Splitting Numbers of Links
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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/. -
Jones Polynomial for Graphs of Twist Knots
Available at Applications and Applied http://pvamu.edu/aam Mathematics: Appl. Appl. Math. An International Journal ISSN: 1932-9466 (AAM) Vol. 14, Issue 2 (December 2019), pp. 1269 – 1278 Jones Polynomial for Graphs of Twist Knots 1Abdulgani ¸Sahinand 2Bünyamin ¸Sahin 1Faculty of Science and Letters 2Faculty of Science Department Department of Mathematics of Mathematics Agrı˘ Ibrahim˙ Çeçen University Selçuk University Postcode 04100 Postcode 42130 Agrı,˘ Turkey Konya, Turkey [email protected] [email protected] Received: January 1, 2019; Accepted: March 16, 2019 Abstract We frequently encounter knots in the flow of our daily life. Either we knot a tie or we tie a knot on our shoes. We can even see a fisherman knotting the rope of his boat. Of course, the knot as a mathematical model is not that simple. These are the reflections of knots embedded in three- dimensional space in our daily lives. In fact, the studies on knots are meant to create a complete classification of them. This has been achieved for a large number of knots today. But we cannot say that it has been terminated yet. There are various effective instruments while carrying out all these studies. One of these effective tools is graphs. Graphs are have made a great contribution to the development of algebraic topology. Along with this support, knot theory has taken an important place in low dimensional manifold topology. In 1984, Jones introduced a new polynomial for knots. The discovery of that polynomial opened a new era in knot theory. In a short time, this polynomial was defined by algebraic arguments and its combinatorial definition was made. -
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. -
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. -
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 . -
Lecture 6 Braids Braids, Like Knots and Links, Are Curves in R3 with A
Lecture 6 Braids Braids, like knots and links, are curves in R3 with a natural composition operation. They have the advantage of forming a group under the composition operation (unlike knots, inverse braids always exist). This group is denoted by Bn. The subscript n is a natural number, so that there is an infinite series of braid groups B1 ⊂ B2 ⊂ · · · ⊂ Bn ⊂ ::: At first we shall define and study these groups geometrically, then look at them as a purely algebraic object via their presenta- tion obtained by Emil Artin (who actually invented braids in the 1920ies). Then we shall see that braids are related to knots and links via a geometric modification called closure and study the consequences of this relationship. We note at once that braids play an important role in many fields of mathematics and theoretical physics, exemplified by such important terms as “braid cohomology”, and this is not due to their relationship to knots. But here we are interested in braids mainly because of this relationship. 6.1. Geometric braids A braid in n strands is a set consisting of n pairwise noninter- secting polygonal curves (called strands) in R3 joining n points aligned on a horizontal line L to n points with the same x; y coordinates aligned on a horizontal line L0 parallel to L and located lower than L; the strands satisfy the following condition: when we move downward along any strand from a point on L to 1 2 a point on L0, the tangent vectors of this motion cannot point upward (i.e., the z-coordinate of these vectors is always negative). -
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 ............................... -
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. -
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. -
Arxiv:1605.01711V1 [Math.GT] 5 May 2016 Diffeomorphisms; See [7] for More Details
MINIMAL BRAID REPRESENTATIVES OF QUASIPOSITIVE LINKS KYLE HAYDEN Abstract. We show that every quasipositive link has a quasipositive minimal braid representative, partially resolving a question posed by Orevkov. These quasipositive minimal braids are used to show that the maximal self-linking number of a quasipositive link is bounded below by the negative of the minimal braid index, with equality if and only if the link is an unlink. This implies that the only amphicheiral quasipositive links are the unlinks, answering a question of Rudolph's. 1. Introduction Quasipositive links in S3 were introduced by Rudolph [14] and defined in terms of special braid diagrams, the details of which we recall below. These links possess a variety of noteworthy features. Perhaps most strikingly, results of Rudolph [14] and Boileau-Orevkov [4] show that quasipositive links are precisely those links which arise as transverse intersections of the 3 2 −1 2 unit sphere S ⊂ C with complex plane curves f (0) ⊂ C , where f is a non-constant polynomial. The hierarchy of braid positive, positive, strongly quasipositive, and quasipositive links interacts in compelling ways with conditions such as fiberedness [6, 10], sliceness [15], homogeneity [1], and symplectic/Lagrangian fillability [4, 9], and quasipositive links have well-understood behavior with respect to invariants such as the four-ball genus, the maximal self-linking number, and the Ozsv´ath-Szab´oconcordance invariant τ [10]. For a different perspective, we can view quasipositive braids as a monoid in the mapping class group of a disk with marked points, where they lie inside the contact-geometrically important monoid of right-veering arXiv:1605.01711v1 [math.GT] 5 May 2016 diffeomorphisms; see [7] for more details.