Epimorphisms Between 2–Bridge Link Groups 1 Introduction
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Hyperbolic Structures from Link Diagrams
Hyperbolic Structures from Link Diagrams Anastasiia Tsvietkova, joint work with Morwen Thistlethwaite Louisiana State University/University of Tennessee Anastasiia Tsvietkova, joint work with MorwenHyperbolic Thistlethwaite Structures (UTK) from Link Diagrams 1/23 Every knot can be uniquely decomposed as a knot sum of prime knots (H. Schubert). It also true for non-split links (i.e. if there is no a 2–sphere in the complement separating the link). Of the 14 prime knots up to 7 crossings, 3 are non-hyperbolic. Of the 1,701,935 prime knots up to 16 crossings, 32 are non-hyperbolic. Of the 8,053,378 prime knots with 17 crossings, 30 are non-hyperbolic. Motivation: knots Anastasiia Tsvietkova, joint work with MorwenHyperbolic Thistlethwaite Structures (UTK) from Link Diagrams 2/23 Of the 14 prime knots up to 7 crossings, 3 are non-hyperbolic. Of the 1,701,935 prime knots up to 16 crossings, 32 are non-hyperbolic. Of the 8,053,378 prime knots with 17 crossings, 30 are non-hyperbolic. Motivation: knots Every knot can be uniquely decomposed as a knot sum of prime knots (H. Schubert). It also true for non-split links (i.e. if there is no a 2–sphere in the complement separating the link). Anastasiia Tsvietkova, joint work with MorwenHyperbolic Thistlethwaite Structures (UTK) from Link Diagrams 2/23 Of the 1,701,935 prime knots up to 16 crossings, 32 are non-hyperbolic. Of the 8,053,378 prime knots with 17 crossings, 30 are non-hyperbolic. Motivation: knots Every knot can be uniquely decomposed as a knot sum of prime knots (H. -
Some Generalizations of Satoh's Tube
SOME GENERALIZATIONS OF SATOH'S TUBE MAP BLAKE K. WINTER Abstract. Satoh has defined a map from virtual knots to ribbon surfaces embedded in S4. Herein, we generalize this map to virtual m-links, and use this to construct generalizations of welded and extended welded knots to higher dimensions. This also allows us to construct two new geometric pictures of virtual m-links, including 1-links. 1. Introduction In [13], Satoh defined a map from virtual link diagrams to ribbon surfaces knotted in S4 or R4. This map, which he called T ube, preserves the knot group and the knot quandle (although not the longitude). Furthermore, Satoh showed that if K =∼ K0 as virtual knots, T ube(K) is isotopic to T ube(K0). In fact, we can make a stronger statement: if K and K0 are equivalent under what Satoh called w- equivalence, then T ube(K) is isotopic to T ube(K0) via a stable equivalence of ribbon links without band slides. For virtual links, w-equivalence is the same as welded equivalence, explained below. In addition to virtual links, Satoh also defined virtual arc diagrams and defined the T ube map on such diagrams. On the other hand, in [15, 14], the notion of virtual knots was extended to arbitrary dimensions, building on the geometric description of virtual knots given by Kuperberg, [7]. It is therefore natural to ask whether Satoh's idea for the T ube map can be generalized into higher dimensions, as well as inquiring into a generalization of the virtual arc diagrams to higher dimensions. -
Arxiv:2003.00512V2 [Math.GT] 19 Jun 2020 the Vertical Double of a Virtual Link, As Well As the More General Notion of a Stack for a Virtual Link
A GEOMETRIC INVARIANT OF VIRTUAL n-LINKS BLAKE K. WINTER Abstract. For a virtual n-link K, we define a new virtual link VD(K), which is invariant under virtual equivalence of K. The Dehn space of VD(K), which we denote by DD(K), therefore has a homotopy type which is an invariant of K. We show that the quandle and even the fundamental group of this space are able to detect the virtual trefoil. We also consider applications to higher-dimensional virtual links. 1. Introduction Virtual links were introduced by Kauffman in [8], as a generalization of classical knot theory. They were given a geometric interpretation by Kuper- berg in [10]. Building on Kuperberg's ideas, virtual n-links were defined in [16]. Here, we define some new invariants for virtual links, and demonstrate their power by using them to distinguish the virtual trefoil from the unknot, which cannot be done using the ordinary group or quandle. Although these knots can be distinguished by means of other invariants, such as biquandles, there are two advantages to the approach used herein: first, our approach to defining these invariants is purely geometric, whereas the biquandle is en- tirely combinatorial. Being geometric, these invariants are easy to generalize to higher dimensions. Second, biquandles are rather complicated algebraic objects. Our invariants are spaces up to homotopy type, with their ordinary quandles and fundamental groups. These are somewhat simpler to work with than biquandles. The paper is organized as follows. We will briefly review the notion of a virtual link, then the notion of the Dehn space of a virtual link. -
