordpress.com/latex.php?latex=Z+%3D+%5Csum_i+e%5E%7B-E_i%2Fk_BT%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Z = \sum_i e^{-E_i/k_BT}' title='Z = \sum_i e^{-E_i/k_BT}' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=k_B&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='k_B' title='k_B' class='latex' /> is Boltzmann&#8217;s constant, <img src='http://l.wordpress.com/latex.php?latex=T&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='T' title='T' class='latex' /> is temperature, and <img src='http://l.wordpress.com/latex.php?latex=E_i&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='E_i' title='E_i' class='latex' /> is the energy of a configuration (which by hypothesis is proportional to <img src='http://l.wordpress.com/latex.php?latex=-%5Cchi&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-\chi' title='-\chi' class='latex' />). At low temperature, minimal energy configurations tend to dominate; these are those that minimize <img src='http://l.wordpress.com/latex.php?latex=-%5Cchi&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-\chi' title='-\chi' class='latex' /> per unit &#8220;volume&#8221;. Topologically, a fatgraph corresponding to such a configuration can be thickened to a surface with boundary. The words along the edges determine a homotopy class of map from such a surface to a <img src='http://l.wordpress.com/latex.php?latex=K%28F_2%2C1%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='K(F_2,1)' title='K(F_2,1)' class='latex' /> (e.g. a once-punctured torus) whose boundary components wrap multiply around the free homotopy class corresponding to the conjugacy class of <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' />. The infimum of <img src='http://l.wordpress.com/latex.php?latex=-%5Cchi%2F2d&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-\chi/2d' title='-\chi/2d' class='latex' /> where <img src='http://l.wordpress.com/latex.php?latex=d&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='d' title='d' class='latex' /> is the winding degree on the boundary, taken over all configurations, is precisely the <em>stable commutator length</em> of <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' />; see e.g. <a href="http://lamington.wordpress.com/2009/06/04/quasimorphisms-and-laws/">here</a> for a definition.</p>
<p>Anyway, this example is perhaps a bit strained (and maybe it owes more to thermodynamics than to biology), but already it suggests a new mathematical object of study, namely the partition function <img src='http://l.wordpress.com/latex.php?latex=Z&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='Z' title='Z' class='latex' /> as above, and one is already inclined to look for examples for which the partition function obeys a symmetry like that enjoyed by the Riemann zeta function, or to specialize temperature to other values, as in random matrix theory. The introduction of new methods into the study of a classical object &#8212; for example, the decision to use thermodynamic methods to organize the study of van Kampen diagrams &#8212; bends the focus of the investigation towards those examples and contexts where the methods and tools are most informative. Phenomena familiar in one context (power laws, frequency locking, phase transitions etc.) suggest new questions and modes of enquiry in another. Uninspired or predictable research programs can benefit tremendously from such infusions, whether the new methods are borrowed from other intellectual disciplines (biology, physics), or depend on new technology (computers), or new methods of indexing (google) or collaboration (<a href="http://gowers.wordpress.com/2009/01/27/is-massively-collaborative-mathematics-possible/">polymath</a>).</p>
<p>One of my intellectual heroes &#8212; <a href="http://en.wikipedia.org/wiki/Wolfgang_Haken">Wolfgang Haken</a> &#8212; worked for eight years in R+D for Siemens in Munich after completing his PhD. I have a conceit (unsubstantiated as far as I know by biographical facts) that his experience working for a big engineering firm colored his approach to mathematics, and made it possible for him to imagine using industrial-scale &#8220;engineering&#8221; tools (e.g. integer programming, exhaustive computer search of combinatorial possibilities) to solve two of the most significant &#8220;pure&#8221; mathematical open problems in topology at the time &#8212; the knot recognition problem, and the four-color theorem. It is an interesting exercise to try to imagine (fantastic) variations. If I sit down and decide to try to prove (for example) Cannon&#8217;s conjecture, I am liable to try minor variations on things I have tried before, appeal for my intuition to examples that I understand well, read papers by others working in similar ways on the problem, etc. If I imagine that I have been given a billion dollars to prove the conjecture, I am almost certain to prioritize the task in different ways, and to entertain (and perhaps create) much more ambitious or innovative research programs to tackle the task. This is the way in which I understand the following quote by John Dewey, which I used as the colophon of my first book:</p>
