Dehn Surgery, Rational Open Books and Knot Floer Homology
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Part III 3-Manifolds Lecture Notes C Sarah Rasmussen, 2019
Part III 3-manifolds Lecture Notes c Sarah Rasmussen, 2019 Contents Lecture 0 (not lectured): Preliminaries2 Lecture 1: Why not ≥ 5?9 Lecture 2: Why 3-manifolds? + Intro to Knots and Embeddings 13 Lecture 3: Link Diagrams and Alexander Polynomial Skein Relations 17 Lecture 4: Handle Decompositions from Morse critical points 20 Lecture 5: Handles as Cells; Handle-bodies and Heegard splittings 24 Lecture 6: Handle-bodies and Heegaard Diagrams 28 Lecture 7: Fundamental group presentations from handles and Heegaard Diagrams 36 Lecture 8: Alexander Polynomials from Fundamental Groups 39 Lecture 9: Fox Calculus 43 Lecture 10: Dehn presentations and Kauffman states 48 Lecture 11: Mapping tori and Mapping Class Groups 54 Lecture 12: Nielsen-Thurston Classification for Mapping class groups 58 Lecture 13: Dehn filling 61 Lecture 14: Dehn Surgery 64 Lecture 15: 3-manifolds from Dehn Surgery 68 Lecture 16: Seifert fibered spaces 69 Lecture 17: Hyperbolic 3-manifolds and Mostow Rigidity 70 Lecture 18: Dehn's Lemma and Essential/Incompressible Surfaces 71 Lecture 19: Sphere Decompositions and Knot Connected Sum 74 Lecture 20: JSJ Decomposition, Geometrization, Splice Maps, and Satellites 78 Lecture 21: Turaev torsion and Alexander polynomial of unions 81 Lecture 22: Foliations 84 Lecture 23: The Thurston Norm 88 Lecture 24: Taut foliations on Seifert fibered spaces 89 References 92 1 2 Lecture 0 (not lectured): Preliminaries 0. Notation and conventions. Notation. @X { (the manifold given by) the boundary of X, for X a manifold with boundary. th @iX { the i connected component of @X. ν(X) { a tubular (or collared) neighborhood of X in Y , for an embedding X ⊂ Y . -
Arxiv:1804.09519V2 [Math.GT] 16 Feb 2020 in an Irreducible 3-Manifold N with Empty Or Toroidal Boundary
SUTURED MANIFOLDS AND `2-BETTI NUMBERS GERRIT HERRMANN Abstract. Using the virtual fibering theorem of Agol we show that a sutured 2 3-manifold (M; R+;R−; γ) is taut if and only if the ` -Betti numbers of the pair (M; R−) are zero. As an application we can characterize Thurston norm minimizing surfaces in a 3-manifold N with empty or toroidal boundary by the vanishing of certain `2-Betti numbers. 1. Introduction A sutured manifold (M; R+;R−; γ) is a compact, oriented 3-manifold M to- gether with a set of disjoint oriented annuli and tori γ on @M which decomposes @M n˚γ into two subsurfaces R− and R+. We refer to Section 2 for a precise defi- nition. We say that a sutured manifold is balanced if χ(R+) = χ(R−). Balanced sutured manifolds arise in many different contexts. For example 3-manifolds cut along non-separating surfaces can give rise to balanced sutured manifolds. Given a surface S with connected components S1 [ ::: [ Sk we define its Pk complexity to be χ−(S) = i=1 max {−χ(Si); 0g. A sutured manifold is called taut if R+ and R− have the minimal complexity among all surfaces representing [R−] = [R+] 2 H2(M; γ; Z). Theorem 1.1 (Main theorem). Let (M; R+;R−; γ) be a connected irreducible balanced sutured manifold. Assume that each component of γ and R± is incom- pressible and π1(M) is infinite, then the following are equivalent (1) the manifold (M; R+;R−; γ) is taut, 2 (2) (2) the ` -Betti numbers of (M; R−) are all zero i.e. -
Lens Spaces We Introduce Some of the Simplest 3-Manifolds, the Lens Spaces
