Alternating Knots More About Polynomial Invariants
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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). -
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. -
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. -
Bracket Calculations -- Pdf Download
Knot Theory Notes - Detecting Links With The Jones Polynonmial by Louis H. Kau®man 1 Some Elementary Calculations The formula for the bracket model of the Jones polynomial can be indicated as follows: The letter chi, Â, denotes a crossing in a link diagram. The barred letter denotes the mirror image of this ¯rst crossing. A crossing in a diagram for the knot or link is expanded into two possible states by either smoothing (reconnecting) the crossing horizontally, , or 2 2 vertically ><. Any closed loop (without crossings) in the plane has value ± = A ³A¡ : ¡ ¡ 1  = A + A¡ >< ³ 1  = A¡ + A >< : ³ One useful consequence of these formulas is the following switching formula 1 2 2 A A¡  = (A A¡ ) : ¡ ¡ ³ Note that in these conventions the A-smoothing of  is ; while the A-smoothing of  is >< : Properly interpreted, the switching formula abo³ve says that you can switch a crossing and smooth it either way and obtain a three diagram relation. This is useful since some computations will simplify quite quickly with the proper choices of switching and smoothing. Remember that it is necessary to keep track of the diagrams up to regular isotopy (the equivalence relation generated by the second and third Reidemeister moves). Here is an example. View Figure 1. K U U' Figure 1 { Trefoil and Two Relatives You see in Figure 1, a trefoil diagram K, an unknot diagram U and another unknot diagram U 0: Applying the switching formula, we have 1 2 2 A¡ K AU = (A¡ A )U 0 ¡ ¡ 3 3 2 6 and U = A and U 0 = ( A¡ ) = A¡ : Thus ¡ ¡ 1 3 2 2 6 A¡ K A( A ) = (A¡ A )A¡ : ¡ ¡ ¡ Hence 1 4 8 4 A¡ K = A + A¡ A¡ : ¡ ¡ Thus 5 3 7 K = A A¡ + A¡ : ¡ ¡ This is the bracket polynomial of the trefoil diagram K: We have used to same symbol for the diagram and for its polynomial. -
The Kauffman Bracket and Genus of Alternating Links
California State University, San Bernardino CSUSB ScholarWorks Electronic Theses, Projects, and Dissertations Office of aduateGr Studies 6-2016 The Kauffman Bracket and Genus of Alternating Links Bryan M. Nguyen Follow this and additional works at: https://scholarworks.lib.csusb.edu/etd Part of the Other Mathematics Commons Recommended Citation Nguyen, Bryan M., "The Kauffman Bracket and Genus of Alternating Links" (2016). Electronic Theses, Projects, and Dissertations. 360. https://scholarworks.lib.csusb.edu/etd/360 This Thesis is brought to you for free and open access by the Office of aduateGr Studies at CSUSB ScholarWorks. It has been accepted for inclusion in Electronic Theses, Projects, and Dissertations by an authorized administrator of CSUSB ScholarWorks. For more information, please contact [email protected]. The Kauffman Bracket and Genus of Alternating Links A Thesis Presented to the Faculty of California State University, San Bernardino In Partial Fulfillment of the Requirements for the Degree Master of Arts in Mathematics by Bryan Minh Nhut Nguyen June 2016 The Kauffman Bracket and Genus of Alternating Links A Thesis Presented to the Faculty of California State University, San Bernardino by Bryan Minh Nhut Nguyen June 2016 Approved by: Dr. Rolland Trapp, Committee Chair Date Dr. Gary Griffing, Committee Member Dr. Jeremy Aikin, Committee Member Dr. Charles Stanton, Chair, Dr. Corey Dunn Department of Mathematics Graduate Coordinator, Department of Mathematics iii Abstract Giving a knot, there are three rules to help us finding the Kauffman bracket polynomial. Choosing knot's orientation, then applying the Seifert algorithm to find the Euler characteristic and genus of its surface. Finally finding the relationship of the Kauffman bracket polynomial and the genus of the alternating links is the main goal of this paper. -
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. -
Jones Polynomial of Knots
KNOTS AND THE JONES POLYNOMIAL MATH 180, SPRING 2020 Your task as a group, is to research the topics and questions below, write up clear notes as a group explaining these topics and the answers to the questions, and then make a video presenting your findings. Your video and notes will be presented to the class to teach them your findings. Make sure that in your notes and video you give examples and intuition, along with formal definitions, theorems, proofs, or calculations. Make sure that you point out what the is most important take away message, and what aspects may be tricky or confusing to understand at first. You will need to work together as a group. You should all work on Problem 1. Each member of the group must be responsible for one full example from problem 2. Then you can split up problem 3-7 as you wish. 1. Resources The primary resource for this project is The Knot Book by Colin Adams, Chapter 6.1 (page 147-155). An Introduction to Knot Theory by Raymond Lickorish Chapter 3, could also be helpful. You may also look at other resources online about knot theory and the Jones polynomial. Make sure to cite the sources you use. If you find it useful and you are comfortable, you can try to write some code to help you with computations. 2. Topics and Questions As you research, you may find more examples, definitions, and questions, which you defi- nitely should feel free to include in your notes and/or video, but make sure you at least go through the following discussion and questions. -
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. -
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. -
A New Symmetry of the Colored Alexander Polynomial
ITEP/TH-04/20 IITP/TH-04/20 MIPT/TH-04/20 A new symmetry of the colored Alexander polynomial V. Mishnyakov a,c,d,∗ A. Sleptsova,b,c,† N. Tselousova,c‡ a Institute for Theoretical and Experimental Physics, Moscow 117218, Russia b Institute for Information Transmission Problems, Moscow 127994, Russia c Moscow Institute of Physics and Technology, Dolgoprudny 141701, Russia d Institute for Theoretical and Mathematical Physics, Moscow State University, Moscow 119991, Russia Abstract We present a new conjectural symmetry of the colored Alexander polynomial, that is the specializa- tion of the quantum slN invariant widely known as the colored HOMFLY-PT polynomial. We provide arguments in support of the existence of the symmetry by studying the loop expansion and the character expansion of the colored HOMFLY-PT polynomial. We study the constraints this symmetry imposes on the group theoretic structure of the loop expansion and provide solutions to those constraints. The symmetry is a powerful tool for research on polynomial knot invariants and in the end we suggest several possible applications of the symmetry. 1 Introduction The colored HOMFLY polynomial is a topological link invariant. It attracts a lot of attention because it is connected to various topics in theoretical and mathematical physics: quantum field theories [5, 6, 7], quantum groups [11, 12, 8], conformal field theories [9], topological strings [10]. Whenever an explicit calculation of a class of HOMFLY invariants is derived it causes advancements in these areas. However, the computations be- come extremely difficult as the representation gets larger. At present moment explicit expressions are available only for several classes of knots and representations, including symmetric and anti-symmetric representations.