Finite Type Invariants for Knotoids
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Complete Invariant Graphs of Alternating Knots
Complete invariant graphs of alternating knots Christian Soulié First submission: April 2004 (revision 1) Abstract : Chord diagrams and related enlacement graphs of alternating knots are enhanced to obtain complete invariant graphs including chirality detection. Moreover, the equivalence by common enlacement graph is specified and the neighborhood graph is defined for general purpose and for special application to the knots. I - Introduction : Chord diagrams are enhanced to integrate the state sum of all flype moves and then produce an invariant graph for alternating knots. By adding local writhe attribute to these graphs, chiral types of knots are distinguished. The resulting chord-weighted graph is a complete invariant of alternating knots. Condensed chord diagrams and condensed enlacement graphs are introduced and a new type of graph of general purpose is defined : the neighborhood graph. The enlacement graph is enriched by local writhe and chord orientation. Hence this enhanced graph distinguishes mutant alternating knots. As invariant by flype it is also invariant for all alternating knots. The equivalence class of knots with the same enlacement graph is fully specified and extended mutation with flype of tangles is defined. On this way, two enhanced graphs are proposed as complete invariants of alternating knots. I - Introduction II - Definitions and condensed graphs II-1 Knots II-2 Sign of crossing points II-3 Chord diagrams II-4 Enlacement graphs II-5 Condensed graphs III - Realizability and construction III - 1 Realizability -
Finite Type Invariants for Knots 3-Manifolds
Pergamon Topology Vol. 37, No. 3. PP. 673-707, 1998 ~2 1997 Elsevier Science Ltd Printed in Great Britain. All rights reserved 0040-9383/97519.00 + 0.00 PII: soo4o-9383(97)00034-7 FINITE TYPE INVARIANTS FOR KNOTS IN 3-MANIFOLDS EFSTRATIA KALFAGIANNI + (Received 5 November 1993; in revised form 4 October 1995; final version 16 February 1997) We use the Jaco-Shalen and Johannson theory of the characteristic submanifold and the Torus theorem (Gabai, Casson-Jungreis)_ to develop an intrinsic finite tvne__ theory for knots in irreducible 3-manifolds. We also establish a relation between finite type knot invariants in 3-manifolds and these in R3. As an application we obtain the existence of non-trivial finite type invariants for knots in irreducible 3-manifolds. 0 1997 Elsevier Science Ltd. All rights reserved 0. INTRODUCTION The theory of quantum groups gives a systematic way of producing families of polynomial invariants, for knots and links in [w3 or S3 (see for example [18,24]). In particular, the Jones polynomial [12] and its generalizations [6,13], can be obtained that way. All these Jones-type invariants are defined as state models on a knot diagram or as traces of a braid group representation. On the other hand Vassiliev [25,26], introduced vast families of numerical knot invariants (Jinite type invariants), by studying the topology of the space of knots in [w3. The compu- tation of these invariants, involves in an essential way the computation of related invariants for special knotted graphs (singular knots). It is known [l-3], that after a suitable change of variable the coefficients of the power series expansions of the Jones-type invariants, are of Jinite type. -
Finite Type Invariants of W-Knotted Objects Iii: the Double Tree Construction
FINITE TYPE INVARIANTS OF W-KNOTTED OBJECTS III: THE DOUBLE TREE CONSTRUCTION DROR BAR-NATAN AND ZSUZSANNA DANCSO Abstract. This is the third in a series of papers studying the finite type invariants of various w-knotted objects and their relationship to the Kashiwara-Vergne problem and Drinfel’d associators. In this paper we present a topological solution to the Kashiwara- Vergne problem.AlekseevEnriquezTorossian:ExplicitSolutions In particular we recover via a topological argument the Alkeseev-Enriquez- Torossian [AET] formula for explicit solutions of the Kashiwara-Vergne equations in terms of associators. We study a class of w-knotted objects: knottings of 2-dimensional foams and various associated features in four-dimensioanl space. We use a topological construction which we name the double tree construction to show that every expansion (also known as universal fi- nite type invariant) of parenthesized braids extends first to an expansion of knotted trivalent graphs (a well known result), and then extends uniquely to an expansion of the w-knotted objects mentioned above. In algebraic language, an expansion for parenthesized braids is the same as a Drin- fel’d associator Φ, and an expansion for the aforementionedKashiwaraVergne:Conjecture w-knotted objects is the same as a solutionAlekseevTorossian:KashiwaraVergneV of the Kashiwara-Vergne problem [KV] as reformulated by AlekseevAlekseevEnriquezTorossian:E and Torossian [AT]. Hence our result provides a topological framework for the result of [AET] that “there is a formula for V in terms of Φ”, along with an independent topological proof that the said formula works — namely that the equations satisfied by V follow from the equations satisfied by Φ. -
