Miller indices are a symbolic representation of an atomic plane's orientation in a crystal lattice. They are defined as the reciprocals of the fractional intercepts the plane makes with the crystallographic axes. To determine the Miller indices of a plane, the intercepts of the plane along the crystallographic axes are found and the reciprocals of the intercepts are taken. The indices are then enclosed in parentheses with any fractions cleared and reduced to lowest terms. This provides a set of numbers that uniquely identifies the plane's orientation.