The Schoenflies (or Schönflies) notation, named after the German mathematician Arthur Moritz Schoenflies, is a notation primarily used to specify point groups in three dimensions. Because a point group alone is completely adequate to describe the symmetry of a molecule, the notation is often sufficient and commonly used for spectroscopy. However, in crystallography, there is additional translational symmetry, and point groups are not enough to describe the full symmetry of crystals, so the full space group is usually used instead. The naming of full space groups usually follows another common convention, the Hermann–Mauguin notation, also known as the international notation.
Although Schoenflies notation without superscripts is a pure point group notation, optionally, superscripts can be added to further specify individual space groups. However, for space groups, the connection to the underlying symmetry elements is much more clear in Hermann–Mauguin notation, so the latter notation is usually preferred for space groups.
Symmetry elements are denoted by i for centers of inversion, C for proper rotation axes, σ for mirror planes, and S for improper rotation axes (rotationreflection axes). C and S are usually followed by a subscript number (abstractly denoted n) denoting the order of rotation possible.
By convention, the axis of proper rotation of greatest order is defined as the principal axis. All other symmetry elements are described in relation to it. A vertical mirror plane (containing the principal axis) is denoted σ_{v}; a horizontal mirror plane (perpendicular to the principal axis) is denoted σ_{h}.
In three dimensions, there are an infinite number of point groups, but all of them can be classified by several families.
All groups that do not contain more than one higherorder axis (order 3 or more) can be arranged as shown in a table below; symbols in red are rarely used.
n = 1  2  3  4  5  6  7  8  ...  ∞  

C_{n}  C_{1}  C_{2}  C_{3}  C_{4}  C_{5}  C_{6}  C_{7}  C_{8}  ...

C_{∞} 
C_{nv}  C_{1v} = C_{1h}  C_{2v}  C_{3v}  C_{4v}  C_{5v}  C_{6v}  C_{7v}  C_{8v}  ...

C_{∞v} 
C_{nh}  C_{1h} = C_{s}  C_{2h}  C_{3h}  C_{4h}  C_{5h}  C_{6h}  C_{7h}  C_{8h}  ...

C_{∞h} 
S_{n}  S_{1} = C_{s}  S_{2} = C_{i}  S_{3} = C_{3h}  S_{4}  S_{5} = C_{5h}  S_{6}  S_{7} = C_{7h}  S_{8}  ...

S_{∞} = C_{∞h} 
C_{ni} (redundant)  C_{1i} = C_{i}  C_{2i} = C_{s}  C_{3i} = S_{6}  C_{4i} = S_{4}  C_{5i} = S_{10}  C_{6i} = C_{3h}  C_{7i} = S_{14}  C_{8i} = S_{8}  ...

C_{∞i} = C_{∞h} 
D_{n}  D_{1} = C_{2}  D_{2}  D_{3}  D_{4}  D_{5}  D_{6}  D_{7}  D_{8}  ...

D_{∞} 
D_{nh}  D_{1h} = C_{2v}  D_{2h}  D_{3h}  D_{4h}  D_{5h}  D_{6h}  D_{7h}  D_{8h}  ...

D_{∞h} 
D_{nd}  D_{1d} = C_{2h}  D_{2d}  D_{3d}  D_{4d}  D_{5d}  D_{6d}  D_{7d}  D_{8d}  ...

D_{∞d} = D_{∞h} 
In crystallography, due to the crystallographic restriction theorem, n is restricted to the values of 1, 2, 3, 4, or 6. The noncrystallographic groups are shown with grayed backgrounds. D_{4d} and D_{6d} are also 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.
Groups with n = ∞ are called limit groups or Curie groups. There are two more limit groups, not listed in the table: K (for Kugel, German for ball, sphere), the group of all rotations in 3dimensional space; and K_{h}, the group of all rotations and reflections. In mathematics and theoretical physics they are known respectively as the special orthogonal group and the orthogonal group in threedimensional space, with the symbols SO(3) and O(3).
The space groups with given point group are numbered by 1, 2, 3, ... (in the same order as their international number) and this number is added as a superscript to the Schönflies symbol for the corresponding point group. For example, groups numbers 3 to 5 whose point group is C_{2} have Schönflies symbols C^{1}
_{2}, C^{2}
_{2}, C^{3}
_{2}.
While in case of point groups, Schönflies symbol defines the symmetry elements of group unambiguously, the additional superscript for space group doesn't have any information about translational symmetry of space group (lattice centering, translational components of axes and planes), hence one needs to refer to special tables, containing information about correspondence between Schönflies and Hermann–Mauguin notation. Such table is given in List of space groups page.