In mathematics, a Coxeter group, named after H. S. M. Coxeter, is an abstract group that admits a formal description in terms of reflections (or kaleidoscopic mirrors). Indeed, the finite Coxeter groups are precisely the finite Euclidean reflection groups; for example, the symmetry group of each regular polyhedron is a finite Coxeter group. However, not all Coxeter groups are finite, and not all can be described in terms of symmetries and Euclidean reflections. Coxeter groups were introduced in 1934 as abstractions of reflection groups,[1] and finite Coxeter groups were classified in 1935.[2]
Coxeter groups find applications in many areas of mathematics. Examples of finite Coxeter groups include the symmetry groups of regular polytopes, and the Weyl groups of simple Lie algebras. Examples of infinite Coxeter groups include the triangle groups corresponding to regular tessellations of the Euclidean plane and the hyperbolic plane, and the Weyl groups of infinite-dimensional Kac–Moody algebras.[3] [4] [5]
Formally, a Coxeter group can be defined as a group with the presentation
\left\langler1,r2,\ldots,rn\mid(rir
mij | |
j) |
=1\right\rangle
where
mii=1
mij=mji\ge2
infty
i ≠ j
mi=infty
(rir
m | |
j) |
=1
m\ge2
The pair
(W,S)
W
S=\{r1,...,rn\}
S
W
B3
A1 x A3
A number of conclusions can be drawn immediately from the above definition.
mii=1
(rir
1 | |
i) |
=
2 | |
(r | |
i) |
=1
i
mij=2
ri
rj
xx=yy=1
together with
xyxy=1
implies that
xy=x(xyxy)y=(xx)yx(yy)=yx
Alternatively, since the generators are involutions,
ri=
-1 | |
r | |
i |
1=(rir
2=r | |
ir |
jrirj=rirjr
-1 | |
i |
-1 | |
r | |
j |
ri
rj
ri
rj
The reason that
mij=mji
i ≠ j
yy=1
(xy)m=1
(yx)m=(yx)myy=y(xy)my=yy=1
(xy)k
(yx)k
y(xy)ky-1=(yx)kyy-1=(yx)k
The Coxeter matrix is the
n x n
mij
\{2,3,\ldots\}\cup\{infty\}
The Coxeter matrix can be conveniently encoded by a Coxeter diagram, as per the following rules.
i
j
mij\geq3
mij
4
In particular, two generators commute if and only if they are not joined by an edge. Furthermore, if a Coxeter graph has two or more connected components, the associated group is the direct product of the groups associated to the individual components.Thus the disjoint union of Coxeter graphs yields a direct product of Coxeter groups.
The Coxeter matrix,
Mij
n x n
C
Cij=-2\cos(\pi/Mij)
Coxeter group | A1×A1 | A2 | B2 | I2(5) | G2 | {\tilde{A}}1=I2(infty) | A3 | B3 | D4 | {\tilde{A}}3 | |
---|---|---|---|---|---|---|---|---|---|---|---|
Coxeter diagram | |||||||||||
Coxeter matrix | \left[ \begin{smallmatrix} 1&2\\ 2&1\ \end{smallmatrix}\right] | \left[ \begin{smallmatrix} 1&3\\ 3&1\ \end{smallmatrix}\right] | \left[ \begin{smallmatrix} 1&4\\ 4&1\ \end{smallmatrix}\right] | \left[ \begin{smallmatrix} 1&5\\ 5&1\ \end{smallmatrix}\right] | \left[ \begin{smallmatrix} 1&6\\ 6&1\ \end{smallmatrix}\right] | \left[ \begin{smallmatrix} 1&infty\\ infty&1\ \end{smallmatrix}\right] | \left[ \begin{smallmatrix} 1&3&2\\ 3&1&3\\ 2&3&1\end{smallmatrix}\right] | \left[ \begin{smallmatrix} 1&4&2\\ 4&1&3\\ 2&3&1\end{smallmatrix}\right] | \left[ \begin{smallmatrix} 1&3&2&2\\ 3&1&3&3\\ 2&3&1&2\\ 2&3&2&1\end{smallmatrix}\right] | \left[ \begin{smallmatrix} 1&3&2&3\\ 3&1&3&2\\ 2&3&1&3\\ 3&2&3&1\end{smallmatrix}\right] | |
