Miller index

See Miller index for a full treatment of this topic.

Orientation is defined by the Miller index with 100 or 111 faces being the most common for silicon.

The Miller indices for a plane are integers with no common factors.

Each point is labelled with its Miller index.

Then, the poles of the other planes are placed on the figure, with the Miller indices for each pole.

Effective mass, being generally dependent on direction (with respect to the Miller index), is a tensor.

These are given in miller indices for simplification purposes.

Each peak represents a certain lattice plane and can therefore be characterized by a Miller index.

The surface coordination number is dependent on the Miller indices of the surface.

I know my Miller indices, I'm also a geologist.

Ordinarily, Miller indices are always integers by definition, and this constraint is physically significant.

This causes continuous sheets to form parallel to its miller index [-101] faces.

Reflexions are labelled by the Miller index hkl, i.e. 3 digits.

Each band can be indexed individually by the Miller indices of the diffracting plane which formed it.

Thus, integer Miller indices implicitly include indices with all rational ratios.

Online tutorial about lattice planes and Miller indices.

In particular, a family of lattice planes is determined by three integers h, k, and ℓ, the Miller indices.

Inverted, from the positions of the reflexion images the orientation of the fiber can be determined, if for the Miller index both and is valid.

Miller indices form a notation system in crystallography for planes in crystal (Bravais) lattices.

Here h, k and ℓ are identical to the Miller index, and i is a redundant index.

Since crystals are often described in terms of their Miller indices, it is useful to examine a specific structure factor in terms of these.

Vectors and atomic planes in a crystal lattice can be described by a three-value Miller index notation (ℓmn).

This construction corresponds precisely to the standard "cut-and-project" method of defining a quasicrystal, using a plane with irrational-ratio Miller indices.

A plane containing a co-ordinate axis is translated so that it no longer contains that axis before its Miller indices are determined.

The linear rate constant depends on the orientation of the crystal (usually indicated by the Miller indices of the crystal plane facing the surface).