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(``Free
Electrons; Sommerfeld")
(AM, Ch 2)
Now let's put
into the model.
The most important effect of putting quantum mechanics into the
theory of metals is the result of treating electrons as fermions with
Fermi-Dirac statistics, rather than as a classical gas of particles
obeying the Kinetic Theory of Gases. But let's start at the
beginning.
When electrons are treated quantum mechanically, 2 things change: (a)
possible states are quantized; (b) particles are indistinguishable.
=2.0 true in
Consider non-interacting electrons moving (freely) in a constant
potential which we take to be zero.
Schroedinger's equation in 1D is
What boundary conditions do we use? (It doesn't matter all that much
because the bulk properties aren't really affected by what goes on at
the surface.)
- (a)
- Realistic, i.e.,
finite outside the metal but
decaying exponentially
as
). This is
practically never used for bulk calculations since
atomic dimensions.
- (b)
- Box: Standing Wave Solutions
at walls
.
We're interested in transport - want traveling waves.
- (c)
- Periodic:
Now traveling wave solutions are allowed.
It is easy to generalize this to 3D. Consider a box with sides
: Schroedinger's equation becomes
For periodic b.c.'s, the solution is a product wavefunction
with
The momentum carried in the plane wave state is
and the velocity
. Each state is characterized by
and by the spin
along some chosen axis. There are 2 different states for each
allowed value of
. Note that the probability density
is uniform in space.
Density of States
Suppose we are interested in some property of the
one-electron states, such as the total average number of electrons in
them. We sum over the states
where
is the number of electrons in state
with
spin
.
Assume that
is a rather smoothly varying function of
. This allows us to transform the sum into an integral.
is the density of states per unit volume of
-space. What is
?
implies that the density of allowed
values along the
-axis is
. Similar
arguments for
and
lead to
Note that this is independent of the ratio of
, and
.
In fact,
is independent of the sample shape in the
limit
, except for the lowest few states.
If spin is included, put in an extra factor of 2. Thus
if
is independent of
. In general for any
dimension
where
is the
-dimensional volume.
Next: Density of States Per
Up: Lecture 2
Previous: Seebeck Effect - Thermopower
Clare Yu
2006-10-03