A Classification of Spanning Surfaces for Alternating Links
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Oriented Pair (S 3,S1); Two Knots Are Regarded As
S-EQUIVALENCE OF KNOTS C. KEARTON Abstract. S-equivalence of classical knots is investigated, as well as its rela- tionship with mutation and the unknotting number. Furthermore, we identify the kernel of Bredon’s double suspension map, and give a geometric relation between slice and algebraically slice knots. Finally, we show that every knot is S-equivalent to a prime knot. 1. Introduction An oriented knot k is a smooth (or PL) oriented pair S3,S1; two knots are regarded as the same if there is an orientation preserving diffeomorphism sending one onto the other. An unoriented knot k is defined in the same way, but without regard to the orientation of S1. Every oriented knot is spanned by an oriented surface, a Seifert surface, and this gives rise to a matrix of linking numbers called a Seifert matrix. Any two Seifert matrices of the same knot are S-equivalent: the definition of S-equivalence is given in, for example, [14, 21, 11]. It is the equivalence relation generated by ambient surgery on a Seifert surface of the knot. In [19], two oriented knots are defined to be S-equivalent if their Seifert matrices are S- equivalent, and the following result is proved. Theorem 1. Two oriented knots are S-equivalent if and only if they are related by a sequence of doubled-delta moves shown in Figure 1. .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .... .. .... .... .... .... .... .... .... .... .... ... -
Of the American Mathematical Society August 2017 Volume 64, Number 7
ISSN 0002-9920 (print) ISSN 1088-9477 (online) of the American Mathematical Society August 2017 Volume 64, Number 7 The Mathematics of Gravitational Waves: A Two-Part Feature page 684 The Travel Ban: Affected Mathematicians Tell Their Stories page 678 The Global Math Project: Uplifting Mathematics for All page 712 2015–2016 Doctoral Degrees Conferred page 727 Gravitational waves are produced by black holes spiraling inward (see page 674). American Mathematical Society LEARNING ® MEDIA MATHSCINET ONLINE RESOURCES MATHEMATICS WASHINGTON, DC CONFERENCES MATHEMATICAL INCLUSION REVIEWS STUDENTS MENTORING PROFESSION GRAD PUBLISHING STUDENTS OUTREACH TOOLS EMPLOYMENT MATH VISUALIZATIONS EXCLUSION TEACHING CAREERS MATH STEM ART REVIEWS MEETINGS FUNDING WORKSHOPS BOOKS EDUCATION MATH ADVOCACY NETWORKING DIVERSITY blogs.ams.org Notices of the American Mathematical Society August 2017 FEATURED 684684 718 26 678 Gravitational Waves The Graduate Student The Travel Ban: Affected Introduction Section Mathematicians Tell Their by Christina Sormani Karen E. Smith Interview Stories How the Green Light was Given for by Laure Flapan Gravitational Wave Research by Alexander Diaz-Lopez, Allyn by C. Denson Hill and Paweł Nurowski WHAT IS...a CR Submanifold? Jackson, and Stephen Kennedy by Phillip S. Harrington and Andrew Gravitational Waves and Their Raich Mathematics by Lydia Bieri, David Garfinkle, and Nicolás Yunes This season of the Perseid meteor shower August 12 and the third sighting in June make our cover feature on the discovery of gravitational waves -
Non-Orientable Lagrangian Cobordisms Between Legendrian Knots
NON-ORIENTABLE LAGRANGIAN COBORDISMS BETWEEN LEGENDRIAN KNOTS ORSOLA CAPOVILLA-SEARLE AND LISA TRAYNOR 3 Abstract. In the symplectization of standard contact 3-space, R × R , it is known that an orientable Lagrangian cobordism between a Leg- endrian knot and itself, also known as an orientable Lagrangian endo- cobordism for the Legendrian knot, must have genus 0. We show that any Legendrian knot has a non-orientable Lagrangian endocobordism, and that the crosscap genus of such a non-orientable Lagrangian en- docobordism must be a positive multiple of 4. The more restrictive exact, non-orientable Lagrangian endocobordisms do not exist for any exactly fillable Legendrian knot but do exist for any stabilized Legen- drian knot. Moreover, the relation defined by exact, non-orientable La- grangian cobordism on the set of stabilized Legendrian knots is symmet- ric and defines an equivalence relation, a contrast to the non-symmetric relation defined by orientable Lagrangian cobordisms. 1. Introduction Smooth cobordisms are a common object of study in topology. Motivated by ideas in symplectic field theory, [19], Lagrangian cobordisms that are cylindrical over Legendrian submanifolds outside a compact set have been an active area of research interest. Throughout this paper, we will study 3 Lagrangian cobordisms in the symplectization of the standard contact R , 3 t namely the symplectic manifold (R×R ; d(e α)) where α = dz−ydx, that co- incide with the cylinders R×Λ+ (respectively, R×Λ−) when the R-coordinate is sufficiently positive (respectively, negative). Our focus will be on non- orientable Lagrangian cobordisms between Legendrian knots Λ+ and Λ− and non-orientable Lagrangian endocobordisms, which are non-orientable Lagrangian cobordisms with Λ+ = Λ−. -
