<?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[FH, T, FLp and all&nbsp;that]]></title><type><![CDATA[link]]></type><html><![CDATA[<p>I am (update: was) currently (update: but am no longer) in Brisbane for the &#8220;<a href="http://sites.google.com/site/ggtbrisbane/">New directions in geometric group theory</a>&#8221; conference, which has been an entirely enjoyable and educational experience. I got to eat fish and chips, to watch Australia make 520 for 7 (declared) against the West Indies at the WACA, and to hear Masato Mimura give a very nice talk about his recent results on rigidity of the &#8220;universal lattice&#8221;.</p>
<p>His talk included a quick and beautiful survey of some geometric aspects of the theory of rigidity for infinite groups, which I will attempt to partially reproduce (despite the limitations of the wordpress format). In this context, rigidity is expressed in terms of isometric affine actions of groups on Banach spaces. This means the following. Suppose <img src="https://s0.wp.com/latex.php?latex=B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B" title="B" class="latex" /> is a Banach space (i.e. a complete, normed vector space) 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 group. A <em>linear</em> isometric action is a representation <img src="https://s0.wp.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho" title="&#92;rho" class="latex" /> from <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> to the group of linear isometries of <img src="https://s0.wp.com/latex.php?latex=B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B" title="B" class="latex" /> &#8212; i.e. linear norm-preserving automorphisms. An <em>affine</em> action is a representation from <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> to the group of <em>affine</em> isometries of <img src="https://s0.wp.com/latex.php?latex=B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B" title="B" class="latex" /> &#8212; i.e. isometries as a metric space that do not necessarily fix the zero element. The group of isometries of a Banach space <img src="https://s0.wp.com/latex.php?latex=B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B" title="B" class="latex" /> is a semi-direct product <img src="https://s0.wp.com/latex.php?latex=B+%5Crtimes+U%28B%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B &#92;rtimes U(B)" title="B &#92;rtimes U(B)" class="latex" /> where <img src="https://s0.wp.com/latex.php?latex=U%28B%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="U(B)" title="U(B)" class="latex" /> is the group of linear isometries, and <img src="https://s0.wp.com/latex.php?latex=B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B" title="B" class="latex" /> is the Banach space, thought of as an Abelian group, acting on itself by (isometric) translations. Such an action is usually encoded by a pair <img src="https://s0.wp.com/latex.php?latex=%5Crho%3AG+%5Cto+U%28B%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho:G &#92;to U(B)" title="&#92;rho:G &#92;to U(B)" class="latex" /> which records the &#8220;linear&#8221; part of the action, and a 1-<em>cocycle</em> with coefficients in <img src="https://s0.wp.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho" title="&#92;rho" class="latex" />, i.e. a function <img src="https://s0.wp.com/latex.php?latex=c%3AG+%5Cto+B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="c:G &#92;to B" title="c:G &#92;to B" class="latex" /> satisfying <img src="https://s0.wp.com/latex.php?latex=c%28gh%29+%3D+c%28g%29+%2B+%5Crho%28g%29c%28h%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="c(gh) = c(g) + &#92;rho(g)c(h)" title="c(gh) = c(g) + &#92;rho(g)c(h)" class="latex" /> for every <img src="https://s0.wp.com/latex.php?latex=g%2Ch+%5Cin+G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="g,h &#92;in G" title="g,h &#92;in G" class="latex" />. This formula might look strange if you don&#8217;t know where it comes from: it is just the way that factors transform in semi-direct products. The affine action is given by sending <img src="https://s0.wp.com/latex.php?latex=g+%5Cin+G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="g &#92;in G" title="g &#92;in G" class="latex" /> to the transformation that sends each <img src="https://s0.wp.com/latex.php?latex=b+%5Cin+B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="b &#92;in B" title="b &#92;in B" class="latex" /> to <img src="https://s0.wp.com/latex.php?latex=%5Crho%28g%29b+%2B+c%28g%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho(g)b + c(g)" title="&#92;rho(g)b + c(g)" class="latex" />. Consequently, <img src="https://s0.wp.com/latex.php?latex=gh&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="gh" title="gh" class="latex" /> is sent to the transformation that sends <img src="https://s0.wp.com/latex.php?latex=b&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="b" title="b" class="latex" /> to <img src="https://s0.wp.com/latex.php?latex=%5Crho%28gh%29b+%2B+c%28gh%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho(gh)b + c(gh)" title="&#92;rho(gh)b + c(gh)" class="latex" /> and the fact that this is a group action becomes the formula</p>
