In 1850, August Bravais established the theory of space lattices, which presents that the internal structure of a crystal is a regular, cyclical and indefinite distribution of some atoms in space. This atom network is called a crystal lattice. There are indefinite families of parallel planes in a crystal lattice. Miller Indices (usually expressed by hkl) are a symbolic vector representation for the orientation of theses crystal planes.
To determine the Miller Indices (hkl) of a plane, one must take the following steps:
In our VRML applications, the Miller Indices hkl are directly specified by the user via selectors for each of the three values. The corresponding intercepts are calculated and their values as well as the resulting plane are displayed.
110 plane (enlarge) |
020 plane (enlarge) |
Load the VRML Model for a Cubic Lattice (32K) |
The Silicon diamond lattice consists of two interleaving face-centered cubic (fcc) cells displaced by 1/4 of the lattice constant. The density of atoms in different Miller Indices planes determines properties related to etching or oxidization.
111 plane and atoms on the plane (enlarge) |
110 plane and atoms on the plane (enlarge) |
Load the VRML Model for a Silicon Lattice Cell (52K) |
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