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Phys 460 Lecture 25
(
pdf version - 6 slides/page
)
Wed, November 29, 2006
Lecturer: Richard Martin
No new homework today
Reading:
Kittel, Ch. 18, p 523-527
Surfaces – Tunneling - STM
Outline
From previous lectures:
Part I: Crystal Structures, Diffraction, Reciprocal Lattice, Crystal binding
Phonons, Dispersion curves, Thermal properties
Part II: Free electron gas, Energy bands for electrons in crystals E
k
n
, gaps, metals vs. insulators, semiconductors
Part III:
Semiconductor devices - inhomogeneous semiconductors - heterostructures
Semiconductor nanostructures
Metals - brief overview - electron gas ideas generalized to real metals
Superconductivity
Magnetism
Surfaces
Termination of a crystal makes a two-dimensional periodic surface
Perfect crystal - perfect 2D periodicity
Real crystals - planes with terraces, steps, .....
Example of GaAs
Tunneling in quantum mechanics
Particles can tunnel through barrier
Exponential decay where E < V
Simple formulas that can be solved exactly for constant V
Example of a barrier of height V
0
STM
Electrons tunnel through space between tip and sample
Extreme sensitivity of tunneling current tas a function of the distance from tip to sample
Dominated by a single atom on tip - an atom that just happens to be on the tip
Atomic scale resolution even though the whole tip is much larger
Examples
GaAs, Mn atoms on GaAs
Adatoms on Cu show ability to move adatoms around, electron waves, ....
GaN surface that illustrate growth, ….
Atomic Force Microscope - AFM
Atomically sharp tip
Detect forces by very sensitive detection of displacement of cantilever
Works on insulators
Article in Physics Today, December, 2006
Email clarification questions and corrections to
rmartin@uiuc.edu
Email questions on solving problems to
xin2@.uiuc.edu