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Mutant Knots and Intersection Graphs 1 Introduction
Mutant knots and intersection graphs S. V. CHMUTOV S. K. LANDO We prove that if a finite order knot invariant does not distinguish mutant knots, then the corresponding weight system depends on the intersection graph of a chord diagram rather than on the diagram itself. Conversely, if we have a weight system depending only on the intersection graphs of chord diagrams, then the composition of such a weight system with the Kontsevich invariant determines a knot invariant that does not distinguish mutant knots. Thus, an equivalence between finite order invariants not distinguishing mutants and weight systems depending on intersections graphs only is established. We discuss relationship between our results and certain Lie algebra weight systems. 57M15; 57M25 1 Introduction Below, we use standard notions of the theory of finite order, or Vassiliev, invariants of knots in 3-space; their definitions can be found, for example, in [6] or [14], and we recall them briefly in Section 2. All knots are assumed to be oriented. Two knots are said to be mutant if they differ by a rotation of a tangle with four endpoints about either a vertical axis, or a horizontal axis, or an axis perpendicular to the paper. If necessary, the orientation inside the tangle may be replaced by the opposite one. Here is a famous example of mutant knots, the Conway (11n34) knot C of genus 3, and Kinoshita–Terasaka (11n42) knot KT of genus 2 (see [1]). C = KT = Note that the change of the orientation of a knot can be achieved by a mutation in the complement to a trivial tangle. -
A Knot-Vice's Guide to Untangling Knot Theory, Undergraduate
A Knot-vice’s Guide to Untangling Knot Theory Rebecca Hardenbrook Department of Mathematics University of Utah Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 1 / 26 What is Not a Knot? Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 2 / 26 What is a Knot? 2 A knot is an embedding of the circle in the Euclidean plane (R ). 3 Also defined as a closed, non-self-intersecting curve in R . 2 Represented by knot projections in R . Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 3 / 26 Why Knots? Late nineteenth century chemists and physicists believed that a substance known as aether existed throughout all of space. Could knots represent the elements? Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 4 / 26 Why Knots? Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 5 / 26 Why Knots? Unfortunately, no. Nevertheless, mathematicians continued to study knots! Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 6 / 26 Current Applications Natural knotting in DNA molecules (1980s). Credit: K. Kimura et al. (1999) Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 7 / 26 Current Applications Chemical synthesis of knotted molecules – Dietrich-Buchecker and Sauvage (1988). Credit: J. Guo et al. (2010) Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 8 / 26 Current Applications Use of lattice models, e.g. the Ising model (1925), and planar projection of knots to find a knot invariant via statistical mechanics. Credit: D. Chicherin, V.P. -
Knot Theory: an Introduction
Knot theory: an introduction Zhen Huan Center for Mathematical Sciences Huazhong University of Science and Technology USTC, December 25, 2019 Knots in daily life Shoelace Zhen Huan (HUST) Knot theory: an introduction USTC, December 25, 2019 2 / 40 Knots in daily life Braids Zhen Huan (HUST) Knot theory: an introduction USTC, December 25, 2019 3 / 40 Knots in daily life Knot bread Zhen Huan (HUST) Knot theory: an introduction USTC, December 25, 2019 4 / 40 Knots in daily life German bread: the pretzel Zhen Huan (HUST) Knot theory: an introduction USTC, December 25, 2019 5 / 40 Knots in daily life Rope Mat Zhen Huan (HUST) Knot theory: an introduction USTC, December 25, 2019 6 / 40 Knots in daily life Chinese Knots Zhen Huan (HUST) Knot theory: an introduction USTC, December 25, 2019 7 / 40 Knots in daily life Knot bracelet Zhen Huan (HUST) Knot theory: an introduction USTC, December 25, 2019 8 / 40 Knots in daily life Knitting Zhen Huan (HUST) Knot theory: an introduction USTC, December 25, 2019 9 / 40 Knots in daily life More Knitting Zhen Huan (HUST) Knot theory: an introduction USTC, December 25, 2019 10 / 40 Knots in daily life DNA Zhen Huan (HUST) Knot theory: an introduction USTC, December 25, 2019 11 / 40 Knots in daily life Wire Mess Zhen Huan (HUST) Knot theory: an introduction USTC, December 25, 2019 12 / 40 History of Knots Chinese talking knots (knotted strings) Inca Quipu Zhen Huan (HUST) Knot theory: an introduction USTC, December 25, 2019 13 / 40 History of Knots Endless Knot in Buddhism Zhen Huan (HUST) Knot theory: an introduction -
