Quandles an Introduction to the Algebra of Knots
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Various Topics in Rack and Quandle Homology
Various topics in rack and quandle homology April 14, 2010 Master's thesis in Mathematics Jorik Mandemaker supervisor: Dr. F.J.-B.J. Clauwens second reader: Prof. Dr. F. Keune student number: 0314145 Faculty of Science (FNWI) Radboud University Nijmegen Contents 1 Introduction 5 1.1 Racks and quandles . 6 1.2 Quandles and knots . 7 1.3 Augmented quandles and the adjoint group . 8 1.3.1 The adjoint group . 9 1.4 Connected components . 9 1.5 Rack and quandle homology . 10 1.6 Quandle coverings . 10 1.6.1 Extensions . 11 1.6.2 The fundamental group of a quandle . 12 1.7 Historical notes . 12 2 The second cohomology group of alexander quandles 14 2.1 The adjoint group of Alexander quandles . 15 2.1.1 Connected Alexander quandles . 15 2.1.2 Alexander quandles with connected components . 18 2.2 The second cohomology group of connected Alexander quandles . 19 3 Polynomial cocycles 22 3.1 Introduction . 23 3.2 Polynomial cochains . 23 3.3 A decomposition and filtration of the complex . 24 3.4 The 3-cocycles . 25 3.5 Variable Reduction . 27 3.6 Proof of surjectivity . 28 3.6.1 t = s .............................. 29 3.6.2 t < s .............................. 30 3.7 Final steps . 33 4 Rack and quandle modules 35 4.1 Rack and Quandle Modules . 36 4.1.1 Definitions . 36 4.1.2 Some examples . 38 4.2 Reduced rack modules . 39 1 4.3 Right modules and tensor products . 40 4.4 The rack algebra . 42 4.5 Examples . 44 4.5.1 A free resolution for trivial quandles . -
Moufang Loops and Alternative Algebras
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 132, Number 2, Pages 313{316 S 0002-9939(03)07260-5 Article electronically published on August 28, 2003 MOUFANG LOOPS AND ALTERNATIVE ALGEBRAS IVAN P. SHESTAKOV (Communicated by Lance W. Small) Abstract. Let O be the algebra O of classical real octonions or the (split) algebra of octonions over the finite field GF (p2);p>2. Then the quotient loop O∗=Z ∗ of the Moufang loop O∗ of all invertible elements of the algebra O modulo its center Z∗ is not embedded into a loop of invertible elements of any alternative algebra. It is well known that for an alternative algebra A with the unit 1 the set U(A) of all invertible elements of A forms a Moufang loop with respect to multiplication [3]. But, as far as the author knows, the following question remains open (see, for example, [1]). Question 1. Is it true that any Moufang loop can be imbedded into a loop of type U(A) for a suitable unital alternative algebra A? A positive answer to this question was announced in [5]. Here we show that, in fact, the answer to this question is negative: the Moufang loop U(O)=R∗ for the algebra O of classical octonions over the real field R andthesimilarloopforthe algebra of octonions over the finite field GF (p2);p>2; are not imbeddable into the loops of type U(A). Below O denotes an algebra of octonions (or Cayley{Dickson algebra) over a field F of characteristic =2,6 O∗ = U(O) is the Moufang loop of all the invertible elements of O, L = O∗=F ∗. -
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. -
MOUFANG LOOPS THAT SHARE ASSOCIATOR and THREE QUARTERS of THEIR MULTIPLICATION TABLES 1. Introduction Moufang Loops, I.E., Loops
MOUFANG LOOPS THAT SHARE ASSOCIATOR AND THREE QUARTERS OF THEIR MULTIPLICATION TABLES ALES· DRAPAL¶ AND PETR VOJTECHOVSK· Y¶ Abstract. Two constructions due to Dr¶apalproduce a group by modifying exactly one quarter of the Cayley table of another group. We present these constructions in a compact way, and generalize them to Moufang loops, using loop extensions. Both constructions preserve associators, the associator subloop, and the nucleus. We con- jecture that two Moufang 2-loops of ¯nite order n with equivalent associator can be connected by a series of constructions similar to ours, and o®er empirical evidence that this is so for n = 16, 24, 32; the only interesting cases with n · 32. We further investigate the way the constructions a®ect code loops and loops of type M(G; 2). The paper closes with several conjectures and research questions concerning the distance of Moufang loops, classi¯cation of small Moufang loops, and generalizations of the two constructions. MSC2000: Primary: 20N05. Secondary: 20D60, 05B15. 1. Introduction Moufang loops, i.e., loops satisfying the Moufang identity ((xy)x)z = x(y(xz)), are surely the most extensively studied loops. Despite this fact, the classi¯cation of Moufang loops is ¯nished only for orders less than 64, and several ingenious constructions are needed to obtain all these loops. The purpose of this paper is to initiate a new approach to ¯nite Moufang 2-loops. Namely, we intend to decide whether all Moufang 2-loops of given order with equivalent associator can be obtained from just one of them, using only group-theoretical constructions. -
