Why Study Solid State Physics?

Slides:



Advertisements
Similar presentations
INTRODUCTION TO CERAMIC MINERALS
Advertisements

Crystal Structure Continued!
Nanochemistry NAN 601 Dr. Marinella Sandros
III Crystal Symmetry 3-1 Symmetry elements (1) Rotation symmetry
3-Dimensional Crystal Structure
CRYSTAL STRUCTURE.
II. Crystal Structure Lattice, Basis, and the Unit Cell
Lecture 2: Crystal Symmetry
When dealing with crsytalline materials, it is often necessary to specify a particular point within a unit cell, a particular direction or a particular.
Wigner-Seitz Cell The Wigner–Seitz cell around a lattice point is defined as the locus of points in space that are closer to that lattice point than to.
II Crystal Structure 2-1 Basic concept
Lec. (4,5) Miller Indices Z X Y (100).
Miller indices and crystal directions
THE “MOST IMPORTANT” CRYSTAL STRUCTURES. NOTE!! Much of the discussion & many figures in what follows was again constructed from lectures posted on the.
Solid State Physics 2. X-ray Diffraction 4/15/2017.
Typical Crystal Structures
Solid State Physics (1) Phys3710
CONDENSED MATTER PHYSICS PHYSICS PAPER A BSc. (III) (NM and CSc.) Harvinder Kaur Associate Professor in Physics PG.Govt College for Girls Sector -11, Chandigarh.
Order in crystals Symmetry, X-ray diffraction. 2-dimensional square lattice.
Mineralogy Carleton College Winter Lattice and its properties Lattice: An imaginary 3-D framework, that can be referenced to a network of regularly.
Lecture 12 (10/30/2006) Crystallography Part 5: Internal Order and 2-D Symmetry Plane Lattices Planar Point Groups Plane Groups.
Crystalline Structures Edward A. Mottel Department of Chemistry Rose-Hulman Institute of Technology.
The internal order of minerals: Lattices, Unit Cell & Bravais Lattices
PH0101 UNIT 4 LECTURE 3 CRYSTAL SYMMETRY CENTRE OF SYMMETRY
Lecture 2: Crystal Structure PHYS 430/603 material Laszlo Takacs UMBC Department of Physics.
Instructor: Dr. Upali Siriwardane
Solid State Physics (1) Phys3710
BRAVAIS LATTICE Infinite array of discrete points arranged (and oriented) in such a way that it looks exactly the same from whichever point the array.
Solid State Physics (1) Phys3710
1 Crystalline Nature of Solids 01 Mar, Crystalline Nature of Solids.
EEE539 Solid State Electronics 1. Crystal Structure Issues that are addressed in this chapter include:  Periodic array of atoms  Fundamental types of.
Chem Lattices By definition, crystals are periodic in three dimensions and the X-ray diffraction experiment must be understood in the context of.
Chapter 1 Crystal Structures. Two Categories of Solid State Materials Crystalline: quartz, diamond….. Amorphous: glass, polymer…..
Crystal Structure A “unit cell” is a subdivision of the lattice that has all the geometric characteristics of the total crystal. The simplest choice of.
W.D. Callister, Materials science and engineering an introduction, 5 th Edition, Chapter 3 MM409: Advanced engineering materials Crystallography.
Bravais Lattices in 2D In 2D there are five ways to order atoms in a lattice Primitive unit cell: contains only one atom (but 4 points?) Are the dotted.
Lecture 12 Crystallography
Prolog Text Book: C.Kittel, "Introduction to Solid State Physics", 8th ed.,Wiley (2005) Website:
STRUCTURE OF SOLID MATERIALS CLASSIFICATION OF SOLIDS SOLIDS CLASSIFIED AS CRYSTALLINE, AMORPHOUS OR A COMBINATION OF THE TWO. CRYSTALLINE - BUILT UP OF.
Crystal Structures Crystal is constructed by the continuous repetition in space of an identical structural unit. Lattice: a periodic array of mathematical.
PHY1039 Properties of Matter Crystallography, Lattice Planes, Miller Indices, and X-ray Diffraction (See on-line resource: )
Crystalline Solids :-In Crystalline Solids the atoms are arranged in some regular periodic geometrical pattern in three dimensions- long range order Eg.
CRYSTAL STRUCTURE.
ESO 214: Nature and Properties of Materials
Lecture 02 Fundamental Properties of Solids. Crystal SystemShape of UCBravais Lattices PIFC 1CubicCube  2TetragonalSquare Prism (general height) 
1 Prof. Ming-Jer Chen Department of Electronics Engineering National Chiao-Tung University 02/24/ /24/2015 DEE3517 Solid State Physics (1) Lecture.
ME 330 Engineering Materials
DESCRIBING CRYSTALS MATHEMATICALLY Three directional vectors Three distances: a, b, c Three angles:   ll points can be described using coordinate.
Symmetry in crystals. Infinitely repeating lattices.
Inorganic Material Chemistry
Crystal Structure NaCl Well defined surfaces
Unit 1 Fundamentals 1  Atomic Structure?  Crystal Structure?  Types of Crystals?
Fundamentals of crystal Structure
Phys 460 Describing and Classifying Crystal Lattices
THE SPACE LATTICE AND UNIT CELLS CRYSTAL SYSTEMS AND BRAVAIS LATTICES.
CHAPTER 3: STRUCTURE OF CRYSTALLINE SOLIDS
Chemistry 481(01) Spring 2017 Instructor: Dr. Upali Siriwardane
CHAPTER 1 CRYSTAL STRUCTURE
CRYSTAL LATTICE & UNIT CELL
Crystals Crystal consist of the periodic arrangement of building blocks Each building block, called a basis, is an atom, a molecule, or a group of atoms.
Crystal Structure Continued!
PH-571 Dr. Hla Ohio University
Crystal Structure and Notation
3-Dimensional Crystal Structure.
Why Study Solid State Physics?
3-Dimensional Crystal Structure
PHY 752 Solid State Physics
Chapter 3: Crystal & Amorphous structure in materials Part 1
L.
Presentation transcript:

