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The Cubic Groups
The Cubic Groups Baccalaureate Thesis in Electrical Engineering Author: Supervisor: Sana Zunic Dr. Wolfgang Herfort 0627758 Vienna University of Technology May 13, 2010 Contents 1 Concepts from Algebra 4 1.1 Groups . 4 1.2 Subgroups . 4 1.3 Actions . 5 2 Concepts from Crystallography 6 2.1 Space Groups and their Classification . 6 2.2 Motions in R3 ............................. 8 2.3 Cubic Lattices . 9 2.4 Space Groups with a Cubic Lattice . 10 3 The Octahedral Symmetry Groups 11 3.1 The Elements of O and Oh ..................... 11 3.2 A Presentation of Oh ......................... 14 3.3 The Subgroups of Oh ......................... 14 2 Abstract After introducing basics from (mathematical) crystallography we turn to the description of the octahedral symmetry groups { the symmetry group(s) of a cube. Preface The intention of this account is to provide a description of the octahedral sym- metry groups { symmetry group(s) of the cube. We first give the basic idea (without proofs) of mathematical crystallography, namely that the 219 space groups correspond to the 7 crystal systems. After this we come to describing cubic lattices { such ones that are built from \cubic cells". Finally, among the cubic lattices, we discuss briefly the ones on which O and Oh act. After this we provide lists of the elements and the subgroups of Oh. A presentation of Oh in terms of generators and relations { using the Dynkin diagram B3 is also given. It is our hope that this account is accessible to both { the mathematician and the engineer. The picture on the title page reflects Ha¨uy'sidea of crystal structure [4]. -
Can Every Face of a Polyhedron Have Many Sides ?
Can Every Face of a Polyhedron Have Many Sides ? Branko Grünbaum Dedicated to Joe Malkevitch, an old friend and colleague, who was always partial to polyhedra Abstract. The simple question of the title has many different answers, depending on the kinds of faces we are willing to consider, on the types of polyhedra we admit, and on the symmetries we require. Known results and open problems about this topic are presented. The main classes of objects considered here are the following, listed in increasing generality: Faces: convex n-gons, starshaped n-gons, simple n-gons –– for n ≥ 3. Polyhedra (in Euclidean 3-dimensional space): convex polyhedra, starshaped polyhedra, acoptic polyhedra, polyhedra with selfintersections. Symmetry properties of polyhedra P: Isohedron –– all faces of P in one orbit under the group of symmetries of P; monohedron –– all faces of P are mutually congru- ent; ekahedron –– all faces have of P the same number of sides (eka –– Sanskrit for "one"). If the number of sides is k, we shall use (k)-isohedron, (k)-monohedron, and (k)- ekahedron, as appropriate. We shall first describe the results that either can be found in the literature, or ob- tained by slight modifications of these. Then we shall show how two systematic ap- proaches can be used to obtain results that are better –– although in some cases less visu- ally attractive than the old ones. There are many possible combinations of these classes of faces, polyhedra and symmetries, but considerable reductions in their number are possible; we start with one of these, which is well known even if it is hard to give specific references for precisely the assertion of Theorem 1. -
Chapter 3: Transformations Groups, Orbits, and Spaces of Orbits
Preprint typeset in JHEP style - HYPER VERSION Chapter 3: Transformations Groups, Orbits, And Spaces Of Orbits Gregory W. Moore Abstract: This chapter focuses on of group actions on spaces, group orbits, and spaces of orbits. Then we discuss mathematical symmetric objects of various kinds. May 3, 2019 -TOC- Contents 1. Introduction 2 2. Definitions and the stabilizer-orbit theorem 2 2.0.1 The stabilizer-orbit theorem 6 2.1 First examples 7 2.1.1 The Case Of 1 + 1 Dimensions 11 3. Action of a topological group on a topological space 14 3.1 Left and right group actions of G on itself 19 4. Spaces of orbits 20 4.1 Simple examples 21 4.2 Fundamental domains 22 4.3 Algebras and double cosets 28 4.4 Orbifolds 28 4.5 Examples of quotients which are not manifolds 29 4.6 When is the quotient of a manifold by an equivalence relation another man- ifold? 33 5. Isometry groups 34 6. Symmetries of regular objects 36 6.1 Symmetries of polygons in the plane 39 3 6.2 Symmetry groups of some regular solids in R 42 6.3 The symmetry group of a baseball 43 7. The symmetries of the platonic solids 44 7.1 The cube (\hexahedron") and octahedron 45 7.2 Tetrahedron 47 7.3 The icosahedron 48 7.4 No more regular polyhedra 50 7.5 Remarks on the platonic solids 50 7.5.1 Mathematics 51 7.5.2 History of Physics 51 7.5.3 Molecular physics 51 7.5.4 Condensed Matter Physics 52 7.5.5 Mathematical Physics 52 7.5.6 Biology 52 7.5.7 Human culture: Architecture, art, music and sports 53 7.6 Regular polytopes in higher dimensions 53 { 1 { 8. -
New Perspectives on Polyhedral Molecules and Their Crystal Structures Santiago Alvarez, Jorge Echeverria
