\documentclass{amsart} \input{diagrams} \begin{document} \title{Syllabus for Qualifying Exam} \author{Danny Calegari} \maketitle {\bf Exam Committee: Andrew Casson, Robion Kirby, Curtis McMullen, Steven Evans (Statistics)} \vskip 12pt {\bf Monday 26th February, 3:00 pm} \vskip 24pt \section{Major Area: Algebraic Topology} \begin{itemize} \item{Fundamental group and higher homotopy groups} For each space $X$ we can define $\pi_n(X)$ to be the space $[S^n,X]_0$ of homotopy classes of based maps $S^n \to X$. Denoting the loop space of $X$ by $\Omega X$ and the suspension by $\Sigma X$, we have the general fact $$[X,\Omega Y]_0 \cong [\Sigma X,Y]_0$$ Moreover, for $n\ge 2$, $\pi_n(X)$ is abelian. \item{Seifert-VanKampen theorem} If $X$ is obtained from $X_1$ and $X_2$ by glueing along $A$, then if $A$ is connected, we have the SVK theorem: $$\pi_1(X) = \pi_1(X_1) *_{\pi_1(A)} \pi_1(X_2)$$ Related to this is the concept of a HNN extension - if $Y$ is obtained from $X$ by gluing a subspace $A$ to itself, then $$\pi_1(Y) = \pi_1(X) *_{\pi_1(A)}$$ \item{Subgroups of fundamental group and covering spaces} For each subgroup $G$ of $\pi_1(X)$ there is a space $X_G$ with $\pi_1(X_G) = G$ such that there is a covering map $\pi: X_G \to X$. If $G$ is a normal subgroup, then the group $\Gamma = \pi_1(X)/G$ acts properly discontinuously on $X_G$ and we have $X_G/\Gamma = X$. \item{Homotopy exact sequence} For any pair of spaces $(X,A)$ there is a long exact sequence $$ \dots \to \pi_n(A) \to \pi_n(X) \to \pi_n(X,A) \to \pi_{n-1}(A) \to \dots $$ This map is an exact sequence of $\pi_1(A)$-modules. For $n>2$, $\pi_n(X,A)$ is abelian. \item{Homology groups: Singular, Cellular, Simplicial} We define the singular homology groups of a space $X$ with coefficients in an abelian group $G$ as follows. Let $C_i$ be the free $G$-module generated by maps from $i$-simplices $\sigma: \Delta_i \to X$. We define a boundary operator $\partial: C_i \to C_{i-1}$ by the formula $$\partial \sigma = \Sigma_j (-1)^j \sigma^j$$ where $\sigma^j$ is the $j$'th $i-1$-face of $\sigma$. Then $\partial \circ \partial = 0$ and we define $$H_i(X,G) = ker(\partial_i)/ im(\partial_{i+1})$$ For a CW-complex $W$, we define the chain complex $$\dots \to H_i(W^i,W^{i-1}) \to H_{i-1}(W^{i-1},W^{i-2}) \to \dots$$ Then the homology of this complex (the Cellular homology of $W$) is isomorphic to the singular homology of $W$. \item{Mayer-Vietoris sequence} There is a long exact sequence in homology for a pair $X_1,X_2$ such that $X_1 \cup X_2 = X$, $X_1 \cap X_2 = A$ obtained by splicing together the long exact sequences of $(X,X_1)$ and $(X_2,A)$ whose $3i$ terms are isomorphic, by excision. This sequence $$\dots \to H_i(A) \to H_i(X_1) \oplus H_i(X_2) \to H_i(X) \to H_{i-1}(A) \to \dots$$ is known as the Mayer-Vietoris sequence. \item{Morse theory (handlebody decomposition)} On any manifold $M$ there exists a function $f$ (in fact, many functions) known as a Morse Function, such that the critical points of $f$ are isolated, and such that for each critical point $p$, there are local co-ordinates on $M$ such that $f$ takes the form $$f(x_1,x_2 \dots x_n) = x_1^2 + \dots + x_i^2 - x_{i+1}^2 - \dots - x_n^2$$ We say that $p$ is a critical point of index $n-i$. Then $M$ has the homotopy type of a CW complex with one cell of dimension $p$ for each critical point of index $p$. The theory of normal surfaces in three-manifolds can be described with respect to how a surface intersects the $0,1,2$ handles of a handle decomposition. \item{Cohomology groups: Singular, Cellular, Simplicial} We