International
Tables for Crystallography Volume A1 Symmetry relations between space groups Edited by Hans Wondratschek and Ulrich Müller © International Union of Crystallography 2011 
International Tables for Crystallography (2011). Vol. A1, Appendix. Differences in the presentation of Parts 2 and 3.
Appendix. Differences in the presentation of Parts 2 and 3^{a}Fachbereich Chemie, PhilippsUniversität, D35032 Marburg, Germany, and ^{b}Institut für Kristallographie, Universität, D76128 Karlsruhe, Germany The tables of Parts 2 and Part 3 of this volume address different subjects, namely symmetry in Part 2 and the implications of symmetry changes for crystal structures in Part 3. To make the tables as convenient as possible for readers interested in these two different subjects, the presentation of the subgroups differs in the two parts. What the differences are and why there are differences are summarized in this Appendix. 
The tables in Parts 2 and 3 of this volume deal with two different aspects of the reduction of crystal symmetry. In Part 2, the loss of symmetry is described for the subgroup of by listing the general position of , i.e. a set of representatives of those symmetry operations (group elements) which are retained in . If there is not enough space to include the full general position, at least a set of generators of is listed. Thus, the subject of Part 2 is symmetry. In Part 3, the splitting of the point orbits (Wyckoff positions) of the space group when the symmetry of is reduced to that of is described. For each Wyckoff position of the corresponding Wyckoff positions of are listed. Thus, in Part 3 the implications of symmetry changes for crystal structures are described.
In both Parts 2 and 3, the data are listed in a way that makes the tables as convenient to use as possible. As the subjects of Parts 2 and 3 are different, the presentation of the data in the two parts differs. In addition, the data in Part 2 are such that they can be used moreorless independently from Volume A of International Tables for Crystallography (2005) (abbreviated as IT A). This independence is not possible for the data in Part 3.
In order to facilitate the combined use of the data in the two parts, the differences in the presentation of these data are summarized in this Appendix.
In IT A, some space groups are described up to six times:
Multiple descriptions of the space group are treated differently in Parts 2 and 3 of this volume:
Multiple descriptions of the subgroup are also sometimes treated differently in the two parts:
When starting from a space group and proceeding to one of its subgroups , the symmetry operations and the point coordinates are primarily referred to the coordinate system of . This coordinate system consists of a coordinate basis of three linearly independent basis vectors and an origin. In general, the conventional coordinate system of will not be identical to that of but the transition from the coordinate system of to that of may involve a change of the basis and an origin shift. This transition or coordinate transformation is not uniquely determined but may be chosen within certain limits. The optimal choice will be the coordinate transformation that is the most convenient and easy for the user to work with.
For the following, it is assumed that the original crystal structure and its space group and symmetry operations are referred to a conventional coordinate system, because the data in the tables of this volume and in IT A are listed under this condition. Otherwise, a coordinate transformation to a conventional coordinate system has to precede the use of most of the data. The coordinate transformation itself is described by the matrix P of the coefficients of the basis vectors of the new basis referred to the old basis and by a column p which consists of the coordinates of the new origin referred to the old coordinate system, cf. Section 2.1.3 or, more explicitly, IT A, Part 5 . The matrix P is presented in Parts 2 and 3 by listing the new basis vectors as linear combinations of the old ones, e.g. . The column p is presented in Part 2 by listing the coefficients of the shift vector, e.g. 0, 1/2, 1/4. For Part 3, the representatives of the Wyckoff positions are taken as triplets of point coordinates. The transformation behaviour of coordinates is different from that of the symmetry operations, viz , where and are the coordinate columns of the points of the crystal structure in the old and in the new coordinate systems.
The criteria for selecting the coordinate transformations are different in Parts 2 and 3. In Part 2, emphasis is placed on homogeneity by using similar transformation matrices in similar situations. In Part 3, the preferred transformation is that which avoids an origin shift, i.e. for which the resulting shift vector is the o vector.
