Numerically Accurate Hyperbolic Embeddings Using Tiling-Based Models
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Models of 2-Dimensional Hyperbolic Space and Relations Among Them; Hyperbolic Length, Lines, and Distances
Models of 2-dimensional hyperbolic space and relations among them; Hyperbolic length, lines, and distances Cheng Ka Long, Hui Kam Tong 1155109623, 1155109049 Course Teacher: Prof. Yi-Jen LEE Department of Mathematics, The Chinese University of Hong Kong MATH4900E Presentation 2, 5th October 2020 Outline Upper half-plane Model (Cheng) A Model for the Hyperbolic Plane The Riemann Sphere C Poincar´eDisc Model D (Hui) Basic properties of Poincar´eDisc Model Relation between D and other models Length and distance in the upper half-plane model (Cheng) Path integrals Distance in hyperbolic geometry Measurements in the Poincar´eDisc Model (Hui) M¨obiustransformations of D Hyperbolic length and distance in D Conclusion Boundary, Length, Orientation-preserving isometries, Geodesics and Angles Reference Upper half-plane model H Introduction to Upper half-plane model - continued Hyperbolic geometry Five Postulates of Hyperbolic geometry: 1. A straight line segment can be drawn joining any two points. 2. Any straight line segment can be extended indefinitely in a straight line. 3. A circle may be described with any given point as its center and any distance as its radius. 4. All right angles are congruent. 5. For any given line R and point P not on R, in the plane containing both line R and point P there are at least two distinct lines through P that do not intersect R. Some interesting facts about hyperbolic geometry 1. Rectangles don't exist in hyperbolic geometry. 2. In hyperbolic geometry, all triangles have angle sum < π 3. In hyperbolic geometry if two triangles are similar, they are congruent. -
1 Euclidean Geometry
Dr. Anna Felikson, Durham University Geometry, 26.02.2015 Outline 1 Euclidean geometry 1.1 Isometry group of Euclidean plane, Isom(E2). A distance on a space X is a function d : X × X ! R,(A; B) 7! d(A; B) for A; B 2 X satisfying 1. d(A; B) ≥ 0 (d(A; B) = 0 , A = B); 2. d(A; B) = d(B; A); 3. d(A; C) ≤ d(A; B) + d(B; C) (triangle inequality). We will use two models of Euclidean plane: p 2 2 a Cartesian plane: f(x; y) j x; y 2 Rg with the distance d(A1;A2) = (x1 − x2) + (y1 − y2) ; a Gaussian plane: fz j z 2 Cg, with the distance d(u; v) = ju − vj. Definition 1.1. A Euclidean isometry is a distance-preserving transformation of E2, i.e. a map f : E2 ! E2 satisfying d(f(A); f(B)) = d(A; B). Corollary 1.2. (a) Every isometry of E2 is a one-to-one map. (b) The composition of any two isometries is an isometry. (c) Isometries of E2 form a group (denoted Isom(E2)). Example 1.3: Translation, rotation, reflection in a line are isometries. Theorem 1.4. Let ABC and A0B0C0 be two congruent triangles. Then there exists a unique isometry sending A to A0, B to B0 and C to C0. Corollary 1.5. Every isometry of E2 is a composition of at most 3 reflections. (In particular, the group Isom(E2) is generated by reflections). Remark: the way to write an isometry as a composition of reflection is not unique. -
Fundamental Principles Governing the Patterning of Polyhedra
FUNDAMENTAL PRINCIPLES GOVERNING THE PATTERNING OF POLYHEDRA B.G. Thomas and M.A. Hann School of Design, University of Leeds, Leeds LS2 9JT, UK. [email protected] ABSTRACT: This paper is concerned with the regular patterning (or tiling) of the five regular polyhedra (known as the Platonic solids). The symmetries of the seventeen classes of regularly repeating patterns are considered, and those pattern classes that are capable of tiling each solid are identified. Based largely on considering the symmetry characteristics of both the pattern and the solid, a first step is made towards generating a series of rules governing the regular tiling of three-dimensional objects. Key words: symmetry, tilings, polyhedra 1. INTRODUCTION A polyhedron has been defined by Coxeter as “a finite, connected set of plane polygons, such that every side of each polygon belongs also to just one other polygon, with