The Ubiquity of ADE Classifications in Nature
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Final Poster
Associating Finite Groups with Dessins d’Enfants Luis Baeza, Edwin Baeza, Conner Lawrence, and Chenkai Wang Abstract Platonic Solids Rotation Group Dn: Regular Convex Polygon Approach Each finite, connected planar graph has an automorphism group G;such Following Magot and Zvonkin, reduce to easier cases using “hypermaps” permutations can be extended to automorphisms of the Riemann sphere φ : P1(C) P1(C), then composing β = φ f where S 2(R) P1(C). In 1984, Alexander Grothendieck, inspired by a result of f : 1( ) ! 1( )isaBely˘ımapasafunctionofeither◦ zn or ' P C P C Gennadi˘ıBely˘ıfrom 1979, constructed a finite, connected planar graph 4 zn/(zn +1)! 2 such that Aut(f ) Z or Aut(f ) D ,respectively. ' n ' n ∆β via certain rational functions β(z)=p(z)/q(z)bylookingatthe inverse image of the interval from 0 to 1. The automorphisms of such a Hypermaps: Rotation Group Zn graph can be identified with the Galois group Aut(β)oftheassociated 1 1 rational function β : P (C) P (C). In this project, we investigate how Rigid Rotations of the Platonic Solids I Wheel/Pyramids (J1, J2) ! w 3 (w +8) restrictive Grothendieck’s concept of a Dessin d’Enfant is in generating all n 2 I φ(w)= 1 1 z +1 64 (w 1) automorphisms of planar graphs. We discuss the rigid rotations of the We have an action : PSL2(C) P (C) P (C). β(z)= : v = n + n, e =2 n, f =2 − n ◦ ⇥ 2 !n 2 4 zn · Platonic solids (the tetrahedron, cube, octahedron, icosahedron, and I Zn = r r =1 and Dn = r, s s = r =(sr) =1 are the rigid I Cupola (J3, J4, J5) dodecahedron), the Archimedean solids, the Catalan solids, and the rotations of the regular convex polygons,with 4w 4(w 2 20w +105)3 I φ(w)= − ⌦ ↵ ⌦ 1 ↵ Rotation Group A4: Tetrahedron 3 2 Johnson solids via explicit Bely˘ımaps. -
Platonic and Archimedean Geometries in Multicomponent Elastic Membranes
Platonic and Archimedean geometries in multicomponent elastic membranes Graziano Vernizzia,1, Rastko Sknepneka, and Monica Olvera de la Cruza,b,c,2 aDepartment of Materials Science and Engineering, Northwestern University, Evanston, IL 60208; bDepartment of Chemical and Biological Engineering, Northwestern University, Evanston, IL 60208; and cDepartment of Chemistry, Northwestern University, Evanston, IL 60208 Edited by L. Mahadevan, Harvard University, Cambridge, MA, and accepted by the Editorial Board February 8, 2011 (received for review August 30, 2010) Large crystalline molecular shells, such as some viruses and fuller- possible to construct a lattice on the surface of a sphere such enes, buckle spontaneously into icosahedra. Meanwhile multi- that each site has only six neighbors. Consequently, any such crys- component microscopic shells buckle into various polyhedra, as talline lattice will contain defects. If one allows for fivefold observed in many organelles. Although elastic theory explains defects only then, according to the Euler theorem, the minimum one-component icosahedral faceting, the possibility of buckling number of defects is 12 fivefold disclinations. In the absence of into other polyhedra has not been explored. We show here that further defects (21), these 12 disclinations are positioned on the irregular and regular polyhedra, including some Archimedean and vertices of an inscribed icosahedron (22). Because of the presence Platonic polyhedra, arise spontaneously in elastic shells formed of disclinations, the ground state of the shell has a finite strain by more than one component. By formulating a generalized elastic that grows with the shell size. When γ > γà (γà ∼ 154) any flat model for inhomogeneous shells, we demonstrate that coas- fivefold disclination buckles into a conical shape (19). -
The Truncated Icosahedron As an Inflatable Ball
