<?xml version="1.0" encoding="UTF-8" standalone="yes"?><oembed><version><![CDATA[1.0]]></version><provider_name><![CDATA[Geometry and the imagination]]></provider_name><provider_url><![CDATA[https://lamington.wordpress.com]]></provider_url><author_name><![CDATA[Danny Calegari]]></author_name><author_url><![CDATA[https://lamington.wordpress.com/author/dannycaltech/]]></author_url><title><![CDATA[The Goldman bracket]]></title><type><![CDATA[link]]></type><html><![CDATA[<p>I was in Stony Brook last week, visiting Moira Chas and Dennis Sullivan, and have been away from blogging for a while; this week I plan to write a few posts about some of the things I discussed with Moira and Dennis. This is an introductory post about the Goldman bracket, an extraordinary mathematical object made out of the combinatorics of immersed curves on surfaces. I don&#8217;t have anything original to say about this object, but for my own benefit I thought I would try to explain what it is, and why Goldman was interested in it.</p>
<p>In his study of symplectic structures on character varieties <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BHom%7D%28%5Cpi%2CG%29%2FG&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Hom}(&#92;pi,G)/G" title="&#92;text{Hom}(&#92;pi,G)/G" class="latex" />, where <img src="https://s0.wp.com/latex.php?latex=%5Cpi&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi" title="&#92;pi" class="latex" /> is the fundamental group of a closed oriented surface and <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> is a Lie group satisfying certain (quite general) conditions, Bill Goldman <a href="http://www.ams.org/mathscinet-getitem?mr=0762512">discovered</a> a remarkable Lie algebra structure on the free abelian group generated by conjugacy classes in <img src="https://s0.wp.com/latex.php?latex=%5Cpi&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi" title="&#92;pi" class="latex" />. Let <img src="https://s0.wp.com/latex.php?latex=%5Chat%7B%5Cpi%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;hat{&#92;pi}" title="&#92;hat{&#92;pi}" class="latex" /> denote the set of homotopy classes of closed oriented curves on <img src="https://s0.wp.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S" title="S" class="latex" />, where <img src="https://s0.wp.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S" title="S" class="latex" /> is itself a compact oriented surface, and let <img src="https://s0.wp.com/latex.php?latex=%5Cmathbb%7BZ%7D%5Chat%7B%5Cpi%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathbb{Z}&#92;hat{&#92;pi}" title="&#92;mathbb{Z}&#92;hat{&#92;pi}" class="latex" /> denote the free abelian group with generating set <img src="https://s0.wp.com/latex.php?latex=%5Chat%7B%5Cpi%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;hat{&#92;pi}" title="&#92;hat{&#92;pi}" class="latex" />. If <img src="https://s0.wp.com/latex.php?latex=%5Calpha%2C%5Cbeta&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha,&#92;beta" title="&#92;alpha,&#92;beta" class="latex" /> are immersed oriented closed curves which intersect transversely (i.e. in double points), define the formal sum</p>
<p style="padding-left:30px;"><img src="https://s0.wp.com/latex.php?latex=%5B%5Calpha%2C%5Cbeta%5D+%3D+%5Csum_%7Bp+%5Cin+%5Calpha+%5Ccap+%5Cbeta%7D+%5Cepsilon%28p%3B+%5Calpha%2C%5Cbeta%29+%7C%5Calpha_p%5Cbeta_p%7C+%5Cin+%5Cmathbb%7BZ%7D%5Chat%7B%5Cpi%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="[&#92;alpha,&#92;beta] = &#92;sum_{p &#92;in &#92;alpha &#92;cap &#92;beta} &#92;epsilon(p; &#92;alpha,&#92;beta) |&#92;alpha_p&#92;beta_p| &#92;in &#92;mathbb{Z}&#92;hat{&#92;pi}" title="[&#92;alpha,&#92;beta] = &#92;sum_{p &#92;in &#92;alpha &#92;cap &#92;beta} &#92;epsilon(p; &#92;alpha,&#92;beta) |&#92;alpha_p&#92;beta_p| &#92;in &#92;mathbb{Z}&#92;hat{&#92;pi}" class="latex" /></p>