Split Octonions
Split Octonions Benjamin Prather Florida State University Department of Mathematics November 15, 2017 Group Algebras Split Octonions Let R be a ring (with unity). Prather Let G be a group. Loop Algebras Octonions Denition Moufang Loops An element of group algebra R[G] is the formal sum: Split-Octonions Analysis X Malcev Algebras rngn Summary gn2G Addition is component wise (as a free module). Multiplication follows from the products in R and G, distributivity and commutativity between R and G. Note: If G is innite only nitely many ri are non-zero. Group Algebras Split Octonions Prather Loop Algebras A group algebra is itself a ring. Octonions In particular, a group under multiplication. Moufang Loops Split-Octonions Analysis A set M with a binary operation is called a magma. Malcev Algebras Summary This process can be generalized to magmas. The resulting algebra often inherit the properties of M. Divisibility is a notable exception. Magmas Split Octonions Prather Loop Algebras Octonions Moufang Loops Split-Octonions Analysis Malcev Algebras Summary Loops Split Octonions Prather Loop Algebras In particular, loops are not associative. Octonions It is useful to dene some weaker properties. Moufang Loops power associative: the sub-algebra generated by Split-Octonions Analysis any one element is associative. Malcev Algebras diassociative: the sub-algebra generated by any Summary two elements is associative. associative: the sub-algebra generated by any three elements is associative. Loops Split Octonions Prather Loop Algebras Octonions Power associativity gives us (xx)x = x(xx). Moufang Loops This allows x n to be well dened. Split-Octonions Analysis −1 Malcev Algebras Diassociative loops have two sided inverses, x . -
A Guide to Self-Distributive Quasigroups, Or Latin Quandles
A GUIDE TO SELF-DISTRIBUTIVE QUASIGROUPS, OR LATIN QUANDLES DAVID STANOVSKY´ Abstract. We present an overview of the theory of self-distributive quasigroups, both in the two- sided and one-sided cases, and relate the older results to the modern theory of quandles, to which self-distributive quasigroups are a special case. Most attention is paid to the representation results (loop isotopy, linear representation, homogeneous representation), as the main tool to investigate self-distributive quasigroups. 1. Introduction 1.1. The origins of self-distributivity. Self-distributivity is such a natural concept: given a binary operation on a set A, fix one parameter, say the left one, and consider the mappings ∗ La(x) = a x, called left translations. If all such mappings are endomorphisms of the algebraic structure (A,∗ ), the operation is called left self-distributive (the prefix self- is usually omitted). Equationally,∗ the property says a (x y) = (a x) (a y) ∗ ∗ ∗ ∗ ∗ for every a, x, y A, and we see that distributes over itself. Self-distributivity∈ was pinpointed already∗ in the late 19th century works of logicians Peirce and Schr¨oder [69, 76], and ever since, it keeps appearing in a natural way throughout mathematics, perhaps most notably in low dimensional topology (knot and braid invariants) [12, 15, 63], in the theory of symmetric spaces [57] and in set theory (Laver’s groupoids of elementary embeddings) [15]. Recently, Moskovich expressed an interesting statement on his blog [60] that while associativity caters to the classical world of space and time, distributivity is, perhaps, the setting for the emerging world of information. -
INTRODUCTION to ALGEBRAIC THEORY of QUANDLES Lecture 1
INTRODUCTION TO ALGEBRAIC THEORY OF QUANDLES Lecture 1 Valeriy Bardakov Sobolev Institute of Mathematics, Novosibirsk August 24-28, 2020 ICTS Bengaluru, India V. Bardakov (Sobolev Institute of Math.) INTRODUCTION TO ALGEBRAIC THEORY OF QUANDLESAugust 27-30, 2019 1 / 53 Green-board in ICTS V. Bardakov (Sobolev Institute of Math.) INTRODUCTION TO ALGEBRAIC THEORY OF QUANDLESAugust 27-30, 2019 2 / 53 Quandles A quandle is a non-empty set with one binary operation that satisfies three axioms. These axioms motivated by the three Reidemeister moves of diagrams 3 of knots in the Euclidean space R . Quandles were introduced independently by S. Matveev and D. Joyce in 1982. V. Bardakov (Sobolev Institute of Math.) INTRODUCTION TO ALGEBRAIC THEORY OF QUANDLESAugust 