Knot Theory and DNA
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Conservation of Complex Knotting and Slipknotting Patterns in Proteins
Conservation of complex knotting and PNAS PLUS slipknotting patterns in proteins Joanna I. Sułkowskaa,1,2, Eric J. Rawdonb,1, Kenneth C. Millettc, Jose N. Onuchicd,2, and Andrzej Stasiake aCenter for Theoretical Biological Physics, University of California at San Diego, La Jolla, CA 92037; bDepartment of Mathematics, University of St. Thomas, Saint Paul, MN 55105; cDepartment of Mathematics, University of California, Santa Barbara, CA 93106; dCenter for Theoretical Biological Physics , Rice University, Houston, TX 77005; and eCenter for Integrative Genomics, Faculty of Biology and Medicine, University of Lausanne, 1015 Lausanne, Switzerland Edited by* Michael S. Waterman, University of Southern California, Los Angeles, CA, and approved May 4, 2012 (received for review April 17, 2012) While analyzing all available protein structures for the presence of ers fixed configurations, in this case proteins in their native folded knots and slipknots, we detected a strict conservation of complex structures. Then they may be treated as frozen and thus unable to knotting patterns within and between several protein families undergo any deformation. despite their large sequence divergence. Because protein folding Several papers have described various interesting closure pathways leading to knotted native protein structures are slower procedures to capture the knot type of the native structure of and less efficient than those leading to unknotted proteins with a protein or a subchain of a closed chain (1, 3, 29–33). In general, similar size and sequence, the strict conservation of the knotting the strategy is to ensure that the closure procedure does not affect patterns indicates an important physiological role of knots and slip- the inherent entanglement in the analyzed protein chain or sub- knots in these proteins. -
Complete Invariant Graphs of Alternating Knots
Complete invariant graphs of alternating knots Christian Soulié First submission: April 2004 (revision 1) Abstract : Chord diagrams and related enlacement graphs of alternating knots are enhanced to obtain complete invariant graphs including chirality detection. Moreover, the equivalence by common enlacement graph is specified and the neighborhood graph is defined for general purpose and for special application to the knots. I - Introduction : Chord diagrams are enhanced to integrate the state sum of all flype moves and then produce an invariant graph for alternating knots. By adding local writhe attribute to these graphs, chiral types of knots are distinguished. The resulting chord-weighted graph is a complete invariant of alternating knots. Condensed chord diagrams and condensed enlacement graphs are introduced and a new type of graph of general purpose is defined : the neighborhood graph. The enlacement graph is enriched by local writhe and chord orientation. Hence this enhanced graph distinguishes mutant alternating knots. As invariant by flype it is also invariant for all alternating knots. The equivalence class of knots with the same enlacement graph is fully specified and extended mutation with flype of tangles is defined. On this way, two enhanced graphs are proposed as complete invariants of alternating knots. I - Introduction II - Definitions and condensed graphs II-1 Knots II-2 Sign of crossing points II-3 Chord diagrams II-4 Enlacement graphs II-5 Condensed graphs III - Realizability and construction III - 1 Realizability -
Ribbon Concordances and Doubly Slice Knots
Ribbon concordances and doubly slice knots Ruppik, Benjamin Matthias Advisors: Arunima Ray & Peter Teichner The knot concordance group Glossary Definition 1. A knot K ⊂ S3 is called (topologically/smoothly) slice if it arises as the equatorial slice of a (locally flat/smooth) embedding of a 2-sphere in S4. – Abelian invariants: Algebraic invari- Proposition. Under the equivalence relation “K ∼ J iff K#(−J) is slice”, the commutative monoid ants extracted from the Alexander module Z 3 −1 A (K) = H1( \ K; [t, t ]) (i.e. from the n isotopy classes of o connected sum S Z K := 1 3 , # := oriented knots S ,→S of knots homology of the universal abelian cover of the becomes a group C := K/ ∼, the knot concordance group. knot complement). The neutral element is given by the (equivalence class) of the unknot, and the inverse of [K] is [rK], i.e. the – Blanchfield linking form: Sesquilin- mirror image of K with opposite orientation. ear form on the Alexander module ( ) sm top Bl: AZ(K) × AZ(K) → Q Z , the definition Remark. We should be careful and distinguish the smooth C and topologically locally flat C version, Z[Z] because there is a huge difference between those: Ker(Csm → Ctop) is infinitely generated! uses that AZ(K) is a Z[Z]-torsion module. – Levine-Tristram-signature: For ω ∈ S1, Some classical structure results: take the signature of the Hermitian matrix sm top ∼ ∞ ∞ ∞ T – There are surjective homomorphisms C → C → AC, where AC = Z ⊕ Z2 ⊕ Z4 is Levine’s algebraic (1 − ω)V + (1 − ω)V , where V is a Seifert concordance group. -
