M210 DISCRETE MATHEMATICS Graph Theory Group Work NAME
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Distance Regular Graphs Simply Explained
Distance Regular Graphs Simply Explained Alexander Coulter Paauwe April 20, 2007 Copyright c 2007 Alexander Coulter Paauwe. Permission is granted to copy, distribute and/or modify this document under the terms of the GNU Free Documentation License, Version 1.2 or any later version published by the Free Software Foundation; with no Invariant Sections, no Front-Cover Texts, and no Back-Cover Texts. A copy of the license is included in the section entitled “GNU Free Documentation License”. Adjacency Algebra and Distance Regular Graphs: In this paper, we will discover some interesting properties of a particular kind of graph, called distance regular graphs, using algebraic graph theory. We will begin by developing some definitions that will allow us to explore the relationship between powers of the adjacency matrix of a graph and its eigenvalues, and ultimately give us particular insight into the eigenvalues of distance regular graphs. Basis for the Polynomial of an Adjacency Matrix We all know that for a given graph G, the powers of its adjacency matrix, A, have as their entries the number of n-walks between two vertices. More succinctly, we know that [An]i,j is the number of n-walks between the two vertices vi and vj. We also know that for a graph with diameter d, the first d powers of A are all linearly independent. Now, let us think of the set of all polynomials of the adjacency matrix, A, for a graph G. We can think of any member of the set as a linear combination of powers of A. -
Investigations on Unit Distance Property of Clebsch Graph and Its Complement
Proceedings of the World Congress on Engineering 2012 Vol I WCE 2012, July 4 - 6, 2012, London, U.K. Investigations on Unit Distance Property of Clebsch Graph and Its Complement Pratima Panigrahi and Uma kant Sahoo ∗yz Abstract|An n-dimensional unit distance graph is on parameters (16,5,0,2) and (16,10,6,6) respectively. a simple graph which can be drawn on n-dimensional These graphs are known to be unique in the respective n Euclidean space R so that its vertices are represented parameters [2]. In this paper we give unit distance n by distinct points in R and edges are represented by representation of Clebsch graph in the 3-dimensional Eu- closed line segments of unit length. In this paper we clidean space R3. Also we show that the complement of show that the Clebsch graph is 3-dimensional unit Clebsch graph is not a 3-dimensional unit distance graph. distance graph, but its complement is not. Keywords: unit distance graph, strongly regular The Petersen graph is the strongly regular graph on graphs, Clebsch graph, Petersen graph. parameters (10,3,0,1). This graph is also unique in its parameter set. It is known that Petersen graph is 2-dimensional unit distance graph (see [1],[3],[10]). It is In this article we consider only simple graphs, i.e. also known that Petersen graph is a subgraph of Clebsch undirected, loop free and with no multiple edges. The graph, see [[5], section 10.6]. study of dimension of graphs was initiated by Erdos et.al [3]. -
Constructing an Infinite Family of Cubic 1-Regular Graphs
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Europ. J. Combinatorics (2002) 23, 559–565 doi:10.1006/eujc.2002.0589 Available online at http://www.idealibrary.com on Constructing an Infinite Family of Cubic 1-Regular Graphs YQAN- UAN FENG† AND JIN HO KWAK A graph is 1-regular if its automorphism group acts regularly on the set of its arcs. Miller [J. Comb. Theory, B, 10 (1971), 163–182] constructed an infinite family of cubic 1-regular graphs of order 2p, where p ≥ 13 is a prime congruent to 1 modulo 3. Marusiˇ cˇ and Xu [J. Graph Theory, 25 (1997), 133– 138] found a relation between cubic 1-regular graphs and tetravalent half-transitive graphs with girth 3 and Alspach et al.[J. Aust. Math. Soc. A, 56 (1994), 391–402] constructed infinitely many tetravalent half-transitive graphs with girth 3. Using these results, Miller’s construction can be generalized to an infinite family of cubic 1-regular graphs of order 2n, where n ≥ 13 is odd such that 3 divides ϕ(n), the Euler function of n. In this paper, we construct an infinite family of cubic 1-regular graphs with order 8(k2 + k + 1)(k ≥ 2) as cyclic-coverings of the three-dimensional Hypercube. c 2002 Elsevier Science Ltd. All rights reserved. 1. INTRODUCTION In this paper we consider an undirected finite connected graph without loops or multiple edges. For a graph G, we denote by V (G), E(G), A(G) and Aut(G) the vertex set, the edge set, the arc set and the automorphism group, respectively. -