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. -
Coefficients of Homfly Polynomial and Kauffman Polynomial Are Not Finite Type Invariants
COEFFICIENTS OF HOMFLY POLYNOMIAL AND KAUFFMAN POLYNOMIAL ARE NOT FINITE TYPE INVARIANTS GYO TAEK JIN AND JUNG HOON LEE Abstract. We show that the integer-valued knot invariants appearing as the nontrivial coe±cients of the HOMFLY polynomial, the Kau®man polynomial and the Q-polynomial are not of ¯nite type. 1. Introduction A numerical knot invariant V can be extended to have values on singular knots via the recurrence relation V (K£) = V (K+) ¡ V (K¡) where K£, K+ and K¡ are singular knots which are identical outside a small ball in which they di®er as shown in Figure 1. V is said to be of ¯nite type or a ¯nite type invariant if there is an integer m such that V vanishes for all singular knots with more than m singular double points. If m is the smallest such integer, V is said to be an invariant of order m. q - - - ¡@- @- ¡- K£ K+ K¡ Figure 1 As the following proposition states, every nontrivial coe±cient of the Alexander- Conway polynomial is a ¯nite type invariant [1, 6]. Theorem 1 (Bar-Natan). Let K be a knot and let 2 4 2m rK (z) = 1 + a2(K)z + a4(K)z + ¢ ¢ ¢ + a2m(K)z + ¢ ¢ ¢ be the Alexander-Conway polynomial of K. Then a2m is a ¯nite type invariant of order 2m for any positive integer m. The coe±cients of the Taylor expansion of any quantum polynomial invariant of knots after a suitable change of variable are all ¯nite type invariants [2]. For the Jones polynomial we have Date: October 17, 2000 (561). -
Introduction to Vassiliev Knot Invariants First Draft. Comments
Introduction to Vassiliev Knot Invariants First draft. Comments welcome. July 20, 2010 S. Chmutov S. Duzhin J. Mostovoy The Ohio State University, Mansfield Campus, 1680 Univer- sity Drive, Mansfield, OH 44906, USA E-mail address: [email protected] Steklov Institute of Mathematics, St. Petersburg Division, Fontanka 27, St. Petersburg, 191011, Russia E-mail address: [email protected] Departamento de Matematicas,´ CINVESTAV, Apartado Postal 14-740, C.P. 07000 Mexico,´ D.F. Mexico E-mail address: [email protected] Contents Preface 8 Part 1. Fundamentals Chapter 1. Knots and their relatives 15 1.1. Definitions and examples 15 § 1.2. Isotopy 16 § 1.3. Plane knot diagrams 19 § 1.4. Inverses and mirror images 21 § 1.5. Knot tables 23 § 1.6. Algebra of knots 25 § 1.7. Tangles, string links and braids 25 § 1.8. Variations 30 § Exercises 34 Chapter 2. Knot invariants 39 2.1. Definition and first examples 39 § 2.2. Linking number 40 § 2.3. Conway polynomial 43 § 2.4. Jones polynomial 45 § 2.5. Algebra of knot invariants 47 § 2.6. Quantum invariants 47 § 2.7. Two-variable link polynomials 55 § Exercises 62 3 4 Contents Chapter 3. Finite type invariants 69 3.1. Definition of Vassiliev invariants 69 § 3.2. Algebra of Vassiliev invariants 72 § 3.3. Vassiliev invariants of degrees 0, 1 and 2 76 § 3.4. Chord diagrams 78 § 3.5. Invariants of framed knots 80 § 3.6. Classical knot polynomials as Vassiliev invariants 82 § 3.7. Actuality tables 88 § 3.8. Vassiliev invariants of tangles 91 § Exercises 93 Chapter 4. -
CALIFORNIA STATE UNIVERSITY, NORTHRIDGE P-Coloring Of
CALIFORNIA STATE UNIVERSITY, NORTHRIDGE P-Coloring of Pretzel Knots A thesis submitted in partial fulfillment of the requirements for the degree of Master of Science in Mathematics By Robert Ostrander December 2013 The thesis of Robert Ostrander is approved: |||||||||||||||||| |||||||| Dr. Alberto Candel Date |||||||||||||||||| |||||||| Dr. Terry Fuller Date |||||||||||||||||| |||||||| Dr. Magnhild Lien, Chair Date California State University, Northridge ii Dedications I dedicate this thesis to my family and friends for all the help and support they have given me. iii Acknowledgments iv Table of Contents Signature Page ii Dedications iii Acknowledgements iv Abstract vi Introduction 1 1 Definitions and Background 2 1.1 Knots . .2 1.1.1 Composition of knots . .4 1.1.2 Links . .5 1.1.3 Torus Knots . .6 1.1.4 Reidemeister Moves . .7 2 Properties of Knots 9 2.0.5 Knot Invariants . .9 3 p-Coloring of Pretzel Knots 19 3.0.6 Pretzel Knots . 19 3.0.7 (p1, p2, p3) Pretzel Knots . 23 3.0.8 Applications of Theorem 6 . 30 3.0.9 (p1, p2, p3, p4) Pretzel Knots . 31 Appendix 49 v Abstract P coloring of Pretzel Knots by Robert Ostrander Master of Science in Mathematics In this thesis we give a brief introduction to knot theory. We define knot invariants and give examples of different types of knot invariants which can be used to distinguish knots. We look at colorability of knots and generalize this to p-colorability. We focus on 3-strand pretzel knots and apply techniques of linear algebra to prove theorems about p-colorability of these knots. -
