Knot Tricolorability Danielle Brushaber & Mckenzie Hennen

Total Page:16

File Type:pdf, Size:1020Kb

Knot Tricolorability Danielle Brushaber & Mckenzie Hennen Knot Tricolorability Danielle Brushaber & McKenzie Hennen Faculty Mentor: Carolyn Otto University of Wisconsin-Eau Claire Problem & Importance Definitions Knot Theory, a field of Topology, can be used to Basic Knot Definitions Linear Algebra Definitions model and understand how enzymes (called topoi- Knot- a curve in R3 that is non-intersecting and closed, similar to a circle but somerases) work in DNA processes to untangle or Matrix of a knot- each intersection’s equation determines a row in a matrix. For example, using WH3 , the equation could be tangled up. Consider a tangled string attached at the ends. 1 repair strands of DNA. In a human cell nucleus, the 2a − b − c = 0 would make one row of a matrix. a Knot invariant b DNA is linear, so the knots can slip off the end, - a characteristic of a knot. Useful for distinguishing when two c Determinant- A property of a square matrix. We used the program Maple to find the determinant, as the matrices are n and it is difficult to recognize what the enzymes do. knots are different. Tricolorable-For a knot to be tricolorable, the three lines involved in an intersec- as large as 26 × 26. In the case of the Trefoil knot, finding the determinant by hand is conducted in the following way: a b c First, look at the number in the top left corner and disregard the adjacent column and row. Repeat this step However, the DNA in mito- tion must either be 3 different colors or all 1 color . Tricolorability is a 2 − − =0 2 −1 −1 b a c with the second number in the first row and once more with the last number in the first row. The matrices chondria is circular, along with topological invariant. The unknot (a circle) is not tricolorable, so therefore anything 2 − − =0 becomes −1 2 −1 2c − a − b =0 below show these steps: prokaryotic cells (bacteria), so that is tricolorable cannot be the unknot. Colorability is the minor determinant of −1 −1 2 the enzyme processes are more the knot’s matrix. Additionally, the factors of this number are the colorability. For Step 1: Step 2: Step 3: For the basic 2 × 2 matrix, noticable in knots in this type example, if a knot is 21 colorable, it is also 3 colorable (tricolorable), and 7 colorable. 2 -1 -1 of DNA. Image from paper by De Witt Full positive twist- a change within the link of a Whitehead Double. We use n 2 2 −1 −(−1) −1 −1 +(−1) −1 2 a b = ad − bc Determinant= Sumners. to denote the number of full positive twists. Images of n = 1 through n = 6 are 2 −1 −1 −1 −1 2 −1 2 −1 2 −1 −1 Invariants prove to be a useful tool in studying when c d pictured in the Conjectures section. two knots are different. Tricolorability is an easily un- −1 2 −1 2 −1 −1 Doubling operator- an operation on a knot doubling Minor determinant- the determinant of the matrix found when the first column and first row are disregarded. For any n × n matrix, the minor derstood invariant that we will use to distinguish dou- the knot segments and adding a link. The Whitehead bles (replications) of certain prime knots. determinant is of an n − 1 × n − 1 matrix. For knots, the minor determinant of the knot’s matrix is the knot’s colorability. (WH) doubling of 31 is pictured to the right. Conjectures Proof for W H51 Conjecture As the number of full positive twists (n) changes, the minor determinant of the knot changes. We have discovered a pattern for knots WH31,WH41, and WH51 For WH51 with link n, n − WH51 is tricolorable when n = 1+3k where k∈ WH31 WH51 N n =1 n =1 is11 WH41 n =1 is21 ∪{0}. n =2 is17 n =2 is31 n =2 Consider WH5 n =3 is23 Regardless