CHAPTER 10 Seifert manifolds In the previous chapter we have proved various general theorems on three- manifolds, and it is now time to construct examples. A rich and important source is a family of manifolds built by Seifert in the 1930s, which generalises circle bundles over surfaces by admitting some “singular”fibres. The three- manifolds that admit such kind offibration are now called Seifert manifolds. In this chapter we introduce and completely classify (up to diffeomor- phisms) the Seifert manifolds. In Chapter 12 we will then show how to ge- ometrise them, by assigning a nice Riemannian metric to each. We will show, for instance, that all the elliptic andflat three-manifolds are in fact particular kinds of Seifert manifolds. 10.1. Lens spaces We introduce some of the simplest 3-manifolds, the lens spaces. These manifolds (and many more) are easily described using an important three- dimensional construction, called Dehnfilling. 10.1.1. Dehnfilling. If a 3-manifoldM has a spherical boundary com- ponent, we can cap it off with a ball. IfM has a toric boundary component, there is no canonical way to cap it off: the simplest object that we can attach to it is a solid torusD S 1, but the resulting manifold depends on the gluing × map. This operation is called a Dehnfilling and we now study it in detail. LetM be a 3-manifold andT ∂M be a boundary torus component. ⊂ Definition 10.1.1. A Dehnfilling ofM alongT is the operation of gluing a solid torusD S 1 toM via a diffeomorphismϕ:∂D S 1 T. -
A Computation of Knot Floer Homology of Special (1,1)-Knots
A COMPUTATION OF KNOT FLOER HOMOLOGY OF SPECIAL (1,1)-KNOTS Jiangnan Yu Department of Mathematics Central European University Advisor: Andras´ Stipsicz Proposal prepared by Jiangnan Yu in part fulfillment of the degree requirements for the Master of Science in Mathematics. CEU eTD Collection 1 Acknowledgements I would like to thank Professor Andras´ Stipsicz for his guidance on writing this thesis, and also for his teaching and helping during the master program. From him I have learned a lot knowledge in topol- ogy. I would also like to thank Central European University and the De- partment of Mathematics for accepting me to study in Budapest. Finally I want to thank my teachers and friends, from whom I have learned so much in math. CEU eTD Collection 2 Abstract We will introduce Heegaard decompositions and Heegaard diagrams for three-manifolds and for three-manifolds containing a knot. We define (1,1)-knots and explain the method to obtain the Heegaard diagram for some special (1,1)-knots, and prove that torus knots and 2- bridge knots are (1,1)-knots. We also define the knot Floer chain complex by using the theory of holomorphic disks and their moduli space, and give more explanation on the chain complex of genus-1 Heegaard diagram. Finally, we compute the knot Floer homology groups of the trefoil knot and the (-3,4)-torus knot. 1 Introduction Knot Floer homology is a knot invariant defined by P. Ozsvath´ and Z. Szabo´ in [6], using methods of Heegaard diagrams and moduli theory of holomorphic discs, combined with homology theory. -
Determining Hyperbolicity of Compact Orientable 3-Manifolds with Torus
Determining hyperbolicity of compact orientable 3-manifolds with torus boundary Robert C. Haraway, III∗ February 1, 2019 Abstract Thurston’s hyperbolization theorem for Haken manifolds and normal sur- face theory yield an algorithm to determine whether or not a compact ori- entable 3-manifold with nonempty boundary consisting of tori admits a com- plete finite-volume hyperbolic metric on its interior. A conjecture of Gabai, Meyerhoff, and Milley reduces to a computation using this algorithm. 1 Introduction The work of Jørgensen, Thurston, and Gromov in the late ‘70s showed ([18]) that the set of volumes of orientable hyperbolic 3-manifolds has order type ωω. Cao and Meyerhoff in [4] showed that the first limit point is the volume of the figure eight knot complement. Agol in [1] showed that the first limit point of limit points is the volume of the Whitehead link complement. Most significantly for the present paper, Gabai, Meyerhoff, and Milley in [9] identified the smallest, closed, orientable hyperbolic 3-manifold (the Weeks-Matveev-Fomenko manifold). arXiv:1410.7115v5 [math.GT] 31 Jan 2019 The proof of the last result required distinguishing hyperbolic 3-manifolds from non-hyperbolic 3-manifolds in a large list of 3-manifolds; this was carried out in [17]. The method of proof was to see whether the canonize procedure of SnapPy ([5]) succeeded or not; identify the successes as census manifolds; and then examine the fundamental groups of the 66 remaining manifolds by hand. This method made the ∗Research partially supported by NSF grant DMS-1006553. -
