<?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[Taut foliations and positive&nbsp;forms]]></title><type><![CDATA[link]]></type><html><![CDATA[<p>This week I visited Washington University in St. Louis to give a <a href="http://wumath.wustl.edu/node/608">colloquium</a>, and caught up with a couple of my old foliations friends, namely Rachel Roberts and Larry Conlon. Actually, I had caught up with Rachel (to some extent) the weekend before, when we both spoke at the <a href="http://www.ma.utexas.edu/tgtc2014/index.html">Texas Geometry and Topology Conference</a> in Austin, where Rachel gave a talk about her recent proof (joint with Will Kazez) that every <img src="https://s0.wp.com/latex.php?latex=C%5E0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C^0" title="C^0" class="latex" /> taut foliation on a 3-manifold <img src="https://s0.wp.com/latex.php?latex=M&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="M" title="M" class="latex" /> (other than <img src="https://s0.wp.com/latex.php?latex=S%5E2+%5Ctimes+S%5E1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S^2 &#92;times S^1" title="S^2 &#92;times S^1" class="latex" />) can be approximated by both positive and negative contact structures; it follows that <img src="https://s0.wp.com/latex.php?latex=M+%5Ctimes+I&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="M &#92;times I" title="M &#92;times I" class="latex" /> admits a symplectic structure with pseudoconvex boundary, and one deduces nontriviality of various invariants associated to <img src="https://s0.wp.com/latex.php?latex=M&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="M" title="M" class="latex" /> (Seiberg-Witten, Heegaard Floer Homology, etc.). This theorem was known for sufficiently smooth (at least <img src="https://s0.wp.com/latex.php?latex=C%5E2&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C^2" title="C^2" class="latex" />) foliations by Eliashberg-Thurston, as exposed in their <a href="http://www.ams.org/mathscinet-getitem?mr=1483314"><em>confoliations</em></a> monograph, and it is one of the cornerstones of <img src="https://s0.wp.com/latex.php?latex=3%2B1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="3+1" title="3+1" class="latex" />-dimensional symplectic geometry; unfortunately (fortunately?) many natural constructions of foliations on 3-manifolds can be done only in the <img src="https://s0.wp.com/latex.php?latex=C%5E1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C^1" title="C^1" class="latex" /> or <img src="https://s0.wp.com/latex.php?latex=C%5E0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C^0" title="C^0" class="latex" /> world. So the theorem of Rachel and Will is a big deal.</p>
<p>If we denote the foliation by <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" /> which is the kernel of a 1-form <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 suppose the approximating positive and negative contact structures are given by the kernels of 1-forms <img src="https://s0.wp.com/latex.php?latex=%5Calpha%5E%5Cpm&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha^&#92;pm" title="&#92;alpha^&#92;pm" class="latex" /> where <img src="https://s0.wp.com/latex.php?latex=%5Calpha%5E%2B+%5Cwedge+d%5Calpha%5E%2B+%3E+0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha^+ &#92;wedge d&#92;alpha^+ &gt; 0" title="&#92;alpha^+ &#92;wedge d&#92;alpha^+ &gt; 0" class="latex" /> and <img src="https://s0.wp.com/latex.php?latex=%5Calpha%5E-+%5Cwedge+d%5Calpha%5E-+%3C+0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha^- &#92;wedge d&#92;alpha^- &lt; 0" title="&#92;alpha^- &#92;wedge d&#92;alpha^- &lt; 0" class="latex" /> pointwise, the symplectic form <img src="https://s0.wp.com/latex.php?latex=%5Comega&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;omega" title="&#92;omega" class="latex" /> on <img src="https://s0.wp.com/latex.php?latex=M+%5Ctimes+I&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="M &#92;times I" title="M &#92;times I" class="latex" /> is given by the formula</p>
<p style="text-align:center;"><img src="https://s0.wp.com/latex.php?latex=%5Comega+%3D+%5Cbeta+%2B+%5Cepsilon+d%28t%5Calpha%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;omega = &#92;beta + &#92;epsilon d(t&#92;alpha)" title="&#92;omega = &#92;beta + &#92;epsilon d(t&#92;alpha)" class="latex" /></p>
