
Brillouin zone
In
mathematics and
solid state physics, the first 'Brillouin zone' is a uniquely defined
primitive cell of the
reciprocal lattice in the
frequency domain. It is found by the same method as for the
Wigner-Seitz cell in the
Bravais lattice. The importance of the Brillouin zone stems from the
Bloch wave description of waves in a periodic medium, in which it is found that the solutions can be completely characterized by their behavior in a single Brillouin zone.
Taking the surfaces at the same distance from one element of the lattice and its neighbours, the
volume included is the first Brillouin zone. Another definition is as the set of points in ''k''-space that can be reached from the origin without crossing any
Bragg plane.
There are also second, third, ''etc.'', Brillouin zones, corresponding to a sequence of disjoint regions (all with the same volume) at increasing distances from the origin, but these are used more rarely. As a result, the ''first'' Brillouin zone is often called simply the ''Brillouin zone''. (In general, the ''n''-th Brillouin zone consist of the set of points that can be reached from the origin by crossing ''n'' − 1 Bragg planes.)
A related concept is that of the 'irreducible Brillouin zone', which is the first Brillouin zone reduced by all of the symmetries in the
point group of the lattice.
The concept of a Brillouin zone was developed by
Leon Brillouin(1889-1969), a French physicist.
Critical points
Several points of high symmetry are of special interest – these are called critical points.
[1]
| Symbol | Description |
|---|
| Γ | Center of the Brillouin zone |
| Simple cube |
|---|
| M | Center of an edge |
| R | Corner point |
| X | Center of a face |
| Face-centered cubic | |
|---|---|
| K | Middle of an edge joining two hexagonal faces |
| L | Center of a hexagonal face |
| U | Middle of an edge joining a hexagonal and a square face |
| W | Corner point |
| X | Center of a square face |
| Body-centered cubic | |
|---|---|
| H | Corner point joining four edges |
| N | Center of a face |
| P | Corner point joining three edges |
| Hexagonal | |
|---|---|
| A | Center of a hexagonal face |
| H | Corner point |
| K | Middle of an edge joining two rectangular faces |
| L | Middle of an edge joining a hexagonal and a rectangular face |
| M | Center of a rectangular face |
See also
★
period lattice
★
fundamental domain
References
1. Harald Ibach & Hans Lüth, ''Solid-State Physics, An Introduction to Principles of Materials Science'', corrected second printing of the second edition, 1996, Springer-Verlag, ISBN 3-540-58573-7
★ Charles Kittel, ''Introduction to Solid State Physics'' (Wiley: New York, 1996).
★ Neil W. Ashcroft and N. David Mermin, ''Solid State Physics'' (Harcourt: Orlando, 1976).
External links
★
Brillouin Zone simple lattice diagrams by Thayer Watkins
★
Brillouin Zone 3d lattice diagrams by Technion.