Cohomology Determinants of Compact 3-Manifolds
COHOMOLOGY DETERMINANTS OF COMPACT 3–MANIFOLDS CHRISTOPHER TRUMAN Abstract. We give definitions of cohomology determinants for compact, connected, orientable 3–manifolds. We also give formu- lae relating cohomology determinants before and after gluing a solid torus along a torus boundary component. Cohomology de- terminants are related to Turaev torsion, though the author hopes that they have other uses as well. 1. Introduction Cohomology determinants are an invariant of compact, connected, orientable 3-manifolds. The author first encountered these invariants in [Tur02], when Turaev gave the definition for closed 3–manifolds, and used cohomology determinants to obtain a leading order term of Tu- raev torsion. In [Tru], the author gives a definition for 3–manifolds with boundary, and derives a similar relationship to Turaev torsion. Here, we repeat the definitions, and give formulae relating the cohomology determinants before and after gluing a solid torus along a boundary component. One can use these formulae, and gluing formulae for Tu- raev torsion from [Tur02] Chapter VII, to re-derive the results of [Tru] from the results of [Tur02] Chapter III, or vice-versa. 2. Integral Cohomology Determinants arXiv:math/0611248v1 [math.GT] 8 Nov 2006 2.1. Closed 3–manifolds. We will simply state the relevant result from [Tur02] Section III.1; the proof is similar to the one below. Let R be a commutative ring with unit, and let N be a free R–module of rank n ≥ 3. Let S = S(N ∗) be the graded symmetric algebra on ∗ ℓ N = HomR(N, R), with grading S = S . Let f : N ×N ×N −→ R ℓL≥0 be an alternate trilinear form, and let g : N × N → N ∗ be induced by f. -
MTH 507 Midterm Solutions
MTH 507 Midterm Solutions 1. Let X be a path connected, locally path connected, and semilocally simply connected space. Let H0 and H1 be subgroups of π1(X; x0) (for some x0 2 X) such that H0 ≤ H1. Let pi : XHi ! X (for i = 0; 1) be covering spaces corresponding to the subgroups Hi. Prove that there is a covering space f : XH0 ! XH1 such that p1 ◦ f = p0. Solution. Choose x ; x 2 p−1(x ) so that p :(X ; x ) ! (X; x ) and e0 e1 0 i Hi ei 0 p (X ; x ) = H for i = 0; 1. Since H ≤ H , by the Lifting Criterion, i∗ Hi ei i 0 1 there exists a lift f : XH0 ! XH1 of p0 such that p1 ◦f = p0. It remains to show that f : XH0 ! XH1 is a covering space. Let y 2 XH1 , and let U be a path-connected neighbourhood of x = p1(y) that is evenly covered by both p0 and p1. Let V ⊂ XH1 be −1 −1 the slice of p1 (U) that contains y. Denote the slices of p0 (U) by 0 −1 0 −1 fVz : z 2 p0 (x)g. Let C denote the subcollection fVz : z 2 f (y)g −1 −1 of p0 (U). Every slice Vz is mapped by f into a single slice of p1 (U), −1 0 as these are path-connected. Also, since f(z) 2 p1 (y), f(Vz ) ⊂ V iff f(z) = y. Hence f −1(V ) is the union of the slices in C. 0 −1 0 0 0 Finally, we have that for Vz 2 C,(p1jV ) ◦ (p0jVz ) = fjVz . -
Sutured Manifold Hierarchies, Essential Laminations, and Dehn Surgery