the provision that the polygons surrounding each vertex form a single circuit” (Coxeter, 1948, p.4). The polygons that join to form polyhedra are called faces, 1 these faces meet at edges, and edges come together at vertices. The polyhedron forms a single closed surface, dissecting space into two regions, the interior, which is finite, and the exterior that is infinite (Coxeter, 1948, p.5). The regularity of polyhedra involves regular faces, equally surrounded vertices and equal solid angles (Coxeter, 1948, p.16). Under these conditions, there are nine regular polyhedra, five being the convex Platonic solids and four being the concave Kepler-Poinsot solids. The term regular polyhedron is often used to refer only to the Platonic solids (Cromwell, 1997, p.53). -
Hyperbolic Geometry on a Hyperboloid, the American Mathematical Monthly, 100:5, 442-455, DOI: 10.1080/00029890.1993.11990430
William F. Reynolds (1993) Hyperbolic Geometry on a Hyperboloid, The American Mathematical Monthly, 100:5, 442-455, DOI: 10.1080/00029890.1993.11990430. (c) 1993 The American Mathematical Monthly 1985 Mathematics Subject Classification 51 M 10 HYPERBOLIC GEOMETRY ON A HYPERBOLOID William F. Reynolds Department of Mathematics, Tufts University, Medford, MA 02155 E-mail: [email protected] 1. Introduction. Hardly anyone would maintain that it is better to begin to learn geography from flat maps than from a globe. But almost all introductions to hyperbolic non-Euclidean geometry, except [6], present plane models, such as the projective and conformal disk models, without even mentioning that there exists a model that has the same relation to plane models that a globe has to flat maps. This model, which is on one sheet of a hyperboloid of two sheets in Minkowski 3-space and which I shall call H2, is over a hundred years old; Killing and Poincar´eboth described it in the 1880's (see Section 14). It is used by differential geometers [29, p. 4] and physicists (see [21, pp. 724-725] and [23, p. 113]). Nevertheless it is not nearly so well known as it should be, probably because, like a globe, it requires three dimensions. The main advantages of this model are its naturalness and its symmetry. Being embeddable (distance function and all) in flat space-time, it is close to our picture of physical reality, and all its points are treated alike in this embedding. Once the strangeness of the Minkowski metric is accepted, it has the familiar geometry of a sphere in Euclidean 3-space E3 as a guide to definitions and arguments. -
Hyperbolic Geometry
Flavors of Geometry MSRI Publications Volume 31,1997 Hyperbolic Geometry JAMES W. CANNON, WILLIAM J. FLOYD, RICHARD KENYON, AND WALTER R. PARRY Contents 1. Introduction 59 2. The Origins of Hyperbolic Geometry 60 3. Why Call it Hyperbolic Geometry? 63 4. Understanding the One-Dimensional Case 65 5. Generalizing to Higher Dimensions 67 6. Rudiments of Riemannian Geometry 68 7. Five Models of Hyperbolic Space 69 8. Stereographic Projection 72 9. Geodesics 77 10. Isometries and Distances in the Hyperboloid Model 80 11. The Space at Infinity 84 12. The Geometric Classification of Isometries 84 13. Curious Facts about Hyperbolic Space 86 14. The Sixth Model 95 15. Why Study Hyperbolic Geometry? 98 16. When Does a Manifold Have a Hyperbolic Structure? 103 17. How to Get Analytic Coordinates at Infinity? 106 References 108 Index 110 1. Introduction Hyperbolic geometry was created in the first half of the nineteenth century in the midst of attempts to understand Euclid’s axiomatic basis for geometry. It is one type of non-Euclidean geometry, that is, a geometry that discards one of Euclid’s axioms. Einstein and Minkowski found in non-Euclidean geometry a This work was supported in part by The Geometry Center, University of Minnesota, an STC funded by NSF, DOE, and Minnesota Technology, Inc., by the Mathematical Sciences Research Institute, and by NSF research grants. 59 60 J. W. CANNON, W. J. FLOYD, R. KENYON, AND W. R. PARRY geometric basis for the understanding of physical time and space. In the early part of the twentieth century every serious student of mathematics and physics studied non-Euclidean geometry. -
