Configuration (geometry)

In mathematics, specifically projective geometry, a configuration in the plane consists of a finite set of points, and a finite arrangement of lines, such that each point is incident to the same number of lines and each line is incident to the same number of points.[1]

Configurations (4₃6₂) (a complete quadrangle, at left) and (6₂4₃) (a complete quadrilateral, at right).

Although certain specific configurations had been studied earlier (for instance by Thomas Kirkman in 1849), the formal study of configurations was first introduced by Theodor Reye in 1876, in the second edition of his book Geometrie der Lage, in the context of a discussion of Desargues' theorem. Ernst Steinitz wrote his dissertation on the subject in 1894, and they were popularized by Hilbert and Cohn-Vossen's 1932 book Anschauliche Geometrie, reprinted in English as Hilbert & Cohn-Vossen (1952).

Configurations may be studied either as concrete sets of points and lines in a specific geometry, such as the Euclidean or projective planes (these are said to be realizable in that geometry), or as a type of abstract incidence geometry. In the latter case they are closely related to regular hypergraphs and biregular bipartite graphs, but with some additional restrictions: every two points of the incidence structure can be associated with at most one line, and every two lines can be associated with at most one point. That is, the girth of the corresponding bipartite graph (the Levi graph of the configuration) must be at least six.

Notation

A configuration in the plane is denoted by ( $p γ ℓ π$ ), where $p$ is the number of points, $ℓ$ the number of lines, $γ$ the number of lines per point, and $π$ the number of points per line. These numbers necessarily satisfy the equation

p\gamma =\ell \pi \,

as this product is the number of point-line incidences (flags).

Configurations having the same symbol, say ( $p γ ℓ π$ ), need not be isomorphic as incidence structures. For instance, there exist three different (9₃ 9₃) configurations: the Pappus configuration and two less notable configurations.

In some configurations, $p = ℓ$ and consequently, $γ = π$ . These are called symmetric or balanced configurations[2] and the notation is often condensed to avoid repetition. For example, (9₃ 9₃) abbreviates to (9₃).

Examples

A (10₃) configuration that is not incidence-isomorphic to a Desargues configuration

Notable projective configurations include the following:

(1₁), the simplest possible configuration, consisting of a point incident to a line. Often excluded as being trivial.
(3₂), the triangle. Each of its three sides meets two of its three vertices, and vice versa. More generally any polygon of $n$ sides forms a configuration of type ( $n 2$ )
(4₃ 6₂) and (6₂ 4₃), the complete quadrangle and complete quadrilateral respectively.
(7₃), the Fano plane. This configuration exists as an abstract incidence geometry, but cannot be constructed in the Euclidean plane.
(8₃), the Möbius–Kantor configuration. This configuration describes two quadrilaterals that are simultaneously inscribed and circumscribed in each other. It cannot be constructed in Euclidean plane geometry but the equations defining it have nontrivial solutions in complex numbers.
(9₃), the Pappus configuration.
(9₄ 12₃), the Hesse configuration of nine inflection points of a cubic curve in the complex projective plane and the twelve lines determined by pairs of these points. This configuration shares with the Fano plane the property that it contains every line through its points; configurations with this property are known as Sylvester–Gallai configurations due to the Sylvester–Gallai theorem that shows that they cannot be given real-number coordinates.[3]
(10₃), the Desargues configuration.
(12₄ 16₃), the Reye configuration.
(12₅ 30₂), the Schläfli double six, formed by 12 of the 27 lines on a cubic surface
(15₃), the Cremona–Richmond configuration, formed by the 15 lines complementary to a double six and their 15 tangent planes
(16₆), the Kummer configuration.
(21₄), the Grünbaum–Rigby configuration.
(27₃), the Gray configuration
(35₄), Danzer's configuration.[4]
(60₁₅), the Klein configuration.

Duality of configurations

The projective dual of a configuration ( $p γ ℓ π$ ) is a ( $ℓ π p γ$ ) configuration in which the roles of "point" and "line" are exchanged. Types of configurations therefore come in dual pairs, except when taking the dual results in an isomorphic configuration. These exceptions are called self-dual configurations and in such cases $p = ℓ$ .[5]

The number of ( $n 3$ ) configurations

The number of nonisomorphic configurations of type ( $n 3$ ), starting at $n = 7$ , is given by the sequence

1, 1, 3, 10, 31, 229, 2036, 21399, 245342, ... (sequence A001403 in the OEIS)

These numbers count configurations as abstract incidence structures, regardless of realizability.[6] As Gropp (1997) discusses, nine of the ten (10₃) configurations, and all of the (11₃) and (12₃) configurations, are realizable in the Euclidean plane, but for each $n \geq 16$ there is at least one nonrealizable ( $n 3$ ) configuration. Gropp also points out a long-lasting error in this sequence: an 1895 paper attempted to list all (12₃) configurations, and found 228 of them, but the 229th configuration, the Gropp configuration, was not discovered until 1988.

Constructions of symmetric configurations

There are several techniques for constructing configurations, generally starting from known configurations. Some of the simplest of these techniques construct symmetric ( $p γ$ ) configurations.

