Braided Compact Closed Categories with Applications to Low Dimensional Topology

Total Page:16

File Type:pdf, Size:1020Kb

Braided Compact Closed Categories with Applications to Low Dimensional Topology CORE Metadata, citation and similar papers at core.ac.uk Provided by Elsevier - Publisher Connector A,,VANCEi IN MATHEMATICS 77. 156-182 (1989) Braided Compact Closed Categories with Applications to Low Dimensional Topology PETER J. FREYD Departmcnr of Mathematics, Universir~ q/ Penns.~lvania, Philadelphia. Penns?;lvania 19104 AND DAVID N. YETTER Department qf Maihematics and Statisfics, McGii/ University. Montreal, Quebec. Canada H3A 2K6 INTRODUCTION The discovery by Jones [4] of a new isotopy invariant of classical links, and its subsequent generalizations [3, 7a, 7b, 7c], has lead to renewed interest in algebraic representations of knotting and linking. Prompted by this, Yetter [16] analysed the structure of “categories of tangles” to give a combinatorial description of composition of generalized tangles. In that work a great simplification was achieved by using a monoidal structure on the categories considered. As we shall see, the assumption in [ 161 that links (or more generally “Markov classes”) arise by the imposition of extrinsic structure (i.e., Markov moves) is unnecessary when the full categorical structure (including the correct generalization of compact closedness to the non-symmetric case) is understood, an observa- tion first made by Freyd [a]. This observation leads to a clear representa- tion-theoretic view of the new link invariants and, when coupled with the encoding of framings by a modified diagrammatic “isotopy” rather than the labels used in [ 161, to an “algebraicized” Kirby calculus from which it is actually possible to calculate invariants of 3-manifolds from their surgery presentation. In a parallel development, Joyal and Street [IS, 141 have considered “braidings” in the context of monoidal category theory: a “braiding” is a natural family of maps a/,,:A@B+B@A satisfying all the usual properties for a symmetry in monoidal category 156 cml-8708/89 $7.50 CopyrIght r!, 1989 by Academic Press. Inc. All rights of reproduction in any form reserved BRAIDED COMPACTCLOSED CATEGORIES 157 theory including the invertibility of the components, but excluding the usual requirement g.4.B”B.A --1 ,408. The first connection between braided categories and topology is given by Joyal and Street’s characterization of the free (strict) braided monoidal category as the category of geometric braids. We are indebted to them for the influence of their work and numerous helpful suggestions. 1. DEFINITIONS AND LEMMAS FROM CATEGORY THEORY We begin by recalling some notions from the theory of monoidal categories: DEFINITION 1.1. A nzonoidal category’ V = (V, 0, Z, CI,p, i) consists of a category V, a functor @ : V x V + V (written in infix notation), and natural isomorphisms c(~,~,~.:(A@B)@C+A@(B@C), p,,:A@Z-+A, and A,,: I@ A + A such that Ml M2 (A@Z)@BA A@(Z@B) A@B V is strict if all components of ~1,p. and 2 are identity maps. Much of the following will be simplified by the fact that the monoidal categories arising from topological considerations are strict, and by the coherence theorem of MacLane [ 121, by which any monoidal category is equivalent to a strict monoidal category. That is, one may safely assume that all monoidal categories are strict. 