define the $i$-cochains of a space $X$ to be the elements of the dual to the $i$-chains, namely $C_i^*$. Then there is a map $\delta: C_i^* \to C_{i+1}^*$ which is simply the adjoint of $\partial$ under the natural pairing. As above, we define $$H^i(X) = ker(\delta_i)/im(\delta_{i-1})$$ Similarly, cellular cohomology is defined to be the cohomology of the cell complex $$ \dots \to H^i(W^i,W^{i-1}) \to H^{i+1}(W^{i+1},W^i) \to \dots $$ \item{De Rham cohomology and Cech cohomology} On a differentiable manifold $M$ we can define the algebra of exterior forms $\Omega^*(M)$ which is a graded algebra whose $i$'th component is given by the differential forms of degree $i$: $$fdx_{r_1} \wedge dx_{r_2} \wedge dx_{r_3} \wedge \dots \wedge dx_{r_i}$$ Multiplication in this algebra is given by the wedge product, and there is a differential operator $d$ which acts as follows: $$d:fdx_{r_1}\wedge \dots \wedge dx_{r_i} = \Sigma_j \partial f/ \partial x_j dx_j \wedge dx_{r_1} \wedge \dots \wedge dx_{r_i}$$ The closed forms are those whose image under $d$ is zero. The De Rham cohomology of $M$ is precisely the cohomology of the differential complex $$\dots \to \Omega^n(M) \to \Omega^{n+1}(M) \to \dots$$ with differential operator $d$. The Cech cohomology of a space with coefficients in $\Bbb(R)$ is the cohomology of the complex $$ \dots \to C^i(U,{\Bbb R}) \to C^{i+1}(U,{\Bbb R}) \to \dots$$ where $U$ is a good open covering of $M$ (i.e. every open set and intersection of open sets is contractible), and the elements of $C^{i}(U,{\Bbb R})$ are the locally constant functions on the $i+1$-fold intersections of open sets. More generally, for some sheaf $\Omega$, the cohomology of the complex $$\dots \to C^i(U,\Omega) \to C^{i+1}(U,\Omega) \to \dots$$ computes the Cech cohomology of $M$ with coefficients in $\Omega$, where $C^i(U,\Omega)$ is the sections of the sheaf $\Omega$ over the $i+1$-fold intersections. Note the following important theorem: a sheaf $\mathcal{F}$ on a topological space $X$ is {\it flasque} if for every inclusion of open sets $V \subset U$ the restriction map $\mathcal{F}(U) \to \mathcal{F}(V)$ is surjective. Then the Cech cohomology of a space with coefficients in a flasque sheaf are zero. Moreover, if we have a short exact sequence of sheaves $$0 \to \mathcal{F} \to \mathcal{G} \to \mathcal{H} \to 0$$ then this induces a long exact sequence of cohomology: $$ \dots \to H^i(X,\mathcal{F}) \to H^i(X,\mathcal{G}) \to H^i(X,\mathcal{H}) \to H^{i+1}(X, \mathcal{F}) \to \dots $$ Generally, we have the following construction. To define $H^*(X,\mathcal{S})$ with $\mathcal{S}$ a sheaf of $K$-modules, let $\mathcal{K}$ be the trivial $K$-sheaf on $X$, and let $$0 \to \mathcal{K} \to \mathcal{C}_0 \to \mathcal{C}_1 \to \dots$$ be a fine resolution of $\mathcal{K}$. Then $H^*(X,\mathcal{S})$ is the cohomology of the complex $$0 \to \Gamma(\mathcal{C}_0 \otimes \mathcal{S}) \to \Gamma(\mathcal{C}_1 \otimes \mathcal{S}) \to \dots$$ \item{Hurewicz theorem (statement)} $$H_1(X,{\Bbb Z}) \cong \pi_1(X) / [\pi_1(X),\pi_1(X)]$$ Moreover, in general if the first $n-1$ homotopy groups of $X$ vanish, then the first $n-1$ homology groups of $X$ with coefficients in ${\Bbb Z}$ vanish, and the natural map $f: \pi_n(X) \to H_n(X,{\Bbb Z})$ is an isomorphism. We also have the Relative Hurewicz theorem; namely, if $\pi_1(A) = 1$ and $\pi_i(X,A) = 1$ for $i 0,\ne 0),(>0,=0),(=0,\ne 0),(=0,=0),(>0,\ne 0),(>0,=0)$$ then the geometric structure will be $${\Bbb S}^3, {\Bbb S}^2 \times {\Bbb R}, Nil, {\Bbb E}^3, {\widetilde