Combining symmetry operations

Size: px
Start display at page:

Download "Combining symmetry operations"

Transcription

1 Combining symmetry operations An object can possess several symmetry elements Not all symmetry elements can be combined arbitrarily - for example, two perpendicular two-fold axes imply the existence of a third perpendicular two-fold Translational symmetry in 3D imposes limitations - only 2, 3, 4 and 6-fold rotation axes allow for space filling translational symmetry The allowed combinations of symmetry elements are called point groups - there are 32 point groups that give rise to periodicity in 3D

2 Space filling repeat patterns Only 2, 3, 4 and 6-fold rotations can produce space filling patterns Structure Determination by X-ray Crystallography, Ladd and Palmer, Plenum, 1994.

3 Point groups Show 3D repeat pattern Contain symmetry elements 32 point groups exist Structure Determination by X-ray Crystallography, Ladd and Palmer, Plenum, 1994.

4 Space groups When talking about crystal structures, people will usually report the space group of a crystal Space groups are made up from - lattice symmetry (translational) - point symmetry (not translational) - glide and/or screw axes (some translational component) There are 230 space groups 7 crystal systems 14 Bravais lattices 32 point groups 230 space groups

5 Screw axes A 2 1 screw axis translates an object by half a unit cell in the direction of the screw axis, followed by a 180 rotation Crystal Structure Analysis for Chemists and Biologists, Glusker, Lewis and Rossi, VCH, 1994.

6 Higher order screws Structure Determination by X-ray Crystallography Ladd and Palmer, Plenum, A C n screw axis translates an object by the unit cell dimension multiplied by n/c along the direction of the screw axis, followed by a C-fold rotation

7 Glide planes A glide plane corresponds to a reflection-translation operation - reflection through the glide plane - translation within the glide plane - exact translation depends on type of glide There are a, b, c, n and d glide planes - a, b and c glides correspond to translations of ½ a, ½ b and ½ c respectively - called axial glide planes - n glide corresponds to a translation of ½ a + ½ b, ½ a + ½ c, or ½ b + ½ c - called diagonal glide plane - d glide corresponds to a translation of ¼ a + ¼ b, ¼ a + ¼ c, or ¼ b + ¼ c - called diamond glide plane

8 Example of an a glide plane Crystal Structure Analysis for Chemists and Biologists, Glusker, Lewis and Rossi, VCH, 1994.

9 Graphical symbols used for symmetry operations International Tables for Crystallography, Vol. A, Kluwer, 1993.

10 Graphical symbols (2) International Tables for Crystallography, Vol. A, Kluwer, 1993.

11 Interpretation of space group symbols All space group symbols start with a letter corresponding to the lattice centering, followed by a collection of symbols for symmetry operations in the three lattice directions There are sometimes short notations for space group symbols - P is usually written as P 2 - primitive cell that has a two-fold rotation along the b axis - P (cannot be abbreviated) - primitive cell that has a 2 1 screw along each axis, orthorhombic - C m m a (full symbol: C 2/m 2/m 2/a) - C-centered cell with a mirror plane perpendicular to a and b and an a glide plane perpendicular to c - also has implied symmetry elements (e.g., the 2-fold rotations)

12 Limitations on combination of symmetry elements As for point groups, not all symmetry elements can be combined arbitrarily For three dimensional lattices - 14 Bravais lattices - 32 point groups - but only 230 space groups For two dimensional lattices - 5 lattices - 10 point groups - but only 17 plane groups

13 The 17 plane groups (1) Structure Determination by X-ray Crystallography, Ladd and Palmer, Plenum, 1994.

14 The 17 plane groups (2) Structure Determination by X-ray Crystallography, Ladd and Palmer, Plenum, 1994.

15 Symmetry elements parallel to the plane of projection International Tables for Crystallography, Vol. A, Kluwer, 1993.

16 Symmetry elements inclined to the plane of projection International Tables for Crystallography, Vol. A, Kluwer, 1993.

Figure.1. The conventional unit cells (thick black outline) of the 14 Bravais lattices. [crystallographic symmetry] 1

Figure.1. The conventional unit cells (thick black outline) of the 14 Bravais lattices. [crystallographic symmetry] 1 [crystallographic symmetry] The crystallographic space groups. Supplementary to { 9.6:324} In the 3-D space there are 7 crystal systems that satisfy the point (e.g., rotation, reflection and inversion)

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 - 3 Symmetry in Perfect Solids (Continued) (Refer Slide Time: 00:26) So, the last lecture,

More information

Analytical Methods for Materials

Analytical Methods for Materials Analytical Methods for Materials Lesson 12 Crystallography and Crystal Structures continued Suggested Reading Ch. 6 in Waseda Ch. 1 C. Kittel, Introduction to Solid State Physics, 3 rd Edition, Wiley (1956).

More information

Physics of Materials: Symmetry and Bravais Lattice To understand Crystal Plane/Face. Dr. Anurag Srivastava

Physics of Materials: Symmetry and Bravais Lattice To understand Crystal Plane/Face. Dr. Anurag Srivastava Physics of Materials: Symmetry and Bravais Lattice To understand Crystal Plane/Face Dr. Anurag Srivastava Atal Bihari Vajpayee Indian Institute of Information Technology and Manegement, Gwalior Physics

More information

Analytical Methods for Materials

Analytical Methods for Materials Analytical Methods for Materials Lesson 13 Crystallography and Crystal Structures continued Chapter 6 in Waseda Excerpt from ASM Metals Handbook. Suggested Reading 337 Notation for crystal structures 1.

