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]
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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.
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 e2πi(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 = e2πi/h, which is important in the Coxeter plane, below.
Coxeter elements of , considered as the symmetric group on n elements, are n-cycles: for simple reflections the adjacent transpositions , a Coxeter element is the n-cycle .[2]
The dihedral group Dihm is generated by two reflections that form an angle of , and thus their product is a rotation by .
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 e2πi/h and e−2πi/h = e2πi(h−1)/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.