Five-Vertex Archimedean Surface Tessellation by Lanthanide-Directed Molecular Self-Assembly
Five-vertex Archimedean surface tessellation by lanthanide-directed molecular self-assembly David Écijaa,1, José I. Urgela, Anthoula C. Papageorgioua, Sushobhan Joshia, Willi Auwärtera, Ari P. Seitsonenb, Svetlana Klyatskayac, Mario Rubenc,d, Sybille Fischera, Saranyan Vijayaraghavana, Joachim Reicherta, and Johannes V. Bartha,1 aPhysik Department E20, Technische Universität München, D-85478 Garching, Germany; bPhysikalisch-Chemisches Institut, Universität Zürich, CH-8057 Zürich, Switzerland; cInstitute of Nanotechnology, Karlsruhe Institute of Technology, D-76344 Eggenstein-Leopoldshafen, Germany; and dInstitut de Physique et Chimie des Matériaux de Strasbourg (IPCMS), CNRS-Université de Strasbourg, F-67034 Strasbourg, France Edited by Kenneth N. Raymond, University of California, Berkeley, CA, and approved March 8, 2013 (received for review December 28, 2012) The tessellation of the Euclidean plane by regular polygons has by five interfering laser beams, conceived to specifically address been contemplated since ancient times and presents intriguing the surface tiling problem, yielded a distorted, 2D Archimedean- aspects embracing mathematics, art, and crystallography. Sig- like architecture (24). nificant efforts were devoted to engineer specific 2D interfacial In the last decade, the tools of supramolecular chemistry on tessellations at the molecular level, but periodic patterns with surfaces have provided new ways to engineer a diversity of sur- distinct five-vertex motifs remained elusive. Here, we report a face-confined molecular architectures, mainly exploiting molecular direct scanning tunneling microscopy investigation on the cerium- recognition of functional organic species or the metal-directed directed assembly of linear polyphenyl molecular linkers with assembly of molecular linkers (5). Self-assembly protocols have terminal carbonitrile groups on a smooth Ag(111) noble-metal sur- been developed to achieve regular surface tessellations, includ- face. -
A. Geodesics in the Hyperboloid Model B. Proof of Theorem 1 C
Hyperbolic Entailment Cones A. Geodesics in the Hyperboloid Model One can sanity check that indeed the formula from theorem n n 1 satisfies the conditions: The hyperboloid model is (H ; h·; ·i1), where H := fx 2 n;1 R : hx; xi1 = −1; x0 > 0g. The hyperboloid model can be viewed from the extrinsically as embedded in the pseudo- • d (γ(0); γ(t)) = t; 8t 2 [0; 1] n;1 D Riemannian manifold Minkowski space (R ; h·; ·i1) and n;1 inducing its metric. The Minkowski metric tensor gR of signature (n; 1) has the components • γ(0) = x 2−1 0 ::: 03 n;1 6 0 1 ::: 07 gR = 6 7 4 0 0 ::: 05 • γ_ (0) = v 0 0 ::: 1 The associated inner-product is hx; yi1 := −x0y0 + • lim γ(t) := γ(1) 2 @ n Pn t!1 D i=1 xiyi. Note that the hyperboloid model is a Rieman- nian manifold because the quadratic form associated with gH is positive definite. C. Proof of Corollary 1.1 n Proof. Denote u = p 1 v. Using the notations from In the extrinsic view, the tangent space at H can be de- gD(v;v) n n;1 x scribed as TxH = fv 2 R : hv; xi1 = 0g. See Robbin p Thm.1, one has expx(v) = γx;u( gxD(v; v)). Using Eq.3 & Salamon(2011); Parkkonen(2013). and6, one derives the result. Geodesics of Hn are given by the following theorem (Eq D. Proof of Corollary 1.2 (6.4.10) in Robbin & Salamon(2011)): n n Proof. -
Grade 6 Math Circles Tessellations Tiling the Plane
