Heegaard Diagrams of Certain 3-Manifolds
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Geometric Methods in Heegaard Theory
GEOMETRIC METHODS IN HEEGAARD THEORY TOBIAS HOLCK COLDING, DAVID GABAI, AND DANIEL KETOVER Abstract. We survey some recent geometric methods for studying Heegaard splittings of 3-manifolds 0. Introduction A Heegaard splitting of a closed orientable 3-manifold M is a decomposition of M into two handlebodies H0 and H1 which intersect exactly along their boundaries. This way of thinking about 3-manifolds (though in a slightly different form) was discovered by Poul Heegaard in his forward looking 1898 Ph. D. thesis [Hee1]. He wanted to classify 3-manifolds via their diagrams. In his words1: Vi vende tilbage til Diagrammet. Den Opgave, der burde løses, var at reducere det til en Normalform; det er ikke lykkedes mig at finde en saadan, men jeg skal dog fremsætte nogle Bemærkninger angaaende Opgavens Løsning. \We will return to the diagram. The problem that ought to be solved was to reduce it to the normal form; I have not succeeded in finding such a way but I shall express some remarks about the problem's solution." For more details and a historical overview see [Go], and [Zie]. See also the French translation [Hee2], the English translation [Mun] and the partial English translation [Prz]. See also the encyclopedia article of Dehn and Heegaard [DH]. In his 1932 ICM address in Zurich [Ax], J. W. Alexander asked to determine in how many essentially different ways a canonical region can be traced in a manifold or in modern language how many different isotopy classes are there for splittings of a given genus. He viewed this as a step towards Heegaard's program. -
Riemann Surfaces
RIEMANN SURFACES AARON LANDESMAN CONTENTS 1. Introduction 2 2. Maps of Riemann Surfaces 4 2.1. Defining the maps 4 2.2. The multiplicity of a map 4 2.3. Ramification Loci of maps 6 2.4. Applications 6 3. Properness 9 3.1. Definition of properness 9 3.2. Basic properties of proper morphisms 9 3.3. Constancy of degree of a map 10 4. Examples of Proper Maps of Riemann Surfaces 13 5. Riemann-Hurwitz 15 5.1. Statement of Riemann-Hurwitz 15 5.2. Applications 15 6. Automorphisms of Riemann Surfaces of genus ≥ 2 18 6.1. Statement of the bound 18 6.2. Proving the bound 18 6.3. We rule out g(Y) > 1 20 6.4. We rule out g(Y) = 1 20 6.5. We rule out g(Y) = 0, n ≥ 5 20 6.6. We rule out g(Y) = 0, n = 4 20 6.7. We rule out g(C0) = 0, n = 3 20 6.8. 21 7. Automorphisms in low genus 0 and 1 22 7.1. Genus 0 22 7.2. Genus 1 22 7.3. Example in Genus 3 23 Appendix A. Proof of Riemann Hurwitz 25 Appendix B. Quotients of Riemann surfaces by automorphisms 29 References 31 1 2 AARON LANDESMAN 1. INTRODUCTION In this course, we’ll discuss the theory of Riemann surfaces. Rie- mann surfaces are a beautiful breeding ground for ideas from many areas of math. In this way they connect seemingly disjoint fields, and also allow one to use tools from different areas of math to study them. -
Mapping Class Group of a Handlebody
FUNDAMENTA MATHEMATICAE 158 (1998) Mapping class group of a handlebody by Bronis law W a j n r y b (Haifa) Abstract. Let B be a 3-dimensional handlebody of genus g. Let M be the group of the isotopy classes of orientation preserving homeomorphisms of B. We construct a 2-dimensional simplicial complex X, connected and simply-connected, on which M acts by simplicial transformations and has only a finite number of orbits. From this action we derive an explicit finite presentation of M. We consider a 3-dimensional handlebody B = Bg of genus g > 0. We may think of B as a solid 3-ball with g solid handles attached to it (see Figure 1). Our goal is to determine an explicit presentation of the map- ping class group of B, the group Mg of the isotopy classes of orientation preserving homeomorphisms of B. Every homeomorphism h of B induces a homeomorphism of the boundary S = ∂B of B and we get an embedding of Mg into the mapping class group MCG(S) of the surface S. z-axis α α α α 1 2 i i+1 . . β β 1 2 ε x-axis i δ -2, i Fig. 1. Handlebody An explicit and quite simple presentation of MCG(S) is now known, but it took a lot of time and effort of many people to reach it (see [1], [3], [12], 1991 Mathematics Subject Classification: 20F05, 20F38, 57M05, 57M60. This research was partially supported by the fund for the promotion of research at the Technion. [195] 196 B.Wajnryb [9], [7], [11], [6], [14]). -
[Math.GT] 31 Mar 2004
