ON KAUFFMAN POLYNOMIALS of LINKS § 1. Introduction
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
THE JONES SLOPES of a KNOT Contents 1. Introduction 1 1.1. The
THE JONES SLOPES OF A KNOT STAVROS GAROUFALIDIS Abstract. The paper introduces the Slope Conjecture which relates the degree of the Jones polynomial of a knot and its parallels with the slopes of incompressible surfaces in the knot complement. More precisely, we introduce two knot invariants, the Jones slopes (a finite set of rational numbers) and the Jones period (a natural number) of a knot in 3-space. We formulate a number of conjectures for these invariants and verify them by explicit computations for the class of alternating knots, the knots with at most 9 crossings, the torus knots and the (−2, 3,n) pretzel knots. Contents 1. Introduction 1 1.1. The degree of the Jones polynomial and incompressible surfaces 1 1.2. The degree of the colored Jones function is a quadratic quasi-polynomial 3 1.3. q-holonomic functions and quadratic quasi-polynomials 3 1.4. The Jones slopes and the Jones period of a knot 4 1.5. The symmetrized Jones slopes and the signature of a knot 5 1.6. Plan of the proof 7 2. Future directions 7 3. The Jones slopes and the Jones period of an alternating knot 8 4. Computing the Jones slopes and the Jones period of a knot 10 4.1. Some lemmas on quasi-polynomials 10 4.2. Computing the colored Jones function of a knot 11 4.3. Guessing the colored Jones function of a knot 11 4.4. A summary of non-alternating knots 12 4.5. The 8-crossing non-alternating knots 13 4.6. -
Arxiv:1501.00726V2 [Math.GT] 19 Sep 2016 3 2 for Each N, Ln Is Assembled from a Tangle S in B , N Copies of a Tangle T in S × I, and the Mirror Image S of S
HIDDEN SYMMETRIES VIA HIDDEN EXTENSIONS ERIC CHESEBRO AND JASON DEBLOIS Abstract. This paper introduces a new approach to finding knots and links with hidden symmetries using \hidden extensions", a class of hidden symme- tries defined here. We exhibit a family of tangle complements in the ball whose boundaries have symmetries with hidden extensions, then we further extend these to hidden symmetries of some hyperbolic link complements. A hidden symmetry of a manifold M is a homeomorphism of finite-degree covers of M that does not descend to an automorphism of M. By deep work of Mar- gulis, hidden symmetries characterize the arithmetic manifolds among all locally symmetric ones: a locally symmetric manifold is arithmetic if and only if it has infinitely many \non-equivalent" hidden symmetries (see [13, Ch. 6]; cf. [9]). Among hyperbolic knot complements in S3 only that of the figure-eight is arith- metic [10], and the only other knot complements known to possess hidden sym- metries are the two \dodecahedral knots" constructed by Aitchison{Rubinstein [1]. Whether there exist others has been an open question for over two decades [9, Question 1]. Its answer has important consequences for commensurability classes of knot complements, see [11] and [2]. The partial answers that we know are all negative. Aside from the figure-eight, there are no knots with hidden symmetries with at most fifteen crossings [6] and no two-bridge knots with hidden symmetries [11]. Macasieb{Mattman showed that no hyperbolic (−2; 3; n) pretzel knot, n 2 Z, has hidden symmetries [8]. Hoffman showed the dodecahedral knots are commensurable with no others [7]. -
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). -
MUTATION of KNOTS Figure 1 Figure 2
proceedings of the american mathematical society Volume 105. Number 1, January 1989 MUTATION OF KNOTS C. KEARTON (Communicated by Haynes R. Miller) Abstract. In general, mutation does not preserve the Alexander module or the concordance class of a knot. For a discussion of mutation of classical links, and the invariants which it is known to preserve, the reader is referred to [LM, APR, MT]. Suffice it here to say that mutation of knots preserves the polynomials of Alexander, Jones, and Homfly, and also the signature. Mutation of an oriented link k can be described as follows. Take a diagram of k and a tangle T with two outputs and two inputs, as in Figure 1. Figure 1 Figure 2 Rotate the tangle about the east-west axis to obtain Figure 2, or about the north-south axis to obtain Figure 3, or about the axis perpendicular to the paper to obtain Figure 4. Keep or reverse all the orientations of T as dictated by the rest of k . Each of the links so obtained is a mutant of k. The reverse k' of a link k is obtained by reversing the orientation of each component of k. Let us adopt the convention that a knot is a link of one component, and that k + I denotes the connected sum of two knots k and /. Lemma. For any knot k, the knot k + k' is a mutant of k + k. Received by the editors September 16, 1987. 1980 Mathematics Subject Classification (1985 Revision). Primary 57M25. ©1989 American Mathematical Society 0002-9939/89 $1.00 + $.25 per page 206 License or copyright restrictions may apply to redistribution; see https://www.ams.org/journal-terms-of-use MUTATION OF KNOTS 207 Figure 3 Figure 4 Proof. -
Mutations of Links in Genus 2 Handlebodies
