Examples of frieze patterns

In mathematics, a frieze or frieze pattern is a two-dimensional design that repeats in one direction. The term is derived from architecture and decorative arts, where such repeating patterns are often used. (See frieze.) Frieze patterns can be classified into seven types according to their symmetries. The set of symmetries of a frieze pattern is called a frieze group.

Frieze groups are two-dimensional line groups, having repetition in only one direction. They are related to the more complex wallpaper groups, which classify patterns that are repetitive in two directions, and crystallographic groups, which classify patterns that are repetitive in three directions.


The seven frieze groups
  1. p1: T (translation only, in the horizontal direction)
  2. p1m1: TV (translation and vertical line reflection)
  3. p11m: THG (translation, horizontal line reflection, and glide reflection)
  4. p11g: TG (translation and glide reflection)
  5. p2: TR (translation and 180° rotation)
  6. p2mg: TRVG (translation, 180° rotation, vertical line reflection, and glide reflection)
  7. p2mm: TRHVG (translation, 180° rotation, horizontal line reflection, vertical line reflection, and glide reflection)

Formally, a frieze group is a class of infinite discrete symmetry groups of patterns on a strip (infinitely wide rectangle), hence a class of groups of isometries of the plane, or of a strip. A symmetry group of a frieze group necessarily contains translations and may contain glide reflections, reflections along the long axis of the strip, reflections along the narrow axis of the strip, and 180° rotations. There are seven frieze groups, listed in the summary table. Many authors present the frieze groups in a different order.[1][2]

The actual symmetry groups within a frieze group are characterized by the smallest translation distance, and, for the frieze groups with vertical line reflection or 180° rotation (groups 2, 5, 6, and 7), by a shift parameter locating the reflection axis or point of rotation. In the case of symmetry groups in the plane, additional parameters are the direction of the translation vector, and, for the frieze groups with horizontal line reflection, glide reflection, or 180° rotation (groups 3–7), the position of the reflection axis or rotation point in the direction perpendicular to the translation vector. Thus there are two degrees of freedom for group 1, three for groups 2, 3, and 4, and four for groups 5, 6, and 7.

For two of the seven frieze groups (groups 1 and 4) the symmetry groups are singly generated, for four (groups 2, 3, 5, and 6) they have a pair of generators, and for group 7 the symmetry groups require three generators. A symmetry group in frieze group 1, 2, 3, or 5 is a subgroup of a symmetry group in the last frieze group with the same translational distance. A symmetry group in frieze group 4 or 6 is a subgroup of a symmetry group in the last frieze group with half the translational distance. This last frieze group contains the symmetry groups of the simplest periodic patterns in the strip (or the plane), a row of dots. Any transformation of the plane leaving this pattern invariant can be decomposed into a translation, (x, y) ↦ (n + x, y), optionally followed by a reflection in either the horizontal axis, (x, y) ↦ (x, −y), or the vertical axis, (x, y) ↦ (−x, y), provided that this axis is chosen through or midway between two dots, or a rotation by 180°, (x, y) ↦ (−x, −y) (ditto). Therefore, in a way, this frieze group contains the "largest" symmetry groups, which consist of all such transformations.

The inclusion of the discrete condition is to exclude the group containing all translations, and groups containing arbitrarily small translations (e.g. the group of horizontal translations by rational distances). Even apart from scaling and shifting, there are infinitely many cases, e.g. by considering rational numbers of which the denominators are powers of a given prime number.

The inclusion of the infinite condition is to exclude groups that have no translations:

Descriptions of the seven frieze groups

There are seven distinct subgroups (up to scaling and shifting of patterns) in the discrete frieze group generated by a translation, reflection (along the same axis) and a 180° rotation. Each of these subgroups is the symmetry group of a frieze pattern, and sample patterns are shown in Fig. 1. The seven different groups correspond to the 7 infinite series of axial point groups in three dimensions, with n = ∞.[3]

They are identified in the table below using Hermann–Mauguin notation (or IUC notation),[4] Coxeter notation, Schönflies notation, orbifold notation, nicknames created by mathematician John H. Conway, and finally a description in terms of translation, reflections and rotations.