<p>for some small <img src="https://s0.wp.com/latex.php?latex=%5Cepsilon&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;epsilon" title="&#92;epsilon" class="latex" />, where <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" /> is any closed 2-form on <img src="https://s0.wp.com/latex.php?latex=M&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="M" title="M" class="latex" /> which is (strictly) positive on <img src="https://s0.wp.com/latex.php?latex=T%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="T&#92;mathcal{F}" title="T&#92;mathcal{F}" class="latex" /> (and therefore also positive on the kernel of <img src="https://s0.wp.com/latex.php?latex=%5Calpha%5E%5Cpm&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;alpha^&#92;pm" title="&#92;alpha^&#92;pm" class="latex" /> if the contact structures approximate the foliation sufficiently closely). The existence of such a closed 2-form <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" /> is one of the well-known characterizations of tautness for foliations of 3-manifolds. I know several proofs, and at one point considered myself an expert in the theory of taut foliations. But when Cliff Taubes happened to ask me a few months ago which <em>cohomology classes</em> in <img src="https://s0.wp.com/latex.php?latex=H%5E2%28M%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H^2(M)" title="H^2(M)" class="latex" /> are represented by such forms <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 in particular whether the Euler class of <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" /> could be represented by such a form, I was embarrassed to discover that I had never considered the question before.</p>
<p>The answer is actually well-known and quite easy to state, and is one of the applications of Sullivan&#8217;s <a href="http://www.ams.org/mathscinet-getitem?mr=433464">theory of foliation cycles</a>. One can also give a more hands-on topological proof which is special to codimension 1 foliations of 3-manifolds. Since the theory of taut foliations of 3-manifolds is a somewhat lost art, I thought it would be worthwhile to write a blog post giving the answer, and explaining the proofs.</p>
<p><!--more--></p>
<p>To be a bit more precise, let me insist in what follows that <img src="https://s0.wp.com/latex.php?latex=M&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="M" title="M" class="latex" /> is closed and oriented, and that <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" /> is oriented and co-oriented. The smoothness of <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" /> is an issue in some of the arguments I will give, but I will not make a big deal of this. Then one has the following:</p>
<p><strong>Theorem:</strong> Let <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" /> be a foliation of a 3-manifold <img src="https://s0.wp.com/latex.php?latex=M&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="M" title="M" class="latex" /> as above. A cohomology class <img src="https://s0.wp.com/latex.php?latex=%5B%5Cbeta%5D+%5Cin+H%5E2%28M%3B%5Cmathbb%7BR%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="[&#92;beta] &#92;in H^2(M;&#92;mathbb{R})" title="[&#92;beta] &#92;in H^2(M;&#92;mathbb{R})" class="latex" /> is represented by a smooth closed 2-form <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" /> positive on <img src="https://s0.wp.com/latex.php?latex=T%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="T&#92;mathcal{F}" title="T&#92;mathcal{F}" class="latex" /> if and only if <img src="https://s0.wp.com/latex.php?latex=%5B%5Cbeta%5D%28%5Cmu%29%3E0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="[&#92;beta](&#92;mu)&gt;0" title="[&#92;beta](&#92;mu)&gt;0" class="latex" /> for every nontrivial transverse invariant measure <img src="https://s0.wp.com/latex.php?latex=%5Cmu&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu" title="&#92;mu" class="latex" /> for <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" />.</p>
