In
mathematics, the Coxeter number ''h'' is the
order
Order, ORDER or Orders may refer to:
* Categorization, the process in which ideas and objects are recognized, differentiated, and understood
* Heterarchy, a system of organization wherein the elements have the potential to be ranked a number of d ...
of a Coxeter element of an irreducible
Coxeter group. It is named after
H.S.M. Coxeter
Harold Scott MacDonald "Donald" Coxeter, (9 February 1907 – 31 March 2003) was a British and later also Canadian geometer. He is regarded as one of the greatest geometers of the 20th century.
Biography
Coxeter was born in Kensington t ...
.
Definitions
Note that this article assumes a finite Coxeter group. For infinite Coxeter groups, there are multiple
conjugacy classes of Coxeter elements, and they have infinite order.
There are many different ways to define the Coxeter number ''h'' of an irreducible root system.
A Coxeter element is a product of all simple reflections. The product depends on the order in which they are taken, but different orderings produce
conjugate elements, which have the same
order
Order, ORDER or Orders may refer to:
* Categorization, the process in which ideas and objects are recognized, differentiated, and understood
* Heterarchy, a system of organization wherein the elements have the potential to be ranked a number of d ...
.
*The Coxeter number is the order of any Coxeter element;.
*The Coxeter number is 2''m''/''n'', where ''n'' is the rank, and ''m'' is the number of reflections. In the crystallographic case, ''m'' is half the number of
roots; and ''2m''+''n'' is the dimension of the corresponding semisimple
Lie algebra
In mathematics, a Lie algebra (pronounced ) is a vector space \mathfrak g together with an operation called the Lie bracket, an alternating bilinear map \mathfrak g \times \mathfrak g \rightarrow \mathfrak g, that satisfies the Jacobi iden ...
.
*If the highest root is Σ''m''
iα
''i'' for simple roots α
''i'', then the Coxeter number is 1 + Σ''m''
i.
*The Coxeter number is the highest degree of a fundamental invariant of the Coxeter group acting on polynomials.
The Coxeter number for each Dynkin type is given in the following table:
The invariants of the Coxeter group acting on polynomials form a polynomial algebra
whose generators are the fundamental invariants; their degrees are given in the table above.
Notice that if ''m'' is a degree of a fundamental invariant then so is ''h'' + 2 − ''m''.
The eigenvalues of a Coxeter element are the numbers ''e''
2π''i''(''m'' − 1)/''h'' as ''m'' runs through the degrees of the fundamental invariants. Since this starts with ''m'' = 2, these include the
primitive ''h''th root of unity, ''ζ
h'' = ''e''
2π''i''/''h'', which is important in the
Coxeter plane, below.
Group order
There are relations between the order ''g'' of the Coxeter group and the Coxeter number ''h'':
*
2h/g
p = 1
*
,q 8/g
p,q = 2/p + 2/q -1
*
,q,r 64h/g
p,q,r = 12 - p - 2q - r + 4/p + 4/r
*
,q,r,s 16/g
p,q,r,s = 8/g
p,q,r + 8/g
q,r,s + 2/(ps) - 1/p - 1/q - 1/r - 1/s +1
* ...
For example,
,3,5has ''h''=30, so 64*30/g = 12 - 3 - 6 - 5 + 4/3 + 4/5 = 2/15, so g = 1920*15/2 = 960*15 = 14400.
Coxeter elements
Distinct Coxeter elements correspond to orientations of the Coxeter diagram (i.e. to Dynkin
quivers): the simple reflections corresponding to source vertices are written first, downstream vertices later, and sinks last. (The choice of order among non-adjacent vertices is irrelevant, since they correspond to commuting reflections.) A special choice is the alternating orientation, in which the simple reflections are partitioned into two sets of non-adjacent vertices, and all edges are oriented from the first to the second set. The alternating orientation produces a special Coxeter element ''w'' satisfying
, where ''w''
0 is the
longest element, provided the Coxeter number ''h'' is even.
