1. What Is Knot Theory? Why Is It in Mathematics?
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The Borromean Rings: a Video About the New IMU Logo
The Borromean Rings: A Video about the New IMU Logo Charles Gunn and John M. Sullivan∗ Technische Universitat¨ Berlin Institut fur¨ Mathematik, MA 3–2 Str. des 17. Juni 136 10623 Berlin, Germany Email: {gunn,sullivan}@math.tu-berlin.de Abstract This paper describes our video The Borromean Rings: A new logo for the IMU, which was premiered at the opening ceremony of the last International Congress. The video explains some of the mathematics behind the logo of the In- ternational Mathematical Union, which is based on the tight configuration of the Borromean rings. This configuration has pyritohedral symmetry, so the video includes an exploration of this interesting symmetry group. Figure 1: The IMU logo depicts the tight config- Figure 2: A typical diagram for the Borromean uration of the Borromean rings. Its symmetry is rings uses three round circles, with alternating pyritohedral, as defined in Section 3. crossings. In the upper corners are diagrams for two other three-component Brunnian links. 1 The IMU Logo and the Borromean Rings In 2004, the International Mathematical Union (IMU), which had never had a logo, announced a competition to design one. The winning entry, shown in Figure 1, was designed by one of us (Sullivan) with help from Nancy Wrinkle. It depicts the Borromean rings, not in the usual diagram (Figure 2) but instead in their tight configuration, the shape they have when tied tight in thick rope. This IMU logo was unveiled at the opening ceremony of the International Congress of Mathematicians (ICM 2006) in Madrid. We were invited to produce a short video [10] about some of the mathematics behind the logo; it was shown at the opening and closing ceremonies, and can be viewed at www.isama.org/jms/Videos/imu/. -
A Knot-Vice's Guide to Untangling Knot Theory, Undergraduate
A Knot-vice’s Guide to Untangling Knot Theory Rebecca Hardenbrook Department of Mathematics University of Utah Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 1 / 26 What is Not a Knot? Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 2 / 26 What is a Knot? 2 A knot is an embedding of the circle in the Euclidean plane (R ). 3 Also defined as a closed, non-self-intersecting curve in R . 2 Represented by knot projections in R . Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 3 / 26 Why Knots? Late nineteenth century chemists and physicists believed that a substance known as aether existed throughout all of space. Could knots represent the elements? Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 4 / 26 Why Knots? Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 5 / 26 Why Knots? Unfortunately, no. Nevertheless, mathematicians continued to study knots! Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 6 / 26 Current Applications Natural knotting in DNA molecules (1980s). Credit: K. Kimura et al. (1999) Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 7 / 26 Current Applications Chemical synthesis of knotted molecules – Dietrich-Buchecker and Sauvage (1988). Credit: J. Guo et al. (2010) Rebecca Hardenbrook A Knot-vice’s Guide to Untangling Knot Theory 8 / 26 Current Applications Use of lattice models, e.g. the Ising model (1925), and planar projection of knots to find a knot invariant via statistical mechanics. Credit: D. Chicherin, V.P. -
Notes on the Self-Linking Number
NOTES ON THE SELF-LINKING NUMBER ALBERTO S. CATTANEO The aim of this note is to review the results of [4, 8, 9] in view of integrals over configuration spaces and also to discuss a generalization to other 3-manifolds. Recall that the linking number of two non-intersecting curves in R3 can be expressed as the integral (Gauss formula) of a 2-form on the Cartesian product of the curves. It also makes sense to integrate over the product of an embedded curve with itself and define its self-linking number this way. This is not an invariant as it changes continuously with deformations of the embedding; in addition, it has a jump when- ever a crossing is switched. There exists another function, the