<p>This requires a bit of explanation. A <em>transverse measure</em> <img src="https://s0.wp.com/latex.php?latex=%5Cmu&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu" title="&#92;mu" class="latex" /> assigns a non-negative number <img src="https://s0.wp.com/latex.php?latex=%5Cmu%28%5Csigma%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu(&#92;sigma)" title="&#92;mu(&#92;sigma)" class="latex" /> to any segment <img src="https://s0.wp.com/latex.php?latex=%5Csigma&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;sigma" title="&#92;sigma" class="latex" /> transverse to <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" />, which is countable additive on unions. Such a measure is <em>invariant</em> if it takes the same value on two transverse segments <img src="https://s0.wp.com/latex.php?latex=%5Csigma&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;sigma" title="&#92;sigma" class="latex" />, <img src="https://s0.wp.com/latex.php?latex=%5Csigma%27&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;sigma&#039;" title="&#92;sigma&#039;" class="latex" /> related to each other by holonomy transport; thus, a transverse measure is really a measure defined on the local leaf space of the foliation, which is compatible on the overlap of leaf space charts (one would like to think of it as a measure on the global leaf space space, but since this space is typically non-Hausdorff, one tends not to express things in such terms). If the foliation is orientable and co-orientable, we can define the measure on <em>oriented</em> transversals in such a way that changing the orientation changes the sign: <img src="https://s0.wp.com/latex.php?latex=%5Cmu%28%5Csigma%5E%7B-1%7D%29+%3D+-+%5Cmu%28%5Csigma%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu(&#92;sigma^{-1}) = - &#92;mu(&#92;sigma)" title="&#92;mu(&#92;sigma^{-1}) = - &#92;mu(&#92;sigma)" class="latex" />, where <img src="https://s0.wp.com/latex.php?latex=%5Csigma%5E%7B-1%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;sigma^{-1}" title="&#92;sigma^{-1}" class="latex" /> denotes <img src="https://s0.wp.com/latex.php?latex=%5Csigma&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;sigma" title="&#92;sigma" class="latex" /> with the opposite orientation. We still insist in this case that <img src="https://s0.wp.com/latex.php?latex=%5Cmu%28%5Csigma%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu(&#92;sigma)" title="&#92;mu(&#92;sigma)" class="latex" /> is non-negative whenever <img src="https://s0.wp.com/latex.php?latex=%5Csigma&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;sigma" title="&#92;sigma" class="latex" /> is positively oriented (with respect to the co-orientation).</p>
<p>Such a measure <img src="https://s0.wp.com/latex.php?latex=%5Cmu&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu" title="&#92;mu" class="latex" /> pairs with 1-chains, and the invariance property implies that it vanishes on 1-boundaries. Thus <img src="https://s0.wp.com/latex.php?latex=%5Cmu&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu" title="&#92;mu" class="latex" /> as above defines a 2-dimensional homology class <img src="https://s0.wp.com/latex.php?latex=%5B%5Cmu%5D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="[&#92;mu]" title="[&#92;mu]" class="latex" />, by how it pairs with 1-cycles, and appealing to Poincaré duality.</p>
<p>Here is another interpretation of an invariant transverse measure. Any compact subsurface <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" /> contained in a union of leaves of <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" /> determines a transverse measure <img src="https://s0.wp.com/latex.php?latex=%5Cmu_D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu_D" title="&#92;mu_D" class="latex" /> by defining <img src="https://s0.wp.com/latex.php?latex=%5Cmu_D%28%5Csigma%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu_D(&#92;sigma)" title="&#92;mu_D(&#92;sigma)" class="latex" /> to be the number of intersections of <img src="https://s0.wp.com/latex.php?latex=%5Csigma&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;sigma" title="&#92;sigma" class="latex" /> with <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" />, when <img src="https://s0.wp.com/latex.php?latex=%5Csigma&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;sigma" title="&#92;sigma" class="latex" /> is a positively-oriented transversal. Now, let&#8217;s suppose that <img src="https://s0.wp.com/latex.php?latex=D_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D_i" title="D_i" class="latex" /> is