 |
If we consider a crystal with dimensions Lx, Ly, Lz,
it has the volume V = Lx· Ly· Lz. |
|
 |
All we have to do is to replace the periodic boundary conditions ψ(x
+ L) = ψ(x) by: |
|
|
ψ(x + Lx, y, z) |
= |
ψ(x , y + Ly, z) |
= |
ψ (x, y, z + Lz) |
= | ψ(x, y, z) |
|
|
 |
This leads to simple expressions for the allowed wave vectors k: |
| |
kx | = |
0, ± |
2π Lx |
, ± | 4π
Lx | , ... |
| | |
| | |
| ky |
| 0, ± |
2π Ly |
, ± | 4π
Ly | , ... |
| | |
| | |
| kz |
| 0, ± |
2π Lz |
, ± | 4π
Lz | , .. |
|
|
|
 |
The pre-exponential factor, which was (1/L)3/2, now changes to (1/V)
1/2. |
 |
Since all relevant quantities are usually expressed as densities, i.e. divided by V,
and the quantization of k is usually given up in favor of a continuous range of k's, we may
just as well stick to the more simple description of a crystal with equal sides - the results are the same. |
| |