158 FREYD AND YETTER Following Joyal and Street [S] we make DEFINITION 1.2. A braiding in a monoidal category is a natural isomorphism satisfying Bl AO(BOC) A (B@C)OA % 2 / \ (AOB)OC BO(COA) O@C B@O \ / (BOA)@C--, B@(AOC) B2 (A@B)@CA CO(AOB) A@(C@B)- (AOC)OB 3-1 For the “correct” generalization of compact closed categories to the non-symmetric case, we take the following partially restricted version of the notion of pivotal category (see Joyal and Street [.5] for the relaxed version 1. DEFINITION 1.3. A (strict) pivotal category is a monoidal category, V, equipped with a (strict) anti-involution of monoidal categories (-)* (i.e., a contravariant functor, satisfying moreover (fog)* =g* of*, I= I*, and (()** = Id,), and a family of maps satisfying BRAIDED COMPACT CLOSED CATEGORIES 159 Pl (AOB)O(B*OA*) x .4@(B@(B*@A*))3=+ AO((BOB*)OA*) P2 and, letting qA = (Ed*)*, P3 Ll* PA* i / B*OI I@A* Epc3.4’ / B*@(A@A*)w B*@“@A*) B*@(B@A*) * ’ + (B*@B)OA* We then have LEMMA 1.4. A pivotal category is closed in the sense that for all objects B, the finctor - @ B has a right adjoint Hom( B, --). 160 FREYD AND YETTER Proof: Let Hom( B, -) = ~ @ B*. The component of the unit (resp. counit) for the adjunction at an object A is then A @qe (resp. A@E~). All necessary verifications follow routinely from P3 and are left to the reader. The following definition and lemma (found in Kelly and Laplaza [9] for the symmetric compact closed case) are crucial to the applications of pivotal categories in low dimensional topology: DEFINITION 1.5. The trace of an endomorphism f: A + A in a pivotal category is the endomorphism of Z given by the formula LEMMA 1.6. In any pivotal category, the trace satisfies Wg) = trkf) whenever f: A -P B and g : B -+ A for anq’ objects A and B. The reader will note that this trace is preserved by monoidal functors which preserve (-)* and E (henceforth called piootal.functors), and that if the pivotal category is additive, then this is a trace in the ordinary sense, taking values in the ring End(I). 2. DEFINITIONS AND LEMMAS FROM CLASSICAL KNOT THEORY Throughout, we work in the piecewise-linear category, except where it is necessary to pass to the smooth category to discuss framings of the normal bundle, and we assume that S3 is endowed with a fixed orientation. We recall the standard reduction of ambient isotopy of piecewise-linear links in S3 to combinatorial moves on regular projections with specified crossing and orientation data (i.e., Knot diagrams) given in Reidemeister [ 133 (see also Burde and Zieschang [ 1 ] for a good exposition): DEFINITION 2.1. A link diagram is a projection of a link in [w3 onto a plane (if we wish we may choose a copy of S’ in S” and project stereographically from any point on it but not on the link) such that the resulting curve has only isolated doubie points with transverse intersection as singularities, together with a choice at each double point of which line is the overcrossing (and, if the link is oriented, the orientation inherited from the link). BRAIDED COMPACT CLOSED CATEGORIES 161 THEOREM 2. (Reidemeister). TLVOlinks are ambient isotopic !f and only ij the}2 have knot diagrams ,rJlich are equivalent under Q.0 Isotopies of the plane qf projection Q.l -\ / i \ f) > ‘Ib / 52.3 Furthermore, isotopies of the projection can he replaced with moves of the f orms A.nl 162 FREYD AND YETTER A.n.2 A-A\ / By abuse of language we will say that two diagrams related by the moves of the previous proposition are isotopic. It is also necessary, following Kauffman, to make DEFINITION 2.3. Two knot diagrams are regulurlv isotopic if they are equivalent under moves 52.2, 0.3, Axl, and A.7c.2 (no Q.l!). Finally, we make DEFINITION 2.4. A tangle is a portion of a knot diagram contained in a rectangle, and incident with the boundary only on the top and bottom edges, where it intersects transversely. We say that two tangles are equal if there is an isotopy of the plane carrying one to the other in such a way that corresponding edges of the rectangle are preserved setwise. 