More information

What is a crystal? Historic definition before the advent of crystallography. - A material with a regularly repeating structural motif

What is a crystal? Historic definition before the advent of crystallography. - A material with a regularly repeating structural motif What is a crystal? Historic definition before the advent of crystallography - A solid with well-defined faces Crystallographic definition - A material with a regularly repeating structural motif The strict

More information

Symmetry in crystalline solids.

Symmetry in crystalline solids. Symmetry in crystalline solids. Translation symmetry n 1,n 2,n 3 are integer numbers 1 Unitary or primitive cells 2D 3D Red, green and cyano depict all primitive (unitary) cells, whereas blue cell is not

More information

4.5 Translational symmetry elements 107. (a) (b)

4.5 Translational symmetry elements 107. (a) (b) .5 Translational symmetry elements 07 Fig..7. Left- and right-handed forms of tartaric acid molecules (from rystals: their Role in Nature and Science by. W. Bunn, cademic Press, New York, 9); and the left-

More information

CHAPTER 3: SYMMETRY AND GROUPS, AND CRYSTAL STRUCTURES. Sarah Lambart

CHAPTER 3: SYMMETRY AND GROUPS, AND CRYSTAL STRUCTURES. Sarah Lambart CHAPTER 3: SYMMETRY AND GROUPS, AND CRYSTAL STRUCTURES Sarah Lambart RECAP CHAP. 2 2 different types of close packing: hcp: tetrahedral interstice (ABABA) ccp: octahedral interstice (ABCABC) Definitions:

More information

GY 302: Crystallography & Mineralogy

GY 302: Crystallography & Mineralogy UNIVERSITY OF SOUTH ALABAMA GY 302: Crystallography & Mineralogy Lecture 5: Space Groups, Crystal Growth and Twinning Instructor: Dr. Douglas Haywick Last Time 1. Stereo Projections and the Wulff Net 2.

More information

Powder X-ray Diffraction

Powder X-ray Diffraction Powder X-ray Diffraction The construction of a simple powder diffractometer was first described by Hull in 1917 1 which was shortly after the discovery of X-rays by Wilhelm Conrad Röntgen in1895 2. Diffractometer

More information

Basics of XRD part I. 1 KIT 10/31/17. Name of Institute, Faculty, Department. The Research University in the Helmholtz Association

Basics of XRD part I.   1 KIT 10/31/17. Name of Institute, Faculty, Department. The Research University in the Helmholtz Association Basics of XRD part I Dr. Peter G. Weidler Institute of Functional Interfaces IFG 1 KIT 10/31/17 The Research University in the Helmholtz Association Name of Institute, Faculty, Department www.kit.edu Overview

More information

Analytical Methods for Materials

Analytical Methods for Materials Analytical Methods for Materials Lesson 10 Crystallography and Crystal Structures, Part 2 Chapters 2 and 6 in Waseda Suggested Reading 258 Symmetry Operators All motions that allow a pattern to be transformed

More information

General Objective. To develop the knowledge of crystal structure and their properties.

General Objective. To develop the knowledge of crystal structure and their properties. CRYSTAL PHYSICS 1 General Objective To develop the knowledge of crystal structure and their properties. 2 Specific Objectives 1. Differentiate crystalline and amorphous solids. 2. To explain nine fundamental

More information

Workshop RIETVELD REFINEMENT OF DIFFRACTION PATTERNS Program Monday June 1st, Introduction to Rietveld refinement S.

Workshop RIETVELD REFINEMENT OF DIFFRACTION PATTERNS Program Monday June 1st, Introduction to Rietveld refinement S. Workshop RIETVELD REFINEMENT OF DIFFRACTION PATTERNS Program Monday June 1st, 2009 9.00 13.00 Introduction to Rietveld refinement S.Enzo Università di Sassari X-ray diffraction for bulk samples and thin

More information

The Structure of Materials

The Structure of Materials The Structure of Materials Samuel M. Allen Edwin L. Thomas Massachusetts Institute of Technology Cambridge, Massachusetts / John Wiley & Sons, Inc. New York Chichester Weinheim Brisbane Singapore Toronto

More information

Übungsaufgaben zur Kristallographie Serie 4

Übungsaufgaben zur Kristallographie Serie 4 Übungsaufgaben zur Kristallographie Serie HS ) Symmetrie Im Folgenden sind Abbildungen.6 und.7 aus dem Skript gegeben. Nummerieren Sie die eingezeichneten Objekte nach der Reihenfolge der Erzeugung wie

More information

Fundamentals of Crystalline State p. 1 Introduction p. 1 Crystalline state p. 2 Crystal lattice and crystal structure p. 4 Shape of the unit cell p.

Fundamentals of Crystalline State p. 1 Introduction p. 1 Crystalline state p. 2 Crystal lattice and crystal structure p. 4 Shape of the unit cell p. Preface p. xvii Fundamentals of Crystalline State p. 1 Introduction p. 1 Crystalline state p. 2 Crystal lattice and crystal structure p. 4 Shape of the unit cell p. 6 Content of the unit cell p. 7 Asymmetric

More information

CRYSTAL LATTICE. Defining lattice: Mathematical construct; ideally infinite arrangement of points in space.