https://doi.org/10.3311/PPar.12375 Creative Commons Attribution b |99 Periodica Polytechnica Architecture, 49(2), pp. 99–108, 2018 The Truncated Icosahedron as an Inflatable Ball Tibor Tarnai1, András Lengyel1* 1 Department of Structural Mechanics, Faculty of Civil Engineering, Budapest University of Technology and Economics, H-1521 Budapest, P.O.B. 91, Hungary * Corresponding author, e-mail: [email protected] Received: 09 April 2018, Accepted: 20 June 2018, Published online: 29 October 2018 Abstract In the late 1930s, an inflatable truncated icosahedral beach-ball was made such that its hexagonal faces were coloured with five different colours. This ball was an unnoticed invention. It appeared more than twenty years earlier than the first truncated icosahedral soccer ball. In connection with the colouring of this beach-ball, the present paper investigates the following problem: How many colourings of the dodecahedron with five colours exist such that all vertices of each face are coloured differently? The paper shows that four ways of colouring exist and refers to other colouring problems, pointing out a defect in the colouring of the original beach-ball. Keywords polyhedron, truncated icosahedron, compound of five tetrahedra, colouring of polyhedra, permutation, inflatable ball 1 Introduction Spherical forms play an important role in different fields – not even among the relics of the Romans who inherited of science and technology, and in different areas of every- many ball games from the Greeks. day life. For example, spherical domes are quite com- The Romans mainly used balls composed of equal mon in architecture, and spherical balls are used in most digonal panels, forming a regular hosohedron (Coxeter, 1973, ball games. -
Arxiv:1403.3190V4 [Gr-Qc] 18 Jun 2014 ‡ † ∗ Stefloig H Oetintr Ftehmloincon Hamiltonian the of [16]
A curvature operator for LQG E. Alesci,∗ M. Assanioussi,† and J. Lewandowski‡ Institute of Theoretical Physics, University of Warsaw (Instytut Fizyki Teoretycznej, Uniwersytet Warszawski), ul. Ho˙za 69, 00-681 Warszawa, Poland, EU We introduce a new operator in Loop Quantum Gravity - the 3D curvature operator - related to the 3-dimensional scalar curvature. The construction is based on Regge Calculus. We define this operator starting from the classical expression of the Regge curvature, we derive its properties and discuss some explicit checks of the semi-classical limit. I. INTRODUCTION Loop Quantum Gravity [1] is a promising candidate to finally realize a quantum description of General Relativity. The theory presents two complementary descriptions based on the canon- ical and the covariant approach (spinfoams) [2]. The first implements the Dirac quantization procedure [3] for GR in Ashtekar-Barbero variables [4] formulated in terms of the so called holonomy-flux algebra [1]: one considers smooth manifolds and defines a system of paths and dual surfaces over which the connection and the electric field can be smeared. The quantiza- tion of the system leads to the full Hilbert space obtained as the projective limit of the Hilbert space defined on a single graph. The second is instead based on the Plebanski formulation [5] of GR, implemented starting from a simplicial decomposition of the manifold, i.e. restricting to piecewise linear flat geometries. Even if the starting point is different (smooth geometry in the first case, piecewise linear in the second) the two formulations share the same kinematics [6] namely the spin-network basis [7] first introduced by Penrose [8]. -
Resolution of ADE Singularities
Resolution of Kleinian Singularities James J. Green April 25, 2014 abstract Firstly, the classification of finite subgroups of SL(2; C), a result of Felix Klein in 1884, is presented. The polynomial invariant subrings of these groups are then found. The generators of these subrings 3 satisfy a polynomial relation in three variables, which can be realised as a hypersurface in C . Each of these surfaces have a singularity at the origin; these are the Kleinian singularities. These singularities are blown-up, and their resolution graphs are shown to be precisely the Coxeter- Dynkin diagrams ADE. The target readership of this project is intended to be undergraduates with a foundational knowledge of group theory, topology and algebraic geometry. 