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A Coxeter system is a group G with
finite generating set S={s1, ..., sn}, defined by the power relations
si2=1 for i=1, ..., n and braid relations
sisjsi ... = sjsisj ... for i, j=1, ..., n with i<j, where each side of this relation has
length mij≥2.
Although traditionally mij=∞ signifies that the corresponding relation
is omitted, for technical reasons, we use mij=0 instead.
Set mji=mij and mii=1. The group G is called a Coxeter
group and S is
called the set of Coxeter generators.
Since every group in Magma has a preferred generating set, no distinction is
made between a Coxeter system and its Coxeter group.
Due to the importance and ubiquity of Coxeter groups, a number of different
ways of describing these groups and their reflections have been developed.
Functions for manipulating these descriptions are described in
Chapter COXETER SYSTEMS.
Coxeter groups are usually described by a Coxeter matrix
M=(mij)i, j=1n, or by a Coxeter graph with vertices 1, ..., n and
an edge connecting i and j labeled by mij whenever
mij≥3.
Coxeter systems are mainly important because they provide presentations for the
real reflection groups. A Cartan matrix describes a particular reflection
representation of a Coxeter group. In certain cases, such a representation can
be described by an integer-labelled digraph, called the Dynkin digraph
(this is equivalent to a Dynkin diagram, but we have modified the
definition for technical reasons).
For finite and affine Coxeter groups, the naming system due to Cartan is also
used. Hyperbolic Coxeter groups of degree larger than 3 are numbered.
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