International
Tables for Crystallography Volume A Spacegroup symmetry Edited by M. I. Aroyo © International Union of Crystallography 2016 
International Tables for Crystallography (2016). Vol. A, ch. 2.1, p. 162

The entries under Positions^{2} (more explicitly called Wyckoff positions) consist of the one General position (upper block) and the Special positions (blocks below). The columns in each block, from left to right, contain the following information for each Wyckoff position.
Detailed treatment of general and special Wyckoff positions, including definitions, theoretical background and examples, is given in Section 1.4.4 .
The two types of positions, general and special, are characterized as follows:
The set of all symmetry operations that map a point onto itself forms a group, known as the `sitesymmetry group' of that point. It is given in the third column by the `oriented sitesymmetry symbol' which is explained in Section 2.1.3.12. General positions always have site symmetry 1, whereas special positions have higher site symmetries, which can differ from one special position to another.
If in a crystal structure the centres of finite objects, such as molecules, are placed at the points of a special position, each such object must display a point symmetry that is at least as high as the site symmetry of the special position. Geometrically, this means that the centres of these objects are located on symmetry elements without translations (centre of symmetry, mirror plane, rotation axis, rotoinversion axis) or at the intersection of several symmetry elements of this kind (cf. the spacegroup diagrams).
Note that the location of an object on a screw axis or on a glide plane does not lead to an increase in the site symmetry and to a corresponding reduction of the multiplicity for that object. Accordingly, a space group that contains only symmetry elements with translation components does not have any special position. Such a space group is called `fixedpointfree' (for further discussion, see Section 1.4.4.2 ).
Example: Space group C12/c1 (15, unique axis b, cell choice 1)
The general position 8f of this space group contains eight equivalent points per cell, each with site symmetry 1. The coordinate triplets of four points, (1) to (4), are given explicitly, the coordinates of the other four points are obtained by adding the components of the Ccentring translation to the coordinate triplets (1) to (4).
The space group has five special positions with Wyckoff letters a to e. The positions 4a to 4d require inversion symmetry, , whereas Wyckoff position 4e requires twofold rotation symmetry, 2, for any object in such a position. For position 4e, for instance, the four equivalent points have the coordinates . The values of x and z are specified, whereas y may take any value. Since each point of position 4e is mapped onto itself by a twofold rotation, the multiplicity of the position is reduced from 8 to 4, whereas the order of the sitesymmetry group is increased from 1 to 2.
From the symmetryelement diagram of C2/c, the locations of the four twofold axes can be deduced as ; ; ; .
From this example, the general rule is apparent that the product of the position multiplicity and the order of the corresponding sitesymmetry group is constant for all Wyckoff positions of a given space group; it is the multiplicity of the general position.
Attention is drawn to ambiguities in the description of crystal structures in a few space groups, depending on whether the coordinate triplets of IT (1952) or of this edition are taken. This problem is analysed by Parthé et al. (1988).
References
International Tables for Xray Crystallography (1952). Vol. I, edited by N. F. M. Henry & K. Lonsdale. Birmingham: Kynoch Press. [Revised editions: 1965, 1969 and 1977. Abbreviated as IT (1952).]Parthé, E., Gelato, L. M. & Chabot, B. (1988). Structure description ambiguity depending upon which edition of International Tables for (Xray) Crystallography is used. Acta Cryst. A44, 999–1002.