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Definition of the notation

The following types of Euclidean transformation can occur in a group described by orbifold notation:

• reflection through a line (or plane)
• translation by a vector
• rotation of finite order around a point
• infinite rotation around a line in 3-space
• glide-reflection, i.e. reflection followed by translation.

All translations which occur are assumed to form a discrete subgroup of the group symmetries being described.

Each group is denoted in orbifold notation by a finite string made up from the following symbols:

• positive integers 1 , 2 , 3 , … {\displaystyle 1,2,3,\dots }
• the infinity symbol, ∞ {\displaystyle \infty }
• the asterisk, *
• the symbol o (a solid circle in older documents), which is called a wonder and also a handle because it topologically represents a torus (1-handle) closed surface. Patterns repeat by two translation.
• the symbol × {\displaystyle \times } (an open circle in older documents), which is called a miracle and represents a topological crosscap where a pattern repeats as a mirror image without crossing a mirror line.

A string written in boldface represents a group of symmetries of Euclidean 3-space. A string not written in boldface represents a group of symmetries of the Euclidean plane, which is assumed to contain two independent translations.

Each symbol corresponds to a distinct transformation:

• an integer n to the left of an asterisk indicates a rotation of order n around a gyration point
• the asterisk, * indicates a reflection
• an integer n to the right of an asterisk indicates a transformation of order 2n which rotates around a kaleidoscopic point and reflects through a line (or plane)
• an × {\displaystyle \times } indicates a glide reflection
• the symbol ∞ {\displaystyle \infty } indicates infinite rotational symmetry around a line; it can only occur for bold face groups. By abuse of language, we might say that such a group is a subgroup of symmetries of the Euclidean plane with only one independent translation. The frieze groups occur in this way.
• the exceptional symbol o indicates that there are precisely two linearly independent translations.

Good orbifolds

An orbifold symbol is called good if it is not one of the following: p, pq, *p, *pq, for p, q ≥ 2, and p ≠ q.

Chirality and achirality

An object is chiral if its symmetry group contains no reflections; otherwise it is called achiral. The corresponding orbifold is orientable in the chiral case and non-orientable otherwise.

The Euler characteristic and the order

The Euler characteristic of an orbifold can be read from its Conway symbol, as follows. Each feature has a value:

• n without or before an asterisk counts as n − 1 n {\displaystyle {\frac {n-1}{n}}}
• n after an asterisk counts as n − 1 2 n {\displaystyle {\frac {n-1}{2n}}}
• asterisk and × {\displaystyle \times } count as 1
• o counts as 2.

Subtracting the sum of these values from 2 gives the Euler characteristic.

If the sum of the feature values is 2, the order is infinite, i.e., the notation represents a wallpaper group or a frieze group. Indeed, Conway's "Magic Theorem" indicates that the 17 wallpaper groups are exactly those with the sum of the feature values equal to 2. Otherwise, the order is 2 divided by the Euler characteristic.

Equal groups

The following groups are isomorphic:

• 1* and *11
• 22 and 221
• *22 and *221
• 2* and 2*1.

This is because 1-fold rotation is the "empty" rotation.

Two-dimensional groups

The symmetry of a 2D object without translational symmetry can be described by the 3D symmetry type by adding a third dimension to the object which does not add or spoil symmetry. For example, for a 2D image we can consider a piece of carton with that image displayed on one side; the shape of the carton should be such that it does not spoil the symmetry, or it can be imagined to be infinite. Thus we have n• and *n•. The bullet (•) is added on one- and two-dimensional groups to imply the existence of a fixed point. (In three dimensions these groups exist in an n-fold digonal orbifold and are represented as nn and *nn.)

Similarly, a 1D image can be drawn horizontally on a piece of carton, with a provision to avoid additional symmetry with respect to the line of the image, e.g. by drawing a horizontal bar under the image. Thus the discrete symmetry groups in one dimension are *•, *1•, ∞• and *∞•.

Another way of constructing a 3D object from a 1D or 2D object for describing the symmetry is taking the Cartesian product of the object and an asymmetric 2D or 1D object, respectively.