JOURNAL OF DIFFERENTIAL GEOMETRY Volume 48 (1998), pages 407{437 SUTURED MANIFOLD HIERARCHIES, ESSENTIAL LAMINATIONS, AND DEHN SURGERY Ying-Qing Wu x0. Introduction A compact orientable surface F with nonnegative Euler characteristic is either a sphere, a disk, a torus, or an annulus. If a 3-manifold M contains such an essential surface, then it is said to be reducible, @-reducible, toroidal, or annular, respectively. Any such surface can be used to decompose the manifold further into simpler manifolds. We say that M is a simple manifold if it has no such surfaces. A simple manifold is expected to have a nice geometric structure. If M has nonempty boundary, then the Geometrization Theorem of Thurston for Haken manifolds says that M with boundary tori removed admits a finite volume hyperbolic structure with totally geodesic boundary. When M has no boundaries, Thurston's Geometrization Conjecture asserts that M is either hyperbolic, or is a Seifert fiber space with orbifold a sphere with at most 3 cone points. Suppose T is a torus boundary component of M. We use M(γ) to denote the manifold obtained by Dehn filling on T so that the slope γ on T bounds a disk in the Dehn filling solid torus. When M = E(K) is the exterior of a knot K in S3, denote M(γ) by K(γ), and call it the manifold obtained by γ surgery on the knot K. It is well known that if M is simple then there are only finitely many Dehn fillings on T which produce non simple manifolds. -
Floer Homology and Surface Decompositions
Geometry & Topology 12 (2008) 299–350 299 Floer homology and surface decompositions ANDRÁS JUHÁSZ Sutured Floer homology, denoted by SFH , is an invariant of balanced sutured manifolds previously defined by the author. In this paper we give a formula that shows how this invariant changes under surface decompositions. In particular, if .M; / .M 0; 0/ is a sutured manifold decomposition then SFH.M 0; 0/ is a direct summand of SFH.M; /. To prove the decomposition formula we give an algorithm that computes SFH.M; / from a balanced diagram defining .M; / that generalizes the algorithm of Sarkar and Wang. As a corollary we obtain that if .M; / is taut then SFH.M; / 0. Other applica- ¤ tions include simple proofs of a result of Ozsváth and Szabó that link Floer homology detects the Thurston norm, and a theorem of Ni that knot Floer homology detects fibred knots. Our proofs do not make use of any contact geometry. Moreover, using these methods we show that if K is a genus g knot in a rational homology 3–sphere Y whose Alexander polynomial has leading coefficient ag 0 ¤ and if rkHFK.Y; K; g/ < 4 then Y N.K/ admits a depth 2 taut foliation n Ä transversal to @N.K/. 57M27, 57R58 1 1 Introduction In[7] we defined a Floer homology invariant for balanced sutured manifolds. In this paper we study how this invariant changes under surface decompositions. We need some definitions before we can state our main result. Recall that Spinc structures on sutured manifolds were defined in[7]; all the necessary definitions can also be found in Section 3 of the present paper. -
Problems in Low-Dimensional Topology
Problems in Low-Dimensional Topology Edited by Rob Kirby Berkeley - 22 Dec 95 Contents 1 Knot Theory 7 2 Surfaces 85 3 3-Manifolds 97 4 4-Manifolds 179 5 Miscellany 259 Index of Conjectures 282 Index 284 Old Problem Lists 294 Bibliography 301 1 2 CONTENTS Introduction In April, 1977 when my first problem list [38,Kirby,1978] was finished, a good topologist could reasonably hope to understand the main topics in all of low dimensional topology. But at that time Bill Thurston was already starting to greatly influence the study of 2- and 3-manifolds through the introduction of geometry, especially hyperbolic. Four years later in September, 1981, Mike Freedman turned a subject, topological 4-manifolds, in which we expected no progress for years, into a subject in which it seemed we knew everything. A few months later in spring 1982, Simon Donaldson brought gauge theory to 4-manifolds with the first of a remarkable string of theorems showing that smooth 4-manifolds which might not exist or might not be diffeomorphic, in fact, didn’t and weren’t. Exotic R4’s, the strangest of smooth manifolds, followed. And then in late spring 1984, Vaughan Jones brought us the Jones polynomial and later Witten a host of other topological quantum field theories (TQFT’s). Physics has had for at least two decades a remarkable record for guiding mathematicians to remarkable mathematics (Seiberg–Witten gauge theory, new in October, 1994, is the latest example). Lest one think that progress was only made using non-topological techniques, note that Freedman’s work, and other results like knot complements determining knots (Gordon- Luecke) or the Seifert fibered space conjecture (Mess, Scott, Gabai, Casson & Jungreis) were all or mostly classical topology. -