Commentary on Thurston's Work on Foliations
COMMENTARY ON FOLIATIONS* Quoting Thurston's definition of foliation [F11]. \Given a large supply of some sort of fabric, what kinds of manifolds can be made from it, in a way that the patterns match up along the seams? This is a very general question, which has been studied by diverse means in differential topology and differential geometry. ... A foliation is a manifold made out of striped fabric - with infintely thin stripes, having no space between them. The complete stripes, or leaves, of the foliation are submanifolds; if the leaves have codimension k, the foliation is called a codimension k foliation. In order that a manifold admit a codimension- k foliation, it must have a plane field of dimension (n − k)." Such a foliation is called an (n − k)-dimensional foliation. The first definitive result in the subject, the so called Frobenius integrability theorem [Fr], concerns a necessary and sufficient condition for a plane field to be the tangent field of a foliation. See [Spi] Chapter 6 for a modern treatment. As Frobenius himself notes [Sa], a first proof was given by Deahna [De]. While this work was published in 1840, it took another hundred years before a geometric/topological theory of foliations was introduced. This was pioneered by Ehresmann and Reeb in a series of Comptes Rendus papers starting with [ER] that was quickly followed by Reeb's foundational 1948 thesis [Re1]. See Haefliger [Ha4] for a detailed account of developments in this period. Reeb [Re1] himself notes that the 1-dimensional theory had already undergone considerable development through the work of Poincare [P], Bendixson [Be], Kaplan [Ka] and others. -
MUTATIONS of LINKS in GENUS 2 HANDLEBODIES 1. Introduction
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 127, Number 1, January 1999, Pages 309{314 S 0002-9939(99)04871-6 MUTATIONS OF LINKS IN GENUS 2 HANDLEBODIES D. COOPER AND W. B. R. LICKORISH (Communicated by Ronald A. Fintushel) Abstract. A short proof is given to show that a link in the 3-sphere and any link related to it by genus 2 mutation have the same Alexander polynomial. This verifies a deduction from the solution to the Melvin-Morton conjecture. The proof here extends to show that the link signatures are likewise the same and that these results extend to links in a homology 3-sphere. 1. Introduction Suppose L is an oriented link in a genus 2 handlebody H that is contained, in some arbitrary (complicated) way, in S3.Letρbe the involution of H depicted abstractly in Figure 1 as a π-rotation about the axis shown. The pair of links L and ρL is said to be related by a genus 2 mutation. The first purpose of this note is to prove, by means of long established techniques of classical knot theory, that L and ρL always have the same Alexander polynomial. As described briefly below, this actual result for knots can also be deduced from the recent solution to a conjecture, of P. M. Melvin and H. R. Morton, that posed a problem in the realm of Vassiliev invariants. It is impressive that this simple result, readily expressible in the language of the classical knot theory that predates the Jones polynomial, should have emerged from the technicalities of Vassiliev invariants. -
Arxiv:Math/0208110V1 [Math.GT] 14 Aug 2002 Disifiieymn Itntsraebnl Structures
STRONGLY IRREDUCIBLE SURFACE AUTOMORPHISMS SAUL SCHLEIMER Abstract. A surface automorphism is strongly irreducible if every essential simple closed curve in the surface has nontrivial geomet- ric intersection with its image. We show that a three-manifold admits only finitely many inequivalent surface bundle structures with strongly irreducible monodromy. 1. Introduction A surface automorphism h : F F is strongly irreducible if every es- sential simple closed curve γ F→has nontrivial geometric intersection with its image, h(γ). This paper⊂ shows that a three-manifold admits only finitely many inequivalent surface bundle structures with strongly irreducible monodromy. This imposes a serious restriction; for exam- ple, any three-manifold which fibres over the circle and has b2(M) 2 admits infinitely many distinct surface bundle structures. ≥ The main step is an elementary proof that all weakly acylindrical sur- faces inside of an irreducible triangulated manifold are isotopic to fun- damental normal surfaces. As weakly acylindrical surfaces are a larger class than the acylindrical surfaces this strengthens a result of Hass [5]; an irreducible three-manifold contains only finitely many acylindrical surfaces. Section 2 gives necessary topological definitions, examples of strongly irreducible automorphisms, and precise statements of the theorems. arXiv:math/0208110v1 [math.GT] 14 Aug 2002 The required tools of normal surface theory are presented in Section 3. Section 4 defines weakly acylindrical and proves that every such sur- face is isotopic to a fundamental surface. In the spirit of the Georgia Topology Conference the paper ends by listing several open questions. Many of the ideas and terminology discussed come from the study of Heegaard splittings as in [2] and in my thesis [11]. -
