The Fundamental Polygon 3 3. Method Two: Sewing Handles and Mobius Strips 13 Acknowledgments 18 References 18
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Note on 6-Regular Graphs on the Klein Bottle Michiko Kasai [email protected]
Theory and Applications of Graphs Volume 4 | Issue 1 Article 5 2017 Note On 6-regular Graphs On The Klein Bottle Michiko Kasai [email protected] Naoki Matsumoto Seikei University, [email protected] Atsuhiro Nakamoto Yokohama National University, [email protected] Takayuki Nozawa [email protected] Hiroki Seno [email protected] See next page for additional authors Follow this and additional works at: https://digitalcommons.georgiasouthern.edu/tag Part of the Discrete Mathematics and Combinatorics Commons Recommended Citation Kasai, Michiko; Matsumoto, Naoki; Nakamoto, Atsuhiro; Nozawa, Takayuki; Seno, Hiroki; and Takiguchi, Yosuke (2017) "Note On 6-regular Graphs On The Klein Bottle," Theory and Applications of Graphs: Vol. 4 : Iss. 1 , Article 5. DOI: 10.20429/tag.2017.040105 Available at: https://digitalcommons.georgiasouthern.edu/tag/vol4/iss1/5 This article is brought to you for free and open access by the Journals at Digital Commons@Georgia Southern. It has been accepted for inclusion in Theory and Applications of Graphs by an authorized administrator of Digital Commons@Georgia Southern. For more information, please contact [email protected]. Note On 6-regular Graphs On The Klein Bottle Authors Michiko Kasai, Naoki Matsumoto, Atsuhiro Nakamoto, Takayuki Nozawa, Hiroki Seno, and Yosuke Takiguchi This article is available in Theory and Applications of Graphs: https://digitalcommons.georgiasouthern.edu/tag/vol4/iss1/5 Kasai et al.: 6-regular graphs on the Klein bottle Abstract Altshuler [1] classified 6-regular graphs on the torus, but Thomassen [11] and Negami [7] gave different classifications for 6-regular graphs on the Klein bottle. In this note, we unify those two classifications, pointing out their difference and similarity. -
An Introduction to Topology the Classification Theorem for Surfaces by E
An Introduction to Topology An Introduction to Topology The Classification theorem for Surfaces By E. C. Zeeman Introduction. The classification theorem is a beautiful example of geometric topology. Although it was discovered in the last century*, yet it manages to convey the spirit of present day research. The proof that we give here is elementary, and its is hoped more intuitive than that found in most textbooks, but in none the less rigorous. It is designed for readers who have never done any topology before. It is the sort of mathematics that could be taught in schools both to foster geometric intuition, and to counteract the present day alarming tendency to drop geometry. It is profound, and yet preserves a sense of fun. In Appendix 1 we explain how a deeper result can be proved if one has available the more sophisticated tools of analytic topology and algebraic topology. Examples. Before starting the theorem let us look at a few examples of surfaces. In any branch of mathematics it is always a good thing to start with examples, because they are the source of our intuition. All the following pictures are of surfaces in 3-dimensions. In example 1 by the word “sphere” we mean just the surface of the sphere, and not the inside. In fact in all the examples we mean just the surface and not the solid inside. 1. Sphere. 2. Torus (or inner tube). 3. Knotted torus. 4. Sphere with knotted torus bored through it. * Zeeman wrote this article in the mid-twentieth century. 1 An Introduction to Topology 5. -
Analytic Vortex Solutions on Compact Hyperbolic Surfaces
Analytic vortex solutions on compact hyperbolic surfaces Rafael Maldonado∗ and Nicholas S. Mantony Department of Applied Mathematics and Theoretical Physics, Wilberforce Road, Cambridge CB3 0WA, U.K. August 27, 2018 Abstract We construct, for the first time, Abelian-Higgs vortices on certain compact surfaces of constant negative curvature. Such surfaces are represented by a tessellation of the hyperbolic plane by regular polygons. The Higgs field is given implicitly in terms of Schwarz triangle functions and analytic solutions are available for certain highly symmetric configurations. 1 Introduction Consider the Abelian-Higgs field theory on a background surface M with metric ds2 = Ω(x; y)(dx2+dy2). At critical coupling the static energy functional satisfies a Bogomolny bound 2 1 Z B Ω 2 E = + jD Φj2 + 1 − jΦj2 dxdy ≥ πN; (1) 2 2Ω i 2 where the topological invariant N (the `vortex number') is the number of zeros of Φ counted with multiplicity [1]. In the notation of [2] we have taken e2 = τ = 1. Equality in (1) is attained when the fields satisfy the Bogomolny vortex equations, which are obtained by completing the square in (1). In complex coordinates z = x + iy these are 2 Dz¯Φ = 0;B = Ω (1 − jΦj ): (2) This set of equations has smooth vortex solutions. As we explain in section 2, analytical results are most readily obtained when M is hyperbolic, having constant negative cur- vature K = −1, a case which is of interest in its own right due to the relation between arXiv:1502.01990v1 [hep-th] 6 Feb 2015 hyperbolic vortices and SO(3)-invariant instantons, [3]. -
