The reciprocal lattice, first constructed by P. Ewald, involves a set of points, each of which represents a set of planes in space, 1/d from the origin. The value of d is the spacing between a set of planes in a unit cell. This lattice is useful to better visualize a diffraction pattern and its geometric relationship to the unit cell of the crystal under study. The relationship is obtained from the modified Bragg equation (1/dhkl = 2sinθ/λ), which is the condition where a possible X-ray reflection can occur. Thus, the point located at 1/d represents the cross-section of the pole of this set of planes, hkl, and corresponds to a possible X-ray reflection from the crystal. The unit cell as determined by the reciprocal lattice (referred to as the “reciprocal unit cell”), by construction, is defined in relation to the unit cell of the atomic structure (referred to as a the “direct cell” or “real cell”) of the crystal under study: a* is perpendicular to the plane containing b and c, b* is perpendicular to the plane containing a and c, and c* is perpendicular to the plane containing a and b, where the * (referred to as “star”, as in “a star”, “b star”, etc.) indicates a reciprocal lattice measurement.
Cf., crystallographic axis, Bragg’s law