Faculty of Mathematics Centre for Education in Waterloo, Ontario N2L 3G1 Mathematics and Computing Grade 6 Math Circles October 13/14, 2015 Tessellations Tiling the Plane Do the following activity on a piece of graph paper. Build a pattern that you can repeat all over the page. Your pattern should use one, two, or three different `tiles' but no more than that. It will need to cover the page with no holes or overlapping shapes. Think of this exercises as if you were using tiles to create a pattern for your kitchen counter or a floor. Your pattern does not have to fill the page with straight edges; it can be a pattern with bumpy edges that does not fit the page perfectly. The only rule here is that we have no holes or overlapping between our tiles. Here are two examples, one a square tiling and another that we will call the up-down arrow tiling: Another word for tiling is tessellation. After you have created a tessellation, study it: did you use a weird shape or shapes? Or is your tiling simple and only uses straight lines and 1 polygons? Recall that a polygon is a many sided shape, with each side being a straight line. For example, triangles, trapezoids, and tetragons (quadrilaterals) are all polygons but circles or any shapes with curved sides are not polygons. As polygons grow more sides or become more irregular, you may find it difficult to use them as tiles. When given the previous activity, many will come up with the following tessellations. -
Unifying the Hyperbolic and Spherical 2-Body Problem with Biquaternions
Unifying the Hyperbolic and Spherical 2-Body Problem with Biquaternions Philip Arathoon December 2020 Abstract The 2-body problem on the sphere and hyperbolic space are both real forms of holo- morphic Hamiltonian systems defined on the complex sphere. This admits a natural description in terms of biquaternions and allows us to address questions concerning the hyperbolic system by complexifying it and treating it as the complexification of a spherical system. In this way, results for the 2-body problem on the sphere are readily translated to the hyperbolic case. For instance, we implement this idea to completely classify the relative equilibria for the 2-body problem on hyperbolic 3-space for a strictly attractive potential. Background and outline The case of the 2-body problem on the 3-sphere has recently been considered by the author in [1]. This treatment takes advantage of the fact that S3 is a group and that the action of SO(4) on S3 is generated by the left and right multiplication of S3 on itself. This allows for a reduction in stages, first reducing by the left multiplication, and then reducing an intermediate space by the residual right-action. An advantage of this reduction-by-stages is that it allows for a fairly straightforward derivation of the relative equilibria solutions: the relative equilibria may first be classified in the intermediate reduced space and then reconstructed on the original phase space. For the 2-body problem on hyperbolic space the same idea does not apply. Hyperbolic 3-space H3 cannot be endowed with an isometric group structure and the symmetry group SO(1; 3) does not arise as a direct product of two groups. -
Self-Organization on Riemannian Manifolds
JOURNAL OF GEOMETRIC MECHANICS doi:10.3934/jgm.2019020 c American Institute of Mathematical Sciences Volume 11, Number 3, September 2019 pp. 397{426 SELF-ORGANIZATION ON RIEMANNIAN MANIFOLDS Razvan C. Fetecau∗ and Beril Zhang Department of Mathematics Simon Fraser University Burnaby, BC V5A 1S6, Canada (Communicated by Darryl D. Holm and Manuel de Le´on) Abstract. We consider an aggregation model that consists of an active trans- port equation for the macroscopic population density, where the velocity has a nonlocal functional dependence on the density, modelled via an interaction potential. We set up the model on general Riemannian manifolds and provide a framework for constructing interaction potentials which lead to equilibria that are constant on their supports. We consider such potentials for two specific cases (the two-dimensional sphere and the two-dimensional hyperbolic space) and investigate analytically and numerically the long-time behaviour and equi- librium solutions of the aggregation model on these manifolds. Equilibria ob- tained numerically with other interaction potentials and an application of the model to aggregation on the rotation group SO(3) are also presented. 1. Introduction. The literature on self-collective behaviour of autonomous agents (e.g., biological organisms, robots, nanoparticles, etc) has been growing very fast recently. One of the main interests of such research is to understand how swarm- ing and flocking behaviours emerge in groups with no leader or external coordina- tion. Such behaviours occur for instance in natural swarms, e.g., flocks of birds or schools of fish [14, 25]. Also, swarming and flocking of artificial mobile agents (e.g., robots) in the absence of a centralized coordination mechanism is of major interest in engineering [37, 38]. -