Graphs on Surfaces, the Generalized Euler's Formula and The
Graphs on surfaces, the generalized Euler's formula and the classification theorem ZdenˇekDvoˇr´ak October 28, 2020 In this lecture, we allow the graphs to have loops and parallel edges. In addition to the plane (or the sphere), we can draw the graphs on the surface of the torus or on more complicated surfaces. Definition 1. A surface is a compact connected 2-dimensional manifold with- out boundary. Intuitive explanation: • 2-dimensional manifold without boundary: Each point has a neighbor- hood homeomorphic to an open disk, i.e., \locally, the surface looks at every point the same as the plane." • compact: \The surface can be covered by a finite number of such neigh- borhoods." • connected: \The surface has just one piece." Examples: • The sphere and the torus are surfaces. • The plane is not a surface, since it is not compact. • The closed disk is not a surface, since it has a boundary. From the combinatorial perspective, it does not make sense to distinguish between some of the surfaces; the same graphs can be drawn on the torus and on a deformed torus (e.g., a coffee mug with a handle). For us, two surfaces will be equivalent if they only differ by a homeomorphism; a function f :Σ1 ! Σ2 between two surfaces is a homeomorphism if f is a bijection, continuous, and the inverse f −1 is continuous as well. In particular, this 1 implies that f maps simple continuous curves to simple continuous curves, and thus it maps a drawing of a graph in Σ1 to a drawing of the same graph in Σ2. -
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. -
Area-Preserving Diffeomorphisms of the Torus Whose Rotation Sets Have
Area-preserving diffeomorphisms of the torus whose rotation sets have non-empty interior Salvador Addas-Zanata Instituto de Matem´atica e Estat´ıstica Universidade de S˜ao Paulo Rua do Mat˜ao 1010, Cidade Universit´aria, 05508-090 S˜ao Paulo, SP, Brazil Abstract ǫ In this paper we consider C1+ area-preserving diffeomorphisms of the torus f, either homotopic to the identity or to Dehn twists. We sup- e pose that f has a lift f to the plane such that its rotation set has in- terior and prove, among other things that if zero is an interior point of e e 2 the rotation set, then there exists a hyperbolic f-periodic point Q∈ IR such that W u(Qe) intersects W s(Qe +(a,b)) for all integers (a,b), which u e implies that W (Q) is invariant under integer translations. Moreover, u e s e e u e W (Q) = W (Q) and f restricted to W (Q) is invariant and topologi- u e cally mixing. Each connected component of the complement of W (Q) is a disk with diameter uniformly bounded from above. If f is transitive, u e 2 e then W (Q) =IR and f is topologically mixing in the whole plane. Key words: pseudo-Anosov maps, Pesin theory, periodic disks e-mail: [email protected] 2010 Mathematics Subject Classification: 37E30, 37E45, 37C25, 37C29, 37D25 The author is partially supported by CNPq, grant: 304803/06-5 1 Introduction and main results One of the most well understood chapters of dynamics of surface homeomor- phisms is the case of the torus. -
Animal Testing
Animal Testing Adrian Dumitrescu∗ Evan Hilscher † Abstract an animal A. Let A′ be the animal such that there is a cube at every integer coordinate within the box, i.e., it A configuration of unit cubes in three dimensions with is a solid rectangular box containing the given animal. integer coordinates is called an animal if the boundary The algorithm is as follows: of their union is homeomorphic to a sphere. Shermer ′ discovered several animals from which no single cube 1. Transform A1 to A1 by addition only. ′ ′ may be removed such that the resulting configurations 2. Transform A1 to A2 . are also animals [6]. Here we obtain a dual result: we ′ give an example of an animal to which no cube may 3. Transform A2 to A2 by removal only. be added within its minimal bounding box such that ′ ′ It is easy to see that A1 can be transformed to A2 . the resulting configuration is also an animal. We also ′ We simply add or remove one layer of A1 , one cube O n present a ( )-time algorithm for determining whether at a time. The only question is, can any animal A be n a configuration of unit cubes is an animal. transformed to A′ by addition only? If the answer is yes, Keywords: Animal, polyomino, homeomorphic to a then the third step above is also feasible. As it turns sphere. out, the answer is no, thus our alternative algorithm is also infeasible. 