3. CATEGORIES OF TANGLES We begin with an omnibus definition: DEFINITION 3.1. The category of oriented tangles up to regular isotopy (resp. oriented tangles up to isotopy; unoriented tangles up to regular isotopy; unoriented tangles up to isotopy; S-colored oriented tangles up to regular isotopy; . ..). denoted IwOUanrmg (resp. OUarmg; RUaung; Tauug; S-ROTaung; . ..). is the category whose objects are words on the symbols ( 1, 7 } (resp. words on the symbols ( 1, r }; natural numbers; natural numbers; words on the symbols ( 1, 7 ) x S; . ..) and whose maps are named by oriented tangles (resp. oriented tangles; unoriented tangles; BRAIDED COMPACT CLOSED CATEGORIES 163 unoriented tangles; oriented tangles each arc of which is assigned a “color” from the set S; . ..) with two tangles naming the same map if they are regularly isotopic (resp. isotopic; regularly isotopic; isotopic; regularly isotopic with no color changes permitted; . ..). The source/target of a tangle is the word of local orientations for (resp. word of local orientations for; number of points in; number of points in; word of local orientations and colors for; . ..) the intersection with the top/bottom of the bounding rec- tangle. In all cases composition is made by matching top and bottom of tangles. Moreover, each of the categories has a strict monoidal structure in which the map f@g is obtained by matching the right edge of a repre- sentative off‘with the left edge of a representative of g, the identity object being the empty word (resp. the empty word: 0; 0; the empty word: ...). The composition and monoidal structure are illustrated in the following scheme: 1 164 FREYD AND YETTER THEOREM 3.2. ROTmng (resp. OTaung; IRTaong; Taq; S-Rolfarm~; ...) has a braiding, o, in which (T,~,~is given by passing the strands of A over the strands of B. Proof. The proof is essentially the same as that given in the case of the braid category, EL, in Joyal and Street [5]; as was dune there, we give pictorial proof: For naturality: X Y ‘Y 7 ‘X = Y X 9 f A W z and for BI: X Y z X Y 2 7‘Y ‘X 1, \v ‘x/ Y X 2 \f!J ‘Y 1, lb r lyj/4jf( \ h\Y 2 X Y z X (this latter is idential to the case of B), B2 being similar.
Recommended publications
  • Two Constructions in Monoidal Categories Equivariantly Extended Drinfel’D Centers and Partially Dualized Hopf Algebras
    Two constructions in monoidal categories Equivariantly extended Drinfel'd Centers and Partially dualized Hopf Algebras Dissertation zur Erlangung des Doktorgrades an der Fakult¨atf¨urMathematik, Informatik und Naturwissenschaften Fachbereich Mathematik der Universit¨atHamburg vorgelegt von Alexander Barvels Hamburg, 2014 Tag der Disputation: 02.07.2014 Folgende Gutachter empfehlen die Annahme der Dissertation: Prof. Dr. Christoph Schweigert und Prof. Dr. Sonia Natale Contents Introduction iii Topological field theories and generalizations . iii Extending braided categories . vii Algebraic structures and monoidal categories . ix Outline . .x 1. Algebra in monoidal categories 1 1.1. Conventions and notations . .1 1.2. Categories of modules . .3 1.3. Bialgebras and Hopf algebras . 12 2. Yetter-Drinfel'd modules 25 2.1. Definitions . 25 2.2. Equivalences of Yetter-Drinfel'd categories . 31 3. Graded categories and group actions 39 3.1. Graded categories and (co)graded bialgebras . 39 3.2. Weak group actions . 41 3.3. Equivariant categories and braidings . 48 4. Equivariant Drinfel'd center 51 4.1. Half-braidings . 51 4.2. The main construction . 55 4.3. The Hopf algebra case . 61 5. Partial dualization of Hopf algebras 71 5.1. Radford biproduct and projection theorem . 71 5.2. The partial dual . 73 5.3. Examples . 75 A. Category theory 89 A.1. Basic notions . 89 A.2. Adjunctions and monads . 91 i ii Contents A.3. Monoidal categories . 92 A.4. Modular categories . 97 References 99 Introduction The fruitful interplay between topology and algebra has a long tradi- tion. On one hand, invariants of topological spaces, such as the homotopy groups, homology groups, etc.