CRYSTAL LATTICE. Defining lattice: Mathematical construct; ideally infinite arrangement of points in space. CRYSTAL LATTICE How to form a crystal? 1. Define the structure of the lattice 2. Define the lattice constant 3. Define the basis Defining lattice: Mathematical construct; ideally infinite arrangement of

More information

Basic Solid State Chemistry, 2 nd ed. West, A. R.

Basic Solid State Chemistry, 2 nd ed. West, A. R. Basic Solid State Chemistry, 2 nd ed. West, A. R. Chapter 1 Crystal Structures Many of the properties and applications of crystalline inorganic materials revolve around a small number of structure types

More information

Two marks questions and answers. 1. what is a Crystal? (or) What are crystalline materials? Give examples

Two marks questions and answers. 1. what is a Crystal? (or) What are crystalline materials? Give examples UNIT V CRYSTAL PHYSICS PART-A Two marks questions and answers 1. what is a Crystal? (or) What are crystalline materials? Give examples Crystalline solids (or) Crystals are those in which the constituent

More information

Two dimensional Bravais lattices

Two dimensional Bravais lattices Two dimensional Bravais lattices Two dimensional Bravais lattices Square lattice Symmetries: reflection about both x and y rotations by 90 o,180 o Two dimensional Bravais lattices Rectangular lattice Square

More information

Bicrystallography in two dimensions: A graphical procedure. Andrew Maas Portland State University Department of Physics Nano-Crystallography Group

Bicrystallography in two dimensions: A graphical procedure. Andrew Maas Portland State University Department of Physics Nano-Crystallography Group Bicrystallography in two dimensions: A graphical procedure Andrew Maas Portland State University Department of Physics Nano-Crystallography Group 1 What s a bicrystal? A bicrystal in this talk is two crystals

More information

Chapter One: The Structure of Metals

Chapter One: The Structure of Metals Fourth Edition SI Version Chapter One: The Structure of Metals 2010. Cengage Learning, Engineering. All Rights Reserved. 1.1 Importance of the structure: Structures Processing Properties Applications Classification

More information

Solid State Device Fundamentals

Solid State Device Fundamentals Solid State Device Fundamentals ENS 345 Lecture Course by Alexander M. Zaitsev alexander.zaitsev@csi.cuny.edu Tel: 718 982 2812 Office 4N101b 1 Solids Three types of solids classified according to atomic

More information

Fundamentals of Crystalline State and Crystal Lattice p. 1 Crystalline State p. 2 Crystal Lattice and Unit Cell p. 4 Shape of the Unit Cell p.

Fundamentals of Crystalline State and Crystal Lattice p. 1 Crystalline State p. 2 Crystal Lattice and Unit Cell p. 4 Shape of the Unit Cell p. Fundamentals of Crystalline State and Crystal Lattice p. 1 Crystalline State p. 2 Crystal Lattice and Unit Cell p. 4 Shape of the Unit Cell p. 7 Crystallographic Planes, Directions, and Indices p. 8 Crystallographic

More information

Solid State Chemistry CHEM-E4155 (5 cr)

Solid State Chemistry CHEM-E4155 (5 cr) Solid State Chemistry CHEM-E4155 (5 cr) Spring 2017 Antti Karttunen Department of Chemistry and Materials Science Aalto University Course outline Teachers: Antti Karttunen and Otto Mustonen Lectures 16

More information

Topic 2-1: Lattice and Basis Kittel Pages: 2-9

Topic 2-1: Lattice and Basis Kittel Pages: 2-9 Topic 2-1: Lattice and Basis Kittel Pages: 2-9 Summary: We begin our introduction of crystal structure by defining a few terms. The first is translational symmetry which explains the periodicity of a crystal.

More information

Symmetry and Properties of Crystals (MSE638) Important Concepts of Crystallography

Symmetry and Properties of Crystals (MSE638) Important Concepts of Crystallography Symmetry and Properties of Crystals (MSE638) Important Concepts of Crystallography Somnath Bhowmick Materials Science and Engineering, IIT Kanpur January 8, 2019 Crystallography Study of the crystals/patterns

More information

Condensed Matter in a Nutshell

Condensed Matter in a Nutshell PHYS 342/555 Condensed Matter in a Nutshell Instructor: Dr. Pengcheng Dai Professor of Physics The University of Tennessee (Room 407A, Nielsen, 974-1509) (Office hours: TR 1:10PM-2:00 PM) Lecture 2, room

More information

GEOL. 40 ELEMENTARY MINERALOGY

GEOL. 40 ELEMENTARY MINERALOGY CRYSTAL SYMMETRY AND CLASSIFICATION A. INTRODUCTION Solid matter, which possesses ordered internal structure, wherever it may be, is called a crystal. Such order in the internal structure is also manifested

More information

Prof. Stephen A. Nelson Geology 211. Crystal Form, Zones, Crystal Habit. Crystal Forms

Prof. Stephen A. Nelson Geology 211. Crystal Form, Zones, Crystal Habit. Crystal Forms Prof. Stephen A. Nelson Geology 211 Tulane University Mineralogy Crystal Form, Zones, Crystal Habit This page last updated on 27-Aug-2002 Crystal Forms As stated at the end of the last lecture, the next

More information

Solid State Physics 460- Lecture 2a Structure of Crystals (Kittel Ch. 1)

Solid State Physics 460- Lecture 2a Structure of Crystals (Kittel Ch. 1) Solid State Physics 460- Lecture 2a Structure of Crystals (Kittel Ch. 1) See many great sites like ob s rock shop with pictures and crystallography info: http://www.rockhounds.com/rockshop/xtal/index.html

More information

MITOCW ocw oct2005-pt2-220k_512kb.mp4

MITOCW ocw oct2005-pt2-220k_512kb.mp4 MITOCW ocw-3.60-20oct2005-pt2-220k_512kb.mp4 PROFESSOR: Since z, that's straight up. And that is going to provide for you a cell that has the shape of a square prism. This would be a1. This would be a2.

