Moore Graphs As Maximal-Girth Graphs, And

Moore Graphs As Maximal-Girth Graphs, And

JUNIOR INDEPENDENT WORK FALL 2002 ALEXEY SPIRIDONOV This paper represents my own work in accordance with University regulations. 1. Introduction This paper concerns two types of simple graphs: (1) Graphs possessing the maximum possible girth with a given diameter. We derive a complete characterization of these. (2) Graphs, which are both their own duals and their own complements. We present a complete listing for ones drawn in the plane and in the torus. 2. Maximal-girth Graphs 2.1. Definitions. Notation. (u; v)G is the shortest path between u and v with u; v V (G) and 2 (u; v)G E(G). (u; v)G denotes the length of this path. We will omit the subscript⊆ when thek contextk is obvious. Most of the time, we use paths as sets of edges. However, we will occasionally refer to the path's vertex set; by that, we mean the set of vertices that are endpoints of members of the path. The ends (or endpoints) of a path are the two vertices that have degree 1 in its edge set. Definition 2.1. The girth of G, g(G), is the number of edges in the shortest cycle of G. Girth is not defined for forests; therefore, this section excludes them from consideration. Definition 2.2. The diameter of G, d(G) is the maximum of (u; v)G over all u; v V (G). k k 2 Definition 2.3. A d; k { Moore graph is a k-regular graph of diameter d with d 1 i 1 + k − (k 1) vertices. Pi=0 − Definition 2.4. G is a maximal-girth graph if no graph with the same diameter has a larger girth. 2.2. Preliminaries. In this subsection, we present some simple results that will be very useful later. We begin with this trivial lemma: Lemma 2.1. For any G, g(G) 2d(G) + 1. ≤ 1 2 ALEXEY SPIRIDONOV Proof. Suppose there exists G such that g(G) 2d(G) + 2. Let C G be a cycle with V (C) minimum. Let a; b V (C) be two≥ vertices separating⊆ C into two j j 2 paths of length at least d(G) + 1. If (a; b)G d(G), C would not be the shortest k k ≤ cycle of G. Hence, (a; b)G d(G) + 1, which contradicts the definition of the k k ≥ diameter. We thus obtain a more precise characterization of maximal-girth graphs: Corollary 2.2. G is maximal-girth iff g(G) = 2d(G) + 1. Proof. : Suppose g(G) = 2d(G) + 1. By Lemma 2.1, no graph with diameter d(G) and( larger girth can exist. Thus, G is maximal-girth. : Suppose G is maximal-girth, but g(G) = 2d(G)+1. Then, from Lemma 2.1, ) 6 g(G) < 2d(G) + 1. Let G0 be the cycle of length 2d(G) + 1. g(G0) > g(G), but d(G0) = d(G), so G is not maximal-girth. That is a contradiction. Another valuable property of maximal-girth graphs is that: Lemma 2.3. All maximal-girth graphs are 2-vertex-connected. Proof. Suppose G has a cut-vertex v. Then, G v has more than one component. n Assume that some component G0 has the property that v C (G0 v ), where C is the shortest cycle through v. By definition, C has size 2 g(G⊆). Let[u f beg a point g(G) ≥ in C that is at the distance (in C) l = 2 from v. Since C is the shortest cycle through v, u is also l edges away from vin G. Now consider w in a component other g(G) than G0. Since v is a cut-vertex, (u; v) (u; w)G, and d(G) (u; w)G > 2 . Therefore, g(G) < 2d(G) + 1 and G is not⊂ maximal-girth. ≥ k k If no component has a cycle containing v, we may contract all the edges leading out of v to obtain G0. The new graph clearly has the same cycles as G, and v is still a cut-vertex. Therefore, g(G0) = g(G) and d(G0) d(G). We can repeat this procedure indefinitely until v does belong to a cycle in≤ some component, at which point we get the previous case: g(G) = g(G0) < 2d(G0) + 1 2d(G) + 1. ≤ 2.3. Main Result. The following observation motivates our further investigation: Proposition 2.4. All Moore graphs are maximal-girth. Proof. Let G be a d; k { Moore graph, and u V (G). Label Sl the set of points v 2 such that (u; v) = l. Obviously, S0 is 1, and S1 is k. k k j j j j In general, for 0 < i d, every vertex v Si has k edges going to Si 1, Si, or ≤ 2 − Si+1. If v had an edge to Sj with j < i 1, (u; v) would be < i | a contradiction − k k since v Si. If v had an edge to w Sj, with j > i + 1, w would actually be in 2 2 Si+1 | again, a contradiction. Obviously, for each v Si at least one of these k edges must go to a v0 Si 1. 