Schläfli matrix | \left[ \begin{smallmatrix} 2&0\\ 0&2\end{smallmatrix}\right] | \left[ \begin{smallmatrix} 2&-1\\ -1& 2\end{smallmatrix}\right] | \left[ \begin{smallmatrix} 2&-\sqrt2\\ -\sqrt2& 2\end{smallmatrix}\right] | \left[ \begin{smallmatrix} 2&-\phi\\ -\phi& 2\end{smallmatrix}\right] | \left[ \begin{smallmatrix} 2&-\sqrt3\\ -\sqrt3& 2\end{smallmatrix}\right] | \left[ \begin{smallmatrix} 2&-2\\ -2& 2\end{smallmatrix}\right] | \left[ \begin{smallmatrix} 2&-1& 0\\ -1& 2&-1\\ 0&-1& 2\end{smallmatrix}\right] | \left[ \begin{smallmatrix} 2&-\sqrt{2}& 0\\ -\sqrt{2}& 2&-1\\ 0& -1& 2\end{smallmatrix}\right] | \left[ \begin{smallmatrix} 2&-1& 0& 0\\ -1& 2&-1&-1\\ 0&-1& 2& 0\\ 0&-1& 0& 2\end{smallmatrix}\right] | \left[ \begin{smallmatrix} 2&-1& 0&-1\\ -1& 2&-1& 0\\ 0&-1& 2&-1\\ -1& 0&-1& 2\end{smallmatrix}\right] |
The graph
An
1
n
Sn+1
(1~~2),(2~~3),...,(n~~n+1)
(k~~k+1) ⋅ (k+1~~k+2)=(k~~k+2~~k+1)
Sn+1
An
Coxeter groups are an abstraction of reflection groups. Coxeter groups are abstract groups, in the sense of being given via a presentation. On the other hand, reflection groups are concrete, in the sense that each of its elements is the composite of finitely many geometric reflections about linear hyperplanes in some euclidean space. Technically, a reflection group is a subgroup of a linear group (or various generalizations) generated by orthogonal matrices of determinant -1. Each generator of a Coxeter group has order 2, which abstracts the geometric fact that performing a reflection twice is the identity. Each relation of the form
(rir
k | |
j) |
\pi/k
2\pi/k
In this way, every reflection group may be presented as a Coxeter group.[1] The converse is partially true: every finite Coxeter group admits a faithful representation as a finite reflection group of some Euclidean space.[2] However, not every infinite Coxeter group admits a representation as a reflection group.
Finite Coxeter groups have been classified.[2]
Finite Coxeter groups are classified in terms of their Coxeter diagrams.[2]
The finite Coxeter groups with connected Coxeter diagrams consist of three one-parameter families of increasing dimension (
An
n\geq1
Bn
n\geq2
Dn
n\geq4
I2(p)
p\geq5
E6,E7,E8,F4,H3,
H4
See main article: Weyl group. Many, but not all of these, are Weyl groups, and every Weyl group can be realized as a Coxeter group. The Weyl groups are the families
An,Bn,
Dn,
E6,E7,E8,F4,
I2(6),
G2.
The non-Weyl ones are the exceptions
H3
H4,
I2(p)
I2(3)\congA2,I2(4)\congB2,
I2(6)\congG2
This can be proven by comparing the restrictions on (undirected) Dynkin diagrams with the restrictions on Coxeter diagrams of finite groups: formally, the Coxeter graph can be obtained from the Dynkin diagram by discarding the direction of the edges, and replacing every double edge with an edge labelled 4 and every triple edge by an edge labelled 6. Also note that every finitely generated Coxeter group is an automatic group.[6] Dynkin diagrams have the additional restriction that the only permitted edge labels are 2, 3, 4, and 6, which yields the above. Geometrically, this corresponds to the crystallographic restriction theorem, and the fact that excluded polytopes do not fill space or tile the plane – for
H3,
H4,
I2(p)
p=3,4,
6
Note further that the (directed) Dynkin diagrams Bn and Cn give rise to the same Weyl group (hence Coxeter group), because they differ as directed graphs, but agree as undirected graphs – direction matters for root systems but not for the Weyl group; this corresponds to the hypercube and cross-polytope being different regular polytopes but having the same symmetry group.
Some properties of the finite irreducible Coxeter groups are given in the following table. The order of a reducible group can be computed by the product of its irreducible subgroup orders.