More information

Lecture course on solid state physics for Nano, 2019

Lecture course on solid state physics for Nano, 2019 Prof. U. Pietsch Department of Physics, University of Siegen Lecture course on solid state physics for Nano, 2019 Lecture 1 Introduction in crystallography Objectives of the course To provide the basic

More information

STATE OF SOLIDIFICATION & CRYSTAL STRUCTURE

STATE OF SOLIDIFICATION & CRYSTAL STRUCTURE STATE OF SOLIDIFICATION & CRYSTAL STRUCTURE Chapter Outline Determination of crystal properties or properties of crystalline materials. Crystal Geometry! Crystal Directions! Linear Density of atoms! Crystal

More information

Review key concepts from last lecture (lattice + basis = unit cell) Bravais lattices Important crystal structures Intro to miller indices

Review key concepts from last lecture (lattice + basis = unit cell) Bravais lattices Important crystal structures Intro to miller indices Outline: Review key concepts from last lecture (lattice + basis = unit cell) Bravais lattices Important crystal structures Intro to miller indices Review (example with square lattice) Lattice: square,

More information

UNIT V -CRYSTAL STRUCTURE

UNIT V -CRYSTAL STRUCTURE UNIT V -CRYSTAL STRUCTURE Solids are of two types: Amorphous and crystalline. In amorphous solids, there is no order in the arrangement of their constituent atoms (molecules). Hence no definite structure

More information

Crystallography. Duration: three weeks (8 to 9 hours) One problem set. Outline: 1- Bravais Lattice and Primitive

Crystallography. Duration: three weeks (8 to 9 hours) One problem set. Outline: 1- Bravais Lattice and Primitive Crystallography Duration: three weeks (8 to 9 hours) One problem set Outline: 1- Bravais Lattice and Primitive 2- Cubic lattices, Simple, Body-centered and Face-centered 3- Primitive Unit Cell, Wigner-Seitz

More information

Protein Structure and Function. Methods for Protein Structure- Function Studies (I) X-ray Crystallography (I)

Protein Structure and Function. Methods for Protein Structure- Function Studies (I) X-ray Crystallography (I) BCHS 6229 Protein Structure and Function Lecture 8 (Nov 3, 2011) Methods for Protein Structure- Function Studies (I) X-ray Crystallography (I) 1 X-ray crystallography Exciting time for structural studies

More information

Bio5325 Fall Crystal Vocabulary

Bio5325 Fall Crystal Vocabulary Crystals and Crystallization Bio5325 Fall 2007 Crystal Vocabulary Mosaicity (mosaic spread) Protein crystals are imperfect, consisting of a mosaic of domains that are slightly misaligned. As a result,

More information

An Introduction to X-Ray Powder Diffraction. credits to: Scott A Speakman, Patrick McArdle Edited by Di Cicco 2014

An Introduction to X-Ray Powder Diffraction. credits to: Scott A Speakman, Patrick McArdle Edited by Di Cicco 2014 An Introduction to X-Ray Powder Diffraction credits to: Scott A Speakman, Patrick McArdle Edited by Di Cicco 2014 LATTICE ARRAYS AND BRAVAIS LATTICES Crystalline materials differ from amorphous materials

More information

MME 2001 MATERIALS SCIENCE

MME 2001 MATERIALS SCIENCE MME 2001 MATERIALS SCIENCE 1 20.10.2015 crystal structures X tal structure Coord. # Atoms/ unit cell a=f(r) APF % SC 6 1 2R 52 BCC 8 2 4R/ 3 68 FCC 12 4 2R 2 74 HCP 12 6 2R 74 Theoretical Density, knowing

More information

Twins & Dislocations in HCP Textbook & Paper Reviews. Cindy Smith

Twins & Dislocations in HCP Textbook & Paper Reviews. Cindy Smith Twins & Dislocations in HCP Textbook & Paper Reviews Cindy Smith Motivation Review: Outline Crystal lattices (fcc, bcc, hcp) Fcc vs. hcp stacking sequences Cubic {hkl} naming Hcp {hkil} naming Twinning

More information

Chapter1: Crystal Structure 1

Chapter1: Crystal Structure 1 Chapter1: Crystal Structure 1 University of Technology Laser Engineering & Optoelectronic Department Glass: 3 rd year Optoelectronic Engineering Subject: Solid state physics & material science Ass. Prof.