For
, the
symmetric group
In abstract algebra, the symmetric group defined over any set is the group whose elements are all the bijections from the set to itself, and whose group operation is the composition of functions. In particular, the finite symmetric group ...
on ''n'' elements, Coxeter elements are certain ''n''-cycles:
the product of simple reflections
is the Coxeter element
. For ''n'' even, the alternating orientation Coxeter element is:
:
There are
distinct Coxeter elements among the
''n''-cycles.
The
dihedral group Dih
''p'' is generated by two reflections that form an angle of
, and thus the two Coxeter elements are their product in either order, which is a rotation by
.
Coxeter plane

For a given Coxeter element ''w,'' there is a unique plane ''P'' on which ''w'' acts by rotation by 2π/''h.'' This is called the Coxeter plane and is the plane on which ''P'' has eigenvalues ''e''
2π''i''/''h'' and ''e''
−2π''i''/''h'' = ''e''
2π''i''(''h''−1)/''h''. This plane was first systematically studied in ,
and subsequently used in to provide uniform proofs about properties of Coxeter elements.
The Coxeter plane is often used to draw diagrams of higher-dimensional polytopes and root systems – the vertices and edges of the polytope, or roots (and some edges connecting these) are
orthogonally projected onto the Coxeter plane, yielding a
Petrie polygon with ''h''-fold rotational symmetry.
For root systems, no root maps to zero, corresponding to the Coxeter element not fixing any root or rather axis (not having eigenvalue 1 or −1), so the projections of orbits under ''w'' form ''h''-fold circular arrangements
and there is an empty center, as in the E
8 diagram at above right. For polytopes, a vertex may map to zero, as depicted below. Projections onto the Coxeter plane are depicted below for the
Platonic solids.
In three dimensions, the symmetry of a
regular polyhedron, , with one directed Petrie polygon marked, defined as a composite of 3 reflections, has
rotoinversion symmetry S
h,
+,h+">+,h+ order ''h''. Adding a mirror, the symmetry can be doubled to antiprismatic symmetry, D
hd,
+,h">+,h order 2''h''. In orthogonal 2D projection, this becomes
dihedral symmetry, Dih
''h'',
order 2''h''.
In four dimensions, the symmetry of a
regular polychoron, , with one directed Petrie polygon marked is a
double rotation, defined as a composite of 4 reflections, with symmetry +
1/
h h×Ch">h×Ch(
John H. Conway), (C
2h/C
1;C
2h/C
1) (#1',
Patrick du Val (1964)
[Patrick Du Val, ''Homographies, quaternions and rotations'', Oxford Mathematical Monographs, Clarendon Press, ]Oxford
Oxford () is a city in England. It is the county town and only city of Oxfordshire. In 2020, its population was estimated at 151,584. It is north-west of London, south-east of Birmingham and north-east of Bristol. The city is home to the Un ...
, 1964.), order ''h''.
In five dimensions, the symmetry of a
regular 5-polytope, , with one directed Petrie polygon marked, is represented by the composite of 5 reflections.
In dimensions 6 to 8 there are 3 exceptional Coxeter groups; one uniform polytope from each dimension represents the roots of the exceptional Lie groups E
n. The Coxeter elements are 12, 18 and 30 respectively.
See also
*
Longest element of a Coxeter group
Notes
References
*
*
*Hiller, Howard ''Geometry of Coxeter groups.'' Research Notes in Mathematics, 54. Pitman (Advanced Publishing Program), Boston, Mass.-London, 1982. iv+213 pp.
*
*
*
*
*Bernšteĭn, I. N.; Gelʹfand, I. M.; Ponomarev, V. A., "Coxeter functors, and Gabriel's theorem" (Russian), ''Uspekhi Mat. Nauk'' 28 (1973), no. 2(170), 19–33
Translation on Bernstein's website
{{refend
Lie groups
Coxeter groups