<blockquote><p>Every great advance in science has issued from a new audacity of the imagination.</p></blockquote>
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<title><![CDATA[PAL-Principal Airlines launches scheduled flights]]></title>
<link>http://worldairlinenews.wordpress.com/2009/06/19/pal-principal-airlines-launches-scheduled-flights/</link>
<pubDate>Fri, 19 Jun 2009 18:30:15 +0000</pubDate>
<dc:creator>brucedrum</dc:creator>
<guid>http://worldairlinenews.wordpress.com/2009/06/19/pal-principal-airlines-launches-scheduled-flights/</guid>
<description><![CDATA[  737-236 CC-CZK displays the new 2009 livery at Santiago. Copyright Photo: Alvaro Romero. PAL-Princ]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p> </p>
<div id="attachment_2029" class="wp-caption aligncenter" style="width: 460px"><a href="http://airlinersgallery.com"><img class="size-full wp-image-2029" title="PAL-Principal 737-200 CC-CZK (09)(Grd) SCL (AR)(LR)" src="http://worldairlinenews.wordpress.com/files/2009/06/pal-principal-737-200-cc-czk-09grd-scl-arlr.jpg" alt="737-236 CC-CZK displays the new 2009 livery at Santiago.  Copyright Photo: Alvaro Romero." width="450" height="300" /></a><p class="wp-caption-text">737-236 CC-CZK displays the new 2009 livery at Santiago.  Copyright Photo: Alvaro Romero.</p></div>
<p>PAL-Principal Airlines (Aeolinea Principal de Chile) (Santiago) began scheduled domestic operations in Chile yesterday (june 18) with a flight linking Santiago with the cities of Antofagasta and Iquique in the north of the country. The first flight, call sign PCP 822 took off from SCL operated by Boeing 737-236 CC-CZK (msn 21804). The second 737-200 (CC-CZO) is currently in maintenance and will soon be ready for service. PAL will operate the northern route two times a day during the week, only once on the weekends.</p>
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<title><![CDATA[Society of Chief Librarian's Conference: public libraries, recession, web 2.0 &amp; social media...]]></title>
<link>http://libraryofdigress.wordpress.com/2009/06/16/society-of-chief-librarians-conference-public-libraries-recession-web-2-0-social-media/</link>
<pubDate>Tue, 16 Jun 2009 14:20:07 +0000</pubDate>
<dc:creator>Christine Rooney-Browne</dc:creator>
<guid>http://libraryofdigress.wordpress.com/2009/06/16/society-of-chief-librarians-conference-public-libraries-recession-web-2-0-social-media/</guid>
<description><![CDATA[Although it&#8217;s still early days in terms of official research, public libraries are emerging on]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p>Although it&#8217;s still early days in terms of official research, public libraries are emerging once again as recession sanctuaries;  providing vital services, in times of economic crisis.</p>
<p><a style="text-decoration:none;" href="http://www.brighton-hove.gov.uk/index.cfm?request=c1200314"><img class="alignright size-medium wp-image-388" title="Brighton-and-Hove-Recession" src="http://libraryofdigress.wordpress.com/files/2009/06/brighton-and-hove-recession3.jpg?w=221" alt="Brighton-and-Hove-Recession" width="112" height="151" /></a></p>
<p>I recently presented on this very topic at the<a href="http://www.goscl.com/home.ikml"> <strong>Society of Chief Librarian&#8217;s</strong> </a>(SCL) Conference at the University of Warwick.  (Presentation available via my SlideShare page, click <strong><a href="http://www.slideshare.net/libraryofdigress">here</a>)</strong>.  Attending the conference was a fantastic experience as I was able to chat to delegates about the impact that the recession has had on their library services; how they&#8217;re managing to deliver high quality services despite ongoing budget cuts; and the innovative ways that they&#8217;re promoting their services to users, including this inspired poster from <a href="http://www.brighton-hove.gov.uk/index.cfm?request=c1200314"><strong>Brighton &#38; Hove</strong></a>&#8230;.</p>
<p>During the Q&#38;A session for my presentaion I noted a strong desire from many delegates to explore <a href="http://en.wikipedia.org/wiki/Web_2.0"><strong>Web 2.0</strong></a> and <a href="http://en.wikipedia.org/wiki/Social_media"><strong>social media</strong></a>.  Unfortunately, however, many are unable to implement their Web 2.0 plans due to restrictions imposed on them by council-wide IT departments and their filtering policies (<a href="http://libraryofdigress.wordpress.com/2009/03/09/when-acceptable-use-policies-go-wrong/"><strong>click here</strong></a><strong> </strong>for a previous blog post about Glasgow City Libraries &#38; internet filtering).  A shame really, given that other authorities, with slightly more liberal approaches to web 2.0 are able to forge ahead, creating interactive and collaborative spaces for library users to visit online (e.g.<strong> </strong><a href="http://www.facebook.com/pages/Manchester/Manchester-Library-Information-Service/10174713053"><strong>Manchester Libraries</strong></a>).</p>
