Symmetry in 2D. 4/24/2013 L. Viciu AC II Symmetry in 2D

Size: px
Start display at page:

Download "Symmetry in 2D. 4/24/2013 L. Viciu AC II Symmetry in 2D"

Transcription

1 Symmetry in 2D 1

2 Outlook Symmetry: definitions, unit cell choice Symmetry operations in 2D Symmetry combinations Plane Point groups Plane (space) groups Finding the plane group: examples 2

3 Symmetry Symmetry is the preservation of form and configuration across a point, a line, or a plane. The techniques that are used to "take a shape and match it exactly to another are called transformations Inorganic crystals usually have the shape which reflects their internal symmetry 3

4 Lattice = an array of points repeating periodically in space (2D or 3D). Motif/Basis = the repeating unit of a pattern (ex. an atom, a group of atoms, a molecule etc.) Unit cell = The smallest repetitive volume of the crystal, which when stacked together with replication reproduces the whole crystal 4

5 Unit cell convention By convention the unit cell is chosen so that it is as small as possible while reflecting the full symmetry of the lattice (b) to (e) correct unit cell: choice of origin is arbitrary but the cells should be identical; (f) incorrect unit cell: not permissible to isolate unit cells from each other (1 and 2 are not identical) 5 A. West: Solid state chemistry and its applications

6 Some Definitions Symmetry element: An imaginary geometric entity (line, point, plane) about which a symmetry operation takes place Symmetry Operation: a permutation of atoms such that an object (molecule or crystal) is transformed into a state indistinguishable from the starting state Invariant point: point that maps onto itself Asymmetric unit: The minimum unit from which the structure can be generated by symmetry operations 6

7 From molecular point group to space groups Complete consideration of all symmetry elements and translation yields to the space groups benzene graphene graphite D6h or 6/mmm Point group p6mm Plane group = point group symmetry + in plane translation P6 3 /mmc Space group = point group symmetry + in 3D translation 7

8 Symmetry operations in 2D*: 1. translation 2. rotations 3. reflections 4. glide reflections Symmetry operations in 3D: the same as in 2D + inversion center, rotoinversions and screw axes * Besides identity 8

9 1. Translation ( move ) Translation moves all the points in the asymmetric unit the same distance in the same direction. There are no invariant points (points that map onto themselves) under a translation. Translation has no effect on the chirality of figures in the plane. 9

10 2. Rotations A rotation turns all the points in the asymmetric unit around one axis, the center of rotation. The center of rotation is the only invariant point. A rotation does not change the chirality of figures. 10

11 Symbols for symmetry axes Drawn symbol One fold rotation axis two fold rotation axis --- (monad) (diad) Axes perpendicular to the plane Axes parallel to the plane three fold rotation axis four fold rotation axis six fold rotation axis (triad) (Tetrad) (Hexad) CRYSTALS MOLECULES 11

12 3. Reflections A reflection flips all points in the asymmetric unit over a line called mirror. The points along the mirror line are all invariant points A reflection changes the chirality of any figures in the asymmetric unit Symbol: m Representation: a solid line 12

13 4. Glide Reflections Glide reflection reflects the asymmetric unit across a mirror and then translates it parallel to the mirror There are no invariant points under a glide reflection. A glide plane changes the chirality of figures in the asymmetric unit. Symbol: g Representation: a dashed line 13

14 Point group symmetry Point group = the collection of symmetry elements of an isolated shape Point group symmetry does not consider translation! The symmetry operations must leave every point in the lattice identical therefore the lattice symmetry is also described as the lattice point symmetry Plane symmetry group or plane crystallographic group is a mathematical classification of a two-dimensional repetitive pattern, based on the symmetries in the pattern 14

15 Examples of plane symmetry in architecture 15

16 Crystallographic plane point groups = (one fold axis) 6. m (mirror line) 2. 2 (two fold axis) 7. 2 mm (two mirror lines and a 2-fold axis)* 3. 3 (three fold axis) 8. 3 m (one 3-fold axis and three mirror lines) 4. 4 (four fold axis) 9. 4 mm (4-fold axis and four mirror lines)* 5. 6 (six fold axis) mm (6-fold axis and 6 mirror lines)* * Second m in the symbol refers to the second type of mirror line 16

17 5-fold, 7-fold, etc. axes are not compatible with translation non-periodic two dimensional patterns Ex: Starfish Non-periodic 2D patterns 5m (five fold axis + mirror) Wikipedia.org A Penrose tiling Group of atoms or viruses can form quasicrystals (quasicristals = ordered structural forms that are non-periodic) Electron diffraction of a Al-Mn quasicrystal showing 5-fold symmetry by Dan Shechtman 17

18 18

19 Combining symmetry operations Ten different plane point groups : 1, 2, 3, 4, 6, m, 2 mm, 3 m, 4 mm, 6 mm Five different cell lattice types: 1. oblique(parallelogram) (a b, 90 ) 2. Rectangular (a b, 90ᵒ) 3. Square (a = b, 90ᵒ) 4. Centered rectangular or diamond (a b, 90ᵒ) 5. Rhombic or hexagonal (a = b, 120ᵒ) When point group symmetries are combined with the possible lattice cells 17 plane groups. 19

20 1. Combining rotation with translation 1. The rotations will always be to the plane (the space in 2D) 2. An -fold rotation followed by translation to it gives another rotation of the same angle (same order), in the same sense 3. The new rotation will be located at a distance x = T/2 x cotg /2 along perpendicular bisector of T (T=cell edge translation) Ex: 2-fold rotation followed by translation ( =180 ) 180 A 1 B x T 2 3 is the motif The second rotation will be on T in the middle at B Steps: 1. 2-fold rotation through A moves the motif from 1 to 2 2. translation by T moves the motif from 2 to 3 Or 1. 2-fold rotation through B moves the motif from 1 to 3 20

21 Pair of motifs: 2-fold axis combined with translation T2 T1 T1 T1+T T fold rotation at 1 combined with translation T 1 gives the rotation 6 (rotation 6 is translated to 7 by T2) 2-fold rotation at 1 combined with translation T 2 gives the rotation 8 (rotation 8 is translated to 9 by T1) 2-fold rotation at 1 combined with translation T 1+T2 gives the rotation in the middle The blue, red, green and yellow marked are independent 2-fold axes: they relate different objects pair-wise in the pattern no any pair of the blue and one of the red, green or yellow 2-fold axis describe the same pair-wise relationship 21

22 6-fold axis combined with translation 6-fold axis contains 2 /6, 2 /3, 2 /2 rotations All the operations of a 3-fold axis combined with translation and of a 2-fold axis combined with translation will be included for a p6 plane group 22