SL}_2({\Bbb R}), {\Bbb H}^2 \times {\Bbb R}$$ If the piece is covered by a torus-bundle over $S^1$ with Anosov monodromy, it has a $Sol$ structure. Finally, if it is none of these things, it admits a hyperbolic structure. Note also that every $M$ with $|\pi_1(M)| < \infty$ should be covered by ${\Bbb S}^3$ as $M = {\Bbb S}^3/\Gamma$ with $\Gamma \subset SO(4)$ Note: this theorem has been proved for Haken manifolds, for surface bundles over $S^1$ and for manifolds admitting a group action which is free on the complement of a codimension 2 set. It is a theorem of Thurston that the geometries indicated above are the only maximal simply connected manifolds admitting a compact manifold quotient for which the group of isometries acts transitively on the points of the space. Note that the manifold $P^3 + P^3$ though not prime, admits a $S^2 \times R$ structure. \item{Geometrization of Seifert-fibered pieces (i.e. classification by Euler characteristic of base orbifold and Euler number of circle bundle) (statement)} As above. Note that for Seifert-fibered pieces the Geometrization Conjecture holds. Every Seifert-fibered manifold is Haken unless it has base space a triangle orbifold and has $H_1$ finite. Also, we have the formula for the Euler number $e(E) = -(b + \Sigma_i \beta_i /\alpha_i)$ and the base orbifold has marked points with angles $2 \pi/\alpha_i$, for a standard surgery presentation of the manifold. \item{Mostow's rigidity theorem} For $n\ge 3$ every finite volume hyperbolic manifold $M$ admits a unique hyperbolic structure. In particular, if $M$, $N$ are two finite volume hyperbolic manifolds and their fundamental groups are isomorphic, then there is an isometry between them. Note that because $M$,$N$ are $K(\pi,1)$'s, they are homotopy equivalent by the hypothesis. The proof proceeds as follows in the case $M,N$ are compact: \begin{enumerate} \item{First we lift a homotopy equivalence $f:M \to N$ to the universal covers. This map is then a quasi-isometry, since in one direction, it magnifies lengths by a bounded amount, and then in the other direction, its inverse magnifies lengths by a bounded amount and moreover is, up to some constant, an inverse to $f$. It can be shown that a quasi-isometry extends continuously to a map from $\bar {\Bbb H}^3$ to itself (i.e. it extends continuously to the boundary)} \item{Next we show that the following equality holds: $$vol(M) = vol(N) vol(\sigma)/average(vol(f(\sigma)))$$ Where $v$ is the volume of a regular ideal hyperbolic simplex, and the average is with respect to some set of coset representatives for $f$ under the action of $\Gamma_1$. In particular, it is the average volume of the {\it straightened} simplices with the same endpoints as $f(\sigma)$ where $\sigma$ ranges over the regular ideal simplices of ${\Bbb H}^3$. To see this, observe that we can define a cycle $\alpha$ by $$\alpha = \int_{\Gamma/G} sign(g) \pi(g\sigma) dg$$ Then this is clearly closed and we have a homology class $[\alpha]$. Now we can evaluate this against the volume form $\Omega$ to obtain $$<[\alpha],\Omega> = \int sign(g) \int_{\pi(g\sigma)} sign(g) \Omega dg$$ $$= \int volume(g\sigma) dg$$ $$= volume(\sigma)$$ Now, evaluating its (straightened) image (which defines the same homology class) against the volume form $\Omega'$ of $N$ we get $$ = average(volume(f\sigma))$$ However, we have $$h^* \Omega' = \Omega vol(N)/vol(M)$$ So that we have $$ = <[\alpha],h^*\Omega'>$$ $$= (vol(N)/vol(M))<[\alpha],\Omega>$$ $$= (vol(N)/vol(M))(vol(\sigma))$$ Therefore the estimate $$vol(M) = vol(N) volume(\sigma)/average(volume(f\sigma))$$ Since $\sigma$ can have volume as close to the maximum possible as we like, we can see that $vol(N)\le vol(M)$. Similarly, $vol(M) \le vol(N)$. Therefore $vol(M)=vol(N)$ and $f$ takes ideal simplices to ideal simplices.