Maximizing the Order of a Regular Graph of Given Valency and Second Eigenvalue∗
SIAM J. DISCRETE MATH. c 2016 Society for Industrial and Applied Mathematics Vol. 30, No. 3, pp. 1509–1525 MAXIMIZING THE ORDER OF A REGULAR GRAPH OF GIVEN VALENCY AND SECOND EIGENVALUE∗ SEBASTIAN M. CIOABA˘ †,JACKH.KOOLEN‡, HIROSHI NOZAKI§, AND JASON R. VERMETTE¶ Abstract. From Alon√ and Boppana, and Serre, we know that for any given integer k ≥ 3 and real number λ<2 k − 1, there are only finitely many k-regular graphs whose second largest eigenvalue is at most λ. In this paper, we investigate the largest number of vertices of such graphs. Key words. second eigenvalue, regular graph, expander AMS subject classifications. 05C50, 05E99, 68R10, 90C05, 90C35 DOI. 10.1137/15M1030935 1. Introduction. For a k-regular graph G on n vertices, we denote by λ1(G)= k>λ2(G) ≥ ··· ≥ λn(G)=λmin(G) the eigenvalues of the adjacency matrix of G. For a general reference on the eigenvalues of graphs, see [8, 17]. The second eigenvalue of a regular graph is a parameter of interest in the study of graph connectivity and expanders (see [1, 8, 23], for example). In this paper, we investigate the maximum order v(k, λ) of a connected k-regular graph whose second largest eigenvalue is at most some given parameter λ. As a consequence of work of Alon and Boppana and of Serre√ [1, 11, 15, 23, 24, 27, 30, 34, 35, 40], we know that v(k, λ) is finite for λ<2 k − 1. The recent result of Marcus, Spielman, and Srivastava [28] showing the existence of infinite families of√ Ramanujan graphs of any degree at least 3 implies that v(k, λ) is infinite for λ ≥ 2 k − 1. -
Perfect Domination in Book Graph and Stacked Book Graph
International Journal of Mathematics Trends and Technology (IJMTT) – Volume 56 Issue 7 – April 2018 Perfect Domination in Book Graph and Stacked Book Graph Kavitha B N#1, Indrani Pramod Kelkar#2, Rajanna K R#3 #1Assistant Professor, Department of Mathematics, Sri Venkateshwara College of Engineering, Bangalore, India *2 Professor, Department of Mathematics, Acharya Institute of Technology, Bangalore, India #3 Professor, Department of Mathematics, Acharya Institute of Technology, Bangalore, India Abstract: In this paper we prove that the perfect domination number of book graph and stacked book graph are same as the domination number as the dominating set satisfies the condition for perfect domination. Keywords: Domination, Cartesian product graph, Perfect Domination, Book Graph, Stacked Book Graph. I. INTRODUCTION By a graph G = (V, E) we mean a finite, undirected graph with neither loops nor multiple edges. The order and size of G are denoted by p and q respectively. For graph theoretic terminology we refer to Chartrand and Lesnaik[3]. Graphs have various special patterns like path, cycle, star, complete graph, bipartite graph, complete bipartite graph, regular graph, strongly regular graph etc. For the definitions of all such graphs we refer to Harry [7]. The study of Cross product of graph was initiated by Imrich [12]. For structure and recognition of Cross Product of graph we refer to Imrich [11]. In literature, the concept of domination in graphs was introduced by Claude Berge in 1958 and Oystein Ore in [1962] by [14]. For review of domination and its related parameters we refer to Acharya et.al. [1979] and Haynes et.al. -
Strongly Regular Graphs
Chapter 4 Strongly Regular Graphs 4.1 Parameters and Properties Recall that a (simple, undirected) graph is regular if all of its vertices have the same degree. This is a strong property for a graph to have, and it can be recognized easily from the adjacency matrix, since it means that all row sums are equal, and that1 is an eigenvector. If a graphG of ordern is regular of degreek, it means that kn must be even, since this is twice the number of edges inG. Ifk�n− 1 and kn is even, then there does exist a graph of ordern that is regular of degreek (showing that this is true is an exercise worth thinking about). Regularity is a strong property for a graph to have, and it implies a kind of symmetry, but there are examples of regular graphs that are not particularly “symmetric”, such as the disjoint union of two cycles of different lengths, or the connected example below. Various properties of graphs that are stronger than regularity can be considered, one of the most interesting of which is strong regularity. Definition 4.1.1. A graphG of ordern is called strongly regular with parameters(n,k,λ,µ) if every vertex ofG has degreek; • ifu andv are adjacent vertices ofG, then the number of common neighbours ofu andv isλ (every • edge belongs toλ triangles); ifu andv are non-adjacent vertices ofG, then the number of common neighbours ofu andv isµ; • 1 k<n−1 (so the complete graph and the null graph ofn vertices are not considered to be • � strongly regular). -
