In geometry and crystallography, a Bravais lattice, studied by Auguste Bravais (1850), is an infinite array of discrete points in three dimensional space generated by a set of discrete translation operations described by:
where ni are any integers and ai are known as the primitive vectors which lie in different directions and span the lattice. This discrete set of vectors must be closed under vector addition and subtraction. For any choice of position vector R, the lattice looks exactly the same.
When the discrete points are atoms, ions, or polymer strings of solid matter, the Bravais lattice concept is used to formally define a crystalline arrangement and its (finite) frontiers. A crystal is made up of a periodic arrangement of one or more atoms (the basis) repeated at each lattice point. Consequently, the crystal looks the same when viewed from any equivalent lattice point, namely those separated by the translation of one unit cell (the motif).
Two Bravais lattices are often considered equivalent if they have isomorphic symmetry groups. In this sense, there are 14 possible Bravais lattices in three-dimensional space. The 14 possible symmetry groups of Bravais lattices are 14 of the 230 space groups.
Bravais lattices in 2 dimensions
In two-dimensional space, there are 5 Bravais lattices, grouped into four crystal families.
|Crystal family||5 Bravais lattices|
The unit cells are specified according to the relative lengths of the cell edges (a and b) and the angle between them (θ). The area of the unit cell can be calculated by evaluating the norm ||a × b||, where a and b are the lattice vectors. The properties of the crystal families are given below:
|Crystal family||Symmetry||Area||Axial distances (edge lengths)||Axial angle|
|Monoclinic||C2||a ≠ b||θ ≠ 90°|
|Orthorhombic||D2||a ≠ b||θ = 90°|
|Hexagonal||D6||a = b||θ = 120°|
|Tetragonal||D4||a = b||θ = 90°|
Bravais lattices in 3 dimensions
In three-dimensional space, there are 14 Bravais lattices. These are obtained by combining one of the crystal families with one of the centering types. The centering types identify the locations of the lattice points in the unit cell as follows:
- Primitive (P): lattice points on the cell corners only (sometimes called simple)
- Base-centered (A, B, or C): lattice points on the cell corners with one additional point at the center of each face of one pair of parallel faces of the cell (sometimes called end-centered)
- Body-centered (I): lattice points on the cell corners with one additional point at the center of the cell
- Face-centered (F): lattice points on the cell corners with one additional point at the center of each of the faces of the cell
- Rhombohedrally-centered (R): lattice points on the cell corners with two additional points along the longest body diagonal (only applies for the hexagonal crystal family)
Not all combinations of crystal families and centering types are needed to describe all of the possible lattices, as it can be shown that several of these are in fact equivalent to each other. For example, the monoclinic I lattice can be described by a monoclinic C lattice by different choice of crystal axes. Similarly, all A- or B-centred lattices can be described either by a C- or P-centering. This reduces the number of combinations to 14 conventional Bravais lattices, shown in the table below.
|Crystal family||Lattice system||14 Bravais lattices|
The unit cells are specified according to the relative lengths of the cell edges (a, b, c) and the angles between them (α, β, γ). The volume of the unit cell can be calculated by evaluating the triple product a · (b × c), where a, b, and c are the lattice vectors. The properties of the crystal families are given below:
|Crystal family||Lattice system||Symmetry||Volume||Axial distances (edge lengths)||Axial angles||Corresponding examples|
|Triclinic||Ci||(All remaining cases)||K2Cr2O7, CuSO4·5H2O, H3BO3|
|Monoclinic||C2h||a ≠ c||α = γ = 90°, β ≠ 90°||Monoclinic sulphur, Na2SO4·10H2O|
|Orthorhombic||D2h||a ≠ b ≠ c||α = β = γ = 90°||Rhombic sulphur, KNO3, BaSO4|
|Tetragonal||D4h||a = b ≠ c||α = β = γ = 90°||White tin, SnO2, TiO2, CaSO4|
|a = b = c
|α = β = γ ≠ 90°
|Calcite (CaCO3), cinnabar (HgS)|
|Hexagonal||D6h||a = b||α = β = 90°, γ = 120°||Graphite, ZnO, CdS|
|Cubic||Oh||a = b = c||α = β = γ = 90°||NaCl, zinc blende, copper metal|
Bravais lattices in 4 dimensions
- Aroyo, Mois I.; Müller, Ulrich; Wondratschek, Hans (2006). "Historical Introduction". International Tables for Crystallography. Springer. A1 (1.1): 2–5. doi:10.1107/97809553602060000537. Archived from the original on 2013-07-04. Retrieved 2008-04-21.
- Kittel, Charles (1996) . "Chapter 1". Introduction to Solid State Physics (Seventh ed.). New York: John Wiley & Sons. p. 10. ISBN 0-471-11181-3. Retrieved 2008-04-21.
- Based on the list of conventional cells found in Hahn (2002), p. 744
- Hahn (2002), p. 758
- Brown, Harold; Bülow, Rolf; Neubüser, Joachim; Wondratschek, Hans; Zassenhaus, Hans (1978), Crystallographic groups of four-dimensional space, New York: Wiley-Interscience [John Wiley & Sons], ISBN 978-0-471-03095-9, MR 0484179
- Bravais, A. (1850). "Mémoire sur les systèmes formés par les points distribués régulièrement sur un plan ou dans l'espace" [Memoir on the systems formed by points regularly distributed on a plane or in space]. J. Ecole Polytech. 19: 1–128. (English: Memoir 1, Crystallographic Society of America, 1949.)
- Hahn, Theo, ed. (2002). International Tables for Crystallography, Volume A: Space Group Symmetry. A (5th ed.). Berlin, New York: Springer-Verlag. ISBN 978-0-7923-6590-7. doi:10.1107/97809553602060000100.