of the n, n =3 is41 1 WOLOG, let WH5 n n with link n being 1 n =3 n =4 is29 the colorability of 4 is always n =4 is51 be colored in this 1 the number of full n n n =4 n n =5 is35 1 . n =5 is61 way, excluding color- positive twists n n =6 is41 n =6 is71 ing the link: =5 (n =1...n = k). n =6 colorability is 5 + 6n colorability is 11 + 10n If the entrances to the twisting are colored in this way , then for every n = 1+3k As the number of full positive twists increases in the Whitehead double of a knot, the matrix behaves in N The matrices for WH3 where n =1, 2 and 3 are shown below respectively. where k∈ ∪{0}, the twisting, and therefore the knot, is tricolorable. the following way. (This pattern occurs when the intersections of the link are represented by the last 1 2 0 −1 0 −100000000000 2 0 −1 0 −10000000000 2 0 −1 0 −1000000000 2 0 0 −1 0 −10000000000 Base Case: k = 0, n = 1+3(0) = 1. Link n =1 is tricolorable. rows in its matrix.) 2 0 0 −1 0 −1000000000 2 0 0 −1 0 −100000000 0 2 0 0 −1000000 −10 0 0 0 0 2 0 0 −1000000 −10 0 0 0 2 0 0 −1000000 −10 0 02000 −10 0 0 0 −100000 For n =1+3(k + 1): n =1+3(k +1)=1+3k +3. Adding 1 to k adds 3 full 02000 −10 0 0 0 −10 0 0 0 General Pattern: n n 02000 −10 0 0 0 −10 0 0 00200000 −10 0 0 0 −10 0 When creating the matrix for = 2 from = 1, a row and column are added. The 00200000 −10 0 0 0 −1 0 00200000 −10 0 0 0 −1 002000000 −10 0 −10 0 0 002000000 −10 0 −10 0 002000000 −10 0 −1 0 −10020000 −10000000 positive twists to n, which looks like . last two rows, an added row, and an added column are the only changing components of the matrix. The −10020000 −1000000 −10020000 −100000 0 −10200000 −1000000 0 −10200000 −100000 0 −10200000 −10 0 0 0 0 0 0 −10 0 −1000200000 Placing multiples of this within a link does not disrupt the entrance coloring, as new column will contain all zero’s in the rows above the blue line. The new row is inserted below the 0 0 0 −10 0 −100020000 0 0 0 −10 0 −10002000 0 0 −10 0 0 0 −100200000 0 0 −10 0 0 0 −10020000 0 0 −10 0 0 0 −1002000 0 −10 0 0 0 −1000020000 the pattern is simply extended. So, adding 3 full positive twists does not change highlighted line of the matrix in n = 1. Besides a zero being added to the end as the new column entry, 0 −10 0 0 0 −100002000 0 −10 0 0 0 −10000200 −1000000 −100020000 −1000000 −10002000 −1000000 −1000200 0000000000 −10 2 0 −1 0 the link’s colorability, and does not change the colorability of the knot. All knots this row will not change to make n = 3. In the last row, a zero is added within the sequence [...2, −1, −1] 0000000000 −10 2 0 −1 0000000000 −1 −12 0 000000000000 −10 2 −1 00000000000 −1 −10 2 000000000002 −1 −1 00000000000 −10 0 −1 2 colored in this way with the link n being n = 1+3k where k∈ N∪{0} are making it [...2, 0, −1, −1]. After n = 3, as n increases, a zero entry is placed between the (−1)’s. 0000000000020 −1 −1 0000000000020 −1 0 −1 tricolorable. Future Research Directions References and Acknowledgments • We will move forward to prove our conjectures, the equations listed above. • Office of Research and Sponsored Programs, UW-Eau Claire • We will attempt to generalize this process to other knots and doubling operators. • Department of Mathematics, UW-Eau Claire • Additionally, we will try to apply these findings more directly to DNA. • Graphics computed and rendered using Inkscape and LATEX • Adams, Colin Conrad. The Knot Book: An Elementary Introduction to the Mathematical Theory of Knots. New York: W.H. Freeman, 1994. Print. • Sumners, De Witt. ”Lifting the Curtain: Using Topology to Probe the Hidden Action of Enzymes.” Notices of the AMS 42.5(1995): n. pag. American Mathematical Society, May 1995. Web. Apr. 2015..
