Structural Building Principles of Complex Face-Centered Cubic Intermetallics

Total Page:16

File Type:pdf, Size:1020Kb

Structural Building Principles of Complex Face-Centered Cubic Intermetallics Research Collection Journal Article Structural building principles of complex face-centered cubic intermetallics Author(s): Dshemuchadse, Julia; Jung, Daniel Y.; Steurer, Walter Publication Date: 2011-08 Permanent Link: https://doi.org/10.3929/ethz-a-009903920 Originally published in: Acta Crystallographica Section B: Structural Science 67(4), http://doi.org/10.1107/ S0108768111025390 Rights / License: In Copyright - Non-Commercial Use Permitted This page was generated automatically upon download from the ETH Zurich Research Collection. For more information please consult the Terms of use. ETH Library electronic reprint Acta Crystallographica Section B Structural Science, Crystal Engineering and Materials ISSN 2052-5192 Structural building principles of complex face-centered cubic intermetallics Julia Dshemuchadse, Daniel Y. Jung and Walter Steurer Acta Cryst. (2011). B67, 269–292 Copyright c International Union of Crystallography Author(s) of this paper may load this reprint on their own web site or institutional repository provided that this cover page is retained. Republication of this article or its storage in electronic databases other than as specified above is not permitted without prior permission in writing from the IUCr. For further information see http://journals.iucr.org/services/authorrights.html Acta Crystallographica Section B: Structural Science publishes papers in structural chem- istry and solid-state physics in which structure is the primary focus of the work reported. The central themes are the acquisition of structural knowledge from novel experimental observations or from existing data, the correlation of structural knowledge with physico- chemical and other properties, and the application of this knowledge to solve problems in the structural domain. The journal covers metals and alloys, inorganics and minerals, metal-organics and purely organic compounds. Crystallography Journals Online is available from journals.iucr.org Acta Cryst. (2011). B67, 269–292 Julia Dshemuchadse et al. · Complex face-centered cubic intermetallics feature articles Acta Crystallographica Section B Structural Structural building principles of complex face- Science centered cubic intermetallics ISSN 0108-7681 Julia Dshemuchadse, Daniel Y. Fundamental structural building principles are discussed for Received 14 February 2011 Jung and Walter Steurer* all 56 known intermetallic phases with approximately 400 or Accepted 28 June 2011 more atoms per unit cell and space-group symmetry F443 m, Fd3m, Fd33, Fm3m or Fm3c. Despite fundamental differences Laboratory of Crystallography, Department of in chemical composition, bonding and electronic band Materials, ETH Zurich, Wolfgang-Pauli-Strasse 10, 8093 Zurich, Switzerland structure, their complex crystal structures show striking similarities indicating common building principles. We demonstrate that the structure-determining elements are flat Correspondence e-mail: [email protected] and puckered atomic {110} layers stacked with periodicities 2p. The atoms on this set of layers, which intersect each other, form pentagon face-sharing endohedral fullerene-like clusters arranged in a face-centered cubic packing (f.c.c.). Due to their topological layer structure, all these crystal structures can be described as (p  p  p)=p3-fold superstructures of a common basic structure of the double-diamond type. The parameter p, with p = 3, 4, 7 or 11, is determined by the number of layers per repeat unit and the type of cluster packing, which in turn are controlled by chemical composition. 1. Introduction Why and how do complex intermetallic phases form with up to thousands of atoms per unit cell or even in a quasiperiodic way without a unit cell? How do all these atoms find their sites during crystal growth? How do their structures depend on chemical composition and do they have anything in common? All these questions are in the focus of our long-term study of the crystallography of complex intermetallics, periodic as well as quasiperiodic ones. In this first comprehensive classification of intermetallics with giant unit cells, we discuss all known f.c.c. structures in the range from approximately 400 up to more than 23 000 atoms per unit cell. Structural complexity can result from: (i) atomic size ratios geometrically hindering optimum atomic interactions and preventing the formation of atomic environment types (AETs), which can be packed efficiently; (ii) energetically favorable electronic band structures (e.g. pseudogaps at the Fermi energy, EF) based on odd stoichio- metries or large unit-cell dimensions; (iii) other parameters that are close to optimum but not optimum (pseudosymmetry) for a simple structural arrange- ment or packing such as a misfit between structural subunits as in composite (host/guest) or modulated structures. In some cases complex structures can be described as modulations or superstructures of rather simple basic struc- tures. We distinguish two classes of modulations: a simple modulation is a correlated displacement