Computing the Writhing Number of a Polygonal Knot
Computing the Writhing Number of a Polygonal Knot ¡ ¡£¢ ¡ Pankaj K. Agarwal Herbert Edelsbrunner Yusu Wang Abstract Here the linking number, , is half the signed number of crossings between the two boundary curves of the ribbon, The writhing number measures the global geometry of a and the twisting number, , is half the average signed num- closed space curve or knot. We show that this measure is ber of local crossing between the two curves. The non-local related to the average winding number of its Gauss map. Us- crossings between the two curves correspond to crossings ing this relationship, we give an algorithm for computing the of the ribbon axis, which are counted by the writhing num- ¤ writhing number for a polygonal knot with edges in time ber, . A small subset of the mathematical literature on ¥§¦ ¨ roughly proportional to ¤ . We also implement a different, the subject can be found in [3, 20]. Besides the mathemat- simple algorithm and provide experimental evidence for its ical interest, the White Formula and the writhing number practical efficiency. have received attention both in physics and in biochemistry [17, 23, 26, 30]. For example, they are relevant in under- standing various geometric conformations we find for circu- 1 Introduction lar DNA in solution, as illustrated in Figure 1 taken from [7]. By representing DNA as a ribbon, the writhing number of its The writhing number is an attempt to capture the physical phenomenon that a cord tends to form loops and coils when it is twisted. We model the cord by a knot, which we define to be an oriented closed curve in three-dimensional space. -
A Remarkable 20-Crossing Tangle Shalom Eliahou, Jean Fromentin
A remarkable 20-crossing tangle Shalom Eliahou, Jean Fromentin To cite this version: Shalom Eliahou, Jean Fromentin. A remarkable 20-crossing tangle. 2016. hal-01382778v2 HAL Id: hal-01382778 https://hal.archives-ouvertes.fr/hal-01382778v2 Preprint submitted on 16 Jan 2017 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. A REMARKABLE 20-CROSSING TANGLE SHALOM ELIAHOU AND JEAN FROMENTIN Abstract. For any positive integer r, we exhibit a nontrivial knot Kr with r− r (20·2 1 +1) crossings whose Jones polynomial V (Kr) is equal to 1 modulo 2 . Our construction rests on a certain 20-crossing tangle T20 which is undetectable by the Kauffman bracket polynomial pair mod 2. 1. Introduction In [6], M. B. Thistlethwaite gave two 2–component links and one 3–component link which are nontrivial and yet have the same Jones polynomial as the corre- sponding unlink U 2 and U 3, respectively. These were the first known examples of nontrivial links undetectable by the Jones polynomial. Shortly thereafter, it was shown in [2] that, for any integer k ≥ 2, there exist infinitely many nontrivial k–component links whose Jones polynomial is equal to that of the k–component unlink U k. -
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). -
On Finite Type 3-Manifold Invariants Iii: Manifold Weight Systems
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Pergamon Top&y?. Vol. 37, No. 2, PP. 221.243, 1998 ~2 1997 Elsevw Science Ltd Printed in Great Britain. All rights reserved 0040-9383/97 $19.00 + 0.00 PII: SOO40-9383(97)00028-l ON FINITE TYPE 3-MANIFOLD INVARIANTS III: MANIFOLD WEIGHT SYSTEMS STAVROSGAROUFALIDIS and TOMOTADAOHTSUKI (Received for publication 9 June 1997) The present paper is a continuation of [11,6] devoted to the study of finite type invariants of integral homology 3-spheres. We introduce the notion of manifold weight systems, and show that type m invariants of integral homology 3-spheres are determined (modulo invariants of type m - 1) by their associated manifold weight systems. In particular, we deduce a vanishing theorem for finite type invariants. We show that the space of manifold weight systems forms a commutative, co-commutative Hopf algebra and that the map from finite type invariants to manifold weight systems is an algebra map. We conclude with better bounds for the graded space of finite type invariants of integral homology 3-spheres. 0 1997 Elsevier Science Ltd. All rights reserved 1. INTRODUCTION 1.1. History The present paper is a continuation of [ll, 63 devoted to the study of finite type invariants of oriented integral homology 3-spheres. There are two main sources of motivation for the present work: (perturbative) Chern-Simons theory in three dimensions, and Vassiliev invariants of knots in S3. Witten [16] in his seminal paper, using path integrals (an infinite dimensional “integra- tion” method) introduced a topological quantum field theory in three dimensions whose Lagrangian was the Chern-Simons function on the space of all connections. -
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. -
Some Remarks on the Chord Index
