# Crystallographic point group

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.$^{:379}$
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

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:
* C$_n$ (for cyclic) indicates that the group has an n-fold rotation axis. C$_{nh}$ is C$_n$ with the addition of a mirror (reflection) plane perpendicular to the axis of rotation. C$_{nv}$ is C$_n$ with the addition of n mirror planes parallel to the axis of rotation.
* S$_{2n}$ (for Spiegel, German for mirror) denotes a group with only a 2n-fold rotation-reflection axis.
* D$_n$ (for dihedral, or two-sided) indicates that the group has an n-fold rotation axis plus n twofold axes perpendicular to that axis. D$_{nh}$ has, in addition, a mirror plane perpendicular to the n-fold axis. D$_{nd}$ has, in addition to the elements of D$_n$, mirror planes parallel to the n-fold axis.
* The letter T (for tetrahedron) indicates that the group has the symmetry of a tetrahedron. T$_d$ includes improper rotation operations, T excludes improper rotation operations, and T$_h$ is T with the addition of an inversion.
* The letter O (for octahedron) indicates that the group has the symmetry of an octahedron, with (O$_h$) 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.
| n | 1 | 2 | 3 | 4 | 6 |
| C$_n$ | C$_1$ | C$_2$ | C$_3$ | C$_4$ | C$_6$ |
| C$_{nv}$ | C$_{1v}$=C$_{1h}$ | C$_{2v}$ | C$_{3v}$ | C$_{4v}$ | C$_{6v}$ |
| C$_{nh}$ | C$_{1h}$ | C$_{2h}$ | C$_{3h}$ | C$_{4h}$ | C$_{6h}$ |
| D$_n$ | D$_1$=C$_2$ | D$_2$ | D$_3$ | D$_4$ | D$_6$ |
| D$_{nh}$ | D$_{1h}$=C$_{2v}$ | D$_{2h}$ | D$_{3h}$ | D$_{4h}$ | D$_{6h}$ |
| D$_{nd}$ | D$_{1d}$=C$_{2h}$ | D$_{2d}$ | D$_{3d}$ | D$_{4d}$ | D$_{6d}$ |
| S$_{2n}$ | S$_2$ | S$_4$ | S$_6$ | S$_8$ | S$_{12}$ |
D$_{4d}$ and D$_{6d}$ are actually forbidden because they contain improper rotations with n=8 and 12 respectively. The 27 point groups in the table plus T, T$_d$, T$_h$, O and O$_h$ 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
| Crystal family | Crystal system | Group names | Group names | Group names | Group names | Group names | Group names | Group names |
| Cubic | Cubic | 23 | m3 | | 432 | 43m | m3m | |
| Hexagonal | Hexagonal | 6 | 6 | $^6$⁄$_m$ | 622 | 6mm | 6m2 | 6/mmm |
| Hexagonal | Trigonal | 3 | 3 | | 32 | 3m | 3m | |
| Tetragonal | Tetragonal | 4 | 4 | $^4$⁄$_m$ | 422 | 4mm | 42m | 4/mmm |
| Orthorhombic | Orthorhombic | | | | 222 | | mm2 | mmm |
| Monoclinic | Monoclinic | 2 | | $^2$⁄$_m$ | | m | | |
| Triclinic | Triclinic | 1 | 1 | | | | | |