or substitution of atoms leading to a comparatively small deviation of the actual # 2011 International Union of Crystallography structure from the underlying basic structure, resulting in a Printed in Singapore – all rights reserved (in)commensuratly modulated structure. A complex modula- Acta Cryst. (2011). B67, 269–292 doi:10.1107/S0108768111025390 269 electronic reprint feature articles tion on the other hand results from a correlated displacement We want to emphasize that our goal is the crystallographic or substitution of atoms leading to the local formation of description of complex structures, to identify their structural clusters yielding a cluster-modulated structure; as we will show, building units and connectivities. A detailed analysis of this is the case for all structures discussed in the following. chemical bonding and the identification of chemically relevant There is no unique way to classify, describe and visualize the subunits such as polyanionic frameworks is beyond the scope crystal structure of a complex intermetallic compound. One of this study. should keep in mind that the visualization of a crystal struc- The paper is organized in the following way: in x2we ture in terms of clusters (in the meaning of structural building describe the data basis of the present study and introduce the blocks) or structure modules can be quite arbitrary. There are general packing principles and peculiarities we derived for some conventions and rules, such as the maximum-gap rule f.c.c. structures with giant unit cells; in xx3, 4 and 5 we apply (Brunner & Schwarze, 1971) for the definition of AETs, which our concept of cluster description, layer decomposition and can be seen, in some cases, as the first shell of a multi-shell average structure derivation to the 56 intermetallics grouped cluster. However, there are not usually such simple rules for according to their symmetries F443 m (39), Fd3m (9), Fd3 (1), higher-order cluster shells. Furthermore, even if one finds a Fm3m (4) or Fm3c (3); in x6 we discuss the results of ab initio topologically elucidating cluster-based description, this does calculations of representatives of the two most frequent not mean that it is supported from a crystal-chemical point of structure types and show that chemical bonding and electronic view, i.e. that the chemical bonds between atoms within a band structure differ significantly between all these geome- cluster differ from those outside a cluster. For a more detailed trically closely related structures. discussion of this problem see Steurer (2006) and Henley et al. (2006). In the following we will pragmatically utilize this kind of 2. Some peculiarities of complex f.c.c. intermetallics cluster description that proves to be most useful. This is the Our study is based on structures taken from Pearson’s Crystal case when it allows for a simpler representation of a structure Data database (PCD; Villars & Cenzual, 2009/10). Full which is simpler than any other geometrical description; it is structural information is only available for 10 655 of the 41 788 particularly justified if the clusters used are constituents of intermetallics1 included in this database. However, these more than just a single structure type. A useful cluster-based numbers refer to database entries and not necessarily to description relates complex structures to simpler ones, thereby structures of different compounds; for some compounds, more reducing the degree of complexity and unveiling the under- than one entry may exist based on different structure deter- lying packing principles. In this case of f.c.c. structures, the minations. We restrict our study to the fully determined fundamental endohedral pentagon face-sharing fullerene-like structures and start with the analysis of 1891 entries with cubic clusters form cubic close packing with the octahedral voids symmetry and focus first on the 842 with f.c.c. lattice filled with a second type of cluster. The choice of this kind of symmetry: Fm3 (4 entries), Fd3 (1 entry), F443 m (305 entries), cluster is particularly justified because it allows the family of Fm3m (249 entries), Fm3c (76 entries) and Fd3m (207 2 giant unit-cell structures cF444-Al63:6Ta 36:4, cFð5928 À xÞ- entries). Al56:6Cu3:9Ta 39:5 and cFð23256 À xÞ-Al55:4Cu5:4Ta 39:1 (Weber et The histogram in Fig. 1 lists the number of database entries al., 2009; Conrad et al., 2009) to be described in a unique way. of f.c.c. structures as a function of the number of atoms per unit cell. Obviously, the majority of f.c.c. structures has unit cells with less than 200 atoms. Another significant clustering of structures is found at around 400 atoms per unit cell, while even larger structures are sparse. These are the structures we will focus on in the following, taking into account both their comparably high frequency and complexity. In this survey, we also consider the two recently discovered structures cFð5928 À xÞ-Al56:6Cu3:9Ta 39:5 and cFð23256 À xÞ- Al55:4Cu5:4Ta 39:1 (Weber et al., 2009; Conrad et al., 2009), with space-group symmetry F443 m, which are not included in the databases yet, as well as structures taken directly from the literature and another database, the ICSD (Belsky et al., 2002).