<p>In this formula, <img src="https://s0.wp.com/latex.php?latex=%5Calpha_p%2C%5Cbeta_p&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha_p,&#92;beta_p" title="&#92;alpha_p,&#92;beta_p" class="latex" /> are <img src="https://s0.wp.com/latex.php?latex=%5Calpha%2C%5Cbeta&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha,&#92;beta" title="&#92;alpha,&#92;beta" class="latex" /> thought of as based loops at the point <img src="https://s0.wp.com/latex.php?latex=p&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p" title="p" class="latex" />, <img src="https://s0.wp.com/latex.php?latex=%5Calpha_p%5Cbeta_p&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha_p&#92;beta_p" title="&#92;alpha_p&#92;beta_p" class="latex" /> represents their product in <img src="https://s0.wp.com/latex.php?latex=%5Cpi_1%28S%2Cp%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi_1(S,p)" title="&#92;pi_1(S,p)" class="latex" />, and <img src="https://s0.wp.com/latex.php?latex=%7C%5Calpha_p%5Cbeta_p%7C&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="|&#92;alpha_p&#92;beta_p|" title="|&#92;alpha_p&#92;beta_p|" class="latex" /> represents the resulting conjugacy class in <img src="https://s0.wp.com/latex.php?latex=%5Cpi&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi" title="&#92;pi" class="latex" />. Moreover, <img src="https://s0.wp.com/latex.php?latex=%5Cepsilon%28p%3B%5Calpha%2C%5Cbeta%29+%3D+%5Cpm+1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;epsilon(p;&#92;alpha,&#92;beta) = &#92;pm 1" title="&#92;epsilon(p;&#92;alpha,&#92;beta) = &#92;pm 1" class="latex" /> is the oriented intersection number of <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" /> and <img src="https://s0.wp.com/latex.php?latex=%5Cbeta&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;beta" title="&#92;beta" class="latex" /> at <img src="https://s0.wp.com/latex.php?latex=p&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p" title="p" class="latex" />.</p>
<p>This operation turns out to depend only on the free homotopy classes of <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" /> and <img src="https://s0.wp.com/latex.php?latex=%5Cbeta&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;beta" title="&#92;beta" class="latex" />, and extends by linearity to a bilinear map <img src="https://s0.wp.com/latex.php?latex=%5B%5Ccdot%2C%5Ccdot%5D%3A%5Cmathbb%7BZ%7D%5Chat%7B%5Cpi%7D+%5Ctimes+%5Cmathbb%7BZ%7D%5Chat%7B%5Cpi%7D+%5Cto+%5Cmathbb%7BZ%7D%5Chat%7B%5Cpi%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="[&#92;cdot,&#92;cdot]:&#92;mathbb{Z}&#92;hat{&#92;pi} &#92;times &#92;mathbb{Z}&#92;hat{&#92;pi} &#92;to &#92;mathbb{Z}&#92;hat{&#92;pi}" title="[&#92;cdot,&#92;cdot]:&#92;mathbb{Z}&#92;hat{&#92;pi} &#92;times &#92;mathbb{Z}&#92;hat{&#92;pi} &#92;to &#92;mathbb{Z}&#92;hat{&#92;pi}" class="latex" />. Goldman shows that this bracket makes <img src="https://s0.wp.com/latex.php?latex=%5Cmathbb%7BZ%7D%5Chat%7B%5Cpi%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathbb{Z}&#92;hat{&#92;pi}" title="&#92;mathbb{Z}&#92;hat{&#92;pi}" class="latex" /> into a Lie algebra over <img src="https://s0.wp.com/latex.php?latex=%5Cmathbb%7BZ%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathbb{Z}" title="&#92;mathbb{Z}" class="latex" />, and that there are natural Lie algebra homomorphisms from <img src="https://s0.wp.com/latex.php?latex=%5Cmathbb%7BZ%7D%5Chat%7B%5Cpi%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathbb{Z}&#92;hat{&#92;pi}" title="&#92;mathbb{Z}&#92;hat{&#92;pi}" class="latex" /> to the Lie algebra of functions on <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BHom%7D%28%5Cpi%2CG%29%2FG&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Hom}(&#92;pi,G)/G" title="&#92;text{Hom}(&#92;pi,G)/G" class="latex" /> with its Poisson bracket.</p>
<p>The connection with character varieties can be summarized as follows. Let <img src="https://s0.wp.com/latex.php?latex=f%3AG+%5Cto+%5Cmathbb%7BR%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="f:G &#92;to &#92;mathbb{R}" title="f:G &#92;to &#92;mathbb{R}" class="latex" /> be a (smooth) class function (i.e. a function which is constant on conjugacy classes) on a Lie group <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" />. Define the variation function <img src="https://s0.wp.com/latex.php?latex=F%3AG+%5Cto+%5Cmathfrak%7Bg%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="F:G &#92;to &#92;mathfrak{g}" title="F:G &#92;to &#92;mathfrak{g}" class="latex" /> by the formula</p>
