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In geometry and crystallography, a Bravais lattice, named after Auguste Bravais (1850), is an infinite array of discrete points generated by a set of discrete translation operations described in three dimensional space by:
where ni are any integers and ai are primitive vectors which lie in different directions (not necessarily mutually perpendicular) 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, or motif) 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.
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.
|Crystal family||Point group
|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||Area||Axial distances (edge lengths)||Axial angle|
|Monoclinic||a ≠ b||θ ≠ 90°|
|Orthorhombic||a ≠ b||θ = 90°|
|Hexagonal||a = b||θ = 120°|
|Tetragonal||a = b||θ = 90°|
In three-dimensional space, there are 14 Bravais lattices. These are obtained by combining one of the seven lattice systems with one of the centering types. The centering types identify the locations of the lattice points in the unit cell as follows:
Not all combinations of lattice systems 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||Schönflies||14 Bravais Lattices|
|Primitive (P)||Base-centered (C)||Body-centered (I)||Face-centered (F)|
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 lattice systems are given below:
|Crystal family||Lattice system||Volume||Axial distances (edge lengths)||Axial angles||Corresponding examples|
|Triclinic||(All remaining cases)||K2Cr2O7, CuSO4·5H2O, H3BO3|
|Monoclinic||a ≠ c||α = γ = 90°, β ≠ 90°||Monoclinic sulphur, Na2SO4·10H2O, PbCrO3|
|Orthorhombic||a ≠ b ≠ c||α = β = γ = 90°||Rhombic sulphur, KNO3, BaSO4|
|Tetragonal||a = b ≠ c||α = β = γ = 90°||White tin, SnO2, TiO2, CaSO4|
|Hexagonal||Rhombohedral||a = b = c||α = β = γ ≠ 90°||Calcite (CaCO3), cinnabar (HgS)|
|Hexagonal||a = b||α = β = 90°, γ = 120°||Graphite, ZnO, CdS|
|Cubic||a = b = c||α = β = γ = 90°||NaCl, zinc blende, copper metal, KCl, Diamond, Silver|