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EE 362 Electric and Magnetic Properties of Materials

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Title: EE 362 Electric and Magnetic Properties of Materials


1
EE 362 Electric and Magnetic Properties of
Materials
  • Dr. Brian T. Hemmelman
  • Chapter 1 Slides

2
Types of Materials (2)
  • Materials can be classified as
  • Conductors Easily conduct current
  • Insulators Do not conduct significant current
  • Semiconductors Conductivity between conductors
    and insulators
  • Superconductors Zero resistance below critical
    temperature

3
Types of Materials (3)
  • Specialty areas concerned with liquid, gaseous,
    and plasma states (LCDs, gas lasers, plasma
    hydrodynamics).
  • Most current electronic materials though are
    solids.

4
Types of Solids (4)
  • Crystalline Have ordered atomic or molecular
    structure throughout.
  • Polycrystalline Have order within grains, but
    grain orientation is random.
  • Amorphous Have no order or very short range
    order.

5
Types of Solids (5)
6
Solid Electronic Materials (6)
  • Conductors insulators, amorphous
    polycrystalline organic materials are all
    important.
  • We will focus on crystalline semiconductors
    (diodes, transistors, CCDs, solar cells, etc.).

7
Crystalline Semiconductors (7)
  • Elemental Semiconductors Composed of only one
    element
  • Silicon Si
  • Germanium Ge
  • Compound Semiconductors Composed of two or more
    different elements
  • Gallium Arsenide GaAs
  • Indium Phosphide - InP

8
Crystal Structures (8)
  • Unit Cell A small volume that can be used to
    reproduce the entire crystal (through translation
    only, no rotation).
  • Primitive Cell Smallest unit cell that can be
    used to repeat (not always the most appropriate
    to visualize or describe a crystal structure).

9
Primitive Unit Cell (9)
All equivalent lattice sites can be found with
where p, q, and s are integers.
10
The 14 Bravais Lattices (10)
11
The 14 Bravais Lattices (11)
12
The 14 Bravais Lattices (12)
13
The 14 Bravais Lattices (13)
14
The 14 Bravais Lattices (14)
15
Silicon A Diamond Lattice (15)
Two interpenetrating face-centered cubic lattices
16
Gallium Arsenide Zincblende (16)
a is defined as the lattice constant (usually
in Angstroms)
17
The Diamond/Zincblende Lattice (17)
  • http//web.cecs.pdx.edu/vanhalen/courses/applets/
    silicon.html

18
Miller Indices (18)
  • We need to keep track of atomic planes and
    orientations inside the crystal.
  • Miller indices are a way to reference these
    atomic planes and directions.
  • We use the intercepts of the unit cell in terms
    of the integers p, q, and s.

19
Typical Crystal Planes (19)
20
Determining Miller Indices (20)
  • Find x, y, z axis intercepts in terms of
    integer unit quantities (does not have to be in
    terms of lattice constant a).These intercepts
    are (d e f).
  • Invert each member of the triplet

21
Determining Miller Indices (21)
  • Multiply through by smallest integer needed to
    make all values in the triplet into
    integers.The resulting integers are the Miller
    indices (h k l).

22
Determining Miller Indices (22)
  • Determine intercepts(1 3 1)
  • Invert each of these(1/1 1/3 1/1)
  • Multiply through by 3 to convert all values to
    integers(3 1 3)
  • This is a (3 1 3) plane.

23
Determining Miller Indices (23)
  • Determine intercepts(4 2 4)
  • Invert each of these(1/4 1/2 1/4)
  • Multiply through by 4 to convert all values to
    integers(1 2 1)
  • This is a (1 2 1) plane

24
Crystal Directions (24)
  • Crystal directions are also defined based on
    Miller indices.
  • A crystal direction is defined by a vector that
    is normal (perpendicular) to the crystal plane
    defined by a particular set of Miller indices.

25
Crystal Directions (25)
26
Atomic Surface Density Example (26)
Total number of atoms in this area is 1 4(1/4)
2 atoms Surface area is (a1)(1.414a1)
1.414a12 If the lattice constant is a1 5
Angstroms 510-8 cm then Surface density is (2
atoms)/(1.414(510-8 cm)2) 5.661014 atoms/cm2
27
Silicon Ingot Wafers (27)
28
Atomic Bonds (28)
  • Ionic Bonding Some atoms lose electrons
    (become ion) and some atoms gain electrons
    (become - ion).Usually atoms from opposite
    sides of the periodic chart form ionic bonds.
    For example, sodium chloride (NaCl).

29
Atomic Bonds (29)
  • Covalent Bonding Atoms share electrons to
    form complete outer shells.Usually atoms from
    middle groups of the periodic chart, e.g. Group
    III Group V, but also hydrogen molecule.

30
Atomic Bonds (30)
  • Metallic Bonds Many atoms with few valence
    electrons (Groups I, II, and III) cluster to
    share electrons and achieve a low energy
    state.Essentially becomes a bunch of nuclei
    surrounded by a sea of loosely bound electrons.

31
Atomic Bonds (31)
  • Van der Waals Some compounds may form through
    ionic bonds, but this can create an imbalance of
    charge in the molecule and establish a dipole
    (e.g. HF).There can then be electrostatic
    interactions between molecular dipoles that cause
    the molecules to cluster into a solid.
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