a sequence of compact subsurfaces in unions of leaves of <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" />, and suppose further that <img src="https://s0.wp.com/latex.php?latex=%5Ctext%7Blength%7D%28%5Cpartial+D_i%29%2F%5Ctext%7Barea%7D%28D_i%29+%5Cto+0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;text{length}(&#92;partial D_i)/&#92;text{area}(D_i) &#92;to 0" title="&#92;text{length}(&#92;partial D_i)/&#92;text{area}(D_i) &#92;to 0" class="latex" /> (i.e. the <img src="https://s0.wp.com/latex.php?latex=D_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D_i" title="D_i" class="latex" /> form a &#8220;Følner sequence&#8221; for <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" />). If we denote the area of <img src="https://s0.wp.com/latex.php?latex=D_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D_i" title="D_i" class="latex" /> by <img src="https://s0.wp.com/latex.php?latex=A_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="A_i" title="A_i" class="latex" />, we can define a sequence of measures <img src="https://s0.wp.com/latex.php?latex=%5Cmu_i%3A%3DA_i%5E%7B-1%7D%5Cmu_%7BD_i%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu_i:=A_i^{-1}&#92;mu_{D_i}" title="&#92;mu_i:=A_i^{-1}&#92;mu_{D_i}" class="latex" />, and then some subsequence will converge to a limiting transverse measure <img src="https://s0.wp.com/latex.php?latex=%5Cmu&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu" title="&#92;mu" class="latex" /> which is <em>invariant</em>. This is because most of the intersections of any transversal <img src="https://s0.wp.com/latex.php?latex=%5Csigma&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;sigma" title="&#92;sigma" class="latex" /> with <img src="https://s0.wp.com/latex.php?latex=D_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D_i" title="D_i" class="latex" /> (for big <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" />) are contained deep in the interior, so that any nearby <img src="https://s0.wp.com/latex.php?latex=%5Csigma%27&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;sigma&#039;" title="&#92;sigma&#039;" class="latex" /> intersects <img src="https://s0.wp.com/latex.php?latex=D_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D_i" title="D_i" class="latex" /> in almost the same number of points, and <img src="https://s0.wp.com/latex.php?latex=%5Cmu_i%28%5Csigma%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu_i(&#92;sigma)" title="&#92;mu_i(&#92;sigma)" class="latex" /> is very close to <img src="https://s0.wp.com/latex.php?latex=%5Cmu_i%28%5Csigma%27%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu_i(&#92;sigma&#039;)" title="&#92;mu_i(&#92;sigma&#039;)" class="latex" /> (here we really need to restrict attention to <img src="https://s0.wp.com/latex.php?latex=D_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D_i" title="D_i" class="latex" /> whose boundary is not too complicated; it is enough for it to have bounded geodesic curvature, for instance). We can think of each weighted surface <img src="https://s0.wp.com/latex.php?latex=A_i%5E%7B-1%7DD_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="A_i^{-1}D_i" title="A_i^{-1}D_i" class="latex" /> as a <em>de Rham</em> <em>2-chain</em> by how it pairs with smooth 2-forms; the limit converges to a well-defined de Rham 2-<em>cycle</em>, representing the 2-dimensional homology class <img src="https://s0.wp.com/latex.php?latex=%5B%5Cmu%5D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="[&#92;mu]" title="[&#92;mu]" class="latex" />. All invariant transverse measures are of this form. When expressed in this language, we refer to such invariant transverse measures as <em>foliation cycles</em>.</p>
<p>Thus one immediately sees one direction of the Theorem: if <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" /> is a closed 2-form strictly positive on every leaf of <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" />, it pairs (uniformly) positively with each <img src="https://s0.wp.com/latex.php?latex=A_i%5E%7B-1%7DD_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="A_i^{-1}D_i" title="A_i^{-1}D_i" class="latex" />, and therefore also with <img src="https://s0.wp.com/latex.php?latex=%5Cmu&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu" title="&#92;mu" class="latex" />.</p>