### The correspondence between different notations

| Crystal family | Crystal system | Hermann-Mauguin | Hermann-Mauguin | Shubnikov | Schoenflies | Orbifold | Coxeter | Order |
| Crystal family | Crystal system | (full) | (short) | Shubnikov | Schoenflies | Orbifold | Coxeter | Order |
| Triclinic | Triclinic | 1 | 1 | $1\$ | C$_1$ | 11 | [ ]$^+$ | 1 |
| Triclinic | Triclinic | 1 | 1 | ${\tilde {2}}$ | C$_i$ = S$_2$ | × | [2$^+$,2$^+$] | 2 |
| Monoclinic | Monoclinic | 2 | 2 | $2\$ | C$_2$ | 22 | [2]$^+$ | 2 |
| Monoclinic | Monoclinic | m | m | $m\$ | C$_s$ = C$_{1h}$ | * | [ ] | 2 |
| Monoclinic | Monoclinic | ${\tfrac {2}{m}}$ | 2/m | $2:m\$ | C$_{2h}$ | 2* | [2,2$^+$] | 4 |
| Orthorhombic | Orthorhombic | 222 | 222 | $2:2\$ | D$_2$ = V | 222 | [2,2]$^+$ | 4 |
| Orthorhombic | Orthorhombic | mm2 | mm2 | $2\cdot m\$ | C$_{2v}$ | *22 | [2] | 4 |
| Orthorhombic | Orthorhombic | ${\tfrac {2}{m}}{\tfrac {2}{m}}{\tfrac {2}{m}}$ | mmm | $m\cdot 2:m\$ | D$_{2h}$ = V$_h$ | *222 | [2,2] | 8 |
| Tetragonal | Tetragonal | 4 | 4 | $4\$ | C$_4$ | 44 | [4]$^+$ | 4 |
| Tetragonal | Tetragonal | 4 | 4 | ${\tilde {4}}$ | S$_4$ | 2× | [2$^+$,4$^+$] | 4 |
| Tetragonal | Tetragonal | ${\tfrac {4}{m}}$ | 4/m | $4:m\$ | C$_{4h}$ | 4* | [2,4$^+$] | 8 |
| Tetragonal | Tetragonal | 422 | 422 | $4:2\$ | D$_4$ | 422 | [4,2]$^+$ | 8 |
| Tetragonal | Tetragonal | 4mm | 4mm | $4\cdot m\$ | C$_{4v}$ | *44 | [4] | 8 |
| Tetragonal | Tetragonal | 42m | 42m | ${\tilde {4}}\cdot m$ | D$_{2d}$ = V$_d$ | 2*2 | [2$^+$,4] | 8 |
| Tetragonal | Tetragonal | ${\tfrac {4}{m}}{\tfrac {2}{m}}{\tfrac {2}{m}}$ | 4/mmm | $m\cdot 4:m\$ | D$_{4h}$ | *422 | [4,2] | 16 |
| Hexagonal | Trigonal | 3 | 3 | $3\$ | C$_3$ | 33 | [3]$^+$ | 3 |
| Hexagonal | Trigonal | 3 | 3 | ${\tilde {6}}$ | C$_{3i}$ = S$_6$ | 3× | [2$^+$,6$^+$] | 6 |
| Hexagonal | Trigonal | 32 | 32 | $3:2\$ | D$_3$ | 322 | [3,2]$^+$ | 6 |
| Hexagonal | Trigonal | 3m | 3m | $3\cdot m\$ | C$_{3v}$ | *33 | [3] | 6 |
| Hexagonal | Trigonal | 3${\tfrac {2}{m}}$ | 3m | ${\tilde {6}}\cdot m$ | D$_{3d}$ | 2*3 | [2$^+$,6] | 12 |
| Hexagonal | Hexagonal | 6 | 6 | $6\$ | C$_6$ | 66 | [6]$^+$ | 6 |
| Hexagonal | Hexagonal | 6 | 6 | $3:m\$ | C$_{3h}$ | 3* | [2,3$^+$] | 6 |
| Hexagonal | Hexagonal | ${\tfrac {6}{m}}$ | 6/m | $6:m\$ | C$_{6h}$ | 6* | [2,6$^+$] | 12 |
| Hexagonal | Hexagonal | 622 | 622 | $6:2\$ | D$_6$ | 622 | [6,2]$^+$ | 12 |
| Hexagonal | Hexagonal | 6mm | 6mm | $6\cdot m\$ | C$_{6v}$ | *66 | [6] | 12 |
| Hexagonal | Hexagonal | 6m2 | 6m2 | $m\cdot 3:m\$ | D$_{3h}$ | *322 | [3,2] | 12 |
| Hexagonal | Hexagonal | ${\tfrac {6}{m}}{\tfrac {2}{m}}{\tfrac {2}{m}}$ | 6/mmm | $m\cdot 6:m\$ | D$_{6h}$ | *622 | [6,2] | 24 |
| Cubic | Cubic | 23 | 23 | $3/2\$ | T | 332 | [3,3]$^+$ | 12 |
| Cubic | Cubic | ${\tfrac {2}{m}}$3 | m3 | ${\tilde {6}}/2$ | T$_h$ | 3*2 | [3$^+$,4] | 24 |
| Cubic | Cubic | 432 | 432 | $3/4\$ | O | 432 | [4,3]$^+$ | 24 |
| Cubic | Cubic | 43m | 43m | $3/{\tilde {4}}$ | T$_d$ | *332 | [3,3] | 24 |
| Cubic | Cubic | ${\tfrac {4}{m}}$3${\tfrac {2}{m}}$ | m3m | ${\tilde {6}}/4$ | O$_h$ | *432 | [4,3] | 48 |