    [Show full text]
  • Categorical Proof of Holomorphic Atiyah-Bott Formula
    Categorical proof of Holomorphic Atiyah-Bott formula Grigory Kondyrev, Artem Prikhodko Abstract Given a 2-commutative diagram FX X / X ϕ ϕ Y / Y FY in a symmetric monoidal (∞, 2)-category E where X, Y ∈ E are dualizable objects and ϕ admits a right adjoint we construct a natural morphism TrE(FX ) / TrE(FY ) between the traces of FX and FY respectively. We then apply this formalism to the case when E is the (∞, 2)-category of k-linear presentable categories which in combination of various calculations in the setting of derived algebraic geometry gives a categorical proof of the classical Atiyah-Bott formula (also known as the Holomorphic Lefschetz fixed point formula). Contents 1 Dualizable objects and traces 4 1.1 Traces in symmetric monoidal (∞, 1)-categories .. .. .. .. .. .. .. 4 1.2 Traces in symmetric monoidal (∞, 2)-categories .. .. .. .. .. .. .. 5 2 Traces in algebraic geometry 11 2.1 Duality for Quasi-Coherent sheaves . .............. 11 2.2 Calculatingthetrace. .. .. .. .. .. .. .. .. .......... 13 3 Holomorphic Atiyah-Bott formula 16 3.1 Statement of Atiyah-Bott formula . ............ 17 3.2 ProofofAtiyah-Bottformula . ........... 19 arXiv:1607.06345v3 [math.AG] 12 Nov 2019 Introduction The well-known Lefschetz fixed point theorem [Lef26, Formula 71.1] states that for a compact manifold f M and an endomorphism M / M with isolated fixed points there is an equality 2dim M i ∗ L(f) := (−1) tr(f|Hi(X,Q))= degx(1 − f) (1) Xi=0 x=Xf(x) The formula (1) made huge impact on algebraic geometry in 20th century leading Grothendieck and co- authors to development of ´etale cohomology theory and their spectacular proof of Weil’s conjectures.
    [Show full text]
  • PULLBACK and BASE CHANGE Contents
    PART II.2. THE !-PULLBACK AND BASE CHANGE Contents Introduction 1 1. Factorizations of morphisms of DG schemes 2 1.1. Colimits of closed embeddings 2 1.2. The closure 4 1.3. Transitivity of closure 5 2. IndCoh as a functor from the category of correspondences 6 2.1. The category of correspondences 6 2.2. Proof of Proposition 2.1.6 7 3. The functor of !-pullback 8 3.1. Definition of the functor 9 3.2. Some properties 10 3.3. h-descent 10 3.4. Extension to prestacks 11 4. The multiplicative structure and duality 13 4.1. IndCoh as a symmetric monoidal functor 13 4.2. Duality 14 5. Convolution monoidal categories and algebras 17 5.1. Convolution monoidal categories 17 5.2. Convolution algebras 18 5.3. The pull-push monad 19 5.4. Action on a map 20 References 21 Introduction Date: September 30, 2013. 1 2 THE !-PULLBACK AND BASE CHANGE 1. Factorizations of morphisms of DG schemes In this section we will study what happens to the notion of the closure of the image of a morphism between schemes in derived algebraic geometry. The upshot is that there is essentially \nothing new" as compared to the classical case. 1.1. Colimits of closed embeddings. In this subsection we will show that colimits exist and are well-behaved in the category of closed subschemes of a given ambient scheme. 1.1.1. Recall that a map X ! Y in Sch is called a closed embedding if the map clX ! clY is a closed embedding of classical schemes.
