Homeomorphisms Which Are Dehn Twists on the Boundary
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Simple Infinite Presentations for the Mapping Class Group of a Compact
SIMPLE INFINITE PRESENTATIONS FOR THE MAPPING CLASS GROUP OF A COMPACT NON-ORIENTABLE SURFACE RYOMA KOBAYASHI Abstract. Omori and the author [6] have given an infinite presentation for the mapping class group of a compact non-orientable surface. In this paper, we give more simple infinite presentations for this group. 1. Introduction For g ≥ 1 and n ≥ 0, we denote by Ng,n the closure of a surface obtained by removing disjoint n disks from a connected sum of g real projective planes, and call this surface a compact non-orientable surface of genus g with n boundary components. We can regard Ng,n as a surface obtained by attaching g M¨obius bands to g boundary components of a sphere with g + n boundary components, as shown in Figure 1. We call these attached M¨obius bands crosscaps. Figure 1. A model of a non-orientable surface Ng,n. The mapping class group M(Ng,n) of Ng,n is defined as the group consisting of isotopy classes of all diffeomorphisms of Ng,n which fix the boundary point- wise. M(N1,0) and M(N1,1) are trivial (see [2]). Finite presentations for M(N2,0), M(N2,1), M(N3,0) and M(N4,0) ware given by [9], [1], [14] and [16] respectively. Paris-Szepietowski [13] gave a finite presentation of M(Ng,n) with Dehn twists and arXiv:2009.02843v1 [math.GT] 7 Sep 2020 crosscap transpositions for g + n > 3 with n ≤ 1. Stukow [15] gave another finite presentation of M(Ng,n) with Dehn twists and one crosscap slide for g + n > 3 with n ≤ 1, applying Tietze transformations for the presentation of M(Ng,n) given in [13]. -
[Math.GT] 9 Jul 2003
LOW-DIMENSIONAL HOMOLOGY GROUPS OF MAPPING CLASS GROUPS: A SURVEY MUSTAFA KORKMAZ Abstract. In this survey paper, we give a complete list of known re- sults on the first and the second homology groups of surface mapping class groups. Some known results on higher (co)homology are also men- tioned. 1. Introduction n Let Σg,r be a connected orientable surface of genus g with r boundary n components and n punctures. The mapping class group of Σg,r may be defined in different ways. For our purpose, it is defined as the group of the n n isotopy classes of orientation-preserving diffeomorphisms Σg,r → Σg,r. The diffeomorphisms and the isotopies are assumed to fix each puncture and the n points on the boundary. We denote the mapping class group of Σg,r by n Γg,r. Here, we see the punctures on the surface as distinguished points. If r and/or n is zero, then we omit it from the notation. We write Σ for the n surface Σg,r when we do not want to emphasize g,r,n. The theory of mapping class groups plays a central role in low-dimensional n topology. When r = 0 and 2g + n ≥ 3, the mapping class group Γg acts properly discontinuously on the Teichm¨uller space which is homeomorphic to some Euclidean space and the stabilizer of each point is finite. The quotient of the Teichm¨uller space by the action of the mapping class group is the moduli space of complex curves. Recent developments in low-dimensional topology made the algebraic structure of the mapping class group more important. -
Lens Spaces We Introduce Some of the Simplest 3-Manifolds, the Lens Spaces
CHAPTER 10 Seifert manifolds In the previous chapter we have proved various general theorems on three- manifolds, and it is now time to construct examples. A rich and important source is a family of manifolds built by Seifert in the 1930s, which generalises circle bundles over surfaces by admitting some “singular”fibres. The three- manifolds that admit such kind offibration are now called Seifert manifolds. In this chapter we introduce and completely classify (up to diffeomor- phisms) the Seifert manifolds. In Chapter 12 we will then show how to ge- ometrise them, by assigning a nice Riemannian metric to each. We will show, for instance, that all the elliptic andflat three-manifolds are in fact particular kinds of Seifert manifolds. 10.1. Lens spaces We introduce some of the simplest 3-manifolds, the lens spaces. These manifolds (and many more) are easily described using an important three- dimensional construction, called Dehnfilling. 10.1.1. Dehnfilling. If a 3-manifoldM has a spherical boundary com- ponent, we can cap it off with a ball. IfM has a toric boundary component, there is no canonical way to cap it off: the simplest object that we can attach to it is a solid torusD S 1, but the resulting manifold depends on the gluing × map. This operation is called a Dehnfilling and we now study it in detail. LetM be a 3-manifold andT ∂M be a boundary torus component. ⊂ Definition 10.1.1. A Dehnfilling ofM alongT is the operation of gluing a solid torusD S 1 toM via a diffeomorphismϕ:∂D S 1 T. -
Recognizing Surfaces
