Point substitution processes for generating icosahedral tilings. Nobuhisa Fujita IMRAM, Tohoku University, Sendai , Japan

Similar documents
Self-interaction mass formula that relates all leptons and quarks to the electron

The graph of y = x (or y = ) consists of two branches, As x 0, y + ; as x 0, y +. x = 0 is the

GEOMETRICAL PHENOMENA IN THE PHYSICS OF SUBATOMIC PARTICLES. Eduard N. Klenov* Rostov-on-Don, Russia

Random Process Part 1

Lecture 2: Discrete-Time Signals & Systems. Reza Mohammadkhani, Digital Signal Processing, 2015 University of Kurdistan eng.uok.ac.

PHYSICS 489/1489 LECTURE 7: QUANTUM ELECTRODYNAMICS

Deepak Rajput

On the Hamiltonian of a Multi-Electron Atom

Decagonal quasicrystals

The Standard Model Lagrangian

First derivative analysis

COMPUTATIONAL NUCLEAR THERMAL HYDRAULICS

Combinatorial Networks Week 1, March 11-12

Basic Polyhedral theory

CPE702 Algorithm Analysis and Design Week 11 String Processing

Status of LAr TPC R&D (2) 2014/Dec./23 Neutrino frontier workshop 2014 Ryosuke Sasaki (Iwate U.)

Association (Part II)

Square of Hamilton cycle in a random graph

San José State University Aerospace Engineering AE 138 Vector-Based Dynamics for Aerospace Applications, Fall 2016

Outerplanar graphs and Delaunay triangulations

Multi-scale Analysis of Void Closure for Heavy Ingot Hot Forging

Approximation and Inapproximation for The Influence Maximization Problem in Social Networks under Deterministic Linear Threshold Model

Finite element discretization of Laplace and Poisson equations

Least Favorable Distributions to Facilitate the Design of Detection Systems with Sensors at Deterministic Locations

MATH 1080 Test 2-SOLUTIONS Spring

Propositional Logic. Combinatorial Problem Solving (CPS) Albert Oliveras Enric Rodríguez-Carbonell. May 17, 2018

Indexed Search Tree (Trie)

Large Scale Topology Optimization Using Preconditioned Krylov Subspace Recycling and Continuous Approximation of Material Distribution

Slide 1. Slide 2. Slide 3 DIGITAL SIGNAL PROCESSING CLASSIFICATION OF SIGNALS

The van der Waals interaction 1 D. E. Soper 2 University of Oregon 20 April 2012

Construction of asymmetric orthogonal arrays of strength three via a replacement method

Linear Non-Gaussian Structural Equation Models

Week 3: Connected Subgraphs

International Journal of Scientific & Engineering Research, Volume 6, Issue 7, July ISSN

Physica D. The semigroup approach to transport processes in networks. B. Dorn a, M. Kramar Fijavž b,c, R. Nagel a,, A. Radl a.

SOME PARAMETERS ON EQUITABLE COLORING OF PRISM AND CIRCULANT GRAPH.

EEO 401 Digital Signal Processing Prof. Mark Fowler

ph People Grade Level: basic Duration: minutes Setting: classroom or field site

Hydrogen Atom and One Electron Ions

Construction of Mimetic Numerical Methods

1 Minimum Cut Problem

Some icosahedral patterns and their isometries

Introduction to Arithmetic Geometry Fall 2013 Lecture #20 11/14/2013

cycle that does not cross any edges (including its own), then it has at least

Runaway Electrons and Current Dynamics During Tokamak Disruptions

Recall that by Theorems 10.3 and 10.4 together provide us the estimate o(n2 ), S(q) q 9, q=1

Lie Groups HW7. Wang Shuai. November 2015

Problem Set #2 Due: Friday April 20, 2018 at 5 PM.

