Incidence structure
Example 1: points and lines of the Euclidean plane (top)
Example 2: points and circles (middle),
Example 3: finite incidence structure defined by an incidence matrix (bottom)
In mathematics, an incidence structure is an abstract system consisting of two types of objects and a single relationship between these types of objects. Consider the points and lines of the Euclidean plane as the two types of objects and ignore all the properties of this geometry except for the relation of which points are incident on which lines for all points and lines. What is left is the incidence structure of the Euclidean plane.
Incidence structures are most often considered in the geometrical context where they are abstracted from, and hence generalize, planes (such as affine, projective, and Möbius planes), but the concept is very broad and not limited to geometric settings. Even in a geometric setting, incidence structures are not limited to just points and lines; higher-dimensional objects (planes, solids, Template:Mvar-spaces, conics, etc.) can be used. The study of finite structures is sometimes called finite geometry.<ref>Template:Harvnb</ref>
Formal definition and terminologyEdit
An incidence structure is a triple (Template:Math) where Template:Mvar is a set whose elements are called points, Template:Mvar is a distinct set whose elements are called lines and Template:Math is the incidence relation. The elements of Template:Mvar are called flags. If (Template:Math) is in Template:Mvar then one may say that point Template:Mvar "lies on" line Template:Mvar or that the line Template:Mvar "passes through" point Template:Mvar. A more "symmetric" terminology, to reflect the symmetric nature of this relation, is that "Template:Mvar is incident with Template:Mvar" or that "Template:Mvar is incident with Template:Mvar" and uses the notation Template:Math synonymously with Template:Math.<ref name=Demb1>Template:Harvnb</ref>
In some common situations Template:Mvar may be a set of subsets of Template:Mvar in which case incidence Template:Mvar will be containment (Template:Math if and only if Template:Mvar is a member of Template:Mvar). Incidence structures of this type are called set-theoretic.<ref>Template:Harvnb</ref> This is not always the case, for example, if Template:Mvar is a set of vectors and Template:Mvar a set of square matrices, we may define <math display=block>I = \{(v, M) : \vec v \text{ is an eigenvector of matrix } M \}.</math> This example also shows that while the geometric language of points and lines is used, the object types need not be these geometric objects.
ExamplesEdit
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An incidence structure is uniform if each line is incident with the same number of points. Each of these examples, except the second, is uniform with three points per line.
GraphsEdit
Any graph (which need not be simple; loops and multiple edges are allowed) is a uniform incidence structure with two points per line. For these examples, the vertices of the graph form the point set, the edges of the graph form the line set, and incidence means that a vertex is an endpoint of an edge.
Linear spacesEdit
Incidence structures are seldom studied in their full generality; it is typical to study incidence structures that satisfy some additional axioms. For instance, a partial linear space is an incidence structure that satisfies:
- Any two distinct points are incident with at most one common line, and
- Every line is incident with at least two points.
If the first axiom above is replaced by the stronger:
- Any two distinct points are incident with exactly one common line,
the incidence structure is called a linear space.<ref>The term linear space is also used to refer to vector spaces, but this will rarely cause confusion.</ref><ref>Template:Harvnb</ref>
NetsEdit
A more specialized example is a Template:Mvar-net. This is an incidence structure in which the lines fall into Template:Mvar parallel classes, so that two lines in the same parallel class have no common points, but two lines in different classes have exactly one common point, and each point belongs to exactly one line from each parallel class. An example of a Template:Mvar-net is the set of points of an affine plane together with Template:Mvar parallel classes of affine lines.
Dual structureEdit
If we interchange the role of "points" and "lines" in <math display="block">C = (P, L, I)</math> we obtain the dual structure, <math display="block">C^* = (L, P, I^*)</math> where Template:Math is the converse relation of Template:Mvar. It follows immediately from the definition that: <math display="block">C^{**} = C</math>
This is an abstract version of projective duality.<ref name=Demb1 />
A structure Template:Mvar that is isomorphic to its dual Template:Math is called self-dual. The Fano plane above is a self-dual incidence structure.
Other terminologyEdit
The concept of an incidence structure is very simple and has arisen in several disciplines, each introducing its own vocabulary and specifying the types of questions that are typically asked about these structures. Incidence structures use a geometric terminology, but in graph theoretic terms they are called hypergraphs and in design theoretic terms they are called block designs. They are also known as a set system or family of sets in a general context.
HypergraphsEdit
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Each hypergraph or set system can be regarded as an incidence structure in which the universal set plays the role of "points", the corresponding family of subsets plays the role of "lines" and the incidence relation is set membership "Template:Math". Conversely, every incidence structure can be viewed as a hypergraph by identifying the lines with the sets of points that are incident with them.
