Representations of Knot Groups in Su(2)
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The Homotopy Types of Free Racks and Quandles
The homotopy types of free racks and quandles Tyler Lawson and Markus Szymik June 2021 Abstract. We initiate the homotopical study of racks and quandles, two algebraic structures that govern knot theory and related braided structures in algebra and geometry. We prove analogs of Milnor’s theorem on free groups for these theories and their pointed variants, identifying the homotopy types of the free racks and free quandles on spaces of generators. These results allow us to complete the stable classification of racks and quandles by identifying the ring spectra that model their stable homotopy theories. As an application, we show that the stable homotopy of a knot quandle is, in general, more complicated than what any Wirtinger presentation coming from a diagram predicts. 1 Introduction Racks and quandles form two algebraic theories that are closely related to groups and symmetry. A rack R has a binary operation B such that the left-multiplications s 7! r Bs are automorphism of R for all elements r in R. This means that racks bring their own symmetries. All natural sym- metries, however, are generated by the canonical automorphism r 7! r B r (see [45, Thm. 5.4]). A quandle is a rack for which the canonical automorphism is the identity. Every group defines −1 a quandle via conjugation g B h = ghg , and so does every subset closed under conjugation. The most prominent applications of these algebraic concepts so far are to the classification of knots, first phrased in terms of quandles by Joyce [28, Cor. 16.3] and Matveev [35, Thm. -
Knots: a Handout for Mathcircles
Knots: a handout for mathcircles Mladen Bestvina February 2003 1 Knots Informally, a knot is a knotted loop of string. You can create one easily enough in one of the following ways: • Take an extension cord, tie a knot in it, and then plug one end into the other. • Let your cat play with a ball of yarn for a while. Then find the two ends (good luck!) and tie them together. This is usually a very complicated knot. • Draw a diagram such as those pictured below. Such a diagram is a called a knot diagram or a knot projection. Trefoil and the figure 8 knot 1 The above two knots are the world's simplest knots. At the end of the handout you can see many more pictures of knots (from Robert Scharein's web site). The same picture contains many links as well. A link consists of several loops of string. Some links are so famous that they have names. For 2 2 3 example, 21 is the Hopf link, 51 is the Whitehead link, and 62 are the Bor- romean rings. They have the feature that individual strings (or components in mathematical parlance) are untangled (or unknotted) but you can't pull the strings apart without cutting. A bit of terminology: A crossing is a place where the knot crosses itself. The first number in knot's \name" is the number of crossings. Can you figure out the meaning of the other number(s)? 2 Reidemeister moves There are many knot diagrams representing the same knot. For example, both diagrams below represent the unknot. -
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. -
Dehn Filling of the “Magic” 3-Manifold
communications in analysis and geometry Volume 14, Number 5, 969–1026, 2006 Dehn filling of the “magic” 3-manifold Bruno Martelli and Carlo Petronio We classify all the non-hyperbolic Dehn fillings of the complement of the chain link with three components, conjectured to be the smallest hyperbolic 3-manifold with three cusps. We deduce the classification of all non-hyperbolic Dehn fillings of infinitely many one-cusped and two-cusped hyperbolic manifolds, including most of those with smallest known volume. Among other consequences of this classification, we mention the following: • for every integer n, we can prove that there are infinitely many hyperbolic knots in S3 having exceptional surgeries {n, n +1, n +2,n+3}, with n +1,n+ 2 giving small Seifert manifolds and n, n + 3 giving toroidal manifolds. • we exhibit a two-cusped hyperbolic manifold that contains a pair of inequivalent knots having homeomorphic complements. • we exhibit a chiral 3-manifold containing a pair of inequivalent hyperbolic knots with orientation-preservingly homeomorphic complements. • we give explicit lower bounds for the maximal distance between small Seifert fillings and any other kind of exceptional filling. 0. Introduction We study in this paper the Dehn fillings of the complement N of the chain link with three components in S3, shown in figure 1. The hyperbolic structure of N was first constructed by Thurston in his notes [28], and it was also noted there that the volume of N is particularly small. The relevance of N to three-dimensional topology comes from the fact that by filling N, one gets most of the hyperbolic manifolds known and most of the interesting non-hyperbolic fillings of cusped hyperbolic manifolds. -
Hyperbolic Structures from Link Diagrams