27-30, 2019 3 / 53 Definition of rack and quandle Definition A rack is a non-empty set X with a binary algebraic operation (a; b) 7! a ∗ b satisfying the following conditions: (R1) For any a; b 2 X there is a unique c 2 X such that a = c ∗ b; (R2) Self-distributivity: (a ∗ b) ∗ c = (a ∗ c) ∗ (b ∗ c) for all a; b; c 2 X. A quandle X is a rack which satisfies the following condition: (Q1) a ∗ a = a for all a 2 X. V. Bardakov (Sobolev Institute of Math.) INTRODUCTION TO ALGEBRAIC THEORY OF QUANDLESAugust 27-30, 2019 4 / 53 Symmetries Let X be a rack. For any a 2 X define a map Sa : X −! X, which sends any element x 2 X to element x ∗ a, i. e. xSa = x ∗ a. We shall call Sa the symmetry at a. -
Moufang Loops General Theory and Visualization of Non-Associative Moufang Loops of Order 16
U.U.D.M. Project Report 2016:18 Moufang Loops General theory and visualization of non-associative Moufang loops of order 16 Mikael Stener Examensarbete i matematik, 15 hp Handledare: Anders Öberg Examinator: Veronica Crispin Quinonez Juni 2016 Department of Mathematics Uppsala University Moufang Loops General theory and visualization of non-associative Moufang loops of order 16 Thesis by: Mikael Stener Supervisor: Anders Oberg¨ Uppsala University Department of Mathematics April 1, 2016 Abstract This thesis examines the algebraic structure of non-associative Moufang loops. We describe their basic properties such as their alternativity and flexibility. A proof of Moufang's Theorem is presented which implies the important notice of di-associativity. We then provide a case study which leads us to find all non- associative Moufang loops of order less than 32. We study in particular the ones of order 16 and provide a visualization of the multiplication in these loops as has been previously done by Vojtˇechovsk´y[6] with the (only) non-associative Moufang loop of order 12. A brief presentation of the life and work of the name giver of Moufang loops, Ruth Moufang, is also given. Contents 1 Introduction 2 2 Theory 4 2.1 Groupoids, quasigroups and loops . .4 2.2 Inverse property and autotopisms . .8 2.3 Moufang loops . .9 3 Moufang's Theorem 13 4 Moufang loops of small order 18 5 Visualization of Moufang loops of order 16 27 5.1 M16(D4; 2) .............................. 29 5.2 M16(Q; 2)............................... 30 5.3 M16(C2 × C4)............................. 31 5.4 M16(C2 × C4;Q).......................... -
Arxiv:2101.01957V2 [Math.CT] 20 Jan 2021 Ytmo Ymtis Tahdt Ahpit Oeprecisel More Point
HIGHER COVERINGS OF RACKS AND QUANDLES – PART II FRANÇOIS RENAUD Abstract. This article is the second part of a series of three articles, in which we develop a higher covering theory of racks and quandles. This project is rooted in M. Eisermann’s work on quandle coverings, and the categorical perspective brought to the subject by V. Even, who characterizes coverings as those surjections which are categorically central, relatively to trivial quandles. We extend this work by applying the techniques from higher categorical Galois theory, in the sense of G. Janelidze, and in particular we identify meaningful higher- dimensional centrality conditions defining our higher coverings of racks and quandles. In this second article (Part II), we show that categorical Galois theory applies to the inclusion of the category of coverings into the category of surjective morphisms of racks and quandles. We characterise the induced Galois theoretic concepts of trivial covering, normal covering and covering in this two-dimensional context. The latter is described via our definition and study of double coverings, also called algebraically central double extensions of racks and quandles. We define a suitable and well-behaved commutator which captures the zero, one and two-dimensional concepts of centralization in the category of quandles. We keep track of the links with the corresponding concepts in the category of groups. 1. Introduction This article (Part II ) is the continuation of [60] which we refer to as Part I. In the following paragraphs we recall enough material from Part I, and the first order covering theory of racks and quandles, in order to contextualize and motivate the content of the present paper, in which, based on the firm theoretical groundings of categorical Galois theory, we identify the second order coverings of racks and quandles, and the relative concept of centralization, together with the definition of a suitable commutator in this context. -
Free Medial Quandles