} \item{Finally, any map which preserves ideal simplices is an isometry and we are done, by extending the action of $\partial {\Bbb H}^3$ to all of ${\Bbb H}^3$.} Note since $M,N$ are $K(\Pi,1)$'s, any isomorphism of their fundamental groups implies they are homotopy equivalent, and therefore isometric. \end{enumerate} \item{Margulis' lemma} This theorem states that there is a universal constant $\epsilon$ such that for $\Gamma$ a discrete group of isometries of ${\Bbb H}^3$, the subgroup $\Gamma_\epsilon$ which is generated by elements which translate points a distance $\le \epsilon$ is virtually nilpotent. (That is, it contains a subgroup of finite index which is nilpotent). A brief sketch of a proof is given as follows: \begin{enumerate} \item{For any Lie group $G$, the differential of the lie bracket as a smooth function $[,]:G\times G \to G$ at the identity is zero. For, $[g,id] = id$ and $[id,g] = id$ for all $g$, and the tangents to these subspaces span the tangent space to $id \times id$. Hence for elements $g,h$ sufficiently close to $0$, $d([g,h],id) \le 1/2 \max(d(g,id),d(h,id))$. } \item{By proper discontinuity of $\Gamma$, there is an $\alpha$ such that every element of $\Gamma$ is at least $\alpha$ from the identity. Then choosing $m$ so that $\epsilon/2^m < \alpha$, the $m$-commutators of the generators of the group in question are trivial. Since any $m$-commutator in this group can be written as a product of $m$-commutators of generators, this group is nilpotent.} \item{Finally, we show that the group generated by small translations contains a subgroup of this with finite index. This follows from the compactness of the point stabilizers of $Isom^+{\Bbb H}^3$ and the fact that parallel transport around the boundary of a geodesic triangle in $X$ can be controlled in a universal way by the diameter of the triangle.} \end{enumerate} Consequently, we have a classification of the $\epsilon$-thin pieces of the manifold as product neighborhoods of short geodesics, or $N \times {\Bbb R}$ for $N$ a Euclidean manifold. \item{Ideal triangulations} By a theorem of Thurston, any hyperbolic $3$-manifold has a degree one decomposition into ideal tetrahedra. If the manifold is non-compact, this can be taken to be an ordinary decomposition. Given a collection of ideal tetrahedra and some glueing maps on their boundaries, we can build a hyperbolic manifold. The condition that this will be a manifold is firstly that the pieces fit nicely around each edge (edge consistency conditions) and secondly that the holonomy of the boundary elements be parabolic (cusp conditions). Each of these conditions gives an integral linear combination in $log(z_i), log(1-z_i)$ for the simplex parameters $z_i$ as a multiple of $2\pi i$. The set of ideal simplex parameters for a triangulation of a hyperbolic manifold satisfy the following identity: $$\Sigma_i (1-z_i) \wedge z_i = 0$$ in $\Lambda^2\bar {\Bbb Q}^*$ This formula captures the fact that the Dehn invariant of any constant curvature manifold vanishes. It is a fact that any two ideal triangulations of a manifold determine the same element of the Bloch group - that is, they are related by cocycle moves, up to homology. These cocycle moves cannot necessarily be performed in the manifold, however. \item{Geometric Dehn surgery theorem (statement)} For any hyperbolic link complement $M$ in $S^3$, with components $L_1 \dots L_n$ there is an open neighborhood $\Omega$ of $\infty,\infty \dots \infty$ in $S^2 \times S^2 \times \dots \times S^2$ such that any generalized geometric Dehn surgery in $\Omega$ gives a complete hyperbolic structure on $M \cup_i \gamma_i$ with singular set either geodesics or points as appropriate. Moreover, $vol(M_\infty) > vol(M_{p,q})$ for any $(p,q) \ne \infty$. \end{itemize} \section{Minor Topic: Complex Analysis} \begin{itemize} \item{A function satisfies the Cauchy-Riemann equations iff it has a local power series expansion (statement)} This theorem is self explanatory. However, it is proved by using the Weierstrass theorem, which states that if $f_n(z)$ is analytic in a region $\Omega$ and the sequence $f_n$ converges uniformly on compact sets to $f$, then $f$ is analytic in $\Omega$, and moreover $f_n'$ converges uniformly to $f'$ on every compact subset of $\Omega$. Note also that having the real and imaginary parts of $f$ harmonic implies that $f$ is $C^\infty$ by elliptic regularity. \item{Schwarz-Pick lemma} An analytic map between Riemann surfaces decreases the hyperbolic metric unless it is a covering. This follows in a straightforward way from the maximum modulus priciple and the classification of automorphism of the disk as functions satisfying the formula $$\frac {w - w_0} {1 - \bar w w_0} = e^{i \theta} \frac {z - z_0} {1- \bar z z_0}$$ which preserves the infinitesimal form $$\frac {2dz} {1 - |z|^2}$$ which is the Poincar\' e metric. \item{Koebe $1/4$ theorem} A univalent function from $D$ to ${\Bbb C}$ with $|f'(0)|=1$ fixing $0$ contains the disk of radius $1/4$ about the origin. Together with the last theorem, this implies that the Poincar\' e metric on a domain $\Omega$ is quasi-isometric to $\frac {dz} {d(z, \partial \Omega)}$ \item{Cauchy integral formulae} Generally, for a simple loop $\gamma$ in a region $\Omega$ in which $$f(z) = a_{-n}(z-w)^{-n} + \dots + a_{-1}(z-w)^{-1} + a_0 + \dots$$ we have the formula $$a_m = \int_\gamma \frac {f(\zeta)} {(\zeta-w)^{m+1}} d\zeta$$ \item{Rouch\' e's theorem} If on some curve $\gamma$ we have the estimate that $|f| > |f-g|$ then the holomorphic function $f$ has the same number of zeroes enclosed by $\gamma$ as $g$ does. This is otherwise known as the ``dog on a leash" theorem. \item{Argument principle} $$1/2\pi i \int_\gamma \frac {f'(z)} {f(z)} dz$$ is equal to the number of zeroes minus the number of poles of $f$ in the region enclosed by $\gamma$. For, suppose $f$ has no poles. Then in the region in question, write it as $(z-\alpha_1)(z-\alpha_2) \dots (z-\alpha_n)k(z)$ where $k$ does not vanish. Then $$f'(z)/f(z) = \sum_i \frac 1 {(z-\alpha_i)}$$ which integrates to give the number $n$. \item{modulus of a quadrilateral; modulus of an annulus} For any quasicircle $Q$ there is a unique quadrilateral $M$ and a conformal map $Q \to M$ extending to a continuous map of the boundaries which takes any four points on $Q$ to the corners of $M$. The modulus of $Q$ is then the ratio of the two sides of $M$. Similarly, for any annulus $A$ there is a unique standard annulus $N$ and a conformal map $A \to N$ extending to a continuous map of the boundaries. This follows from Andre\' ev's theorem. The log of the ratio of the inner and outer circles of $N$ is the modulus of $A$. \item{Riemann mapping theorem} Any simply connected domain $\Omega$ in ${\Bbb C}$ which omits at least two points is conformally equivalent to the unit disk $D$. The proof consists in first