are the building blocks of crystalline solids, defining how atoms arrange in 3D space. These infinite arrays of points form 14 distinct types, classified into 7 crystal systems based on symmetry and .
Understanding Bravais lattices is crucial for grasping crystal structures and their properties. They provide a framework for describing atomic arrangements, interpreting X-ray diffraction patterns, and analyzing electronic and vibrational properties of materials.
Definition of Bravais lattices
Bravais lattices are infinite arrays of discrete points that appear exactly the same from every point in the array
They form the basis for describing the atomic structure of crystalline solids in three dimensions
The points in a Bravais lattice represent the locations of atoms, ions, or molecules in a crystal
14 types of Bravais lattices
7 crystal systems
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The 14 Bravais lattices are classified into 7 crystal systems based on their symmetry: triclinic, monoclinic, orthorhombic, tetragonal, cubic, trigonal, and hexagonal
Each crystal system is defined by the relationships between the lattice parameters (lengths and angles) and the presence of certain symmetry elements (rotation axes, mirror planes, etc.)
The crystal systems impose constraints on the possible Bravais lattices that can occur within them
Lattice centering
Bravais lattices can have different types of lattice centering: primitive (P), body-centered (I), face-centered (F), and base-centered (A, B, or C)
Primitive lattices have lattice points only at the corners of the , while non-primitive lattices have additional lattice points at the center of the unit cell or on the faces
The type of lattice centering affects the number of atoms per unit cell and the atomic packing density
Properties of Bravais lattices
Lattice parameters
Lattice parameters are the lengths (a, b, c) and angles (α, β, γ) that define the size and shape of the unit cell in a Bravais lattice
The relationships between the lattice parameters determine the crystal system and the symmetry of the lattice
Lattice parameters can be measured experimentally using techniques such as X-ray diffraction or neutron scattering
Symmetry operations
Bravais lattices possess various symmetry operations that leave the lattice unchanged, such as translations, rotations, reflections, and inversions
The set of symmetry operations that a Bravais lattice possesses determines its point group and
Symmetry operations are important for understanding the physical properties of crystals, such as electronic band structure and phonon modes
Primitive vs non-primitive cells
Wigner-Seitz cell
The is a primitive unit cell that contains only one lattice point and is constructed by drawing perpendicular bisector planes between a chosen lattice point and its nearest neighbors
It represents the smallest repeating unit of the Bravais lattice and has the same symmetry as the lattice
The Wigner-Seitz cell is useful for visualizing the atomic arrangement and calculating properties such as the atomic packing factor
Bravais lattices in reciprocal space
Reciprocal lattice vectors
The is a Fourier transform of the real-space Bravais lattice and represents the wavevectors of plane waves that have the same periodicity as the lattice
Reciprocal lattice vectors (a*, b*, c*) are defined as the vectors perpendicular to the planes of the real-space lattice and have magnitudes inversely proportional to the interplanar spacings
The reciprocal lattice is important for understanding diffraction patterns and electronic band structures in crystalline solids
Importance in crystallography
Relationship to crystal structure
Bravais lattices provide a mathematical framework for describing the periodic arrangement of atoms in crystalline solids
The crystal structure of a material can be described as a Bravais lattice with a basis, which is the arrangement of atoms associated with each lattice point
Understanding the Bravais lattice and crystal structure is essential for predicting and explaining the physical properties of materials
X-ray diffraction patterns
X-ray diffraction is a powerful technique for determining the Bravais lattice and crystal structure of a material
The diffraction pattern is a Fourier transform of the electron density in the crystal and consists of a series of peaks that correspond to the reciprocal lattice points
The positions and intensities of the diffraction peaks provide information about the lattice parameters, symmetry, and atomic positions in the crystal
Bravais lattices vs space groups
Additional symmetry elements
Space groups are a more complete description of the symmetry of a crystal than Bravais lattices alone
In addition to the of the Bravais lattice, space groups include elements such as rotations, reflections, and screw axes
There are 230 unique space groups in three dimensions, which are determined by the combination of the Bravais lattice and the additional symmetry elements
Examples of Bravais lattices
Cubic lattices
There are three types of cubic Bravais lattices: simple cubic (SC), body-centered cubic (BCC), and face-centered cubic (FCC)
SC lattices have atoms only at the corners of the cube, BCC lattices have an additional atom at the center of the cube, and FCC lattices have additional atoms at the center of each face
Examples of materials with cubic Bravais lattices include copper (FCC), iron (BCC), and polonium (SC)
Hexagonal lattices
The hexagonal Bravais lattice is characterized by two equal lattice parameters (a = b) and one unique lattice parameter (c), with angles of 90°, 90°, and 120°
It has a six-fold rotational symmetry axis along the c-direction and additional mirror planes and two-fold rotation axes
Examples of materials with hexagonal Bravais lattices include graphite, zinc, and magnesium
Brillouin zones of Bravais lattices
First Brillouin zone
The first is the Wigner-Seitz cell of the reciprocal lattice and represents the smallest repeating unit in reciprocal space
It is constructed by drawing perpendicular bisector planes between the origin and the nearest reciprocal lattice points
The first Brillouin zone is important for understanding electronic band structures and phonon dispersion relations in crystalline solids
Higher-order Brillouin zones
Higher-order Brillouin zones are constructed by extending the perpendicular bisector planes beyond the first Brillouin zone
They represent regions in reciprocal space that are further away from the origin and have higher wavevectors
Higher-order Brillouin zones are important for understanding complex band structures and phenomena such as Fermi surface nesting
Applications of Bravais lattices
Electronic band structure
The electronic band structure of a crystalline solid describes the allowed energy states of electrons as a function of their wavevector in reciprocal space
The symmetry and periodicity of the Bravais lattice determine the shape and connectivity of the electronic bands
Understanding the electronic band structure is essential for predicting properties such as electrical conductivity, optical absorption, and magnetism
Phonon dispersion relations
Phonons are quantized lattice vibrations in a crystalline solid and can be described as waves propagating through the Bravais lattice
The phonon dispersion relations represent the frequencies of the phonon modes as a function of their wavevector in reciprocal space
The symmetry and periodicity of the Bravais lattice determine the number and degeneracy of the phonon modes and their dispersion relations
Phonon dispersion relations are important for understanding thermal properties such as heat capacity and thermal conductivity