HOMEOMORPHISMS of 3-MANIFOLDS and the REALIZATION of NIELSEN NUMBER Boju Jiang1, Shicheng Wang1,2, and Ying-Qing Wu2 §0. Introd
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The Birman-Hilden Theory
THE BIRMAN{HILDEN THEORY DAN MARGALIT AND REBECCA R. WINARSKI Abstract. In the 1970s Joan Birman and Hugh Hilden wrote several papers on the problem of relating the mapping class group of a surface to that of a cover. We survey their work, give an overview of the subsequent developments, and discuss open questions and new directions. 1. Introduction In the early 1970s Joan Birman and Hugh Hilden wrote a series of now- classic papers on the interplay between mapping class groups and covering spaces. The initial goal was to determine a presentation for the mapping class group of S2, the closed surface of genus two (it was not until the late 1970s that Hatcher and Thurston [33] developed an approach for finding explicit presentations for mapping class groups). The key innovation by Birman and Hilden is to relate the mapping class group Mod(S2) to the mapping class group of S0;6, a sphere with six marked points. Presentations for Mod(S0;6) were already known since that group is closely related to a braid group. The two surfaces S2 and S0;6 are related by a two-fold branched covering map S2 ! S0;6: arXiv:1703.03448v1 [math.GT] 9 Mar 2017 The six marked points in the base are branch points. The deck transforma- tion is called the hyperelliptic involution of S2, and we denote it by ι. Every element of Mod(S2) has a representative that commutes with ι, and so it follows that there is a map Θ : Mod(S2) ! Mod(S0;6): The kernel of Θ is the cyclic group of order two generated by (the homotopy class of) the involution ι. -
Picard Groupoids and $\Gamma $-Categories
PICARD GROUPOIDS AND Γ-CATEGORIES AMIT SHARMA Abstract. In this paper we construct a symmetric monoidal closed model category of coherently commutative Picard groupoids. We construct another model category structure on the category of (small) permutative categories whose fibrant objects are (permutative) Picard groupoids. The main result is that the Segal’s nerve functor induces a Quillen equivalence between the two aforementioned model categories. Our main result implies the classical result that Picard groupoids model stable homotopy one-types. Contents 1. Introduction 2 2. The Setup 4 2.1. Review of Permutative categories 4 2.2. Review of Γ- categories 6 2.3. The model category structure of groupoids on Cat 7 3. Two model category structures on Perm 12 3.1. ThemodelcategorystructureofPermutativegroupoids 12 3.2. ThemodelcategoryofPicardgroupoids 15 4. The model category of coherently commutatve monoidal groupoids 20 4.1. The model category of coherently commutative monoidal groupoids 24 5. Coherently commutative Picard groupoids 27 6. The Quillen equivalences 30 7. Stable homotopy one-types 36 Appendix A. Some constructions on categories 40 AppendixB. Monoidalmodelcategories 42 Appendix C. Localization in model categories 43 Appendix D. Tranfer model structure on locally presentable categories 46 References 47 arXiv:2002.05811v2 [math.CT] 12 Mar 2020 Date: Dec. 14, 2019. 1 2 A. SHARMA 1. Introduction Picard groupoids are interesting objects both in topology and algebra. A major reason for interest in topology is because they classify stable homotopy 1-types which is a classical result appearing in various parts of the literature [JO12][Pat12][GK11]. The category of Picard groupoids is the archetype exam- ple of a 2-Abelian category, see [Dup08]. -
3-Manifold Groups