CORES OF S-COBORDISMS OF 4-MANIFOLDS Frank Quinn March 2004 Abstract. The main result is that an s-cobordism (topological or smooth) of 4- manifolds has a product structure outside a “core” sub s-cobordism. These cores are arranged to have quite a bit of structure, for example they are smooth and abstractly (forgetting boundary structure) diffeomorphic to a standard neighborhood of a 1-complex. The decomposition is highly nonunique so cannot be used to define an invariant, but it shows the topological s-cobordism question reduces to the core case. The simply-connected version of the decomposition (with 1-complex a point) is due to Curtis, Freedman, Hsiang and Stong. Controlled surgery is used to reduce topological triviality of core s-cobordisms to a question about controlled homotopy equivalence of 4-manifolds. There are speculations about further reductions. 1. Introduction The classical s-cobordism theorem asserts that an s-cobordism of n-manifolds (the bordism itself has dimension n + 1) is isomorphic to a product if n ≥ 5. “Isomorphic” means smooth, PL or topological, depending on the structure of the s-cobordism. In dimension 4 it is known that there are smooth s-cobordisms without smooth product structures; existence was demonstrated by Donaldson [3], and spe- cific examples identified by Akbulut [1]. In the topological case product structures follow from disk embedding theorems. The best current results require “small” fun- damental group, Freedman-Teichner [5], Krushkal-Quinn [9] so s-cobordisms with these groups are topologically products. The large fundamental group question is still open. Freedman has developed several link questions equivalent to the 4-dimensional “surgery conjecture” for arbitrary fundamental groups. -
Heegaard Splittings of Knot Exteriors 1 Introduction
Geometry & Topology Monographs 12 (2007) 191–232 191 arXiv version: fonts, pagination and layout may vary from GTM published version Heegaard splittings of knot exteriors YOAV MORIAH The goal of this paper is to offer a comprehensive exposition of the current knowledge about Heegaard splittings of exteriors of knots in the 3-sphere. The exposition is done with a historical perspective as to how ideas developed and by whom. Several new notions are introduced and some facts about them are proved. In particular the concept of a 1=n-primitive meridian. It is then proved that if a knot K ⊂ S3 has a 1=n-primitive meridian; then nK = K# ··· #K n-times has a Heegaard splitting of genus nt(K) + n which has a 1-primitive meridian. That is, nK is µ-primitive. 57M25; 57M05 1 Introduction The goal of this survey paper is to sum up known results about Heegaard splittings of knot exteriors in S3 and present them with some historical perspective. Until the mid 80’s Heegaard splittings of 3–manifolds and in particular of knot exteriors were not well understood at all. Most of the interest in studying knot spaces, up until then, was directed at various knot invariants which had a distinct algebraic flavor to them. Then in 1985 the remarkable work of Vaughan Jones turned the area around and began the era of the modern knot invariants a` la the Jones polynomial and its descendants and derivatives. However at the same time there were major developments in Heegaard theory of 3–manifolds in general and knot exteriors in particular. -
Applications of Quantum Invariants in Low Dimensional Topology
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Pergamon Topo/ogy Vol. 37, No. I, pp. 219-224, 1598 Q 1997 Elsevier Science Ltd Printed in Great Britain. All rights resewed 0040-9383197 $19.00 + 0.M) PII: soo4o-9383(97)00009-8 APPLICATIONS OF QUANTUM INVARIANTS IN LOW DIMENSIONAL TOPOLOGY STAVROSGAROUFALIDIS + (Received 12 November 1992; in revised form 1 November 1996) In this short note we give lower bounds for the Heegaard genus of 3-manifolds using various TQFT in 2+1 dimensions. We also study the large k limit and the large G limit of our lower bounds, using a conjecture relating the various combinatorial and physical TQFTs. We also prove, assuming this conjecture, that the set of colored SU(N) polynomials of a framed knot in S’ distinguishes the knot from the unknot. 0 1997 Elsevier Science Ltd 1. INTRODUCTION In recent years a remarkable relation between physics and low-dimensional topology has emerged, under the name of fopological quantum field theory (TQFT for short). An axiomatic definition of a TQFT in d + 1 dimensions has been provided by Atiyah- Segal in [l]. We briefly recall it: l To an oriented d dimensional manifold X, one associates a complex vector space Z(X). l To an oriented d + 1 dimensional manifold M with boundary 8M, one associates an element Z(M) E Z(&V). This (functor) Z usually satisfies extra compatibility conditions (depending on the di- mension d), some of which are: l For a disjoint union of d dimensional manifolds X, Y Z(X u Y) = Z(X) @ Z(Y). -
Uniformization of Riemann Surfaces Revisited