Why Study Solid State Physics?

Ideal Crystal An ideal crystal is a periodic array of structural units, such as atoms or molecules. It can be constructed by the infinite repetition of these identical structural units in space. Structure can be described in terms of a lattice, with a group of atoms attached to each lattice point. The group of atoms is the basis.

Bravais Lattice An infinite array of discrete points with an arrangement and orientation that appears exactly the same, from any of the points the array is viewed from. A three dimensional Bravais lattice consists of all points with position vectors R that can be written as a linear combination of primitive vectors. The expansion coefficients must be integers.

Crystal lattice: Proteins

Crystal Structure

Honeycomb: NOT Bravais

Honeycomb net: Bravais lattice with two point basis

Crystal structure: basis

Translation Vector T

Translation(a1,a2), Nontranslation Vectors(a1’’’,a2’’’)

Primitive Unit Cell A primitive cell or primitive unit cell is a volume of space that when translated through all the vectors in a Bravais lattice just fills all of space without either overlapping itself or leaving voids. A primitive cell must contain precisely one lattice point.

Fundamental Types of Lattices Crystal lattices can be mapped into themselves by the lattice translations T and by various other symmetry operations. A typical symmetry operation is that of rotation about an axis that passes through a lattice point. Allowed rotations of : 2 π, 2π/2, 2π/3,2π/4, 2π/6 (Note: lattices do not have rotation axes for 1/5, 1/7 …) times 2π

Five fold axis of symmetry cannot exist

Two Dimensional Lattices There is an unlimited number of possible lattices, since there is no restriction on the lengths of the lattice translation vectors or on the angle between them. An oblique lattice has arbitrary a1 and a2 and is invariant only under rotation of π and 2 π about any lattice point.

Oblique lattice: invariant only under rotation of pi and 2 pi

Two Dimensional Lattices

Three Dimensional Lattice Types

Wigner-Seitz Primitive Cell: Full symmetry of Bravais Lattice

Conventional Cells

Cubic space lattices

Cubic lattices

BCC Structure

BCC Crystal

BCC Lattice

Primitive vectors BCC

Elements with BCC Structure Note: This was the end of lecture 1

Summary: Bravais Lattices (Nets) in Two Dimensions

Escher loved two dimensional structures too

Summary: Fourteen Bravais Lattices in Three Dimensions

Fourteen Bravais Lattices …

FCC Structure

FCC lattice

Primitive Cell: FCC Lattice

FCC: Conventional Cell With Basis We can also view the FCC lattice in terms of a conventional unit cell with a four point basis. Similarly, we can view the BCC lattice in terms of a conventional unit cell with a two point basis.

Elements That Have FCC Structure

Simple Hexagonal Bravais Lattice

Primitive Cell: Hexagonal System

HCP Crystal

Hexagonal Close Packing

HexagonalClosePacked HCP lattice is not a Bravais lattice, because orientation of the environment Of a point varies from layer to layer along the c-axis.

HCP: Simple Hexagonal Bravais With Basis of Two Atoms Per Point

Miller indices of lattice plane The indices of a crystal plane (h,k,l) are defined to be a set of integers with no common factors, inversely proportional to the intercepts of the crystal plane along the crystal axes:

Indices of Crystal Plane

Indices of Planes: Cubic Crystal

001 Plane

110 Planes

111 Planes

Simple Crystal Structures There are several crystal structures of common interest: sodium chloride, cesium chloride, hexagonal close-packed, diamond and cubic zinc sulfide. Each of these structures have many different realizations.

NaCl Structure

NaCl Basis

NaCl Type Elements

CsCl Structure

CsCl Basis

CsCl Basis

CeCl Crystals

Diamond Crystal Structure

ZincBlende structure

Symmetry planes

The End: Chapter 1

Bravais Lattice: Two Definitions The expansion coefficients n1, n2, n3 must be integers. The vectors a1,a2,a3 are primitive vectors and span the lattice.

HCP Close Packing

HCP Close Packing

Close Packing 2

Close Packing 3

Close Packing 4

Close Packing 5

NaCl Basis

Close Packing of Spheres