RECOGNIZING SURFACES Ivo Nikolov and Alexandru I. Suciu Mathematics Department College of Arts and Sciences Northeastern University Abstract The subject of this poster is the interplay between the topology and the combinatorics of surfaces. The main problem of Topology is to classify spaces up to continuous deformations, known as homeomorphisms. Under certain conditions, topological invariants that capture qualitative and quantitative properties of spaces lead to the enumeration of homeomorphism types. Surfaces are some of the simplest, yet most interesting topological objects. The poster focuses on the main topological invariants of two-dimensional manifolds—orientability, number of boundary components, genus, and Euler characteristic—and how these invariants solve the classification problem for compact surfaces. The poster introduces a Java applet that was written in Fall, 1998 as a class project for a Topology I course. It implements an algorithm that determines the homeomorphism type of a closed surface from a combinatorial description as a polygon with edges identified in pairs. The input for the applet is a string of integers, encoding the edge identifications. The output of the applet consists of three topological invariants that completely classify the resulting surface. Topology of Surfaces Topology is the abstraction of certain geometrical ideas, such as continuity and closeness. Roughly speaking, topol- ogy is the exploration of manifolds, and of the properties that remain invariant under continuous, invertible transforma- tions, known as homeomorphisms. The basic problem is to classify manifolds according to homeomorphism type. In higher dimensions, this is an impossible task, but, in low di- mensions, it can be done. Surfaces are some of the simplest, yet most interesting topological objects. -
Calculus Terminology
AP Calculus BC Calculus Terminology Absolute Convergence Asymptote Continued Sum Absolute Maximum Average Rate of Change Continuous Function Absolute Minimum Average Value of a Function Continuously Differentiable Function Absolutely Convergent Axis of Rotation Converge Acceleration Boundary Value Problem Converge Absolutely Alternating Series Bounded Function Converge Conditionally Alternating Series Remainder Bounded Sequence Convergence Tests Alternating Series Test Bounds of Integration Convergent Sequence Analytic Methods Calculus Convergent Series Annulus Cartesian Form Critical Number Antiderivative of a Function Cavalieri’s Principle Critical Point Approximation by Differentials Center of Mass Formula Critical Value Arc Length of a Curve Centroid Curly d Area below a Curve Chain Rule Curve Area between Curves Comparison Test Curve Sketching Area of an Ellipse Concave Cusp Area of a Parabolic Segment Concave Down Cylindrical Shell Method Area under a Curve Concave Up Decreasing Function Area Using Parametric Equations Conditional Convergence Definite Integral Area Using Polar Coordinates Constant Term Definite Integral Rules Degenerate Divergent Series Function Operations Del Operator e Fundamental Theorem of Calculus Deleted Neighborhood Ellipsoid GLB Derivative End Behavior Global Maximum Derivative of a Power Series Essential Discontinuity Global Minimum Derivative Rules Explicit Differentiation Golden Spiral Difference Quotient Explicit Function Graphic Methods Differentiable Exponential Decay Greatest Lower Bound Differential -
THE DISJOINT ANNULUS PROPERTY 1. History And
THE DISJOINT ANNULUS PROPERTY SAUL SCHLEIMER Abstract. A Heegaard splitting of a closed, orientable three-manifold satis- ¯es the Disjoint Annulus Property if each handlebody contains an essential annulus and these are disjoint. This paper proves that, for a ¯xed three- manifold, all but ¯nitely many splittings have the disjoint annulus property. As a corollary, all but ¯nitely many splittings have distance three or less, as de¯ned by Hempel. 1. History and overview Great e®ort has been spent on the classi¯cation problem for Heegaard splittings of three-manifolds. Haken's lemma [2], that all splittings of a reducible manifold are themselves reducible, could be considered one of the ¯rst results in this direction. Weak reducibility was introduced by Casson and Gordon [1] as a generalization of reducibility. They concluded that a weakly reducible splitting is either itself reducible or the manifold in question contains an incompressible surface. Thomp- son [16] later de¯ned the disjoint curve property as a further generalization of weak reducibility. She deduced that all splittings of a toroidal three-manifold have the disjoint curve property. Hempel [5] generalized these ideas to obtain the distance of a splitting, de¯ned in terms of the curve complex. He then adapted an argument of Kobayashi [9] to produce examples of splittings of arbitrarily large distance. Hartshorn [3], also following the ideas of [9], proved that Hempel's distance is bounded by twice the genus of any incompressible surface embedded in the given manifold. Here we introduce the twin annulus property (TAP) for Heegaard splittings as well as the weaker notion of the disjoint annulus property (DAP). -
