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| PHY.F20 Molecular and Solid State Physics | |||
The eigenfunction solutions of the Schrödinger equation for free electrons are plane waves,
\[ \begin{equation} \psi(\vec{r}) = e^{i\vec{k}\cdot\vec{r}}. \end{equation} \]If the $\vec{k}$ vector is outside the first Brillouin zone, the plane wave solution can be written in Bloch form with a vector $\vec{k}'$ inside the first Brillouin zone,
\[ \begin{equation} \psi(\vec{r}) = e^{i\vec{k}'\cdot\vec{r}}e^{i\vec{G}\cdot\vec{r}}, \end{equation} \]where $\vec{k}=\vec{k}'+\vec{G}$. By writing every plane wave as a Bloch wave with a $\vec{k}$ vector inside the First Brillouin zone, the dispersion relation can be expressed as,
\[ \begin{equation} E =\frac{\hbar^2(\vec{k}'+\vec{G})^2}{2m}, \end{equation} \]where every reciprocal lattice vector $\vec{G}$ produces a different band in the first Brillouin zone.
The resulting dispersion relations for some Bravais lattices are shown below. Click on the buttons to choose a different order for the symmetry points.
1-D | |
2-D square |
2-D hexagonal |
Simple cubic |
Face centered cubic |
Body centered cubic |
Hexagonal |
Tetragonal |
Orthorhombic |
Some examples of the utility of the empty lattice approximation are shown below.
On the left is the empty lattice approximation for an fcc crystal and on the right is the calculated band structure of aluminum (an fcc metal). The right image was taken from W.A. Harrison, Physical Review, vol. 118 pp. 1182-1189 (1960).