UNIFORMIZATION OF RIEMANN SURFACES REVISITED CIPRIANA ANGHEL AND RARES¸STAN ABSTRACT. We give an elementary and self-contained proof of the uniformization theorem for non-compact simply-connected Riemann surfaces. 1. INTRODUCTION Paul Koebe and shortly thereafter Henri Poincare´ are credited with having proved in 1907 the famous uniformization theorem for Riemann surfaces, arguably the single most important result in the whole theory of analytic functions of one complex variable. This theorem generated con- nections between different areas and lead to the development of new fields of mathematics. After Koebe, many proofs of the uniformization theorem were proposed, all of them relying on a large body of topological and analytical prerequisites. Modern authors [6], [7] use sheaf cohomol- ogy, the Runge approximation theorem, elliptic regularity for the Laplacian, and rather strong results about the vanishing of the first cohomology group of noncompact surfaces. A more re- cent proof with analytic flavour appears in Donaldson [5], again relying on many strong results, including the Riemann-Roch theorem, the topological classification of compact surfaces, Dol- beault cohomology and the Hodge decomposition. In fact, one can hardly find in the literature a self-contained proof of the uniformization theorem of reasonable length and complexity. Our goal here is to give such a minimalistic proof. Recall that a Riemann surface is a connected complex manifold of dimension 1, i.e., a connected Hausdorff topological space locally homeomorphic to C, endowed with a holomorphic atlas. Uniformization theorem (Koebe [9], Poincare´ [15]). Any simply-connected Riemann surface is biholomorphic to either the complex plane C, the open unit disk D, or the Riemann sphere C^. -
Floer Homology, Gauge Theory, and Low-Dimensional Topology
Floer Homology, Gauge Theory, and Low-Dimensional Topology Clay Mathematics Proceedings Volume 5 Floer Homology, Gauge Theory, and Low-Dimensional Topology Proceedings of the Clay Mathematics Institute 2004 Summer School Alfréd Rényi Institute of Mathematics Budapest, Hungary June 5–26, 2004 David A. Ellwood Peter S. Ozsváth András I. Stipsicz Zoltán Szabó Editors American Mathematical Society Clay Mathematics Institute 2000 Mathematics Subject Classification. Primary 57R17, 57R55, 57R57, 57R58, 53D05, 53D40, 57M27, 14J26. The cover illustrates a Kinoshita-Terasaka knot (a knot with trivial Alexander polyno- mial), and two Kauffman states. These states represent the two generators of the Heegaard Floer homology of the knot in its topmost filtration level. The fact that these elements are homologically non-trivial can be used to show that the Seifert genus of this knot is two, a result first proved by David Gabai. Library of Congress Cataloging-in-Publication Data Clay Mathematics Institute. Summer School (2004 : Budapest, Hungary) Floer homology, gauge theory, and low-dimensional topology : proceedings of the Clay Mathe- matics Institute 2004 Summer School, Alfr´ed R´enyi Institute of Mathematics, Budapest, Hungary, June 5–26, 2004 / David A. Ellwood ...[et al.], editors. p. cm. — (Clay mathematics proceedings, ISSN 1534-6455 ; v. 5) ISBN 0-8218-3845-8 (alk. paper) 1. Low-dimensional topology—Congresses. 2. Symplectic geometry—Congresses. 3. Homol- ogy theory—Congresses. 4. Gauge fields (Physics)—Congresses. I. Ellwood, D. (David), 1966– II. Title. III. Series. QA612.14.C55 2004 514.22—dc22 2006042815 Copying and reprinting. Material in this book may be reproduced by any means for educa- tional and scientific purposes without fee or permission with the exception of reproduction by ser- vices that collect fees for delivery of documents and provided that the customary acknowledgment of the source is given. -
Poincare Complexes: I
Poincare complexes: I By C. T. C. WALL Recent developments in differential and PL-topology have succeeded in reducing a large number of problems (classification and embedding, for ex- ample) to problems in homotopy theory. The classical methods of homotopy theory are available for these problems, but are often not strong enough to give the results needed. In this paper we attempt to develop a branch of homotopy theory applicable to the classification problem for compact manifolds. A Poincare complex is (approximately) a finite cw-complex which satisfies the Poincare duality theorem. A precise definition is given in ? 1, together with a discussion of chain complexes. In Chapter 2, we give a cutting and gluing theorem, define connected sum, and give a theorem on product decompositions. Chapter 3 is devoted to an account of the tangential proper- ties first introduced by M. Spivak (Princeton thesis, 1964). We then start our classification theorems; in Chapter 4, for dimensions up to 3, where the dominant invariant is the fundamental group; and in Chapter 5, for dimension 4, where we obtain a classification theorem when the fundamental group has prime order. It is complicated to use, but allows us to construct two inter- esting examples. In the second part of this paper, we intend to classify highly connected Poin- care complexes; to show how to perform surgery, and give some applications; by constructing handle decompositions and computing some cobordism groups. This paper was originally planned when the only known fact about topological manifolds (of dimension >3) was that they were Poincare com- plexes. -
