Coxeter element

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In mathematics, the Coxeter number h is the order of a Coxeter element of an irreducible Coxeter group, hence also of a root system or its Weyl group. It is named after H.S.M. Coxeter.[1]

Definitions

Warning: 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.

  • The Coxeter number is the number of roots divided by the rank.
  • The Coxeter number is the order of a Coxeter element; note that conjugate elements have the same order.
  • If the highest root is ∑miαi for simple roots αi, then the Coxeter number is 1 + mi
  • The dimension of the corresponding Lie algebra is n(h + 1), where n is the rank and h is the Coxeter number.
  • The Coxeter number is the highest degree of a fundamental invariant of the Weyl group acting on polynomials.
  • The Coxeter number is given by the following table:
Coxeter group Coxeter number h Dual Coxeter number Degrees of fundamental invariants
An ... n + 1 n + 1 2, 3, 4, ..., n + 1
Bn ... 2n 2n 1 2, 4, 6, ..., 2n
Cn n + 1
Dn ... 2n 2 2n 2 n; 2, 4, 6, ..., 2n 2
E6 12 12 2, 5, 6, 8, 9, 12
E7 18 18 2, 6, 8, 10, 12, 14, 18
E8 30 30 2, 8, 12, 14, 18, 20, 24, 30
F4 12 9 2, 6, 8, 12
G2 = I2(6) 6 4 2, 6
H3 10 2, 6, 10
H4 30 2, 12, 20, 30
I2(p) p 2, p

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 ei(m  1)/h as m runs through the degrees of the fundamental invariants. Since this starts with m = 2, these include the primitive hth root of unity, ζh = ei/h, which is important in the Coxeter plane, below.

Coxeter elements

Coxeter elements of A_{{n-1}}\cong S_{n}, considered as the symmetric group on n elements, are n-cycles: for simple reflections the adjacent transpositions (1,2),(2,3),\dots , a Coxeter element is the n-cycle (1,2,3,\dots ,n).[2]

The dihedral group Dihm is generated by two reflections that form an angle of 2\pi /2m, and thus their product is a rotation by 2\pi /m.

Coxeter plane

Projection of E8 root system onto Coxeter plane, showing 30-fold symmetry.

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 ei/h and ei/h = ei(h1)/h.[3] This plane was first systematically studied in (Coxeter 1948),[4] and subsequently used in (Steinberg 1959) to provide uniform proofs about properties of Coxeter elements.[4]

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.[5] 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[5] and there is an empty center, as in the E8 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.

See also

Notes

  1. Coxeter, Harold Scott Macdonald; Chandler Davis, Erlich W. Ellers (2006), The Coxeter Legacy: Reflections and Projections, AMS Bookstore, p. 112, ISBN 978-0-8218-3722-1 
  2. (Humphreys 1992, p. 75)
  3. (Humphreys 1992, Section 3.17, "Action on a Plane", pp. 76–78)
  4. 4.0 4.1 (Reading 2010, p. 2)
  5. 5.0 5.1 (Stembridge 2007)

References

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