Block designsEdit
{{#invoke:Labelled list hatnote|labelledList|Main article|Main articles|Main page|Main pages}} A (general) block design is a set Template:Mvar together with a [[Family of sets|family Template:Mvar of subsets]] of Template:Mvar (repeated subsets are allowed). Normally a block design is required to satisfy numerical regularity conditions. As an incidence structure, Template:Mvar is the set of points and Template:Mvar is the set of lines, usually called blocks in this context (repeated blocks must have distinct names, so Template:Mvar is actually a set and not a multiset). If all the subsets in Template:Mvar have the same size, the block design is called uniform. If each element of Template:Mvar appears in the same number of subsets, the block design is said to be regular. The dual of a uniform design is a regular design and vice versa.
Example: Fano planeEdit
Consider the block design/hypergraph given by: <math display="block">\begin{align} P &= \{1,2,3,4,5,6,7\}, \\[2pt] L &= \left\{ \begin{array}{ll}
\{1,2,3\}, & \{1,4,5\}, \\ \{1,6,7\}, & \{2,4,6\}, \\ \{2,5,7\}, & \{3,4,7\}, \\ \{3,5,6\} \end{array} \right\}.
\end{align}</math>
This incidence structure is called the Fano plane. As a block design it is both uniform and regular.
In the labeling given, the lines are precisely the subsets of the points that consist of three points whose labels add up to zero using nim addition. Alternatively, each number, when written in binary, can be identified with a non-zero vector of length three over the binary field. Three vectors that generate a subspace form a line; in this case, that is equivalent to their vector sum being the zero vector.
RepresentationsEdit
Incidence structures may be represented in many ways. If the sets Template:Mvar and Template:Mvar are finite these representations can compactly encode all the relevant information concerning the structure.
Incidence matrixEdit
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The incidence matrix of a (finite) incidence structure is a (0,1) matrix that has its rows indexed by the points Template:Mvar and columns indexed by the lines Template:Math where the Template:Mvar-th entry is a 1 if Template:Math and 0 otherwise.Template:Efn An incidence matrix is not uniquely determined since it depends upon the arbitrary ordering of the points and the lines.<ref name=Beth17>Template:Harvnb</ref>
The non-uniform incidence structure pictured above (example number 2) is given by: <math display=block>\begin{align} P &= \{ A, B, C, D, E, P \} \\[2pt] L &= \left\{ \begin{array}{ll}
l = \{C, P, E \}, & m = \{ P \}, \\ n = \{ P, D \}, & o = \{ P, A \}, \\ p = \{ A, B \}, & q = \{ P, B \} \end{array} \right\}
\end{align}</math>
An incidence matrix for this structure is: <math display="block"> \begin{pmatrix} 0 & 0 & 0 & 1 & 1 & 0 \\ 0 & 0 & 0 & 0 & 1 & 1 \\ 1 & 0 & 0 & 0 & 0 & 0 \\ 0 & 0 & 1 & 0 & 0 & 0 \\ 1 & 0 & 0 & 0 & 0 & 0 \\ 1 & 1 & 1 & 1 & 0 & 1 \end{pmatrix} </math> which corresponds to the incidence table:
Template:Math | Template:Mvar | Template:Mvar | Template:Mvar | Template:Mvar | Template:Mvar | Template:Mvar |
---|---|---|---|---|---|---|
Template:Mvar | 0 | 0 | 0 | 1 | 1 | 0 |
Template:Mvar | 0 | 0 | 0 | 0 | 1 | 1 |
Template:Mvar | 1 | 0 | 0 | 0 | 0 | 0 |
Template:Mvar | 0 | 0 | 1 | 0 | 0 | 0 |
Template:Mvar | 1 | 0 | 0 | 0 | 0 | 0 |
Template:Mvar | 1 | 1 | 1 | 1 | 0 | 1 |
If an incidence structure Template:Mvar has an incidence matrix Template:Mvar, then the dual structure Template:Math has the transpose matrix Template:MvarT as its incidence matrix (and is defined by that matrix).
An incidence structure is self-dual if there exists an ordering of the points and lines so that the incidence matrix constructed with that ordering is a symmetric matrix.