New Perspectives on Polyhedral Molecules and their Crystal Structures Santiago Alvarez, Jorge Echeverria To cite this version: Santiago Alvarez, Jorge Echeverria. New Perspectives on Polyhedral Molecules and their Crystal Structures. Journal of Physical Organic Chemistry, Wiley, 2010, 23 (11), pp.1080. 10.1002/poc.1735. hal-00589441 HAL Id: hal-00589441 https://hal.archives-ouvertes.fr/hal-00589441 Submitted on 29 Apr 2011 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Journal of Physical Organic Chemistry New Perspectives on Polyhedral Molecules and their Crystal Structures For Peer Review Journal: Journal of Physical Organic Chemistry Manuscript ID: POC-09-0305.R1 Wiley - Manuscript type: Research Article Date Submitted by the 06-Apr-2010 Author: Complete List of Authors: Alvarez, Santiago; Universitat de Barcelona, Departament de Quimica Inorganica Echeverria, Jorge; Universitat de Barcelona, Departament de Quimica Inorganica continuous shape measures, stereochemistry, shape maps, Keywords: polyhedranes http://mc.manuscriptcentral.com/poc Page 1 of 20 Journal of Physical Organic Chemistry 1 2 3 4 5 6 7 8 9 10 New Perspectives on Polyhedral Molecules and their Crystal Structures 11 12 Santiago Alvarez, Jorge Echeverría 13 14 15 Departament de Química Inorgànica and Institut de Química Teòrica i Computacional, 16 Universitat de Barcelona, Martí i Franquès 1-11, 08028 Barcelona (Spain). -
Molecular Symmetry 6
Molecular symmetry 6 Symmetry governs the bonding and hence the physical and spectroscopic properties of molecules. An introduction to symmetry In this chapter we explore some of the consequences of molecular symmetry and introduce the analysis systematic arguments of group theory. We shall see that symmetry considerations are essential for 6.1 Symmetry operations, elements constructing molecular orbitals and analysing molecular vibrations. They also enable us to extract and point groups information about molecular and electronic structure from spectroscopic data. 6.2 Character tables The systematic treatment of symmetry makes use of a branch of mathematics called group Applications of symmetry theory. Group theory is a rich and powerful subject, but we shall confine our use of it at 6.3 Polar molecules this stage to the classification of molecules in terms of their symmetry properties, the con- 6.4 Chiral molecules struction of molecular orbitals, and the analysis of molecular vibrations and the selection 6.5 Molecular vibrations rules that govern their excitation. We shall also see that it is possible to draw some general conclusions about the properties of molecules without doing any calculations at all. The symmetries of molecular orbitals 6.6 Symmetry-adapted linear combinations 6.7 The construction of molecular orbitals An introduction to symmetry analysis 6.8 The vibrational analogy That some molecules are ‘more symmetrical’ than others is intuitively obvious. Our aim Representations though, is to define the symmetries of individual molecules precisely, not just intuitively, 6.9 The reduction of a representation and to provide a scheme for specifying and reporting these symmetries. -
The Double Cover of the Icosahedral Symmetry Group and Quark Mass
MADPHYS-10-1566 The Double Cover of the Icosahedral Symmetry Group and Quark Mass Textures Lisa L. Everett and Alexander J. Stuart Department of Physics, University of Wisconsin, Madison, WI, 53706, USA (Dated: October 25, 2018) We investigate the idea that the double cover of the rotational icosahedral symmetry group is the family symmetry group in the quark sector. The icosahedral ( 5) group was previously proposed as a viable family symmetry group for the leptons. To incorporateA the quarks, it is highly advantageous to extend the group to its double cover, as in the case of tetrahedral (A4) symmetry. We provide the basic group theoretical tools for flavor model-building based on the binary icosahedral group ′ and construct a model of the quark masses and mixings that yields many of the successful predictionsI of the well-known U(2) quark texture models. PACS numbers: 12.15Ff,12.60.Jv I. INTRODUCTION With the measurement of neutrino oscillations [1–6], an intriguing pattern of lepton mixing has emerged. The neu- trino oscillation data have revealed that two of the mixing angles of the Maki-Nakagawa-Sakata-Pontecorvo (MNSP) [8] mixing matrix are large and the third angle is bounded from above by the Cabibbo angle (for global fits, see [7]). This pattern, with its striking differences from the quark mixing angles of the Cabibbo-Kobayashi-Maskawa (CKM) matrix, has shifted the paradigm for addressing the Standard Model (SM) flavor puzzle. More precisely, while the quark sector previously indicated a flavor model-building framework based on the Froggatt- Nielsen mechanism [10] with continuous family symmetries (see also [9]), the large lepton mixing angles suggest discrete non-Abelian family symmetries. -
Hamiltonian Cycles on Symmetrical Graphs