Correspondence tables

Spherical

Fundamental domains of reflective 3D point groups

(*11), C1v = Cs	(*22), C2v	(*33), C3v	(*44), C4v	(*55), C5v	(*66), C6v
Order 2	Order 4	Order 6	Order 8	Order 10	Order 12
(*221), D1h = C2v	(*222), D2h	(*223), D3h	(*224), D4h	(*225), D5h	(*226), D6h
Order 4	Order 8	Order 12	Order 16	Order 20	Order 24
(*332), Td		(*432), Oh		(*532), Ih
Order 24		Order 48		Order 120

See also: List of spherical symmetry groups

Spherical symmetry groups¹

Orbifold signature	Coxeter	Schönflies	Hermann–Mauguin	Order
Polyhedral groups
*532	[3,5]	Ih	53m	120
532	[3,5]+	I	532	60
*432	[3,4]	Oh	m3m	48
432	[3,4]+	O	432	24
*332	[3,3]	Td	43m	24
3*2	[3+,4]	Th	m3	24
332	[3,3]+	T	23	12
Dihedral and cyclic groups: n = 3, 4, 5 ...
*22n	[2,n]	Dnh	n/mmm or 2nm2	4n
2*n	[2+,2n]	Dnd	2n2m or nm	4n
22n	[2,n]+	Dn	n2	2n
*nn	[n]	Cnv	nm	2n
n*	[n+,2]	Cnh	n/m or 2n	2n
n×	[2+,2n+]	S2n	2n or n	2n
nn	[n]+	Cn	n	n
Special cases
*222	[2,2]	D2h	2/mmm or 22m2	8
2*2	[2+,4]	D2d	222m or 2m	8
222	[2,2]+	D2	22	4
*22	[2]	C2v	2m	4
2*	[2+,2]	C2h	2/m or 22	4
2×	[2+,4+]	S4	22 or 2	4
22	[2]+	C2	2	2
*22	[1,2]	D1h = C2v	1/mmm or 21m2	4
2*	[2+,2]	D1d = C2h	212m or 1m	4
22	[1,2]+	D1 = C2	12	2
*1	[ ]	C1v = Cs	1m	2
1*	[2,1+]	C1h = Cs	1/m or 21	2
1×	[2+,2+]	S2 = Ci	21 or 1	2
1	[ ]+	C1	1	1

Euclidean plane

See also: List of planar symmetry groups

Frieze groups

Frieze groups

IUC	Cox.	Schön.*	Orbifold	Diagram§	Examples and Conway nickname2		Description
p1	[∞]+	C∞Z∞	∞∞			hop	(T) Translations only:This group is singly generated, by a translation by the smallest distance over which the pattern is periodic.
p11g	[∞+,2+]	S∞Z∞	∞×			step	(TG) Glide-reflections and Translations:This group is singly generated, by a glide reflection, with translations being obtained by combining two glide reflections.
p1m1	[∞]	C∞vDih∞	*∞∞			sidle	(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]+	D∞Dih∞	22∞			spinning hop	(TR) Translations and 180° Rotations:The group is generated by a translation and a 180° rotation.
p2mg	[∞,2+]	D∞dDih∞	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]	C∞hZ∞×Dih1	∞*			jump	(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]	D∞hDih∞×Dih1	*22∞			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.

Wallpaper groups

Fundamental domains of Euclidean reflective groups

(*442), p4m	(4*2), p4g
(*333), p3m	(632), p6

17 wallpaper groups³

Orbifoldsignature	Coxeter	Hermann–Mauguin	SpeiserNiggli	PolyaGuggenhein	Fejes TothCadwell
*632	[6,3]	p6m	C(I)6v	D6	W16
632	[6,3]+	p6	C(I)6	C6	W6
*442	[4,4]	p4m	C(I)4	D*4	W14
4*2	[4+,4]	p4g	CII4v	Do4	W24
442	[4,4]+	p4	C(I)4	C4	W4
*333	[3[3]]	p3m1	CII3v	D*3	W13
3*3	[3+,6]	p31m	CI3v	Do3	W23
333	[3[3]]+	p3	CI3	C3	W3
*2222	[∞,2,∞]	pmm	CI2v	D2kkkk	W22
2*22	[∞,2+,∞]	cmm	CIV2v	D2kgkg	W12
22*	[(∞,2)+,∞]	pmg	CIII2v	D2kkgg	W32
22×	[∞+,2+,∞+]	pgg	CII2v	D2gggg	W42
2222	[∞,2,∞]+	p2	C(I)2	C2	W2
**	[∞+,2,∞]	pm	CIs	D1kk	W21
*×	[∞+,2+,∞]	cm	CIIIs	D1kg	W11
××	[∞+,(2,∞)+]	pg	CII2	D1gg	W31
o	[∞+,2,∞+]	p1	C(I)1	C1	W1