<p><img src="https://s0.wp.com/latex.php?latex=%5Crho%28gh%29b+%2B+c%28gh%29+%3D+%5Crho%28g%29%28%5Crho%28h%29b+%2B+c%28h%29%29+%2B+c%28g%29+%3D+%5Crho%28gh%29b+%2B+%5Crho%28g%29c%28h%29+%2B+c%28g%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho(gh)b + c(gh) = &#92;rho(g)(&#92;rho(h)b + c(h)) + c(g) = &#92;rho(gh)b + &#92;rho(g)c(h) + c(g)" title="&#92;rho(gh)b + c(gh) = &#92;rho(g)(&#92;rho(h)b + c(h)) + c(g) = &#92;rho(gh)b + &#92;rho(g)c(h) + c(g)" class="latex" /></p>
<p>Equating the left and right hand sides gives the cocycle condition. Given one affine isometric action, one can obtain another in a silly way by conjugating by an isometry <img src="https://s0.wp.com/latex.php?latex=b+%5Cto+b+%2B+b%27&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="b &#92;to b + b&#039;" title="b &#92;to b + b&#039;" class="latex" /> for some <img src="https://s0.wp.com/latex.php?latex=b%27+%5Cin+B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="b&#039; &#92;in B" title="b&#039; &#92;in B" class="latex" />. Under conjugation by such an isometry, a cocycle <img src="https://s0.wp.com/latex.php?latex=c&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="c" title="c" class="latex" /> transforms by <img src="https://s0.wp.com/latex.php?latex=c%28g%29+%5Cto+c%28g%29+%2B+%5Crho%28g%29b%27+-+b%27&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="c(g) &#92;to c(g) + &#92;rho(g)b&#039; - b&#039;" title="c(g) &#92;to c(g) + &#92;rho(g)b&#039; - b&#039;" class="latex" />. A function of the form <img src="https://s0.wp.com/latex.php?latex=c%28g%29+%3D+%5Crho%28g%29b%27+-+b%27&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="c(g) = &#92;rho(g)b&#039; - b&#039;" title="c(g) = &#92;rho(g)b&#039; - b&#039;" class="latex" /> is called a 1-<em>coboundary</em>, and the quotient of the space of 1-cocycles by the space of 1-coboundaries is the 1 dimensional cohomology of <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> <em>with coefficients in</em> <img src="https://s0.wp.com/latex.php?latex=%5Crho%3AG+%5Cto+U%28B%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho:G &#92;to U(B)" title="&#92;rho:G &#92;to U(B)" class="latex" />. This is usually denoted <img src="https://s0.wp.com/latex.php?latex=H%5E1%28G%2C%5Crho%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H^1(G,&#92;rho)" title="H^1(G,&#92;rho)" class="latex" />, where <img src="https://s0.wp.com/latex.php?latex=B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B" title="B" class="latex" /> is suppressed in the notation. In particular, an affine isometric action of <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> on <img src="https://s0.wp.com/latex.php?latex=B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B" title="B" class="latex" /> with linear part <img src="https://s0.wp.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho" title="&#92;rho" class="latex" /> has a global fixed point iff it represents <img src="https://s0.wp.com/latex.php?latex=0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="0" title="0" class="latex" /> in <img src="https://s0.wp.com/latex.php?latex=H%5E1%28G%2C%5Crho%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H^1(G,&#92;rho)" title="H^1(G,&#92;rho)" class="latex" />. Contrapositively, <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" /> admits an affine isometric action on <img src="https://s0.wp.com/latex.php?latex=B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B" title="B" class="latex" /> without a global fixed point iff <img src="https://s0.wp.com/latex.php?latex=H%5E1%28G%2C%5Crho%29+%5Cne+0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H^1(G,&#92;rho) &#92;ne 0" title="H^1(G,&#92;rho) &#92;ne 0" class="latex" /> for some <img src="https://s0.wp.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho" title="&#92;rho" class="latex" />.</p>