1 1 Classifying the Finite Subgroups of SL(2; C) 1.1 Important Subgroups of the General Linear Group Recall: The general linear group of a vector space V over a field F is given by GL(V ) = ff : V −! V j f is linear and invertibleg: n In particular, we denote GL(F ) by GL(n; F). Since we can view linear maps as matrices, GL(n; F) can also be viewed as the set of invertible n × n matrices with entries in F. The next few definitions include important subgroups of GL(n; F). Definition 1.1. The special linear group over F is given by SL(n; F) = fA 2 GL(n; F) j det A = 1g: Definition 1.2. The orthogonal group over F is given by T O(n; F) = fA 2 GL(n; F) j AA = Ig where AT denotes the transpose of A, and I denotes the n × n identity matrix. -
Swampland Constraints on 5D N = 1 Supergravity Arxiv:2004.14401V2
Prepared for submission to JHEP Swampland Constraints on 5d N = 1 Supergravity Sheldon Katz, a Hee-Cheol Kim, b;c Houri-Christina Tarazi, d Cumrun Vafa d aDepartment of Mathematics, MC-382, University of Illinois at Urbana-Champaign, Ur- bana, IL 61801, USA bDepartment of Physics, POSTECH, Pohang 790-784, Korea cAsia Pacific Center for Theoretical Physics, Postech, Pohang 37673, Korea dDepartment of Physics, Harvard University, Cambridge, MA 02138, USA Abstract: We propose Swampland constraints on consistent 5-dimensional N = 1 supergravity theories. We focus on a special class of BPS magnetic monopole strings which arise in gravitational theories. The central charges and the levels of current algebras of 2d CFTs on these strings can be calculated by anomaly inflow mechanism and used to provide constraints on the low-energy particle spectrum and the effective action of the 5d supergravity based on unitarity of the worldsheet CFT. In M-theory, where these theories are realized by compactification on Calabi-Yau 3-folds, the spe- cial monopole strings arise from wrapped M5-branes on special (\semi-ample") 4- cycles in the threefold. We identify various necessary geometric conditions for such cycles to lead to requisite BPS strings and translate these into constraints on the low-energy theories of gravity. These and other geometric conditions, some of which can be related to unitarity constraints on the monopole worldsheet, are additional arXiv:2004.14401v2 [hep-th] 13 Jul 2020 candidates for Swampland constraints on 5-dimensional N = 1 supergravity -
Little String Defects and Nilpotent Orbits by Christian Schmid A
Little String Defects and Nilpotent Orbits by Christian Schmid A dissertation submitted in partial satisfaction of the requirements for the degree of Doctor of Philosophy in Physics in the Graduate Division of the University of California, Berkeley Committee in charge: Professor Mina Aganagic, Chair Professor Ori Ganor Professor Nicolai Reshetikhin Spring 2020 Little String Defects and Nilpotent Orbits Copyright 2020 by Christian Schmid 1 Abstract Little String Defects and Nilpotent Orbits by Christian Schmid Doctor of Philosophy in Physics University of California, Berkeley Professor Mina Aganagic, Chair In this thesis, we first derive and analyze the Gukov{Witten surface defects of four- dimensional N = 4 Super Yang-Mills (SYM) theory from little string theory. The little string theory arises from type IIB string theory compactified on an ADE singularity. Defects are introduced as D-branes wrapping the 2-cycles of the singularity. In a suitable limit, these become defects of the six-dimensional superconformal N = (2; 0) field theory, which reduces to SYM after further compactification. We then use this geometric setting to connect to the complete nilpotent orbit classification of codimension-two defects, and find relations to ADE-type Toda CFT. We highlight the differences between the defect classification in the little string theory and its (2; 0) CFT limit, and find physical insights into nilpotent orbits and their classification by Bala{Carter labels and weighted Dynkin diagrams. i Contents Contents i 1 Introduction1 1.1 Little string theory................................ 2 1.2 Six-Dimensional (2; 0) Superconformal Field Theory ............. 3 1.3 Gukov{Witten Surface Defects of N = 4 SYM................ -
Flippable Tilings of Constant Curvature Surfaces