23 Combination of the rotation axes with a plane lattice = translation Two fold axis Three fold axis Four non-equivalent 2-fold axes to the plane (0 0; ½ ½, ½ 0, 0 ½ ) Four fold axis Three non-equivalent 3-fold axes to the plane 00, 2 / 3 1 / 3, 1 / 3 2 / 3 ) Six fold axis Two non-equivalent 4-fold axes to the plane; One non-equivalent 2-fold axis to the plane; (00, ½ ½) and ( ½ 0, 0 ½ ) Martin Buerger: An introduction to fundamental geometric features of crystals One non-equivalent 6-fold axes to the plane; One non-equivalent 3-fold axis to the plane; (0 0) ; ( 2 / 3 1 / 3, 1 / 3 2 / 3 ) and ( ½ 0) 23

24 2. Combining a reflection with translation A reflection combined with a translation to it is another reflection at ½ of that perpendicular translation 1. A rectangular cell Pair of motifs Translatio n 3 * 2 *the mirror 2 is situated at ½ distance of the translation The mirror 2 is independent from 1 because the position of the objects (1 and 2) relative to the mirror in the center ( 2 )of the cell is distinct from the position of the same objects relative to the first mirror ( 1 ) 24

25 2. A centered rectangular cell 1 and 2 are equivalent because we must have a motif in the center A glide line results in here - Pair of motifs A glide is the result of a reflection and a translation 1 T T *T(T +T )=glide plane The glide will be at the half distance of T T 25

26 3. Combining a glide with a translation 1. A rectangular cell gliding 1 2 Translatio n 3 2 g 1 1 g 2 3 gliding by g 2 The glide g 2 is situated at half of the translation which is perpendicular to it - Motif 2 g1 1 T( ) g2 3 3 Reflecting 1 by a mirror in the center of the edges gives 3 ; Gliding 3 half of T parallel gives 3 26

27 2. A centered rectangular cell Combining a glide plane with a translation in a centered rectangular lattice gives a mirror plane situated at ½ of T/2. 2 g1 1 g2 27

28 4. Combining two reflections The operation of applying two reflections in which the mirror planes ( 1 and 2 ) are making an angle with each other is the same with the rotation by an 2 angle Guide to the eye Two reflections: 1 1 by reflection on by reflection on ' 2 One rotation: 1 2 by two times rotation rotation by 2 28

29 5. Combining a rotation with a reflection A rotation by followed by a reflection 1 will result in another reflection which will be situated at an angle /2 relative to the first reflection rotationby reflection 2 by 3 reflection by 2 29

30 Combining symmetry operations 1. Oblique (parallelogram) (a b, 90 ) Plane groups p1 and p2 p stands for the fact that we have only one lattice point per cell primitive lattice p1 p2 Examples of motifs having point group 1: (The motif itself should have no symmetry) and Examples of motifs having point group 2: and (The motif itself should have a 2-fold axis) 30

31 Plane group symbol rules/meaning 1. First letter: p or c translation symmetry + type of centering 2. The orientation of the symmetry elements: to coordinate system x, y and z. The highest multiplicity axis or if only one symmetry axis present they are on z Ex: p4mm: 4-fold axis in the z direction; p3m1: 3-fold axis in the z direction The highest symmetry axis is mentioned first and the rest are omitted ex: p4mmm: 4-fold axis on z and two 2-fold axes are omitted If highest multiplicity axis is 2-fold the sequence is x-y-z ex: pmm2; pgm2; cmm2: 2-fold axis on z 3. The addition of 1 is often used as a place holder to ensure the mirror or glide line is correctly placed ex: p3m1 and p31m 4/24/2013 L. Viciu AC II Symmetry in 2D m y m x m z 31

32 2. Rectangular (a b, 90ᵒ) Plane groups: pm, pg, pmg2, pmm2 and pgg2 pmg2 pgg2 pmm2 Possible motifs: 4/24/2013 m L. Viciu AC II Symmetry in 2D 2mm 32

33 2. Examples of Rectangular plane groups with glide lines motif: motif: pmg2 pgg2 pmg2 pgg2 33

34 3. Square (a = b, 90ᵒ) Plane groups: p4, p4mm and p4gm Possible motifs: 4 4mm 34

35 Questions to recognize a square plane group 1. Is there a 4-fold axis? It should be otherwise it cannot be a square lattice 2. Is there a mirror line in there? If No, then is a p4 plane group If Yes, 3. Is the mirror line passing through a 4-fold axis? If Yes then the plane group is p4mm If No then the group is a p4mg 35

36 4. Centered rectangular (a b, 90ᵒ) The dash lined cell is known as diamond or rhombus cell Plane groups: cm and cmm2 Possible motifs: cmm2 m 2mm 36

37 Diamond vs. centered rectangular The diamond lattice has a mirror through it such that always a = b but the angle is general a a=b The centered rectangular lattice has now 2 atoms per unit cell The centered rectangular lattice has 2-fold redundancy (two diamond unit cells) but it has the big advantage of an orthogonal coordinate system. Therefore it is the standard cell 37

38 5. Rhombic or hexagonal (a = b, 120ᵒ) Plane groups: p3, p31m, p3m1, p6 and p6mm Possible motifs: 6 6mm 3 3m 38

39 How the motifs are oriented in p3m plane group p3m1 The mirrors are to the translation (the translation comes in the middle of the mirrors) p31m The translation is along the mirror planes On the second place in the plane group symbol comes what is to the cell edge and on the third place comes what is to the cell edge 4/23/2013 L. Viciu AC II Symmetry in 2D 39

40 When we have translations which are inclined to the mirrors like in p3m1 plane group, a glide is always interleaved between the two mirrors The glide is parallel to the mirrors at half distance between them 1 2 a) the inclination of translation relative to the mirrors b) the location of glide (between the mirrors at the half distance) 4/23/2013 L. Viciu AC II Symmetry in 2D 40

41 When we have translations which are inclined to the mirrors like in p31m plane group, a glide is always interleaved between the two mirrors. The glide is parallel to the mirrors at half distance between them. a) The inclination of the translation relative to the mirrors b) The location of the glides (between the mirrors at the half distance) 4/23/2013 L. Viciu AC II Symmetry in 2D 41

42 The p6mm plane group has the symmetry elements of both p3m1 and p31m groups because both of these groups are present simultaneously in p6mm plane group. p3m1 +p31m When we add the symmetry elements we should make sure that all the symmetry elements are left invariant (we don t create additional translations or consequently more axes and planes; 4/23/2013 L. Viciu AC II Symmetry in 2D 42

43 Symmetry Elements of the 2D Space Groups 4/23/2013 Unit cell edge mirror line L. Viciu AC II Symmetry in 2D glide line 2, 3, 4, 6 fold axes 43

