International
Tables for
Crystallography
Volume A
Space-group symmetry
Edited by Th. Hahn

International Tables for Crystallography (2006). Vol. A, ch. 2.2, pp. 26-27

Section 2.2.9. Symmetry operations

Th. Hahna* and A. Looijenga-Vosb

aInstitut für Kristallographie, Rheinisch-Westfälische Technische Hochschule, Aachen, Germany, and bLaboratorium voor Chemische Fysica, Rijksuniversiteit Groningen, The Netherlands
Correspondence e-mail:  hahn@xtl.rwth-aachen.de

2.2.9. Symmetry operations

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As explained in Sections 8.1.6[link] and 11.1.1[link] , the coordinate triplets of the General position of a space group may be interpreted as a shorthand description of the symmetry operations in matrix notation. The geometric description of the symmetry operations is found in the space-group tables under the heading Symmetry operations.

2.2.9.1. Numbering scheme

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The numbering [(1) \ldots (\;p) \ldots] of the entries in the blocks Symmetry operations and General position (first block below Positions) is the same. Each listed coordinate triplet of the general position is preceded by a number between parentheses (p). The same number (p) precedes the corresponding symmetry operation. For space groups with primitive cells, both lists contain the same number of entries.

For space groups with centred cells, to the one block General position several (2, 3 or 4) blocks Symmetry operations correspond. The numbering scheme of the general position is applied to each one of these blocks. The number of blocks equals the multiplicity of the centred cell, i.e. the number of centring translations below the subheading Coordinates, such as [(0,0,0)\! +, ({2 \over 3}, {1 \over 3}, {1 \over 3})\! +, ({1 \over 3}, {2 \over 3}, {2 \over 3}) +].

Whereas for the Positions the reader is expected to add these centring translations to each printed coordinate triplet himself (in order to obtain the complete general position), for the Symmetry operations the corresponding data are listed explicitly. The different blocks have the subheadings `For (0,0,0)[+] set', `For [({1 \over 2},{1 \over 2},{1 \over 2}) +] set', etc. Thus, an obvious one-to-one correspondence exists between the analytical description of a symmetry operation in the form of its general-position coordinate triplet and the geometrical description under Symmetry operations. Note that the coordinates are reduced modulo 1, where applicable, as shown in the example below.

Example: Ibca (73)

The centring translation is [t({1 \over 2},{1 \over 2},{1 \over 2})]. Accordingly, above the general position one finds [({0}, {0}, {0})+] and [({1 \over 2},{1 \over 2},{1 \over 2}) +]. In the block Symmetry operations, under the subheading `For [(0, 0, 0)+] set', entry (2) refers to the coordinate triplet [\bar{x} + {1 \over 2},\;\bar{y},\;z + {1 \over 2}]. Under the subheading `For [({1 \over 2},{1 \over 2},{1 \over 2}) +] set', however, entry (2) refers to [\bar{x},\;\bar{y} + {1 \over 2},\;z]. The triplet [\bar{x},\;\bar{y} + {1 \over 2},\;z] is selected rather than [\bar{x} + 1,\; \bar{y} + {1 \over 2},\;z + 1], because the coordinates are reduced modulo 1.

In space groups with two origins where a `symmetry element' and an `additional symmetry element' are of different type (e.g. mirror versus glide plane, rotation versus screw axis, Tables 4.1.2.2[link] and 4.1.2.3[link] ), the origin shift may interchange the two different types in the same location (referred to the appropriate origin) under the same number (p). Thus, in [P4/nmm] (129), (p) = (7) represents a [\bar 2] and a 21 axis, both in [x, x, 0], whereas (p) = (16) represents a g and an m plane, both in [x, x, z].

2.2.9.2. Designation of symmetry operations

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An entry in the block Symmetry operations is characterized as follows.

  • (i) A symbol denoting the type of the symmetry operation (cf. Chapter 1.3[link] ), including its glide or screw part, if present. In most cases, the glide or screw part is given explicitly by fractional coordinates between parentheses. The sense of a rotation is indicated by the superscript [+] or −. Abbreviated notations are used for the glide reflections [a({1 \over 2},0,0) \equiv a]; [b(0,{1 \over 2},0) \equiv b]; [c(0,0,{1 \over 2}) \equiv c]. Glide reflections with complicated and unconventional glide parts are designated by the letter g, followed by the glide part between parentheses.

  • (ii) A coordinate triplet indicating the location and orientation of the symmetry element which corresponds to the symmetry operation. For rotoinversions, the location of the inversion point is given in addition.

Details of this symbolism are presented in Section 11.1.2[link] .

Examples

  • (1) [a\ \ \ x,y,{1 \over 4}]

    Glide reflection with glide component [({1 \over 2},0,0)] through the plane [x,y,{1 \over 4}], i.e. the plane parallel to (001) at [z = {1 \over 4}].

  • (2) [\bar{4}^{+}\ \ \ {1 \over 4},{1 \over 4},z\semi \ \ {1 \over 4},{1 \over 4},{1 \over 4}]

    Fourfold rotoinversion, consisting of a counter clockwise rotation by 90° around the line [{1 \over 4},{1 \over 4}, z], followed by an inversion through the point [{1 \over 4},{1 \over 4},{1 \over 4}].

  • (3) [g({1 \over 4},{1 \over 4},{1 \over 2})\ \ \ x,x,z]

    Glide reflection with glide component [({1 \over 4},{1 \over 4},{1 \over 2})] through the plane x, x, z, i.e. the plane parallel to [(1\bar{1}0)] containing the point 0, 0, 0.

  • (4) [g({1 \over 3},{1 \over 6},{1 \over 6})\ \ \ 2x - {1 \over 2}, x,z] (hexagonal axes)

    Glide reflection with glide component [({1 \over 3},{1 \over 6},{1 \over 6})] through the plane [2x-{1 \over 2}, x,z], i.e. the plane parallel to [(1\bar{2}10)], which intersects the a axis at [-{1 \over 2}] and the b axis at [{1 \over 4}]; this operation occurs in [R\bar{3}c] (167, hexagonal axes).

  • (5) Symmetry operations in Ibca (73)

    Under the subheading `For (0, 0, 0)[+] set', the operation generating the coordinate triplet (2) [\bar{x} + {1 \over 2},\bar{y},z + {1 \over 2}] from (1) x, y, z is symbolized by [2 (0,0, {1 \over 2})\ \ {1 \over 4},0,z]. This indicates a twofold screw rotation with screw part [(0,0,{1 \over 2})] for which the corresponding screw axis coincides with the line [{1 \over 4},0,z], i.e. runs parallel to [001] through the point [{1 \over 4},0,0]. Under the subheading `For [({1 \over 2},{1 \over 2},{1 \over 2}) +] set', the operation generating the coordinate triplet (2) [\bar{x},\bar{y} + {1 \over 2}, z] from (1) x, y, z is symbolized by [2\ \ 0, {1 \over 4}, z]. It is thus a twofold rotation (without screw part) around the line [0,{1 \over 4},z].








































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