Anthony R. West - Solid State Chemistry and its Applications

Figure 1.66 Tetragonal space group I41 (No 80); coordinates of equivalent positions 8(b):

Special positions with point symmetry 2, 4(a): 0, 0, z; 0, ½, + z; ½, ½, ½ + z; ½, 0, + z.

The purpose of this section is to show the fundamental importance of space groups to crystal structures and how the atomic coordinates of a structure are related to the space group. As examples, two simple but important structures, which have already been described earlier in this chapter, are considered in some detail.

The basic information that we need to know is the following:

Unit cell: cubic, a = 3.905 Å

Space group: Pm3m(number 221)

Atomic coordinates: Ti in 1(a) at 0, 0, 0; Sr in 1(b) at ½, ½, ½; O in 3(d) at 0, 0, ½

This is, in fact, a very simple example since although the space group Рm 3 m is complicated, as are all cubic space groups, all the atoms in perovskite lie on special positions. There are 48 general equivalent positions in this space group, but a large number of special positions arise when atoms lie on symmetry elements. Ti occupies a 1‐fold special position at the origin of the unit cell; the symbol 1(a) indicates that there is only one position in this set and (a) the Wyckoff label, for this (set of) position(s). Sr also occupies a 1‐fold special position, 1(b), at the body centre of the cell. Oxygen occupies a 3‐fold special position 3(d); the coordinates of one of these positions, 0, 0, ½ are given and the only remaining information that is needed from the space group are the coordinates of the other two oxygen positions. From International Tables, these are 0, ½, 0 and ½, 0, 0.

From this information, the unit cell and atomic positions may be drawn, first as a projection down one of the cubic cell axes, Fig. 1.41(a) and then as an oblique projection to show the atomic positions more clearly, Fig. 1.41(c). [Note: Fig. 1.41(b) shows an alternative unit cell with Sr at the origin, as discussed in Section 1.17.7.] The coordination environment of each atom may be seen in (c) and interatomic distances calculated by simple geometry, as detailed in Section 1.17.7, together with a more extended discussion of perovskites, structural distortions in some cases and structure–property relations.

We need to know the following information:

Unit cell: tetragonal, a = 4.594, с = 2.958 Å

Space group: P 4 2 /mnm (No 136)

Atomic coordinates: Ti in 2(a) at (0, 0, 0); (½, ½, ½); О in 4(f) at ( x , x , 0); ( ); (½ + x , ½ – x , ½); (½ – x , ½ + x , ½)

As in the perovskite structure, only special positions are used to accommodate atoms and the 16‐fold general positions are unoccupied. The Ti positions are fixed at the corner and body centre but O has a variable parameter, x , whose value must be determined experimentally. Crystal structure determination and refinement gives x = 0.30 for TiO 2. The unit cell of rutile is shown projected onto the xy plane in Fig. 1.37(a) and the structure is described fully in Section 1.17.6.

The symmetry elements in space group P 4 2 /mnm are shown in Fig. 1.67; most should also be readily apparent on inspection of the structural model shown in Fig. 1.37(a and f). Thus, the 4 2axes are located halfway along the cell edges although no atoms lie on these 4 2axes. The oxygen atoms are arranged on spirals around the 4 2axes such that translation by c /2 and rotation by 90° convert one oxygen position to another. Centres of symmetry are present, for example, at the cell corners; also 2 and 2 1axes and (not shown) mirror planes and glide planes are present.

Figure 1.67 The symmetry elements in space group P42/mnm.

We see in Chapter 5how the presence of lattice centring or elements of space symmetry lead to systematically absent reflections from X‐ray (but also electron and neutron) diffraction patterns. For example, in space group C 2, the C ‐centring imposes the condition that only those reflections that satisfy the rule: for ( hkl : h + k = 2 n ) are allowed. The 2 1screw axes parallel to b impose the condition for reflection: for ( 0k0 : k = 2 n) . However, this is also a consequence of the C ‐centring condition, for the special case that h = l = 0, and so does not lead to any extra systematic absences . Information on the conditions limiting possible reflections is given for every space group in International Tables for X‐ray Crystallography . In the above case, since the 2 1screw axes do not impose an extra set of conditions, they are often written in parentheses.

The presence of glide planes in a crystal may sometimes by detected by the absence of a set of X‐ray reflections. For an a glide perpendicular to b, the condition limiting the h 0 l reflections is that h = 2 n (i.e. only even h values may be observed). In the space group C 2/ m , this condition is part of the more general condition for C ‐centring, namely: for hkl , h + k = 2 n . Independent evidence for the existence of the glide plane is therefore not immediately available from the X‐ray patterns.

Two further examples: in space group P 222 1, the only symmetry element which causes systematic absences is the 2 1axis parallel to z , i.e. for 00 l reflections, only those for which l = 2 n may be observed; there are no general conditions on hkl reflections since the space group is primitive. For space group I 4 1, two conditions are imposed on the possible reflections: for the body centring, only the reflections hkl: h + k + l = 2 n may be observed; the 4 1screw axis places the additional condition that: for 00 l reflections, l = 4 n .

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