    [Show full text]
  • On Framings of Knots in 3-Manifolds
    ON FRAMINGS OF KNOTS IN 3-MANIFOLDS RHEA PALAK BAKSHI, DIONNE IBARRA, GABRIEL MONTOYA-VEGA, JÓZEF H. PRZYTYCKI, AND DEBORAH WEEKS Abstract. We show that the only way of changing the framing of a knot or a link by ambient isotopy in an oriented 3-manifold is when the manifold has a properly embedded non-separating S2. This change of framing is given by the Dirac trick, also known as the light bulb trick. The main tool we use is based on McCullough’s work on the mapping class groups of 3-manifolds. We also relate our results to the theory of skein modules. Contents 1. Introduction1 1.1. History of the problem2 2. Preliminaries3 3. Main Results4 3.1. Proofs of the Main Theorems5 3.2. Spin structures and framings7 4. Ramications and Connections to Skein Modules8 4.1. From the Kauman bracket skein module to spin twisted homology9 4.2. The q-homology skein module9 5. Future Directions 10 6. Acknowledgements 11 References 11 1. Introduction We show that the only way to change the framing of a knot in an oriented 3-manifold by ambient isotopy is when the manifold has a properly embedded non-separating S2. More precisely the only change of framing is by the light bulb trick as illustrated in the Figure1. Here the change arXiv:2001.07782v1 [math.GT] 21 Jan 2020 of framing is very local (takes part in S2 × »0; 1¼ embedded in the manifold) and is related to the fact that the fundamental group of SO¹3º is Z2. Furthermore, we use the fact that 3-manifolds possess spin structures given by the parallelization of their tangent bundles.
    [Show full text]
  • Most Human Things Go in Pairs. Alcmaeon, ∼ 450 BC
    Most human things go in pairs. Alcmaeon, 450 BC ∼ true false good bad right left up down front back future past light dark hot cold matter antimatter boson fermion How can we formalize a general concept of duality? The Chinese tried yin-yang theory, which inspired Leibniz to develop binary notation, which in turn underlies digital computation! But what's the state of the art now? In category theory the fundamental duality is the act of reversing an arrow: • ! • • • We use this to model switching past and future, false and true, small and big... Every category has an opposite op, where the arrows are C C reversed. This is a symmetry of the category of categories: op : Cat Cat ! and indeed the only nontrivial one: Aut(Cat) = Z=2 In logic, the simplest duality is negation. It's order-reversing: if P implies Q then Q implies P : : and|ignoring intuitionism!|it's an involution: P = P :: Thus if is a category of propositions and proofs, we C expect a functor: : op : C ! C with a natural isomorphism: 2 = 1 : ∼ C This has two analogues in quantum theory. One shows up already in the category of finite-dimensional vector spaces, FinVect. Every vector space V has a dual V ∗. Taking the dual is contravariant: if f : V W then f : W V ! ∗ ∗ ! ∗ and|ignoring infinite-dimensional spaces!|it's an involution: V ∗∗ ∼= V This kind of duality is captured by the idea of a -autonomous ∗ category. Recall that a symmetric monoidal category is roughly a category with a unit object I and a tensor product C 2 C : ⊗ C × C ! C that is unital, associative and commutative up to coherent natural isomorphisms.
    [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]
  • Actions of Mapping Class Groups Athanase Papadopoulos
    Actions of mapping class groups Athanase Papadopoulos To cite this version: Athanase Papadopoulos. Actions of mapping class groups. L. Ji, A. Papadopoulos and S.-T. Yau. Handbook of Group Actions, Vol. I, 31, Higher Education Press; International Press, p. 189-248., 2014, Advanced Lectures in Mathematics, 978-7-04-041363-2. hal-01027411 HAL Id: hal-01027411 https://hal.archives-ouvertes.fr/hal-01027411 Submitted on 21 Jul 2014 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. ACTIONS OF MAPPING CLASS GROUPS ATHANASE PAPADOPOULOS Abstract. This paper has three parts. The first part is a general introduction to rigidity and to rigid actions of mapping class group actions on various spaces. In the second part, we describe in detail four rigidity results that concern actions of mapping class groups on spaces of foliations and of laminations, namely, Thurston’s sphere of projective foliations equipped with its projective piecewise-linear structure, the space of unmeasured foliations equipped with the quotient topology, the reduced Bers boundary, and the space of geodesic laminations equipped with the Thurston topology. In the third part, we present some perspectives and open problems on other actions of mapping class groups.