More information

External Symmetry of Crystals, 32 Crystal Classes

External Symmetry of Crystals, 32 Crystal Classes Prof. Stephen A. Nelson Geology 211 Tulane University Mineralogy External Symmetry of Crystals, 32 Crystal Classes This page last updated on 03-Sep-2002 As stated in the last lecture, there are 32 possible

More information

GEOLOGY 585: OPTICAL MINERALOGY & PETROLOGY

GEOLOGY 585: OPTICAL MINERALOGY & PETROLOGY Dr. Helen Lang Dept. of Geology & Geography West Virginia University SPRING 2009 GEOLOGY 585: OPTICAL MINERALOGY & PETROLOGY A Mineral must be crystalline Crystalline means that it has an orderly and repetitive

More information

Solid State Device Fundamentals

Solid State Device Fundamentals Solid State Device Fundamentals ENS 345 Lecture Course by Alexander M. Zaitsev alexander.zaitsev@csi.cuny.edu Tel: 718 982 2812 Office 4N101b 1 Interatomic bonding Bonding Forces and Energies Equilibrium

More information

S. PFLANZ AND W. MORITZ 727

S. PFLANZ AND W. MORITZ 727 S. PFLANZ AND W. MORITZ 727 FENTER, P. & Lu, T.-M. (1985). Su~ Sci. 154, 15-21. HENDRICKS, S. B. & TELLER, E. (1942). J. Chem. Phys. 10, 147-167. HOSEMANN, R. & BAGCHI, S. N. (1962). Direct Analysis of

More information

ENGINEERING GEOLOGY PROF: DEBASIS ROY DEPARTMENT OF CIVIL ENGINEERING. INDIAN INSTITUTE OF TECHNOLOGY, Kharagpur LECTURE - 6

ENGINEERING GEOLOGY PROF: DEBASIS ROY DEPARTMENT OF CIVIL ENGINEERING. INDIAN INSTITUTE OF TECHNOLOGY, Kharagpur LECTURE - 6 ENGINEERING GEOLOGY PROF: DEBASIS ROY DEPARTMENT OF CIVIL ENGINEERING INDIAN INSTITUTE OF TECHNOLOGY, Kharagpur LECTURE - 6 Crystallography and Optical Properties of Minerals Hello every one and welcome

More information

Density Computations

Density Computations CHAPTER 3 THE STRUCTURE OF CRYSTALLINE SOLIDS Fundamental Concepts 3.1 What is the difference between atomic structure and crystal structure? Unit Cells Metallic Crystal Structures 3.2 If the atomic radius

More information

Example: Compute the wavelength of a 1 [kg] block moving at 1000 [m/s].

Example: Compute the wavelength of a 1 [kg] block moving at 1000 [m/s]. Example: Calculate the energy required to excite the hydrogen electron from level n = 1 to level n = 2. Also calculate the wavelength of light that must be absorbed by a hydrogen atom in its ground state

More information

Primitive cells, Wigner-Seitz cells, and 2D lattices. 4P70, Solid State Physics Chris Wiebe

Primitive cells, Wigner-Seitz cells, and 2D lattices. 4P70, Solid State Physics Chris Wiebe Primitive cells, Wigner-Seitz cells, and 2D lattices 4P70, Solid State Physics Chris Wiebe Choice of primitive cells! Which unit cell is a good choice?! A, B, and C are primitive unit cells. Why?! D, E,

More information

Chapter-3 MSE-201-R. Prof. Dr. Altan Türkeli

Chapter-3 MSE-201-R. Prof. Dr. Altan Türkeli Chapter-3 MSE-201-R Prof. Dr. Altan Türkeli The Structure of Crystalline Solids FUNDAMENTAL CONCEPTS Solid materials may be classified according to the regularity with which atoms or ions are arranged

More information

Crystallographic orientation

Crystallographic orientation Crystallographic orientation Orientations and misorientations Orientation (g): The orientation of the crystal lattice with respect to some reference frame; usual a frame defined by the processing or sample

More information

MSE420/514: Session 1. Crystallography & Crystal Structure. (Review) Amaneh Tasooji

MSE420/514: Session 1. Crystallography & Crystal Structure. (Review) Amaneh Tasooji MSE420/514: Session 1 Crystallography & Crystal Structure (Review) Crystal Classes & Lattice Types 4 Lattice Types 7 Crystal Classes SIMPLE CUBIC STRUCTURE (SC) Rare due to poor packing (only Po has this

More information

GEOLOGY 284: MINERALOGY

GEOLOGY 284: MINERALOGY Dr. Helen Lang Dept. of Geology & Geography West Virginia University FALL 2005 GEOLOGY 284: MINERALOGY The Six Crystal Systems Minerals are Grouped into Six Crystal Systems based on Symmetry System Characteristic

More information

CHAPTER 4 INTRODUCTION TO DISLOCATIONS. 4.1 A single crystal of copper yields under a shear stress of about 0.62 MPa. The shear modulus of

CHAPTER 4 INTRODUCTION TO DISLOCATIONS. 4.1 A single crystal of copper yields under a shear stress of about 0.62 MPa. The shear modulus of CHAPTER 4 INTRODUCTION TO DISLOCATIONS 4.1 A single crystal of copper yields under a shear stress of about 0.62 MPa. The shear modulus of copper is approximately. With this data, compute an approximate

More information

Chapter 1. Crystal Structure

Chapter 1. Crystal Structure Chapter 1. Crystal Structure Crystalline solids: The atoms, molecules or ions pack together in an ordered arrangement Amorphous solids: No ordered structure to the particles of the solid. No well defined