<p>The converse direction is also easy to see, modulo some functional analysis. A sketch of the idea is as follows. In the space <img src="https://s0.wp.com/latex.php?latex=V&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="V" title="V" class="latex" /> of de Rham 2-chains, the weighted surfaces carried by the foliation as above are dense in a closed convex <em>cone</em> <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" />. An element of the dual space <img src="https://s0.wp.com/latex.php?latex=%5Cbeta+%5Cin+V%5E%2A&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;beta &#92;in V^*" title="&#92;beta &#92;in V^*" class="latex" /> is positive on <img src="https://s0.wp.com/latex.php?latex=T%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="T&#92;mathcal{F}" title="T&#92;mathcal{F}" class="latex" /> if it is positive on <img src="https://s0.wp.com/latex.php?latex=C+-+0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C - 0" title="C - 0" class="latex" />. It is closed if it vanishes on all de Rham 2-boundaries <img src="https://s0.wp.com/latex.php?latex=B+%5Csubset+V&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="B &#92;subset V" title="B &#92;subset V" class="latex" />. Since <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" /> is closed, by the Hahn-Banach theorem such a <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" /> exists if and only if <img src="https://s0.wp.com/latex.php?latex=C+%5Ccap+B+%3D+0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="C &#92;cap B = 0" title="C &#92;cap B = 0" class="latex" />; equivalently, if and only if there is no foliation cycle <img src="https://s0.wp.com/latex.php?latex=%5Cmu&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu" title="&#92;mu" class="latex" /> representing 0 in (de Rham) homology. Such a <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" /> can be approximated by a smooth 2-form (since such forms are dense in <img src="https://s0.wp.com/latex.php?latex=V%5E%2A&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="V^*" title="V^*" class="latex" />) which is also positive on <img src="https://s0.wp.com/latex.php?latex=T%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="T&#92;mathcal{F}" title="T&#92;mathcal{F}" class="latex" />. A foliation with no null-homologous foliation cycle is said to be <em>homologically taut</em>, so we deduce that any homologically taut foliation admits a smooth closed form <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" /> positive on the leaves. But by the same reasoning, we can find <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" /> in a particular cohomology class <img src="https://s0.wp.com/latex.php?latex=%5B%5Cbeta%5D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="[&#92;beta]" title="[&#92;beta]" class="latex" /> if and only if <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" /> does not intersect the subspace <img src="https://s0.wp.com/latex.php?latex=Z_%7B%5B%5Cbeta%5D%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="Z_{[&#92;beta]}" title="Z_{[&#92;beta]}" class="latex" /> of de Rham 2-cycles pairing to zero with <img src="https://s0.wp.com/latex.php?latex=%5B%5Cbeta%5D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="[&#92;beta]" title="[&#92;beta]" class="latex" />. This concludes the sketch of the proof of the theorem; for details consult Sullivan&#8217;s paper, Thm.II.3.</p>
<p>Note that the theorem is very interesting even in the case that the foliation admits <em>no</em> invariant transverse measure. In some sense, this is the <em>generic</em> situation for a taut foliation of a 3-manifold; the existence of a nontrivial invariant transverse measure imposes strong (polynomial!) growth conditions on leaves in the support of the measure. In this case, <em>every</em> cohomology class is represented by a form positive on the leaves of the foliation.</p>