Recommended publications
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • CALIFORNIA STATE UNIVERSITY, NORTHRIDGE P-Coloring Of
    CALIFORNIA STATE UNIVERSITY, NORTHRIDGE P-Coloring of Pretzel Knots A thesis submitted in partial fulfillment of the requirements for the degree of Master of Science in Mathematics By Robert Ostrander December 2013 The thesis of Robert Ostrander is approved: |||||||||||||||||| |||||||| Dr. Alberto Candel Date |||||||||||||||||| |||||||| Dr. Terry Fuller Date |||||||||||||||||| |||||||| Dr. Magnhild Lien, Chair Date California State University, Northridge ii Dedications I dedicate this thesis to my family and friends for all the help and support they have given me. iii Acknowledgments iv Table of Contents Signature Page ii Dedications iii Acknowledgements iv Abstract vi Introduction 1 1 Definitions and Background 2 1.1 Knots . .2 1.1.1 Composition of knots . .4 1.1.2 Links . .5 1.1.3 Torus Knots . .6 1.1.4 Reidemeister Moves . .7 2 Properties of Knots 9 2.0.5 Knot Invariants . .9 3 p-Coloring of Pretzel Knots 19 3.0.6 Pretzel Knots . 19 3.0.7 (p1, p2, p3) Pretzel Knots . 23 3.0.8 Applications of Theorem 6 . 30 3.0.9 (p1, p2, p3, p4) Pretzel Knots . 31 Appendix 49 v Abstract P coloring of Pretzel Knots by Robert Ostrander Master of Science in Mathematics In this thesis we give a brief introduction to knot theory. We define knot invariants and give examples of different types of knot invariants which can be used to distinguish knots. We look at colorability of knots and generalize this to p-colorability. We focus on 3-strand pretzel knots and apply techniques of linear algebra to prove theorems about p-colorability of these knots.
    [Show full text]
  • How Can We Say 2 Knots Are Not the Same?
    How can we say 2 knots are not the same? SHRUTHI SRIDHAR What’s a knot? A knot is a smooth embedding of the circle S1 in IR3. A link is a smooth embedding of the disjoint union of more than one circle Intuitively, it’s a string knotted up with ends joined up. We represent it on a plane using curves and ‘crossings’. The unknot A ‘figure-8’ knot A ‘wild’ knot (not a knot for us) Hopf Link Two knots or links are the same if they have an ambient isotopy between them. Representing a knot Knots are represented on the plane with strands and crossings where 2 strands cross. We call this picture a knot diagram. Knots can have more than one representation. Reidemeister moves Operations on knot diagrams that don’t change the knot or link Reidemeister moves Theorem: (Reidemeister 1926) Two knot diagrams are of the same knot if and only if one can be obtained from the other through a series of Reidemeister moves. Crossing Number The minimum number of crossings required to represent a knot or link is called its crossing number. Knots arranged by crossing number: Knot Invariants A knot/link invariant is a property of a knot/link that is independent of representation. Trivial Examples: • Crossing number • Knot Representations / ~ where 2 representations are equivalent via Reidemester moves Tricolorability We say a knot is tricolorable if the strands in any projection can be colored with 3 colors such that every crossing has 1 or 3 colors and or the coloring uses more than one color.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • Petal Projections, Knot Colorings and Determinants
    PETAL PROJECTIONS, KNOT COLORINGS & DETERMINANTS ALLISON HENRICH AND ROBIN TRUAX Abstract. An ¨ubercrossing diagram is a knot diagram with only one crossing that may involve more than two strands of the knot. Such a diagram without any nested loops is called a petal projection. Every knot has a petal projection from which the knot can be recovered using a permutation that represents strand heights. Using this permutation, we give an algorithm that determines the p-colorability and the determinants of knots from their petal projections. In particular, we compute the determinants of all prime knots with crossing number less than 10 from their petal permutations. 1. Background There are many different ways to define a knot. The standard definition of a knot, which can be found in [1] or [4], is an embedding of a closed curve in three-dimensional space, K : S1 ! R3. Less formally, we can think of a knot as a knotted circle in 3-space. Though knots exist in three dimensions, we often picture them via 2-dimensional representations called knot diagrams. In a knot diagram, crossings involve two strands of the knot, an overstrand and an understrand. The relative height of the two strands at a crossing is conveyed by putting a small break in one strand (to indicate the understrand) while the other strand continues over the crossing, unbroken (this is the overstrand). Figure 1 shows an example of this. Two knots are defined to be equivalent if one can be continuously deformed (without passing through itself) into the other. In terms of diagrams, two knot diagrams represent equivalent knots if and only if they can be related by a sequence of Reidemeister moves and planar isotopies (i.e.