<p>Seems unfair that public library users and staff, many of whom could benefit greatly from accessing web 2.0 and  social media sites are being prevented from doing so as a  result of a web 2.0 postcode lottery.  Wouldn&#8217;t it be great if all public library services across the UK were at the same operational level with web 2.0 and social media&#8230;before we have to deal with the challenges and possibilities that <a href="http://howtosplitanatom.com/news/how-to-define-web-30-2/"><strong>web 3.0</strong></a> presents? Just a thought! <img src='http://s.wordpress.com/wp-includes/images/smilies/icon_smile.gif' alt=':)' class='wp-smiley' /> </p>
<div id="attachment_391" class="wp-caption aligncenter" style="width: 310px"><img class="size-medium wp-image-391" title="Word-Cloud---Twitter-Feed" src="http://libraryofdigress.wordpress.com/files/2009/06/word-cloud-twitter-feed1.jpg?w=300" alt="Twitter Feed - SCL Conference 09 - #scl &#38;#scl09" width="300" height="163" /><p class="wp-caption-text">Twitter Feed - SCL Conference 09 - #scl &#38; #scl09</p></div>
<p>There were lots of other topics discussed over the two days and to highlight some of the burning issues I&#8217;ve created a word cloud, using <strong><a href="http://www.wordle.net/">Wordle</a>, </strong>based on keywords from the Twitter feed (see above).</p>
<p>If you&#8217;re keen to find out more about the role of public libraries in times of recession then why not click <strong><a href="http://www.emeraldinsight.com/Insight/viewContentItem.do;jsessionid=50CE52E7E78C22EDF4AC5E7B0E1E4440?contentType=Article&#38;contentId=1795573">here</a> </strong>to check out my recently published article &#8220;Rising to the Challenge&#8221;,  featured in the latest edition of Library Review.</p>
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<title><![CDATA[SCL Farmakologi]]></title>
<link>http://rdsofyan.wordpress.com/2009/06/06/scl-farmakologi-2/</link>
<pubDate>Sat, 06 Jun 2009 02:52:08 +0000</pubDate>
<dc:creator>rdsofyan</dc:creator>
<guid>http://rdsofyan.wordpress.com/2009/06/06/scl-farmakologi-2/</guid>
<description><![CDATA[Teman-teman&#8230;. File-file SCL Farkol bisa didownload lewat link-link di bawah Kalo ada apa-apa, ]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p>Teman-teman&#8230;.<br />
File-file SCL Farkol bisa didownload lewat link-link di bawah<br />
Kalo ada apa-apa, bisa tulis di komen ja&#8230;</p>
<p><a title="Antiamuba" href="http://www.mediafire.com/file/oabiznyxqtq/PPT Antiamuba.rar" target="_blank">http://www.mediafire.com/file/oabiznyxqtq/PPT Antiamuba.rar</a></p>
<p><a title="Antibakteri" href="http://www.mediafire.com/file/qt4ymczwjzq/PPT Antibakteri.rar" target="_blank">http://www.mediafire.com/file/qt4ymczwjzq/PPT Antibakteri.rar</a></p>
<p><a title="Antijamur" href="http://www.mediafire.com/file/zmw5yq5etjj/PPT Antijamur.rar" target="_blank">http://www.mediafire.com/file/zmw5yq5etjj/PPT Antijamur.rar</a></p>
<p><a title="Antivirus" href="http://www.mediafire.com/file/utknyejznmh/PPT Antivirus.rar" target="_blank">http://www.mediafire.com/file/utknyejznmh/PPT Antivirus.rar</a></p>
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<title><![CDATA[Quasimorphisms and laws]]></title>
<link>http://lamington.wordpress.com/2009/06/04/quasimorphisms-and-laws/</link>
<pubDate>Thu, 04 Jun 2009 23:57:41 +0000</pubDate>
<dc:creator>Danny Calegari</dc:creator>
<guid>http://lamington.wordpress.com/2009/06/04/quasimorphisms-and-laws/</guid>
<description><![CDATA[A basic reference for the background to this post is my monograph. Let be a group, and let denote th]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p>A basic reference for the background to this post is <a href="http://www.its.caltech.edu/~dannyc/scl/toc.html">my monograph</a>.</p>