3-Manifold Groups Matthias Aschenbrenner Stefan Friedl Henry Wilton University of California, Los Angeles, California, USA E-mail address: [email protected] Fakultat¨ fur¨ Mathematik, Universitat¨ Regensburg, Germany E-mail address: [email protected] Department of Pure Mathematics and Mathematical Statistics, Cam- bridge University, United Kingdom E-mail address: [email protected] Abstract. We summarize properties of 3-manifold groups, with a particular focus on the consequences of the recent results of Ian Agol, Jeremy Kahn, Vladimir Markovic and Dani Wise. Contents Introduction 1 Chapter 1. Decomposition Theorems 7 1.1. Topological and smooth 3-manifolds 7 1.2. The Prime Decomposition Theorem 8 1.3. The Loop Theorem and the Sphere Theorem 9 1.4. Preliminary observations about 3-manifold groups 10 1.5. Seifert fibered manifolds 11 1.6. The JSJ-Decomposition Theorem 14 1.7. The Geometrization Theorem 16 1.8. Geometric 3-manifolds 20 1.9. The Geometric Decomposition Theorem 21 1.10. The Geometrization Theorem for fibered 3-manifolds 24 1.11. 3-manifolds with (virtually) solvable fundamental group 26 Chapter 2. The Classification of 3-Manifolds by their Fundamental Groups 29 2.1. Closed 3-manifolds and fundamental groups 29 2.2. Peripheral structures and 3-manifolds with boundary 31 2.3. Submanifolds and subgroups 32 2.4. Properties of 3-manifolds and their fundamental groups 32 2.5. Centralizers 35 Chapter 3. 3-manifold groups after Geometrization 41 3.1. Definitions and conventions 42 3.2. Justifications 45 3.3. Additional results and implications 59 Chapter 4. The Work of Agol, Kahn{Markovic, and Wise 63 4.1. -
Floer Homology, Gauge Theory, and Low-Dimensional Topology
Floer Homology, Gauge Theory, and Low-Dimensional Topology Clay Mathematics Proceedings Volume 5 Floer Homology, Gauge Theory, and Low-Dimensional Topology Proceedings of the Clay Mathematics Institute 2004 Summer School Alfréd Rényi Institute of Mathematics Budapest, Hungary June 5–26, 2004 David A. Ellwood Peter S. Ozsváth András I. Stipsicz Zoltán Szabó Editors American Mathematical Society Clay Mathematics Institute 2000 Mathematics Subject Classification. Primary 57R17, 57R55, 57R57, 57R58, 53D05, 53D40, 57M27, 14J26. The cover illustrates a Kinoshita-Terasaka knot (a knot with trivial Alexander polyno- mial), and two Kauffman states. These states represent the two generators of the Heegaard Floer homology of the knot in its topmost filtration level. The fact that these elements are homologically non-trivial can be used to show that the Seifert genus of this knot is two, a result first proved by David Gabai. Library of Congress Cataloging-in-Publication Data Clay Mathematics Institute. Summer School (2004 : Budapest, Hungary) Floer homology, gauge theory, and low-dimensional topology : proceedings of the Clay Mathe- matics Institute 2004 Summer School, Alfr´ed R´enyi Institute of Mathematics, Budapest, Hungary, June 5–26, 2004 / David A. Ellwood ...[et al.], editors. p. cm. — (Clay mathematics proceedings, ISSN 1534-6455 ; v. 5) ISBN 0-8218-3845-8 (alk. paper) 1. Low-dimensional topology—Congresses. 2. Symplectic geometry—Congresses. 3. Homol- ogy theory—Congresses. 4. Gauge fields (Physics)—Congresses. I. Ellwood, D. (David), 1966– II. Title. III. Series. QA612.14.C55 2004 514.22—dc22 2006042815 Copying and reprinting. Material in this book may be reproduced by any means for educa- tional and scientific purposes without fee or permission with the exception of reproduction by ser- vices that collect fees for delivery of documents and provided that the customary acknowledgment of the source is given. -
Homeotopy Groups by G
HOMEOTOPY GROUPS BY G. s. Mccarty, jr. o Introduction. A principal goal in algebraic topology has been to classify and characterize spaces by means of topological invariants. One such is certainly the group G(X) of homeomorphisms of a space X. And, for a large class of spaces X (including manifolds), the compact-open topology is a natural choice for GiX), making it a topological transformation group on X. GiX) is too large and complex for much direct study; however, homotopy invariants of GiX) are not homotopy invariants of X. Thus, the homeotopy groups of X are defined to be the homotopy groups of GiX). The Jf kiX) = 7tt[G(Z)] are topological in- variants of X which are shown (§2) not to be invariant even under isotopy, yet the powerful machinery of homotopy theory is available for their study. In (2) some of the few published results