Counting Essential Surfaces in 3-Manifolds
Counting essential surfaces in 3-manifolds Nathan M. Dunfield, Stavros Garoufalidis, and J. Hyam Rubinstein Abstract. We consider the natural problem of counting isotopy classes of es- sential surfaces in 3-manifolds, focusing on closed essential surfaces in a broad class of hyperbolic 3-manifolds. Our main result is that the count of (possibly disconnected) essential surfaces in terms of their Euler characteristic always has a short generating function and hence has quasi-polynomial behavior. This gives remarkably concise formulae for the number of such surfaces, as well as detailed asymptotics. We give algorithms that allow us to compute these generating func- tions and the underlying surfaces, and apply these to almost 60,000 manifolds, providing a wealth of data about them. We use this data to explore the delicate question of counting only connected essential surfaces and propose some con- jectures. Our methods involve normal and almost normal surfaces, especially the work of Tollefson and Oertel, combined with techniques pioneered by Ehrhart for counting lattice points in polyhedra with rational vertices. We also introduce arXiv:2007.10053v1 [math.GT] 20 Jul 2020 a new way of testing if a normal surface in an ideal triangulation is essential that avoids cutting the manifold open along the surface; rather, we use almost normal surfaces in the original triangulation. Contents 1 Introduction3 1.2 Main results . .4 1.5 Motivation and broader context . .5 1.7 The key ideas behind Theorem 1.3......................6 2 1.8 Making Theorem 1.3 algorithmic . .8 1.9 Ideal triangulations and almost normal surfaces . .8 1.10 Computations and patterns . -
Crosscap Number and Knot Projections
CROSSCAP NUMBER AND KNOT PROJECTIONS NOBORU ITO AND YUSUKE TAKIMURA Abstract. We introduce an unknotting-type number of knot projections that gives an upper bound of the crosscap number of knots. We determine the set of knot projections with the unknotting-type number at most two, and this result implies classical and new results that determine the set of alternating knots with the crosscap number at most two. 1. Introduction In this paper, we introduce an unknotting-type number of knot projections (Def- inition 1) as follows. Every double point in a knot projection can be spliced two different ways (Figure 2), one of which gives another knot projection (Definition 2). A special case of such operations is a first Reidemeister move RI−, as shown in Fig- ure 2. If the other case of such operations, which is not of type RI−, it is denoted by S−. Beginning with an n-crossing knot projection P , there are many sequences of n splices of type RI− and type S−, all of which end with the simple closed curve O. Then, we define the number u−(P ) as the minimum number of splices of type S− (Definition 3). For this number, we determine the set of knot projections with u−(P ) = 1 or u−(P ) = 2 (Theorem 1, Section 3). Here, we provide an efficient method to obtain a knot projection P with u−(P ) = n for a given n (Move 1). Further, for a connected sum (Definition 4) of knot projections, we show that the additivity of u− under the connected sum (Section 7). -
Crosscap Numbers of Alternating Knots Via Unknotting Splices
Crosscap numbers of alternating knots via unknotting splices THOMAS KINDRED Ito-Takimura recently defined a splice-unknotting number u−(D) for knot diagrams. They proved that this number provides an upper bound for the crosscap number of any prime knot, asking whether equality holds in the alternating case. We answer their question in the affirmative. (Ito has independently proven the same result.) As an application, we compute the crosscap numbers of all prime alternating knots through at least 13 crossings, using Gauss codes. 57M25 1 Introduction Let K ⊂ S3 be a knot. An embedded, compact, connected surface F ⊂ S3 is said to span K if @F = K . The crosscap number of K , denoted cc(K), is the smallest value of 12 β1(F) among all 1-sided spanning surfaces for K. A theorem of Adams and the author [4] states that, given an alternating diagram D of a knot K, the crosscap number of K is realized by some state surface from D. (Section 2 reviews background.) Moreover, given such D and K, an algorithm in [4] finds a 1-sided state surface F from D with β1(F) = cc(K). Ito-Takimura recently introduced a splice-unknotting number u−(D) for knot diagrams. Minimizing this number across all diagrams of a given knot K defines a knot invariant, arXiv:1905.11367v1 [math.GT] 27 May 2019 u−(K). After proving that u−(D) ≥ cc(K) holds for any diagram D of any nontrivial knot K, Ito-Takimura ask whether this inequality is ever strict in the case of prime alternating diagrams. -