Estimation of apparent fraction defective: A mathematical approach

Solution: APPM 1360 Final (150 pts) Spring (60 pts total) The following parts are not related, justify your answers:

Gamma-ray burst spectral evolution in the internal shock model

Dealing with quantitative data and problem solving life is a story problem! Attacking Quantitative Problems

A Non-Quadratic Irrationality Associated to an Enneagonal Quasiperiodic Tiling of the Plane

Higher-Order Discrete Calculus Methods

A Polynomial-Time Approximation Scheme for the Minimum-Connected Dominating Set in Ad Hoc Wireless Networks

DIELECTRIC AND MAGNETIC PROPERTIES OF MATERIALS

Computing and Communications -- Network Coding

DIFFERENTIAL EQUATION

Derangements and Applications

CS 361 Meeting 12 10/3/18

TuLiP: A Software Toolbox for Receding Horizon Temporal Logic Planning & Computer Lab 2

Higher order derivatives

Another view for a posteriori error estimates for variational inequalities of the second kind

perm4 A cnt 0 for for if A i 1 A i cnt cnt 1 cnt i j. j k. k l. i k. j l. i l

The pn junction: 2 Current vs Voltage (IV) characteristics

Division of Mechanics Lund University MULTIBODY DYNAMICS. Examination Name (write in block letters):.

Chemical Physics II. More Stat. Thermo Kinetics Protein Folding...

Limiting value of higher Mahler measure

Quasicrystals Structure and dynamics. M. de Boissieu SIMaP, Grenoble- INP, CNRS, UJF St Mar=n d Hères France.

Learning Spherical Convolution for Fast Features from 360 Imagery

Bifurcation Theory. , a stationary point, depends on the value of α. At certain values

SCHUR S THEOREM REU SUMMER 2005

ME469A Numerical Methods for Fluid Mechanics

TOPOLOGY DESIGN OF STRUCTURE LOADED BY EARTHQUAKE. Vienna University of Technology

Finding low cost TSP and 2-matching solutions using certain half integer subtour vertices

Chapter 6 Folding. Folding

ARIMA Methods of Detecting Outliers in Time Series Periodic Processes

MHD Effects in Laser-Produced Plasmas

Partition Information and its Transmission over Boolean Multi-Access Channels

ONE primary objective of many coordination processes is

Non-universal Gauge Bosons Z and the Process e + e f f

5. B To determine all the holes and asymptotes of the equation: y = bdc dced f gbd

Magnetic Neutron Scattering and Spin-Polarized Neutrons

Detection of Energetic Particles by a Network of HF Propagation Paths in Alaska

Characterizing and Estimating Block DCT Image Compression Quantization Parameters

Order-disorder transition in the Cd-Ca cubic approximant

VII. Quantum Entanglement

hep-lat/ Dec 93

Section 6.1. Question: 2. Let H be a subgroup of a group G. Then H operates on G by left multiplication. Describe the orbits for this operation.

Give the letter that represents an atom (6) (b) Atoms of A and D combine to form a compound containing covalent bonds.

(Upside-Down o Direct Rotation) β - Numbers

Outline. Why speech processing? Speech signal processing. Advanced Multimedia Signal Processing #5:Speech Signal Processing 2 -Processing-

INTEGRATION BY PARTS

A Sub-Optimal Log-Domain Decoding Algorithm for Non-Binary LDPC Codes

Ordering and correlation of cluster orientations in CaCd 6

Aim To manage files and directories using Linux commands. 1. file Examines the type of the given file or directory

State-space behaviours 2 using eigenvalues

3 Finite Element Parametric Geometry

ANALYSIS IN THE FREQUENCY DOMAIN

EE 6882 Statistical Methods for Video Indexing and Analysis

Transcription:

Point substitution procsss for gnrating icosahdral tilings Nobuhisa Fujita IMRAM, Tohoku Univrsity, Sndai 980-8577, Japan

Outlin Part I. 1. Basic icosahdral tilings 2. Point substitution procsss Part II. 3. Tilings constructd with PIRs 4. Canonical cll tilings 5. Toward icosahdral CCTs

Outlin Part I. 1. Basic icosahdral tilings 2. Point substitution procsss Part II. 3. Tilings constructd with PIRs 4. Canonical cll tilings 5. Toward icosahdral CCTs

Icosahdral QCs Icosahdral tilings ED pattrn along 5-fold axis of an icosahdral quasicrystal Mn icosahdra b-c packing of icosahdral clustrs (F-typ) basd on th rhombohdral tiling (Ammann-Kramr tiling). Modl of i -(Al-Mn), M. Audir and P. Guyot, Phil. Mag. B 53, L43 (1986)

T *(P) tiling (Ammann-Kramr tiling) Basic tils OR, AR (Ammann rhombohdra) 5-fold viw 2-fold viw M. Dunau and A. Katz, Phys. Rv. Ltt. 54, 2688 (1985). P. Kramr and R. Nri, Acta Cryst. A 40, 580 (1984).