    [Show full text]
  • I.2 Curves and Knots
    8 I Graphs I.2 Curves and Knots Topology gets quickly more complicated when the dimension increases. The first step up from (0-dimensional) points are (1-dimensional) curves. Classify- ing them intrinsically is straightforward but can be complicated extrinsically. Curve models. A homeomorphism between two topological spaces is a con- tinuous bijection h : X ! Y whose inverse is also continuous. If such a map exists then X and Y are considered the same. More formally, X and Y are said to be homeomorphic or topology equivalent. If two spaces are homeo- morphic then they are either both connected or both not connected. Any two closed intervals are homeomorphic so it makes sense to use the unit in- terval, [0; 1], as the standard model. Similarly, any two half-open intervals are homeomorphic and any two open intervals are homeomorphic, but [0; 1], [0; 1), and (0; 1) are pairwise non-homeomorphic. Indeed, suppose there is a homeomorphism h : [0; 1] ! (0; 1). Removing the endpoint 0 from [0; 1] leaves the closed interval connected, but removing h(0) from (0; 1) neces- sarily disconnects the open interval. Similarly the other two pairs are non- homeomorphic. The half-open interval can be continuously and bijectively mapped to the circle S1 = fx 2 R2 j kxk = 1g. Indeed, f : [0; 1) ! S1 defined by f(x) = (sin 2πx; cos 2πx) and illustrated in Figure I.7 is such a map. Removing the midpoint disconnects any one of the three intervals but f 0 1 Figure I.7: A continuous bijection whose inverse is not continuous.
    [Show full text]
  • Writing@SVSU 2016–2017
    SAGINAW VALLEY STATE UNIVERSITY 2016-2017 7400 Bay Road University Center, MI 48710 svsu.edu ©Writing@SVSU 7400 Bay Road University Center, MI 48710 CREDITS Writing@SVSU is funded by the Office of the Dean of the College of Arts & Behavioral Sciences. Editorial Staff Christopher Giroux Associate Professor of English and Writing Center Assistant Director Joshua Atkins Literature and Creative Writing Major Alexa Foor English Major Samantha Geffert Secondary Education Major Sara Houser Elementary Education and English Language Arts Major Brianna Rivet Literature and Creative Writing Major Kylie Wojciechowski Professional and Technical Writing Major Production Layout and Photography Tim Inman Director of Marketing Support Jennifer Weiss Administrative Secretary University Communications Cover Design Justin Bell Graphic Design Major Printing SVSU Graphics Center Editor’s Note Welcome to the 2016-2017 issue of Writing@SVSU, our yearly attempt to capture a small slice of the good writing that occurs at and because of SVSU. Whether the pieces in Writing@SVSU are attached to a prize, the works you’ll find here emphasize that all writing matters, even when it’s not done for an English class (to paraphrase the title of an essay that follows). Given the political climate, where commentary is often delivered by our leaders through late- night or early-a.m. tweets, we hope you find it refreshing to read the pieces on the following pages. Beyond incorporating far more than 140 characters, these pieces encourage us to reflect at length, as they themselves were the product of much thought and reflection. Beyond being sources and the product of reflection, these texts remind us that the work of the university is, in part, to build bridges, often through words.