integrated torsion, which has op- posite variation under continuous deformations but is defined on the whole space of immersions (and consequently has no discontinuities at a crossing change), but depends on a choice of framing. The sum of the self-linking number and the integrated torsion is therefore an invariant of embedded curves with framings and turns out simply to be the linking number between the given embedding and its small displacement by the framing. This also allows one to compute the jump at a crossing change. The main application is that the self-linking number or the integrated torsion may be added to the integral expressions of [3] to make them into knot invariants. We also discuss on the geometrical meaning of the integrated torsion. 1. The trivial case Let us start recalling the case of embeddings and immersions in R3. -
Gauss' Linking Number Revisited
October 18, 2011 9:17 WSPC/S0218-2165 134-JKTR S0218216511009261 Journal of Knot Theory and Its Ramifications Vol. 20, No. 10 (2011) 1325–1343 c World Scientific Publishing Company DOI: 10.1142/S0218216511009261 GAUSS’ LINKING NUMBER REVISITED RENZO L. RICCA∗ Department of Mathematics and Applications, University of Milano-Bicocca, Via Cozzi 53, 20125 Milano, Italy [email protected] BERNARDO NIPOTI Department of Mathematics “F. Casorati”, University of Pavia, Via Ferrata 1, 27100 Pavia, Italy Accepted 6 August 2010 ABSTRACT In this paper we provide a mathematical reconstruction of what might have been Gauss’ own derivation of the linking number of 1833, providing also an alternative, explicit proof of its modern interpretation in terms of degree, signed crossings and inter- section number. The reconstruction presented here is entirely based on an accurate study of Gauss’ own work on terrestrial magnetism. A brief discussion of a possibly indepen- dent derivation made by Maxwell in 1867 completes this reconstruction. Since the linking number interpretations in terms of degree, signed crossings and intersection index play such an important role in modern mathematical physics, we offer a direct proof of their equivalence. Explicit examples of its interpretation in terms of oriented area are also provided. Keywords: Linking number; potential; degree; signed crossings; intersection number; oriented area. Mathematics Subject Classification 2010: 57M25, 57M27, 78A25 1. Introduction The concept of linking number was introduced by Gauss in a brief note on his diary in 1833 (see Sec. 2 below), but no proof was given, neither of its derivation, nor of its topological meaning. Its derivation remained indeed a mystery. -
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. -
Computing the Writhing Number of a Polygonal Knot
Computing the Writhing Number of a Polygonal Knot ¡ ¡£¢ ¡ Pankaj K. Agarwal Herbert Edelsbrunner Yusu Wang Abstract Here the linking number, , is half the signed number of crossings between the two boundary curves of the ribbon, The writhing number measures the global geometry of a and the twisting number, , is half the average signed num- closed space curve or knot. We show that this measure is ber of local crossing between the two curves. The non-local related to the average winding number of its Gauss map. Us- crossings between the two curves correspond to crossings ing this relationship, we give an algorithm for computing the of the ribbon axis, which are counted by the writhing num- ¤ writhing number for a polygonal knot with edges in time ber, . A small subset of the mathematical literature on ¥§¦ ¨ roughly proportional to ¤ . We also implement a different, the subject can be found in [3, 20]. Besides the mathemat- simple algorithm and provide experimental evidence for its ical interest, the White Formula and the writhing number practical efficiency. have received attention both in physics and in biochemistry [17, 23, 26, 30]. For example, they are relevant in under- standing various geometric conformations we find for circu- 1 Introduction lar DNA in solution, as illustrated in Figure 1 taken from [7]. By representing DNA as a ribbon, the writhing number of its The writhing number is an attempt to capture the physical phenomenon that a cord tends to form loops and coils when it is twisted. We model the cord by a knot, which we define to be an oriented closed curve in three-dimensional space. -