1 2 3 4 5 6 ( ) = 1 0 1 0 1 0 0 1 0 1 1 0 6 5 4 3 2 1 τ τ τ τ τ τ Icosahdral basis st 2 5 1+ = τ th goldn man = 2 +τ 1

Icosahdral moduls } ) ( { : 6 6 6 5 5 4 4 3 3 2 2 1 1 Ζ + + + + + = j P n n n n n n n M Ζ[τ ] } ) ( 2, mod 0 { : 6 6 6 5 5 4 4 3 3 2 2 1 1 Ζ = + + + + + = j j j F n n n n n n n n M Ζ[τ ] [ 3 ] Ζ τ [1] T. Janssn, Acta Cryst. A 42 (1986) 261. [2] D. S. Rokhsar t al., Phys. Rv. B 35 (1987) 5487. [3] L.S. Lvitov and J. Rhynr, J. Physiqu 49 (1988) 1835. ( ) )} (111111 2 1 { : 6 6 6 6 5 5 4 4 3 3 2 2 1 1 + Ζ Ζ + + + + + = j I ν ν ν ν ν ν ν M intgr ring

Scal invarianc of th moduls M I : = M = M P F M P + 1 2 (111111) [ M + (100000) ] M + (1 11111) M + (111111) F F 1 2 F 1 2 V V o B B o τ-scaling τ B V τ τ B o τ V o M M M P F I τ 3 τ = = M τ = M M I F P

T *(2F) tiling (Kramr t al.) P. Kramr t al., in Symmtris in Scinc V: Algbraic Structurs, thir Rprsntions, Ralizations and Physical Applications, Ed. by B. Grubr t al., Plnum Prss, Nw York, 1991, pp. 395.

Outlin Part I. 1. Basic icosahdral tilings 2. Point substitution procsss Part II. 3. Tilings constructd with PIRs 4. Canonical cll tilings 5. Toward icosahdral CCTs

Point substitution procsss for dcagonal tilings R P H N. Fujita, Acta Cryst. A 65, 342 (2009)

Point substitution procsss for dcagonal tilings (1)Expansion (σ =τ 2 ) R P H N. Fujita, Acta Cryst. A 65, 342 (2009)

Point substitution procsss for dcagonal tilings (1)Expansion (σ =τ 2 ) (2)Plac S at vry vrtx R P H N. Fujita, Acta Cryst. A 65, 342 (2009)

Point substitution procsss for dcagonal tilings (1)Expansion (σ =τ 2 ) (2)Plac S at vry vrtx R P H N. Fujita, Acta Cryst. A 65, 342 (2009)

Point substitution procsss for dcagonal tilings (1)Expansion (σ =τ 2 ) (2)Plac S at vry vrtx (3)Eliminat xcssiv points R P H N. Fujita, Acta Cryst. A 65, 342 (2009)

Point substitution procsss for dcagonal tilings (1)Expansion (σ =τ 2 ) (2)Plac S at vry vrtx (3)Eliminat xcssiv points R P H N. Fujita, Acta Cryst. A 65, 342 (2009)

Point substitution procsss for dcagonal tilings (1)Expansion (σ =τ 2 ) (2)Plac S at vry vrtx (3)Eliminat xcssiv points R P H N. Fujita, Acta Cryst. A 65, 342 (2009)

Window N. Fujita, Acta Cryst. A 65, 342 (2009)

Point Substitution Procss (for constructing icosahdral quasipriodic tilings) (1)Expansiv similarity transformation: T i σ T i (T i M, σ =ρ n, ρ=τ 3 (P), τ(f), τ(i)) (2) Rplicat th I h -star at vry vrtx: T i = σ T i + S (S M) (3) Dcimation of points by local ruls: T i T i+1 ( T i ) N. Fujita, Acta Cryst. A 65, 342 (2009) Stp (3) is ndd if thr is rdundancy in th points gnratd through (1) and (2) ( Point inflation rul) K. Niizki, J.Phys.A:Math.Thor.41,175208 (2008)

Outlin Part I. 1. Basic icosahdral tilings 2. Point substitution procsss Part II. 3. Tilings constructd with PIRs 4. Canonical cll tilings 5. Toward icosahdral CCTs

Windows T *(P) P-typ T *(2F) F-typ 1 τ 1 Point dnsity W P Ω P 3 W F τ W = Ω 2 Ω F P P