    [Show full text]
  • A Study of Topological Invariants in the Braid Group B2 Andrew Sweeney East Tennessee State University
    East Tennessee State University Digital Commons @ East Tennessee State University Electronic Theses and Dissertations Student Works 5-2018 A Study of Topological Invariants in the Braid Group B2 Andrew Sweeney East Tennessee State University Follow this and additional works at: https://dc.etsu.edu/etd Part of the Geometry and Topology Commons Recommended Citation Sweeney, Andrew, "A Study of Topological Invariants in the Braid Group B2" (2018). Electronic Theses and Dissertations. Paper 3407. https://dc.etsu.edu/etd/3407 This Thesis - Open Access is brought to you for free and open access by the Student Works at Digital Commons @ East Tennessee State University. It has been accepted for inclusion in Electronic Theses and Dissertations by an authorized administrator of Digital Commons @ East Tennessee State University. For more information, please contact [email protected]. A Study of Topological Invariants in the Braid Group B2 A thesis presented to the faculty of the Department of Mathematics East Tennessee State University In partial fulfillment of the requirements for the degree Master of Science in Mathematical Sciences by Andrew Sweeney May 2018 Frederick Norwood, Ph.D., Chair Robert Gardner, Ph.D. Rodney Keaton, Ph.D. Keywords: Jones polynomial, ambient isotopy, B2, Temperley-Lieb algebra ABSTRACT A Study of Topological Invariants in the Braid Group B2 by Andrew Sweeney The Jones polynomial is a special topological invariant in the field of Knot Theory. Created by Vaughn Jones, in the year 1984, it is used to study when links in space are topologically different and when they are topologically equivalent. This thesis discusses the Jones polynomial in depth as well as determines a general form for the closure of any braid in the braid group B2 where the closure is a knot.
    [Show full text]
  • Tricolorability
    Knot Theory Week 2: Tricolorability Xiaoyu Qiao, E. L. January 20, 2015 A central problem in knot theory is concerned with telling different knots apart. We introduce the notion of what it means for two knots to be \the same" or “different," and how we may distinguish one kind of knot from another. 1 Knot Equivalence Definition. Two knots are equivalent if one can be transformed into another by stretching or moving it around without tearing it or having it intersect itself. Below is an example of two equivalent knots with different regular projections (Can you see why?). Two knots are equivalent if and only if the regular projection of one knot can be transformed into that of the other knot through a finite sequence of Reidemeister moves. Then, how do we know if two knots are different? For example, how can we tell that the trefoil knot and the figure-eight knot are actually not the same? An equivalent statement to the biconditional above would be: two knots are not equivalent if and only if there is no finite sequence of Reidemeister moves that can be used to transform one into another. Since there is an infinite number of possible sequences of Reidemeister moves, we certainly cannot try all of them. We need a different method to prove that two knots are not equivalent: a knot invariant. 1 2 Knot Invariant A knot invariant is a function that assigns a quantity or a mathematical expression to each knot, which is preserved under knot equivalence. In other words, if two knots are equivalent, then they must be assigned the same quantity or expression.
    [Show full text]
  • Properties and Applications of the Annular Filtration on Khovanov Homology
    Properties and applications of the annular filtration on Khovanov homology Author: Diana D. Hubbard Persistent link: http://hdl.handle.net/2345/bc-ir:106791 This work is posted on eScholarship@BC, Boston College University Libraries. Boston College Electronic Thesis or Dissertation, 2016 Copyright is held by the author. This work is licensed under a Creative Commons Attribution 4.0 International License. http://creativecommons.org/licenses/by/4.0/ Properties and applications of the annular filtration on khovanov homology Diana D. Hubbard Adissertation submitted to the Faculty of the Department of Mathematics in partial fulfillment of the requirements for the degree of Doctor of Philosophy Boston College Morrissey College of Arts and Sciences Graduate School March 2016 © Copyright 2016 Diana D. Hubbard PROPERTIES AND APPLICATIONS OF THE ANNULAR FILTRATION ON KHOVANOV HOMOLOGY Diana D. Hubbard Advisor: J. Elisenda Grigsby Abstract The first part of this thesis is on properties of annular Khovanov homology. We prove a connection between the Euler characteristic of annular Khovanov homology and the clas- sical Burau representation for closed braids. This yields a straightforward method for distinguishing, in some cases, the annular Khovanov homologies of two closed braids. As a corollary, we obtain the main result of the first project: that annular Khovanov homology is not invariant under a certain type of mutation on closed braids that we call axis-preserving. The second project is joint work with Adam Saltz. Plamenevskaya showed in 2006 that the homology class of a certain distinguished element in Khovanov homology is an invariant of transverse links. In this project we define an annular refinement of this element, , and show that while is not an invariant of transverse links, it is a conjugacy class invariant of braids.
    [Show full text]