Odd graph | |
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The Petersen graph as an odd graph O3 |
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Vertices | |
Edges | |
Diameter | n − 1[1][2] |
Girth | 3 if n = 2 5 if n = 3 6 if n > 3[3] |
Properties | Distance-transitive |
Notation | On |
In the mathematical field of graph theory, the odd graphs On are a family of symmetric graphs with high odd girth, defined from certain set systems. They include and generalize the Petersen graph.
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The odd graph On has one vertex for each of the (n − 1)-element subsets of a (2n − 1)-element set. Two vertices are connected by an edge if and only if the corresponding subsets are disjoint.[4] That is, On is a Kneser graph KG(2n − 1,n − 1).
O2 is a triangle, while O3 is the familiar Petersen graph.
The generalized odd graphs include the odd graphs and the folded cube graphs, and are defined as distance-regular graphs with diameter n − 1 and odd girth 2n − 1 for some n.[5]
Although the Petersen graph has been known since 1898, its definition as an odd graph dates to the work of Kowalewski (1917), who also studied the odd graph O4.[2][6] Odd graphs have been studied for their applications in chemical graph theory, in modeling the shifts of carbonium ions.[7][8] They have also been proposed as a network topology in parallel computing.[9]
The notation On for these graphs was introduced by Norman Biggs in 1972.[10] Biggs and Anthony Gardiner explain the name of odd graphs in an unpublished manuscript from 1974: each edge of an odd graph can be assigned the unique element of X which is the "odd man out", i.e., not a member of either subset associated with the vertices incident to that edge.[11][12]
The odd graph On is regular of degree n. It has vertices and edges. Therefore, the number of vertices for n = 1, 2,... is
If two vertices in On correspond to sets that differ from each other by the removal of k elements from one set and the addition of k different elements, then they may be reached from each other in 2k steps, each pair of which performs a single addition and removal. If 2k < n, this is a shortest path; otherwise, it is shorter to find a path of this type from the first set to a set complementary to the second, and then reach the second set in one more step. Therefore, the diameter of On is n − 1.[1][2]
Every odd graph is 3-arc-transitive: every directed three-edge path in an odd graph can be transformed into every other such path by a symmetry of the graph.[13] Odd graphs are distance transitive, hence distance regular.[2] As distance-regular graphs, they are uniquely defined by their intersection array: no other distance-regular graphs can have the same parameters as an odd graph.[14] However, despite their high degree of symmetry, the odd graphs On for n > 2 are never Cayley graphs.[15]
Odd graphs with n ≥ 3 have girth six; however, although they are not bipartite graphs, their odd cycles are much longer. Specifically, the odd graph On has odd girth 2n − 1. If a n-regular graph has diameter n − 1 and odd girth 2n − 1, and has only n distinct eigenvalues, it must be distance-regular. Distance-regular graphs with diameter n − 1 and odd girth 2n − 1 are known as the generalized odd graphs, and include the folded cube graphs as well as the odd graphs themselves.[5]
Let On be an odd graph defined from the subsets of a (2n − 1)-element set X, and let x be any member of X. Then, among the vertices of On, exactly vertices correspond to sets that contain x. Because all these sets contain x, they are not disjoint, and form an independent set of On. That is, On has 2n − 1 different independent sets of size . It follows from the Erdős–Ko–Rado theorem that these are the maximum independent sets of On. that is, the independence number of On is Further, every maximum independent set must have this form, so On has exactly 2n − 1 maximum independent sets.[2]
If I is a maximum independent set, formed by the sets that contain x, then the complement of I is the set of vertices that do not contain x. This complementary set induces a matching in G. Each vertex of the independent set is adjacent to n vertices of the matching, and each vertex of the matching is adjacent to n − 1 vertices of the independent set.[2] Because of this decomposition, and because odd graphs are not bipartite, they have chromatic number three: the vertices of the maximum independent set can be assigned a single color, and two more colors suffice to color the complementary matching.
By Vizing's theorem, the number of colors needed to color the edges of the odd graph On is either n or n + 1, and in the case of the Petersen graph O3 it is n + 1. When n is a power of two, the number of vertices in the graph is odd, from which it again follows that the number of edge colors is n + 1.[16] However, O5, O6, and O7 can each be edge-colored with n colors.[2][16]
Biggs[10] explains this problem with the following story: eleven soccer players in the fictional town of Croam wish to form up pairs of five-man teams (with an odd man out to serve as referee) in all 1386 possible ways, and they wish to schedule the games between each pair in such a way that the six games for each team are played on six different days of the week, with Sundays off for all teams. Is it possible to do so? In this story, each game represents an edge of O6, each weekday is represented by a color, and a 6-color edge coloring of O6 provides a solution to the players' scheduling problem.
The Petersen graph O3 is a well known non-Hamiltonian graph, but O4 through O14 have been shown to contain Hamiltonian cycles.[8][17][18][19] More strongly, combining the Hamiltonian cycle and edge coloring problems, it is possible to partition the edges of On (for n = 4, 5, 6, 7) into floor(n/2) Hamiltonian cycles; when n is odd, the leftover edges form a perfect matching.[2][16] For n = 8, the odd number of vertices in On prevents an 8-color edge coloring from existing, but does not rule out the possibility of a partition into four Hamiltonian cycles.
The Lovász conjecture implies that every odd graph has a Hamiltonian path and that every odd graph On with n ≥ 4 has a Hamiltonian cycle.