Roots of Crosscap Slides and Crosscap Transpositions
Period Math Hung DOI 10.1007/s10998-017-0210-3 Roots of crosscap slides and crosscap transpositions Anna Parlak1 · Michał Stukow1 © The Author(s) 2017. This article is an open access publication Abstract Let Ng denote a closed nonorientable surface of genus g.Forg ≥ 2 the mapping class group M(Ng) is generated by Dehn twists and one crosscap slide (Y -homeomorphism) or by Dehn twists and a crosscap transposition. Margalit and Schleimer observed that Dehn twists on orientable surfaces have nontrivial roots. We give necessary and sufficient conditions for the existence of roots of crosscap slides and crosscap transpositions. Keywords Mapping class group · Nonorientable surface · Punctured sphere · Elementary braid · Crosscap slide · Crosscap transposition Mathematics Subject Classification 57N05 · 20F38 · 57M99 1 Introduction n Let Ng,s be a connected nonorientable surface of genus g with s boundary components and n punctures, that is a surface obtained from a connected sum of g projective planes Ng by removing s open disks and specifying the set ={p1,...,pn} of n distinguished points in the interior of Ng.Ifs or/and n equals zero, we omit it from notation. The mapping class M( n ) : n → n group Ng,s consists of isotopy classes of self-homeomorphisms h Ng,s Ng,s fixing () = M( n ) boundary components pointwise and such that h . The mapping class group Sg,s of an orientable surface is defined analogously, but we consider only orientation-preserving Both authors are supported by Grant 2015/17/B/ST1/03235 of National Science Centre, Poland. B Michał Stukow [email protected] Anna Parlak [email protected] 1 Institute of Mathematics, Faculty of Mathematics, Physics and Informatics, University of Gda´nsk, 80-308 Gda´nsk, Poland 123 A. -
Math.GT] 11 Aug 1998 Nec Once Opnn of Component Connected Each on Hr Xsssc an Such Exists There Has Let Ubro Udul Onsi O 2
QUADRUPLE POINTS OF REGULAR HOMOTOPIES OF SURFACES IN 3-MANIFOLDS TAHL NOWIK 1. Introduction Definition 1.1. Let F be a (finite) system of closed surfaces and M a 3-manifold. A regular homotopy Ht : F → M, t ∈ [0, 1] will be called closed if H0 = H1. We will denote a closed generic regular homotopy by CGRH. The number mod 2 of quadruple points of a generic regular homotopy Ht will be denoted by q(Ht) (∈ Z/2.) Max and Banchoff in [MB] proved that any generic regular homotopy of S2 in R3 which “turns S2 inside out,” has an odd number of quadruple points. The main point was showing that any CGRH of S2 in R3 has an even number of quadruple points. Goryunov in [G] expresses this from the Vassiliev Invariants point of view, as follows: Let Imm(S2, R3) be the space of all immersions of S2 in R3, and let ∆ ⊆ Imm(S2, R3) be the subspace of all non-generic immersions. Choose some 2 3 2 3 generic immersion f0 : S → R as a base immersion. For any generic immersion f : S → R let Q(f) ∈ Z/2 be defined as q(Ht) where Ht is some generic regular homotopy between f0 and f. 2 3 There exists such an Ht since Imm(S , R ) is connected, and this is well defined since any CGRH has q = 0. Furthermore, since generic immersions do not have quadruple points, Q will be constant on each connected component of Imm(S2, R3) − ∆. [G] then raises the question whether such a Q may be defined for any surface in R3, that is, whether for any CGRH of any surface in R3 the number of quadruple points is 0 mod 2. -
A Computation of Knot Floer Homology of Special (1,1)-Knots
A COMPUTATION OF KNOT FLOER HOMOLOGY OF SPECIAL (1,1)-KNOTS Jiangnan Yu Department of Mathematics Central European University Advisor: Andras´ Stipsicz Proposal prepared by Jiangnan Yu in part fulfillment of the degree requirements for the Master of Science in Mathematics. CEU eTD Collection 1 Acknowledgements I would like to thank Professor Andras´ Stipsicz for his guidance on writing this thesis, and also for his teaching and helping during the master program. From him I have learned a lot knowledge in topol- ogy. I would also like to thank Central European University and the De- partment of Mathematics for accepting me to study in Budapest. Finally I want to thank my teachers and friends, from whom I have learned so much in math. CEU eTD Collection 2 Abstract We will introduce Heegaard decompositions and Heegaard diagrams for three-manifolds and for three-manifolds containing a knot. We define (1,1)-knots and explain the method to obtain the Heegaard diagram for some special (1,1)-knots, and prove that torus knots and 2- bridge knots are (1,1)-knots. We also define the knot Floer chain complex by using the theory of holomorphic disks and their moduli space, and give more explanation on the chain complex of genus-1 Heegaard diagram. Finally, we compute the knot Floer homology groups of the trefoil knot and the (-3,4)-torus knot. 1 Introduction Knot Floer homology is a knot invariant defined by P. Ozsvath´ and Z. Szabo´ in [6], using methods of Heegaard diagrams and moduli theory of holomorphic discs, combined with homology theory. -