FLIPPABLE TILINGS OF CONSTANT CURVATURE SURFACES FRANÇOIS FILLASTRE AND JEAN-MARC SCHLENKER Abstract. We call “flippable tilings” of a constant curvature surface a tiling by “black” and “white” faces, so that each edge is adjacent to two black and two white faces (one of each on each side), the black face is forward on the right side and backward on the left side, and it is possible to “flip” the tiling by pushing all black faces forward on the left side and backward on the right side. Among those tilings we distinguish the “symmetric” ones, for which the metric on the surface does not change under the flip. We provide some existence statements, and explain how to parameterize the space of those tilings (with a fixed number of black faces) in different ways. For instance one can glue the white faces only, and obtain a metric with cone singularities which, in the hyperbolic and spherical case, uniquely determines a symmetric tiling. The proofs are based on the geometry of polyhedral surfaces in 3-dimensional spaces modeled either on the sphere or on the anti-de Sitter space. 1. Introduction We are interested here in tilings of a surface which have a striking property: there is a simple specified way to re-arrange the tiles so that a new tiling of a non-singular surface appears. So the objects under study are actually pairs of tilings of a surface, where one tiling is obtained from the other by a simple operation (called a “flip” here) and conversely. The definition is given below. -
Visualization of Regular Maps
Symmetric Tiling of Closed Surfaces: Visualization of Regular Maps Jarke J. van Wijk Dept. of Mathematics and Computer Science Technische Universiteit Eindhoven [email protected] Abstract The first puzzle is trivial: We get a cube, blown up to a sphere, which is an example of a regular map. A cube is 2×4×6 = 48-fold A regular map is a tiling of a closed surface into faces, bounded symmetric, since each triangle shown in Figure 1 can be mapped to by edges that join pairs of vertices, such that these elements exhibit another one by rotation and turning the surface inside-out. We re- a maximal symmetry. For genus 0 and 1 (spheres and tori) it is quire for all solutions that they have such a 2pF -fold symmetry. well known how to generate and present regular maps, the Platonic Puzzle 2 to 4 are not difficult, and lead to other examples: a dodec- solids are a familiar example. We present a method for the gener- ahedron; a beach ball, also known as a hosohedron [Coxeter 1989]; ation of space models of regular maps for genus 2 and higher. The and a torus, obtained by making a 6 × 6 checkerboard, followed by method is based on a generalization of the method for tori. Shapes matching opposite sides. The next puzzles are more challenging. with the proper genus are derived from regular maps by tubifica- tion: edges are replaced by tubes. Tessellations are produced us- ing group theory and hyperbolic geometry. The main results are a generic procedure to produce such tilings, and a collection of in- triguing shapes and images. -
Representations of Quivers & Gabriel's Theorem
Level 5M Project: Representations of Quivers & Gabriel's Theorem Emma Cummin (0606574) March 24, 2011 Abstract Gabriel's theorem, first proved by Peter Gabriel in 1972 [1], comes in two parts. Part (i) states that \a quiver Q is of finite orbit type if and only if each component of its underlying undirected graph Q^ is a simply{laced Dynkin diagram" and part (ii) states \let Q be a quiver such that Q^ is a simply{laced Dynkin diagram; then n is the dimension of a (unique) indecomposable representation of Q if and only if n 2 Φ+" [2]. This surprising theorem gives a deceptively simply result which links isomorphism classes of representations of a given quiver with an assigned dimension vector, with the root system of the geometric object underlying such a quiver. This project introduces quivers and representation theory to the reader, with the intention of heading towards proving Gabriel's theorem. This is the main result in the project, and so a proof of both parts is provided. On the way, the reader is introduced to quivers, the category of quiver representations and its equivalence with the category of KQ{modules, Dynkin diagrams, root systems and the Weyl group and the Coxeter functors. 1 Contents 1 Introduction 3 2 Quiver Representations and Categories 4 2.1 Quivers and Representations . .4 2.1.1 Introduction to Quivers . .4 2.1.2 The Kroenecker Quiver . .5 2.2 Path Algebras . .7 2.3 Introduction to Category Theory . .8 2.4 Equivalence of Categories . 11 3 Geometric Interpretation of Isomorphism Classes of Quiver Representa- tions 15 3.1 The Representation Space . -