With the labels as given in example number 1 above and with points ordered Template:Math and lines ordered Template:Math, the Fano plane has the incidence matrix: <math display="block"> \begin{pmatrix} 1 & 1 & 1 & 0 & 0 & 0 & 0\\ 1 & 0 & 0 & 1 & 1 & 0 & 0 \\ 1 & 0 & 0 & 0 & 0 & 1 & 1 \\ 0 & 1 & 0 & 1 & 0 & 1 & 0 \\ 0 & 1 & 0 & 0 & 1 & 0 & 1 \\ 0 & 0 & 1 & 1 & 0 & 0 & 1 \\ 0 & 0 & 1 & 0 & 1 & 1 & 0 \end{pmatrix} . </math> Since this is a symmetric matrix, the Fano plane is a self-dual incidence structure.
Pictorial representationsEdit
An incidence figure (that is, a depiction of an incidence structure), is constructed by representing the points by dots in a plane and having some visual means of joining the dots to correspond to lines.<ref name=Beth17 /> The dots may be placed in any manner, there are no restrictions on distances between points or any relationships between points. In an incidence structure there is no concept of a point being between two other points; the order of points on a line is undefined. Compare this with ordered geometry, which does have a notion of betweenness. The same statements can be made about the depictions of the lines. In particular, lines need not be depicted by "straight line segments" (see examples 1, 3 and 4 above). As with the pictorial representation of graphs, the crossing of two "lines" at any place other than a dot has no meaning in terms of the incidence structure; it is only an accident of the representation. These incidence figures may at times resemble graphs, but they aren't graphs unless the incidence structure is a graph.
RealizabilityEdit
Incidence structures can be modelled by points and curves in the Euclidean plane with the usual geometric meaning of incidence. Some incidence structures admit representation by points and (straight) lines. Structures that can be are called realizable. If no ambient space is mentioned then the Euclidean plane is assumed. The Fano plane (example 1 above) is not realizable since it needs at least one curve. The Möbius–Kantor configuration (example 4 above) is not realizable in the Euclidean plane, but it is realizable in the complex plane.<ref>Template:Harvnb</ref> On the other hand, examples 2 and 5 above are realizable and the incidence figures given there demonstrate this. Steinitz (1894)<ref>E. Steinitz (1894), Über die Construction der Configurationen Template:Math, Dissertation, Breslau</ref> has shown that Template:Nowrap (incidence structures with Template:Mvar points and Template:Mvar lines, three points per line and three lines through each point) are either realizable or require the use of only one curved line in their representations.<ref>Template:Citation</ref> The Fano plane is the unique (Template:Math) and the Möbius–Kantor configuration is the unique (Template:Math).
Incidence graph (Levi graph)Edit
Each incidence structure Template:Mvar corresponds to a bipartite graph called the Levi graph or incidence graph of the structure. As any bipartite graph is two-colorable, the Levi graph can be given a black and white vertex coloring, where black vertices correspond to points and white vertices correspond to lines of Template:Mvar. The edges of this graph correspond to the flags (incident point/line pairs) of the incidence structure. The original Levi graph was the incidence graph of the generalized quadrangle of order two (example 3 above),<ref>Template:Citation</ref> but the term has been extended by H.S.M. Coxeter<ref>Template:Citation</ref> to refer to an incidence graph of any incidence structure.<ref name=Pisanski158>Template:Harvnb</ref>
Levi graph examplesEdit
The Levi graph of the Fano plane is the Heawood graph. Since the Heawood graph is connected and vertex-transitive, there exists an automorphism (such as the one defined by a reflection about the vertical axis in the figure of the Heawood graph) interchanging black and white vertices. This, in turn, implies that the Fano plane is self-dual.
The specific representation, on the left, of the Levi graph of the Möbius–Kantor configuration (example 4 above) illustrates that a rotation of Template:Math about the center (either clockwise or counterclockwise) of the diagram interchanges the blue and red vertices and maps edges to edges. That is to say that there exists a color interchanging automorphism of this graph. Consequently, the incidence structure known as the Möbius–Kantor configuration is self-dual.
GeneralizationEdit
It is possible to generalize the notion of an incidence structure to include more than two types of objects. A structure with Template:Mvar types of objects is called an incidence structure of rank Template:Mvar or a rank Template:Mvar geometry.<ref name=Pisanski158 /> Formally these are defined as Template:Math tuples Template:Math with Template:Math and <math display="block">I \subseteq \bigcup_{i < j} P_i \times P_j.</math>
The Levi graph for these structures is defined as a multipartite graph with vertices corresponding to each type being colored the same.
See alsoEdit
NotesEdit
ReferencesEdit
BibliographyEdit
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Further readingEdit
- CRC Press (2000). Handbook of discrete and combinatorial mathematics, (Chapter 12.2), Template:ISBN
- Harold L. Dorwart (1966) The Geometry of Incidence, Prentice Hall