Generalized polygon

In combinatorial theory, a generalized polygon is an incidence structure introduced by Jacques Tits. Generalized polygons encompass as special cases projective planes (generalized triangles, n = 3) and generalized quadrangles (n = 4), which form the most complex kinds of axiomatic projective and polar spaces. Many generalized polygons arise from groups of Lie type, but there are also exotic ones that cannot be obtained in this way. Generalized polygons satisfying a technical condition known as the Moufang property have been completely classified by Tits and Weiss.

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Definition

A generalized polygon is an incidence structure (P,L,I), where P is the set of points, L is the set of lines and I\subseteq P\times L is the incidence relation, satisfying certain regularity conditions. In order to express them, consider the bipartite incidence graph with the vertex set P ∪ L and the edges connecting the incident pairs of points and lines.

This condition is frequently stated as follows: any pair consisting of a point and a line is contained in an ordinary n-gon and there are no ordinary k-gons for k < n. When it is important to specify the diameter, a generalized polygon of diameter n is called a generalized n-gon, and the normal names for small polygons are used.

A generalized polygon is of order (s,t) if:

We say a generalized polygon is thick if every point (line) is incident with at least three lines (points). All thick generalized polygons have an order.

The dual of a generalized n-gon (P,L,I) is the incidence structure (P,L,I-1), which is again a generalized n-gon.

Examples

Feit-Higman theorem

Walter Feit and Graham Higman proved that finite generalized n-gons with s ≥ 2, t ≥ 2 can exist only for the following values of n:

2, 3, 4, 6 or 8.

Moreover,

If s and t are both infinite then generalized polygons exist for each n greater or equal to 2. It is unknown whether or not there exist generalized polygons with one of the parameters finite and the other infinite (these cases are called semi-finite).

See also

References