More information

Semiconductor Physics

Semiconductor Physics 10p PhD Course Semiconductor Physics 18 Lectures Nov-Dec 2011 and Jan Feb 2012 Literature Semiconductor Physics K. Seeger The Physics of Semiconductors Grundmann Basic Semiconductors Physics - Hamaguchi

More information

CRYSTAL GEOMETRY. An Introduction to the theory of lattice transformation in metallic materials with Matlab applications. 8 courses of 2 hours

CRYSTAL GEOMETRY. An Introduction to the theory of lattice transformation in metallic materials with Matlab applications. 8 courses of 2 hours CRYSTAL GEOMETRY An Introduction to the theory of lattice transformation in metallic materials with Matlab applications Français Cours 0 : lundi 4 décembre 9h30-11h30 Cours 1 : vendredi 8 décembre 9h30-11h30

More information

ECE440 Nanoelectronics. Lecture 08 Review of Solid State Physics

ECE440 Nanoelectronics. Lecture 08 Review of Solid State Physics ECE440 Nanoelectronics Lecture 08 Review of Solid State Physics A Brief review of Solid State Physics Crystal lattice, reciprocal lattice, symmetry Crystal directions and planes Energy bands, bandgap Direct

More information

Close Packings of Spheres I.

Close Packings of Spheres I. Close Packings of Spheres I. close packed layer a non-close packed layer stacking of 2 close packed layers 3rd layer at position S: h.c.p. 3rd layer at position T: c.c.p. h.c.p.: hexagonal close packing

More information

CHAPTER 3. Crystal Structures and Crystal Geometry 3-1

CHAPTER 3. Crystal Structures and Crystal Geometry 3-1 CHAPTER 3 Crystal Structures and Crystal Geometry 3-1 The Space Lattice and Unit Cells 3-2 Atoms, arranged in repetitive 3-Dimensional pattern, in long range order (LRO) give rise to crystal structure.

More information

Orientation / Texture Polyethylene films

Orientation / Texture Polyethylene films Application Note PT-002 Orientation / Texture Polyethylene films Polyethylene (PE) film is one of the most commonly used polymeric products and orientation measurements of this material are of great interest.

More information

Single crystal X-ray diffraction. Zsolt Kovács

Single crystal X-ray diffraction. Zsolt Kovács Single crystal X-ray diffraction Zsolt Kovács based on the Hungarian version of the Laue lab description which was written by Levente Balogh, Jenő Gubicza and Lehel Zsoldos INTRODUCTION X-ray diffraction

More information

EP 364 SOLID STATE PHYSICS. Prof. Dr. Beşire Gönül. Course Coordinator

EP 364 SOLID STATE PHYSICS. Prof. Dr. Beşire Gönül. Course Coordinator EP 364 SOLID STATE PHYSICS Course Coordinator Prof. Dr. Beşire Gönül INTRODUCTION AIM OF SOLID STATE PHYSICS WHAT IS SOLID STATE PHYSICS AND WHY DO IT? CONTENT REFERENCES EP364 SOLID STATE PHYSICS INTRODUCTION

More information

Solids can be distinguished from liquids and gases due to their characteristic properties. Some of these are as follows:

Solids can be distinguished from liquids and gases due to their characteristic properties. Some of these are as follows: We know solids are the substances which have definite volume and definite shape. A solid is nearly incompressible state of matter. This is because the particles or units (atoms, molecules or ions) making

More information

بسم هللا الرحمن الرحیم. Materials Science. Chapter 3 Structures of Metals & Ceramics

بسم هللا الرحمن الرحیم. Materials Science. Chapter 3 Structures of Metals & Ceramics بسم هللا الرحمن الرحیم Materials Science Chapter 3 Structures of Metals & Ceramics 1 ISSUES TO ADDRESS... How do atoms assemble into solid structures? How does the density of a material depend on its structure?

More information

3. Anisotropic blurring by dislocations

3. Anisotropic blurring by dislocations Dynamical Simulation of EBSD Patterns of Imperfect Crystals 1 G. Nolze 1, A. Winkelmann 2 1 Federal Institute for Materials Research and Testing (BAM), Berlin, Germany 2 Max-Planck- Institute of Microstructure

More information

UNIVERSITY OF OSLO. Faculty of Mathematics and Natural Sciences

UNIVERSITY OF OSLO. Faculty of Mathematics and Natural Sciences Page 1 UNIVERSITY OF OSLO Faculty of Mathematics and Natural Sciences Exam in MENA3100 Characterization of materials Day of exam: 12th. June 2015 Exam hours: 14:30 This examination paper consists of 5

More information

Crystal Structure. Andrew R. Barron Carissa Smith. 1 Introduction. 2 Crystallography

Crystal Structure. Andrew R. Barron Carissa Smith. 1 Introduction. 2 Crystallography OpenStax-CNX module: m16927 1 Crystal Structure Andrew R. Barron Carissa Smith This work is produced by OpenStax-CNX and licensed under the Creative Commons Attribution License 2.0 1 Introduction In any

More information

X-RAY DIFFRACTIO N B. E. WARREN

X-RAY DIFFRACTIO N B. E. WARREN X-RAY DIFFRACTIO N B. E. WARREN Chapter 1 X-Ray Scattering by Atom s 1.1 Classical scattering by a free electron 1 1.2 Polarization by scattering 4 1.3 Scattering from several centers, complex representation