An Introduction to Knot Theory and the Knot Group
AN INTRODUCTION TO KNOT THEORY AND THE KNOT GROUP LARSEN LINOV Abstract. This paper for the University of Chicago Math REU is an expos- itory introduction to knot theory. In the first section, definitions are given for knots and for fundamental concepts and examples in knot theory, and motivation is given for the second section. The second section applies the fun- damental group from algebraic topology to knots as a means to approach the basic problem of knot theory, and several important examples are given as well as a general method of computation for knot diagrams. This paper assumes knowledge in basic algebraic and general topology as well as group theory. Contents 1. Knots and Links 1 1.1. Examples of Knots 2 1.2. Links 3 1.3. Knot Invariants 4 2. Knot Groups and the Wirtinger Presentation 5 2.1. Preliminary Examples 5 2.2. The Wirtinger Presentation 6 2.3. Knot Groups for Torus Knots 9 Acknowledgements 10 References 10 1. Knots and Links We open with a definition: Definition 1.1. A knot is an embedding of the circle S1 in R3. The intuitive meaning behind a knot can be directly discerned from its name, as can the motivation for the concept. A mathematical knot is just like a knot of string in the real world, except that it has no thickness, is fixed in space, and most importantly forms a closed loop, without any loose ends. For mathematical con- venience, R3 in the definition is often replaced with its one-point compactification S3. Of course, knots in the real world are not fixed in space, and there is no interesting difference between, say, two knots that differ only by a translation. -
Hyperbolic Structures from Link Diagrams
University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Doctoral Dissertations Graduate School 5-2012 Hyperbolic Structures from Link Diagrams Anastasiia Tsvietkova [email protected] Follow this and additional works at: https://trace.tennessee.edu/utk_graddiss Part of the Geometry and Topology Commons Recommended Citation Tsvietkova, Anastasiia, "Hyperbolic Structures from Link Diagrams. " PhD diss., University of Tennessee, 2012. https://trace.tennessee.edu/utk_graddiss/1361 This Dissertation is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Doctoral Dissertations by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a dissertation written by Anastasiia Tsvietkova entitled "Hyperbolic Structures from Link Diagrams." I have examined the final electronic copy of this dissertation for form and content and recommend that it be accepted in partial fulfillment of the equirr ements for the degree of Doctor of Philosophy, with a major in Mathematics. Morwen B. Thistlethwaite, Major Professor We have read this dissertation and recommend its acceptance: Conrad P. Plaut, James Conant, Michael Berry Accepted for the Council: Carolyn R. Hodges Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) Hyperbolic Structures from Link Diagrams A Dissertation Presented for the Doctor of Philosophy Degree The University of Tennessee, Knoxville Anastasiia Tsvietkova May 2012 Copyright ©2012 by Anastasiia Tsvietkova. All rights reserved. ii Acknowledgements I am deeply thankful to Morwen Thistlethwaite, whose thoughtful guidance and generous advice made this research possible. -
Dynamics, and Invariants
k k On Groups Gn and Γn: A Study of Manifolds, Dynamics, and Invariants Vassily O. Manturov, Denis A. Fedoseev, Seongjeong Kim, Igor M. Nikonov A long time ago, when I first encountered knot tables and started un- knotting knots “by hand”, I was quite excited with the fact that some knots may have more than one minimal representative. In other words, in order to make an object simpler, one should first make it more complicated, for example, see Fig. 1 [72]: this diagram represents the trivial knot, but in order to simplify it, one needs to perform an increasing Reidemeister move first. Figure 1: Culprit knot Being a first year undergraduate student (in the Moscow State Univer- sity), I first met free groups and their presentation. The power and beauty, arXiv:1905.08049v4 [math.GT] 29 Mar 2021 and simplicity of these groups for me were their exponential growth and ex- tremely easy solution to the word problem and conjugacy problem by means of a gradient descent algorithm in a word (in a cyclic word, respectively). Also, I was excited with Diamond lemma (see Fig. 2): a simple condition which guarantees the uniqueness of the minimal objects, and hence, solution to many problems. Being a last year undergraduate and teaching a knot theory course for the first time, I thought: “Why do not we have it (at least partially) in knot theory?” 1 A A1 A2 A12 = A21 Figure 2: The Diamond lemma By that time I knew about the Diamond lemma and solvability of many problems like word problem in groups by gradient descent algorithm. -