BRIDGES Mathematical Connections in Art, Music, and Science Hamiltonian Cycles on Symmetrical Graphs Carlo H. Sequin Computer Science Division, EECS Department University of California, Berkeley, CA 94720 E-mail: [email protected] Abstract The edges of highly-connected symmetrical graphs are colored so that they form Hamiltonian cycles. As an introduction we discuss the coloring of the complete graphs K2m+1 for m> 1, but the focus is on the graphs resulting from symmetrical perspective projections of the edges of the regu .Iar 4-dimensional polytopes into 3-space. The goal is to color all edges in these graphs with multi ple congruent copies of Hamiltonian cycles exhibiting as much symmetry as possible. Figure 1: Map of Konigsberg (a) and equivalent graph (b). 1. Introduction In 1735, Euler learned of.a popular problem in the town of Konigsberg: Is it possible to cross all seven bridges in this town exactly once and then return to the starting point? This can be seen as a graph problem. With a suitable degree of abstraction, the city map can be reduced to a graph (Fig. 1) with just seven edges, i.e., the seven bridges, and with just four nodes representing the quarters in town from which these bridges emerge. Euler quickly showed that the desired tour was not possible, and as a generalization of the Konigs berg bridge problem, also showed (without proof) that a connected graph has an Eulerian circuit iff it has no vertices of odd valence. In this context, let's review the following definitions: • Euler Path: A path on a graph whose edges consist of all graph edges. -
An Introduction to Molecular Symmetry
Chapter 3 An introduction to molecular symmetry TOPICS & Symmetry operators and symmetry elements & Point groups & An introduction to character tables & Infrared spectroscopy & Chiral molecules the resulting structure is indistinguishable from the first; 3.1 Introduction another 1208 rotation results in a third indistinguishable molecular orientation (Figure 3.1). This is not true if we Within chemistry, symmetry is important both at a molecu- carry out the same rotational operations on BF2H. lar level and within crystalline systems, and an understand- Group theory is the mathematical treatment of symmetry. ing of symmetry is essential in discussions of molecular In this chapter, we introduce the fundamental language of spectroscopy and calculations of molecular properties. A dis- group theory (symmetry operator, symmetry element, point cussion of crystal symmetry is not appropriate in this book, group and character table). The chapter does not set out to and we introduce only molecular symmetry. For qualitative give a comprehensive survey of molecular symmetry, but purposes, it is sufficient to refer to the shape of a molecule rather to introduce some common terminology and its using terms such as tetrahedral, octahedral or square meaning. We include in this chapter an introduction to the planar. However, the common use of these descriptors is vibrational spectra of simple inorganic molecules, with an not always precise, e.g. consider the structures of BF3, 3.1, emphasis on using this technique to distinguish between pos- and BF2H, 3.2, both of which are planar. A molecule of sible structures for XY2,XY3 and XY4 molecules. Complete BF3 is correctly described as being trigonal planar, since its normal coordinate analysis of such species is beyond the symmetry properties are fully consistent with this descrip- remit of this book. -
Spherical Symmetries from Dynamics
Computers Math. Applic. Vol. 29, No. 7, pp. 67-81, 1995 Pergamon Copyright©1995 Elsevier Science Ltd Printed in Great Britain. All rights reserved 0898-1221/95 $9.50+ 0.00 0898-1221(95)00019-4 Spherical Symmetries from Dynamics K. W. CHUNG AND H. S. Y. CHAN Department of Mathematics, City University of Hong Kong Kowloon, Hong Kong Dedicated to the memory of Professor Feng Kang (Received January 1994; revised and accepted June 1994) Abstract--Computer generation of colored spherical patterns is considered from a dynamical system's point of view. To demonstrate the generality of the method, colored patterns related to the five Platonic solids are constructed. The method is able to create unlimited varieties of patterns and can be extended to create patterns with symmetric groups of finite orders. Keywords--Computer graphics, Dynamical systems, Spherical tessellations, Symmetric groups, Generators of a group. 1. INTRODUCTION The study of symmetrical forms has long occupied human interest. Modern considerations with the aid of the computer have become prolific; see for example [1,2]. To relate such static concept in terms of dynamical modeling is, however, more recent. Dynamical systems describe the way some quantities undergo changes through time. Studies of the behavior of these systems are important in sciences and engineering. Graphical presentations have aided in the understanding of complex dynamical behavior, of which symmetry is a fundamental concept [3-5]. The understanding of symmetry on various spaces and manifolds has both scientific and artistic appeal. For example, symmetry in Euclidean plane was considered in [5]. Symmetry in hyperbolic geometry was considered in [6]. -