Hyperbolic plane

Poincaré disk model of fundamental domain triangles

Example https://www.icann.org/en/data-protection triangles (*2pq)
*237	*238	*239	*23∞
*245	*246	*247	*248	*∞42
*255	*256	*257	*266	*2∞∞
Example general triangles (*pqr)
*334	*335	*336	*337	*33∞
*344	*366	*3∞∞	*63	*∞3
Example higher polygons (*pqrs...)
*2223	*(23)2	*(24)2	*34	*44
*25	*26	*27	*28
*222∞	*(2∞)2	*∞4	*2∞	*∞∞

A first few hyperbolic groups, ordered by their Euler characteristic are:

Hyperbolic symmetry groups⁴

−1/χ	Orbifolds	Coxeter
84	*237	[7,3]
48	*238	[8,3]
42	237	[7,3]+
40	*245	[5,4]
36–26.4	*239, *2 3 10	[9,3], [10,3]
26.4	*2 3 11	[11,3]
24	*2 3 12, *246, *334, 3*4, 238	[12,3], [6,4], [(4,3,3)], [3+,8], [8,3]+
22.3–21	*2 3 13, *2 3 14	[13,3], [14,3]
20	*2 3 15, *255, 5*2, 245	[15,3], [5,5], [5+,4], [5,4]+
19.2	*2 3 16	[16,3]
18+2⁄3	*247	[7,4]
18	*2 3 18, 239	[18,3], [9,3]+
17.5–16.2	*2 3 19, *2 3 20, *2 3 21, *2 3 22, *2 3 23	[19,3], [20,3], [20,3], [21,3], [22,3], [23,3]
16	*2 3 24, *248	[24,3], [8,4]
15	*2 3 30, *256, *335, 3*5, 2 3 10	[30,3], [6,5], [(5,3,3)], [3+,10], [10,3]+
14+2⁄5–13+1⁄3	*2 3 36 ... *2 3 70, *249, *2 4 10	[36,3] ... [60,3], [9,4], [10,4]
13+1⁄5	*2 3 66, 2 3 11	[66,3], [11,3]+
12+8⁄11	*2 3 105, *257	[105,3], [7,5]
12+4⁄7	*2 3 132, *2 4 11 ...	[132,3], [11,4], ...
12	*23∞, *2 4 12, *266, 6*2, *336, 3*6, *344, 4*3, *2223, 2*23, 2 3 12, 246, 334	[∞,3] [12,4], [6,6], [6+,4], [(6,3,3)], [3+,12], [(4,4,3)], [4+,6], [∞,3,∞], [12,3]+, [6,4]+ [(4,3,3)]+
...

See also

• Mutation of orbifolds
• Fibrifold notation - an extension of orbifold notation for 3d space groups

• John H. Conway, Olaf Delgado Friedrichs, Daniel H. Huson, and William P. Thurston. On Three-dimensional Space Groups. Contributions to Algebra and Geometry, 42(2):475-507, 2001.
• J. H. Conway, D. H. Huson. The Orbifold Notation for Two-Dimensional Groups. Structural Chemistry, 13 (3-4): 247–257, August 2002.
• J. H. Conway (1992). "The Orbifold Notation for Surface Groups". In: M. W. Liebeck and J. Saxl (eds.), Groups, Combinatorics and Geometry, Proceedings of the L.M.S. Durham Symposium, July 5–15, Durham, UK, 1990; London Math. Soc. Lecture Notes Series 165. Cambridge University Press, Cambridge. pp. 438–447
• John H. Conway, Heidi Burgiel, Chaim Goodman-Strauss, The Symmetries of Things 2008, ISBN 978-1-56881-220-5
• Hughes, Sam (2022), "Cohomology of Fuchsian groups and non-Euclidean crystallographic groups", Manuscripta Mathematica, 170 (3–4): 659–676, arXiv:1910.00519, Bibcode:2019arXiv191000519H, doi:10.1007/s00229-022-01369-z, S2CID 203610179

External links

• A field guide to the orbifolds (Notes from class on "Geometry and the Imagination" in Minneapolis, with John Conway, Peter Doyle, Jane Gilman and Bill Thurston, on June 17–28, 1991. See also PDF, 2006)
• Tegula Software for visualizing two-dimensional tilings of the plane, sphere and hyperbolic plane, and editing their symmetry groups in orbifold notation

References

1. Symmetries of Things, Appendix A, page 416 ↩

2. Frieze Patterns Mathematician John Conway created names that relate to footsteps for each of the frieze groups. https://www.maa.org/sites/default/files/images/upload_library/4/vol1/architecture/Math/seven.html ↩

3. Symmetries of Things, Appendix A, page 416 ↩

4. Symmetries of Things, Chapter 18, More on Hyperbolic groups, Enumerating hyperbolic groups, p239 ↩