University of Tennessee, Knoxville TRACE: Tennessee Research and Creative Exchange Doctoral Dissertations Graduate School 5-2012 Hyperbolic Structures from Link Diagrams Anastasiia Tsvietkova [email protected] Follow this and additional works at: https://trace.tennessee.edu/utk_graddiss Part of the Geometry and Topology Commons Recommended Citation Tsvietkova, Anastasiia, "Hyperbolic Structures from Link Diagrams. " PhD diss., University of Tennessee, 2012. https://trace.tennessee.edu/utk_graddiss/1361 This Dissertation is brought to you for free and open access by the Graduate School at TRACE: Tennessee Research and Creative Exchange. It has been accepted for inclusion in Doctoral Dissertations by an authorized administrator of TRACE: Tennessee Research and Creative Exchange. For more information, please contact [email protected]. To the Graduate Council: I am submitting herewith a dissertation written by Anastasiia Tsvietkova entitled "Hyperbolic Structures from Link Diagrams." I have examined the final electronic copy of this dissertation for form and content and recommend that it be accepted in partial fulfillment of the equirr ements for the degree of Doctor of Philosophy, with a major in Mathematics. Morwen B. Thistlethwaite, Major Professor We have read this dissertation and recommend its acceptance: Conrad P. Plaut, James Conant, Michael Berry Accepted for the Council: Carolyn R. Hodges Vice Provost and Dean of the Graduate School (Original signatures are on file with official studentecor r ds.) Hyperbolic Structures from Link Diagrams A Dissertation Presented for the Doctor of Philosophy Degree The University of Tennessee, Knoxville Anastasiia Tsvietkova May 2012 Copyright ©2012 by Anastasiia Tsvietkova. All rights reserved. ii Acknowledgements I am deeply thankful to Morwen Thistlethwaite, whose thoughtful guidance and generous advice made this research possible. -
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. -
A New Technique for the Link Slice Problem
Invent. math. 80, 453 465 (1985) /?/ven~lOnSS mathematicae Springer-Verlag 1985 A new technique for the link slice problem Michael H. Freedman* University of California, San Diego, La Jolla, CA 92093, USA The conjectures that the 4-dimensional surgery theorem and 5-dimensional s-cobordism theorem hold without fundamental group restriction in the to- pological category are equivalent to assertions that certain "atomic" links are slice. This has been reported in [CF, F2, F4 and FQ]. The slices must be topologically flat and obey some side conditions. For surgery the condition is: ~a(S 3- ~ slice)--, rq (B 4- slice) must be an epimorphism, i.e., the slice should be "homotopically ribbon"; for the s-cobordism theorem the slice restricted to a certain trivial sublink must be standard. There is some choice about what the atomic links are; the current favorites are built from the simple "Hopf link" by a great deal of Bing doubling and just a little Whitehead doubling. A link typical of those atomic for surgery is illustrated in Fig. 1. (Links atomic for both s-cobordism and surgery are slightly less symmetrical.) There has been considerable interplay between the link theory and the equivalent abstract questions. The link theory has been of two sorts: algebraic invariants of finite links and the limiting geometry of infinitely iterated links. Our object here is to solve a class of free-group surgery problems, specifically, to construct certain slices for the class of links ~ where D(L)eCg if and only if D(L) is an untwisted Whitehead double of a boundary link L. -
UW Math Circle May 26Th, 2016
UW Math Circle May 26th, 2016 We think of a knot (or link) as a piece of string (or multiple pieces of string) that we can stretch and move around in space{ we just aren't allowed to cut the string. We draw a knot on piece of paper by arranging it so that there are two strands at every crossing and by indicating which strand is above the other. We say two knots are equivalent if we can arrange them so that they are the same. 1. Which of these knots do you think are equivalent? Some of these have names: the first is the unkot, the next is the trefoil, and the third is the figure eight knot. 2. Find a way to determine all the knots that have just one crossing when you draw them in the plane. Show that all of them are equivalent to an unknotted circle. The Reidemeister moves are operations we can do on a diagram of a knot to get a diagram of an equivalent knot. In fact, you can get every equivalent digram by doing Reidemeister moves, and by moving the strands around without changing the crossings. Here are the Reidemeister moves (we also include the mirror images of these moves). We want to have a way to distinguish knots and links from one another, so we want to extract some information from a digram that doesn't change when we do Reidemeister moves. Say that a crossing is postively oriented if it you can rotate it so it looks like the left hand picture, and negatively oriented if you can rotate it so it looks like the right hand picture (this depends on the orientation you give the knot/link!) For a link with two components, define the linking number to be the absolute value of the number of positively oriented crossings between the two different components of the link minus the number of negatively oriented crossings between the two different components, #positive crossings − #negative crossings divided by two. -