1 Introduction Our results. In Section 2 we present a construction of an animal to which no cube may be added within its An animal is defined as a configuration of axis-aligned minimal bounding box such that the resulting collection unit cubes with integer coordinates in 3-space such of unit cubes is an animal. -
Space Complexity of Perfect Matching in Bounded Genus Bipartite Graphs
Space Complexity of Perfect Matching in Bounded Genus Bipartite Graphs Samir Datta1, Raghav Kulkarni2, Raghunath Tewari3, and N. Variyam Vinodchandran4 1 Chennai Mathematical Institute Chennai, India [email protected] 2 University of Chicago Chicago, USA [email protected] 3 University of Nebraska-Lincoln Lincoln, USA [email protected] 4 University of Nebraska-Lincoln Lincoln, USA [email protected] Abstract We investigate the space complexity of certain perfect matching problems over bipartite graphs embedded on surfaces of constant genus (orientable or non-orientable). We show that the prob- lems of deciding whether such graphs have (1) a perfect matching or not and (2) a unique perfect matching or not, are in the logspace complexity class SPL. Since SPL is contained in the logspace counting classes ⊕L (in fact in ModkL for all k ≥ 2), C=L, and PL, our upper bound places the above-mentioned matching problems in these counting classes as well. We also show that the search version, computing a perfect matching, for this class of graphs is in FLSPL. Our results extend the same upper bounds for these problems over bipartite planar graphs known earlier. As our main technical result, we design a logspace computable and polynomially bounded weight function which isolates a minimum weight perfect matching in bipartite graphs embedded on surfaces of constant genus. We use results from algebraic topology for proving the correctness of the weight function. 1998 ACM Subject Classification Computational Complexity Keywords and phrases perfect matching, bounded genus graphs, isolation problem Digital Object Identifier 10.4230/LIPIcs.STACS.2011.579 1 Introduction The perfect matching problem and its variations are one of the most well-studied prob- lems in theoretical computer science. -
2 Non-Orientable Surfaces §
2 NON-ORIENTABLE SURFACES § 2 Non-orientable Surfaces § This section explores stranger surfaces made from gluing diagrams. Supplies: Glass Klein bottle • Scarf and hat • Transparency fish • Large pieces of posterboard to cut • Markers • Colored paper grid for making the room a gluing diagram • Plastic tubes • Mobius band templates • Cube templates from Exploring the Shape of Space • 24 Mobius Bands 2 NON-ORIENTABLE SURFACES § Mobius Bands 1. Cut a blank sheet of paper into four long strips. Make one strip into a cylinder by taping the ends with no twist, and make a second strip into a Mobius band by taping the ends together with a half twist (a twist through 180 degrees). 2. Mark an X somewhere on your cylinder. Starting at the X, draw a line down the center of the strip until you return to the starting point. Do the same for the Mobius band. What happens? 3. Make a gluing diagram for a cylinder by drawing a rectangle with arrows. Do the same for a Mobius band. 4. The gluing diagram you made defines a virtual Mobius band, which is a little di↵erent from a paper Mobius band. A paper Mobius band has a slight thickness and occupies a small volume; there is a small separation between its ”two sides”. The virtual Mobius band has zero thickness; it is truly 2-dimensional. Mark an X on your virtual Mobius band and trace down the centerline. You’ll get back to your starting point after only one trip around! 25 Multiple twists 2 NON-ORIENTABLE SURFACES § 5. -
Classification of Compact Orientable Surfaces Using Morse Theory