Recommended publications
  • 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.
    [Show full text]
  • 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].
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • On Some Properties of Distance in TO-Space
    Aksaray University Aksaray J. Sci. Eng. Journal of Science and Engineering Volume 4, Issue 2, pp. 113-126 e-ISSN: 2587-1277 doi: 10.29002/asujse.688279 http://dergipark.gov.tr/asujse http://asujse.aksaray.edu.tr Available online at Research Article On Some Properties of Distance in TO-Space Zeynep Can* Department of Mathematics, Faculty of Science and Letters, Aksaray University, Aksaray 68100, Turkey ▪Received Date: Feb 12, 2020 ▪Revised Date: Dec 21, 2020 ▪Accepted Date: Dec 24, 2020 ▪Published Online: Dec 25, 2020 Abstract The aim of this work is to investigate some properties of the truncated octahedron metric introduced in the space in further studies on metric geometry. With this metric, the 3- dimensional analytical space is a Minkowski geometry which is a non-Euclidean geometry in a finite number of dimensions. In a Minkowski geometry, the unit ball is a certain symmetric closed convex set instead of the usual sphere in Euclidean space. The unit ball of the truncated octahedron geometry is a truncated octahedron which is an Archimedean solid. In this study, 2 first, metric properties of truncated octahedron distance, 푑푇푂, in ℝ has been examined by 3 metric approach. Then, by using synthetic approach some distance formulae in ℝ푇푂, 3- dimensional analytical space furnished with the truncated octahedron metric has been found. Keywords Metric, Convex polyhedra, Truncated octahedron, Distance of a point to a line, Distance of a point to a plane, Distance between two lines *Corresponding Author: Zeynep Can, [email protected], 0000-0003-2656-5555 2017-2020©Published by Aksaray University 113 Zeynep Can (2020).
    [Show full text]
  • 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).
    [Show full text]
  • [ENTRY POLYHEDRA] Authors: Oliver Knill: December 2000 Source: Translated Into This Format from Data Given In
    ENTRY POLYHEDRA [ENTRY POLYHEDRA] Authors: Oliver Knill: December 2000 Source: Translated into this format from data given in http://netlib.bell-labs.com/netlib tetrahedron The [tetrahedron] is a polyhedron with 4 vertices and 4 faces. The dual polyhedron is called tetrahedron. cube The [cube] is a polyhedron with 8 vertices and 6 faces. The dual polyhedron is called octahedron. hexahedron The [hexahedron] is a polyhedron with 8 vertices and 6 faces. The dual polyhedron is called octahedron. octahedron The [octahedron] is a polyhedron with 6 vertices and 8 faces. The dual polyhedron is called cube. dodecahedron The [dodecahedron] is a polyhedron with 20 vertices and 12 faces. The dual polyhedron is called icosahedron. icosahedron The [icosahedron] is a polyhedron with 12 vertices and 20 faces. The dual polyhedron is called dodecahedron. small stellated dodecahedron The [small stellated dodecahedron] is a polyhedron with 12 vertices and 12 faces. The dual polyhedron is called great dodecahedron. great dodecahedron The [great dodecahedron] is a polyhedron with 12 vertices and 12 faces. The dual polyhedron is called small stellated dodecahedron. great stellated dodecahedron The [great stellated dodecahedron] is a polyhedron with 20 vertices and 12 faces. The dual polyhedron is called great icosahedron. great icosahedron The [great icosahedron] is a polyhedron with 12 vertices and 20 faces. The dual polyhedron is called great stellated dodecahedron. truncated tetrahedron The [truncated tetrahedron] is a polyhedron with 12 vertices and 8 faces. The dual polyhedron is called triakis tetrahedron. cuboctahedron The [cuboctahedron] is a polyhedron with 12 vertices and 14 faces. The dual polyhedron is called rhombic dodecahedron.