<p>A group <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> is said to satisfy <em>Serre&#8217;s Property (FH) </em>if every affine isometric action of <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> on a Hilbert space has a global fixed point. In 2007, Bader-Furman-Gelander-Monod <a href="http://www.ams.org/mathscinet-getitem?mr=2316269">introduced</a> a property (FB) for a group <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> to mean that every affine isometric action of <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> on some (out of a class of) Banach space(s) <img src="https://s0.wp.com/latex.php?latex=B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B" title="B" class="latex" /> has a global fixed point. Mimura used the notation property (FL_p) for the case that <img src="https://s0.wp.com/latex.php?latex=B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B" title="B" class="latex" /> is allowed to range over the class of <img src="https://s0.wp.com/latex.php?latex=L_p&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="L_p" title="L_p" class="latex" /> spaces (for some fixed <img src="https://s0.wp.com/latex.php?latex=1+%3C+p+%3C+%5Cinfty&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="1 &lt; p &lt; &#92;infty" title="1 &lt; p &lt; &#92;infty" class="latex" />).</p>
<p>Intimately related is Kazhdan&#8217;s Property (T), introduced by Kazhdan in <a href="http://www.ams.org/mathscinet-getitem?mr=209390">this paper</a>. Let <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> be a locally compact topological group (for example, a discrete group). The set of irreducible unitary representations of <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> is called its <em>dual</em>, and denoted <img src="https://s0.wp.com/latex.php?latex=%5Chat%7BG%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;hat{G}" title="&#92;hat{G}" class="latex" />. This dual is topologized in the following way. Associated to a representation <img src="https://s0.wp.com/latex.php?latex=%5Crho%3AG+%5Cto+U%28L%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho:G &#92;to U(L)" title="&#92;rho:G &#92;to U(L)" class="latex" />, a unit vector <img src="https://s0.wp.com/latex.php?latex=X+%5Cin+L&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X &#92;in L" title="X &#92;in L" class="latex" />, a positive number <img src="https://s0.wp.com/latex.php?latex=%5Cepsilon+%3E+0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;epsilon &gt; 0" title="&#92;epsilon &gt; 0" class="latex" /> and a compact subset <img src="https://s0.wp.com/latex.php?latex=K+%5Csubset+G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="K &#92;subset G" title="K &#92;subset G" class="latex" /> there is an open neighborhood of <img src="https://s0.wp.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho" title="&#92;rho" class="latex" /> consisting of representations <img src="https://s0.wp.com/latex.php?latex=%5Crho%27%3AG+%5Cto+U%28L%27%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho&#039;:G &#92;to U(L&#039;)" title="&#92;rho&#039;:G &#92;to U(L&#039;)" class="latex" /> for which there is a unit vector <img src="https://s0.wp.com/latex.php?latex=Y+%5Cin+L&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="Y &#92;in L" title="Y &#92;in L" class="latex" /> such that <img src="https://s0.wp.com/latex.php?latex=%7C%5Clangle+%5Crho%28g%29X%2CX%5Crangle+-+%5Clangle+%5Crho%28g%27%29Y%2C+Y%5Crangle%7C+%3C+%5Cepsilon&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="|&#92;langle &#92;rho(g)X,X&#92;rangle - &#92;langle &#92;rho(g&#039;)Y, Y&#92;rangle| &lt; &#92;epsilon" title="|&#92;langle &#92;rho(g)X,X&#92;rangle - &#92;langle &#92;rho(g&#039;)Y, Y&#92;rangle| &lt; &#92;epsilon" class="latex" /> whenever <img src="https://s0.wp.com/latex.php?latex=g+%5Cin+K&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="g &#92;in K" title="g &#92;in K" class="latex" />. With this topology (called the <em>Fell topology</em>), one says that a group <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> has property (T) if the trivial representation is isolated in <img src="https://s0.wp.com/latex.php?latex=%5Chat%7BG%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;hat{G}" title="&#92;hat{G}" class="latex" />. Note that this topology is very far from being Hausdorff: the trivial representation fails to be isolated exactly when there are a sequence of representations <img src="https://s0.wp.com/latex.php?latex=%5Crho_i%3AG+%5Cto+U%28L_i%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho_i:G &#92;to U(L_i)" title="&#92;rho_i:G &#92;to U(L_i)" class="latex" />, unit vectors <img src="https://s0.wp.com/latex.php?latex=X_i+%5Cin+L_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X_i &#92;in L_i" title="X_i &#92;in L_i" class="latex" />, numbers <img src="https://s0.wp.com/latex.php?latex=%5Cepsilon_i+%5Cto+0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;epsilon_i &#92;to 0" title="&#92;epsilon_i &#92;to 0" class="latex" /> and compact sets <img src="https://s0.wp.com/latex.php?latex=K_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="K_i" title="K_i" class="latex" /> exhausting <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" /> so that <img src="https://s0.wp.com/latex.php?latex=%7C%5Clangle%5Crho_i%28g%29X_i%2CX_i%5Crangle%7C+%3C+%5Cepsilon_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="|&#92;langle&#92;rho_i(g)X_i,X_i&#92;rangle| &lt; &#92;epsilon_i" title="|&#92;langle&#92;rho_i(g)X_i,X_i&#92;rangle| &lt; &#92;epsilon_i" class="latex" /> for any <img src="https://s0.wp.com/latex.php?latex=g+%5Cin+K_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="g &#92;in K_i" title="g &#92;in K_i" class="latex" />. The vectors <img src="https://s0.wp.com/latex.php?latex=X_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="X_i" title="X_i" class="latex" /> are said to be (a sequence of) <em>almost invariant vectors</em>. Hence (informally) a group has property (T) if some compact subset must move some unit vector a definite amount in every irreducible nontrivial unitary representation. If a group fails to have property (T), one can rescale a sequence of irreducible actions near a sequence of almost invariant vectors in such a way that one obtains in the geometric limit a nontrivial isometric action on <img src="https://s0.wp.com/latex.php?latex=L%5E2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="L^2" title="L^2" class="latex" /> without a global fixed point. A famous theorem of <a href="http://www.ams.org/mathscinet-getitem?mr=578893">Delorme</a>&#8211;<a href="http://www.ams.org/mathscinet-getitem?mr=340464">Guichardet</a> says that property (T) and property (FH) are <em>equivalent</em> for (locally compact second countable) groups. Property (T) passes to quotients, and to lattices (i.e. finite covolume discrete subgroups of a topological group). Kazhdan already showed in his paper that <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BSL%7D%28n%2C%5Cmathbb%7BR%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{SL}(n,&#92;mathbb{R})" title="&#92;text{SL}(n,&#92;mathbb{R})" class="latex" /> has property (T) for <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" /> at least <img src="https://s0.wp.com/latex.php?latex=3&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="3" title="3" class="latex" />, and therefore the same is true for lattices in this groups, such as <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BSL%7D%28n%2C%5Cmathbb%7BZ%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{SL}(n,&#92;mathbb{Z})" title="&#92;text{SL}(n,&#92;mathbb{Z})" class="latex" />, a fact which is not easy to see directly from the definition. One beautiful application, already pointed out by Kazhdan, is that this means that all lattices in <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BSL%7D%28n%2C%5Cmathbb%7BR%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{SL}(n,&#92;mathbb{R})" title="&#92;text{SL}(n,&#92;mathbb{R})" class="latex" />, for instance the groups <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BSL%7D%28n%2C%5Cmathbb%7BZ%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{SL}(n,&#92;mathbb{Z})" title="&#92;text{SL}(n,&#92;mathbb{Z})" class="latex" /> (and in fact, all discrete groups with property (T)) are finitely generated. Kazhdan&#8217;s proof of this is incredibly short: let <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> be a discrete group and <img src="https://s0.wp.com/latex.php?latex=g_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="g_i" title="g_i" class="latex" /> and sequence of elements. For each <img src="https://s0.wp.com/latex.php?latex=i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="i" title="i" class="latex" />, let <img src="https://s0.wp.com/latex.php?latex=G_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G_i" title="G_i" class="latex" /> be the subgroup of <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> generated by <img src="https://s0.wp.com/latex.php?latex=%5Clbrace+g_1%2Cg_2%2C%5Ccdots%2Cg_i%5Crbrace&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;lbrace g_1,g_2,&#92;cdots,g_i&#92;rbrace" title="&#92;lbrace g_1,g_2,&#92;cdots,g_i&#92;rbrace" class="latex" />. Notice that <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> is finitely generated iff <img src="https://s0.wp.com/latex.php?latex=G_i%3DG&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G_i=G" title="G_i=G" class="latex" /> for all sufficiently large <img src="https://s0.wp.com/latex.php?latex=i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="i" title="i" class="latex" />. On the other hand, consider the unitary representations of <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> induced by the trivial representations on the <img src="https://s0.wp.com/latex.php?latex=G_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G_i" title="G_i" class="latex" />. Every compact subset of <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> is finite, and therefore eventually fixes a vector in every one of these representations; thus there is a sequence of almost fixed vectors. 