Frieze groups
IUC Cox. Schön.* Orbifold Diagram§ Examples and
Conway nickname[5]
p1 [∞]+
(T) Translations only:
This group is singly generated, by a translation by the smallest distance over which the pattern is periodic.
p11g [∞+,2+]
(TG) Glide-reflections and Translations:
This group is singly generated, by a glide reflection, with translations being obtained by combining two glide reflections.
p1m1 [∞]
(TV) Vertical reflection lines and Translations:
The group is the same as the non-trivial group in the one-dimensional case; it is generated by a translation and a reflection in the vertical axis.
p2 [∞,2]+
spinning hop
(TR) Translations and 180° Rotations:
The group is generated by a translation and a 180° rotation.
p2mg [∞,2+]
spinning sidle
(TRVG) Vertical reflection lines, Glide reflections, Translations and 180° Rotations:
The translations here arise from the glide reflections, so this group is generated by a glide reflection and either a rotation or a vertical reflection.
p11m [∞+,2]
(THG) Translations, Horizontal reflections, Glide reflections:
This group is generated by a translation and the reflection in the horizontal axis. The glide reflection here arises as the composition of translation and horizontal reflection
p2mm [∞,2]
spinning jump
(TRHVG) Horizontal and Vertical reflection lines, Translations and 180° Rotations:
This group requires three generators, with one generating set consisting of a translation, the reflection in the horizontal axis and a reflection across a vertical axis.
*Schönflies's point group notation is extended here as infinite cases of the equivalent dihedral points symmetries
§The diagram shows one fundamental domain in yellow, with reflection lines in blue, glide reflection lines in dashed green, translation normals in red, and 2-fold gyration points as small green squares.

Of the seven frieze groups, there are only four up to isomorphism. Two are singly generated and isomorphic to ; four of them are doubly generated, among which one is abelian and three are nonabelian and isomorphic to , the infinite dihedral group; and one of them has three generators.[6]

Lattice types: Oblique and rectangular

The groups can be classified by their type of two-dimensional grid or lattice.[7] The lattice being oblique means that the second direction need not be orthogonal to the direction of repeat.

Lattice type Groups
Oblique p1, p2
Rectangular p1m1, p11m, p11g, p2mm, p2mg

See also

Web demo and software

There exist software graphic tools that create 2D patterns using frieze groups. Usually, the entire pattern is updated automatically in response to edits of the original strip.


  1. ^ Coxeter, H. S. M. (1969). Introduction to Geometry. New York: John Wiley & Sons. pp. 47–49. ISBN 0-471-50458-0.
  2. ^ Cederberg, Judith N. (2001). A Course in Modern Geometries, 2nd ed. New York: Springer-Verlag. pp. 117–118, 165–171. ISBN 0-387-98972-2.
  3. ^ Fisher, G.L.; Mellor, B. (2007), "Three-dimensional finite point groups and the symmetry of beaded beads" (PDF), Journal of Mathematics and the Arts, 1 (2): 85–96, doi:10.1080/17513470701416264, S2CID 40755219
  4. ^ Radaelli, Paolo G., Fundamentals of Crystallographic Symmetry (PDF)[permanent dead link]
  5. ^ Frieze Patterns Mathematician John Conway created names that relate to footsteps for each of the frieze groups.
  6. ^ https://www.whitman.edu/documents/Academics/Mathematics/2019/Landau-Balof.pdf [bare URL PDF]
  7. ^ Hitzer, E.S.M.; Ichikawa, D. (2008), "Representation of crystallographic subperiodic groups by geometric algebra" (PDF), Electronic Proc. Of AGACSE (3, 17–19 Aug. 2008), Leipzig, Germany, archived from the original (PDF) on 2012-03-14