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. -
CROSSING CHANGES and MINIMAL DIAGRAMS the Unknotting
CROSSING CHANGES AND MINIMAL DIAGRAMS ISABEL K. DARCY The unknotting number of a knot is the minimal number of crossing changes needed to convert the knot into the unknot where the minimum is taken over all possible diagrams of the knot. For example, the minimal diagram of the knot 108 requires 3 crossing changes in order to change it to the unknot. Thus, by looking only at the minimal diagram of 108, it is clear that u(108) ≤ 3 (figure 1). Nakanishi [5] and Bleiler [2] proved that u(108) = 2. They found a non-minimal diagram of the knot 108 in which two crossing changes suffice to obtain the unknot (figure 2). Lower bounds on unknotting number can be found by looking at how knot invariants are affected by crossing changes. Nakanishi [5] and Bleiler [2] used signature to prove that u(108)=2. Figure 1. Minimal dia- Figure 2. A non-minimal dia- gram of knot 108 gram of knot 108 Bernhard [1] noticed that one can determine that u(108) = 2 by using a sequence of crossing changes within minimal diagrams and ambient isotopies as shown in figure. A crossing change within the minimal diagram of 108 results in the knot 62. We then use an ambient isotopy to change this non-minimal diagram of 62 to a minimal diagram. The unknot can then be obtained by changing one crossing within the minimal diagram of 62. Bernhard hypothesized that the unknotting number of a knot could be determined by only looking at minimal diagrams by using ambient isotopies between crossing changes. -
On the Number of Unknot Diagrams Carolina Medina, Jorge Luis Ramírez Alfonsín, Gelasio Salazar
On the number of unknot diagrams Carolina Medina, Jorge Luis Ramírez Alfonsín, Gelasio Salazar To cite this version: Carolina Medina, Jorge Luis Ramírez Alfonsín, Gelasio Salazar. On the number of unknot diagrams. SIAM Journal on Discrete Mathematics, Society for Industrial and Applied Mathematics, 2019, 33 (1), pp.306-326. 10.1137/17M115462X. hal-02049077 HAL Id: hal-02049077 https://hal.archives-ouvertes.fr/hal-02049077 Submitted on 26 Feb 2019 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. On the number of unknot diagrams Carolina Medina1, Jorge L. Ramírez-Alfonsín2,3, and Gelasio Salazar1,3 1Instituto de Física, UASLP. San Luis Potosí, Mexico, 78000. 2Institut Montpelliérain Alexander Grothendieck, Université de Montpellier. Place Eugèene Bataillon, 34095 Montpellier, France. 3Unité Mixte Internationale CNRS-CONACYT-UNAM “Laboratoire Solomon Lefschetz”. Cuernavaca, Mexico. October 17, 2017 Abstract Let D be a knot diagram, and let D denote the set of diagrams that can be obtained from D by crossing exchanges. If D has n crossings, then D consists of 2n diagrams. A folklore argument shows that at least one of these 2n diagrams is unknot, from which it follows that every diagram has finite unknotting number. -
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. -
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. -
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. -
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. -
Results on Nonorientable Surfaces for Knots and 2-Knots
University of Nebraska - Lincoln DigitalCommons@University of Nebraska - Lincoln Dissertations, Theses, and Student Research Papers in Mathematics Mathematics, Department of 8-2021 Results on Nonorientable Surfaces for Knots and 2-knots Vincent Longo University of Nebraska-Lincoln, [email protected] Follow this and additional works at: https://digitalcommons.unl.edu/mathstudent Part of the Geometry and Topology Commons Longo, Vincent, "Results on Nonorientable Surfaces for Knots and 2-knots" (2021). Dissertations, Theses, and Student Research Papers in Mathematics. 111. https://digitalcommons.unl.edu/mathstudent/111 This Article is brought to you for free and open access by the Mathematics, Department of at DigitalCommons@University of Nebraska - Lincoln. It has been accepted for inclusion in Dissertations, Theses, and Student Research Papers in Mathematics by an authorized administrator of DigitalCommons@University of Nebraska - Lincoln. RESULTS ON NONORIENTABLE SURFACES FOR KNOTS AND 2-KNOTS by Vincent Longo A DISSERTATION Presented to the Faculty of The Graduate College at the University of Nebraska In Partial Fulfillment of Requirements For the Degree of Doctor of Philosophy Major: Mathematics Under the Supervision of Professors Alex Zupan and Mark Brittenham Lincoln, Nebraska May, 2021 RESULTS ON NONORIENTABLE SURFACES FOR KNOTS AND 2-KNOTS Vincent Longo, Ph.D. University of Nebraska, 2021 Advisor: Alex Zupan and Mark Brittenham A classical knot is a smooth embedding of the circle S1 into the 3-sphere S3. We can also consider embeddings of arbitrary surfaces (possibly nonorientable) into a 4-manifold, called knotted surfaces. In this thesis, we give an introduction to some of the basics of the studies of classical knots and knotted surfaces, then present some results about nonorientable surfaces bounded by classical knots and embeddings of nonorientable knotted surfaces.