<p>It is worth pointing out an important application. A foliation is said to be <em>geometrically taut</em> if there exists a Riemannian metric for which all the leaves are minimal surfaces. A necessary and sufficient condition for this is the existence of a form <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" /> as above which is closed and positive on <img src="https://s0.wp.com/latex.php?latex=T%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="T&#92;mathcal{F}" title="T&#92;mathcal{F}" class="latex" />, and furthermore is <em>pure</em>: i.e. the kernel of <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" /> is a complementary subspace to <img src="https://s0.wp.com/latex.php?latex=T%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="T&#92;mathcal{F}" title="T&#92;mathcal{F}" class="latex" /> at each point. In codimension one this condition is vacuous, but in higher codimension Sullivan <a href="http://www.ams.org/mathscinet-getitem?mr=535056">shows</a> how to derive a pure (closed) form from an arbitrary one by an algebraic operation called <em>purification</em>. Anyway, from this one (i.e. Sullivan) deduces Sullivan&#8217;s theorem, to wit: a foliation is homologically taut if and only if it is geometrically taut. Note that this theorem is interesting even for 1-dimensional foliations &#8212; i.e. <em>flows</em>, since geometrically taut is equivalent to geodesibility of the flow.</p>
<p>The proof above is short, but the appeal to Hahn-Banach and the analytic details in Sullivan&#8217;s paper is unsatisfying. Here is the sketch of a topological argument which gets to the point. First consider a special case: s<span class="Apple-style-span">uppose some homologically trivial loop <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 transverse to <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" /> and intersects every leaf. Then we can find representatives of <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" /> that contain any tiny transverse segment, and by swapping a negative tiny segment of <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" /> for the (positive) rest of it, we can replace any loop with a homologically equivalent loop which is positive; in this case <em>every</em> class is representable. In the general case, the support of the nontrivial invariant transverse measures is some closed union of leaves, and we focus attention on a complementary open pocket. Because this pocket has no invariant transverse measure, lots of directions in many leaves have contracting holonomy; thus we can find small intervals <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" /> in the leaf space so that for every subinterval <img src="https://s0.wp.com/latex.php?latex=J+%5Csubset+I&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="J &#92;subset I" title="J &#92;subset I" class="latex" /> there is a pair of elements <img src="https://s0.wp.com/latex.php?latex=g%2Ch&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="g,h" title="g,h" class="latex" /> and a point <img src="https://s0.wp.com/latex.php?latex=p+%5Cin+I&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p &#92;in I" title="p &#92;in I" class="latex" /> so 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" /> takes <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 <img src="https://s0.wp.com/latex.php?latex=gp+%5Cin+I&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="gp &#92;in I" title="gp &#92;in I" class="latex" /> not equal to <img src="https://s0.wp.com/latex.php?latex=p&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="p" title="p" class="latex" />, and <img src="https://s0.wp.com/latex.php?latex=h&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="h" title="h" class="latex" /> takes the interval <img src="https://s0.wp.com/latex.php?latex=%5Bp%2Cgp%5D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="[p,gp]" title="[p,gp]" class="latex" /> properly inside <img src="https://s0.wp.com/latex.php?latex=J+%5Csubset+I&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="J &#92;subset I" title="J &#92;subset I" class="latex" />. Thus the commutator <img src="https://s0.wp.com/latex.php?latex=%5Bg%2Ch%5D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="[g,h]" title="[g,h]" class="latex" /> (which is homologically trivial) represents a transverse loop intersecting any given collection of leaves in the pocket. So by the argument above we can take any transverse loop which intersects the invariantly measured leaves positively, and replace it by a positively oriented transverse loop in the same homology class. </span></p>
