In mathematics and solid state physics, the first Brillouin zone is a uniquely defined primitive cell in reciprocal space. In the same way the Bravais lattice is divided up into Wigner–Seitz cells in the real lattice, the reciprocal lattice is broken up into Brillouin zones. The boundaries of this cell are given by planes related to points on the reciprocal 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.
The first Brillouin zone is the locus of points in reciprocal space that are closer to the origin of the reciprocal lattice than they are to any other reciprocal lattice points (see the derivation of the Wigner-Seitz cell). Another definition is as the set of points in k-space that can be reached from the origin without crossing any Bragg plane. Equivalently, this is the Voronoi cell around the origin of the reciprocal lattice.
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 less frequently. As a result, the first Brillouin zone is often called simply the Brillouin zone. (In general, the n-th Brillouin zone consists of the set of points that can be reached from the origin by crossing exactly n − 1 distinct Bragg planes.)
The concept of a Brillouin zone was developed by Léon Brillouin (1889–1969), a French physicist.
Several points of high symmetry are of special interest – these are called critical points.
|Γ||Center of the Brillouin zone|
|M||Center of an edge|
|X||Center of a face|
|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|
|X||Center of a square face|
|H||Corner point joining four edges|
|N||Center of a face|
|P||Corner point joining three edges|
|A||Center of a hexagonal face|
|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|
Other lattices have different types of high-symmetry points. They can be found in the illustrations below.
|Lattice system||Bravais lattice
|Triclinic Lattice type 1a (TRI1a)||Triclinic Lattice type 1b (TRI1b)||Triclinic Lattice type 2a (TRI2a)||Triclinic Lattice type 2b (TRI2b)|
|Monoclinic Lattice (MCL)|
|Base Centered Monoclinic Lattice type 1 (MCLC1)||Base Centered Monoclinic Lattice type 2 (MCLC2)||Base Centered Monoclinic Lattice type 3 (MCLC3)||Base Centered Monoclinic Lattice type 4 (MCLC4)||Base Centered Monoclinic Lattice type 5 (MCLC5)|
|Simple Orthorhombic Lattice (ORC)|
|Base Centered Orthorhombic Lattice (ORCC)|
|Body Centered Orthorhombic Lattice (ORCI)|
|Face Centered Orthorhombic Lattice type 1 (ORCF1)||Face Centered Orthorhombic Lattice type 2 (ORCF2)||Face Centered Orthorhombic Lattice type 3 (ORCF3)|
|Simple Tetragonal Lattice (TET)|
|Body Centered Tetragonal Lattice type 1 (BCT1)||Body Centered Tetragonal Lattice type 2 (BCT2)|
|Rhombohedral Lattice type 1 (RHL1)||Rhombohedral Lattice type 2 (RHL2)|
|Hexagonal Lattice (HEX)|
|Simple Cubic Lattice (CUB)|
|Body Centered Cubic Lattice (BCC)|
|Face Centered Cubic Lattice (FCC)|
- Thompson, Nick. "Irreducible Brillouin Zones and Band Structures". bandgap.io. Retrieved 13 December 2017.
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- Setyawan, Wahyu; Curtarolo, Stefano (2010). "High-throughput electronic band structure calculations: Challenges and tools". Computational Materials Science. 49 (2): 299–312. arXiv:1004.2974. Bibcode:2010arXiv1004.2974S. doi:10.1016/j.commatsci.2010.05.010.
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- Ashcroft, Neil W.; Mermin, N. David (1976). Solid State Physics. Orlando: Harcourt. ISBN 978-0-03-049346-1.
- Brillouin, Léon (1930). "Les électrons dans les métaux et le classement des ondes de de Broglie correspondantes". Comptes Rendus Hebdomadaires des Séances de l'Académie des Sciences. 191 (292).