Rank n | Group symbol | Alternate symbol | Bracket notation | Coxeter graph | data-sort-type="number" | Reflections m = nh[7] | data-sort-type="number" | Coxeter number h | data-sort-type="number" | Group structure | Related polytopes | |||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
1 | A1 | A1 | [] | 1 | 2 | 2 | S2 | |||||||||||||||
2 | A2 | A2 | [3] | 3 | 3 | 6 | S3\congD6\cong
| |||||||||||||||
3 | A3 | A3 | [3,3] | 6 | 4 | 24 | S4 | |||||||||||||||
4 | A4 | A4 | [3,3,3] | 10 | 5 | 120 | S5 | |||||||||||||||
5 | A5 | A5 | [3,3,3,3] | 15 | 6 | 720 | S6 | |||||||||||||||
n | An | An | [3<sup>''n''−1</sup>] | ... | n(n + 1)/2 | n + 1 | (n + 1)! | Sn+1 | ||||||||||||||
2 | B2 | C2 | [4] | 4 | 4 | 8 | C2\wrS2\congD8\cong
| |||||||||||||||
3 | B3 | C3 | [4,3] | 9 | 6 | 48 | C2\wrS3\congS4 x 2 | |||||||||||||||
4 | B4 | C4 | [4,3,3] | 16 | 8 | 384 | C2\wrS4 | |||||||||||||||
5 | B5 | C5 | [4,3,3,3] | 25 | 10 | 3840 | C2\wrS5 | |||||||||||||||
n | Bn | Cn | [4,3<sup>''n''−2</sup>] | ... | n2 | 2n | 2n n! | C2\wrSn | ||||||||||||||
4 | D4 | B4 | [3<sup>1,1,1</sup>] | 12 | 6 | 192 |
S4\cong21+4\colonS3 | h / | ||||||||||||||
5 | D5 | B5 | [3<sup>2,1,1</sup>] | 20 | 8 | 1920 |
S5 | h / | ||||||||||||||
n | Dn | Bn | [3<sup>''n''−3,1,1</sup>] | ... | n(n − 1) | 2(n − 1) | 2n-1 n! |
Sn | n-demicube / n-orthoplex | |||||||||||||
6 | E6 | E6 | [3<sup>2,2,1</sup>] | 36 | 12 | 51840 (72x6!) |
(2)\cong\operatorname{SO}5(3)\cong\operatorname{PSp}4(3)\colon2\cong\operatorname{PSU}4(2)\colon2 | |||||||||||||||
7 | E7 | E7 | [3<sup>3,2,1</sup>] | 63 | 18 | 2903040 (72x8!) | \operatorname{GO}7(2) x 2\cong\operatorname{Sp}6(2) x 2 | |||||||||||||||
8 | E8 | E8 | [3<sup>4,2,1</sup>] | 120 | 30 | 696729600 (192x10!) |
(2) | |||||||||||||||
4 | F4 | F4 | [3,4,3] | 24 | 12 | 1152 |
21+4\colon(S3 x S3) | |||||||||||||||
2 | G2 | – (D) | [6] | 6 | 6 | 12 | D12\cong
| |||||||||||||||
2 | I2(5) | G2 | [5] | 5 | 5 | 10 | D10\cong
| |||||||||||||||
3 | H3 | G3 | [3,5] | 15 | 10 | 120 | 2 x A5 | |||||||||||||||
4 | H4 | G4 | [3,3,5] | 60 | 30 | 14400 | 2 ⋅ (A5 x A5)\colon2 | |||||||||||||||
2 | I2(n) | D | [''n''] | n | n | 2n | D2n \cong
\cong
|
The symmetry group of every regular polytope is a finite Coxeter group. Note that dual polytopes have the same symmetry group.
There are three series of regular polytopes in all dimensions. The symmetry group of a regular n-simplex is the symmetric group Sn+1, also known as the Coxeter group of type An. The symmetry group of the n-cube and its dual, the n-cross-polytope, is Bn, and is known as the hyperoctahedral group.
The exceptional regular polytopes in dimensions two, three, and four, correspond to other Coxeter groups. In two dimensions, the dihedral groups, which are the symmetry groups of regular polygons, form the series I2(p), for p ≥ 3. In three dimensions, the symmetry group of the regular dodecahedron and its dual, the regular icosahedron, is H3, known as the full icosahedral group. In four dimensions, there are three exceptional regular polytopes, the 24-cell, the 120-cell, and the 600-cell. The first has symmetry group F4, while the other two are dual and have symmetry group H4.
The Coxeter groups of type Dn, E6, E7, and E8 are the symmetry groups of certain semiregular polytopes.
See also: Affine root system.