<p>OK, back to 3-manifolds and cohomology classes. What about Taubes&#8217; question: when can the Euler class <img src="https://s0.wp.com/latex.php?latex=e%28%5Cmathcal%7BF%7D%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="e(&#92;mathcal{F})" title="e(&#92;mathcal{F})" class="latex" /> of <img src="https://s0.wp.com/latex.php?latex=T%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="T&#92;mathcal{F}" title="T&#92;mathcal{F}" class="latex" /> be represented by a form <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" /> positive on the leaves of <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" />? To answer this we need to talk about the Euler characteristic of a transverse measure, and the foliated Gauss-Bonnet theorem. Recall that the ordinary Gauss-Bonnet theorem says that for a closed oriented 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" /> we have an equality</p>
<p style="text-align:center;"><img src="https://s0.wp.com/latex.php?latex=%5Cint_S+K+d%5Ctext%7Barea%7D+%3D+2%5Cpi+%5Cchi%28S%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;int_S K d&#92;text{area} = 2&#92;pi &#92;chi(S)" title="&#92;int_S K d&#92;text{area} = 2&#92;pi &#92;chi(S)" class="latex" /></p>
<p style="text-align:left;">where <img src="https://s0.wp.com/latex.php?latex=K&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="K" title="K" class="latex" /> is the curvature of any Riemannian metric 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" />. For a surface with boundary there is a correction term, which involves the integral of the geodesic curvature over the boundary. If we apply this theorem to each of our surfaces <img src="https://s0.wp.com/latex.php?latex=D_i&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="D_i" title="D_i" class="latex" /> in turn we see that we can <em>define</em></p>
<p style="text-align:center;"><img src="https://s0.wp.com/latex.php?latex=%5Clim_%7Bi+%5Cto+%5Cinfty%7D+A_i%5E%7B-1%7D%5Cint_%7BD_i%7D+K+d%5Ctext%7Barea%7D+%3D%3A+%5Cchi%28%5Cmu%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;lim_{i &#92;to &#92;infty} A_i^{-1}&#92;int_{D_i} K d&#92;text{area} =: &#92;chi(&#92;mu)" title="&#92;lim_{i &#92;to &#92;infty} A_i^{-1}&#92;int_{D_i} K d&#92;text{area} =: &#92;chi(&#92;mu)" class="latex" /></p>
<p style="text-align:left;">On the other hand, if <img src="https://s0.wp.com/latex.php?latex=e%28S%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="e(S)" title="e(S)" class="latex" /> denotes the Euler class of <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" />, thought of as an element of <img src="https://s0.wp.com/latex.php?latex=H%5E2%28S%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="H^2(S)" title="H^2(S)" class="latex" />, then <img src="https://s0.wp.com/latex.php?latex=e%28S%29%5BS%5D+%3D+%5Cchi%28S%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="e(S)[S] = &#92;chi(S)" title="e(S)[S] = &#92;chi(S)" class="latex" />. Taking limits as above, we deduce the formula <img src="https://s0.wp.com/latex.php?latex=e%28%5Cmathcal%7BF%7D%29%5B%5Cmu%5D+%3D+%5Cchi%28%5Cmu%29&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="e(&#92;mathcal{F})[&#92;mu] = &#92;chi(&#92;mu)" title="e(&#92;mathcal{F})[&#92;mu] = &#92;chi(&#92;mu)" class="latex" /> for any foliation cycle <img src="https://s0.wp.com/latex.php?latex=%5Cmu&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu" title="&#92;mu" class="latex" />.</p>
<p style="text-align:left;">A theorem of Ghys says that for any Riemann surface lamination <img src="https://s0.wp.com/latex.php?latex=%5CLambda&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;Lambda" title="&#92;Lambda" class="latex" /> and any invariant transverse measure <img src="https://s0.wp.com/latex.php?latex=%5Cmu&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu" title="&#92;mu" class="latex" /> with <img src="https://s0.wp.com/latex.php?latex=%5Cchi%28%5Cmu%29%3E0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;chi(&#92;mu)&gt;0" title="&#92;chi(&#92;mu)&gt;0" class="latex" />, some positive measure of leaves must be 2-spheres. For a foliation of a 3-manifold, the Reeb stability theorem says that the existence of one spherical leaf implies that (up to taking double covers) the manifold is <img src="https://s0.wp.com/latex.php?latex=S%5E2+%5Ctimes+S%5E1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="S^2 &#92;times S^1" title="S^2 &#92;times S^1" class="latex" /> with the product foliation by spheres. So we can ignore this possibility by fiat.</p>