I h -star S 1: (000000) 1 2 : (1 1 1 1 1 2 3: (111000) 1)

Point inflation rul (viwd in th xtrnal spac) sd 1 st itration 2 nd itration τ τ Q (S,τ)

I h -star (mappd to th intrnal spac) S T 1: (000000) 1 2 : (1 1 1 1 1 2 3: (111000) 1)

in th intrnal spac 1 window 1: (000000) 1 1 + L = 1 τ 1 2 3 4 5 + τ + τ + τ + τ + τ 1 2 = τ = 2.61803 1 2 : (1 1 1 1 1 2 3: (111000) 1)

5-fold dirction Q (S,τ) M P

Inflation rul of th Ammann- Kramr tiling Inflation ruls by τ 3 scaling T. Ogawa, J. Phys. Soc. Jpn. 54, 3205 (1985).

Outlin Part I. 1. Basic icosahdral tilings 2. Point substitution procsss Part II. 3. Tilings constructd with PIRs 4. Canonical cll tilings 5. Toward icosahdral CCTs

Canonical cll tiling 4 polyhdra: A-, B-, C-, D-clls Cll gomtry for clustr-basd quasicrystal modls, C. L. Hnly, Phys. Rv. B 43 (1991) 993. A-cll B-cll C-cll D-cll c c c c b c c b c b c b b b b b c c b c b b c b c c b b b Thr ar 32 classs of nods in a CCT (68) 0 (62) 222222 (67) 333

i-cdcanonical 5.7 Yb: Quasicrystal Cll Tiling (QC) RTH AR H. Takakura & C.P. Gomz t al., (2007). M. Mihalkovic t al., Phys. Rv. B 53, 9002-9020 (1996).

M. Mihalkovic t al., Phys. Rv. B 53, 9002-9020 (1996).

Outlin Part I. 1. Basic icosahdral tilings 2. Point substitution procsss Part II. 3. Tilings constructd with PIRs 4. Canonical cll tilings 5. Toward icosahdral CCTs

Is thr an icosahdral CCT? NO PROOF is givn of th xistnc of an ICOSAHEDRAL CCT Mthods to construct approximant CCTs (undr priodic boundary conditions) A Mont Carlo dnsity optimization mthod: M. Mihalkovic and P. Mrafko, Europhys. Ltt. 21 (1993) 463. A brut forc algorithm: M.E.J. Nwman, C.L. Hnly, and M. Oxborrow, Phil. Mag. B 71 (1995) 991.

Point sutstitution procsss for icosahdral CCTs I h -star th magic star 5-fold viw

Th I h -star is placd on vry vrtx of th xpandd CCT (scaling ratio=τ 3 )

Fix th cntr to b th (68) 0 typ nod. Th I h -star

A-packing (body cntrd cubic) 2 vrtics 12 A-clls 0 B-cll 0 C-cll 0 D-cll 138 vrtics 348 A-clls 136 B-clls 136 C-clls 24 D-clls

BC-packing (rhombohdral) 1 vrtx 0 A-cll 2 B-clls 2 C-clls 0 D-cll 77 vrtics 192 A-clls 76 B-clls 76 C-clls 14 D-clls

D-packing (simpl hxagonal) (67) 333 Th cntr is missing! 1 vrtx 0 A-clls 0 B-clls 0 C-clls 2 D-clls

D-packing (simpl hxagonal) (67) 333 Th cntr is missing! 1 vrtx 0 A-clls 0 B-clls 0 C-clls 2 D-clls 103 vrtics 252 A-clls 102 B-clls 102 C-clls 20 D-clls

τ 3 A-packing τ 3 D-packing τ 3 BC-packing 138 vrtics 348 A-clls 136 B-clls 136 C-clls 24 D-clls τ 3 2/1 cubic-packing 103 vrtics 252 A-clls 102 B-clls 102 C-clls 20 D-clls 77 vrtics 192 A-clls 76 B-clls 76 C-clls 14 D-clls 584 vrtics 1464 A-clls 576 B-clls 576 C-clls 104 D-clls

Conclusion Th prsnt schm has turnd out to b usful for constructing icosahdral tilings. Th magic star can gnrat all th vrtics of an inflatd CCT xcpt a point in th cntr of ach xpandd D-cll. It is likly that thr xist τ 3 -inflation ruls for gnrating an icosahdral CCT, th proof of which still nds to b workd out.