The affine Coxeter groups form a second important series of Coxeter groups. These are not finite themselves, but each contains a normal abelian subgroup such that the corresponding quotient group is finite. In each case, the quotient group is itself a Coxeter group, and the Coxeter graph of the affine Coxeter group is obtained from the Coxeter graph of the quotient group by adding another vertex and one or two additional edges. For example, for n ≥ 2, the graph consisting of n+1 vertices in a circle is obtained from An in this way, and the corresponding Coxeter group is the affine Weyl group of An (the affine symmetric group). For n = 2, this can be pictured as a subgroup of the symmetry group of the standard tiling of the plane by equilateral triangles.
In general, given a root system, one can construct the associated Stiefel diagram, consisting of the hyperplanes orthogonal to the roots along with certain translates of these hyperplanes. The affine Coxeter group (or affine Weyl group) is then the group generated by the (affine) reflections about all the hyperplanes in the diagram.[8] The Stiefel diagram divides the plane into infinitely many connected components called alcoves, and the affine Coxeter group acts freely and transitively on the alcoves, just as the ordinary Weyl group acts freely and transitively on the Weyl chambers. The figure at right illustrates the Stiefel diagram for the
G2
Suppose
R
r>1
\alpha1,\ldots,\alphar
\alphar+1
\alpha1,\ldots,\alphar
\alphar+1
R
\alphar+1
\alphar+1
A list of the affine Coxeter groups follows:
Group symbol | Witt symbol | Bracket notation | Coxeter graph | Related uniform tessellation(s) | |
---|---|---|---|---|---|
{\tilde{A}}n | Pn+1 | [3<sup>[''n'']] | ... or ... | Simplectic honeycomb | |
{\tilde{B}}n | Sn+1 | [4,3<sup>''n'' − 3</sup>,3<sup>1,1</sup>] | ... | Demihypercubic honeycomb | |
{\tilde{C}}n | Rn+1 | [4,3<sup>''n''−2</sup>,4] | ... | Hypercubic honeycomb | |
{\tilde{D}}n | Qn+1 | [3<sup>1,1</sup>,3<sup>''n''−4</sup>,3<sup>1,1</sup>] | ... | Demihypercubic honeycomb | |
{\tilde{E}}6 | T7 | [3<sup>2,2,2</sup>] | or | 222 | |
{\tilde{E}}7 | T8 | [3<sup>3,3,1</sup>] | or | 331, 133 | |
{\tilde{E}}8 | T9 | [3<sup>5,2,1</sup>] | 521, 251, 152 | ||
{\tilde{F}}4 | U5 | [3,4,3,3] | 16-cell honeycomb 24-cell honeycomb | ||
{\tilde{G}}2 | V3 | [6,3] | Hexagonal tiling and Triangular tiling | ||
{\tilde{A}}1=I2(infty) | W2 | [∞] | Apeirogon |
The group symbol subscript is one less than the number of nodes in each case, since each of these groups was obtained by adding a node to a finite group's graph.
There are infinitely many hyperbolic Coxeter groups describing reflection groups in hyperbolic space, notably including the hyperbolic triangle groups.
A Coxeter group is said to be irreducible if its Coxeter–Dynkin diagram is connected. Every Coxeter group is the direct product of the irreducible groups that correspond to the components of its Coxeter–Dynkin diagram.
A choice of reflection generators gives rise to a length function ℓ on a Coxeter group, namely the minimum number of uses of generators required to express a group element; this is precisely the length in the word metric in the Cayley graph. An expression for v using ℓ(v) generators is a reduced word. For example, the permutation (13) in S3 has two reduced words, (12)(23)(12) and (23)(12)(23). The function
v\to(-1)\ell(v)
G\to\{\pm1\},
Using reduced words one may define three partial orders on the Coxeter group, the (right) weak order, the absolute order and the Bruhat order (named for François Bruhat). An element v exceeds an element u in the Bruhat order if some (or equivalently, any) reduced word for v contains a reduced word for u as a substring, where some letters (in any position) are dropped. In the weak order, v ≥ u if some reduced word for v contains a reduced word for u as an initial segment. Indeed, the word length makes this into a graded poset. The Hasse diagrams corresponding to these orders are objects of study, and are related to the Cayley graph determined by the generators. The absolute order is defined analogously to the weak order, but with generating set/alphabet consisting of all conjugates of the Coxeter generators.
For example, the permutation (1 2 3) in S3 has only one reduced word, (12)(23), so covers (12) and (23) in the Bruhat order but only covers (12) in the weak order.
Since a Coxeter group
W
Z2
W
M(W)
W
\{Wn\}
M(Wn)
n
2 | |
r | |
i |
=(rirj
kij | |
) |
=1