Content deleted Content added
No edit summary |
|||
Line 1:
The '''Empty Lattice Approximation''' is a theoretical [[electronic band structure]] model in which the periodic potential of the crystal lattice is defined not more precisely than '''"periodic"''' and it is assumed that the potential is '''weak'''. The Empty Lattice Approximation is a description of the properties of electrons in an [[Fermi gas|electron gas]] of non-interacting [[Free electron model|free electrons]] that move through a weak periodic potential of a [[crystal structure]]. The model mainly serves to illustrate a number of concepts which are fundamental to all electronic band structure phenomena.
==
[[Image:Empty-Lattice-Approximation-FCC-bands.svg|thumb|300px|Free electron bands in a FCC crystal structure]]
[[Image:Empty-Lattice-Approximation-BCC-bands.svg|thumb|300px|Free electron bands in a BCC crystal structure]]
[[Image:Empty-Lattice-Approximation-HCP-bands.svg|thumb|500px|Free electron bands in a HCP crystal structure]]
The periodic potential of the lattice must be weak because otherwise the
{{cite book |author=C. Kittel |title=Introduction to Solid State Physics |year= 1953-1976 |publisher=Wiley & Sons |isbn=0-471-49024-5 }}
</ref>
|