<p>Let <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> be a group, and let <img src='http://l.wordpress.com/latex.php?latex=%5BG%2CG%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[G,G]' title='[G,G]' class='latex' /> denote the commutator subgroup. Every element of <img src='http://l.wordpress.com/latex.php?latex=%5BG%2CG%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[G,G]' title='[G,G]' class='latex' /> can be expressed as a product of commutators; the <em>commutator length</em> of an element <img src='http://l.wordpress.com/latex.php?latex=g&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g' title='g' class='latex' /> is the minimum number of commutators necessary, and is denoted <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bcl%7D%28g%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{cl}(g)' title='\text{cl}(g)' class='latex' />. The <em>stable commutator length</em> is the growth rate of the commutator lengths of powers of an element; i.e. <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D%28g%29+%3D+%5Clim_%7Bn+%5Cto+%5Cinfty%7D+%5Ctext%7Bcl%7D%28g%5En%29%2Fn&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}(g) = \lim_{n \to \infty} \text{cl}(g^n)/n' title='\text{scl}(g) = \lim_{n \to \infty} \text{cl}(g^n)/n' class='latex' />. Recall that a group <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> is said to satisfy a <em>law</em> if there is a nontrivial word <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> in a free group <img src='http://l.wordpress.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F' title='F' class='latex' /> for which every homomorphism from <img src='http://l.wordpress.com/latex.php?latex=F&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='F' title='F' class='latex' /> to <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> sends <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> to <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bid%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{id}' title='\text{id}' class='latex' />.</p>
<p>The purpose of this post is to give a very short proof of the following proposition (modulo some background that I wanted to talk about anyway):</p>
<p><strong>Proposition:</strong> Suppose <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> obeys a law. Then the stable commutator length vanishes identically on <img src='http://l.wordpress.com/latex.php?latex=%5BG%2CG%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[G,G]' title='[G,G]' class='latex' />.</p>
<p>The proof depends on a duality between stable commutator length and a certain class of functions, called <em>homogeneous quasimorphisms</em>. </p>
<p><strong>Definition:</strong> A function <img src='http://l.wordpress.com/latex.php?latex=%5Cphi%3AG+%5Cto+%5Cmathbb%7BR%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi:G \to \mathbb{R}' title='\phi:G \to \mathbb{R}' class='latex' /> is a <em>quasimorphism</em> if there is some least number <img src='http://l.wordpress.com/latex.php?latex=D%28%5Cphi%29%5Cge+0&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='D(\phi)\ge 0' title='D(\phi)\ge 0' class='latex' /> (called the<em> defect</em>) so that for any pair of elements <img src='http://l.wordpress.com/latex.php?latex=g%2Ch+%5Cin+G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g,h \in G' title='g,h \in G' class='latex' /> there is an inequality <img src='http://l.wordpress.com/latex.php?latex=%26%23124%3B%5Cphi%28x%29+%2B+%5Cphi%28y%29+-+%5Cphi%28xy%29%26%23124%3B+%5Cle+D%28%5Cphi%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='&#124;\phi(x) + \phi(y) - \phi(xy)&#124; \le D(\phi)' title='&#124;\phi(x) + \phi(y) - \phi(xy)&#124; \le D(\phi)' class='latex' />. A quasimorphism is <em>homogeneous</em> if it satisfies <img src='http://l.wordpress.com/latex.php?latex=%5Cphi%28g%5En%29+%3D+n%5Cphi%28g%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi(g^n) = n\phi(g)' title='\phi(g^n) = n\phi(g)' class='latex' /> for all integers <img src='http://l.wordpress.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n' title='n' class='latex' />.</p>
<p>Note that a homogeneous quasimorphism with defect zero is a homomorphism (to <img src='http://l.wordpress.com/latex.php?latex=%5Cmathbb%7BR%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\mathbb{R}' title='\mathbb{R}' class='latex' />). The defect satisfies the following formula:</p>
<p><strong>Lemma: </strong>Let <img src='http://l.wordpress.com/latex.php?latex=f&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f' title='f' class='latex' /> be a homogeneous quasimorphism. Then <img src='http://l.wordpress.com/latex.php?latex=D%28%5Cphi%29+%3D+%5Csup_%7Bg%2Ch%7D+%5Cphi%28%5Bg%2Ch%5D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='D(\phi) = \sup_{g,h} \phi([g,h])' title='D(\phi) = \sup_{g,h} \phi([g,h])' class='latex' />.</p>
<p>A fundamental theorem, due to Bavard, is the following:</p>
<p><strong>Theorem:</strong> (Bavard duality) There is an equality <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D%28g%29+%3D+%5Csup_%5Cphi+%5Cfrac+%7B%5Cphi%28g%29%7D+%7B2D%28%5Cphi%29%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}(g) = \sup_\phi \frac {\phi(g)} {2D(\phi)}' title='\text{scl}(g) = \sup_\phi \frac {\phi(g)} {2D(\phi)}' class='latex' /> where the supremum is taken over all homogeneous quasimorphisms with nonzero defect.</p>
