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

International Tables for Crystallography (2006). Vol. A, ch. 2.1, p. 14

Section 2.1.2. Space-group classification

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

2.1.2. Space-group classification

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In this volume, the plane groups and space groups are classified according to three criteria:

  • (i) According to geometric crystal classes, i.e. according to the crystallographic point group to which a particular space group belongs. There are 10 crystal classes in two dimensions and 32 in three dimensions. They are described and listed in Part 10[link] and in column 4 of Table 2.1.2.1[link]. [For arithmetic crystal classes, see Section 8.2.3[link] in this volume and Chapter 1.4[link] of International Tables for Crystallography, Vol. C (2004)[link].]

    Table 2.1.2.1| top | pdf |
    Crystal families, crystal systems, conventional coordinate systems and Bravais lattices in one, two and three dimensions

    Crystal familySymbolCrystal systemCrystallographic point groupsNo. of space groupsConventional coordinate systemBravais lattices
    Restrictions on cell parametersParameters to be determined
    One dimension
    [Scheme scheme1] 2 None a [{\scr p}]
    Two dimensions
    [\matrix{\hbox{Oblique}\hfill\cr \quad\hbox{(monoclinic)}\hfill\cr}] m Oblique [Scheme scheme2] 2 None [\matrix{a, b\hfill\cr \gamma\hfill\cr}] § mp
    [\matrix{\hbox{Rectangular}\hfill\cr \quad\hbox{(orthorhombic)}\hfill\cr}] o Rectangular [Scheme scheme3] 7 [\gamma = 90^{\circ}] a, b [\matrix{op\hfill\cr oc\hfill\cr}]
    [\matrix{\hbox{Square}\hfill\cr \quad\hbox{(tetragonal)}\cr}] t Square [Scheme scheme4] 3 [\matrix{a = b\hfill\cr \gamma = 90^{\circ}\hfill\cr}] a tp
    Hexagonal h Hexagonal [Scheme scheme5] 5 [\matrix{a = b\hfill\cr \gamma = 120^{\circ}\hfill\cr}] a hp
    Three dimensions
    [\matrix{\hbox{Triclinic}\hfill\cr \quad\hbox{(anorthic)}\cr}] a Triclinic [Scheme scheme6] 2 None [\matrix{a,b,c,\hfill\cr \alpha, \beta, \gamma\hfill\cr}] aP
    Monoclinic m Monoclinic [Scheme scheme7] 13 [\matrix{b\hbox{-unique setting}\hfill\cr \alpha = \gamma = 90^{\circ}\hfill\cr}] [\matrix{a,b,c \cr \beta\hfill\cr}] § [\!\matrix{mP\hfill\cr mS\; (mC, mA, mI)}]
    [\matrix{c\hbox{-unique setting}\hfill\cr \alpha = \beta = 90^{\circ}\hfill\cr}] [\matrix{a, b, c,\hfill\cr \gamma\hfill\cr}] § [\!\matrix{mP\hfill\cr mS\; (mA, mB, mI)\hfill\cr}]
    Orthorhombic o Orthorhombic [Scheme scheme8] 59 [\alpha = \beta = \gamma = 90^{\circ}] a, b, c oP
    oS (oC, oA, oB)
    oI
    oF
    Tetragonal t Tetragonal [Scheme scheme9] 68 [\matrix{a = b\hfill\cr\alpha = \beta = \gamma = 90^{\circ}\hfill\cr}] a, c [\matrix{tP\hfill\cr tI\hfill\cr}]
    Hexagonal h Trigonal [Scheme scheme10] 18 [\matrix{a = b\hfill\cr\alpha = \beta = 90^{\circ},\ \gamma = 120^{\circ}\hfill}] a, c hP
    7 [\matrix{a = b = c\hfill\cr \alpha = \beta = \gamma\hfill\cr \quad(\hbox{rhombohedral axes,}\hfill\cr \quad\hbox{primitive cell})\hfill\cr\cr a = b\hfill\cr \alpha = \beta = 90^{\circ}, \gamma = 120^{\circ}\hfill\cr \quad(\hbox{hexagonal axes,}\hfill\cr \quad\hbox{triple obverse cell})\hfill\cr}] a, α hR
    Hexagonal [Scheme scheme11] 27 [\matrix{a = b\hfill\cr \alpha = \beta = 90^{\circ}, \gamma = 120^{\circ}\hfill\cr}] a, c hP
    Cubic c Cubic [Scheme scheme12] 36 [\matrix{a = b = c\hfill\cr \alpha = \beta = \gamma = 90^{\circ}\hfill\cr}] a [\matrix{cP\hfill\cr cI\hfill\cr cF\hfill\cr}]
    The symbols for crystal families (column 2) and Bravais lattices (column 8) were adopted by the International Union of Crystallography in 1985; cf. de Wolff et al. (1985).
    Symbols surrounded by dashed or full lines indicate Laue groups; full lines indicate Laue groups which are also lattice point symmetries (holohedries).
    §These angles are conventionally taken to be non-acute, i.e. [\geq 90^{\circ}].
  • (ii) According to crystal families. The term crystal family designates the classification of the 17 plane groups into four categories and of the 230 space groups into six categories, as displayed in column 1 of Table 2.1.2.1[link]. Here all `hexagonal', `trigonal' and `rhombohedral' space groups are contained in one family, the hexagonal crystal family. The `crystal family' thus corresponds to the term `crystal system', as used frequently in the American and Russian literature.