More information

X-ray diffraction and structure analysis Introduction

X-ray diffraction and structure analysis Introduction Teknillisen fysiikan ohjelmatyö X-ray diffraction and structure analysis Introduction Oleg Heczko 120 100 80 118 12-5 125 Ni-Mn-Ga (298K) SQRT(Intensity) 60 40 20 015 200 123 12-7 20-10 20,10 20-8 040

More information

Solid State-1 1) Ionic solids are characterised by 1) Good conductivity in solid state 2) High vapour pressure 3) Low melting point 4) Solubility in polar solvents 2) Three metals X, Y and Z are crystallised

More information

Defects in solids http://www.bath.ac.uk/podcast/powerpoint/inaugural_lecture_250407.pdf http://www.materials.ac.uk/elearning/matter/crystallography/indexingdirectionsandplanes/indexing-of-hexagonal-systems.html

More information

ECE236A Semiconductor Heterostructure Materials Defects in Semiconductor Crystals Lecture 6 Oct. 19, 2017

ECE236A Semiconductor Heterostructure Materials Defects in Semiconductor Crystals Lecture 6 Oct. 19, 2017 ECE236A Semiconductor Heterostructure Materials Defects in Semiconductor Crystals Lecture 6 Oct. 19, 2017 Stacking sequence in simple crystals. Stacking faults (intrinsic, extrinsic) Twin boundaries Dislocations

More information

X-RAY DIFFRACTION IN SEMICONDUCTOR INDUSTRY AND RESEARCH

X-RAY DIFFRACTION IN SEMICONDUCTOR INDUSTRY AND RESEARCH X-RAY DIFFRACTION IN SEMICONDUCTOR INDUSTRY AND RESEARCH M. Leszczyński High Pressure Research Center UNIPRESS, Sokolowska 29/37, 01 142 Warsaw, Poland, e-mail: mike@unipress.waw.pl ABSTRACT The paper

More information

This lecture is part of the Basic XRD Course.

This lecture is part of the Basic XRD Course. This lecture is part of the Basic XRD Course. Basic XRD Course 1 A perfect polycrystalline sample should contain a large number of crystallites. Ideally, we should always be able to find a set of crystallites

More information

Unit-I. Engineering Physics-I.

Unit-I. Engineering Physics-I. Unit-I Engineering Physics-I INTRODUCTION TO CRYSTAL PHYSICS CRYSTALLINE AND NONCRYSTALLINE SOLIDS SPACE LATTICE CRYSTAL STRUCTURE LATTICE PARAMETERS CRYSTAL SYSTEMS BRAVAIS LATTICES INTRODUCTION TO CRYSTAL

More information

3D 14 BRAVAIS LATTICES AND THE SEVEN CRYSTAL SYSTEM

3D 14 BRAVAIS LATTICES AND THE SEVEN CRYSTAL SYSTEM االنظمة البلورية CRYSTAL SYSTEMS 3D 14 BRAVAIS LATTICES AND THE SEVEN CRYSTAL SYSTEM There are only seven different shapes of unit cell which can be stacked together to completely fill all space (in 3

More information

CRYOLITE. INrnonucrtoN

CRYOLITE. INrnonucrtoN CRYOLITE TWINNING J. D. H. DoNNav, The Johns Hopkins (Jni,tersity, B alti.more I 8, M aryland,. Ansrnecr Thirteen twin laws are predicted by ttreory (Friedel); most of trem are observed (Bdggild). The

More information

Chapter 3: Atomic and Ionic Arrangements. Chapter 3: Atomic and Ionic Arrangements Cengage Learning Engineering. All Rights Reserved.

Chapter 3: Atomic and Ionic Arrangements. Chapter 3: Atomic and Ionic Arrangements Cengage Learning Engineering. All Rights Reserved. Chapter 3: Atomic and Ionic Arrangements 3-1 Learning Objectives 1. 2. 3. 4. 5. 6. 7. 8. Short-range order versus long-range order Amorphous materials Lattice, basis, unit cells, and crystal structures

More information

Lectures on: Introduction to and fundamentals of discrete dislocations and dislocation dynamics. Theoretical concepts and computational methods

Lectures on: Introduction to and fundamentals of discrete dislocations and dislocation dynamics. Theoretical concepts and computational methods Lectures on: Introduction to and fundamentals of discrete dislocations and dislocation dynamics. Theoretical concepts and computational methods Hussein M. Zbib School of Mechanical and Materials Engineering

More information

Key crystallographic concepts: Theory of diffraction. (Crystallography y without tears, Part 1)

Key crystallographic concepts: Theory of diffraction. (Crystallography y without tears, Part 1) Protein Crystallography (3) Key crystallographic concepts: Theory of diffraction. (Crystallography y without tears, Part 1) Cele Abad-Zapatero University of Illinois at Chicago Center for Pharmaceutical

More information

X-Ray Diffraction by Macromolecules

X-Ray Diffraction by Macromolecules N. Kasai M. Kakudo X-Ray Diffraction by Macromolecules With 351 Figures and 56 Tables Kodansha ~Springer ... Contents Preface v Part I Fundamental 1. Essential Properties of X-Rays................. 3 1.1

More information

Energy and Packing. typical neighbor bond energy. typical neighbor bond energy. Dense, regular-packed structures tend to have lower energy.