2 2 − If i < d, the others can (obviously) and must go to distinct vertices in Si+1. In other words, (1) Si+1 = (k 1) Si j j − j j Suppose some edge other than (v; v0) goes to Si 1 (0 < i d). Then, the Si i 2 − j ≤ i 1 d j i j ≤ (k 1) Si 1 1, and hence V (G) 1+k j−=0(k 1) +(k(k 1) − 1) j=0− (k − j− j j−d 1 i j j ≤ P − − − P − 1) < 1 + k − (k 1) , so G is not a Moore graph | a contradiction. Similarly, Pi=0 − if we suppose that some edge goes from v to Si (0 < i < d), Si+2 (k 1) Si 2 and G once again cannot be a Moore graph. j j ≤ − j j − JUNIOR INDEPENDENT WORK FALL 2002 3 Moreover, if some v1; v2 Si, 0 < i < d, have a common neighbor w in Si+1, 2 then w has two different neighbors in S(i+1) 1, which was shown to be impossible − above. Therefore, the neighbors of every v1 Si in Si+1 are distinct from those of 2 every other v2 Si. That proves (1). Therefore, every2 cycle through u is of length at least 2d+1 (otherwise, (1) would have to be violated). Since u was chosen arbitrarily, g(G) = 2d + 1. This proposition makes it natural to ask whether there are any non-Moore maximal-girth graphs. Arriving at the answer becomes a relatively simple mat- ter once we describe Moore graphs as follows: Lemma 2.5. A regular maximal-girth graph is a Moore graph. Proof. Suppose G is a k-regular maximal-girth graph. Using the notation from the proof of Proposition 2.4, we want to show that 0 < i < d(G), Si+1 = (k 1) Si . 8 j j − j j As in Proposition 2.4, given v Si with 0 < i d(G), the k edges leaving it go to 2 ≤ Si 1, Si, or Si+1, and at least one, (v; v0), goes to Si 1. − − Suppose some (v; w), v0 = w Si 1 is an edge. Let C0 = (u; v0) (u; w) (w; v) 6 2 − [ [ [ (v0; v). It is the union of two paths, each at most d(G) in length. The paths have the same endpoints, but do not share all vertices. Therefore, C0 contains the edge set of a cycle. The cycle must be at most 2d(G) in length | a contradiction, since G is maximal-girth. Suppose i < d(G) and some (v; w), w Si is an edge. As before, let C0 = 2 (u; v) (u; w) (v; w). C0 then contains the edge set of a cycle, and is of size < 2d(G[) + 1 |[ again, a contradiction. Now we know that k 1 neighbors of every v1 Si are in Si+1; these neighbors − 2 are also distinct from those of every other v2 Si. If that was not the case, the 2 shared neighbor w Si+1 would have two different neighbors in S(i+1) 1, previously shown to be impossible.2 − d(G) d 1 i Therefore, Si+1 = (k 1) Si and V (G) = Si = 1 + k − (k 1) . j j − j j j j Pi=0 j j Pi=0 − Hence, G is a Moore graph. Now we can rephrase our question as whether there are any non-regular maximal- girth graphs. Proposition 2.6. All maximal-girth graphs are regular. Proof. Let G be maximal-girth with d(G) = n, and C | some cycle of size g(G) = 2n + 1 with vertices v0; v1; : : : ; v2n (subscripts in Z=(2n + 1); such a cycle exists by definition of g(G)). Suppose some v = vi has deg v = d + 2 neighbors: (1) (d) (j) vi+1; vi 1; vi ; :::; vi . No vi is in V (C): if it were otherwise, there would exist a cycle shorter− than g(G) (contradicting the definition of girth). (j) Consider u = vi n and some v0 = vi . Define C0 with V (C0) = V (C) v0 − [ f g and E(C0) = E(C) (v; v0) . There are three paths of interest: pC = (u; v0)C , [ f g 0 p ¯ = (E(C) (u; v)) (v; v0), and pG = (u; v0)G.

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