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" /> has property (T), this sequence eventually contains a fixed vector, which can only happen if <img src="https://s0.wp.com/latex.php?latex=G%2FG_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G/G_i" title="G/G_i" class="latex" /> is finite, in which case <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 finitely generated, as claimed.</p>
<p>Property (FL_p) generalizes (FH) (equivalently (T)) in many significant ways, with interesting applications to dynamics. For example, Navas <a href="http://www.ams.org/mathscinet-getitem?mr=1951442">showed</a> that 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 a group with property (T) then every action of <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> on a circle which is at least <img src="https://s0.wp.com/latex.php?latex=C%5E%7B1%2B1%2F2+%2B+%5Cepsilon%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C^{1+1/2 + &#92;epsilon}" title="C^{1+1/2 + &#92;epsilon}" class="latex" /> factors through a finite group. Navas&#8217;s argument can be generalized straightforwardly to show that 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" /> has (FL_p) for some <img src="https://s0.wp.com/latex.php?latex=p%3E2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p&gt;2" title="p&gt;2" class="latex" /> then every action of <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" /> on a circle which is at least <img src="https://s0.wp.com/latex.php?latex=C%5E%7B1%2B1%2Fp%2B%5Cepsilon%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C^{1+1/p+&#92;epsilon}" title="C^{1+1/p+&#92;epsilon}" class="latex" /> factors through a finite group. The proof rests on a beautiful construction due to <a href="http://arxiv.org/abs/math/0001135">Reznikov</a> (although a similar construction can be found in <a href="http://www.ams.org/mathscinet-getitem?mr=900587">Pressley-Segal</a>) of certain functions on a configuration space of the circle which are not in <img src="https://s0.wp.com/latex.php?latex=L%5Ep&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="L^p" title="L^p" class="latex" /> but have coboundaries which are; this gives rise to nontrivial cohomology with <img src="https://s0.wp.com/latex.php?latex=L%5Ep&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="L^p" title="L^p" class="latex" /> coefficients for groups acting on the circle in a sufficiently interesting way.</p>
<p>(Update: Nicolas Monod points out in an email that the &#8220;function on a configuration space&#8221; is morally just the derivative. In fact, he made the nice remark that if <img src="https://s0.wp.com/latex.php?latex=D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D" title="D" class="latex" /> is any elliptic operator on an <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" />-manifold, then the commutator <img src="https://s0.wp.com/latex.php?latex=%5BD%2Cg%5D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="[D,g]" title="[D,g]" class="latex" /> is of <a href="http://en.wikipedia.org/wiki/Schatten_class_operator">Schatten class</a> <img src="https://s0.wp.com/latex.php?latex=%28n%2B1%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="(n+1)" title="(n+1)" class="latex" /> whenever <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 sufficiently smooth function; morally this should give rise to nontrivial cohomology with suitable coefficients for groups acting with enough regularity on any given <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" />-manifold, and one would like to use this e.g. to approach Zimmer&#8217;s conjecture, but nobody seems to know how to make this work as yet; in fact the work of Monod et. al. on (FL_p) is at least partly motivated by this general picture.)</p>