Splitting Numbers of Links
Splitting numbers of links Jae Choon Cha, Stefan Friedl, and Mark Powell Department of Mathematics, POSTECH, Pohang 790{784, Republic of Korea, and School of Mathematics, Korea Institute for Advanced Study, Seoul 130{722, Republic of Korea E-mail address: [email protected] Mathematisches Institut, Universit¨atzu K¨oln,50931 K¨oln,Germany E-mail address: [email protected] D´epartement de Math´ematiques,Universit´edu Qu´ebec `aMontr´eal,Montr´eal,QC, Canada E-mail address: [email protected] Abstract. The splitting number of a link is the minimal number of crossing changes between different components required, on any diagram, to convert it to a split link. We introduce new techniques to compute the splitting number, involving covering links and Alexander invariants. As an application, we completely determine the splitting numbers of links with 9 or fewer crossings. Also, with these techniques, we either reprove or improve upon the lower bounds for splitting numbers of links computed by J. Batson and C. Seed using Khovanov homology. 1. Introduction Any link in S3 can be converted to the split union of its component knots by a sequence of crossing changes between different components. Following J. Batson and C. Seed [BS13], we define the splitting number of a link L, denoted by sp(L), as the minimal number of crossing changes in such a sequence. We present two new techniques for obtaining lower bounds for the splitting number. The first approach uses covering links, and the second method arises from the multivariable Alexander polynomial of a link. Our general covering link theorem is stated as Theorem 3.2. -
Matrix Integrals and Knot Theory 1
Matrix Integrals and Knot Theory 1 Matrix Integrals and Knot Theory Paul Zinn-Justin et Jean-Bernard Zuber math-ph/9904019 (Discr. Math. 2001) math-ph/0002020 (J.Kn.Th.Ramif. 2000) P. Z.-J. (math-ph/9910010, math-ph/0106005) J. L. Jacobsen & P. Z.-J. (math-ph/0102015, math-ph/0104009). math-ph/0303049 (J.Kn.Th.Ramif. 2004) G. Schaeffer and P. Z.-J., math-ph/0304034 P. Z.-J. and J.-B. Z., review article in preparation Carghjese, March 25, 2009 Matrix Integrals and Knot Theory 2 Courtesy of “U Rasaghiu” Matrix Integrals and Knot Theory 3 Main idea : Use combinatorial tools of Quantum Field Theory in Knot Theory Plan I Knot Theory : a few definitions II Matrix integrals and Link diagrams 1 2 4 dMeNtr( 2 M + gM ) N N matrices, N ∞ − × → RemovalsR of redundancies reproduces recent results of Sundberg & Thistlethwaite (1998) ⇒ based on Tutte (1963) III Virtual knots and links : counting and invariants Matrix Integrals and Knot Theory 4 Basics of Knot Theory a knot , links and tangles Equivalence up to isotopy Problem : Count topologically inequivalent knots, links and tangles Represent knots etc by their planar projection with minimal number of over/under-crossings Theorem Two projections represent the same knot/link iff they may be transformed into one another by a sequence of Reidemeister moves : ; ; Matrix Integrals and Knot Theory 5 Avoid redundancies by keeping only prime links (i.e. which cannot be factored) Consider the subclass of alternating knots, links and tangles, in which one meets alternatingly over- and under-crossings. For n 8 (resp. -
Comultiplication in Link Floer Homologyand Transversely Nonsimple Links
Algebraic & Geometric Topology 10 (2010) 1417–1436 1417 Comultiplication in link Floer homology and transversely nonsimple links JOHN ABALDWIN For a word w in the braid group Bn , we denote by Tw the corresponding transverse 3 braid in .R ; rot/. We exhibit, for any two g; h Bn , a “comultiplication” map on 2 link Floer homology ˆ HFL.m.Thg// HFL.m.Tg#Th// which sends .Thg/ z W ! z to .z Tg#Th/. We use this comultiplication map to generate infinitely many new examples of prime topological link types which are not transversely simple. 