    The crystal families are symbolized by the lower-case letters a, m, o, t, h, c, as listed in column 2 of Table 2.1.2.1[link]. If these letters are combined with the appropriate capital letters for the lattice-centring types (cf. Chapter 1.2[link] ), symbols for the 14 Bravais lattices result. These symbols and their occurrence in the crystal families are shown in column 8 of Table 2.1.2.1[link]; mS and oS are the standard setting-independent symbols for the centred monoclinic and the one-face centred orthorhombic Bravais lattices, cf. de Wolff et al. (1985)[link]; symbols between parentheses represent alternative settings of these Bravais lattices.

  • (iii) According to crystal systems. This classification collects the plane groups into four categories and the space groups into seven categories. The classifications according to crystal families and crystal systems are the same for two dimensions.

For three dimensions, this applies to the triclinic, monoclinic, orthorhombic, tetragonal and cubic systems. The only complication exists in the hexagonal crystal family for which several subdivisions into systems have been proposed in the literature. In this volume, as well as in IT (1952)[link], the space groups of the hexagonal crystal family are grouped into two `crystal systems' as follows: all space groups belonging to the five crystal classes 3, [\bar{3}], 32, 3m and [\bar{3}m], i.e. having 3, [3_{1}], [3_{2}] or [\bar{3}] as principal axis, form the trigonal crystal system, irrespective of whether the Bravais lattice is hP or hR; all space groups belonging to the seven crystal classes 6, [\bar{6}, 6/m], 622, 6mm, [\bar{6}]2m and [6/mmm], i.e. having 6, [6_{1}], [6_{2}], [6_{3}], [6_{4}], [6_{5}] or [\bar{6}] as principal axis, form the hexagonal crystal system; here the lattice is always hP (cf. Section 8.2.8[link] ). The crystal systems, as defined above, are listed in column 3 of Table 2.1.2.1[link].

A different subdivision of the hexagonal crystal family is in use, mainly in the French literature. It consists of grouping all space groups based on the hexagonal Bravais lattice hP (lattice point symmetry [6/mmm]) into the `hexagonal' system and all space groups based on the rhombohedral Bravais lattice hR (lattice point symmetry [\bar{3}m]) into the `rhombohedral' system. In Section 8.2.8[link] , these systems are called `Lattice systems'. They were called `Bravais systems' in earlier editions of this volume.

The theoretical background for the classification of space groups is provided in Chapter 8.2[link] .

References

International Tables for Crystallography (2004). Vol. C, 3rd ed., edited by A. J. C. Wilson & E. Prince. Dordrecht: Kluwer Academic Publishers.
International Tables for X-ray 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).]
Wolff, P. M. de, Belov, N. V., Bertaut, E. F., Buerger, M. J., Donnay, J. D. H., Fischer, W., Hahn, Th., Koptsik, V. A., Mackay, A. L., Wondratschek, H., Wilson, A. J. C. & Abrahams, S. C. (1985). Nomenclature for crystal families, Bravais-lattice types and arithmetic classes. Report of the International Union of Crystallography Ad-hoc Committee on the Nomenclature of Symmetry. Acta Cryst. A41, 278–280.








































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