<p>In particular, <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}' title='\text{scl}' class='latex' /> vanishes identically on <img src='http://l.wordpress.com/latex.php?latex=%5BG%2CG%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[G,G]' title='[G,G]' class='latex' /> if and only if every homogeneous quasimorphism on <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> is a homomorphism.</p>
<p>One final ingredient is another geometric definition of <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}' title='\text{scl}' class='latex' /> in terms of Euler characteristic. Let <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' /> be a space with <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_1%28X%29+%3D+G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_1(X) = G' title='\pi_1(X) = G' class='latex' />, and let <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma%3AS%5E1+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma:S^1 \to X' title='\gamma:S^1 \to X' class='latex' /> be a free homotopy class representing a given conjugacy class <img src='http://l.wordpress.com/latex.php?latex=g&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g' title='g' class='latex' />. If <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> is a compact, oriented surface without sphere or disk components, a map <img src='http://l.wordpress.com/latex.php?latex=f%3AS+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f:S \to X' title='f:S \to X' class='latex' /> is <em>admissible</em> if the map on <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial S' title='\partial S' class='latex' /> factors through <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+f%3A%5Cpartial+S+%5Cto+S%5E1+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial f:\partial S \to S^1 \to X' title='\partial f:\partial S \to S^1 \to X' class='latex' />, where the second map is <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' />. For an admissible map, define <img src='http://l.wordpress.com/latex.php?latex=n%28S%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n(S)' title='n(S)' class='latex' /> by the equality <img src='http://l.wordpress.com/latex.php?latex=%5B%5Cpartial+S%5D+%5Cto+n%28S%29+%5BS%5E1%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[\partial S] \to n(S) [S^1]' title='[\partial S] \to n(S) [S^1]' class='latex' /> in <img src='http://l.wordpress.com/latex.php?latex=H_1%28S%5E1%3B%5Cmathbb%7BZ%7D%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='H_1(S^1;\mathbb{Z})' title='H_1(S^1;\mathbb{Z})' class='latex' /> (i.e. <img src='http://l.wordpress.com/latex.php?latex=n%28S%29&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n(S)' title='n(S)' class='latex' /> is the degree with which <img src='http://l.wordpress.com/latex.php?latex=%5Cpartial+S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\partial S' title='\partial S' class='latex' /> wraps around <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' />). With this notation, one has the following:</p>
<p><strong>Lemma:</strong> There is an equality <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D%28g%29+%3D+%5Cinf_S+%5Cfrac+%7B-%5Cchi%5E-%28S%29%7D+%7B2n%28S%29%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}(g) = \inf_S \frac {-\chi^-(S)} {2n(S)}' title='\text{scl}(g) = \inf_S \frac {-\chi^-(S)} {2n(S)}' class='latex' />.</p>
<p>Note: the function <img src='http://l.wordpress.com/latex.php?latex=-%5Cchi%5E-&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-\chi^-' title='-\chi^-' class='latex' /> is the sum of <img src='http://l.wordpress.com/latex.php?latex=-%5Cchi&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-\chi' title='-\chi' class='latex' /> over non-disk and non-sphere components of <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' />. By hypothesis, there are none, so we could just write <img src='http://l.wordpress.com/latex.php?latex=-%5Cchi&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-\chi' title='-\chi' class='latex' />. However, it is worth writing <img src='http://l.wordpress.com/latex.php?latex=-%5Cchi%5E-&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-\chi^-' title='-\chi^-' class='latex' /> and observing that for more general (orientable) surfaces, this function is equal to the function <img src='http://l.wordpress.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\rho' title='\rho' class='latex' /> defined in a <a href="http://lamington.wordpress.com/2009/05/29/the-strengthened-hanna-neumann-conjecture/">previous post</a>.</p>
<p>We now give the proof of the Proposition.</p>