57M27, 57R17 e e 1 Introduction Transverse links feature prominently in the study of contact 3–manifolds. They arise very naturally – for instance, as binding components of open book decompositions – and can be used to discern important properties of the contact structures in which they sit (see Baker, Etnyre and Van Horn-Morris [1, Theorem 1.15] for a recent example). Yet, 3 transverse links, even in the standard tight contact structure std on R , are notoriously difficult to classify up to transverse isotopy. A transverse link T comes equipped with two “classical” invariants which are preserved under transverse isotopy: its topological link type and its self-linking number sl.T /. For transverse links with more than one component, it makes sense to refine the notion of self-linking number as follows. Let T and T 0 be two transverse representatives of some l –component topological link type, and suppose there are labelings T T1 T D [ [ l and T T T of the components of T and T such that 0 D 10 [ [ l0 0 (1) there is a topological isotopy sending T to T 0 which sends Ti to Ti0 for each i , (2) sl.S/ sl.S / for any sublinks S Tn Tn and S T T . -
Invariants of Knots and 3-Manifolds: Survey on 3-Manifolds
Invariants of knots and 3-manifolds: Survey on 3-manifolds Wolfgang Lück Bonn Germany email [email protected] http://131.220.77.52/lueck/ Bonn, 10. & 12. April 2018 Wolfgang Lück (MI, Bonn) Survey on 3-manifolds Bonn, 10. & 12. April 2018 1 / 44 Tentative plan of the course title date lecturer Introduction to 3-manifolds I & II April, 10 & 12 Lück Cobordism theory and the April, 17 Lück s-cobordism theorem Introduction to Surgery theory April 19 Lück L2-Betti numbers April, 24 & 26 Lück Introduction to Knots and Links May 3 Teichner Knot invariants I May, 8 Teichner Knot invariants II May,15 Teichner Introduction to knot concordance I May, 17 Teichner Whitehead torsion and L2-torsion I May 29th Lück L2-signatures I June 5 Teichner tba June, 7 tba Wolfgang Lück (MI, Bonn) Survey on 3-manifolds Bonn, 10. & 12. April 2018 2 / 44 title date lecturer Whitehead torsion and L2-torsion II June, 12 Lück L2-invariants und 3-manifolds I June, 14 Lück L2-invariants und 3-manifolds II June, 19 Lück L2-signatures II June, 21 Teichner L2-signatures as knot concordance June, 26 & 28 Teichner invariants I & II tba July, 3 tba Further aspects of L2-invariants July 10 Lück tba July 12 Teichner Open problems in low-dimensional July 17 & 19 Teichner topology No talks on May 1, May 10, May 22, May 24, May 31, July 5. On demand there can be a discussion session at the end of the Thursday lecture. Wolfgang Lück (MI, Bonn) Survey on 3-manifolds Bonn, 10. -
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 ............................... -
Knot and Link Tricolorability Danielle Brushaber Mckenzie Hennen Molly Petersen Faculty Mentor: Carolyn Otto University of Wisconsin-Eau Claire
Knot and Link Tricolorability Danielle Brushaber McKenzie Hennen Molly Petersen Faculty Mentor: Carolyn Otto University of Wisconsin-Eau Claire Problem & Importance Colorability Tables of Characteristics Theorem: For WH 51 with n twists, WH 5 is tricolorable when Knot Theory, a field of Topology, can be used to model Original Knot The unknot is not tricolorable, therefore anything that is tri- 1 colorable cannot be the unknot. The prime factors of the and understand how enzymes (called topoisomerases) work n = 3k + 1 where k ∈ N ∪ {0}. in DNA processes to untangle or repair strands of DNA. In a determinant of the knot or link provides the colorability. For human cell nucleus, the DNA is linear, so the knots can slip off example, if a knot’s determinant is 21, it is 3-colorable (tricol- orable), and 7-colorable. This is known by the theorem that Proof the end, and it is difficult to recognize what the enzymes do. Consider WH 5 where n is the number of the determinant of a knot is 0 mod n if and only if the knot 1 However, the DNA in mitochon- full positive twists. n is n-colorable. dria is circular, along with prokary- Link Colorability Det(L) Unknot/Link (n = 1...n = k) otic cells (bacteria), so the enzyme L Number Theorem: If det(L) = 0, then L is WOLOG, let WH 51 be colored in this way, processes are more noticeable in 3 3 3 1 n 1 n-colorable for all n. excluding coloring the twist component. knots in this type of DNA.