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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). -
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. -
Alternating Knots
ALTERNATING KNOTS WILLIAM W. MENASCO Abstract. This is a short expository article on alternating knots and is to appear in the Concise Encyclopedia of Knot Theory. Introduction Figure 1. P.G. Tait's first knot table where he lists all knot types up to 7 crossings. (From reference [6], courtesy of J. Hoste, M. Thistlethwaite and J. Weeks.) 3 ∼ A knot K ⊂ S is alternating if it has a regular planar diagram DK ⊂ P(= S2) ⊂ S3 such that, when traveling around K , the crossings alternate, over-under- over-under, all the way along K in DK . Figure1 show the first 15 knot types in P. G. Tait's earliest table and each diagram exhibits this alternating pattern. This simple arXiv:1901.00582v1 [math.GT] 3 Jan 2019 definition is very unsatisfying. A knot is alternating if we can draw it as an alternating diagram? There is no mention of any geometric structure. Dissatisfied with this characterization of an alternating knot, Ralph Fox (1913-1973) asked: "What is an alternating knot?" black white white black Figure 2. Going from a black to white region near a crossing. 1 2 WILLIAM W. MENASCO Let's make an initial attempt to address this dissatisfaction by giving a different characterization of an alternating diagram that is immediate from the over-under- over-under characterization. As with all regular planar diagrams of knots in S3, the regions of an alternating diagram can be colored in a checkerboard fashion. Thus, at each crossing (see figure2) we will have \two" white regions and \two" black regions coming together with similarly colored regions being kitty-corner to each other. -
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. -
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 ............................... -
Rotationally Symmetric Rose Links
Rose-Hulman Undergraduate Mathematics Journal Volume 14 Issue 1 Article 3 Rotationally Symmetric Rose Links Amelia Brown Simpson College, [email protected] Follow this and additional works at: https://scholar.rose-hulman.edu/rhumj Recommended Citation Brown, Amelia (2013) "Rotationally Symmetric Rose Links," Rose-Hulman Undergraduate Mathematics Journal: Vol. 14 : Iss. 1 , Article 3. Available at: https://scholar.rose-hulman.edu/rhumj/vol14/iss1/3 Rose- Hulman Undergraduate Mathematics Journal Rotationally Symmetric Rose Links Amelia Browna Volume 14, No. 1, Spring 2013 Sponsored by Rose-Hulman Institute of Technology Department of Mathematics Terre Haute, IN 47803 Email: [email protected] a http://www.rose-hulman.edu/mathjournal Simpson College Rose-Hulman Undergraduate Mathematics Journal Volume 14, No. 1, Spring 2013 Rotationally Symmetric Rose Links Amelia Brown Abstract. This paper is an introduction to rose links and some of their properties. We used a series of invariants to distinguish some rose links that are rotationally symmetric. We were able to distinguish all 3-component rose links and narrow the bounds on possible distinct 4 and 5-component rose links to between 2 and 8, and 2 and 16, respectively. An algorithm for drawing rose links and a table of rose links with up to five components are included. Acknowledgements: The initial cursory observations on rose links were made during the 2011 Dr. Albert H. and Greta A. Bryan Summer Research Program at Simpson College in conjunction with fellow students Michael Comer and Jes Toyne, with Dr. William Schellhorn serving as research advisor. The research presented in this paper, including developing the definitions and related concepts about rose links and applying invariants, was conducted as a part of the author's senior research project at Simpson College, again under the advisement of Dr. -
Knot Polynomials
Knot Polynomials André Schulze & Nasim Rahaman July 24, 2014 1 Why Polynomials? First introduced by James Wadell Alexander II in 1923, knot polynomials have proved themselves by being one of the most efficient ways of classifying knots. In this spirit, one expects two different projections of a knot to have the same knot polynomial; one therefore demands that a good knot polynomial be invariant under the three Reide- meister moves (although this is not always case, as we shall find out). In this report, we present 5 selected knot polynomials: the Bracket, Kauffman X, Jones, Alexander and HOMFLY polynomials. 2 The Bracket Polynomial 2.1 Calculating the Bracket Polynomial The Bracket polynomial makes for a great starting point in constructing knotpoly- nomials. We start with three simple rules, which are then iteratively applied to all crossings in the knot: A direct application of the third rule leads to the following relation for (untangled) unknots: The process of obtaining the Bracket polynomial can be streamlined by evaluating the contribution of a particular sequence of actions in undoing the knot (states) and summing over all such contributions to obtain the net polynomial. 2.2 The Problem with Bracket Polynomials The bracket polynomials can be shown to be invariant under types 2 and 3Reidemeis- ter moves. However by considering type 1 moves, its one major drawback becomes apparent. From: 1 we conclude that that the Bracket polynomial does not remain invariant under type 1 moves. This can be fixed by introducing the writhe of a knot, as we shallsee in the next section. -
HOMFLY Polynomials of Pretzel Knots