concerning the component group Ji?0iX) = jr0[G(X)] are recounted. This group is then shown to distinguish members of some pairs of homotopic spaces. In (3) the topological group G(X) is given the structure of a fiber bundle over X, with the isotropy group xGiX) at x e X as fiber, for a class of homogeneous spaces X. This structure defines a topologically invariant, exact sequence, Jf^iX). In (4), ¿FJJi) is shown to be defined for manifolds, and this definition is ex- tended to manifolds with boundary. Relations are then derived among the homeo- topy groups of the set of manifolds got by deletion of finite point sets from a compact manifold. -
Commentary on Thurston's Work on Foliations
COMMENTARY ON FOLIATIONS* Quoting Thurston's definition of foliation [F11]. \Given a large supply of some sort of fabric, what kinds of manifolds can be made from it, in a way that the patterns match up along the seams? This is a very general question, which has been studied by diverse means in differential topology and differential geometry. ... A foliation is a manifold made out of striped fabric - with infintely thin stripes, having no space between them. The complete stripes, or leaves, of the foliation are submanifolds; if the leaves have codimension k, the foliation is called a codimension k foliation. In order that a manifold admit a codimension- k foliation, it must have a plane field of dimension (n − k)." Such a foliation is called an (n − k)-dimensional foliation. The first definitive result in the subject, the so called Frobenius integrability theorem [Fr], concerns a necessary and sufficient condition for a plane field to be the tangent field of a foliation. See [Spi] Chapter 6 for a modern treatment. As Frobenius himself notes [Sa], a first proof was given by Deahna [De]. While this work was published in 1840, it took another hundred years before a geometric/topological theory of foliations was introduced. This was pioneered by Ehresmann and Reeb in a series of Comptes Rendus papers starting with [ER] that was quickly followed by Reeb's foundational 1948 thesis [Re1]. See Haefliger [Ha4] for a detailed account of developments in this period. Reeb [Re1] himself notes that the 1-dimensional theory had already undergone considerable development through the work of Poincare [P], Bendixson [Be], Kaplan [Ka] and others. -
Classification of 3-Manifolds with Certain Spines*1 )
TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 205, 1975 CLASSIFICATIONOF 3-MANIFOLDSWITH CERTAIN SPINES*1 ) BY RICHARD S. STEVENS ABSTRACT. Given the group presentation <p= (a, b\ambn, apbq) With m, n, p, q & 0, we construct the corresponding 2-complex Ky. We prove the following theorems. THEOREM 7. Jf isa spine of a closed orientable 3-manifold if and only if (i) \m\ = \p\ = 1 or \n\ = \q\ = 1, or (") (m, p) = (n, q) = 1. Further, if (ii) holds but (i) does not, then the manifold is unique. THEOREM 10. If M is a closed orientable 3-manifold having K^ as a spine and \ = \mq — np\ then M is a lens space L\ % where (\,fc) = 1 except when X = 0 in which case M = S2 X S1. It is well known that every connected compact orientable 3-manifold with or without boundary has a spine that is a 2-complex with a single vertex. Such 2-complexes correspond very naturally to group presentations, the 1-cells corre- sponding to generators and the 2-cells corresponding to relators. In the case of a closed orientable 3-manifold, there are equally many 1-cells and 2-cells in the spine, i.e., equally many generators and relators in the corresponding presentation. Given a group presentation one is motivated to ask the following questions: (1) Is the corresponding 2-complex a spine of a compact orientable 3-manifold? (2) If there are equally many generators and relators, is the 2-complex a spine of a closed orientable 3-manifold? (3) Can we say what manifold(s) have the 2-complex as a spine? L. -
Manifolds: Where Do We Come From? What Are We? Where Are We Going
