Point-Group Diagrams |

The majority of the table is reference material.

**Point-Group Diagrams**

The previous two pages were an introduction to the concepts of molecular point symmetry and the crystallographic notation used to define it. We now return to the concept of stereographic projections to illustrate the symmetry elements of the 32 crystallographic point groups.

The figure below shows a ball & stick figure of a water molecule viewed
down the twofold rotation axis that passes through the central oxygen
atom. As pointed out earlier, this molecule has the crystallographic
point-group symmetry *mm*2. Superimposed on the molecule is the
steroegraphic diagram for this particular point group.

The lens-shaped symbol represents the twofold rotation axis, and the two solid thick lines show two mutually-perpendicular mirror planes whose line of intersection contains the twofold. In addition, the figure shows how an arbitrary point (shown top right as an open circle with a "+" symbol), which is not lying on any of the symmetry elements, is symmetry related to three other points, two of which have an opposite handedness to the original.

The table that follows contains clickable links to stereographic diagrams for all of the 32 crystallographic point groups. Note that additional comments are made only concerning the figures of the low-symmetry point groups.

Crystal System | 32 Crystallographic Point Groups | ||||||
---|---|---|---|---|---|---|---|

Triclinic | 1 | -1 | |||||

Monoclinic | 2 | m |
2/m |
||||

Orthorhombic | 222 | mm2 |
mmm |
||||

Tetragonal | 4 | -4 | 4/m |
422 | 4mm |
-42m |
4/mmm |

Trigonal | 3 | -3 | 32 | 3m |
-3m |
||

Hexagonal | 6 | -6 | 6/m |
622 | 6mm |
-62m |
6/mmm |

Cubic | 23 | m-3 |
432 | -43m |
m-3m |

**Special Positions**

The above figure also introduces the concept of *special positions*.
This is a term frequently used to describe the coordinates of atoms
in a crystal structure that do not have the
general coordinates, *x*,*y*,*z*.
In the above figure, the hydrogen atoms lie on one of the mirror plane and
the oxygen lies on the twofold rotation axis formed by the intersection
of the two mirror planes. Applying the various symmetry elements to
one of the hydrogen atoms can generate the second, but no more. Likewise,
applying the symmetry elements to the oxygen atom generates only the original
atom and nothing else. Thus all three atoms lie on so-called special positions,
and only the coordinates of two of them are required in order to
completely specify the position of the water molecule given
its point-group symmetry of *mm*2.
This concept will be developed further in the later
section on space-group symmetry.

© Copyright 1995-2006. Birkbeck College, University of London. |
Author(s):
Jeremy Karl Cockcroft |