Crystallographic point group

Classification system for crystals From Wikipedia, the free encyclopedia

In crystallography, a crystallographic point group is a three dimensional point group whose symmetry operations are compatible with a three dimensional crystallographic lattice. According to the crystallographic restriction it may only contain one-, two-, three-, four- and sixfold rotations or rotoinversions. This reduces the number of crystallographic point groups to 32 (from an infinity of general point groups). These 32 groups are one-and-the-same as the 32 types of morphological (external) crystalline symmetries derived in 1830 by Johann Friedrich Christian Hessel from a consideration of observed crystal forms. In 1867 Axel Gadolin, who was unaware of the previous work of Hessel, found the crystallographic point groups independently using stereographic projection to represent the symmetry elements of the 32 groups.[1]:379

In the classification of crystals, to each space group is associated a crystallographic point group by "forgetting" the translational components of the symmetry operations. That is, by turning screw rotations into rotations, glide reflections into reflections and moving all symmetry elements into the origin. Each crystallographic point group defines the (geometric) crystal class of the crystal.

The point group of a crystal determines, among other things, the directional variation of physical properties that arise from its structure, including optical properties such as birefringency, or electro-optical features such as the Pockels effect.

Notation

Summarize
Perspective

The point groups are named according to their component symmetries. There are several standard notations used by crystallographers, mineralogists, and physicists.

For the correspondence of the two systems below, see crystal system.

Schoenflies notation

In Schoenflies notation, point groups are denoted by a letter symbol with a subscript. The symbols used in crystallography mean the following:

  • Cn (for cyclic) indicates that the group has an n-fold rotation axis. Cnh is Cn with the addition of a mirror (reflection) plane perpendicular to the axis of rotation. Cnv is Cn with the addition of n mirror planes parallel to the axis of rotation.
  • S2n (for Spiegel, German for mirror) denotes a group with only a 2n-fold rotation-reflection axis.
  • Dn (for dihedral, or two-sided) indicates that the group has an n-fold rotation axis plus n twofold axes perpendicular to that axis. Dnh has, in addition, a mirror plane perpendicular to the n-fold axis. Dnd has, in addition to the elements of Dn, mirror planes parallel to the n-fold axis.
  • The letter T (for tetrahedron) indicates that the group has the symmetry of a tetrahedron. Td includes improper rotation operations, T excludes improper rotation operations, and Th is T with the addition of an inversion.
  • The letter O (for octahedron) indicates that the group has the symmetry of an octahedron, with (Oh) or without (O) improper operations (those that change handedness).

Due to the crystallographic restriction theorem, n = 1, 2, 3, 4, or 6 in 2- or 3-dimensional space.

More information n ...
n 1 2 3 4 6
Cn C1 C2 C3 C4 C6
Cnv C1v=C1h C2v C3v C4v C6v
Cnh C1h C2h C3h C4h C6h
Dn D1=C2 D2 D3 D4 D6
Dnh D1h=C2v D2h D3h D4h D6h
Dnd D1d=C2h D2d D3d D4d D6d
S2n S2 S4 S6 S8 S12
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D4d and D6d are actually forbidden because they contain improper rotations with n=8 and 12 respectively. The 27 point groups in the table plus T, Td, Th, O and Oh constitute 32 crystallographic point groups.

Hermann–Mauguin notation

An abbreviated form of the Hermann–Mauguin notation commonly used for space groups also serves to describe crystallographic point groups. Group names are

More information Crystal family, Crystal system ...
Crystal family Crystal system Group names
Cubic 23m343243mm3m
Hexagonal Hexagonal 666m6226mm6m26/mmm
Trigonal 33323m3m
Tetragonal 444m4224mm42m4/mmm
Orthorhombic 222mm2mmm
Monoclinic 22mm
Triclinic 11
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The correspondence between different notations

More information , ...
Crystal family Crystal system Hermann-Mauguin Shubnikov[2] Schoenflies Orbifold Coxeter Order
(full) (short)
Triclinic 11C111[ ]+1
11Ci = S2×[2+,2+]2
Monoclinic 22C222[2]+2
mmCs = C1h*[ ]2
2/mC2h2*[2,2+]4
Orthorhombic 222222D2 = V222[2,2]+4
mm2mm2C2v*22[2]4
mmmD2h = Vh*222[2,2]8
Tetragonal 44C444[4]+4
44 S4[2+,4+]4
4/mC4h4*[2,4+]8
422422D4422[4,2]+8
4mm4mmC4v*44[4]8
42m42mD2d = Vd2*2[2+,4]8
4/mmmD4h*422[4,2]16
Hexagonal Trigonal 33C333[3]+3
33C3i = S6[2+,6+]6
3232D3322[3,2]+6
3m3mC3v*33[3]6
33mD3d2*3[2+,6]12
Hexagonal 66C666[6]+6
66C3h3*[2,3+]6
6/mC6h6*[2,6+]12
622622D6622[6,2]+12
6mm6mmC6v*66[6]12
6m26m2D3h*322[3,2]12
6/mmmD6h*622[6,2]24
Cubic 2323T332[3,3]+12
3m3Th3*2[3+,4]24
432432O432[4,3]+24
43m43mTd*332[3,3]24
3m3mOh*432[4,3]48
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Isomorphisms

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Perspective

Many of the crystallographic point groups share the same internal structure. For example, the point groups 1, 2, and m contain different geometric symmetry operations, (inversion, rotation, and reflection, respectively) but all share the structure of the cyclic group C2. All isomorphic groups are of the same order, but not all groups of the same order are isomorphic. The point groups which are isomorphic are shown in the following table:[3]

More information , ...
Hermann-Mauguin Schoenflies Order Abstract group
1C11C1
1Ci = S22C2
2C22
mCs = C1h2
3C33C3
4C44C4
4S44
2/m C2h4D2 = C2 × C2
 222D2 = V4
mm2C2v 4
3C3i = S66C6
6C66
6C3h6
32D36D3
3mC3v6
mmmD2h = Vh8D2 × C2
 4/mC4h8C4 × C2
422D48D4
4mmC4v8
42mD2d = Vd8
6/mC6h12C6 × C2
23T12A4
3mD3d12D6
622D612
6mmC6v12
6m2D3h12
4/mmmD4h16D4 × C2
6/mmmD6h24D6 × C2
m3Th24A4 × C2
432O  24S4
43mTd24
m3mOh48S4 × C2
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This table makes use of cyclic groups (C1, C2, C3, C4, C6), dihedral groups (D2, D3, D4, D6), one of the alternating groups (A4), and one of the symmetric groups (S4). Here the symbol " × " indicates a direct product.

Deriving the crystallographic point group (crystal class) from the space group

  1. Leave out the Bravais lattice type.
  2. Convert all symmetry elements with translational components into their respective symmetry elements without translation symmetry. (Glide planes are converted into simple mirror planes; screw axes are converted into simple axes of rotation.)
  3. Axes of rotation, rotoinversion axes, and mirror planes remain unchanged.

See also

References

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