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 127, Number 1, January 1999, Pages 309–314 S0002-9939(99)04871-6 MUTATIONS OF LINKS IN GENUS 2 HANDLEBODIES D. COOPER AND W. B. R. LICKORISH (Communicated by Ronald A. Fintushel) Abstract. Ashortproofisgiventoshowthatalinkinthe3-sphereandany link related to it by genus 2 mutation have the same Alexander polynomial. This verifies a deduction from the solution to the Melvin-Morton conjecture. The proof here extends to show that the link signatures are likewise the same and that these results extend to links in a homology 3-sphere. 1. Introduction Suppose L is an oriented link in a genus 2 handlebody H that is contained, in some arbitrary (complicated) way, in S3.Let⇢ be the involution of H depicted abstractly in Figure 1 as a ⇡-rotation about the axis shown. The pair of links L and ⇢L is said to be related by a genus 2 mutation. The first purpose of this note is to prove, by means of long established techniques of classical knot theory, that L and ⇢L always have the same Alexander polynomial. As described briefly below, this actual result for knots can also be deduced from the recent solution to aconjecture,ofP.M.MelvinandH.R.Morton,thatposedaproblemintherealm of Vassiliev invariants. It is impressive that this simple result, readily expressible in the language of the classical knot theory that predates the Jones polynomial, should have emerged from the technicalities of Vassiliev invariants. It may be the first such new result to arrive in this way. However, the method of proof used here depends only on elementary homology theory and so the result extends at once to give a new result for links in a homology 3-sphere. -
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. -
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. -
Kontsevich's Integral for the Kauffman Polynomial Thang Tu Quoc Le and Jun Murakami
T.T.Q. Le and J. Murakami Nagoya Math. J. Vol. 142 (1996), 39-65 KONTSEVICH'S INTEGRAL FOR THE KAUFFMAN POLYNOMIAL THANG TU QUOC LE AND JUN MURAKAMI 1. Introduction Kontsevich's integral is a knot invariant which contains in itself all knot in- variants of finite type, or Vassiliev's invariants. The value of this integral lies in an algebra d0, spanned by chord diagrams, subject to relations corresponding to the flatness of the Knizhnik-Zamolodchikov equation, or the so called infinitesimal pure braid relations [11]. For a Lie algebra g with a bilinear invariant form and a representation p : g —» End(V) one can associate a linear mapping WQtβ from dQ to C[[Λ]], called the weight system of g, t, p. Here t is the invariant element in g ® g corresponding to the bilinear form, i.e. t = Σa ea ® ea where iea} is an orthonormal basis of g with respect to the bilinear form. Combining with Kontsevich's integral we get a knot invariant with values in C [[/*]]. The coefficient of h is a Vassiliev invariant of degree n. On the other hand, for a simple Lie algebra g, t ^ g ® g as above, and a fi- nite dimensional irreducible representation p, there is another knot invariant, con- structed from the quantum i?-matrix corresponding to g, t, p. Here i?-matrix is the image of the universal quantum i?-matrix lying in °Uq(φ ^^(g) through the representation p. The construction is given, for example, in [17, 18, 20]. The in- variant is a Laurent polynomial in q, by putting q — exp(h) we get a formal series in h. -
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. -
The Conway Knot Is Not Slice
THE CONWAY KNOT IS NOT SLICE LISA PICCIRILLO Abstract. A knot is said to be slice if it bounds a smooth properly embedded disk in B4. We demonstrate that the Conway knot, 11n34 in the Rolfsen tables, is not slice. This com- pletes the classification of slice knots under 13 crossings, and gives the first example of a non-slice knot which is both topologically slice and a positive mutant of a slice knot. 1. Introduction The classical study of knots in S3 is 3-dimensional; a knot is defined to be trivial if it bounds an embedded disk in S3. Concordance, first defined by Fox in [Fox62], is a 4-dimensional extension; a knot in S3 is trivial in concordance if it bounds an embedded disk in B4. In four dimensions one has to take care about what sort of disks are permitted. A knot is slice if it bounds a smoothly embedded disk in B4, and topologically slice if it bounds a locally flat disk in B4. There are many slice knots which are not the unknot, and many topologically slice knots which are not slice. It is natural to ask how characteristics of 3-dimensional knotting interact with concordance and questions of this sort are prevalent in the literature. Modifying a knot by positive mutation is particularly difficult to detect in concordance; we define positive mutation now. A Conway sphere for an oriented knot K is an embedded S2 in S3 that meets the knot 3 transversely in four points. The Conway sphere splits S into two 3-balls, B1 and B2, and ∗ K into two tangles KB1 and KB2 . -
New Skein Invariants of Links
NEW SKEIN INVARIANTS OF LINKS LOUIS H. KAUFFMAN AND SOFIA LAMBROPOULOU Abstract. We introduce new skein invariants of links based on a procedure where we first apply the skein relation only to crossings of distinct components, so as to produce collections of unlinked knots. We then evaluate the resulting knots using a given invariant. A skein invariant can be computed on each link solely by the use of skein relations and a set of initial conditions. The new procedure, remarkably, leads to generalizations of the known skein invariants. We make skein invariants of classical links, H[R], K[Q] and D[T ], based on the invariants of knots, R, Q and T , denoting the regular isotopy version of the Homflypt polynomial, the Kauffman polynomial and the Dubrovnik polynomial. We provide skein theoretic proofs of the well- definedness of these invariants. These invariants are also reformulated into summations of the generating invariants (R, Q, T ) on sublinks of a given link L, obtained by partitioning L into collections of sublinks. Contents Introduction1 1. Previous work9 2. Skein theory for the generalized invariants 11 3. Closed combinatorial formulae for the generalized invariants 28 4. Conclusions 38 5. Discussing mathematical directions and applications 38 References 40 Introduction Skein theory was introduced by John Horton Conway in his remarkable paper [16] and in numerous conversations and lectures that Conway gave in the wake of publishing this paper. He not only discovered a remarkable normalized recursive method to compute the classical Alexander polynomial, but he formulated a generalized invariant of knots and links that is called skein theory. -
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.