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Why Study Solid State Physics?
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Crystalstructure

Feb 24, 2023

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Page 1: Crystalstructure

Why Study Solid State Physics?

Page 2: Crystalstructure

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.

Page 3: Crystalstructure

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.

Page 4: Crystalstructure

Crystal lattice: Proteins

Page 5: Crystalstructure

Crystal Structure

Page 6: Crystalstructure

Honeycomb: NOT Bravais

Page 7: Crystalstructure

Honeycomb net: Bravais lattice with two point

basis

Page 8: Crystalstructure

Crystal structure: basis

Page 9: Crystalstructure

Translation Vector T

Page 10: Crystalstructure

Translation(a1,a2), Nontranslation

Vectors(a1’’’,a2’’’)

Page 11: Crystalstructure

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.

Page 12: Crystalstructure
Page 13: Crystalstructure

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

Page 14: Crystalstructure

Five fold axis of symmetry cannot exist

Page 15: Crystalstructure

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.

Page 16: Crystalstructure

Oblique lattice: invariant only under rotation of pi

and 2 pi

Page 17: Crystalstructure

Two Dimensional Lattices

Page 18: Crystalstructure

Three Dimensional Lattice Types

Page 19: Crystalstructure

Wigner-Seitz Primitive Cell: Full symmetry of

Bravais Lattice

Page 20: Crystalstructure

Conventional Cells

Page 21: Crystalstructure

Cubic space lattices

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Cubic lattices

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BCC Structure

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BCC Crystal

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BCC Lattice

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Primitive vectors BCC

Page 27: Crystalstructure

Elements with BCC Structure

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Summary: Bravais Lattices (Nets) in Two Dimensions

Page 29: Crystalstructure

Escher loved two dimensional structures too

Page 30: Crystalstructure

Summary: Fourteen Bravais Lattices in Three

Dimensions

Page 31: Crystalstructure

Fourteen Bravais Lattices …

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FCC Structure

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FCC lattice

Page 34: Crystalstructure

Primitive Cell: FCC Lattice

Page 35: Crystalstructure

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.

Page 36: Crystalstructure

Elements That Have FCC Structure

Page 37: Crystalstructure

Simple Hexagonal Bravais Lattice

Page 38: Crystalstructure

Primitive Cell: Hexagonal System

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HCP Crystal

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Hexagonal Close Packing

Page 41: Crystalstructure

HexagonalClosePacked

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

Page 42: Crystalstructure

HCP: Simple Hexagonal Bravais With Basis of Two

Atoms Per Point

Page 43: Crystalstructure

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:

Page 44: Crystalstructure

Indices of Crystal Plane

Page 45: Crystalstructure

Indices of Planes: Cubic Crystal

Page 46: Crystalstructure

001 Plane

Page 47: Crystalstructure

110 Planes

Page 48: Crystalstructure

111 Planes

Page 49: Crystalstructure

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.

Page 50: Crystalstructure

NaCl Structure

Page 51: Crystalstructure

NaCl Basis

Page 52: Crystalstructure

NaCl Type Elements

Page 53: Crystalstructure

CsCl Structure

Page 54: Crystalstructure

CsCl Basis

Page 55: Crystalstructure

CsCl Basis

Page 56: Crystalstructure

CeCl Crystals

Page 57: Crystalstructure

Diamond Crystal Structure

Page 58: Crystalstructure

ZincBlende structure

Page 59: Crystalstructure

Symmetry planes

Page 60: Crystalstructure

The End: Chapter 1

Page 61: Crystalstructure
Page 62: Crystalstructure

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.

Page 63: Crystalstructure

HCP Close Packing

Page 64: Crystalstructure

HCP Close Packing

Page 65: Crystalstructure

Close Packing 2

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Close Packing 3

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Close Packing 4

Page 68: Crystalstructure

Close Packing 5

Page 69: Crystalstructure

NaCl Basis

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Close Packing of Spheres

Page 71: Crystalstructure