On Cayley Graphs of Algebraic Structures
On Cayley graphs of algebraic structures Didier Caucal1 1 CNRS, LIGM, University Paris-East, France [email protected] Abstract We present simple graph-theoretic characterizations of Cayley graphs for left-cancellative monoids, groups, left-quasigroups and quasigroups. We show that these characterizations are effective for the end-regular graphs of finite degree. 1 Introduction To describe the structure of a group, Cayley introduced in 1878 [7] the concept of graph for any group (G, ·) according to any generating subset S. This is simply the set of labeled s oriented edges g −→ g·s for every g of G and s of S. Such a graph, called Cayley graph, is directed and labeled in S (or an encoding of S by symbols called letters or colors). The study of groups by their Cayley graphs is a main topic of algebraic graph theory [3, 8, 2]. A characterization of unlabeled and undirected Cayley graphs was given by Sabidussi in 1958 [15] : an unlabeled and undirected graph is a Cayley graph if and only if we can find a group with a free and transitive action on the graph. However, this algebraic characterization is not well suited for deciding whether a possibly infinite graph is a Cayley graph. It is pertinent to look for characterizations by graph-theoretic conditions. This approach was clearly stated by Hamkins in 2010: Which graphs are Cayley graphs? [10]. In this paper, we present simple graph-theoretic characterizations of Cayley graphs for firstly left-cancellative and cancellative monoids, and then for groups. These characterizations are then extended to any subset S of left-cancellative magmas, left-quasigroups, quasigroups, and groups. -
Towards a Classification of Distance-Transitive Graphs
数理解析研究所講究録 1063 巻 1998 年 72-83 72 Towards a classification of distance-transitive graphs John van Bon Abstract We outline the programme of classifying all finite distance-transitive graphs. We men- tion the most important classification results obtained so far and give special attention to the so called affine graphs. 1. Introduction The graphs in this paper will be always assumed to be finite, connected, undirected and without loops or multiple edges. The edge set of a graph can thus be identified with a subset of the set of unoidered pairs of vertices. Let $\Gamma=(V\Gamma, E\Gamma)$ be a graph and $x,$ $y\in V\Gamma$ . With $d(x, y)$ we will denote the usual distance $\Gamma$ in between the vertices $x$ and $y$ (i.e., the length of the shortest path connecting $x$ and $y$ ) and with $d$ we will denote the diameter of $\Gamma$ , the maximum of all possible values of $d(x, y)$ . Let $\Gamma_{i}(x)=\{y|y\in V\Gamma, d(x, y)=i\}$ be the set of all vertices at distance $i$ of $x$ . An $aut_{omo}rph7,sm$ of a graph is a permutation of the vertex set that maps edges to edges. Let $G$ be a group acting on a graph $\Gamma$ (i.e. we are given a morphism $Garrow Aut(\Gamma)$ ). For a $x\in V\Gamma$ $x^{g}$ vertex and $g\in G$ the image of $x$ under $g$ will be denoted by . The set $\{g\in G|x^{g}=x\}$ is a subgroup of $G$ , called that stabilizer in $G$ of $x$ and will be denoted by $G_{x}$ . -
On Snarks That Are Far from Being 3-Edge Colorable
On snarks that are far from being 3-edge colorable Jonas H¨agglund Department of Mathematics and Mathematical Statistics Ume˚aUniversity SE-901 87 Ume˚a,Sweden [email protected] Submitted: Jun 4, 2013; Accepted: Mar 26, 2016; Published: Apr 15, 2016 Mathematics Subject Classifications: 05C38, 05C70 Abstract In this note we construct two infinite snark families which have high oddness and low circumference compared to the number of vertices. Using this construction, we also give a counterexample to a suggested strengthening of Fulkerson's conjecture by showing that the Petersen graph is not the only cyclically 4-edge connected cubic graph which require at least five perfect matchings to cover its edges. Furthermore the counterexample presented has the interesting property that no 2-factor can be part of a cycle double cover. 1 Introduction A cubic graph is said to be colorable if it has a 3-edge coloring and uncolorable otherwise. A snark is an uncolorable cubic cyclically 4-edge connected graph. It it well known that an edge minimal counterexample (if such exists) to some classical conjectures in graph theory, such as the cycle double cover conjecture [15, 18], Tutte's 5-flow conjecture [19] and Fulkerson's conjecture [4], must reside in this family of graphs. There are various ways of measuring how far a snark is from being colorable. One such measure which was introduced by Huck and Kochol [8] is the oddness. The oddness of a bridgeless cubic graph G is defined as the minimum number of odd components in any 2-factor in G and is denoted by o(G). -
