Coefficients of Homfly Polynomial and Kauffman Polynomial Are Not Finite Type Invariants

Total Page:16

File Type:pdf, Size:1020Kb

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). 2000 Mathematics Subject Classi¯cation. 57M27. Key words and phrases. knot, ¯nite type invariant, homfly polynomial, Kau®man polynomial. This work was supported by Brain Korea 21 Project. 1 2 G.T. JIN AND J.H. LEE Theorem 2 (Birman-Lin). Let K be a knot and let JK (t) be its Jones polynomial. x Let UK (x) be obtained from JK (t) by replacing the variable t by e . Express UK (x) as a power series in x: X1 n UK (x) = un(K)x : n=0 Then u0 ´ 1 and, for each n ¸ 1, un is an invariant of order (at most) n. But the coe±cients of the original Jones polynomial are all non-¯nite type in- variants. Theorem 3 (Zhu). Let K be a knot and let X1 n JK (t) = bn(K)t n=¡1 be the Jones polynomial of K. Then bn is not a ¯nite type invariant for any n. 2. HOMFLY polynomial The HOMFLY polynomial PK (v; z) of an oriented knot or link K is determined by the following two conditions: (H1) PO(v; z) = 1, where O is the trivial knot. (H2) For three knots or links K+, K¡ and K0 which are identical outside a small ball in which they di®er as shown in Figure 2, we have the relation: ¡1 v PK+ (v; z) ¡ vPK¡ (v; z) = zPK0 (v; z) - - - @- ¡- - K+ K¡ K0 Figure 2 Theorem 4. Let K be a knot and let X i j PK (v; z) = cij (K)v z : Then, cij is not a ¯nite type invarianat if i, j are even integers with j ¸ 0, and cij = 0 for any knot otherwise. Let Tn and Kn denote the torus knot of type (2; 2n + 1) and the torus knot of type (2; 2n + 1) together with 2n singular crossings, respectively, as shown in Figure 3. Let E denote the ¯gure eight knot. For a knot K, let Kl denote the iterated connected sum K] ¢ ¢ ¢ ]K of l copies of K. For a knot or a singular knot K, let K¹ denote the mirror image of K. To simplify notations, let P (K) denote the HOMFLY polynomial PK (v; z) of K. Lemma 5. Let n ¸ 1. Then l (a) c2l;2m(T1]Tn) = 0, for l ¸ 0. m m¡l (b) c2l;2m(T1 ]E ]Tn) = 0, for m > l ¸ 0. COEFFICIENTS OF HOMFLY POLYNOMIAL AND KAUFFMAN POLYNOMIAL 3 - 2n + 1 - 2n + 1 2n - - q q Tn Kn Figure 3 Proof. We have 2 2 2 P (T1) = v (2 + z ¡ v ) P (E) = v¡2(1 ¡ (1 + z2)v2 + v4) and inductively, we may show that the minimum v-degree of P (Tn) is 2n. Therefore l l m m¡l the minimum v-degrees of P (T1]Tn) = P (T1) ¢ P (Tn) and P (T1 ]E ]Tn) = m m¡l P (T1) ¢ P (E) ¢ P (Tn) are both 2l + 2n > 2l. This completes the proof. Proof of Theorem 4. It is an elementary result that cij(K) = 0 for any knot K when j < 0 or at least one of i and j is an odd integer. Now we show that there exist singular knots with arbitrarily many singular double points on which c2l;2m with m ¸ 0 does not vanish. When l ¸ 0, we have two cases: Case 1. l ¸ m ¸ 0 : If we resolve any p singular crossings of Kn into negative crossings and the rest 2n ¡ p into positive ones, we obtain T2n¡p. By Lemma 5(a), l 2l 2 2 l and since P (T1) = v (2 + z ¡ v ) , we have µ ¶ X2n 2n c (T l]K ) = (¡1)p c (T l]T ) 2l;2m 1 n p 2l;2m 1 2n¡p p=0 µ ¶ l = c (T l) = 2l¡m 6= 0 2l;2m 1 m for any n ¸ 1: Case 2. m > l ¸ 0 : By Lemma 5(b), and since m m¡l 2l 2 2 m 2 2 4 m¡l P (T1 ]E ) = v (2 ¡ v + z ) (1 ¡ (1 + z )v + v ) we have µ ¶ X2n 2n c (T m]Em¡l]K ) = (¡1)p c (T m]Em¡l]T ) 2l;2m 1 n p 2l;2m 1 2n¡p p=0 m m¡l = c2l;2m(T1 ]E ) = 1 6= 0 for any n ¸ 1: ¡1 Let l < 0. Combining the fact PK¹ (v; z) = PK (¡v ; z) with the above two cases, we obtain ¹jlj ¹ jlj c2l;2m(T1 ]Kn) = cj2lj;2m(T1 ]Kn) 6= 0 if jlj ¸ m ¸ 0, and ¹m m¡jlj ¹ m m¡jlj c2l;2m(T1 ]E ]Kn) = cj2lj;2m(T1 ]E ]Kn) 6= 0 if m > jlj. Consequently, c2l;2m is not a ¯nite type invariant for any l and for any m ¸ 0. 4 G.T. JIN AND J.H. LEE 3. Kauffman polynomial The Kau®man polynomial FK (a; x) of an oriented knot or link K is de¯ned by ¡w(D) FK (a; x) = a ¤D(a; x) where D is a diagram of K, w(D) its writhe and ¤D(a; x) the polynomial determined by the following conditions: (K1) ¤O(a; x) = 1 where O is the trivial knot diagram. (K2) For any four diagrams D+, D¡, D0 and D1 which are identical outside a small disk in which they di®er as shown in Figure 4, we have the relation: ¤D+ (a; x) + ¤D¡ (a; x) = x(¤D0 (a; x) + ¤D1 (a; x)) @ ¡ D+ D¡ D0 D1 Figure 4 (K3) For any three diagrams D+, D and D¡ which are identical outside a small disk in which they di®er as shown in Figure 5, we have the relation: ¡1 a ¤D+ (a; x) = ¤D(a; x) = a ¤D¡ (a; x) @ ¡ D+ D D¡ Figure 5 Theorem 6. Let K be a knot and let X i j FK (a; x) = dij (K)a x : Then, dij is not a ¯nite type invariant if i, j are integers with i + j even and j ¸ 0, and dij = for any knot otherwise. Lemma 7. Let n ¸ 1. Then ¹l ¹ ¹l ¹ (a) d2l;2m(T1]Tn) = d2l+1;2m+1(T1]Tn) = 0, for l ¸ 0. ¹l+1 ¹ (b) d2l+1;2l+1(T1 ]E]Tn) = 0, for l ¸ 0. ¹m m¡l ¹ ¹m m¡l ¹ (c) d2l;2m(T1 ]E ]Tn) = d2l+1;2m+1(T1 ]E ]Tn) = 0, for m > l ¸ 0. Proof. To simplify notations, let F (K) denote the Kau®man polynomial FK (a; x) of K. We have 2 2 2 2 3 F (T¹1) = a (¡2 + x + ax + a (¡1 + x ) + a x) F (E) = a¡2((1 + ax)(¡1 + x2) + a2(¡1 + 2x2) + a3(¡x + x3) + a4(¡1 + x2)) COEFFICIENTS OF HOMFLY POLYNOMIAL AND KAUFFMAN POLYNOMIAL 5 and inductively, we may show that the minimum a-degree of F (T¹n) is 2n. The ¹l ¹ ¹ l ¹ minimum a-degree of F (T1]Tn) = F (T1) ¢ F (Tn) is 2l + 2n > 2l + 1. This proves ¹l+1 ¹ ¹ l+1 ¹ the part (a). The minimum a-degrees of F (T1 ]E]Tn) = F (T1) ¢ F (E) ¢ F (Tn) ¹m m¡l ¹ ¹ m m¡l ¹ and F (T1 ]E ]Tn) = F (T1) ¢ F (E) ¢ F (Tn) are both 2l + 2n > 2l + 1. This proves the parts (b) and (c). Proof of Theorem 6. It is an elementary result that dij(K) = 0 for any knot K when j < 0 or i + j is odd. Part 1. We show that d2l;2m is not of ¯nite type by ¯nding singular knots with arbitrarily many double points making d2l;2m 6= 0. ¹l ¹ If l ¸ m ¸ 0, we consider the singular knot T1]Kn. Since the coe±cient of 2l 2m ¹l ¹ l 2m 2 l a x in F (T1) = F (T1) is equal to that of x in (¡2+x ) and by Lemma 7(a), we have µ ¶ X2n 2n d (T¹l]K¹ ) = (¡1)p d (T¹l]T¹ ) 2l;2m 1 n p 2l;2m 1 2n¡p p=0 µ ¶ l = d (T¹l) = (¡2)l¡m 6= 0 2l;2m 1 m for any n ¸ 1.