Energy and Packing. typical neighbor bond energy. typical neighbor bond energy. Dense, regular-packed structures tend to have lower energy. Energy and Packing Non dense, random packing Energy typical neighbor bond length typical neighbor bond energy r Dense, regular packing Energy typical neighbor bond length typical neighbor bond energy r

More information

Rounding a method for estimating a number by increasing or retaining a specific place value digit according to specific rules and changing all

Rounding a method for estimating a number by increasing or retaining a specific place value digit according to specific rules and changing all Unit 1 This unit bundles student expectations that address whole number estimation and computational fluency and proficiency. According to the Texas Education Agency, mathematical process standards including

More information

The object of this experiment is to test the de Broglie relationship for matter waves,

The object of this experiment is to test the de Broglie relationship for matter waves, Experiment #58 Electron Diffraction References Most first year texts discuss optical diffraction from gratings, Bragg s law for x-rays and electrons and the de Broglie relation. There are many appropriate

More information

arxiv: v2 [cond-mat.mtrl-sci] 18 Dec 2016

arxiv: v2 [cond-mat.mtrl-sci] 18 Dec 2016 Energy of low angle grain boundaries based on continuum dislocation structure Luchan Zhang a, Yejun Gu b, Yang Xiang a, arxiv:161.4318v2 [cond-mat.mtrl-sci] 18 Dec 216 a Department of Mathematics, The

More information

Answer All Questions. All Questions Carry Equal Marks. Time: 20 Min. Marks: 10.

Answer All Questions. All Questions Carry Equal Marks. Time: 20 Min. Marks: 10. Code No: 09A1BS02 Set No. 1 JAWAHARLAL NEHRU TECHNOLOGICAL UNIVERSITY HYDERABAD I B.Tech. I Mid Examinations, November 2009 ENGINEERING PHYSICS Objective Exam Name: Hall Ticket No. A Answer All Questions.

More information

Application of Backscatter Kikuchi Diffraction in the Scanning Electron Microscope to the Study of NiS2

Application of Backscatter Kikuchi Diffraction in the Scanning Electron Microscope to the Study of NiS2 189 J. Appl. Cryst. (1989). 22, 189-200 Application of Backscatter Kikuchi Diffraction in the Scanning Electron Microscope to the Study of NiS2 By K. Z. BABA-KISHI* AND D. J. DINGLEY H. H. Wills Physics

More information

Crystallographic aspects of L1 0 magnetic materials

Crystallographic aspects of L1 0 magnetic materials Scripta Materialia 53 (2005) 383 388 www.actamat-journals.com Crystallographic aspects of L1 0 magnetic materials David E. Laughlin a,b, Kumar Srinivasan a,b,1, Mihaela Tanase b,c, *, Lisha Wang a,2 a

More information

Activation of deformation mechanism

Activation of deformation mechanism Activation of deformation mechanism The deformation mechanism activates when a critical amount of mechanical stress imposed to the crystal The dislocation glide through the slip systems when the required

More information

Reflection of X-rays with change of frequency- Part 111. The case of sodium nitrate

Reflection of X-rays with change of frequency- Part 111. The case of sodium nitrate Proc. Indian Acad. Sci. All 398-408 (1940) Reflection of X-rays with change of frequency- Part 111. The case of sodium nitrate SIR C V RAMAN and DR P NILAKANTAN Department of *Physics, Indian Institute

More information

Chemistry/Materials Science and Engineering C150 Introduction to Materials Chemistry

Chemistry/Materials Science and Engineering C150 Introduction to Materials Chemistry Chemistry/Materials Science and Engineering C150 Introduction to Materials Chemistry Class will meet Tuesdays and Thursdays, 8:00-9:30 am, in 433 Latimer Hall. Instructor: Office Hours: Jeffrey Long (211

More information

Index. Cambridge University Press Introduction to Elasticity Theory for Crystal Defects R. W. Balluffi. Index.

Index. Cambridge University Press Introduction to Elasticity Theory for Crystal Defects R. W. Balluffi. Index. Airy stress functions formulation of 60 1 table of 426 alternator operator 419 Brown s formula 255 Burgers equation 264 5 Christoffel stiffness tensor 34 corresponding elastic fields 25 7 curvature tensor,

More information

Quiz on Monday covering: -symmetry operations -notations of axes, vectors, and face notation -Miller indices

Quiz on Monday covering: -symmetry operations -notations of axes, vectors, and face notation -Miller indices OTHER ANNOUNCEMENTS Quiz on Monday covering: -symmetry operations -notations of axes, vectors, and face notation -Miller indices 2 nd Draft of References due Monday Field Trip Saturday 10/4 and Sunday

More information

Introduction to Solid State Physics

Introduction to Solid State Physics z y x Introduction to Solid State Physics Lecture 2 Prof. Igor Shvets ivchvets@tcd.ie Slide 1Lecture 2 Primitive Vectors of a Bravais Lattice By definition all Bravais lattices must be described by a set

More information

STANDARD 1 NUMBER and OPERATION

STANDARD 1 NUMBER and OPERATION Goal 1.1: Understand and use numbers. STANDARD 1 NUMBER and OPERATION 6.M.1.1.1 Compare magnitudes and relative magnitudes of positive rational numbers, including whole numbers through billions, fractions,

More information