Topological Surgery and Its Dynamics
TOPOLOGICAL SURGERY AND ITS DYNAMICS SOFIA LAMBROPOULOU, STATHIS ANTONIOU, AND NIKOLA SAMARDZIJA Abstract. Topological surgery occurs in natural phenomena where two points are selected and attracting or repelling forces are applied. The two points are connected via an invisible `thread'. In order to model topologically such phenomena we introduce dynamics in 1-, 2- and 3-dimensional topological surgery, by means of attracting or repelling forces between two selected points in the manifold, and we address examples. We also introduce the notions of solid 1- and 2-dimensional topological surgery, and of truncated 1-, 2- and 3-dimensional topological surgery, which are more appropriate for modelling natural processes. On the theoretical level, these new notions allow to visualize 3-dimensional surgery and to connect surgeries in different dimensions. We hope that through this study, topology and dynamics of many natural phenomena as well as topological surgery may now be better understood. Introduction The aim of this study is to draw a connection between topological surgery in dimensions 1, 2 and 3 and many natural phenomena. For this we introduce new theoretical concepts which allow to explain the topology of such phenomena via surgery and also to connect topological surgeries in different dimensions. The new concepts are the introduction of forces, attracting or repelling, in the process of surgery, the notion of solid 1- and 2-dimensional surgery and the notion of truncated 1-, 2- and 3-dimensional surgery. Topological surgery is a technique used for changing the homeomorphism type of a topolog- ical manifold, thus for creating new manifolds out of known ones. -
HOMEOMORPHISMS on a SOLID TORUS to If
HOMEOMORPHISMS ON A SOLID TORUS d. R. McMillan, jr. 1. Introduction. An orientable 3-manifold with boundary can be represented as a solid torus H ("cube with handles") plus a disjoint collection of 3-cells attached to the boundary of H along annuli.1 Hence, a natural (but difficult) approach to the study of such 3- manifolds is to associate with each a system of disjoint simple closed curves in the boundary of a solid torus. It would be useful (e.g., in proving that two 3-manifolds are homeomorphic) to have conditions under which one such system of curves is topologically equivalent to another. A special case of this problem is considered here. Let H be a solid torus of genus » and let / and J* be two collections of « disjoint simple closed curves in the boundary of H. The result is that if each of the collections "generates" TiiH) (see §2), then the collections are topologically equivalent. Some care must be exercised in producing the homeomorphism, since not every homeomorphism on the bound- ary of H which throws one collection onto the other can be extended to if. 2. Preliminaries. Two simplicial complexes will be called equivalent if they have rectilinear subdivisions which are isomorphic complexes. An n-cell in-sphere) is a complex equivalent to an «-simplex (bound- ary of an M+ 1-simplex, respectively). If the closed star of each vertex in the complex M is equivalent to an »-cell, then M is by definition an n-manifold. The union of those simplexes of M each of whose links is not a sphere is the boundary of M (Bd M) and the interior of M (Int M) is M—Bd M.