<p style="padding-left:30px;"><img src="https://s0.wp.com/latex.php?latex=%5Clangle+F%28A%29%2CX%5Crangle+%3D+%5Cfrac+%7Bd%7D%7Bdt%7D%7C_%7Bt%3D0%7D+f%28A%5Ctext%7Bexp%7D%7BtX%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;langle F(A),X&#92;rangle = &#92;frac {d}{dt}|_{t=0} f(A&#92;text{exp}{tX})" title="&#92;langle F(A),X&#92;rangle = &#92;frac {d}{dt}|_{t=0} f(A&#92;text{exp}{tX})" class="latex" /></p>
<p>where <img src="https://s0.wp.com/latex.php?latex=%5Clangle+%5Ccdot%2C%5Ccdot%5Crangle&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;langle &#92;cdot,&#92;cdot&#92;rangle" title="&#92;langle &#92;cdot,&#92;cdot&#92;rangle" class="latex" /> is some (fixed) <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BAd%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Ad}" title="&#92;text{Ad}" class="latex" />-invariant orthogonal structure on the Lie algebra <img src="https://s0.wp.com/latex.php?latex=%5Cmathfrak%7Bg%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathfrak{g}" title="&#92;mathfrak{g}" class="latex" /> (for example, if <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> is reductive (eg if <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> is semisimple), one can take <img src="https://s0.wp.com/latex.php?latex=%5Clangle+X%2CY%5Crangle+%3D+%5Ctext%7Btr%7D%28XY%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;langle X,Y&#92;rangle = &#92;text{tr}(XY)" title="&#92;langle X,Y&#92;rangle = &#92;text{tr}(XY)" class="latex" />). The tangent space to the character variety <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BHom%7D%28%5Cpi%2CG%29%2FG&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Hom}(&#92;pi,G)/G" title="&#92;text{Hom}(&#92;pi,G)/G" class="latex" /> at <img src="https://s0.wp.com/latex.php?latex=%5Cphi&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;phi" title="&#92;phi" class="latex" /> is the first cohomology group of <img src="https://s0.wp.com/latex.php?latex=%5Cpi&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi" title="&#92;pi" class="latex" /> with coefficients in <img src="https://s0.wp.com/latex.php?latex=%5Cmathfrak%7Bg%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathfrak{g}" title="&#92;mathfrak{g}" class="latex" />, thought of as a <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> module with the <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BAd%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Ad}" title="&#92;text{Ad}" class="latex" /> action, and then as a <img src="https://s0.wp.com/latex.php?latex=%5Cpi&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi" title="&#92;pi" class="latex" /> module by the representation <img src="https://s0.wp.com/latex.php?latex=%5Cphi&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;phi" title="&#92;phi" class="latex" />. Cup product and the pairing <img src="https://s0.wp.com/latex.php?latex=%5Clangle%5Ccdot%2C%5Ccdot%5Crangle&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;langle&#92;cdot,&#92;cdot&#92;rangle" title="&#92;langle&#92;cdot,&#92;cdot&#92;rangle" class="latex" /> determine a pairing</p>
<p style="padding-left:30px;"><img src="https://s0.wp.com/latex.php?latex=H%5E1%28%5Cpi%2C%5Cmathfrak%7Bg%7D%29%5Ctimes+H%5E1%28%5Cpi%2C%5Cmathfrak%7Bg%7D%29+%5Cto+H%5E2%28%5Cpi%2C%5Cmathbb%7BR%7D%29+%3D+%5Cmathbb%7BR%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H^1(&#92;pi,&#92;mathfrak{g})&#92;times H^1(&#92;pi,&#92;mathfrak{g}) &#92;to H^2(&#92;pi,&#92;mathbb{R}) = &#92;mathbb{R}" title="H^1(&#92;pi,&#92;mathfrak{g})&#92;times H^1(&#92;pi,&#92;mathfrak{g}) &#92;to H^2(&#92;pi,&#92;mathbb{R}) = &#92;mathbb{R}" class="latex" /></p>
<p>where the last equality uses the fact that <img src="https://s0.wp.com/latex.php?latex=%5Cpi&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi" title="&#92;pi" class="latex" /> is a closed surface group; this pairing defines the symplectic structure on <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BHom%7D%28%5Cpi%2CG%29%2FG&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Hom}(&#92;pi,G)/G" title="&#92;text{Hom}(&#92;pi,G)/G" class="latex" />.</p>