<p>Mimura discussed a spectrum of rigid behaviour for infinite groups, ranging from most rigid (property (FL_p) for every <img src="https://s0.wp.com/latex.php?latex=p&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p" title="p" class="latex" />) to least rigid (amenable) (note: every finite group is both amenable and has property (T), so this only really makes sense for infinite groups; moreover, every reasonable measure of rigidity for infinite groups is usually invariant under passing to subgroups of finite index). Free groups, <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BSL%7D%282%2C%5Cmathbb%7BZ%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{SL}(2,&#92;mathbb{Z})" title="&#92;text{SL}(2,&#92;mathbb{Z})" class="latex" /> and so on are very non-rigid. However, it is well-known that certain infinite families of (word) hyperbolic groups, including lattices in groups of isometries of quaternion-hyperbolic symmetric spaces, and &#8220;random&#8221; groups with relations having density parameter <img src="https://s0.wp.com/latex.php?latex=1%2F3+%3C+d+%3C+1%2F2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="1/3 &lt; d &lt; 1/2" title="1/3 &lt; d &lt; 1/2" class="latex" /> (see <a href="http://www.ams.org/mathscinet-getitem?mr=1995802">Zuk</a> or <a href="http://www.yann-ollivier.org/rech/publs/randomgroups.pdf">Ollivier</a>) are both hyperbolic and have property (T). Nevertheless, these groups are not as rigid as higher rank lattices like <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BSL%7D%28n%2C%5Cmathbb%7BZ%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{SL}(n,&#92;mathbb{Z})" title="&#92;text{SL}(n,&#92;mathbb{Z})" class="latex" /> for <img src="https://s0.wp.com/latex.php?latex=n%3E2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n&gt;2" title="n&gt;2" class="latex" />. The latter have property (FL_p) for every <img src="https://s0.wp.com/latex.php?latex=1%3C+p+%3C+%5Cinfty&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="1&lt; p &lt; &#92;infty" title="1&lt; p &lt; &#92;infty" class="latex" />, whereas Yu <a href="http://www.ams.org/mathscinet-getitem?mr=2221161">showed</a> that <em>every</em> hyperbolic group admits a proper affine isometric action on <img src="https://s0.wp.com/latex.php?latex=%5Cell%5Ep&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;ell^p" title="&#92;ell^p" class="latex" /> for some <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" /> (the existence of a proper affine isometric action on a Hilbert space is called &#8220;a-T-menability&#8221; by Gromov, and the &#8220;Haagerup property&#8221; by some. Groups satisfying this property, or even Yu&#8217;s weaker property, are known to satisfy some version of the Baum-Connes conjecture, the subject of a very nice minicourse by Graham Niblo at the same conference).</p>
<p>It is in this context that one can appreciate Mimura&#8217;s <a href="http://arxiv.org/abs/0904.4650">results</a>. His first main result is that the group <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BSL%7D_n%28%5Cmathbb%7BZ%7D%5Bx_1%2Cx_2%2C%5Ccdots%2Cx_n%5D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{SL}_n(&#92;mathbb{Z}[x_1,x_2,&#92;cdots,x_n])" title="&#92;text{SL}_n(&#92;mathbb{Z}[x_1,x_2,&#92;cdots,x_n])" class="latex" /> (i.e. the &#8220;universal lattice&#8221;) has property (FL_p) for every <img src="https://s0.wp.com/latex.php?latex=1%3Cp%3C%5Cinfty&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="1&lt;p&lt;&#92;infty" title="1&lt;p&lt;&#92;infty" class="latex" /> provided <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" /> is at least 4. Since property (FL_p) (like (T)) passes to quotients, this implies that <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7BSL%7D_n%28R%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{SL}_n(R)" title="&#92;text{SL}_n(R)" class="latex" /> has (FL_p) for every unital, commutative, finitely generated ring <img src="https://s0.wp.com/latex.php?latex=R&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="R" title="R" class="latex" />.</p>
<p>His second main result concerns a &#8220;quasification&#8221; of FL_p, to a property called (FFL_p). Without getting too technical, this property concerns &#8220;quasi-actions&#8221; of a group on a Banach space by affine isometries; algebraically these are encoded by 1-cochains <img src="https://s0.wp.com/latex.php?latex=c%3AG+%5Cto+B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="c:G &#92;to B" title="c:G &#92;to B" class="latex" /> for which there is a universal constant <img src="https://s0.wp.com/latex.php?latex=D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D" title="D" class="latex" /> so that <img src="https://s0.wp.com/latex.php?latex=%7Cc%28gh%29+-+c%28g%29+-%5Crho%28g%29c%28h%29%7C+%3C+D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="|c(gh) - c(g) -&#92;rho(g)c(h)| &lt; D" title="|c(gh) - c(g) -&#92;rho(g)c(h)| &lt; D" class="latex" /> as