Miller index
Miller indices are used to describe planes and directions in a crystal.
It is necessary to define a basis for the single crystal; see Primitive cell.
In case of directions, a Miller index is of the form of
- [u v w]
where the integers in the square brackets represent the coordinates of the vector in the real space.
In the case of planes, a Miller index is of the form
- (h k l)
where the integers h, k, and l represent the x-, y-, and z-intercepts of the plane respectively:
- if P, Q and R are the coordinates of the intercept of the plane (the closest to the origin) with the axes, then
- h = 1/P
- k = 1/Q
- l = 1/R
In Miller indices, a bar above one of the numbers indicates a negative value.
The crystallographic planes and directions
The crystallographic directions are fictitious lines linking nodes (atoms, ions or molecules) of a crystal. The crystallographic planes are fictitious planes linking nodes. Some directions and planes have a higher density of nodes; these dense planes have an influence on the behaviour of the crystal:
- optical properties: in condensed matter, the light "jumps" from one atom to the other with the Rayleigh scattering; the velocity of light thus varies according to the directions, whether the atoms are close or far; this gives the birefringence
- adsorption and reactivity: the adsorption and the chemical reactions occur on atoms or molecules, these phenomena are thus sensitive to the density of nodes;
- surface tension: the condensation of a material means that the atoms, ions or molecules are more stable if they are surrounded by other similar species; the surface tension of an interface thus varies according to the density on the surface
- the pores and crystallites tend to have straight grain boundaries following dense planes
- cleavage
- dislocations (plastic deformation)
- the dislocation core tends to spread on dense planes (the elastic perturbation is "diluted"); this reduces the friction (Peierls-Nabarro force), the sliding occurs more frequently on dense planes;
- the perturbation carried by the dislocation (Burgers vector) is along a dense direction: the shift of one node in a dense direction is a lesser distortion;
- the dislocation line tends to follow a dense direction, the dislocation line is often a straight line, a dislocation loop is often a polygon.
For all these reasons, it is important to determine the planes and thus to have a notation system.
Case of the cubic structures
In case of the cubic structures, the Miller index of a plane, in parentheses such as (100), are also the coordinates of the direction of a plane normal. It stands for a vector perpendicular to the family of planes, with a length of d-1, where d is the inter-plane spacing.
Due to the symmetries of cubic crystals, it is possible to change the place and sign of the integers and have equivalent directions and planes:
- Coordinates in angle brackets or chevrons such as <100> denote a family of directions which are equivalent due to symmetry operations. If it refers to a cubic system, this example could mean [100], [010], [001] or the negative of any of those directions.
- Coordinates in curly brackets or braces such as {100} denote a family of plane normals which are equivalent due to symmetry operations, much the way angle brackets denote a family of directions.
Case of the hexagonal and rhombohedral structures
With hexagonal and rhombohedral crystal systems, it is possible to use the Bravais-Miller index which has 4 numbers (h k i l)
- i = -h-k
where h, k and l are identical to the Miller index.
The (100) plane has a 3-fold symmetry, it remains unchanged by a rotation of 1/3 (2π/3 rad, 120°). The [100], [010] and the directions are really similar. If S is the intercept of the plane with the axis, then
- i = 1/S
i is redundant and not necessary.
See also
External links
- http://www.ece.byu.edu/cleanroom/EW_orientation.phtml - Miller index description with diagrams