44 The equivalence of atom positions results from translation y x y x The atom will be then moved by translation to every lattice point y x The atom at the lattice point has the coordinates: (x, y) The 2 fold axes place the atoms at the opposite direction It is possible to say also 1-x 1-y But is more esthetic to give the positions x y and x y y x 1-x 1-y 4/23/2013 L. Viciu AC II Symmetry in 2D 44

45 1. Highest order rotation? Yes 2. Has reflection? 6-fold p6mm p6 4-fold 3-fold 2-fold Yes: p4mm 3. Has mirrors at 45? No: p4gm 3. Has rot. centre off mirrors? Yes: p31m No: p3m1 3. Has perpendicular reflections? Yes Has rot. centre off mirrors? Yes: cmm2 No: pmm2 No No p4 p3 Has glide reflection? pmg2 Yes: pgg2 No: p2 none Has glide axis off mirrors? Has glide reflection? Yes: cm No: pm Yes: pg No: p1 4/23/2013 L. Viciu AC II Symmetry in 2D 45

46 Fundamental Steps in Plane Groups Identification 1. Locate the motif present in the pattern. This can be a molecule, molecules, atom, group of atoms, a shape or group of shapes. The motif can usually be discovered by noting the periodicity of the pattern. 2. Identify any symmetry elements in the motif. 3. Locate a single lattice point for each occurrence of the motif. It is a good idea to locate the lattice points at a symmetry element location. 4. Connect the lattice points to form the unit cell. 5. Determine the plane group by comparing the symmetry elements present to the 17 plane patterns. 4/23/2013 L. Viciu AC II Symmetry in 2D 46

47 Finding the plane group No symmetry besides translation: The lattice type is oblique, plane group p1. Each unit mesh (unit cell) contains 1 white bird and 1 blue bird. 4/23/2013 L. Viciu AC II Symmetry in 2D 47

48 Finding the plane group No symmetry besides translation: The lattice type is oblique, plane group p1. Each unit mesh (unit cell) contains 1 white bird and 1 blue bird. 4/23/2013 L. Viciu AC II Symmetry in 2D 48

49 Finding the plane group 4/23/2013 L. Viciu AC II Symmetry in 2D 49

50 Finding the plane group 1. Highest order rotation? A: 2 2. Has reflections? A: yes 3. Has rotation centers off mirrors? A: yes 4. Space group: A: cmm2 4/23/2013 L. Viciu AC II Symmetry in 2D 50

51 Finding the plane group The unit cell is square. Symmetry elements: -2-fold axis -Two mirror lines ( to each other) - Two glide lines Plane group: cmm2 4/23/2013 L. Viciu AC II Symmetry in 2D 51

52 Finding the plane group 4/23/2013 L. Viciu AC II Symmetry in 2D 52

53 Finding the plane group 1. Highest order rotation? A: 3 2. Has reflections? A: yes 3. Has rotation centers off mirrors? A: No 4. Space group: A: p3m1 4/23/2013 L. Viciu AC II Symmetry in 2D 53

54 Finding the plane group 4/23/2013 L. Viciu AC II Symmetry in 2D 54

55 Finding the plane group 1. Highest order rotation? A: 6 2. Has reflections? A: yes 3. Space group: A: p6mm 4/23/2013 L. Viciu AC II Symmetry in 2D 55

56 Finding the plane group 4/23/2013 L. Viciu AC II Symmetry in 2D Christopher Hammond: The basics of crystallography and diffraction (third edition) 56

57 Finding the plane group 4/23/2013 L. Viciu AC II Symmetry in 2D Christopher Hammond: The basics of crystallography and diffraction (third edition) 57

58 Finding the plane group 4/23/2013 L. Viciu AC II Symmetry in 2D 58

59 p4gm 4/23/2013 L. Viciu AC II Symmetry in 2D 59

60 Finding the plane group 4/23/2013 L. Viciu AC II Symmetry in 2D 60

61 Finding the plane group 4/23/2013 L. Viciu AC II Symmetry in 2D 61

SPACE GROUPS AND SYMMETRY

SPACE GROUPS AND SYMMETRY SPACE GROUPS AND SYMMETRY Michael Landsberg Electron Crystallography Workshop C-CINA, Basel, 1-7 Aug 2010 m.landsberg@uq.edu.au Averaging Why single molecule EM techniques are far superior in resolution

More information

WALLPAPER GROUPS. Julija Zavadlav

WALLPAPER GROUPS. Julija Zavadlav WALLPAPER GROUPS Julija Zavadlav Abstract In this paper we present the wallpaper groups or plane crystallographic groups. The name wallpaper groups refers to the symmetry group of periodic pattern in two

More information

THE FIVE TYPES OF PLANAR 2-D LATTICES. (d) (e)

THE FIVE TYPES OF PLANAR 2-D LATTICES. (d) (e) THE FIVE TYPES OF PLANAR 2-D LATTICES (a) (d) (b) (d) and (e) are the same (e) (c) (f) (a) OBLIQUE LATTICE - NO RESTRICTIONS ON ANGLES BETWEEN THE UNIT CELL EDGES (b) RECTANGULAR LATTICE - ANGLE BETWEEN

More information

Lecture course on crystallography, 2015 Lecture 9: Space groups and International Tables for Crystallography

Lecture course on crystallography, 2015 Lecture 9: Space groups and International Tables for Crystallography Dr Semën Gorfman Department of Physics, University of SIegen Lecture course on crystallography, 2015 Lecture 9: Space groups and International Tables for Crystallography UNIT CELL and ATOMIC POSITIONS

More information

Crystallographic Point Groups and Space Groups

Crystallographic Point Groups and Space Groups Crystallographic Point Groups and Space Groups Physics 251 Spring 2011 Matt Wittmann University of California Santa Cruz June 8, 2011 Mathematical description of a crystal Definition A Bravais lattice

More information

Structure of Earth Materials

Structure of Earth Materials 12.108 Structure of Earth Materials I. Lecture 1: Minerals and Symmetry Operations Definition of a mineral A mineral is a naturally occurring homogeneous solid usually formed by inorganic processes. It

More information

Tim Hughbanks CHEMISTRY 634. Two Covers. Required Books, etc.