Harmonic Analysis on the Proper Velocity Gyrogroup ∗ 1 Introduction
Harmonic Analysis on the Proper Velocity gyrogroup ∗ Milton Ferreira School of Technology and Management, Polytechnic Institute of Leiria, Portugal 2411-901 Leiria, Portugal. Email: [email protected] and Center for Research and Development in Mathematics and Applications (CIDMA), University of Aveiro, 3810-193 Aveiro, Portugal. Email [email protected] Abstract In this paper we study harmonic analysis on the Proper Velocity (PV) gyrogroup using the gyrolanguage of analytic hyperbolic geometry. PV addition is the relativis- tic addition of proper velocities in special relativity and it is related with the hy- perboloid model of hyperbolic geometry. The generalized harmonic analysis depends on a complex parameter z and on the radius t of the hyperboloid and comprises the study of the generalized translation operator, the associated convolution operator, the generalized Laplace-Beltrami operator and its eigenfunctions, the generalized Poisson transform and its inverse, the generalized Helgason-Fourier transform, its inverse and Plancherel's Theorem. In the limit of large t; t ! +1; the generalized harmonic analysis on the hyperboloid tends to the standard Euclidean harmonic analysis on Rn; thus unifying hyperbolic and Euclidean harmonic analysis. Keywords: PV gyrogroup, Laplace Beltrami operator, Eigenfunctions, Generalized Helgason- Fourier transform, Plancherel's Theorem. 1 Introduction Harmonic analysis is the branch of mathematics that studies the representation of functions or signals as the superposition of basic waves called harmonics. It investigates and gen- eralizes the notions of Fourier series and Fourier transforms. In the past two centuries, it has become a vast subject with applications in diverse areas as signal processing, quantum mechanics, and neuroscience (see [18] for an overview). -
Dispersion Relations of Periodic Quantum Graphs Associated with Archimedean Tilings (I)
Dispersion relations of periodic quantum graphs associated with Archimedean tilings (I) Yu-Chen Luo1, Eduardo O. Jatulan1,2, and Chun-Kong Law1 1 Department of Applied Mathematics, National Sun Yat-sen University, Kaohsiung, Taiwan 80424. Email: [email protected] 2 Institute of Mathematical Sciences and Physics, University of the Philippines Los Banos, Philippines 4031. Email: [email protected] January 15, 2019 Abstract There are totally 11 kinds of Archimedean tiling for the plane. Applying the Floquet-Bloch theory, we derive the dispersion relations of the periodic quantum graphs associated with a number of Archimedean tiling, namely the triangular tiling (36), the elongated triangular tiling (33; 42), the trihexagonal tiling (3; 6; 3; 6) and the truncated square tiling (4; 82). The derivation makes use of characteristic functions, with the help of the symbolic software Mathematica. The resulting dispersion relations are surpris- ingly simple and symmetric. They show that in each case the spectrum is composed arXiv:1809.09581v2 [math.SP] 12 Jan 2019 of point spectrum and an absolutely continuous spectrum. We further analyzed on the structure of the absolutely continuous spectra. Our work is motivated by the studies on the periodic quantum graphs associated with hexagonal tiling in [13] and [11]. Keywords: characteristic functions, Floquet-Bloch theory, quantum graphs, uniform tiling, dispersion relation. 1 1 Introduction Recently there have been a lot of studies on quantum graphs, which is essentially the spectral problem of a one-dimensional Schr¨odinger operator acting on the edge of a graph, while the functions have to satisfy some boundary conditions as well as vertex conditions which are usually the continuity and Kirchhoff conditions.