Tetrahedral Symmetry and the Graviton 1 Introduction
International Mathematical Forum, 2, 2007, no. 31, 1537 - 1551 Tetrahedral Symmetry and the Graviton J. A. de Wet Box 514, Plettenberg Bay, 6600, South Africa Abstract We attempt to give a purely geometric interpretation of the Standard Model and trace of the graviton. The concept of a ”point” particle is replaced by fundamental symmetries assumed to characterize physical space. In particular the construction rests on Equation (1) which is an irreducible representation (or IR) of the Dirac ring, in line with some of Einstein’s last ideas that view ”particles” not as objects sitting in space-time but rather as parts of space-time itself.Essentially (1), governing the nucleon,imposes tetrahedral symmetry and consequently the Clebsch cubic of Fig.4 that carries the famous 27 lines that will be identified with E6 and the Standard Model.A section is the Cayley cubic of Fig.6 that shows a circle belonging to a photon γ. To find the other half of the Standard Model we study E7 , homomorphic to the binary octahedral group,, that introduces the product γ.γ with spin 2 thought to represent the graviton. Mathematics Subject Classification: 14J30, 22E70, 81V05, 81V35 Keywords: Standard Model, Quarks, Gluon Condensate, Clebsch Cubic, Strong Interaction, Graviton 1 Introduction In his book [14] Penrose, Section 22.1,refers to a point particle as a myste- rious spread out wavy thing in the quantum formalism. Such a ”spread out wave” may account for the Uncertainty Principle and for quantum entangle- ment where entangled ”particles” ,described by the wave function,may inter- act at a distance. -
Polyhedral-Edge Knots
Polyhedral-Edge Knots Carlo H. Séquin CS Division, University of California, Berkeley; [email protected] Abstract Mathematical knots are severely restricted in the symmetries they can exhibit; they cannot assume the symmetries of the Platonic solids. An approach is presented that forms tubular knot sculptures that display in their overall structure the shapes of regular or semi-regular polyhedra: The knot strand passes along all the edges of such a polyhedron once or twice, so that an Eulerian circuit can be formed. Results are presented in the form of small 3D prints. 1. Introduction Several artists have used tubular representations of mathematical knots and links to make attractive constructivist sculptures (Figure 1). Often, they try to make these sculptures as symmetrical as possible (Figures 1c, 1d); but there are restrictions how symmetrical a mathematical knot can be made. Section 2 reviews the symmetry types that are achievable by mathematical knots. Subsequently I explore ways in which I can design knot sculptures so that their overall shape approximates the higher-order symmetries exhibited by the Platonic and Archimedean solids. (a) (b) (c) (d) Figure 1: Knot sculptures: (a) de Rivera: “Construction #35” [2]. (b) Zawitz: “Infinite Trifoil” [11]. (c) Escher: “The Knot” [3]. (d) Finegold: “Torus (3,5) Knot” [4]. 2. The Symmetries of Knots All finite 3-dimensional objects fall into one of 14 possible symmetry families. First, there are the seven roughly spherical Platonic symmetries (Figure 2) derived from the regular and semi-regular polyhedra. The first three are: Td, the tetrahedral symmetry; Oh, the octahedral (or cube) symmetry; and Ih, the icosahedral (or dodecahedral) symmetry. -
Hamiltonian Cycles on Symmetrical Graphs
Hamiltonian Cycles on Symmetrical Graphs Carlo H. Séquin Computer Science Division, EECS Department University of California, Berkeley, CA 94720 E-mail: [email protected] Abstract The edges of highly-connected symmetrical graphs are colored so that they form Hamiltonian cycles. As an introduction we discuss the coloring of the complete graphs K2m+1 for m>1, but the focus is on the graphs resulting from symmetrical perspective projections of the edges of the regu- lar 4-dimensional polytopes into 3-space. The goal is to color all edges in these graphs with multi- ple congruent copies of Hamiltonian cycles exhibiting as much symmetry as possible. Figure 1: Map of Königsberg (a) and equivalent graph (b). 1. Introduction In 1735, Euler learned of a popular problem in the town of Königsberg: Is it possible to cross all seven bridges in this town exactly once and then return to the starting point? This can be seen as a graph problem. With a suitable degree of abstraction, the city map can be reduced to a graph (Fig.1) with just seven edges, i.e., the seven bridges, and with just four nodes representing the quarters in town from which these bridges emerge. Euler quickly showed that the desired tour was not possible, and as a generalization of the Königs- berg bridge problem, also showed (without proof) that a connected graph has an Eulerian circuit iff it has no vertices of odd valence. In this context, let’s review the following definitions: • Euler Path: A path on a graph whose edges consist of all graph edges.