measured in the Banach norm on <img src="https://s0.wp.com/latex.php?latex=B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B" title="B" class="latex" />. Any bounded map <img src="https://s0.wp.com/latex.php?latex=c%3AG+%5Cto+B&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="c:G &#92;to B" title="c:G &#92;to B" class="latex" /> defines a 1-cochain; such (bounded) 1-cochains corresponds to  quasi-action with a bounded orbit. Associated to <img src="https://s0.wp.com/latex.php?latex=%5Crho%3A+G+%5Cto+U%28B%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho: G &#92;to U(B)" title="&#92;rho: G &#92;to U(B)" class="latex" /> one defines in a similar way a complex of bounded cochains; quasi-actions modulo bounded quasi-actions are parameterized by the kernel of the comparison map <img src="https://s0.wp.com/latex.php?latex=H%5E2_b%28G%2C%5Crho%29+%5Cto+H%5E2%28G%2C%5Crho%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H^2_b(G,&#92;rho) &#92;to H^2(G,&#92;rho)" title="H^2_b(G,&#92;rho) &#92;to H^2(G,&#92;rho)" class="latex" /> from bounded to ordinary cohomology. Mimura&#8217;s second main result is that when <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 the universal lattice as above, and <img src="https://s0.wp.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho" title="&#92;rho" class="latex" /> has no invariant vectors, the comparison map from bounded to ordinary cohomology in dimension 2 is injective.</p>
<p>The fact that <img src="https://s0.wp.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho" title="&#92;rho" class="latex" /> as above is required to have no invariant vectors is a technical necessity of Mimura&#8217;s proof. When <img src="https://s0.wp.com/latex.php?latex=%5Crho&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;rho" title="&#92;rho" class="latex" /> is trivial, one is studying &#8220;ordinary&#8221; bounded cohomology, and there is an exact sequence</p>
<p style="padding-left:30px;"><img src="https://s0.wp.com/latex.php?latex=0+%5Cto+H%5E1%28G%29+%5Cto+Q%28G%29+%5Cto+H%5E2_b%28G%29+%5Cto+H%5E2%28G%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="0 &#92;to H^1(G) &#92;to Q(G) &#92;to H^2_b(G) &#92;to H^2(G)" title="0 &#92;to H^1(G) &#92;to Q(G) &#92;to H^2_b(G) &#92;to H^2(G)" class="latex" /></p>
<p>with real coefficients for any <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" /> (here <img src="https://s0.wp.com/latex.php?latex=Q%28G%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="Q(G)" title="Q(G)" class="latex" /> denotes the vector space of homogeneous quasimorphisms on <img src="https://s0.wp.com/latex.php?latex=G&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="G" title="G" class="latex" />). In this context, one knows by Bavard duality that <img src="https://s0.wp.com/latex.php?latex=H%5E2_b+%5Cto+H%5E2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H^2_b &#92;to H^2" title="H^2_b &#92;to H^2" class="latex" /> is injective if and only if the <em>stable commutator length</em> is identically zero on <img src="https://s0.wp.com/latex.php?latex=%5BG%2CG%5D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="[G,G]" title="[G,G]" class="latex" />. By quite a different method, Mimura <a href="http://arxiv.org/abs/0911.1341">shows</a> that for <img src="https://s0.wp.com/latex.php?latex=n&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="n" title="n" class="latex" /> at least <img src="https://s0.wp.com/latex.php?latex=6&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="6" title="6" class="latex" />, and for any Euclidean ring <img src="https://s0.wp.com/latex.php?latex=R&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="R" title="R" class="latex" /> (i.e. a ring for which one has a Euclidean algorithm; for example, <img src="https://s0.wp.com/latex.php?latex=R+%3D+%5Cmathbb%7BC%7D%5Bx%5D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="R = &#92;mathbb{C}[x]" title="R = &#92;mathbb{C}[x]" class="latex" />) the group <img src="https://s0.wp.com/latex.php?latex=SL_n%28R%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="SL_n(R)" title="SL_n(R)" class="latex" /> has vanishing stable commutator length, and therefore one has injectivity of bounded to ordinary cohomology in dimension <img src="https://s0.wp.com/latex.php?latex=2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="2" title="2" class="latex" />.</p>
<p><strong>(Update 1/9/2010):</strong> Nicholas Monod sent me a nice email commenting on a couple of points in this blog entry, and I have consequently modified the language a bit in a few places. Ta much!</p>
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