Physics 7D Makeup Midterm Solutions
Physics 7D Makeup Midterm Solutions Problem 1 A hollow, conducting sphere with an outer radius of 0:253 m and an inner radius of 0:194 m has a uniform surface charge density of 6:96 × 10−6 C/m2. A charge of −0:510 µC is now introduced into the cavity inside the sphere. (a) What is the new charge density on the outside of the sphere? (b) Calculate the strength of the electric field just outside the sphere. (c) What is the electric flux through a spherical surface just inside the inner surface of the sphere? Solution (a) Because there is no electric field inside a conductor the sphere must acquire a charge of +0:510 µC on its inner surface. Because there is no net flow of charge onto or off of the conductor this charge must come from the outer surface, so that the total charge of the outer 2 surface is now Qi − 0:510µC = σ(4πrout) − 0:510µC = 5:09µC. Now we divide again by the surface area to obtain the new charge density. 5:09 × 10−6C σ = = 6:32 × 10−6C/m2 (1) new 4π(0:253m)2 (b) The electric field just outside the sphere can be determined by Gauss' law once we determine the total charge on the sphere. We've already accounted for both the initial surface charge and the newly introduced point charge in our expression above, which tells us that −6 Qenc = 5:09 × 10 C. Gauss' law then tells us that Qenc 5 E = 2 = 7:15 × 10 N/C (2) 4π0rout (c) Finally we want to find the electric flux through a spherical surface just inside the sphere's cavity. -
An Introduction to Mapping Class Groups. In: Clay, M
Brendle, T., and Childers, L. (2015) Surfaces and their symmetries: an introduction to mapping class groups. In: Clay, M. and Margalit, D.(eds.) Office Hours With a Geometric Group Theorist. Princeton University Press. Copyright © 2015 Princeton University Press A copy can be downloaded for personal non-commercial research or study, without prior permission or charge Content must not be changed in any way or reproduced in any format or medium without the formal permission of the copyright holder(s) When referring to this work, full bibliographic details must be given http://eprints.gla.ac.uk/101049/ Deposited on: 9 January 2015 Enlighten – Research publications by members of the University of Glasgow http://eprints.gla.ac.uk SURFACES AND THEIR SYMMETRIES: AN INTRODUCTION TO MAPPING CLASS GROUPS TARA E. BRENDLE AND LEAH CHILDERS 1. Introduction An overarching theme in mathematics is that one can learn a vast deal about an object by studying its group of symmetries. For example, in abstract algebra we study two fundamental objects in mathematics, a finite set, and a regular polygon, via symmetric groups and dihedral groups, respectively. The primary goal of this chapter is to introduce the mapping class group Mod(S), that is, the group of symmetries of another fundamental object: a surface S. We will acquaint the reader with a few of its fascinating properties and give a brief glimpse of some active research related to this class of groups. We do not assume a background in topology. Therefore in Section 2 we give an introduction to surfaces and explain the concept of a homeomorphism, our working notion of \sameness" for surfaces. -
Volume Growth in the Component of the Dehn–Seidel Twist
VOLUME GROWTH IN THE COMPONENT OF THE DEHN–SEIDEL TWIST URS FRAUENFELDER AND FELIX SCHLENK Abstract. We consider an entropy-type invariant which mea- sures the polynomial volume growth of submanifolds under the iterates of a map, and we show that this invariant is at least 1 for every diffeomorphism in the symplectic isotopy class of the Dehn– Seidel twist. Contents 1. Introduction and main results 1 2. Proofs 5 2.1. Idea of the proof of Theorem 1 5 2.2. P -manifolds 6 2.3. Twists 7 2.4. LagrangianFloerhomology 10 m 2.5. Computation of HF∗ (ϑ (Dx),Dy) 15 2.6. EndoftheproofofTheorem1 23 2.7. Proof of Corollary 1 25 2.8. A remark on smoothness 26 2.9. Differential topology of twists 26 References 29 1. Introduction and main results The complexity of a compactly supported smooth diffeomorphism ϕ of a smooth manifold M can be measured in the following way: Fix a Riemannian metric g on M. For i ∈ {1,..., dim M} denote by Σi the set of smooth embeddings σ of the cube Qi = [0, 1]i into M, and i by µg(σ) the volume of σ (Q ) ⊂ M computed with respect to the measure on σ (Qi) induced by g. Following [21], we define for each i ∈ Date: January 12, 2005. 2000 Mathematics Subject Classification. Primary 53D35, Secondary 37B40, 53D40. 1 2 Volume growth in the component of the Dehn–Seidel twist {1,..., dim M} the i-dimensional slow volume growth si(ϕ) ∈ [0, ∞] by n log µg (ϕ (σ)) si(ϕ) = sup lim inf .