This article deals with the four infinite series of point groups in three dimensions (n≥1) with n-fold rotational symmetry about one axis (rotation by an angle of 360°/n does not change the object), and no other rotational symmetry (n=1 covers the cases of no rotational symmetry at all):

Chiral:

• C_n (nn) of order n - n-fold rotational symmetry (abstract group C_n); for n=1: no symmetry (trivial group)

• C_nh (n*) of order 2n - prismatic symmetry (abstract group D_n × C₂); for n=1 this is denoted by C_s (1*) and called reflection symmetry, also bilateral symmetry.
• C_nv (*nn) of order 2n - pyramidal symmetry (abstract group D_n); in biology C_2v is called biradial symmetry. For n=1 we have again C_s (1*).
• S_2n (n×) of order 2n (not to be confused with symmetric groups, for which the same notation is used; abstract group C_2n); for n=1 we have S₂ (1×), also denoted by C_i; this is inversion symmetry

They are the finite symmetry groups on a cone. For n = $\backslash infty$ they correspond to four frieze groups. Schönflies notation is used, and, in parentheses, Conway's orbifold notation. The terms horizontal (h) and vertical (v) are used with respect to a vertical axis of rotation.

C_nh (n*) has reflection symmetry with respect to a plane perpendicular to the n-fold rotation axis. C_nv (*nn) has vertical mirror planes. This is the symmetry group for a regular n-sided pyramid.

S_2n (n×) has a 2n-fold rotoreflection axis, also called 2n-fold improper rotation axis, i.e., the symmetry group contains a combination of a reflection in the horizontal plane and a rotation by an angle 180°/n. Thus, like D_nd, it contains a number of improper rotations without containing the corresponding rotations.

C_2h (2*) and C_2v (*22) of order 4 are two of the three 3D symmetry group types with the Klein four-group as abstract group. C_2v applies e.g. for a rectangular tile with its top side different from its bottom side.

Examples

C_4v (*44):'''

C_5v (*55):'''

Symmetry