<p><em>Proof.</em> Suppose to the contrary that stable commutator length does not vanish on <img src='http://l.wordpress.com/latex.php?latex=%5BG%2CG%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[G,G]' title='[G,G]' class='latex' />. By Bavard duality, there is a homogeneous quasimorphism <img src='http://l.wordpress.com/latex.php?latex=%5Cphi&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi' title='\phi' class='latex' /> with nonzero defect. Rescale <img src='http://l.wordpress.com/latex.php?latex=%5Cphi&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi' title='\phi' class='latex' /> to have defect <img src='http://l.wordpress.com/latex.php?latex=1&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='1' title='1' class='latex' />. Then for any <img src='http://l.wordpress.com/latex.php?latex=%5Cepsilon&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\epsilon' title='\epsilon' class='latex' /> there are elements <img src='http://l.wordpress.com/latex.php?latex=g%2Ch&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g,h' title='g,h' class='latex' /> with <img src='http://l.wordpress.com/latex.php?latex=%5Cphi%28%5Bg%2Ch%5D%29+%5Cge+1-%5Cepsilon&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\phi([g,h]) \ge 1-\epsilon' title='\phi([g,h]) \ge 1-\epsilon' class='latex' />, and consequently <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D%28%5Bg%2Ch%5D%29+%5Cge+1%2F2+-+%5Cepsilon%2F2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}([g,h]) \ge 1/2 - \epsilon/2' title='\text{scl}([g,h]) \ge 1/2 - \epsilon/2' class='latex' /> by Bavard duality. On the other hand, if <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' /> is a space with <img src='http://l.wordpress.com/latex.php?latex=%5Cpi_1%28X%29%3DG&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\pi_1(X)=G' title='\pi_1(X)=G' class='latex' />, and <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma%3AS%5E1+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma:S^1 \to X' title='\gamma:S^1 \to X' class='latex' /> is a loop representing the conjugacy class of <img src='http://l.wordpress.com/latex.php?latex=%5Bg%2Ch%5D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='[g,h]' title='[g,h]' class='latex' />, there is a map <img src='http://l.wordpress.com/latex.php?latex=f%3AS+%5Cto+X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='f:S \to X' title='f:S \to X' class='latex' /> from a once-punctured torus <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> to <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' /> whose boundary represents <img src='http://l.wordpress.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\gamma' title='\gamma' class='latex' />. The fundamental group of <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> is free on two generators <img src='http://l.wordpress.com/latex.php?latex=x%2Cy&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='x,y' title='x,y' class='latex' /> which map to the class of <img src='http://l.wordpress.com/latex.php?latex=g%2Ch&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='g,h' title='g,h' class='latex' /> respectively. If <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' /> is a word in <img src='http://l.wordpress.com/latex.php?latex=x%2Cy&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='x,y' title='x,y' class='latex' /> mapping to the identity in <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' />, there is an essential loop <img src='http://l.wordpress.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha' title='\alpha' class='latex' /> in <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' /> that maps inessentially to <img src='http://l.wordpress.com/latex.php?latex=X&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='X' title='X' class='latex' />. There is a finite cover <img src='http://l.wordpress.com/latex.php?latex=%5Cwidetilde%7BS%7D&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\widetilde{S}' title='\widetilde{S}' class='latex' /> of <img src='http://l.wordpress.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S' title='S' class='latex' />, of degree <img src='http://l.wordpress.com/latex.php?latex=d&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='d' title='d' class='latex' /> depending on the word length of <img src='http://l.wordpress.com/latex.php?latex=w&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='w' title='w' class='latex' />, for which <img src='http://l.wordpress.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\alpha' title='\alpha' class='latex' /> lifts to an embedded loop. This can be compressed to give a surface <img src='http://l.wordpress.com/latex.php?latex=S%27&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='S&#039;' title='S&#039;' class='latex' /> with <img src='http://l.wordpress.com/latex.php?latex=-%5Cchi%5E-%28S%27%29+%5Cle+-%5Cchi%5E-%28%5Cwidetilde%7BS%7D%29-2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-\chi^-(S&#039;) \le -\chi^-(\widetilde{S})-2' title='-\chi^-(S&#039;) \le -\chi^-(\widetilde{S})-2' class='latex' />. However, Euler characteristic is multiplicative under coverings, so <img