Recommended publications
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • Section 10.2. New Polynomial Invariants
    10.2. New Polynomial Invariants 1 Section 10.2. New Polynomial Invariants Note. In this section we mention the Jones polynomial and give a recursion for- mula for the HOMFLY polynomial. We give an example of the computation of a HOMFLY polynomial. Note. Vaughan F. R. Jones introduced a new knot polynomial in: A Polynomial Invariant for Knots via von Neumann Algebra, Bulletin of the American Mathe- matical Society, 12, 103–111 (1985). A copy is available online at the AMS.org website (accessed 4/11/2021). This is now known as the Jones polynomial. It is also a knot invariant and so can be used to potentially distinguish between knots. Shortly after the appearance of Jones’ paper, it was observed that the recursion techniques used to find the Jones polynomial and Conway polynomial can be gen- eralized to a 2-variable polynomial that contains information beyond that of the Jones and Conway polynomials. Note. The 2-variable polynomial was presented in: P. Freyd, D. Yetter, J. Hoste, W.B.R. Lickorish, and A. Ocneanu, A New Polynomial of Knots and Links, Bul- letin of the American Mathematical Society, 12(2): 239–246 (1985). This paper is also available online at the AMS.org website (accessed 4/11/2021). Based on a permutation of the first letters of the names of the authors, this has become knows as the “HOMFLY polynomial.” 10.2. New Polynomial Invariants 2 Definition. The HOMFLY polynomial, PL(`, m), is given by the recursion formula −1 `PL+ (`, m) + ` PL− (`, m) = −mPLS (`, m), and the condition PU (`, m) = 1 for U the unknot.
    [Show full text]
  • 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.
    [Show full text]
  • Restrictions on Homflypt and Kauffman Polynomials Arising from Local Moves
    RESTRICTIONS ON HOMFLYPT AND KAUFFMAN POLYNOMIALS ARISING FROM LOCAL MOVES SANDY GANZELL, MERCEDES GONZALEZ, CHLOE' MARCUM, NINA RYALLS, AND MARIEL SANTOS Abstract. We study the effects of certain local moves on Homflypt and Kauffman polynomials. We show that all Homflypt (or Kauffman) polynomials are equal in a certain nontrivial quotient of the Laurent polynomial ring. As a consequence, we discover some new properties of these invariants. 1. Introduction The Jones polynomial has been widely studied since its introduction in [5]. Divisibility criteria for the Jones polynomial were first observed by Jones 3 in [6], who proved that 1 − VK is a multiple of (1 − t)(1 − t ) for any knot K. The first author observed in [3] that when two links L1 and L2 differ by specific local moves (e.g., crossing changes, ∆-moves, 4-moves, forbidden moves), we can find a fixed polynomial P such that VL1 − VL2 is always a multiple of P . Additional results of this kind were studied in [11] (Cn-moves) and [1] (double-∆-moves). The present paper follows the ideas of [3] to establish divisibility criteria for the Homflypt and Kauffman polynomials. Specifically, we examine the effect of certain local moves on these invariants to show that the difference of Homflypt polynomials for n-component links is always a multiple of a4 − 2a2 + 1 − a2z2, and the difference of Kauffman polynomials for knots is always a multiple of (a2 + 1)(a2 + az + 1). In Section 2 we define our main terms and recall constructions of the Hom- flypt and Kauffman polynomials that are used throughout the paper.
    [Show full text]
  • The Jones Polynomial Through Linear Algebra
    The Jones polynomial through linear algebra Iain Moffatt University of South Alabama Workshop in Knot Theory Waterloo, 24th September 2011 I. Moffatt (South Alabama) UW 2011 1 / 39 What and why What we’ll see The construction of link invariants through R-matrices. (c.f. Reshetikhin-Turaev invariants, quantum invariants) Why this? Can do some serious math using material from Linear Algebra 1. Illustrates how math works in the wild: start with a problem you want to solve; figure out an easier problem that you can solve; build up from this to solve your original problem. See the interplay between algebra, combinatorics and topology! It’s my favourite bit of math! I. Moffatt (South Alabama) UW 2011 2 / 39 What we’re trying to do A knot is a circle, S1, sitting in 3-space R3. A link is a number of disjoint circles in 3-space R3. Knots and links are considered up to isotopy. This means you can “move then round in space, but you can’t cut or glue them”. I. Moffatt (South Alabama) UW 2011 3 / 39 What we’re trying to do A knot is a circle, S1, sitting in 3-space R3. A link is a number of disjoint circles in 3-space R3. Knots and links are considered up to isotopy. This means you can “move then round in space, but you can’t cut or glue them”. The fundamental problem in knot theory is to determine whether or not two links are isotopic. =? =? I. Moffatt (South Alabama) UW 2011 3 / 39 To do this we need knot invariants: F : Links (a set) such (Isotopy) ! that F(L) = F(L0) = L = L0, Aim: construct6 link invariants) 6 using linear algebra.
    [Show full text]