Editing Miller index (section)

==Case of cubic structures==
For the special case of simple cubic crystals, the lattice vectors are orthogonal and of equal length (usually denoted ''a''), as are those of the reciprocal lattice. Thus, in this common case, the Miller indices (''hkℓ'') and [''hkℓ''] both simply denote normals/directions in [[Cartesian coordinates]].

For cubic crystals with [[lattice constant]] ''a'', the spacing ''d'' between adjacent (''hkℓ'') lattice planes is (from above)
: <math>d_{hk \ell}= \frac {a} { \sqrt{h^2 + k^2 + \ell ^2} }</math>.

Because of the symmetry of cubic crystals, it is possible to change the place and sign of the integers and have equivalent directions and planes:
*Indices in ''angle brackets'' such as ⟨100⟩ denote a ''family'' of directions which are equivalent due to symmetry operations, such as [100], [010], [001] or the negative of any of those directions.
*Indices 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.

For [[face-centered cubic]] and [[body-centered cubic]] lattices, the primitive lattice vectors are not orthogonal. However, in these cases the Miller indices are conventionally defined relative to the lattice vectors of the cubic [[supercell (crystal)|supercell]] and hence are again simply the Cartesian directions.