Some remarks on the chord index Hongzhu Gao A joint work with Prof. Zhiyun Cheng and Dr. Mengjian Xu Beijing Normal University Novosibirsk State University June 17-21, 2019 1 / 54 Content 1. A brief review on virtual knot theory 2. Two virtual knot invariants derived from the chord index 3. From the viewpoint of finite type invariant 4. Flat virtual knot invariants 2 / 54 A brief review on virtual knot theory Classical knot theory: Knot types=fknot diagramsg/fReidemeister movesg Ω1 Ω2 Ω3 Figure 1: Reidemeister moves Virtual knot theory: Besides over crossing and under crossing, we add another structure to a crossing point: virtual crossing virtual crossing b Figure 2: virtual crossing 3 / 54 A brief review on virtual knot theory Virtual knot types= fall virtual knot diagramsg/fgeneralized Reidemeister movesg Ω1 Ω2 Ω3 Ω10 Ω20 Ω30 s Ω3 Figure 3: generalized Reidemeister moves 4 / 54 A brief review on virtual knot theory Flat virtual knots (or virtual strings by Turaev) can be regarded as virtual knots without over/undercrossing information. More precisely, a flat virtual knot diagram can be obtained from a virtual knot diagram by replacing all real crossing points with flat crossing points. By replacing all real crossing points with flat crossing points in Figure 3 one obtains the flat generalized Reidemeister moves. Then Flat virtual knot types= fall flat virtual knot diagramsg/fflat generalized Reidemeister movesg 5 / 54 A brief review on virtual knot theory Virtual knot theory was introduced by L. Kauffman. Roughly speaking, there are two motivations to extend the classical knot theory to virtual knot theory. -
The Hyperbolic Volume of Knots from Quantum Dilogarithm
The hyperbolic volume of knots from quantum dilogarithm R.M. Kashaev∗ Laboratoire de Physique Th´eorique enslapp† ENSLyon, 46 All´ee d’Italie, 69007 Lyon, FRANCE E-mail: [email protected] January, 1996 Abstract The invariant of a link in three-sphere, associated with the cyclic quantum dilogarithm, depends on a natural number N. By the analysis of particular examples it is argued that for a hyperbolic knot (link) the absolute value of this invariant grows exponentially at large N, the hyperbolic volume of the knot (link) complement being the growth rate. arXiv:q-alg/9601025v2 25 Mar 1996 ENSLAPP-L-577/96 ∗On leave of absence from St. Petersburg Branch of the Steklov Mathematical Institute, Fontanka 27, St. Petersburg 191011, RUSSIA †URA 14-36 du CNRS, associ´ee `al’E.N.S. de Lyon, au LAPP d’Annecy et `al’Universit`e de Savoie 1 1 Introduction Many known knot and link invariants, including Alexander [1] and Jones [2] polynomials, can be obtained from R-matrices, solutions to the Yang-Baxter equation (YBE) [3, 4]. Remarkably, many R-matrices in turn appear in quantum 3-dimensional Chern-Simons (CS) theory as partition functions of a 3-manifold with boundary, and with properly chosen Wilson lines [8]. The corresponding knot invariant acquires an interpretation in terms of a meanvalue of a Wilson loop. Note, that the quantum CS theory is an example of the topological quantum field theory (TQFT) defined axiomatically in [9]. Thurston in his theory of hyperbolic 3-manifolds [5] introduces the notion of a hyperbolic knot: a knot that has a complement that can be given a metric of negative constant curvature. -
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. -
Exact Results for Perturbative Chern–Simons Theory with Complex Gauge Group Tudor Dimofte, Sergei Gukov, Jonatan Lenells and Don Zagier
communications in number theory and physics Volume 3, Number 2, 363–443, 2009 Exact results for perturbative Chern–Simons theory with complex gauge group Tudor Dimofte, Sergei Gukov, Jonatan Lenells and Don Zagier We develop several methods that allow us to compute all-loop par- tition functions in perturbative Chern–Simons theory with com- plex gauge group GC, sometimes in multiple ways. In the back- ground of a non-abelian irreducible flat connection, perturbative GC invariants turn out to be interesting topological invariants, which are very different from the finite-type (Vassiliev) invariants usually studied in a theory with compact gauge group G and a triv- ial flat connection. We explore various aspects of these invariants and present an example where we compute them explicitly to high loop order. We also introduce a notion of “arithmetic topological quantum field theory” and conjecture (with supporting numerical evidence) that SL(2, C) Chern–Simons theory is an example of such a theory. 1. Introduction and summary 364 2. Perturbation theory around a non-trivial flat connection 373 2.1. Feynman diagrams and arithmetic TQFT 374 2.2. Quantization of Mflat(GC, Σ) 380 2.2.1 Analytic continuation. 384 2.2.2 A hierarchy of differential equations. 386 2.3. Classical and quantum symmetries 390 2.4. Brane quantization 394 3. A state integral model for perturbative SL(2, C) Chern−Simons theory 396 3.1. Ideal triangulations of hyperbolic 3-manifolds 397 363 364 Tudor Dimofte, Sergei Gukov, Jonatan Lenells and Don Zagier 3.2. Hikami’s invariant 402 3.3.