Geometry in Design Geometrical Construction in 3D Forms by Prof
D’source 1 Digital Learning Environment for Design - www.dsource.in Design Course Geometry in Design Geometrical Construction in 3D Forms by Prof. Ravi Mokashi Punekar and Prof. Avinash Shide DoD, IIT Guwahati Source: http://www.dsource.in/course/geometry-design 1. Introduction 2. Golden Ratio 3. Polygon - Classification - 2D 4. Concepts - 3 Dimensional 5. Family of 3 Dimensional 6. References 7. Contact Details D’source 2 Digital Learning Environment for Design - www.dsource.in Design Course Introduction Geometry in Design Geometrical Construction in 3D Forms Geometry is a science that deals with the study of inherent properties of form and space through examining and by understanding relationships of lines, surfaces and solids. These relationships are of several kinds and are seen in Prof. Ravi Mokashi Punekar and forms both natural and man-made. The relationships amongst pure geometric forms possess special properties Prof. Avinash Shide or a certain geometric order by virtue of the inherent configuration of elements that results in various forms DoD, IIT Guwahati of symmetry, proportional systems etc. These configurations have properties that hold irrespective of scale or medium used to express them and can also be arranged in a hierarchy from the totally regular to the amorphous where formal characteristics are lost. The objectives of this course are to study these inherent properties of form and space through understanding relationships of lines, surfaces and solids. This course will enable understanding basic geometric relationships, Source: both 2D and 3D, through a process of exploration and analysis. Concepts are supported with 3Dim visualization http://www.dsource.in/course/geometry-design/in- of models to understand the construction of the family of geometric forms and space interrelationships. -
Visualization of Regular Maps Scientific Visualization – Math Vis Vis – Human Computer Interaction – Visual Analytics – Parallel
2/2/2016 Visualization Eindhoven – information visualization – software visualization – perception – geographic visualization Visualization of Regular Maps scientific visualization – math vis vis – human computer interaction – visual analytics – parallel Jarke J. van Wijk Eindhoven University of Technology JCB 2016, Bordeaux Data : flow fields – trees – graphs – tables – mobile data – events – … Applications : software analysis – business cases – bioinformatics – … Can you draw a Seifert surface? Eindhoven 2004 Huh? Starting MathVis Arjeh Cohen Me Discrete geometry, Visualization algebra Seifert surface Eindhoven 2006 1 2/2/2016 Can you show 364 triangles in 3D? Aberdeenshire Sure! 2000 BC I’ll give you the Arjeh Cohenpattern, you can Me pick a nice shape. Discrete geometry, Visualization algebra Ok! Athens 450 BC Scottish Neolithic carved stone balls 8 12 20 8 12 20? 6 6 4 4 Platonic solids: perfectly symmetric Platonic solids: perfectly symmetric 2 2/2/2016 How to get more faces, How to get more faces, all perfectly symmetric? all perfectly symmetric? Use shapes with holes Aim only at topological symmetry 64 64 #faces? Königsberg 1893 3 2/2/2016 Adolf Hurwitz 1859-1919 max. #faces: 3 28(genus – 1) 7 Genus Faces Genus Faces 3 56 3 56 7 168 7 168 14 364 14 364 … … … … Can you show 364 triangles in 3D? New Orleans Sure! 2009 I’ll give you the three years later Arjeh pattern, you can Me Cohen pick a nice shape. Ok! 4 2/2/2016 The general puzzle Construct space models of regular maps Symmetric Tiling of Closed Surfaces: Visualization of