Orbifold notation
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In geometry, orbifold notation (or orbifold signature) is a system popularized by the mathematician John Horton Conway for representing types of symmetry groups in two-dimensional spaces of constant curvature. The advantage of the notation is that it describes these groups in a way which indicates many of the groups' properties: in particular, it describes the orbifold obtained by taking the quotient of Euclidean space by the group under consideration.
Groups representable in this notation include the wallpaper groups and frieze groups on the Euclidean plane (E2), the groups on the sphere (S2), and their analogues on the hyperbolic plane (H2).
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[edit] 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

- the infinity symbol,

- the asterisk, *
- the symbol o, which is called a wonder
- the symbol x, which is called a miracle
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 point
- an integer n to the right of an asterisk indicates a transformation of order 2n which rotates around a point and reflects through a line (or plane)
- an x indicates a glide reflection
- the symbol
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.
[edit] 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.
[edit] 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 after an asterisk counts as

- asterisk and x 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.
[edit] 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.
[edit] Other objects
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 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 11, *11,
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.
[edit] Correspondence tables
The 17 plane wallpaper symmetry groups:[1]
| Orbifold Signature |
International notation Coxeter and Moses |
Speiser Niggli |
Polya Guggenhein |
Fejes Toth Cadwell |
|---|---|---|---|---|
| *632 | p6m | C(I)6v | D6 | W16 |
| 632 | p6 | C(I)6 | C6 | W6 |
| *442 | p4m | C(I)4 | D*4 | W14 |
| 4*2 | p4g | CII4v | Do4 | W24 |
| 442 | p4 | C(I)4 | C4 | W4 |
| *333 | p3m1 | CII3v | D*3 | W13 |
| 3*3 | p31m | CI3v | Do4 | W23 |
| 333 | p3 | CI3 | C3 | W3 |
| *2222 | pmm | CI2v | D2kkkk | W22 |
| 2*22 | cmm | CIV2v | D2kgkg | W12 |
| 22* | pmg | CIII2v | D2kkgg | W32 |
| 22x | pgg | CII2v | D2gggg | W42 |
| 2222 | p2 | C(I)2 | C2 | W2 |
| ** | pm | CIs | D1kk | W21 |
| *x | cm | CIIIs | D1kg | W11 |
| xx | pg | CII2 | D1gg | W31 |
| o | p1 | C(I)1 | C1 | W1 |
The spherical symmetry groups: (N=1,2,3,..)[2]
| Orbifold Signature |
Coxeter | Schönflies | Weyl | Pólya and Meyer | International notation |
|---|---|---|---|---|---|
| *532 | [3,5] | Ih | 53m | ||
| 532 | [3,5]+ | I | 532 | ||
| *432 | [3,4] | Oh | m3m | ||
| 432 | [3,4]+ | O | 432 | ||
| *332 | [3,3] | Td | 4-3m | ||
| 3*2 | [3+,4] | Th | m3 | ||
| 332 | [3,3]+ | T | 23 | ||
| *22N | [2,N] | DNh | N/mmm or 2N-m2 | ||
| 2*N | [2+,2N] | DNd | 2N-2m or N-m | ||
| 22N | [2,N]+ | DN | N2 | ||
| *NN | [N] | CNv | Nm | ||
| N* | [2,N+] | CNh | N/m or 2N- | ||
| Nx | [2+,2N+] | S2N | 2N- or N- | ||
| NN | [N]+ | CN | N |
[edit] 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)
[edit] See also
[edit] References
- 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-Strass, The Symmetry of Things 2008, ISBN 978-1-56881-220-5