Milnor Invariants of String Links, Trivalent Trees, and Configuration Space Integrals
MILNOR INVARIANTS OF STRING LINKS, TRIVALENT TREES, AND CONFIGURATION SPACE INTEGRALS ROBIN KOYTCHEFF AND ISMAR VOLIC´ Abstract. We study configuration space integral formulas for Milnor's homotopy link invari- ants, showing that they are in correspondence with certain linear combinations of trivalent trees. Our proof is essentially a combinatorial analysis of a certain space of trivalent \homotopy link diagrams" which corresponds to all finite type homotopy link invariants via configuration space integrals. An important ingredient is the fact that configuration space integrals take the shuffle product of diagrams to the product of invariants. We ultimately deduce a partial recipe for writing explicit integral formulas for products of Milnor invariants from trivalent forests. We also obtain cohomology classes in spaces of link maps from the same data. Contents 1. Introduction 2 1.1. Statement of main results 3 1.2. Organization of the paper 4 1.3. Acknowledgment 4 2. Background 4 2.1. Homotopy long links 4 2.2. Finite type invariants of homotopy long links 5 2.3. Trivalent diagrams 5 2.4. The cochain complex of diagrams 7 2.5. Configuration space integrals 10 2.6. Milnor's link homotopy invariants 11 3. Examples in low degrees 12 3.1. The pairwise linking number 12 3.2. The triple linking number 12 3.3. The \quadruple linking numbers" 14 4. Main Results 14 4.1. The shuffle product and filtrations of weight systems for finite type link invariants 14 4.2. Specializing to homotopy weight systems 17 4.3. Filtering homotopy link invariants 18 4.4. The filtrations and the canonical map 18 4.5. -
A New Technique for the Link Slice Problem
Invent. math. 80, 453 465 (1985) /?/ven~lOnSS mathematicae Springer-Verlag 1985 A new technique for the link slice problem Michael H. Freedman* University of California, San Diego, La Jolla, CA 92093, USA The conjectures that the 4-dimensional surgery theorem and 5-dimensional s-cobordism theorem hold without fundamental group restriction in the to- pological category are equivalent to assertions that certain "atomic" links are slice. This has been reported in [CF, F2, F4 and FQ]. The slices must be topologically flat and obey some side conditions. For surgery the condition is: ~a(S 3- ~ slice)--, rq (B 4- slice) must be an epimorphism, i.e., the slice should be "homotopically ribbon"; for the s-cobordism theorem the slice restricted to a certain trivial sublink must be standard. There is some choice about what the atomic links are; the current favorites are built from the simple "Hopf link" by a great deal of Bing doubling and just a little Whitehead doubling. A link typical of those atomic for surgery is illustrated in Fig. 1. (Links atomic for both s-cobordism and surgery are slightly less symmetrical.) There has been considerable interplay between the link theory and the equivalent abstract questions. The link theory has been of two sorts: algebraic invariants of finite links and the limiting geometry of infinitely iterated links. Our object here is to solve a class of free-group surgery problems, specifically, to construct certain slices for the class of links ~ where D(L)eCg if and only if D(L) is an untwisted Whitehead double of a boundary link L. -
Arxiv:2002.01505V2 [Math.GT] 9 May 2021 Ocratt Onayln,Ie Ikwoecmoet B ¯ Components the Whose Particular, Link in a Surfaces
Milnor’s concordance invariants for knots on surfaces MICAH CHRISMAN Milnor’sµ ¯ -invariants of links in the 3-sphere S3 vanish on any link concordant to a boundary link. In particular, they are trivial on any knot in S3 . Here we consider knots in thickened surfaces Σ × [0, 1], where Σ is closed and oriented. We construct new concordance invariants by adapting the Chen-Milnor theory of links in S3 to an extension of the group of a virtual knot. A key ingredient is the Bar-Natan Ж map, which allows for a geometric interpretation of the group extension. The group extension itself was originally defined by Silver-Williams. Our extendedµ ¯ -invariants obstruct concordance to homologically trivial knots in thickened surfaces. We use them to give new examples of non-slice virtual knots having trivial Rasmussen invariant, graded genus, affine index (or writhe) polyno- mial, and generalized Alexander polynomial. Furthermore, we complete the slice status classification of all virtual knots up to five classical crossings and reduce to four (out of 92800)the numberof virtual knots up to six classical crossings having unknown slice status. Our main application is to Turaev’s concordance group VC of long knots on sur- faces. Boden and Nagel proved that the concordance group C of classical knots in S3 embeds into the center of VC. In contrast to the classical knot concordance group, we show VC is not abelian; answering a question posed by Turaev. 57K10, 57K12, 57K45 arXiv:2002.01505v2 [math.GT] 9 May 2021 1 Overview For an m-component link L in the 3-sphere S3 , Milnor [43] introduced an infinite family of link isotopy invariants called theµ ¯ -invariants. -