KNOTS and SEIFERT SURFACES Your Task As a Group, Is to Research the Topics and Questions Below, Write up Clear Notes As a Group
KNOTS AND SEIFERT SURFACES MATH 180, SPRING 2020 Your task as a group, is to research the topics and questions below, write up clear notes as a group explaining these topics and the answers to the questions, and then make a video presenting your findings. Your video and notes will be presented to the class to teach them your findings. Make sure that in your notes and video you give examples and intuition, along with formal definitions, theorems, proofs, or calculations. Make sure that you point out what the is most important take away message, and what aspects may be tricky or confusing to understand at first. You will need to work together as a group. Every member of the group must understand Problems 1,2, and 3, and each group member should solve at least one example from problem (4). You may split up Problems 5-9. 1. Resources The primary resource for this project is The Knot Book by Colin Adams, Chapter 4.3 (page 95-106). An Introduction to Knot Theory by Raymond Lickorish Chapter 2, could also be helpful. You may also look at other resources online about knot theory and Seifert surfaces. Make sure to cite the sources you use. 2. Topics and Questions As you research, you may find more examples, definitions, and questions, which you defi- nitely should feel free to include in your notes and/or video, but make sure you at least go through the following discussion and questions. (1) What is a Seifert surface for a knot? Describe Seifert's algorithm for finding Seifert surfaces: how do you find Seifert circles and how do you use those Seifert -
CROSSCAP NUMBERS of PRETZEL KNOTS 1. Introduction It Is Well
CROSSCAP NUMBERS OF PRETZEL KNOTS 市原 一裕 (KAZUHIRO ICHIHARA) 大阪産業大学教養部 (OSAKA SANGYO UNIVERSITY) 水嶋滋氏 (東京工業大学大学院情報理工学研究科) との共同研究 (JOINT WORK WITH SHIGERU MIZUSHIMA (TOKYO INSTITUTE OF TECHNOLOGY)) Abstract. For a non-trivial knot in the 3-sphere, the crosscap number is de¯ned as the minimal ¯rst betti number of non-orientable spanning surfaces for it. In this article, we report a simple formula of the crosscap number for pretzel knots. 1. Introduction It is well-known that any knot in the 3-sphere S3 bounds an orientable subsurface in S3; called a Seifert surface. One of the most basic invariant in knot theory, the genus of a knot K, is de¯ned to be the minimal genus of a Seifert surface for K. On the other hand, any knot in S3 also bounds a non-orientable subsurface in S3: Consider checkerboard surfaces for a diagram of the knot, one of which is shown to be non-orientable. In view of this, similarly as the genus of a knot, B.E. Clark de¯ned the crosscap number of a knot as follows. De¯nition (Clark, [1]). The crosscap number γ(K) of a knot K is de¯ned to be the minimal ¯rst betti number of a non-orientable surface spanning K in S3. For completeness we de¯ne γ(K) = 0 if and only if K is the unknot. Example. The ¯gure-eight knot K in S3 bounds a once-punctured Klein bottle S, appearing as a checkerboard surface for the diagram of K with minimal crossings. Thus γ(K) · ¯1(S) = 2. -
Arxiv:2101.02945V3 [Math.GT] 15 Apr 2021
On Crossing Ball Structure in Knot and Link Complements Wei Lin Abstract We develop a word mechanism applied in knot and link diagrams for the illustra- tion of a diagrammatic property. We also give a necessary condition for determining incompressible and pairwise incompressible surfaces, that are embedded in knot or link complements. Finally, we give a finiteness theorem and an upper bound on the Euler characteristic of such surfaces. 1 Introduction 1.1 Preliminary Discussion Let L ⊂ S3 be a link and π(L) ⊂ S2(⊂ S3) be a regular link projection. Additionally, let F ⊂ S3 − L be an closed incompressible surface. In 1981 Menasco introduced his crossing ball technology for classical link projections [7] that replaced π(L) in S2 with two 2-spheres, 2 2 2 3 2 2 S±, which had the salient features that L was embedded in S+ [ S− and S n (S+ [ S−) 3 2 was a collection of open 3-balls|B± that correspond to the boundaries S± and a collect of crossing balls. (Please see §1.2 for formal definition.) Using general position arguments, 2 2 this technology allows for placing F into normal position with respect to S± so that F \S± is a collection of simple closed curves (s.c.c.'s). When one imposes the assumption that π(L) is an alternating projection, the normal position of an essential surface is exceedingly well behaved to the point where by direct observation one can definitively state whether the link is split, prime, cabled or a satellite. As such, any alternating knot can by direct observation be placed into one of William Thurston's three categories|torus knot, satellite knot or hyperbolic knot [10].