    [Show full text]
  • UNIVERSITY of CALIFORNIA Los Angeles Design, Structural
    UNIVERSITY OF CALIFORNIA Los Angeles Design, Structural Characterization and Application of High Symmetry Protein Nanocages A dissertation submitted in partial satisfaction of the requirements for the degree Doctor of Philosophy in Chemistry by Kevin Alexander Cannon 2019 © Copyright by Kevin Alexander Cannon 2019 ABSTRACT OF THE DISSERTATION Design, Structural Characterization and Application of High Symmetry Protein Nanocages by Kevin Alexander Cannon Doctor of Philosophy in Chemistry University of California, Los Angeles, 2019 Professor Todd O. Yeates, Chair In nature, it is extremely common to find proteins that assemble into homo-oligomeric complexes from multiple copies of themselves. Almost half of known proteins form such complexes, most of which are cyclically or dihedrally symmetric. In some exceptional cases, however, protein molecules will self-assemble into much larger, closed three-dimensional geometries resembling the Platonic solids. Examples include icosahedral viral capsids, bacterial microcompartment shells, and octahedral ferritin assemblies. Protein scientists have studied and marveled at these exquisite protein cage structures for decades, and some have even ventured to produce novel types of protein cage assemblies unseen in nature through their own engineering efforts. In recent years, the field of protein design has seen striking progress in the development of design methodologies for taking proteins found in nature and modifying them to self-assemble into cages of tetrahedral, octahedral, or icosahedral point group symmetry, and these unique new ii types of protein assemblies are even beginning to find use in medicine, imaging, and biomaterials applications. My thesis work addresses both the design and application areas of the field of symmetric protein cage design.
    [Show full text]
  • 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.
    [Show full text]
  • Spectral Realizations of Graphs
    SPECTRAL REALIZATIONS OF GRAPHS B. D. S. \DON" MCCONNELL 1. Introduction 2 The boundary of the regular hexagon in R and the vertex-and-edge skeleton of the regular tetrahe- 3 dron in R , as geometric realizations of the combinatorial 6-cycle and complete graph on 4 vertices, exhibit a significant property: Each automorphism of the graph induces a \rigid" isometry of the figure. We call such a figure harmonious.1 Figure 1. A pair of harmonious graph realizations (assuming the latter in 3D). Harmonious realizations can have considerable value as aids to the intuitive understanding of the graph's structure, but such realizations are generally elusive. This note explains and explores a proposition that provides a straightforward way to generate an entire family of harmonious realizations of any graph: A matrix whose rows form an orthogonal basis of an eigenspace of a graph's adjacency matrix has columns that serve as coordinate vectors of the vertices of an harmonious realization of the graph. This is a (projection of a) spectral realization. The hundreds of diagrams in Section 42 illustrate that spectral realizations of graphs with a high degree of symmetry can have great visual appeal. Or, not: they may exist in arbitrarily-high- dimensional spaces, or they may appear as an uninspiring jumble of points in one-dimensional space. In most cases, they collapse vertices and even edges into single points, and are therefore only very rarely faithful. Nevertheless, spectral realizations can often provide useful starting points for visualization efforts. (A basic Mathematica recipe for computing (projected) spectral realizations appears at the end of Section 3.) Not every harmonious realization of a graph is spectral.