## Isomorphisms

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 C$_2$. 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:
| Hermann-Mauguin | Schoenflies | Order | Abstract group | Abstract group |
| 1 | C$_1$ | 1 | C$_1$ | $G_{1}^{1}$ |
| 1 | C$_i$ = S$_2$ | 2 | C$_2$ | $G_{2}^{1}$ |
| 2 | C$_2$ | 2 | C$_2$ | $G_{2}^{1}$ |
| m | C$_s$ = C$_{1h}$ | 2 | C$_2$ | $G_{2}^{1}$ |
| 3 | C$_3$ | 3 | C$_3$ | $G_{3}^{1}$ |
| 4 | C$_4$ | 4 | C$_4$ | $G_{4}^{1}$ |
| 4 | S$_4$ | 4 | C$_4$ | $G_{4}^{1}$ |
| 2/m | C$_{2h}$ | 4 | D$_2$ = C$_2$ × C$_2$ | $G_{4}^{2}$ |
| 222 | D$_2$ = V | 4 | D$_2$ = C$_2$ × C$_2$ | $G_{4}^{2}$ |
| mm2 | C$_{2v}$ | 4 | D$_2$ = C$_2$ × C$_2$ | $G_{4}^{2}$ |
| 3 | C$_{3i}$ = S$_6$ | 6 | C$_6$ | $G_{6}^{1}$ |
| 6 | C$_6$ | 6 | C$_6$ | $G_{6}^{1}$ |
| 6 | C$_{3h}$ | 6 | C$_6$ | $G_{6}^{1}$ |
| 32 | D$_3$ | 6 | D$_3$ | $G_{6}^{2}$ |
| 3m | C$_{3v}$ | 6 | D$_3$ | $G_{6}^{2}$ |
| mmm | D$_{2h}$ = V$_h$ | 8 | D$_2$ × C$_2$ | $G_{8}^{3}$ |
| 4/m | C$_{4h}$ | 8 | C$_4$ × C$_2$ | $G_{8}^{2}$ |
| 422 | D$_4$ | 8 | D$_4$ | $G_{8}^{4}$ |
| 4mm | C$_{4v}$ | 8 | D$_4$ | $G_{8}^{4}$ |
| 42m | D$_{2d}$ = V$_d$ | 8 | D$_4$ | $G_{8}^{4}$ |
| 6/m | C$_{6h}$ | 12 | C$_6$ × C$_2$ | $G_{12}^{2}$ |
| 23 | T | 12 | A$_4$ | $G_{12}^{5}$ |
| 3m | D$_{3d}$ | 12 | D$_6$ | $G_{12}^{3}$ |
| 622 | D$_6$ | 12 | D$_6$ | $G_{12}^{3}$ |
| 6mm | C$_{6v}$ | 12 | D$_6$ | $G_{12}^{3}$ |
| 6m2 | D$_{3h}$ | 12 | D$_6$ | $G_{12}^{3}$ |
| 4/mmm | D$_{4h}$ | 16 | D$_4$ × C$_2$ | $G_{16}^{9}$ |
| 6/mmm | D$_{6h}$ | 24 | D$_6$ × C$_2$ | $G_{24}^{5}$ |
| m3 | T$_h$ | 24 | A$_4$ × C$_2$ | $G_{24}^{10}$ |
| 432 | O | 24 | S$_4$ | $G_{24}^{7}$ |
| 43m | T$_d$ | 24 | S$_4$ | $G_{24}^{7}$ |
| m3m | O$_h$ | 48 | S$_4$ × C$_2$ | $G_{48}^{7}$ |
This table makes use of cyclic groups (C$_1$, C$_2$, C$_3$, C$_4$, C$_6$), dihedral groups (D$_2$, D$_3$, D$_4$, D$_6$), one of the alternating groups (A$_4$), and one of the symmetric groups (S$_4$). Here the symbol " × " indicates a direct product.

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

* Leave out the Bravais lattice type.
* 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.)
* Axes of rotation, rotoinversion axes, and mirror planes remain unchanged.