<p>Every element <img src="https://s0.wp.com/latex.php?latex=%5Calpha+%5Cin+%5Cpi&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha &#92;in &#92;pi" title="&#92;alpha &#92;in &#92;pi" class="latex" /> determines a function <img src="https://s0.wp.com/latex.php?latex=f_%5Calpha%3A%5Ctext%7BHom%7D%28%5Cpi%2CG%29%2FG+%5Cto+%5Cmathbb%7BR%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="f_&#92;alpha:&#92;text{Hom}(&#92;pi,G)/G &#92;to &#92;mathbb{R}" title="f_&#92;alpha:&#92;text{Hom}(&#92;pi,G)/G &#92;to &#92;mathbb{R}" class="latex" /> by sending a (conjugacy class of) representation <img src="https://s0.wp.com/latex.php?latex=%5B%5Cphi%5D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="[&#92;phi]" title="[&#92;phi]" class="latex" /> to <img src="https://s0.wp.com/latex.php?latex=f%28%5Cphi%28%5Calpha%29%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="f(&#92;phi(&#92;alpha))" title="f(&#92;phi(&#92;alpha))" class="latex" />. Note that <img src="https://s0.wp.com/latex.php?latex=f_%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="f_&#92;alpha" title="f_&#92;alpha" class="latex" /> only depends on the conjugacy class of <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" /> in <img src="https://s0.wp.com/latex.php?latex=%5Cpi&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi" title="&#92;pi" class="latex" />. It is natural to ask: what is the Hamiltonian flow on <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BHom%7D%28%5Cpi%2CG%29%2FG&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Hom}(&#92;pi,G)/G" title="&#92;text{Hom}(&#92;pi,G)/G" class="latex" /> generated by the function <img src="https://s0.wp.com/latex.php?latex=f_%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="f_&#92;alpha" title="f_&#92;alpha" class="latex" />? It turns out that when <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" /> is a <em>simple</em> closed curve, it is very easy to describe this Hamiltonian flow. If <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" /> is nonseparating, then define a flow <img src="https://s0.wp.com/latex.php?latex=%5Cpsi_t&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;psi_t" title="&#92;psi_t" class="latex" /> by <img src="https://s0.wp.com/latex.php?latex=%5Cpsi_t%5Cphi%28%5Cgamma%29%3D%5Cphi%28%5Cgamma%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;psi_t&#92;phi(&#92;gamma)=&#92;phi(&#92;gamma)" title="&#92;psi_t&#92;phi(&#92;gamma)=&#92;phi(&#92;gamma)" class="latex" /> when <img src="https://s0.wp.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;gamma" title="&#92;gamma" class="latex" /> is represented by a curve disjoint from <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" />, and <img src="https://s0.wp.com/latex.php?latex=%5Cpsi_t%5Cphi%28%5Cgamma%29%3D+%5Ctext%7Bexp%7D+tF_%5Calpha%28%5Cphi%29%5Cphi%28%5Cgamma%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;psi_t&#92;phi(&#92;gamma)= &#92;text{exp} tF_&#92;alpha(&#92;phi)&#92;phi(&#92;gamma)" title="&#92;psi_t&#92;phi(&#92;gamma)= &#92;text{exp} tF_&#92;alpha(&#92;phi)&#92;phi(&#92;gamma)" class="latex" /> if <img src="https://s0.wp.com/latex.php?latex=%5Cgamma&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;gamma" title="&#92;gamma" class="latex" /> intersects <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" /> exactly once with a positive orientation (there is a similar formula when <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" /> is separating). In other words, the representation is constant on the fundamental group of the surface &#8220;cut open&#8221; along the curve <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" />, and only deforms in the way the two conjugacy classes of <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" /> in the cut open surface are identified in <img src="https://s0.wp.com/latex.php?latex=%5Cpi&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;pi" title="&#92;pi" class="latex" />.</p>