Strongly Regular Graphs, Part 1 23.1 Introduction 23.2 Definitions
Spectral Graph Theory Lecture 23 Strongly Regular Graphs, part 1 Daniel A. Spielman November 18, 2009 23.1 Introduction In this and the next lecture, I will discuss strongly regular graphs. Strongly regular graphs are extremal in many ways. For example, their adjacency matrices have only three distinct eigenvalues. If you are going to understand spectral graph theory, you must have these in mind. In many ways, strongly-regular graphs can be thought of as the high-degree analogs of expander graphs. However, they are much easier to construct. Many times someone has asked me for a matrix of 0s and 1s that \looked random", and strongly regular graphs provided a resonable answer. Warning: I will use the letters that are standard when discussing strongly regular graphs. So λ and µ will not be eigenvalues in this lecture. 23.2 Definitions Formally, a graph G is strongly regular if 1. it is k-regular, for some integer k; 2. there exists an integer λ such that for every pair of vertices x and y that are neighbors in G, there are λ vertices z that are neighbors of both x and y; 3. there exists an integer µ such that for every pair of vertices x and y that are not neighbors in G, there are µ vertices z that are neighbors of both x and y. These conditions are very strong, and it might not be obvious that there are any non-trivial graphs that satisfy these conditions. Of course, the complete graph and disjoint unions of complete graphs satisfy these conditions. -
Self-Dual Configurations and Regular Graphs
SELF-DUAL CONFIGURATIONS AND REGULAR GRAPHS H. S. M. COXETER 1. Introduction. A configuration (mci ni) is a set of m points and n lines in a plane, with d of the points on each line and c of the lines through each point; thus cm = dn. Those permutations which pre serve incidences form a group, "the group of the configuration." If m — n, and consequently c = d, the group may include not only sym metries which permute the points among themselves but also reci procities which interchange points and lines in accordance with the principle of duality. The configuration is then "self-dual," and its symbol («<*, n<j) is conveniently abbreviated to na. We shall use the same symbol for the analogous concept of a configuration in three dimensions, consisting of n points lying by d's in n planes, d through each point. With any configuration we can associate a diagram called the Menger graph [13, p. 28],x in which the points are represented by dots or "nodes," two of which are joined by an arc or "branch" when ever the corresponding two points are on a line of the configuration. Unfortunately, however, it often happens that two different con figurations have the same Menger graph. The present address is concerned with another kind of diagram, which represents the con figuration uniquely. In this Levi graph [32, p. 5], we represent the points and lines (or planes) of the configuration by dots of two colors, say "red nodes" and "blue nodes," with the rule that two nodes differently colored are joined whenever the corresponding elements of the configuration are incident. -
Snarks and Flow-Critical Graphs 1
Snarks and Flow-Critical Graphs 1 CˆandidaNunes da Silva a Lissa Pesci a Cl´audioL. Lucchesi b a DComp – CCTS – ufscar – Sorocaba, sp, Brazil b Faculty of Computing – facom-ufms – Campo Grande, ms, Brazil Abstract It is well-known that a 2-edge-connected cubic graph has a 3-edge-colouring if and only if it has a 4-flow. Snarks are usually regarded to be, in some sense, the minimal cubic graphs without a 3-edge-colouring. We defined the notion of 4-flow-critical graphs as an alternative concept towards minimal graphs. It turns out that every snark has a 4-flow-critical snark as a minor. We verify, surprisingly, that less than 5% of the snarks with up to 28 vertices are 4-flow-critical. On the other hand, there are infinitely many 4-flow-critical snarks, as every flower-snark is 4-flow-critical. These observations give some insight into a new research approach regarding Tutte’s Flow Conjectures. Keywords: nowhere-zero k-flows, Tutte’s Flow Conjectures, 3-edge-colouring, flow-critical graphs. 1 Nowhere-Zero Flows Let k > 1 be an integer, let G be a graph, let D be an orientation of G and let ϕ be a weight function that associates to each edge of G a positive integer in the set {1, 2, . , k − 1}. The pair (D, ϕ) is a (nowhere-zero) k-flow of G 1 Support by fapesp, capes and cnpq if every vertex v of G is balanced, i. e., the sum of the weights of all edges leaving v equals the sum of the weights of all edges entering v.