Uniformization of Riemann Surfaces
CHAPTER 3 Uniformization of Riemann surfaces 3.1 The Dirichlet Problem on Riemann surfaces 128 3.2 Uniformization of simply connected Riemann surfaces 141 3.3 Uniformization of Riemann surfaces and Kleinian groups 148 3.4 Hyperbolic Geometry, Fuchsian Groups and Hurwitz’s Theorem 162 3.5 Moduli of Riemann surfaces 178 127 128 3. UNIFORMIZATION OF RIEMANN SURFACES One of the most important results in the area of Riemann surfaces is the Uni- formization theorem, which classifies all simply connected surfaces up to biholomor- phisms. In this chapter, after a technical section on the Dirichlet problem (solutions of equations involving the Laplacian operator), we prove that theorem. It turns out that there are very few simply connected surfaces: the Riemann sphere, the complex plane and the unit disc. We use this result in 3.2 to give a general formulation of the Uniformization theorem and obtain some consequences, like the classification of all surfaces with abelian fundamental group. We will see that most surfaces have the unit disc as their universal covering space, these surfaces are the object of our study in 3.3 and 3.5; we cover some basic properties of the Riemaniann geometry, §§ automorphisms, Kleinian groups and the problem of moduli. 3.1. The Dirichlet Problem on Riemann surfaces In this section we recall some result from Complex Analysis that some readers might not be familiar with. More precisely, we solve the Dirichlet problem; that is, to find a harmonic function on a domain with given boundary values. This will be used in the next section when we classify all simply connected Riemann surfaces. -
How to Depict 5-Dimensional Manifolds
HOW TO DEPICT 5-DIMENSIONAL MANIFOLDS HANSJORG¨ GEIGES Abstract. We usually think of 2-dimensional manifolds as surfaces embedded in Euclidean 3-space. Since humans cannot visualise Euclidean spaces of higher dimensions, it appears to be impossible to give pictorial representations of higher-dimensional manifolds. However, one can in fact encode the topology of a surface in a 1-dimensional picture. By analogy, one can draw 2-dimensional pictures of 3-manifolds (Heegaard diagrams), and 3-dimensional pictures of 4- manifolds (Kirby diagrams). With the help of open books one can likewise represent at least some 5-manifolds by 3-dimensional diagrams, and contact geometry can be used to reduce these to drawings in the 2-plane. In this paper, I shall explain how to draw such pictures and how to use them for answering topological and geometric questions. The work on 5-manifolds is joint with Fan Ding and Otto van Koert. 1. Introduction A manifold of dimension n is a topological space M that locally ‘looks like’ Euclidean n-space Rn; more precisely, any point in M should have an open neigh- bourhood homeomorphic to an open subset of Rn. Simple examples (for n = 2) are provided by surfaces in R3, see Figure 1. Not all 2-dimensional manifolds, however, can be visualised in 3-space, even if we restrict attention to compact manifolds. Worse still, these pictures ‘use up’ all three spatial dimensions to which our brains are adapted by natural selection. arXiv:1704.00919v1 [math.GT] 4 Apr 2017 2 2 Figure 1. The 2-sphere S , the 2-torus T , and the surface Σ2 of genus two. -
Lecture 1 Rachel Roberts
Lecture 1 Rachel Roberts Joan Licata May 13, 2008 The following notes are a rush transcript of Rachel’s lecture. Any mistakes or typos are mine, and please point these out so that I can post a corrected copy online. Outline 1. Three-manifolds: Presentations and basic structures 2. Foliations, especially codimension 1 foliations 3. Non-trivial examples of three-manifolds, generalizations of foliations to laminations 1 Three-manifolds Unless otherwise noted, let M denote a closed (compact) and orientable three manifold with empty boundary. (Note that these restrictions are largely for convenience.) We’ll start by collecting some useful facts about three manifolds. Definition 1. For our purposes, a triangulation of M is a decomposition of M into a finite colleciton of tetrahedra which meet only along shared faces. Fact 1. Every M admits a triangulation. This allows us to realize any M as three dimensional simplicial complex. Fact 2. M admits a C ∞ structure which is unique up to diffeomorphism. We’ll work in either the C∞ or PL category, which are equivalent for three manifolds. In partuclar, we’ll rule out wild (i.e. pathological) embeddings. 2 Examples 1. S3 (Of course!) 2. S1 × S2 3. More generally, for F a closed orientable surface, F × S1 1 Figure 1: A Heegaard diagram for the genus four splitting of S3. Figure 2: Left: Genus one Heegaard decomposition of S3. Right: Genus one Heegaard decomposi- tion of S2 × S1. We’ll begin by studying S3 carefully. If we view S3 as compactification of R3, we can take a neighborhood of the origin, which is a solid ball.