src='http://l.wordpress.com/latex.php?latex=-%5Cchi%5E-%28%5Cwidetilde%7BS%7D%29+%3D+-%5Cchi%5E-%28S%29%5Ccdot+d&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='-\chi^-(\widetilde{S}) = -\chi^-(S)\cdot d' title='-\chi^-(\widetilde{S}) = -\chi^-(S)\cdot d' class='latex' />. On the other hand, <img src='http://l.wordpress.com/latex.php?latex=n%28S%27%29+%3D+n%28%5Cwidetilde%7BS%7D%29%3Dd&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='n(S&#039;) = n(\widetilde{S})=d' title='n(S&#039;) = n(\widetilde{S})=d' class='latex' /> so <img src='http://l.wordpress.com/latex.php?latex=%5Ctext%7Bscl%7D%28%5Bg%2Ch%5D%29+%5Cle+1%2F2+-+1%2Fd&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\text{scl}([g,h]) \le 1/2 - 1/d' title='\text{scl}([g,h]) \le 1/2 - 1/d' class='latex' />. If <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> obeys a law, then <img src='http://l.wordpress.com/latex.php?latex=d&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='d' title='d' class='latex' /> is fixed, but <img src='http://l.wordpress.com/latex.php?latex=%5Cepsilon&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='\epsilon' title='\epsilon' class='latex' /> can be made arbitrarily small. So <img src='http://l.wordpress.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='G' title='G' class='latex' /> does not obey a law. qed.</p>
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<title><![CDATA[Immunity]]></title>
<link>http://maryrussell.wordpress.com/2009/06/03/immunity/</link>
<pubDate>Wed, 03 Jun 2009 15:01:21 +0000</pubDate>
<dc:creator>Mary</dc:creator>
<guid>http://maryrussell.wordpress.com/2009/06/03/immunity/</guid>
<description><![CDATA[1.) Read this: immunity This is from Jon Acuff at Stuff Christians Like. Definitely one of my favori]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p>1.) Read this: <a title="SCL" href="http://stufffchristianslike.blogspot.com/2009/06/552-judging-pop-culture-as-if-were.html" target="_blank">immunity</a> This is from Jon Acuff at Stuff Christians Like. Definitely one of my favorite blogs.</p>
<p>2.) Then read this:</p>
<p>Brian and I watched the episode of J&#38;K+8 that Jon is referring to in this post. It was so sad. Brian and I kept pausing it and discussing what/how they said what was going on. It really made us talk about our marriage. On one hand, it really made us appreciate how open and honest we are with each other. We talk to each other all the time, but also allow for some time alone. We found ourselves referring to our devotional book we&#8217;ve been studying saying, &#8220;that sounds like the other day when our devo was talking about &#8230;&#8221; On the other hand, we&#8217;re not immune to anything. We constantly struggle to be reminded of grace, of love, and that we don&#8217;t deserve anything.</p>
<p>I far too easily get wrapped up in what people deserve, making sure the &#8220;right&#8221; consequences are endured, and that people don&#8217;t get away with anything. God has to <em>constantly</em> remind me of grace. God is justice but He is also grace. Who do I think I am sometimes? I&#8217;m surely not God, not perfect, not faultless, not always right (shhh don&#8217;t tell!), not always loving or forgiving. If I&#8217;m none of those things, then who am I? I&#8217;m a sinner, saved by grace.</p>
<p> </p>
<p>Praise God: We&#8217;re not immune to His grace.</p>
<p> </p>
<p>3.) Answer this: What do you think?</p>
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<title><![CDATA[five week plan]]></title>
<link>http://lamington.wordpress.com/2009/05/25/five-week-plan/</link>
<pubDate>Tue, 26 May 2009 03:09:07 +0000</pubDate>
<dc:creator>Danny Calegari</dc:creator>
<guid>http://lamington.wordpress.com/2009/05/25/five-week-plan/</guid>
<description><![CDATA[As an experiment, I plan to spend the next five weeks documenting my current research on this blog. ]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p>As an experiment, I plan to spend the next five weeks documenting my current research on this blog. This research comprises several related projects, but most are concerned in one way or another with the general program of studying the geometry of a space by probing it with surfaces. Since I am nominally a topologist, these surfaces are real <img src='http://l.wordpress.com/latex.php?latex=2&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='2' title='2' class='latex' />-manifolds, and I am usually interested in working in the homotopy category (or some rational &#8220;quotient&#8221; of it). I am especially concerned with surfaces with boundary, and even (occasionally) with corners. </p>
<p>Since it is good to have a &#8220;big question&#8221; lurking somewhere in the background (for the purposes of motivation and advertising, if nothing else), I should admit from the start that I am interested in Gromov&#8217;s well-known question about surface subgroups, which asks:</p>