Manifolds: Where Do We Come From? What Are We? Where Are We Going Misha Gromov September 13, 2010 Contents 1 Ideas and Definitions. 2 2 Homotopies and Obstructions. 4 3 Generic Pullbacks. 9 4 Duality and the Signature. 12 5 The Signature and Bordisms. 25 6 Exotic Spheres. 36 7 Isotopies and Intersections. 39 8 Handles and h-Cobordisms. 46 9 Manifolds under Surgery. 49 1 10 Elliptic Wings and Parabolic Flows. 53 11 Crystals, Liposomes and Drosophila. 58 12 Acknowledgments. 63 13 Bibliography. 63 Abstract Descendants of algebraic kingdoms of high dimensions, enchanted by the magic of Thurston and Donaldson, lost in the whirlpools of the Ricci flow, topologists dream of an ideal land of manifolds { perfect crystals of mathematical structure which would capture our vague mental images of geometric spaces. We browse through the ideas inherited from the past hoping to penetrate through the fog which conceals the future. 1 Ideas and Definitions. We are fascinated by knots and links. Where does this feeling of beauty and mystery come from? To get a glimpse at the answer let us move by 25 million years in time. 25 106 is, roughly, what separates us from orangutans: 12 million years to our common ancestor on the phylogenetic tree and then 12 million years back by another× branch of the tree to the present day orangutans. But are there topologists among orangutans? Yes, there definitely are: many orangutans are good at "proving" the triv- iality of elaborate knots, e.g. they fast master the art of untying boats from their mooring when they fancy taking rides downstream in a river, much to the annoyance of people making these knots with a different purpose in mind. -
Fibrations I
Fibrations I Tyrone Cutler May 23, 2020 Contents 1 Fibrations 1 2 The Mapping Path Space 5 3 Mapping Spaces and Fibrations 9 4 Exercises 11 1 Fibrations In the exercises we used the extension problem to motivate the study of cofibrations. The idea was to allow for homotopy-theoretic methods to be introduced to an otherwise very rigid problem. The dual notion is the lifting problem. Here p : E ! B is a fixed map and we would like to known when a given map f : X ! B lifts through p to a map into E E (1.1) |> | p | | f X / B: Asking for the lift to make the diagram to commute strictly is neither useful nor necessary from our point of view. Rather it is more natural for us to ask that the lift exist up to homotopy. In this lecture we work in the unpointed category and obtain the correct conditions on the map p by formally dualising the conditions for a map to be a cofibration. Definition 1 A map p : E ! B is said to have the homotopy lifting property (HLP) with respect to a space X if for each pair of a map f : X ! E, and a homotopy H : X×I ! B starting at H0 = pf, there exists a homotopy He : X × I ! E such that , 1) He0 = f 2) pHe = H. The map p is said to be a (Hurewicz) fibration if it has the homotopy lifting property with respect to all spaces. 1 Since a diagram is often easier to digest, here is the definition exactly as stated above f X / E x; He x in0 x p (1.2) x x H X × I / B and also in its equivalent adjoint formulation X B H B He B B p∗ EI / BI (1.3) f e0 e0 # p E / B: The assertion that p is a fibration is the statement that the square in the second diagram is a weak pullback. -
Boundary Volume and Length Spectra of Riemannian Manifolds: What the Middle Degree Hodge Spectrum Doesn’T Reveal Tome 53, No 7 (2003), P
R AN IE N R A U L E O S F D T E U L T I ’ I T N S ANNALES DE L’INSTITUT FOURIER Carolyn S. GORDON & Juan Pablo ROSSETTI Boundary volume and length spectra of Riemannian manifolds: what the middle degree Hodge spectrum doesn’t reveal Tome 53, no 7 (2003), p. 2297-2314. <http://aif.cedram.org/item?id=AIF_2003__53_7_2297_0> © Association des Annales de l’institut Fourier, 2003, tous droits réservés. L’accès aux articles de la revue « Annales de l’institut Fourier » (http://aif.cedram.org/), implique l’accord avec les conditions générales d’utilisation (http://aif.cedram.org/legal/). Toute re- production en tout ou partie cet article sous quelque forme que