HOMFLY Polynomials of Pretzel Knots William Qin∗ Abstract HOMFLY polynomials are one of the major knot invariants being actively studied. They are difficult to compute in the general case but can be far more easily expressed in certain specific cases. In this paper, we examine two particular knots, as well as one more general infinite class of knots. From our calculations, we see some apparent patterns in the polynomials for the knots 935 and 946, and in particular their F -factors. These properties are of a form that seems conducive to finding a general formula for them, which would yield a general formula for the HOMFLY polynomials of the two knots. Motivated by these observations, we demonstrate and conjecture some properties both of the F - factors and HOMFLY polynomials of these knots and of the more general class that contains them, namely pretzel knots with 3 odd parameters. We make the first steps toward a matrix-less general formula for the HOMFLY polynomials of these knots. 1 Introduction HOMFLY polynomials are subcategory of knot polynomial, that generalizes the Jones and Alexander 1 polynomials. In the fundamental representation, they satisfy the skein relation A H(L+) − AH(L−) = −1 (q − q )H(L0). HOMFLY polynomials can be generalized to non-fundamental representations of SU(2), creating the \colored" HOMFLY polynomials. While the normal HOMFLY polynomials are relatively easy to com- pute and have been computed for hundreds of knots in repositories like [1], colored HOMFLY polynomials are difficult to compute in general for any non-(anti)symmetric representations, and computations even in the simplest such representation, namely that corresponding to the smallest L-shaped Young diagram, are difficult to do for more than a few knots. -
Polynomial Invariants and Vassiliev Invariants 1 Introduction
ISSN 1464-8997 (on line) 1464-8989 (printed) 89 eometry & opology onographs G T M Volume 4: Invariants of knots and 3-manifolds (Kyoto 2001) Pages 89–101 Polynomial invariants and Vassiliev invariants Myeong-Ju Jeong Chan-Young Park Abstract We give a criterion to detect whether the derivatives of the HOMFLY polynomial at a point is a Vassiliev invariant or not. In partic- (m,n) ular, for a complex number b we show that the derivative PK (b, 0) = ∂m ∂n ∂am ∂xn PK (a, x) (a,x)=(b,0) of the HOMFLY polynomial of a knot K at (b, 0) is a Vassiliev| invariant if and only if b = 1. Also we analyze the ± space Vn of Vassiliev invariants of degree n for n =1, 2, 3, 4, 5 by using the ¯–operation and the ∗ –operation in [5].≤ These two operations are uni- fied to the ˆ –operation. For each Vassiliev invariant v of degree n,v ˆ is a Vassiliev invariant of degree n and the valuev ˆ(K) of a knot≤ K is a polynomial with multi–variables≤ of degree n and we give some questions on polynomial invariants and the Vassiliev≤ invariants. AMS Classification 57M25 Keywords Knots, Vassiliev invariants, double dating tangles, knot poly- nomials 1 Introduction In 1990, V. A. Vassiliev introduced the concept of a finite type invariant of knots, called Vassiliev invariants [13]. There are some analogies between Vassiliev invariants and polynomials. For example, in 1996 D. Bar–Natan showed that when a Vassiliev invariant of degree m is evaluated on a knot diagram having n crossings, the result is approximately bounded by a constant times of nm [2] and S. -
An Introduction to Knot Theory
An Introduction to Knot Theory Matt Skerritt (c9903032) June 27, 2003 1 Introduction A knot, mathematically speaking, is a closed curve sitting in three dimensional space that does not intersect itself. Intuitively if we were to take a piece of string, cord, or the like, tie a knot in it and then glue the loose ends together, we would have a knot. It should be impossible to untangle the knot without cutting the string somewhere. The use of the word `should' here is quite deliberate, however. It is possible, if we have not tangled the string very well, that we will be able to untangle the mess we created and end up with just a circle of string. Of course, this circle of string still ¯ts the de¯nition of a closed curve sitting in three dimensional space and so is still a knot, but it's not very interesting. We call such a knot the trivial knot or the unknot. Knots come in many shapes and sizes from small and simple like the unknot through to large and tangled and messy, and beyond (and everything in between). The biggest questions to a knot theorist are \are these two knots the same or di®erent" or even more importantly \is there an easy way to tell if two knots are the same or di®erent". This is the heart of knot theory. Merely looking at two tangled messes is almost never su±cient to tell them apart, at least not in any interesting cases. Consider the following four images for example. -
Grid Homology for Knots and Links
Grid Homology for Knots and Links Peter S. Ozsvath, Andras I. Stipsicz, and Zoltan Szabo This is a preliminary version of the book Grid Homology for Knots and Links published by the American Mathematical Society (AMS). This preliminary version is made available with the permission of the AMS and may not be changed, edited, or reposted at any other website without explicit written permission from the author and the AMS. Contents Chapter 1. Introduction 1 1.1. Grid homology and the Alexander polynomial 1 1.2. Applications of grid homology 3 1.3. Knot Floer homology 5 1.4. Comparison with Khovanov homology 7 1.5. On notational conventions 7 1.6. Necessary background 9 1.7. The organization of this book 9 1.8. Acknowledgements 11 Chapter 2. Knots and links in S3 13 2.1. Knots and links 13 2.2. Seifert surfaces 20 2.3. Signature and the unknotting number 21 2.4. The Alexander polynomial 25 2.5. Further constructions of knots and links 30 2.6. The slice genus 32 2.7. The Goeritz matrix and the signature 37 Chapter 3. Grid diagrams 43 3.1. Planar grid diagrams 43 3.2. Toroidal grid diagrams 49 3.3. Grids and the Alexander polynomial 51 3.4. Grid diagrams and Seifert surfaces 56 3.5. Grid diagrams and the fundamental group 63 Chapter 4. Grid homology 65 4.1. Grid states 65 4.2. Rectangles connecting grid states 66 4.3. The bigrading on grid states 68 4.4. The simplest version of grid homology 72 4.5. -