<p>In the important motivating case that <img src="https://s0.wp.com/latex.php?latex=G+%3D+%5Ctext%7BPSL%7D%282%2C%5Cmathbb%7BR%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G = &#92;text{PSL}(2,&#92;mathbb{R})" title="G = &#92;text{PSL}(2,&#92;mathbb{R})" class="latex" />, so that one component of <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BHom%7D%28%5Cpi%2CG%29%2FG&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{Hom}(&#92;pi,G)/G" title="&#92;text{Hom}(&#92;pi,G)/G" class="latex" /> is the Teichmüller space of hyperbolic structures on the surface <img src="https://s0.wp.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S" title="S" class="latex" />, one can take <img src="https://s0.wp.com/latex.php?latex=f+%3D+2%5Ccosh%5E%7B-1%7D%5Ctext%7Btr%2F2%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="f = 2&#92;cosh^{-1}&#92;text{tr/2}" title="f = 2&#92;cosh^{-1}&#92;text{tr/2}" class="latex" />, and then <img src="https://s0.wp.com/latex.php?latex=f_%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="f_&#92;alpha" title="f_&#92;alpha" class="latex" /> is just the length of the geodesic in the free homotopy class of <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" />, in the hyperbolic structure on <img src="https://s0.wp.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S" title="S" class="latex" /> associated to a representation. In this case, the symplectic structure on the character variety restricts to the Weil-Petersson symplectic structure on Teichmüller space, and the Hamiltonian flow associated to the length function <img src="https://s0.wp.com/latex.php?latex=f_%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="f_&#92;alpha" title="f_&#92;alpha" class="latex" /> is a family of Fenchel-Nielsen twists, i.e. the deformations of the hyperbolic structure obtained by cutting along the geodesic <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" />, rotating through some angle, and regluing. This latter observation recovers a famous theorem of <a href="http://www.ams.org/mathscinet-getitem?mr=0690844">Wolpert</a>, connected in an obvious way to his formula for the symplectic form <img src="https://s0.wp.com/latex.php?latex=%5Comega+%3D+%5Csum+dl_%5Calpha+%5Cwedge+d%5Ctheta_%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;omega = &#92;sum dl_&#92;alpha &#92;wedge d&#92;theta_&#92;alpha" title="&#92;omega = &#92;sum dl_&#92;alpha &#92;wedge d&#92;theta_&#92;alpha" class="latex" /> where <img src="https://s0.wp.com/latex.php?latex=%5Ctheta&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;theta" title="&#92;theta" class="latex" /> is angle and <img src="https://s0.wp.com/latex.php?latex=l&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="l" title="l" class="latex" /> is length, and the sum is taken over a maximal system of disjoint essential simple curves <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" /> for the surface <img src="https://s0.wp.com/latex.php?latex=S&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S" title="S" class="latex" />.</p>
<p>The combinatorial nature of the Goldman bracket suggests that it might have applications in combinatorial group theory. Turaev <a href="http://www.ams.org/mathscinet-getitem?mr=1062423">discovered</a> a Lie cobracket on <img src="https://s0.wp.com/latex.php?latex=%5Cmathbb%7BZ%7D%5Chat%7B%5Cpi%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathbb{Z}&#92;hat{&#92;pi}" title="&#92;mathbb{Z}&#92;hat{&#92;pi}" class="latex" />, and showed that together with the Goldman bracket, one obtains a Lie bialgebra. Motivated by Stallings&#8217; reformulation of the Poincaré conjecture in terms of group theory, Turaev asked whether a free homotopy class contains a power of a simple curve if and only if the cobracket of the class is zero. The answer to this question is negative, as shown by Chas; on the other hand, Chas and Krongold <a href="http://arxiv.org/abs/0801.3944">showed</a> that a class <img src="https://s0.wp.com/latex.php?latex=%5Calpha&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha" title="&#92;alpha" class="latex" /> is simple if and only if <img src="https://s0.wp.com/latex.php?latex=%5B%5Calpha%2C%5Calpha%5E3%5D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="[&#92;alpha,&#92;alpha^3]" title="[&#92;alpha,&#92;alpha^3]" class="latex" /> is zero. Nevertheless, the full geometric meaning of the Goldman bracket remains mysterious, and a topic worthy of investigation.</p>
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