ce soit pour tout usage autre que l’utilisation à fin strictement per- sonnelle du copiste est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. cedram Article mis en ligne dans le cadre du Centre de diffusion des revues académiques de mathématiques http://www.cedram.org/ 2297- BOUNDARY VOLUME AND LENGTH SPECTRA OF RIEMANNIAN MANIFOLDS: WHAT THE MIDDLE DEGREE HODGE SPECTRUM DOESN’T REVEAL by C.S. GORDON and J.P. ROSSETTI (1) To what extent does spectral data associated with the Hodge Laplacian dd* + d*d on a compact Riemannian manifold M determine the geometry and topology of M? Let specp (M) denote the spectrum of the Hodge Laplacian acting on the space of p-forms on M, with absolute boundary conditions in case the boundary of M is non-empty. -
Homotopy Is Not Isotopy for Homeomorphisms of 3-Manifolds
CORE Metadata, citation and similar papers at core.ac.uk Provided by Elsevier - Publisher Connector KMC-9383,86 13.00+ .CO C 1986 Rrgamon Res Ltd. HOMOTOPY IS NOT ISOTOPY FOR HOMEOMORPHISMS OF 3-MANIFOLDS JOHN L. FRIEDMAN? and DONALD M. WIT-I (Received in reuised form 7 May 1985) IXl-RODUCTION THE existence of a homeomorphism that is homotopic but not isotopic to the identity has remained an open question for closed 3-manifolds [I, 23. We consider here homeotopy groups:: of spherical spaces, finding as a by-product of our work an example of such a homeomorphism for a closed 3-manifold whose prime factors include certain spherical spaces. The homeotopy groups of a composite 3-manifold have as subgroups the disk-fixing or point-fixing homeotopy groups of each prime factor [3,4]. In the work reported here our primary aim has been to calculate, for spherical spaces the corresponding 0th homeotopy groups, the groups of path connected components of the spaces of disk-fixing and point- fixing homeomorphisms. Homeomorphism groups of spherical spaces have been considered recently by Rubinstein et al. [S-7]. Asano [8], Bonahon [9] and Ivanov [lo]. Their results are consistent with Hatcher’s conjecture [ 1 l] that for each spherical space the group of homeomorphisms has the same homotopy type as the group of isometries. Homotopy classes of the groups HO and XX of homeomorphisms that fix respectively a disk and a point do not generally have this character (for spherical spaces): in particular, nonzero elements of ~,,(&‘a) and rr,, (XX) are commonly not represented by isometries. -
Notes on Spectral Sequence
Notes on spectral sequence He Wang Long exact sequence coming from short exact sequence of (co)chain com- plex in (co)homology is a fundamental tool for computing (co)homology. Instead of considering short exact sequence coming from pair (X; A), one can consider filtered chain complexes coming from a increasing of subspaces X0 ⊂ X1 ⊂ · · · ⊂ X. We can see it as many pairs (Xp; Xp+1): There is a natural generalization of a long exact sequence, called spectral sequence, which is more complicated and powerful algebraic tool in computation in the (co)homology of the chain complex. Nothing is original in this notes. Contents 1 Homological Algebra 1 1.1 Definition of spectral sequence . 1 1.2 Construction of spectral sequence . 6 2 Spectral sequence in Topology 12 2.1 General method . 12 2.2 Leray-Serre spectral sequence . 15 2.3 Application of Leray-Serre spectral sequence . 18 1 Homological Algebra 1.1 Definition of spectral sequence Definition 1.1. A differential bigraded module over a ring R, is a collec- tion of R-modules, fEp;qg, where p, q 2 Z, together with a R-linear mapping, 1 H.Wang Notes on spectral Sequence 2 d : E∗;∗ ! E∗+s;∗+t, satisfying d◦d = 0: d is called the differential of bidegree (s; t). Definition 1.2. A spectral sequence is a collection of differential bigraded p;q R-modules fEr ; drg, where r = 1; 2; ··· and p;q ∼ p;q ∗;∗ ∼ p;q ∗;∗ ∗;∗ p;q Er+1 = H (Er ) = ker(dr : Er ! Er )=im(dr : Er ! Er ): In practice, we have the differential dr of bidegree (r; 1 − r) (for a spec- tral sequence of cohomology type) or (−r; r − 1) (for a spectral sequence of homology type).