    [Show full text]
  • Categories with Fuzzy Sets and Relations
    Categories with Fuzzy Sets and Relations John Harding, Carol Walker, Elbert Walker Department of Mathematical Sciences New Mexico State University Las Cruces, NM 88003, USA jhardingfhardy,[email protected] Abstract We define a 2-category whose objects are fuzzy sets and whose maps are relations subject to certain natural conditions. We enrich this category with additional monoidal and involutive structure coming from t-norms and negations on the unit interval. We develop the basic properties of this category and consider its relation to other familiar categories. A discussion is made of extending these results to the setting of type-2 fuzzy sets. 1 Introduction A fuzzy set is a map A : X ! I from a set X to the unit interval I. Several authors [2, 6, 7, 20, 22] have considered fuzzy sets as a category, which we will call FSet, where a morphism from A : X ! I to B : Y ! I is a function f : X ! Y that satisfies A(x) ≤ (B◦f)(x) for each x 2 X. Here we continue this path of investigation. The underlying idea is to lift additional structure from the unit interval, such as t-norms, t-conorms, and negations, to provide additional structure on the category. Our eventual aim is to provide a setting where processes used in fuzzy control can be abstractly studied, much in the spirit of recent categorical approaches to processes used in quantum computation [1]. Order preserving structure on I, such as t-norms and conorms, lifts to provide additional covariant structure on FSet. In fact, each t-norm T lifts to provide a symmetric monoidal tensor ⊗T on FSet.
    [Show full text]
  • Arxiv:1701.03895V2 [Math.QA] 24 Feb 2018 Indeed Classifies Fully Extended Oriented 2-Dimensional Tqfts Valued in Alg2
    ZMP-HH/16-29 Hamburger Beiträge zur Mathematik Nr. 636 THE SERRE AUTOMORPHISM VIA HOMOTOPY ACTIONS AND THE COBORDISM HYPOTHESIS FOR ORIENTED MANIFOLDS JAN HESSE AND ALESSANDRO VALENTINO Abstract. We explicitly construct an SO(2)-action on a skeletal version of the 2-dimensional framed bordism bicategory. By the 2-dimensional Cobordism Hypothesis for framed manifolds, we obtain an SO(2)-action on the core of fully-dualizable objects of the target bicategory. This action is shown to coincide with the one given by the Serre automorphism. We give an explicit description of the bicategory of homotopy fixed points of this action, and discuss its relation to the classification of oriented 2d topological quantum field theories. 1. Introduction As defined by Atiyah in [Ati88] and Segal in [Seg04], an n-dimensional Topological Quantum Field Theory (TQFT) consists of a functor between two symmetric monoidal categories, namely a category of n-cobordisms, and a category of algebraic objects. This definition was introduced to axiomatize the locality properties of the path integral, and has given rise to a fruitful interplay between mathematics and physics in the last 30 years. A prominent example is given by a quantum-field-theoretic interpretation of the Jones polynomial by Witten in [Wit89]. More recently, there has been a renewed interest in the study of TQFTs, due in great part to the Baez- Dolan Cobordism Hypothesis and its proof by Lurie, whose main objects of investigation are fully extended TQFTs. These are a generalization of the notion of n-dimensional TQFTs, where data is assigned to manifolds of codimension up to n.
    [Show full text]
  • Problems in Low-Dimensional Topology
    Problems in Low-Dimensional Topology Edited by Rob Kirby Berkeley - 22 Dec 95 Contents 1 Knot Theory 7 2 Surfaces 85 3 3-Manifolds 97 4 4-Manifolds 179 5 Miscellany 259 Index of Conjectures 282 Index 284 Old Problem Lists 294 Bibliography 301 1 2 CONTENTS Introduction In April, 1977 when my first problem list [38,Kirby,1978] was finished, a good topologist could reasonably hope to understand the main topics in all of low dimensional topology. But at that time Bill Thurston was already starting to greatly influence the study of 2- and 3-manifolds through the introduction of geometry, especially hyperbolic. Four years later in September, 1981, Mike Freedman turned a subject, topological 4-manifolds, in which we expected no progress for years, into a subject in which it seemed we knew everything. A few months later in spring 1982, Simon Donaldson brought gauge theory to 4-manifolds with the first of a remarkable string of theorems showing that smooth 4-manifolds which might not exist or might not be diffeomorphic, in fact, didn’t and weren’t. Exotic R4’s, the strangest of smooth manifolds, followed. And then in late spring 1984, Vaughan Jones brought us the Jones polynomial and later Witten a host of other topological quantum field theories (TQFT’s). Physics has had for at least two decades a remarkable record for guiding mathematicians to remarkable mathematics (Seiberg–Witten gauge theory, new in October, 1994, is the latest example). Lest one think that progress was only made using non-topological techniques, note that Freedman’s work, and other results like knot complements determining knots (Gordon- Luecke) or the Seifert fibered space conjecture (Mess, Scott, Gabai, Casson & Jungreis) were all or mostly classical topology.