Tim Hughbanks CHEMISTRY 634. Two Covers. Required Books, etc. CHEMISTRY 634 This course is for 3 credits. Lecture: 2 75 min/week; TTh 11:10-12:25, Room 2122 Grades will be based on the homework (roughly 25%), term paper (15%), midterm and final exams Web site: http://www.chem.tamu.edu/rgroup/

More information

Crystal Structure. Dr Bindu Krishnan

Crystal Structure. Dr Bindu Krishnan Solid State Physics-1 Crystal Structure Dr Bindu Krishnan CRYSTAL LATTICE What is crystal (space) lattice? In crystallography, only the geometrical properties of the crystal are of interest, therefore

More information

Analytical Methods for Materials

Analytical Methods for Materials Analytical Methods for Materials Lesson 11 Crystallography and Crystal Structures, Part 3 Suggested Reading Chapter 6 in Waseda Chapter 1 in F.D. Bloss, Crystallography and Crystal Chemistry: An Introduction,

More information

Lecture 1 Symmetry in the solid state -

Lecture 1 Symmetry in the solid state - Lecture 1 Symmetry in the solid state - Part I: Simple patterns and groups 1 Symmetry operators: key concepts Operators: transform (move) the whole pattern (i.e., the attributes, or content, of all points

More information

Lecture Note on Crystal structures Masatsugu Sei Suzuki and Itsuko S. Suzuki Department of Physics, SUNY at Binghamton (Date: February 03, 2012)

Lecture Note on Crystal structures Masatsugu Sei Suzuki and Itsuko S. Suzuki Department of Physics, SUNY at Binghamton (Date: February 03, 2012) Lecture Note on Crystal structures Masatsugu Sei Suzuki and Itsuko S. Suzuki Department of Physics, SUNY at Binghamton (Date: February 03, 2012) This is a part of lecture note on solid state physics (Phys.472/572)

More information

The structure of liquids and glasses. The lattice and unit cell in 1D. The structure of crystalline materials. Describing condensed phase structures

The structure of liquids and glasses. The lattice and unit cell in 1D. The structure of crystalline materials. Describing condensed phase structures Describing condensed phase structures Describing the structure of an isolated small molecule is easy to do Just specify the bond distances and angles How do we describe the structure of a condensed phase?

More information

Crystallographic Symmetry. Jeremy Karl Cockcroft

Crystallographic Symmetry. Jeremy Karl Cockcroft Crystallographic Symmetry Jeremy Karl Cockcroft Why bother? To describe crystal structures Simplifies the description, e.g. NaCl structure Requires coordinates for just 2 atoms + space group symmetry!

More information

Lecture course on crystallography, 2015 Lecture 5: Symmetry in crystallography

Lecture course on crystallography, 2015 Lecture 5: Symmetry in crystallography Dr Semën Gorfman Department of Physics, University of SIegen Lecture course on crystallography, 2015 Lecture 5: Symmetry in crystallography What is symmetry? Symmetry is a property of an object to stay

More information

The 17 Plane Symmetry Groups. Samantha Burns Courtney Fletcher Aubray Zell Boise State University

The 17 Plane Symmetry Groups. Samantha Burns Courtney Fletcher Aubray Zell Boise State University The 17 Plane Symmetry Groups Samantha Burns Courtney Fletcher Aubray Zell Boise State University INTRODUCTION Our paper is going to be about the 17 plane Symmetry Groups, also called the wallpaper groups,

More information

Phys 412 Solid State Physics. Lecturer: Réka Albert

Phys 412 Solid State Physics. Lecturer: Réka Albert Phys 412 Solid State Physics Lecturer: Réka Albert What is a solid? A material that keeps its shape Can be deformed by stress Returns to original shape if it is not strained too much Solid structure

More information

Symmetry Crystallography

Symmetry Crystallography Crystallography Motif: the fundamental part of a symmetric design that, when repeated, creates the whole pattern In 3-D, translation defines operations which move the motif into infinitely repeating patterns

More information

Tables of crystallographic properties of double antisymmetry space groups

Tables of crystallographic properties of double antisymmetry space groups Tables of crystallographic properties of double antisymmetry space groups Mantao Huang a, Brian K. VanLeeuwen a, Daniel B. Litvin b and Venkatraman Gopalan a * a Department of Materials Science and Engineering,

More information

Chapter 4. Crystallography. 4.1 The crystalline state

Chapter 4. Crystallography. 4.1 The crystalline state Crystallography Atoms form bonds which attract them to one another. When you put many atoms together and they form bonds amongst themselves, are there any rules as to how they order themselves? Can we

More information

From Wikipedia, the free encyclopedia

From Wikipedia, the free encyclopedia 1 of 6 8/28/2011 1:45 PM From Wikipedia, the free encyclopedia Generally speaking, an object with rotational symmetry is an object that looks the same after a certain amount of rotation. An object may

More information

TILES, TILES, TILES, TILES, TILES, TILES

TILES, TILES, TILES, TILES, TILES, TILES 3.012 Fund of Mat Sci: Structure Lecture 15 TILES, TILES, TILES, TILES, TILES, TILES Photo courtesy of Chris Applegate. Homework for Fri Nov 4 Study: Allen and Thomas from 3.1.1 to 3.1.4 and 3.2.1, 3.2.4

More information

DIFFRACTION METHODS IN MATERIAL SCIENCE. PD Dr. Nikolay Zotov Lecture 4_2

DIFFRACTION METHODS IN MATERIAL SCIENCE. PD Dr. Nikolay Zotov   Lecture 4_2 DIFFRACTION METHODS IN MATERIAL SCIENCE PD Dr. Nikolay Zotov Email: zotov@imw.uni-stuttgart.de Lecture 4_2 OUTLINE OF THE COURSE 0. Introduction 1. Classification of Materials 2. Defects in Solids 3. Basics

More information

Helpful resources for all X ray lectures Crystallization http://www.hamptonresearch.com under tech support: crystal growth 101 literature Spacegroup tables http://img.chem.ucl.ac.uk/sgp/mainmenu.htm Crystallography

More information

Wednesday, April 12. Today:

Wednesday, April 12. Today: Wednesday, April 2 Last Time: - The solid state - atomic arrangement in solids - why do solids form: energetics - Lattices, translations, rotation, & other symmetry operations Today: Continue with lattices,

More information

Mineralogy Problem Set Crystal Systems, Crystal Classes

Mineralogy Problem Set Crystal Systems, Crystal Classes Mineralogy Problem Set Crystal Systems, Crystal Classes (1) For each of the three accompanying plane patterns: (a) Use a ruler to draw solid lines to show where there are mirror planes on the pattern.

More information

Investigation Of Plane Symmetry In Lattice Designs

Investigation Of Plane Symmetry In Lattice Designs Salem State University Digital Commons at Salem State University Honors Theses Student Scholarship 2016-12-01 Investigation Of Plane Symmetry In Lattice Designs Katyana Sheridan Salem State University

More information

Applications of X-ray and Neutron Scattering in Biological Sciences: Symmetry in direct and reciprocal space 2012

Applications of X-ray and Neutron Scattering in Biological Sciences: Symmetry in direct and reciprocal space 2012 Department of Drug Design and Pharmacology Applications of X-ray and Neutron Scattering in Biological Sciences: Symmetry in direct and reciprocal space 2012 Michael Gajhede Biostructural Research Copenhagen

More information

Planar Symmetries. Chapter Introduction

Planar Symmetries. Chapter Introduction Chapter 6 Planar Symmetries 6.1 Introduction The use of symmetry as an aspect of art goes back several millennia, and some early samples of artistic creations into which symmetry was consciously incorporated

More information

We need to be able to describe planes and directions.