    [Show full text]
  • Local Symmetry Preserving Operations on Polyhedra
    Local Symmetry Preserving Operations on Polyhedra Pieter Goetschalckx Submitted to the Faculty of Sciences of Ghent University in fulfilment of the requirements for the degree of Doctor of Science: Mathematics. Supervisors prof. dr. dr. Kris Coolsaet dr. Nico Van Cleemput Chair prof. dr. Marnix Van Daele Examination Board prof. dr. Tomaž Pisanski prof. dr. Jan De Beule prof. dr. Tom De Medts dr. Carol T. Zamfirescu dr. Jan Goedgebeur © 2020 Pieter Goetschalckx Department of Applied Mathematics, Computer Science and Statistics Faculty of Sciences, Ghent University This work is licensed under a “CC BY 4.0” licence. https://creativecommons.org/licenses/by/4.0/deed.en In memory of John Horton Conway (1937–2020) Contents Acknowledgements 9 Dutch summary 13 Summary 17 List of publications 21 1 A brief history of operations on polyhedra 23 1 Platonic, Archimedean and Catalan solids . 23 2 Conway polyhedron notation . 31 3 The Goldberg-Coxeter construction . 32 3.1 Goldberg ....................... 32 3.2 Buckminster Fuller . 37 3.3 Caspar and Klug ................... 40 3.4 Coxeter ........................ 44 4 Other approaches ....................... 45 References ............................... 46 2 Embedded graphs, tilings and polyhedra 49 1 Combinatorial graphs .................... 49 2 Embedded graphs ....................... 51 3 Symmetry and isomorphisms . 55 4 Tilings .............................. 57 5 Polyhedra ............................ 59 6 Chamber systems ....................... 60 7 Connectivity .......................... 62 References
    [Show full text]
  • Paper Models of Polyhedra
    Paper Models of Polyhedra Gijs Korthals Altes Polyhedra are beautiful 3-D geometrical figures that have fascinated philosophers, mathematicians and artists for millennia Copyrights © 1998-2001 Gijs.Korthals Altes All rights reserved . It's permitted to make copies for non-commercial purposes only email: [email protected] Paper Models of Polyhedra Platonic Solids Dodecahedron Cube and Tetrahedron Octahedron Icosahedron Archimedean Solids Cuboctahedron Icosidodecahedron Truncated Tetrahedron Truncated Octahedron Truncated Cube Truncated Icosahedron (soccer ball) Truncated dodecahedron Rhombicuboctahedron Truncated Cuboctahedron Rhombicosidodecahedron Truncated Icosidodecahedron Snub Cube Snub Dodecahedron Kepler-Poinsot Polyhedra Great Stellated Dodecahedron Small Stellated Dodecahedron Great Icosahedron Great Dodecahedron Other Uniform Polyhedra Tetrahemihexahedron Octahemioctahedron Cubohemioctahedron Small Rhombihexahedron Small Rhombidodecahedron S mall Dodecahemiododecahedron Small Ditrigonal Icosidodecahedron Great Dodecahedron Compounds Stella Octangula Compound of Cube and Octahedron Compound of Dodecahedron and Icosahedron Compound of Two Cubes Compound of Three Cubes Compound of Five Cubes Compound of Five Octahedra Compound of Five Tetrahedra Compound of Truncated Icosahedron and Pentakisdodecahedron Other Polyhedra Pentagonal Hexecontahedron Pentagonalconsitetrahedron Pyramid Pentagonal Pyramid Decahedron Rhombic Dodecahedron Great Rhombihexacron Pentagonal Dipyramid Pentakisdodecahedron Small Triakisoctahedron Small Triambic
    [Show full text]