Alexander Polynomial, Finite Type Invariants and Volume of Hyperbolic
ISSN 1472-2739 (on-line) 1472-2747 (printed) 1111 Algebraic & Geometric Topology Volume 4 (2004) 1111–1123 ATG Published: 25 November 2004 Alexander polynomial, finite type invariants and volume of hyperbolic knots Efstratia Kalfagianni Abstract We show that given n > 0, there exists a hyperbolic knot K with trivial Alexander polynomial, trivial finite type invariants of order ≤ n, and such that the volume of the complement of K is larger than n. This contrasts with the known statement that the volume of the comple- ment of a hyperbolic alternating knot is bounded above by a linear function of the coefficients of the Alexander polynomial of the knot. As a corollary to our main result we obtain that, for every m> 0, there exists a sequence of hyperbolic knots with trivial finite type invariants of order ≤ m but ar- bitrarily large volume. We discuss how our results fit within the framework of relations between the finite type invariants and the volume of hyperbolic knots, predicted by Kashaev’s hyperbolic volume conjecture. AMS Classification 57M25; 57M27, 57N16 Keywords Alexander polynomial, finite type invariants, hyperbolic knot, hyperbolic Dehn filling, volume. 1 Introduction k i Let c(K) denote the crossing number and let ∆K(t) := Pi=0 cit denote the Alexander polynomial of a knot K . If K is hyperbolic, let vol(S3 \ K) denote the volume of its complement. The determinant of K is the quantity det(K) := |∆K(−1)|. Thus, in general, we have k det(K) ≤ ||∆K (t)|| := X |ci|. (1) i=0 It is well know that the degree of the Alexander polynomial of an alternating knot equals twice the genus of the knot. -
Results on Nonorientable Surfaces for Knots and 2-Knots
University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Dissertations, Theses, and Student Research Papers in Mathematics Mathematics, Department of 8-2021 Results on Nonorientable Surfaces for Knots and 2-knots Vincent Longo University of Nebraska-Lincoln, [email protected] Follow this and additional works at: https://digitalcommons.unl.edu/mathstudent Part of the Geometry and Topology Commons Longo, Vincent, "Results on Nonorientable Surfaces for Knots and 2-knots" (2021). Dissertations, Theses, and Student Research Papers in Mathematics. 111. https://digitalcommons.unl.edu/mathstudent/111 This Article is brought to you for free and open access by the Mathematics, Department of at DigitalCommons@University of Nebraska - Lincoln. It has been accepted for inclusion in Dissertations, Theses, and Student Research Papers in Mathematics by an authorized administrator of DigitalCommons@University of Nebraska - Lincoln. RESULTS ON NONORIENTABLE SURFACES FOR KNOTS AND 2-KNOTS by Vincent Longo A DISSERTATION Presented to the Faculty of The Graduate College at the University of Nebraska In Partial Fulfillment of Requirements For the Degree of Doctor of Philosophy Major: Mathematics Under the Supervision of Professors Alex Zupan and Mark Brittenham Lincoln, Nebraska May, 2021 RESULTS ON NONORIENTABLE SURFACES FOR KNOTS AND 2-KNOTS Vincent Longo, Ph.D. University of Nebraska, 2021 Advisor: Alex Zupan and Mark Brittenham A classical knot is a smooth embedding of the circle S1 into the 3-sphere S3. We can also consider embeddings of arbitrary surfaces (possibly nonorientable) into a 4-manifold, called knotted surfaces. In this thesis, we give an introduction to some of the basics of the studies of classical knots and knotted surfaces, then present some results about nonorientable surfaces bounded by classical knots and embeddings of nonorientable knotted surfaces. -
Knot Cobordisms, Bridge Index, and Torsion in Floer Homology