    [Show full text]
  • Arxiv:1608.05905V3 [Math.CT] 1 Sep 2018 Ti Neetn N Motn Oko Hnatno Aeoyadmit Category Tensor a When Know to Important and Structure
    PIVOTAL STRUCTURES OF THE DRINFELD CENTER OF A FINITE TENSOR CATEGORY KENICHI SHIMIZU Abstract. We classify the pivotal structures of the Drinfeld center Z(C) of a finite tensor category C. As a consequence, every pivotal structure of Z(C) can be obtained from a pair (β,j) consisting of an invertible object β of C and an isomorphism j : β ⊗ (−) ⊗ β∗ → (−)∗∗ of monoidal functors. 1. Introduction Throughout this paper, we work over an algebraically closed field k of arbi- trary characteristic. By a tensor category over k, we mean a k-linear abelian rigid monoidal category satisfying natural conditions [EGNO15]. The rigidity means that every object X in a tensor category has a well-behaved dual object X∗. Al- though the dual object generalizes the contragradient representation in the group representation theory, the ‘double dual’ object X∗∗ is no longer isomorphic to X in general. The assignment X 7→ X∗∗ extends to a tensor autoequivalence on C. ∗∗ A pivotal structure of a tensor category is an isomorphism idC → (−) of tensor functors. Such an isomorphism does not exist in general, however, we often re- quire a pivotal structure in some applications of tensor categories to, for example, representation theory, low-dimensional topology, and conformal field theory. Thus it is interesting and important to know when a tensor category admits a pivotal structure. A finite tensor category [EO04] is a tensor category satisfying a certain finiteness condition. In this paper, we classify the pivotal structures of the Drinfeld center of a finite tensor category. To state our main result, we introduce some notations: Let C be a finite tensor category, and let Z(C) denote the Drinfeld center of C.
    [Show full text]
  • A Diagrammatic Presentation and Its Characterization of Non-Split Compact Surfaces in the 3-Sphere
    A DIAGRAMMATIC PRESENTATION AND ITS CHARACTERIZATION OF NON-SPLIT COMPACT SURFACES IN THE 3-SPHERE SHOSAKU MATSUZAKI Abstract. We give a presentation for a non-split compact surface embedded in the 3-sphere S3 by using diagrams of spatial trivalent graphs equipped with signs and we define Reidemeister moves for such signed diagrams. We show that two diagrams of embedded surfaces are related by Reidemeister moves if and only if the surfaces represented by the diagrams are ambient isotopic in S3. 1. Introduction A fundamental problem in Knot Theory is to classify knots and links up to ambient isotopy in S3. Two knots are equivalent if and only if diagrams of them are related by Reidemeister moves [7]: Reidemeister moves characterize a combinatorial structure of knots. Diagrammatic characterizations for spatial graphs, handlebody-knots and surface-knots are also known, where a spatial graph is a graph in S3, a handlebody-knot is a handlebody in S3, and a surface-knot is a closed surface in S4 (cf. [4], [5], [8]). We often use invariants to distinguish the above knots. Many invariants have been discovered on the basis of diagrammatic characterizations. In this paper, we consider presentation of a compact surface embedded in S3, which we call a spatial surface. For a knot or link, we immediately obtain its diagram by perturbing the z-axis of projection slightly. For a spatial surface, however, perturbing the spatial surface is not enough to present it in a useful form: it may be overlapped and folded complexly by multiple layers in the direction of the z-axis of R3 ⊂ S3.
    [Show full text]