constructing some conformal map into the unit disk and then by means of the Schwartz lemma, and simple facts about normal families, constructing a maximal such map which must therefore be onto. To construct some conformal map: first take a single-valued square root of $(x-p)(x-q)$ where $p,q$ are the two omitted values. The image of this omits some disk, so by means of a suitable Mobius transformation, we can put it into the unit disk. \item{Reflection principle} If an analytic map $f:A \to B$ maps some circular arc $a$ of $\partial A$ to some circular arc $b$ of $\partial B$ we can analytically continue $f$ from $A \cup \bar A$ to $B \cup \bar B$ where $\bar A$ is the reflection of $A$ in this arc, and $\bar B$ the reflection of $B$ is the other. If, more generally, we merely have that for any $z_i \to a$ that $f(z_i) \to b$, then by a suitable estimate, and use of Morera's theorem, we can make the same claim. \item{Morera's theorem} If a function satisfies Cauchy's integral formula in some domain, and is continuous there, then it is analytic. Here we use the fact that $$g(\zeta) = \frac 1 {2 \pi i} \int_\gamma \frac {\varphi(z)} {(z - \zeta)}$$ is analytic for any continuous $\varphi$. \item{Definition of a normal family - condition for a family to be normal} A family is {\it normal} on some domain $\Omega$ if each sequence of functions contains a convergent subsequence (i.e. convergent uniformly on compact subsets). By Arzela-Ascoli, it is sufficient that the family be equicontinuous and locally bounded. In fact, it is sufficient to assume the family is locally bounded. In fact, it is enough to assume the sequence omits two values in ${\Bbb C}$. \item{Liouville's theorem} A bounded entire holomorphic function is constant. This follows from the estimate for $f'$ obtained from $$f'(\zeta) = \frac 1 {2 \pi i} \int_\gamma \frac {f(z)} {(z-\zeta)^2}$$ \item{Picard's theorem} An entire holomorphic function which omits two values is constant. This follows by a developing argument. (Use the modular invariant $\lambda$ to uniformize the triply punctured sphere) \item{Maximum modulus principle} A function holomorphic in an open set $\Omega$ does not attain a maximum on $\Omega$ unless it is constant. Equivalently, non-constant holomorphic maps are open. \item{The real and complex parts of an analytic function are harmonic} Follows immediately from the Cauchy-Riemann equations: if $z=x+iy$ and $f(z) = u+iv$ then we have for an analytic function, $$\frac {\partial u} {\partial x} = \frac {\partial v} {\partial y}$$ and $$\frac {\partial u} {\partial y} = -\frac {\partial v} {\partial x}$$ \item{Gauss' lemma (the value of a harmonic function at the center of a circle is the average of its value on the circle)} This just follows from the above remark and the Cauchy integral formula for a circle. In particular, any function $\varphi$ on $\partial D$ can be extended to a harmonic function on $D$ by the ``visual extension". \item{Definition of Weierstrass $\wp$ function} For any lattice $\Lambda = {\Bbb Z} \oplus \tau {\Bbb Z}$ in ${\Bbb C}$, we define the function $$\wp(z) = \frac 1 {z^2} + \sum_{\omega \in \Lambda} (\frac 1 {(z-\omega)^2} - \frac 1 {\omega^2}) $$ This satisfies a functional equation $$\wp'(z)^2 = 4\wp(z)^3 - 60g_2 \wp(z) - 140 g_3$$ where $g_2$ is the sum of the reciprocals of the fourth powers of elements in $\Lambda$, and $g_3$ is the sum of the reciprocals of the sixth powers. The cross product of the roots of this cubic and $\infty$ is the modular invariant $\lambda(\tau)$. \end{itemize} \end{document}