<p style="text-align:left;"><span class="Apple-style-span">If there is a transverse measure <img src="https://s0.wp.com/latex.php?latex=%5Cmu&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu" title="&#92;mu" class="latex" /> with <img src="https://s0.wp.com/latex.php?latex=%5Cchi%28%5Cmu%29%3D0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;chi(&#92;mu)=0" title="&#92;chi(&#92;mu)=0" class="latex" /> then a theorem of <a href="http://www.ams.org/mathscinet-getitem?mr=1235439">Candel</a> implies that some positive measure of leaves must be conformally parabolic. If we assume that the foliation is taut, then this implies that <img src="https://s0.wp.com/latex.php?latex=M&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="M" title="M" class="latex" /> contains an essential torus. So if we restrict attention to the &#8220;generic&#8221; case that <img src="https://s0.wp.com/latex.php?latex=M&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="M" title="M" class="latex" /> is a hyperbolic 3-manifold, then for any taut foliation <img src="https://s0.wp.com/latex.php?latex=%5Cmathcal%7BF%7D&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mathcal{F}" title="&#92;mathcal{F}" class="latex" />, every leaf is conformally hyperbolic. In this case, Candel shows that leafwise uniformization is continuous, so that <img src="https://s0.wp.com/latex.php?latex=M&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="M" title="M" class="latex" /> admits a metric in which every leaf has constant curvature <img src="https://s0.wp.com/latex.php?latex=-1&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="-1" title="-1" class="latex" />. In particular, every invariant transverse measure <img src="https://s0.wp.com/latex.php?latex=%5Cmu&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;mu" title="&#92;mu" class="latex" /> has <img src="https://s0.wp.com/latex.php?latex=%5Cchi%28%5Cmu%29%3C0&#038;bg=ffffff&#038;fg=000&#038;s=0" alt="&#92;chi(&#92;mu)&lt;0" title="&#92;chi(&#92;mu)&lt;0" class="latex" />. Thus for a (coorientable, orientable) taut foliation of a hyperbolic 3-manifold, the <em>negative</em> of the Euler class is <em>always </em>represented by a closed 2-form <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" />, positive on every leaf.</span></p>
<p style="text-align:left;">Feels like old times . . .</p>
<p style="text-align:center;"><a href="https://lamington.files.wordpress.com/2014/11/img_1919.jpg"><img data-attachment-id="2363" data-permalink="https://lamington.wordpress.com/2014/11/23/taut-foliations-and-positive-forms/img_1919/" data-orig-file="https://lamington.files.wordpress.com/2014/11/img_1919.jpg" data-orig-size="2592,1936" data-comments-opened="1" data-image-meta="{&quot;aperture&quot;:&quot;2.8&quot;,&quot;credit&quot;:&quot;&quot;,&quot;camera&quot;:&quot;iPhone 4&quot;,&quot;caption&quot;:&quot;&quot;,&quot;created_timestamp&quot;:&quot;1416516621&quot;,&quot;copyright&quot;:&quot;&quot;,&quot;focal_length&quot;:&quot;3.85&quot;,&quot;iso&quot;:&quot;1000&quot;,&quot;shutter_speed&quot;:&quot;0.066666666666667&quot;,&quot;title&quot;:&quot;&quot;,&quot;orientation&quot;:&quot;1&quot;}" data-image-title="IMG_1919" data-image-description="" data-medium-file="https://lamington.files.wordpress.com/2014/11/img_1919.jpg?w=300" data-large-file="https://lamington.files.wordpress.com/2014/11/img_1919.jpg?w=1024" class="alignnone size-large wp-image-2363" src="https://lamington.files.wordpress.com/2014/11/img_1919.jpg?w=1024&#038;h=765" alt="IMG_1919" srcset="https://lamington.files.wordpress.com/2014/11/img_1919.jpg?w=1024&amp;h=765 1024w, https://lamington.files.wordpress.com/2014/11/img_1919.jpg?w=2048&amp;h=1530 2048w, https://lamington.files.wordpress.com/2014/11/img_1919.jpg?w=150&amp;h=112 150w, https://lamington.files.wordpress.com/2014/11/img_1919.jpg?w=300&amp;h=224 300w, https://lamington.files.wordpress.com/2014/11/img_1919.jpg?w=768&amp;h=574 768w" sizes="(max-width: 1024px) 100vw, 1024px"   /></a>(some of) the old foliations gang together again &#8211; Renato Feres, me, Larry Conlon, and Rachel Roberts</p>
<p style="text-align:center;">
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