Algebra Univers. 78 (2017) 43–54 DOI 10.1007/s00012-017-0443-2 Published online May 23, 2017 © 2017 The Author(s) Algebra Universalis This article is an open access publication Free medial quandles Premyslˇ Jedlicka,ˇ Agata Pilitowska, and Anna Zamojska-Dzienio Abstract. This paper gives the construction of free medial quandles as well as free n-symmetric medial quandles and free m-reductive medial quandles. 1. Introduction A binary algebra (Q, ) is called a rack if the following conditions hold, for · every x, y, z Q: ∈ x(yz)=(xy)(xz) (we say Q is left distributive), • the equation xu = y has a unique solution u Q (we say Q is a left • ∈ quasigroup). An idempotent rack is called a quandle (we say Q is idempotent if xx = x for every x Q). A quandle Q is medial if, for every x, y, u, v Q, ∈ ∈ (xy)(uv)=(xu)(yv). An important example of a medial quandle is an abelian group A with an operation defined by a b = (1 h)(a)+h(b), where h is an automorphism ∗ ∗ − of A. This construction is called an affine quandle (or sometimes an Alexander quandle) and denoted by Aff(A, h). In the literature [6, 7], the group A is 1 usually considered to be a Z[t, t− ]-module, where t a = h(a), for each a A. · ∈ We shall adopt this point of view here as well and we usually write Aff(A, r) instead, where r is a ring element. Note that in universal algebra terminology, an algebra is said to be affine if it is polynomially equivalent to a module. -
The Moufang Loops of Order 64 and 81
The Moufang Loops of Order 64 and 81 G´abor P. Nagy Bolyai Institute, University of Szeged, Aradi vertanuk tere 1, 6720 Szeged, Hungary Petr Vojtˇechovsk´y Department of Mathematics, University of Denver, Denver, Colorado 80208, U.S.A. Abstract We classify Moufang loops of order 64 and 81 up to isomorphism, using a linear algebraic approach to central loop extensions. In addition to the 267 groups of order 64, there are 4262 nonassociative Moufang loops of order 64. In addition to the 15 groups of order 81, there are 5 nonassociative Moufang loops of order 81, 2 of which are commutative. Key words: Moufang loop, code loop, 2-loop, classification of Moufang loops, GAP. 1. Introduction 1.1. Mathematical background Let Q be a set with one binary operation, denoted by juxtaposition. For x ∈ Q, define the left translation Lx and the right translation Rx by Lx(y) = xy, Rx(y) = yx. Then Q is a loop if all translations are bijections of Q, and if Q possesses a neutral element 1 satisfying 1x = x = x1 for every x ∈ Q. A loop Q is Moufang if it satisfies the Moufang identity (xy)(zx)= x((yz)x). Although Moufang loops are not associative in general, they have many properties we are familiar with from the theory of groups. For instance, every element x of a Moufang loop is arXiv:1509.05700v1 [math.GR] 18 Sep 2015 paired with its inverse x−1 satisfying x−1(xy)= y = (yx)x−1, any two elements generate a subgroup (this property is called diassociativity), and any three elements that associate generate a subgroup (the famous Moufang theorem). -
On Malcev Algebras Nilpotent by Lie Center and Corresponding Analytic Moufang Loops
On Malcev algebras nilpotent by Lie center and corresponding analytic Moufang loops. Alexander Grishkov, Marina Rasskazova, Liudmila Sabinina, Mohamed Salim May, 2020 Abstract In this note we describe the structure of finite dimensional Malcev al- gebras over a field of real numbers R, which are nilpotent module its Lie center. It is proved that the corresponding analytic global Moufang loops are nilpotent module their nucleus. Key words: Malcev algebras, Moufang loops, Global Moufang loops. 2010 Mathematics Subject Classification: 17D10, 20N05. 1 Introduction The theory of analytic loops started with the work of A.I. Malcev in [Ma1]. In this article, the correspondence between the analytic local diassociative loops and the binary Lie algebras was established. A loop is a set M, endowed with a binary operation M × M → M, with the neutral element e ∈ M and the condition that the equations ax = b,ya = b for all a,b ∈ M have a unique solution. A loop is called diassociative, if every two elements of this loop generate a subgroup. Malcev showed that for an analytic loop, with the Moufang identity: (xy)(zx) = x(yz)x the corresponding tangent algebra satisfies the following identities: 2 arXiv:2005.07331v1 [math.RA] 15 May 2020 x = [J(x,y,z), x] − J(x, y, [x, z]) = 0, where J(x,y,z) = [[x, y],z] + [[x, z], x] + [[z, x],y] (See [1]). Algebras with these defining identities are currently called Malcev algebras. The more difficult ques- tion, if every finite dimensional Malcev R-algebra is the tangent algebra of some local analytic Moufang loop was solved positively by E.Kuzmin in 1969 in [Kuzm2].