We need to be able to describe planes and directions. We need to be able to describe planes and directions. Miller Indices & XRD 1 2 Determining crystal structure and identifying materials (B) Plastic deformation Plastic deformation and mechanical properties

More information

The Seventeen Plane Groups (Two-dimensional Space Groups)

The Seventeen Plane Groups (Two-dimensional Space Groups) Korean J. Crystallography Vol. 16, o. 1, pp.11~20, 2005 The Seventeen Plane Groups (Two-dimensional Space Groups) ƒá Á a Á Ÿ a Á~ a Áªœ a Á ž a ano-œ ª, ªƒ ª œ œ a ˆ ª Ÿ ª ( campus) The Seventeen Plane

More information

Crystallography basics

Crystallography basics Crystallography basics 1 ? 2 Family of planes (hkl) - Family of plane: parallel planes and equally spaced. The indices correspond to the plane closer to the origin which intersects the cell at a/h, b/k

More information

Symmetry. 2-D Symmetry. 2-D Symmetry. Symmetry. EESC 2100: Mineralogy 1. Symmetry Elements 1. Rotation. Symmetry Elements 1. Rotation.

Symmetry. 2-D Symmetry. 2-D Symmetry. Symmetry. EESC 2100: Mineralogy 1. Symmetry Elements 1. Rotation. Symmetry Elements 1. Rotation. Symmetry a. Two-fold rotation = 30 o /2 rotation a. Two-fold rotation = 30 o /2 rotation Operation Motif = the symbol for a two-fold rotation EESC 2100: Mineralogy 1 a. Two-fold rotation = 30 o /2 rotation

More information

Basics of crystallography

Basics of crystallography Basics of crystallography 1 Family of planes (hkl) - Family of plane: parallel planes and equally spaced. The indices correspond to the plane closer to the origin which intersects the cell at a/h, b/k

More information

Lecture 2 Symmetry in the solid state -

Lecture 2 Symmetry in the solid state - Lecture 2 Symmetry in the solid state - Part II: Crystallographic coordinates and Space Groups. 1 Coordinate systems in crystallography and the mathematical form of the symmetry operators 1.1 Introduction

More information

Crystallography Reading: Warren, Chapters 2.1, 2.2, 2.6, 8 Surface symmetry: Can be a clue to underlying structure. Examples:

Crystallography Reading: Warren, Chapters 2.1, 2.2, 2.6, 8 Surface symmetry: Can be a clue to underlying structure. Examples: Crystallography Reading: Warren, Chapters 2.1, 2.2, 2.6, 8 Surface symmetry: Can be a clue to underlying structure. Examples: Snow (SnowCrystals.com) Bismuth (Bao, Kavanagh, APL 98 66103 (2005) Hexagonal,

More information

1/2, 1/2,1/2, is the center of a cube. Induces of lattice directions and crystal planes (a) Directions in a crystal Directions in a crystal are

1/2, 1/2,1/2, is the center of a cube. Induces of lattice directions and crystal planes (a) Directions in a crystal Directions in a crystal are Crystallography Many materials in nature occur as crystals. Examples include the metallic elements gold, copper and silver, ionic compounds such as salt (e.s. NaCl); ceramics, rutile TiO2; and nonmetallic

More information

Overview - Macromolecular Crystallography

Overview - Macromolecular Crystallography Overview - Macromolecular Crystallography 1. Overexpression and crystallization 2. Crystal characterization and data collection 3. The diffraction experiment 4. Phase problem 1. MIR (Multiple Isomorphous

More information

UNIT I SOLID STATE PHYSICS

UNIT I SOLID STATE PHYSICS UNIT I SOLID STATE PHYSICS CHAPTER 1 CRYSTAL STRUCTURE 1.1 INTRODUCTION When two atoms are brought together, two kinds of forces: attraction and repulsion come into play. The force of attraction increases

More information

X-ray analysis. 1. Basic crystallography 2. Basic diffraction physics 3. Experimental methods

X-ray analysis. 1. Basic crystallography 2. Basic diffraction physics 3. Experimental methods X-ray analysis 1. Basic crystallography 2. Basic diffraction physics 3. Experimental methods Introduction Noble prizes associated with X-ray diffraction 1901 W. C. Roentgen (Physics) for the discovery

More information

Protein Structure Determination. Part 1 -- X-ray Crystallography

Protein Structure Determination. Part 1 -- X-ray Crystallography Protein Structure Determination Part 1 -- X-ray Crystallography Topics covering in this 1/2 course Crystal growth Diffraction theory Symmetry Solving phases using heavy atoms Solving phases using a model

More information

5 Symmetries and point group in a nut shell

5 Symmetries and point group in a nut shell 30 Phys520.nb 5 Symmetries and point group in a nut shell 5.1. Basic ideas: 5.1.1. Symmetry operations Symmetry: A system remains invariant under certain operation. These operations are called symmetry

More information

Review of Last Class 1

Review of Last Class 1 Review of Last Class 1 X-Ray diffraction of crystals: the Bragg formulation Condition of diffraction peak: 2dd sin θθ = nnλλ Review of Last Class 2 X-Ray diffraction of crystals: the Von Laue formulation

More information

Crystallographic structure Physical vs Chemical bonding in solids

Crystallographic structure Physical vs Chemical bonding in solids Crystallographic structure Physical vs Chemical bonding in solids Inert gas and molecular crystals: Van der Waals forces (physics) Water and organic chemistry H bonds (physics) Quartz crystal SiO 2 : covalent

More information

CHAPTER 8 WHY PRECISELY SEVENTEEN TYPES?

CHAPTER 8 WHY PRECISELY SEVENTEEN TYPES? 2006 George Baloglou first draft: summer 2001 CHAPTER 8 WHY PRECISELY SEVENTEEN TYPES? 8.0 Classification of wallpaper patterns 8.0.1 The goal. Back in section 2.8 it was rather easy to explain why there

More information

Introduction to Solid State Physics or the study of physical properties of matter in a solid phase

Introduction to Solid State Physics or the study of physical properties of matter in a solid phase Introduction to Solid State Physics or the study of physical properties of matter in a solid phase Prof. Germar Hoffmann 1. Crystal Structures 2. Reciprocal Lattice 3. Crystal Binding and Elastic Constants

More information

Fundamentals. Crystal patterns and crystal structures. Lattices, their symmetry and related basic concepts

Fundamentals. Crystal patterns and crystal structures. Lattices, their symmetry and related basic concepts Fundamentals. Crystal patterns and crystal structures. Lattices, their symmetry and related basic concepts Didactic material for the MaThCryst schools, France massimo.nespolo@univ-lorraine.fr Ideal vs.