Any finite projective plane of order $n$ is an (( $n 2 + n + 1) n + 1)$ configuration. Let $Π$ be a projective plane of order $n$ . Remove from $Π$ a point $P$ and all the lines of $Π$ which pass through $P$ (but not the points which lie on those lines except for $P$ ) and remove a line $ℓ$ not passing through $P$ and all the points that are on line $ℓ$ . The result is a configuration of type (( $n 2 - 1) n)$ . If, in this construction, the line $ℓ$ is chosen to be a line which does pass through $P$ , then the construction results in a configuration of type (( $n 2) n)$ . Since projective planes are known to exist for all orders $n$ which are powers of primes, these constructions provide infinite families of symmetric configurations.

Not all configurations are realizable, for instance, a (43₇) configuration does not exist.[7] However, Gropp (1990) has provided a construction which shows that for $k \geq 3$ , a ( $p k$ ) configuration exists for all $p \geq 2 ℓ k + 1$ , where $ℓ k$ is the length of an optimal Golomb ruler of order $k$ .

Unconventional configurations

Higher dimensions

The Schläfli double six.

The concept of a configuration may be generalized to higher dimensions,[8] for instance to points and lines or planes in space. In such cases, the restrictions that no two points belong to more than one line may be relaxed, because it is possible for two points to belong to more than one plane.

Notable three-dimensional configurations are the Möbius configuration, consisting of two mutually inscribed tetrahedra, Reye's configuration, consisting of twelve points and twelve planes, with six points per plane and six planes per point, the Gray configuration consisting of a 3×3×3 grid of 27 points and the 27 orthogonal lines through them, and the Schläfli double six, a configuration with 30 points, 12 lines, two lines per point, and five points per line.

Topological configurations

Configuration in the projective plane that is realized by points and pseudolines is called topological configuration.[2] For instance, it is known that there exists no point-line (19₄) configurations, however, there exists a topological configuration with these parameters.

Configurations of points and circles

Another generalization of the concept of a configuration concerns configurations of points and circles, a notable example being the (8₃ 6₄) Miquel configuration.[2]

Notes

In the literature, the terms projective configuration (Hilbert & Cohn-Vossen 1952) and tactical configuration of type (1,1) (Dembowski 1968) are also used to describe configurations as defined here.
Grünbaum 2009.
Kelly 1986.
Grünbaum 2008, Boben, Gévay & Pisanski 2015
Coxeter 1999, pp. 106–149
Betten, Brinkmann & Pisanski 2000.
This configuration would be a projective plane of order 6 which does not exist by the Bruck–Ryser theorem.
Gévay 2014.

References

Berman, Leah W., "Movable (n₄) configurations", The Electronic Journal of Combinatorics, 13 (1): R104.
Betten, A; Brinkmann, G.; Pisanski, T. (2000), "Counting symmetric configurations", Discrete Applied Mathematics, 99 (1–3): 331–338, doi:10.1016/S0166-218X(99)00143-2.
Boben, Marko; Gévay, Gábor; Pisanski, T. (2015), "Danzer's configuration revisited", Advances in Geometry, 15 (4): 393–408.
Coxeter, H.S.M. (1999), "Self-dual configurations and regular graphs", The Beauty of Geometry, Dover, ISBN 0-486-40919-8
Dembowski, Peter (1968), Finite geometries, Ergebnisse der Mathematik und ihrer Grenzgebiete, Band 44, Berlin, New York: Springer-Verlag, ISBN 3-540-61786-8, MR 0233275
Gévay, Gábor (2014), "Constructions for large point-line (n_k) configurations", Ars Mathematica Contemporanea, 7: 175-199.
Gropp, Harald (1990), "On the existence and non-existence of configurations n_k", Journal of Combinatorics and Information System Science, 15: 34–48
Gropp, Harald (1997), "Configurations and their realization", Discrete Mathematics, 174 (1–3): 137–151, doi:10.1016/S0012-365X(96)00327-5.
Grünbaum, Branko (2006), "Configurations of points and lines", in Davis, Chandler; Ellers, Erich W. (eds.), The Coxeter Legacy: Reflections and Projections, American Mathematical Society, pp. 179–225.
Grünbaum, Branko (2008), "Musing on an example of Danzer's", European Journal of Combinatorics, 29: 1910-1918.
Grünbaum, Branko (2009), Configurations of Points and Lines, Graduate Studies in Mathematics, vol. 103, American Mathematical Society, ISBN 978-0-8218-4308-6.
Hilbert, David; Cohn-Vossen, Stephan (1952), Geometry and the Imagination (2nd ed.), Chelsea, pp. 94–170, ISBN 0-8284-1087-9.
Kelly, L. M. (1986), "A resolution of the Sylvester–Gallai problem of J. P. Serre", Discrete and Computational Geometry, 1 (1): 101–104, doi:10.1007/BF02187687.
Pisanski, Tomaž; Servatius, Brigitte (2013), Configurations from a Graphical Viewpoint, Springer, ISBN 9780817683641.

External links

Weisstein, Eric W., "Configuration", MathWorld

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[1] In the literature, the terms projective configuration (Hilbert & Cohn-Vossen 1952) and tactical configuration of type (1,1) (Dembowski 1968) are also used to describe configurations as defined here.

[FOOTNOTEGrünbaum2009-2] Grünbaum 2009.

[FOOTNOTEKelly1986-3] Kelly 1986.

[4] Grünbaum 2008, Boben, Gévay & Pisanski 2015

[5] Coxeter 1999, pp. 106–149

[FOOTNOTEBettenBrinkmannPisanski2000-6] Betten, Brinkmann & Pisanski 2000.

[7] This configuration would be a projective plane of order 6 which does not exist by the Bruck–Ryser theorem.

[FOOTNOTEGévay2014-8] Gévay 2014.