U.U.D.M. Project Report 2016:37 Classification of Compact Orientable Surfaces using Morse Theory Johan Rydholm Examensarbete i matematik, 15 hp Handledare: Thomas Kragh Examinator: Jörgen Östensson Augusti 2016 Department of Mathematics Uppsala University Classication of Compact Orientable Surfaces using Morse Theory Johan Rydholm 1 Introduction Here we classify surfaces up to dieomorphism. The classication is done in section Construction of the Genus-g Toruses, as an application of the previously developed Morse theory. The objects which we study, surfaces, are dened in section Surfaces, together with other denitions and results which lays the foundation for the rest of the essay. Most of the section Surfaces is taken from chapter 0 in [2], and gives a quick introduction to, among other things, smooth manifolds, dieomorphisms, smooth vector elds and connected sums. The material in section Morse Theory and section Existence of a Good Morse Function uses mainly chapter 1 in [5] and chapters 2,4 and 5 in [4] (but not necessarily only these chapters). In these two sections we rst prove Lemma of Morse, which is probably the single most important result, even though the proof is far from the hardest. We prove the existence of a Morse function, existence of a self-indexing Morse function, and nally the existence of a good Morse function, on any surface; while doing this we also prove the existence of one of our most important tools: a gradient-like vector eld for the Morse function. The results in sections Morse Theory and Existence of a Good Morse Func- tion contains the main resluts and ideas. -
How to Make a Torus Laszlo C
DO THE MATH! How to Make a Torus Laszlo C. Bardos sk a topologist how to make a model of a torus and your instructions will be to tape two edges of a piece of paper together to form a tube and then to tape the ends of the tube together. This process is math- Aematically correct, but the result is either a flat torus or a crinkled mess. A more deformable material such as cloth gives slightly better results, but sewing a torus exposes an unexpected property of tori. Start by sewing the torus The sticky notes inside out so that the stitching will be hidden when illustrate one of three the torus is reversed. Leave a hole in the side for this types of circular cross purpose. Wait a minute! Can you even turn a punctured sections. We find the torus inside out? second circular cross Surprisingly, the answer is yes. However, doing so section by cutting a yields a baffling result. A torus that started with a torus with a plane pleasing doughnut shape transforms into a one with perpendicular to different, almost unrecognizable dimensions when turned the axis of revolu- right side out. (See figure 1.) tion (both such cross So, if the standard model of a torus doesn’t work well, sections are shown we’ll need to take another tack. A torus is generated Figure 2. A torus made from on the green torus in sticky notes. by sweeping a figure 3). circle around But there is third, an axis in the less obvious way to same plane as create a circular cross the circle. -
Torus and Klein Bottle Tessellations with a Single Tile of Pied De Poule (Houndstooth)
Bridges 2018 Conference Proceedings Torus and Klein Bottle Tessellations with a Single Tile of Pied de Poule (Houndstooth) Loe M.G. Feijs Eindhoven University of Technology, The Netherlands; [email protected] Abstract We design a 3D surface made by continuous deformation applied to a single tile. The contour edges are aligned according to the network topology of a Pied-de-poule tessellation. In a classical tessellation, each edge is aligned with a matching edge of a neighbouring tile, but here the single tile acts as a neighbouring tile too. The continuous deformation mapping the Pied-de-poule tile to the 3D surface preserves the staircase nature of the contour edges of the tile. It is a diffeomorphism. The 3D surface thus appears as a torus with gaps where the sides of the tile meet. Next we present another surface, also a single Pied-de-poule tile, but with different tessellation type, a Klein bottle. Both surfaces are 3D printed as innovative art works, connecting topological manifolds and the famous fashion pattern. Introduction Pied-de-poule (houndstooth) denotes a family of fashion patterns, see the Bridges 2012 paper [3] and Abdalla Ahmed’s work on weaving design [1] for more background information. In this project, we study tessellations obtained by continuous deformation of a Pied-de-poule’s basic tile. In particular, we construct tessellations with a single copy of one basic tile. The network topology of the tessellation was analysed in [3]. A typical piece of Pied-de-poule fabric can be seen in Figure 1 (left).