More information

Nove fizickohemijske metode. Ivana Radosavljevic Evans Durham University, UK

Nove fizickohemijske metode. Ivana Radosavljevic Evans Durham University, UK Nove fizickohemijske metode Ivana Radosavljevic Evans Durham University, UK Nove fizickohemijske metode: Metode zasnovane na sinhrotronskom zracenju Plan predavanja: Difrakcione metode strukturne karakterizacije

More information

Decagonal quasicrystals

Decagonal quasicrystals Decagonal quasicrystals higher dimensional description & structure determination Hiroyuki Takakura Division of Applied Physics, Faculty of Engineering, Hokkaido University 1 Disclaimer and copyright notice

More information

AM 106/206: Applied Algebra Madhu Sudan 1. Lecture Notes 12

AM 106/206: Applied Algebra Madhu Sudan 1. Lecture Notes 12 AM 106/206: Applied Algebra Madhu Sudan 1 Lecture Notes 12 October 19 2016 Reading: Gallian Chs. 27 & 28 Most of the applications of group theory to the physical sciences are through the study of the symmetry

More information

Condensed Matter Physics Prof. G. Rangarajan Department of Physics Indian Institute of Technology, Madras

Condensed Matter Physics Prof. G. Rangarajan Department of Physics Indian Institute of Technology, Madras Condensed Matter Physics Prof. G. Rangarajan Department of Physics Indian Institute of Technology, Madras Lecture - 03 Symmetry in Perfect Solids Worked Examples Stated without prove to be in the lecture.

More information

INTERNATIONAL SCHOOL ON FUNDAMENTAL CRYSTALLOGRAPHY

INTERNATIONAL SCHOOL ON FUNDAMENTAL CRYSTALLOGRAPHY INTERNATIONAL SCHOOL ON FUNDAMENTAL CRYSTALLOGRAPHY SPACE-GROUP SYMMETRY (short overview) Mois I. Aroyo Universidad del Pais Vasco, Bilbao, Spain SPACE GROUPS Crystal pattern: infinite, idealized crystal

More information

POINT SYMMETRY AND TYPES OF CRYSTAL LATTICE

POINT SYMMETRY AND TYPES OF CRYSTAL LATTICE POINT SYMMETRY AND TYPES OF CRYSTAL LATTICE Abdul Rashid Mirza Associate Professor of Physics. Govt. College of Science, wahdatroad, Lahore. 1 WHAT ARE CRYSTALS? The word crystal means icy or frozen water.

More information

PX-CBMSO Course (2) of Symmetry

PX-CBMSO Course (2) of Symmetry PX-CBMSO Course (2) The mathematical description of Symmetry y PX-CBMSO-June 2011 Cele Abad-Zapatero University of Illinois at Chicago Center for Pharmaceutical Biotechnology. Lecture no. 2 This material

More information

Finite Symmetry Elements and Crystallographic Point Groups

Finite Symmetry Elements and Crystallographic Point Groups Chapter 2 Finite Symmetry Elements and Crystallographic Point Groups In addition to simple translations, which are important for understanding the concept of the lattice, other types of symmetry may be,

More information

Yanxi Liu.

Yanxi Liu. Yanxi Liu yanxi@cse.psu.edu Today s Theme: What is symmetry? From real world to mathematics, and back to the real world Real World Instances of Symmetry Symmetry Patterns from Real World (1) Symmetry Patterns

More information

VERTEX-TRANSITIVE MAPS ON A TORUS. 1. Introduction

VERTEX-TRANSITIVE MAPS ON A TORUS. 1. Introduction VERTEX-TRANSITIVE MAPS ON A TORUS ONDREJ ŠUCH Abstract. We examine FVT (free, vertex transitive) actions of wallpaper groups on semiregular tilings. By taking quotients by lattices we then obtain various

More information

Solid State Physics 460- Lecture 5 Diffraction and the Reciprocal Lattice Continued (Kittel Ch. 2)

Solid State Physics 460- Lecture 5 Diffraction and the Reciprocal Lattice Continued (Kittel Ch. 2) Solid State Physics 460- Lecture 5 Diffraction and the Reciprocal Lattice Continued (Kittel Ch. 2) Ewald Construction 2θ k out k in G Physics 460 F 2006 Lect 5 1 Recall from previous lectures Definition

More information

Chapter 1. Crystal structure. 1.1 Crystal lattices

Chapter 1. Crystal structure. 1.1 Crystal lattices Chapter 1 Crystal structure 1.1 Crystal lattices We will concentrate as stated in the introduction, on perfect crystals, i.e. on arrays of atoms, where a given arrangement is repeated forming a periodic

More information

Chapter 2 Introduction to Phenomenological Crystal Structure

Chapter 2 Introduction to Phenomenological Crystal Structure Chapter 2 Introduction to Phenomenological Crystal Structure 2.1 Crystal Structure An ideal crystal represents a periodic pattern generated by infinite, regular repetition of identical microphysical structural

More information

Aperiodic tilings and quasicrystals

Aperiodic tilings and quasicrystals Aperiodic tilings and quasicrystals Perleforedrag, NTNU Antoine Julien Nord universitet Levanger, Norway October 13 th, 2017 A. Julien (NordU) Aperiodic tilings and quasicrystals October 13 th, 2017 1

More information

Structure of Materials Prof. Anandh Subramaniam Department of Material Science and Engineering Indian Institute of Technology, Kanpur

Structure of Materials Prof. Anandh Subramaniam Department of Material Science and Engineering Indian Institute of Technology, Kanpur Structure of Materials Prof. Anandh Subramaniam Department of Material Science and Engineering Indian Institute of Technology, Kanpur Lecture - 5 Geometry of Crystals: Symmetry, Lattices The next question

More information

Group theory applied to crystallography

Group theory applied to crystallography International Union of Crystallography Commission on Mathematical and Theoretical Crystallography Summer School on Mathematical and Theoretical Crystallography 7 April - May 8, Gargnano, Italy Group theory

More information

2. Diffraction as a means to determine crystal structure

2. Diffraction as a means to determine crystal structure 2. Diffraction as a means to determine crystal structure Recall de Broglie matter waves: He atoms: [E (ev)] 1/2 = 0.14 / (Å) E 1Å = 0.0196 ev Neutrons: [E (ev)] 1/2 = 0.28 / (Å) E 1Å = 0.0784 ev Electrons:

More information

CS123 INTRODUCTION TO COMPUTER GRAPHICS. Linear Algebra /34

CS123 INTRODUCTION TO COMPUTER GRAPHICS. Linear Algebra /34 Linear Algebra /34 Vectors A vector is a magnitude and a direction Magnitude = v Direction Also known as norm, length Represented by unit vectors (vectors with a length of 1 that point along distinct axes)

