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In mathematics, point group is a group of geometric symmetries (isometries) leaving a point fixed. Point groups can exist in a Euclidean space of any dimension. In 2D, a discrete point group is sometimes called a rosette group, and is used to describe the symmetries of an ornament. The 3D discrete point groups are heavily used in chemistry, especially to describe the symmetries of a molecule and of orbitals forming covalent bonds, and in this context they are also called molecular point groups. See point groups in three dimensions.

There are infinitely many discrete point groups in each number of dimensions. However, only a finite number is compatible with translational symmetry. This is stated in the crystallographic restriction theorem. In 1D there are 2, in 2D 10, and in 3D 32. They are called crystallographic point groups.

Point groups in 2D fall into two distinct families, according to whether they consist of rotations only, or include reflections. The cyclic groups, C_n (abstract group type Z_n), consist of rotations by 360°/n, and all integer multiples. For example, a swastika has symmetry group C₄, consisting of rotations by 0°, 90°, 180°, and 270°. The symmetry group of a square belongs to the family of dihedral groups, D_n (abstract group type Dih_n), including as many reflections as rotations. The infinite rotational symmetry of the circle implies reflection symmetry as well, but formally the circle group S₁ is distinct from Dih(S₁) because it explicitly includes the reflections. Note that an infinite group need not be continuous; for example, we have a group of all integer multiples of rotation by 360°/√2, which does not include rotation by 180°. Depending on application, homogeneity up to arbitrarily fine detail in transverse direction may be considered equivalent to full homogeneity in that direction, in which case these symmetry groups can be ignored. See also point groups in two dimensions.

C_n and D_n for n = 1, 2, 3, 4, and 6 can be combined with translational symmetry, sometimes in more than one way. Thus these 10 groups give rise to 17 wallpaper groups.

More complex symmetries arise in 3D, see point groups in three dimensions.

In any dimension, d, the continuous group of all possible fixed point isometries is the orthogonal group, denoted by O(d); and its continuous subgroup of all possible rotations is the special orthogonal group, denoted by SO(d). This is not Schönflies notation, but the conventional names from Lie group theory.