<p><strong>Question </strong>(Gromov): Does every one-ended word-hyperbolic group contain a closed hyperbolic surface subgroup?</p>
<p>I don&#8217;t have strong feelings about whether the answer to this question is &#8220;yes&#8221; or &#8220;no&#8221;, but I do think the question can be sharpened usefully in many ways, and it is my intention to do so. Gromov&#8217;s question is certainly inspired by questions such as Waldhausen&#8217;s conjecture and the virtual fibration conjecture in <img src='http://l.wordpress.com/latex.php?latex=3&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='3' title='3' class='latex' />-manifold topology, but it is hard to imagine that a proof of one of these conjectures would shed much light on Gromov&#8217;s question in general. At least one essential tool in <img src='http://l.wordpress.com/latex.php?latex=3&#038;bg=ffffff&#038;fg=000000&#038;s=0' alt='3' title='3' class='latex' />-manifold topology &#8212; namely Dehn&#8217;s lemma &#8212; has no meaningful analogue in geometric group theory, and I think it is important to try to imagine different methods of constructing surface groups from &#8220;first principles&#8221;.</p>
<p>Another long-term project that informs much of my current research is the problem of understanding stable commutator length in free groups. The interested reader can learn something about this from my monograph (which can be downloaded from <a href="http://www.its.caltech.edu/~dannyc/scl/toc.html">this page</a>). I hope to explain why this is a fundamental and interesting problem, with rich structure and many potential applications.</p>
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<title><![CDATA[A summer of library conferences to look forward to...]]></title>
<link>http://libraryofdigress.wordpress.com/2009/05/19/a-summer-of-library-conferences-to-look-forward-to/</link>
<pubDate>Tue, 19 May 2009 13:15:26 +0000</pubDate>
<dc:creator>Christine Rooney-Browne</dc:creator>
<guid>http://libraryofdigress.wordpress.com/2009/05/19/a-summer-of-library-conferences-to-look-forward-to/</guid>
<description><![CDATA[It&#8217;s that time of year again; I&#8217;m gearing up for a summer of library conferences and I]]></description>
<content:encoded><![CDATA[<div class='snap_preview'><p>It&#8217;s that time of year again; I&#8217;m gearing up for a summer of library conferences and I&#8217;m so, so excited!   </p>
<p>First up there&#8217;s the <a href="http://www.slainte.org.uk/CILIPS/conference/conferenceindex.htm"><strong>CILIPS conference</strong></a> (Branch Group Day) on 3rd June at Peebles Hydro, featuring sessions with <a href="http://www.oclc.org/about/management/default.htm"><strong>Jay Jordan (OCLC)</strong></a>, <a href="http://www.bl.uk/about/annual/2007to2008/governance/boulderstone.html"><strong>Richard Boulderstone (British Library)</strong></a>, <a href="http://ukwebfocus.wordpress.com/"><strong>Brian Kelly (UKOLN)</strong></a> and <a href="http://www.mla.gov.uk/about/who/staff"><strong>David Potts (MLA)</strong></a>&#8230;plus lots more; check out the programme <a href="http://www.slainte.org.uk/files/pdf/cilips/conf09/RunningOrder2.pdf"><strong>here</strong></a>.  </p>
<p>Then the next day I&#8217;m heading down to Warwick for the <a href="http://www.goscl.com/home.ikml"><strong>Society of Chief Librarians Conference</strong></a>, which I&#8217;m presenting at on the Friday.  I&#8217;ll be discussing<em> &#8220;Social Value: identifying, measuring and sharing some of the less obvious ways that public libraries contribute to economic regeneration&#8221;</em>.  </p>
<p>A few weeks later it&#8217;s off to Turin, Italy to attend the <strong><a href="http://www.ifla2009.it/web/eventi/ifla_preconference_torino.htm">Pre-congress satellite for the IFLA World Library and Information Congress (2009)</a></strong> to present a co-authored paper on &#8220;<em>Public libraries as impartial spaces in the 21st Century&#8221;</em> .  The programme for this looks amazing; check it out <a href="http://www.ifla2009.it/web/eventi/ifla_preconference_torino_programma_en.htm"><strong>here</strong></a>.  Then it&#8217;s a quick train journey through to Milan to attend the <a href="http://www.ifla.org/annual-conference/ifla75/"><strong>75th IFLA General Conference and Assembly!</strong></a></p>
<p><a href="http://www.ifla.org/annual-conference/ifla75/"><strong></strong></a></p>
<p>Phew!  Will be a busy few months but <a href="http://libraryofdigress.wordpress.com/2008/08/26/travelling-librarian-returns-from-canada/"><strong>I know I&#8217;ll have a fantastic time</strong></a>! Drop me a line if you&#8217;re planning to attend any of these conferences and we can arrange to meet up in the hallways! <img src='http://s.wordpress.com/wp-includes/images/smilies/icon_smile.gif' alt=':)' class='wp-smiley' /> </p>
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