More information

Introduction to Materials Science Graduate students (Applied Physics)

Introduction to Materials Science Graduate students (Applied Physics) Introduction to Materials Science Graduate students (Applied Physics) Prof. Michael Roth Chapter 1 Crystallography Overview Performance in Engineering Components Properties Mechanical, Electrical, Thermal

More information

CRYSTALLOGRAPHIC SYMMETRY OPERATIONS. Mois I. Aroyo Universidad del Pais Vasco, Bilbao, Spain

CRYSTALLOGRAPHIC SYMMETRY OPERATIONS. Mois I. Aroyo Universidad del Pais Vasco, Bilbao, Spain CRYSTALLOGRAPHIC SYMMETRY OPERATIONS Mois I. Aroyo Universidad del Pais Vasco, Bilbao, Spain SYMMETRY OPERATIONS AND THEIR MATRIX-COLUMN PRESENTATION Mappings and symmetry operations Definition: A mapping

More information

Crystal Symmetries and Space Groups

Crystal Symmetries and Space Groups Crystal Symmetries and Space Groups Robert B. Griffiths Version of 18 Feb. 2009 References: M. S. Dresselhaus, G. Dresselhaus and A. Jorio, Group Theory: Applications to the Physics of Condensed Matter

More information

MITOCW ocw sep2005-part1-220k_512kb.mp4

MITOCW ocw sep2005-part1-220k_512kb.mp4 MITOCW ocw-3.60-29sep2005-part1-220k_512kb.mp4 I think it's about five after the hour so we ought to get started. Before we forge bravely ahead, I'd like to make sure that everybody has a copy of the things

More information

2. Diffraction as a means to determine crystal structure

2. Diffraction as a means to determine crystal structure Page 1 of 22 2. Diffraction as a means to determine crystal structure Recall de Broglie matter waves: 2 p h E = where p = 2m λ h 1 E = ( ) 2m λ hc E = hυ = ( photons) λ ( matter wave) He atoms: [E (ev)]

More information

Lattices and Symmetry Scattering and Diffraction (Physics)

Lattices and Symmetry Scattering and Diffraction (Physics) Lattices and Symmetry Scattering and Diffraction (Physics) James A. Kaduk INEOS Technologies Analytical Science Research Services Naperville IL 60566 James.Kaduk@innovene.com 1 Harry Potter and the Sorcerer

More information

Space groups. Bernd Souvignier

Space groups. Bernd Souvignier MaThCryst summer school 5- July 7, Havana, Cuba Space groups Bernd Souvignier Definition A crystal pattern is a set of points in R n such that the translations leaving it invariant form a (vector lattice

More information

M\1any arguments have been concerned with what these symbols mean, and how they

M\1any arguments have been concerned with what these symbols mean, and how they SOME DESIRABLE MODIFICATIONS OF THE INTERNATIONAL SYMMETRY SYMBOLS* BY MARTIN J. BUERGER MASSACHUSETTS INSTITUTE OF TECHNOLOGY Communicated August 21, 1967 With the publication of Hilton's Mathematical

More information

Introduction to mathematical quasicrystals

Introduction to mathematical quasicrystals Introduction to mathematical quasicrystals F S W Alan Haynes Topics to be covered Historical overview: aperiodic tilings of Euclidean space and quasicrystals Lattices, crystallographic point sets, and

More information

Structure of Crystalline Solids

Structure of Crystalline Solids Structure of Crystalline Solids Solids- Effect of IMF s on Phase Kinetic energy overcome by intermolecular forces C 60 molecule llotropes of Carbon Network-Covalent solid Molecular solid Does not flow

More information

MATRIX CALCULUS APPLIED TO CRYSTALLOGRAPHY. (short revision) Mois I. Aroyo Universidad del Pais Vasco, Bilbao, Spain

MATRIX CALCULUS APPLIED TO CRYSTALLOGRAPHY. (short revision) Mois I. Aroyo Universidad del Pais Vasco, Bilbao, Spain MATRIX CALCULUS APPLIED TO CRYSTALLOGRAPHY (short revision) Mois I. Aroyo Universidad del Pais Vasco, Bilbao, Spain INTRODUCTION TO MATRIX CALCULUS Some of the slides are taken from the presentation Introduction

More information

n-dimensional, infinite, periodic array of points, each of which has identical surroundings.

n-dimensional, infinite, periodic array of points, each of which has identical surroundings. crystallography ll Lattice n-dimensional, infinite, periodic array of points, each of which has identical surroundings. use this as test for lattice points A2 ("bcc") structure lattice points Lattice n-dimensional,

More information

SPACE GROUPS. International Tables for Crystallography, Volume A: Space-group Symmetry. Mois I. Aroyo Universidad del Pais Vasco, Bilbao, Spain

SPACE GROUPS. International Tables for Crystallography, Volume A: Space-group Symmetry. Mois I. Aroyo Universidad del Pais Vasco, Bilbao, Spain SPACE GROUPS International Tables for Crystallography, Volume A: Space-group Symmetry Mois I. Aroyo Universidad del Pais Vasco, Bilbao, Spain SPACE GROUPS Crystal pattern: Space group G: A model of the

More information

Basic Principles of Quasicrystallography

Basic Principles of Quasicrystallography Chapter 2 Basic Principles of Quasicrystallography Conventional crystals are constructed by a periodic repetition of a single unit-cell. This periodic long-range order only agrees with two-, three-, four-

More information

Mineralogy ( ) Chapter 5: Crystallography

Mineralogy ( ) Chapter 5: Crystallography Hashemite University Faculty of Natural Resources and Environment Department of earth and environmental sciences Mineralogy (1201220) Chapter 5: Crystallography Dr. Faten Al-Slaty First Semester 2015/2016

More information

Phys 460 Describing and Classifying Crystal Lattices

Phys 460 Describing and Classifying Crystal Lattices Phys 460 Describing and Classifying Crystal Lattices What is a material? ^ crystalline Regular lattice of atoms Each atom has a positively charged nucleus surrounded by negative electrons Electrons are

More information

- A general combined symmetry operation, can be symbolized by β t. (SEITZ operator)

- A general combined symmetry operation, can be symbolized by β t. (SEITZ operator) SPACE GROUP THEORY (cont) It is possible to represent combined rotational and translational symmetry operations in a single matrix, for example the C6z operation and translation by a in D 6h is represented

More information

Space Group: translations and point Group

Space Group: translations and point Group Space Group: translations and point Group Fyodorov and Schönflies in 1891 listed the 230 space Groups in 3d Group elements: r ' r a with a traslation rotation matrix ( 1 No rotation). The ope ration denoted