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. -
Arxiv:1601.05292V3 [Math.GT] 28 Mar 2017
LINK HOMOTOPIC BUT NOT ISOTOPIC BAKUL SATHAYE Abstract. Given an m-component link L in S3 (m ≥ 2), we construct a family of links which are link homotopic, but not link isotopic, to L. Every proper sublink of such a link is link isotopic to the corresponding sublink of L. Moreover, if L is an unlink then there exist links that in addition to the above properties have all Milnor invariants zero. 1. Introduction 3 1 3 An n-component link L in S is a collection of piecewise linear maps (l1; : : : ; ln): S ! S , 1 1 where the images l1(S ); : : : ; ln(S ) are pairwise disjoint. A link with one component is a knot. 3 Two links in S , L1 and L2, are said to be isotopic if there is an orientation preserving homeo- 3 3 morphism h : S ! S such that h(L1) = L2 and h is isotopic to the identity map. The notion of link homotopy was introduced by Milnor in [4]. Two links L and L0 are said 0 to be link homotopic if there exist homotopies hi;t, between the maps li and the maps li so that 1 1 the sets h1;t(S ); : : : ; hn;t(S ) are disjoint for each value of t. In particular, a link is said to be link homotopically trivial if it is link homotopic to the unlink. Notice that this equivalence allows self-crossings, that is, crossing changes involving two strands of the same component. The question that arises now is: how different are these two notions of link equivalence? From the definition it is clear that a link isotopy is a link homotopy as well. -
Lecture 1 Knots and Links, Reidemeister Moves, Alexander–Conway Polynomial
Lecture 1 Knots and links, Reidemeister moves, Alexander–Conway polynomial 1.1. Main definitions A(nonoriented) knot is defined as a closed broken line without self-intersections in Euclidean space R3.A(nonoriented) link is a set of pairwise nonintertsecting closed broken lines without self-intersections in R3; the set may be empty or consist of one element, so that a knot is a particular case of a link. An oriented knot or link is a knot or link supplied with an orientation of its line(s), i.e., with a chosen direction for going around its line(s). Some well known knots and links are shown in the figure below. (The lines representing the knots and links appear to be smooth curves rather than broken lines – this is because the edges of the broken lines and the angle between successive edges are tiny and not distinguished by the human eye :-). (a) (b) (c) (d) (e) (f) (g) Figure 1.1. Examples of knots and links The knot (a) is the right trefoil, (b), the left trefoil (it is the mirror image of (a)), (c) is the eight knot), (d) is the granny knot; 1 2 the link (e) is called the Hopf link, (f) is the Whitehead link, and (g) is known as the Borromeo rings. Two knots (or links) K, K0 are called equivalent) if there exists a finite sequence of ∆-moves taking K to K0, a ∆-move being one of the transformations shown in Figure 1.2; note that such a transformation may be performed only if triangle ABC does not intersect any other part of the line(s). -
Altering the Trefoil Knot
Altering the Trefoil Knot Spencer Shortt Georgia College December 19, 2018 Abstract A mathematical knot K is defined to be a topological imbedding of the circle into the 3-dimensional Euclidean space. Conceptually, a knot can be pictured as knotted shoe lace with both ends glued together. Two knots are said to be equivalent if they can be continuously deformed into each other. Different knots have been tabulated throughout history, and there are many techniques used to show if two knots are equivalent or not. The knot group is defined to be the fundamental group of the knot complement in the 3-dimensional Euclidean space. It is known that equivalent knots have isomorphic knot groups, although the converse is not necessarily true. This research investigates how piercing the space with a line changes the trefoil knot group based on different positions of the line with respect to the knot. This study draws comparisons between the fundamental groups of the altered knot complement space and the complement of the trefoil knot linked with the unknot. 1 Contents 1 Introduction to Concepts in Knot Theory 3 1.1 What is a Knot? . .3 1.2 Rolfsen Knot Tables . .4 1.3 Links . .5 1.4 Knot Composition . .6 1.5 Unknotting Number . .6 2 Relevant Mathematics 7 2.1 Continuity, Homeomorphisms, and Topological Imbeddings . .7 2.2 Paths and Path Homotopy . .7 2.3 Product Operation . .8 2.4 Fundamental Groups . .9 2.5 Induced Homomorphisms . .9 2.6 Deformation Retracts . 10 2.7 Generators . 10 2.8 The Seifert-van Kampen Theorem .