KNOT COBORDISMS, BRIDGE INDEX, AND TORSION IN FLOER HOMOLOGY ANDRAS´ JUHASZ,´ MAGGIE MILLER AND IAN ZEMKE Abstract. Given a connected cobordism between two knots in the 3-sphere, our main result is an inequality involving torsion orders of the knot Floer homology of the knots, and the number of local maxima and the genus of the cobordism. This has several topological applications: The torsion order gives lower bounds on the bridge index and the band-unlinking number of a knot, the fusion number of a ribbon knot, and the number of minima appearing in a slice disk of a knot. It also gives a lower bound on the number of bands appearing in a ribbon concordance between two knots. Our bounds on the bridge index and fusion number are sharp for Tp;q and Tp;q#T p;q, respectively. We also show that the bridge index of Tp;q is minimal within its concordance class. The torsion order bounds a refinement of the cobordism distance on knots, which is a metric. As a special case, we can bound the number of band moves required to get from one knot to the other. We show knot Floer homology also gives a lower bound on Sarkar's ribbon distance, and exhibit examples of ribbon knots with arbitrarily large ribbon distance from the unknot. 1. Introduction The slice-ribbon conjecture is one of the key open problems in knot theory. It states that every slice knot is ribbon; i.e., admits a slice disk on which the radial function of the 4-ball induces no local maxima. -
ON TANGLES and MATROIDS 1. Introduction Two Binary Operations on Matroids, the Two-Sum and the Tensor Product, Were Introduced I
ON TANGLES AND MATROIDS STEPHEN HUGGETT School of Mathematics and Statistics University of Plymouth, Plymouth PL4 8AA, Devon ABSTRACT Given matroids M and N there are two operations M ⊕2 N and M ⊗ N. When M and N are the cycle matroids of planar graphs these operations have interesting interpretations on the corresponding link diagrams. In fact, given a planar graph there are two well-established methods of generating an alternating link diagram, and in each case the Tutte polynomial of the graph is related to polynomial invariant (Jones or homfly) of the link. Switching from one of these methods to the other corresponds in knot theory to tangle insertion in the link diagrams, and in combinatorics to the tensor product of the cycle matroids of the graphs. Keywords: tangles, knots, Jones polynomials, Tutte polynomials, matroids 1. Introduction Two binary operations on matroids, the two-sum and the tensor product, were introduced in [13] and [4]. In the case when the matroids are the cycle matroids of graphs these give rise to corresponding operations on graphs. Strictly speaking, however, these operations on graphs are not in general well defined, being sensitive to the Whitney twist. Consider the two-sum for a moment: when it is well defined it can be seen simply in terms of the replacement of an edge by a new subgraph: a special case of this is the operation leading to the homeomorphic graphs studied in [11]. Planar graphs define alternating link diagrams, and so the two-sum and tensor product operations are defined on these too: they correspond to insertions of tangles. -
TANGLES for KNOTS and LINKS 1. Introduction It Is
TANGLES FOR KNOTS AND LINKS ZACHARY ABEL 1. Introduction It is often useful to discuss only small \pieces" of a link or a link diagram while disregarding everything else. For example, the Reidemeister moves describe manipulations surrounding at most 3 crossings, and the skein relations for the Jones and Conway polynomials discuss modifications on one crossing at a time. Tangles may be thought of as small pieces or a local pictures of knots or links, and they provide a useful language to describe the above manipulations. But the power of tangles in knot and link theory extends far beyond simple diagrammatic convenience, and this article provides a short survey of some of these applications. 2. Tangles As Used in Knot Theory Formally, we define a tangle as follows (in this article, everything is in the PL category): Definition 1. A tangle is a pair (A; t) where A =∼ B3 is a closed 3-ball and t is a proper 1-submanifold with @t 6= ;. Note that t may be disconnected and may contain closed loops in the interior of A. We consider two tangles (A; t) and (B; u) equivalent if they are isotopic as pairs of embedded manifolds. An n-string tangle consists of exactly n arcs and 2n boundary points (and no closed loops), and the trivial n-string 2 tangle is the tangle (B ; fp1; : : : ; png) × [0; 1] consisting of n parallel, unintertwined segments. See Figure 1 for examples of tangles. Note that with an appropriate isotopy any tangle (A; t) may be transformed into an equivalent tangle so that A is the unit ball in R3, @t = A \ t lies on the great circle in the xy-plane, and the projection (x; y; z) 7! (x; y) is a regular projection for t; thus, tangle diagrams as shown in Figure 1 are justified for all tangles.