# Point groups

Nonaxial groups Cn groups Dn groups Cnv groups Cnh groups Dnh groups Dnd groups C1 - $1$ Cs - $m$ Ci - $\bar{1}$ C2 - $2$ C3 - $3$ C4 - $4$ C5 - $5$ C6 - $6$ C7 - $7$ C8 - $8$ D2 - $222$ D3 - $32$ D4 - $422$ D5 - $52$ D6 - $622$ D7 - $722$ D8 - $822$ C2v - $mm2$ C3v - $3m$ C4v - $4mm$ C5v - $5m$ C6v - $6mm$ C7v - $7m$ C8v - $8mm$ C2h - $2/m$ C3h - $\bar{6}$ C4h - $4/m$ C5h - $\bar{10}$ C6h - $6/m$ D2h - $mmm$ D3h - $\bar{6}m2$ D4h - $4/mmm$ D5h - $\bar{10}m2$ D6h - $6/mmm$ D7h - $\bar{14}m2$ D8h - $8/mmm$ D2d - $\bar{4}2m$ D3d - $\bar{3}m$ D4d - $\bar{8}2m$ D5d - $\bar{5}m$ D6d - $\bar{12}2m$ D7d - $\bar{7}m$ D8d - $\bar{16}2m$ S2 - $\bar{2}$ S4 - $\bar{4}$ S6 - $\bar{6}$ S8 - $\bar{8}$ S10 - $\bar{10}$ S12 - $\bar{12}$ T - $23$ Th - $m\bar{3}$ Td - $\bar{4}3m$ O - $432$ Oh - $m\bar{3}m$ I - $532$ Ih - $\bar{5}\bar{3}m$ C$\infty$v D$\infty$h

The following set of pages list properties of the different point groups and their irreducible representations. The table above links to the main page of each of the different point group. For each group we list the character and product table. Often one needs to answer the question how a potential in a given point group looks like and what the eigen-states of that potential are. The eigen states can be grouped according to the irreducible representations of the group and for each of these representations one can give representing functions. The form of these functions and the potential however do depend on the orientation of the point group. We therefor list for each point group different orientations.

## Different orientations

As we are interested in explicit representations we do need to specify the orientation of the symmetry operators. This results in several tables for the same point group but with different choices for the symmetry operations. For example the cubic $O_h$ point group can be represented with the $C_4$ axes in the $x$, $y$ and $z$ direction, or with a $C_3$ axis in the $z$ direction. We list several orientations of the different point-groups available.

## Symmetry operations

We use the following notation for symmetry operations.

E = identity

Cn = n-fold rotation

Sn = n-fold rotation plus reflection through a plane perpendicular to the axis of rotation

i = inversion through a centre of symmetry

$\sigma$v = reflection through a mirror plane (called “vertical”) parallel to the principal axis

$\sigma$h = reflection through a mirror plane (called “horizontal”) perpendicular to the principal axis

$\sigma$d = reflection through a vertical mirror plane bisecting the angle between two C2 axes

## Irreducible representations

We use the following notation for the irreducible representations.

A = one-dimensional irreducible representation with character +1 under the principal rotation

B = one-dimensional irreducible representation with character -1 under the principal rotation

E = two-dimensional irreducible representation

T = three-dimensional irreducible representation

Point groups with inversion symmetry are separated into even (g) and odd (u) irreducible representations

## Acknowledgements

These pages and tables on point groups are generated from a small code written in Quanty and Mathematica developed and tested by Maurits W. Haverkort, Vincent Vercamer and Stefano Agrestini.

## Table of several point groups

Nonaxial groups Cn groups Dn groups Cnv groups Cnh groups Dnh groups Dnd groups C1 Cs Ci C2 C3 C4 C5 C6 C7 C8 D2 D3 D4 D5 D6 D7 D8 C2v C3v C4v C5v C6v C7v C8v C2h C3h C4h C5h C6h D2h D3h D4h D5h D6h D7h D8h D2d D3d D4d D5d D6d D7d D8d S2 S4 S6 S8 S10 S12 T Th Td O Oh I Ih C$\infty$v D$\infty$h