Example
In the relation the axes must be transformed, either by or by . If origin choice 1 is selected for both space groups, then the first of these transformations requires an origin shift of (referred to the coordinate system of ). The first transformation is used in Part 2 because in all such relations the new basis of is rotated against the old basis of by a clockwise rotation of 45° and the necessary origin shift is then accepted. No origin shift is needed for the second transformation and, therefore, it has been used in Part 3; this can be seen in the transformation of the coordinates:
Another difference between Parts 2 and 3 concerns the origin shifts chosen and their presentation. The common point of view is to make the origin shift positive unless special conditions lead to a preference for negative coefficients. However, the shift vector of Part 3 is calculated by from the shift vector of Part 2, so the two vectors usually have opposite directions. Therefore, very often a positive shift vector in Part 2 corresponds to a negative shift vector in Part 3 and vice versa. This is not obvious at first glance, because in Part 2 the vector is listed, whereas in Part 3 the shift vector is given as part of the coordinate transformations.
Example
Consider Pccn, No. 56, as a subgroup of Cccm, No. 66, in the block `Loss of centring translations'. The origin shift of Part 2 has the opposite direction to that of Part 3, where it is indicated as part of the transformation `'. The components of this transformation correspond to a vector , which is the opposite of the vector of Part 2.
Since the Wyckoff letters of the positions in IT A may depend not only on the chosen basis but also on the chosen origin, a difference in the origin shift may induce a difference in the relations between the Wyckoff positions.
Example
Consider , No. 84, as a translationengleiche subgroup of , No. 136. The coordinate transformation of Part 3 results in the relations and of the Wyckoff positions. The origin shift 0, 1/2, 0 of Part 2 (which corresponds to a coordinate transformation ) results in the relations and .
If the setting of a subgroup is nonconventional, in Part 2, as in IT A, a nonconventional Hermann–Mauguin symbol is listed referred to the basis of , followed by the spacegroup number and the conventional symbol in parentheses. In Part 3, nonconventional settings are given only by Hermann–Mauguin symbols that correspond to the conventions of the crystal system followed on the next line by and the symbol of the conventional setting.
In Part 3, unlike Part 2, no use is made of centred triclinic cells, F and Rcentred monoclinic cells, C and Fcentred tetragonal cells and Hcentred hexagonal cells.
The sequence of the subgroups follows the same principles in both parts. The translationengleiche subgroups are listed first, the klassengleiche subgroups follow. The subgroups are distributed into blocks; within the same block the index generally determines the sequence (lower index precedes higher index). For the same index, the spacegroup number determines the sequence (higher spacegroup number precedes lower spacegroup number). A difference in the sequence is caused by two special rules that apply to Part 3:

The sequence of the listings of the klassengleiche subgroups differs more often, because the partition of the subgroups into blocks in Part 2 is different from and finer than that in Part 3. The blocks in Part 2 are determined by the relation of the lattice of to that of , i.e. by the different kinds of cell enlargement, and the index and spacegroup numbers are decisive for the sequence within these (small) blocks only.
The isomorphic subgroups are placed differently in Parts 2 and 3. Those with index values of 2, 3 and 4 are listed in Part 2 together with the other klassengleiche subgroups; they may also be contained in the infinite series of isomorphic subgroups that follow. In Part 3, all isomorphic subgroups are listed in a separate block.
Conjugate subgroups are listed in Part 3 only in the case of orientational conjugation, cf. Section 3.1.5.2 . They are marked by the word `conjugate'. In Part 2, all conjugate subgroups of index 3 and 4 are listed individually and are joined by a left brace. In the series of maximal isomorphic subgroups, the conjugacy relations are given by statements.
References
International Tables for Crystallography (2005). Vol. A, SpaceGroup Symmetry, edited by Th. Hahn, 5th ed. Heidelberg: Springer.Google Scholar