More information

Natural Sciences Tripos Part IA. Course A: Atomic Structure of Materials. Name... College... Prof. Paul Midgley Michaelmas Term

Natural Sciences Tripos Part IA. Course A: Atomic Structure of Materials. Name... College... Prof. Paul Midgley Michaelmas Term Natural Sciences Tripos Part IA MATEIALS SCIENCE Course A: Atomic Structure of Materials Name... College... Prof. Paul Midgley Michaelmas Term 2013-14 14 IA AH1 MATEIALS SCIENCE Course A: Atomic Structure

More information

Introduction to crystallography The unitcell The resiprocal space and unitcell Braggs law Structure factor F hkl and atomic scattering factor f zθ

Introduction to crystallography The unitcell The resiprocal space and unitcell Braggs law Structure factor F hkl and atomic scattering factor f zθ Introduction to crystallography The unitcell The resiprocal space and unitcell Braggs law Structure factor F hkl and atomic scattering factor f zθ Introduction to crystallography We divide materials into

More information

M.S. Dresselhaus G. Dresselhaus A. Jorio. Group Theory. Application to the Physics of Condensed Matter. With 131 Figures and 219 Tables.

M.S. Dresselhaus G. Dresselhaus A. Jorio. Group Theory. Application to the Physics of Condensed Matter. With 131 Figures and 219 Tables. M.S. Dresselhaus G. Dresselhaus A. Jorio Group Theory Application to the Physics of Condensed Matter With 131 Figures and 219 Tables 4) Springer Contents Part I Basic Mathematics 1 Basic Mathematical Background:

More information

Geometric Transformations and Wallpaper. Groups. Lance Drager Math Camp

Geometric Transformations and Wallpaper. Groups. Lance Drager Math Camp How to Geometric Transformations and Department of Mathematics and Statistics Texas Tech University Lubbock, Texas 2010 Math Camp Outline How to 1 How to Outline How to 1 How to How to to A Group is a

More information

Translational symmetry, point and space groups in solids

Translational symmetry, point and space groups in solids Translational symmetry, point and space groups in solids Michele Catti Dipartimento di Scienza dei Materiali, Universita di Milano Bicocca, Milano, Italy ASCS26 Spokane Michele Catti a = b = 4.594 Å; Å;

More information

Tables of crystallographic properties of magnetic space groups

Tables of crystallographic properties of magnetic space groups Acta Crystallographica Section A Foundations of Crystallography ISSN 0108-7673 Editor: D. Schwarzenbach Tables of crystallographic properties of magnetic space groups D. B. Litvin Acta Cryst. (2008). A64,

More information

On the Collapse of Locally Isostatic Networks

On the Collapse of Locally Isostatic Networks On the Collapse of Locally Isostatic Networks By Vitaliy Kapko 1, M.M.J. Treacy 1, M.F. Thorpe 1, S.D. Guest 2 1 Arizona State University, Department of Physics and Astronomy, P.O. Box 871504, Tempe, AZ,

More information

CS123 INTRODUCTION TO COMPUTER GRAPHICS. Linear Algebra 1/33

CS123 INTRODUCTION TO COMPUTER GRAPHICS. Linear Algebra 1/33 Linear Algebra 1/33 Vectors A vector is a magnitude and a direction Magnitude = v Direction Also known as norm, length Represented by unit vectors (vectors with a length of 1 that point along distinct

More information

Basic Crystallography Part 1. Theory and Practice of X-ray Crystal Structure Determination

Basic Crystallography Part 1. Theory and Practice of X-ray Crystal Structure Determination Basic Crystallography Part 1 Theory and Practice of X-ray Crystal Structure Determination We have a crystal How do we get there? we want a structure! The Unit Cell Concept Ralph Krätzner Unit Cell Description

More information

3.1 Symmetry & Coordinate Graphs

3.1 Symmetry & Coordinate Graphs 3.1 Symmetry & Coordinate Graphs I. Symmetry Point symmetry two distinct points P and P are symmetric with respect to point M if and only is M is the midpoint of PP' When the definition is extended to

More information

Outline 1 Introduction Tiling definitions 2 Conway s Game of Life 3 The Projection Method

Outline 1 Introduction Tiling definitions 2 Conway s Game of Life 3 The Projection Method A Game of Life on Penrose Tilings Kathryn Lindsey Department of Mathematics Cornell University Olivetti Club, Sept. 1, 2009 Outline 1 Introduction Tiling definitions 2 Conway s Game of Life 3 The Projection

More information

Space Group: translations and point Group

Space Group: translations and point Group Space Group: translations and point Group Fyodorov and Schönflies in 1891 listed the 230 space Groups in 3d G= space Group with elements: r' = αr + a a = traslation, α = rotation matrix ( α = 1 No rotation).

More information

NAEP Questions, Pre-Algebra, Unit 13: Angle Relationships and Transformations

NAEP Questions, Pre-Algebra, Unit 13: Angle Relationships and Transformations NAEP Questions, Pre-Algebra, Unit 13: Angle Relationships and Transformations SOURCE: U.S. Department of Education, Institute of Education Sciences, National Center for Education Statistics, National Assessment

More information

A web based crystallographic tool for the construction of nanoparticles

A web based crystallographic tool for the construction of nanoparticles A web based crystallographic tool for the construction of nanoparticles Alexios Chatzigoulas 16/5/2018 + = 1 Outline Introduction Motivation Crystallography theory Creation of a web based crystallographic

More information

SUPPLEMENTARY INFORMATION

SUPPLEMENTARY INFORMATION In the format provided by the authors and unedited. DOI: 10.1038/NMAT4890 Electron-crystallography for determining the handedness of a chiral zeolite nano-crystal Yanhang Ma 1,2, Peter Oleynikov 1,2,*

More information

Notes: Most of the material presented in this chapter is taken from Bunker and Jensen (2005), Chap. 3, and Atkins and Friedman, Chap. 5.

Notes: Most of the material presented in this chapter is taken from Bunker and Jensen (2005), Chap. 3, and Atkins and Friedman, Chap. 5. Chapter 5. Geometrical Symmetry Notes: Most of the material presented in this chapter is taken from Bunker and Jensen (005), Chap., and Atkins and Friedman, Chap. 5. 5.1 Symmetry Operations We have already

More information

Crystal Chem Crystallography

Crystal Chem Crystallography Crystal Chem Crystallography Chemistry behind minerals and how they are assembled Bonding properties and ideas governing how atoms go together Mineral assembly precipitation/ crystallization and defects

More information

Geometry of Crystal Lattice

Geometry of Crystal Lattice 0 Geometry of Crystal Lattice 0.1 Translational Symmetry The crystalline state of substances is different from other states (gaseous, liquid, amorphous) in that the atoms are in an ordered and symmetrical

More information