Knot Theory and the Alexander Polynomial
Knot Theory and the Alexander Polynomial Reagin Taylor McNeill Submitted to the Department of Mathematics of Smith College in partial fulfillment of the requirements for the degree of Bachelor of Arts with Honors Elizabeth Denne, Faculty Advisor April 15, 2008 i Acknowledgments First and foremost I would like to thank Elizabeth Denne for her guidance through this project. Her endless help and high expectations brought this project to where it stands. I would Like to thank David Cohen for his support thoughout this project and through- out my mathematical career. His humor, skepticism and advice is surely worth the $.25 fee. I would also like to thank my professors, peers, housemates, and friends, particularly Kelsey Hattam and Katy Gerecht, for supporting me throughout the year, and especially for tolerating my temporary insanity during the final weeks of writing. Contents 1 Introduction 1 2 Defining Knots and Links 3 2.1 KnotDiagramsandKnotEquivalence . ... 3 2.2 Links, Orientation, and Connected Sum . ..... 8 3 Seifert Surfaces and Knot Genus 12 3.1 SeifertSurfaces ................................. 12 3.2 Surgery ...................................... 14 3.3 Knot Genus and Factorization . 16 3.4 Linkingnumber.................................. 17 3.5 Homology ..................................... 19 3.6 TheSeifertMatrix ................................ 21 3.7 TheAlexanderPolynomial. 27 4 Resolving Trees 31 4.1 Resolving Trees and the Conway Polynomial . ..... 31 4.2 TheAlexanderPolynomial. 34 5 Algebraic and Topological Tools 36 5.1 FreeGroupsandQuotients . 36 5.2 TheFundamentalGroup. .. .. .. .. .. .. .. .. 40 ii iii 6 Knot Groups 49 6.1 TwoPresentations ................................ 49 6.2 The Fundamental Group of the Knot Complement . 54 7 The Fox Calculus and Alexander Ideals 59 7.1 TheFreeCalculus ............................... -
How Can We Say 2 Knots Are Not the Same?
How can we say 2 knots are not the same? SHRUTHI SRIDHAR What’s a knot? A knot is a smooth embedding of the circle S1 in IR3. A link is a smooth embedding of the disjoint union of more than one circle Intuitively, it’s a string knotted up with ends joined up. We represent it on a plane using curves and ‘crossings’. The unknot A ‘figure-8’ knot A ‘wild’ knot (not a knot for us) Hopf Link Two knots or links are the same if they have an ambient isotopy between them. Representing a knot Knots are represented on the plane with strands and crossings where 2 strands cross. We call this picture a knot diagram. Knots can have more than one representation. Reidemeister moves Operations on knot diagrams that don’t change the knot or link Reidemeister moves Theorem: (Reidemeister 1926) Two knot diagrams are of the same knot if and only if one can be obtained from the other through a series of Reidemeister moves. Crossing Number The minimum number of crossings required to represent a knot or link is called its crossing number. Knots arranged by crossing number: Knot Invariants A knot/link invariant is a property of a knot/link that is independent of representation. Trivial Examples: • Crossing number • Knot Representations / ~ where 2 representations are equivalent via Reidemester moves Tricolorability We say a knot is tricolorable if the strands in any projection can be colored with 3 colors such that every crossing has 1 or 3 colors and or the coloring uses more than one color. -
On the Center of the Group of a Link
ON THE CENTER OF THE GROUP OF A LINK KUNIO MURASUGI 1. Introduction. A group G is said to be finitely presented if it has a finite presentation (P, i.e., (P consists of a finite number, « say, of gen- erators and a finite number, m say, of defining relations. The de- ficiency of (P, d((P), is defined as n—m. Then, by the deficiency, d(G), of G is meant the maximum of deficiencies of all finite presenta- tions of G. For example, it is well known that if G is a group with a single defining relation, i.e., w= 1, then d(G) =« —1 [l, p. 207]. Recently we proved [5] that for any group G with a single defining relation, if d(G) ^2 then the center, C(G), of G is trivial, and if d(G) = 1 and if G is not abelian, then either C(G) is trivial or infinite cyclic. This leads to the following conjecture. Conjecture. For any finitely presented group G, ifd(G) ^ 2 then C(G) is trivial, and if d(G) = 1 and if G is not abelian, then C(G) is either trivial or infinite cyclic. The purpose of this paper is to show that the conjecture is true for the group of any link in 3-sphere S3. Namely we obtain : Theorem 1. If a non-abelian link group G has a nontrivial center C(G), then C(G) is infinite cyclic. Remark. If d(G) ^2, then G must be a free product of two non- trivial groups.