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Phys 460 Lecture 14
(
pdf version - 6 slides/page
)
Monday, October 16, 2006
Lecturer: Richard Martin
Homework 6
Reading:
Kittel, Chapt. 7
Energy Bands for Electrons in Crystals
Outline
From previous lectures:
Part I: Crystal Structures, Diffraction, Reciprocal Lattice, Crystal binding
Phonons, Dispersion curves,Thermal properties
Free electron gas
Recall from last two lectures on the electron gas
Chose non-interacting electron gas as the simplest model for electrons
"Electrons in a box of size L x L x L "
Solved Schrodinger Equation for electrons
Result: Wavefunction psi
k
(r) = exp (i k r); energy = E
k
= (hbar
2
/2m) k
2
k determined by boundary condition that electrons fit in the box
Periodic boundary condition is simplest: leads to k
x
= integer (2 pi /L), etc.
Pauli exclusion principle leads to states being filled up to an energy called the Fermi energy
The electron gas is always a metal
The next steps
How do we understand that some materials are insulators and some are metals?
Are there simple principles that help us understand and even predict which materials will be metals vs which will be insulators?
What is a semiconductor? (Answered later.)
The first step: Qualitative ideas that show the effect of the lattice on electrons in one dimension
Consider the lattice as a weak effect upon the free electron gas that we studied before
Bragg reflection at the zone boundary
Leads to energy bands with an energy gap
Interpretation of why states at the zone boundary become standing waves with a splitting of the energy to form a gap
[Note similarity to phonons!]
Qualitative Picture of he effect of the lattice
"Allowed" energy bands - energies of allowed quantum states
"Forbidden" energy gaps - energies where there are no allowed quantum states
Simple principles that help us understand that a material can be a metal or an insulators
More complete discussion next time - more about semiconductors later
Next time
Bloch Theorem
How bands give us the basis understanding of metals vs. insulators
Email clarification questions and corrections to
rmartin@uiuc.edu
Email questions on solving problems to
xin2@.uiuc.edu