SINGULAR VALUE DECOMPOSITION for INFORMATION RETRIEVAL, GRAPH BISECTION, and GENETIC ALGORITHMS by JACOB GILMORE MARTIN (Under the Direction of E
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Arxiv:1711.06300V1
EXPLICIT BLOCK-STRUCTURES FOR BLOCK-SYMMETRIC FIEDLER-LIKE PENCILS∗ M. I. BUENO†, M. MARTIN ‡, J. PEREZ´ §, A. SONG ¶, AND I. VIVIANO k Abstract. In the last decade, there has been a continued effort to produce families of strong linearizations of a matrix polynomial P (λ), regular and singular, with good properties, such as, being companion forms, allowing the recovery of eigen- vectors of a regular P (λ) in an easy way, allowing the computation of the minimal indices of a singular P (λ) in an easy way, etc. As a consequence of this research, families such as the family of Fiedler pencils, the family of generalized Fiedler pencils (GFP), the family of Fiedler pencils with repetition, and the family of generalized Fiedler pencils with repetition (GFPR) were con- structed. In particular, one of the goals was to find in these families structured linearizations of structured matrix polynomials. For example, if a matrix polynomial P (λ) is symmetric (Hermitian), it is convenient to use linearizations of P (λ) that are also symmetric (Hermitian). Both the family of GFP and the family of GFPR contain block-symmetric linearizations of P (λ), which are symmetric (Hermitian) when P (λ) is. Now the objective is to determine which of those structured linearizations have the best numerical properties. The main obstacle for this study is the fact that these pencils are defined implicitly as products of so-called elementary matrices. Recent papers in the literature had as a goal to provide an explicit block-structure for the pencils belonging to the family of Fiedler pencils and any of its further generalizations to solve this problem. -
Two-Graphs and Skew Two-Graphs in Finite Geometries
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Two-Graphs and Skew Two-Graphs in Finite Geometries G. Eric Moorhouse Department of Mathematics University of Wyoming Laramie Wyoming Dedicated to Professor J. J. Seidel Submitted by Aart Blokhuis ABSTRACT We describe the use of two-graphs and skew (oriented) two-graphs as isomor- phism invariants for translation planes and m-systems (including avoids and spreads) of polar spaces in odd characteristic. 1. INTRODUCTION Two-graphs were first introduced by G. Higman, as natural objects for the action of certain sporadic simple groups. They have since been studied extensively by Seidel, Taylor, and others, in relation to equiangular lines, strongly regular graphs, and other notions; see [26]-[28]. The analogous oriented two-graphs (which we call skew two-graphs) were introduced by Cameron [7], and there is some literature on the equivalent notion of switching classes of tournaments. Our exposition focuses on the use of two-graphs and skew two-graphs as isomorphism invariants of translation planes, and caps, avoids, and spreads of polar spaces in odd characteristic. The earliest precedent for using two-graphs to study ovoids and caps is apparently owing to Shult [29]. The degree sequences of these two-graphs and skew two-graphs yield the invariants known as fingerprints, introduced by J. H. Conway (see Chames [9, lo]). Two LZNEAR ALGEBRA AND ITS APPLZCATZONS 226-228:529-551 (1995) 0 Elsevier Science Inc., 1995 0024-3795/95/$9.50 655 Avenue of the Americas, New York, NY 10010 SSDI 0024-3795(95)00242-J 530 G. -
"Distance Measures for Graph Theory"
Distance measures for graph theory : Comparisons and analyzes of different methods Dissertation presented by Maxime DUYCK for obtaining the Master’s degree in Mathematical Engineering Supervisor(s) Marco SAERENS Reader(s) Guillaume GUEX, Bertrand LEBICHOT Academic year 2016-2017 Acknowledgments First, I would like to thank my supervisor Pr. Marco Saerens for his presence, his advice and his precious help throughout the realization of this thesis. Second, I would also like to thank Bertrand Lebichot and Guillaume Guex for agreeing to read this work. Next, I would like to thank my parents, all my family and my friends to have accompanied and encouraged me during all my studies. Finally, I would thank Malian De Ron for creating this template [65] and making it available to me. This helped me a lot during “le jour et la nuit”. Contents 1. Introduction 1 1.1. Context presentation .................................. 1 1.2. Contents .......................................... 2 2. Theoretical part 3 2.1. Preliminaries ....................................... 4 2.1.1. Networks and graphs .............................. 4 2.1.2. Useful matrices and tools ........................... 4 2.2. Distances and kernels on a graph ........................... 7 2.2.1. Notion of (dis)similarity measures ...................... 7 2.2.2. Kernel on a graph ................................ 8 2.2.3. The shortest-path distance .......................... 9 2.3. Kernels from distances ................................. 9 2.3.1. Multidimensional scaling ............................ 9 2.3.2. Gaussian mapping ............................... 9 2.4. Similarity measures between nodes .......................... 9 2.4.1. Katz index and its Leicht’s extension .................... 10 2.4.2. Commute-time distance and Euclidean commute-time distance .... 10 2.4.3. SimRank similarity measure ......................... -
Chapter 4 Introduction to Spectral Graph Theory
Chapter 4 Introduction to Spectral Graph Theory Spectral graph theory is the study of a graph through the properties of the eigenvalues and eigenvectors of its associated Laplacian matrix. In the following, we use G = (V; E) to represent an undirected n-vertex graph with no self-loops, and write V = f1; : : : ; ng, with the degree of vertex i denoted di. For undirected graphs our convention will be that if there P is an edge then both (i; j) 2 E and (j; i) 2 E. Thus (i;j)2E 1 = 2jEj. If we wish to sum P over edges only once, we will write fi; jg 2 E for the unordered pair. Thus fi;jg2E 1 = jEj. 4.1 Matrices associated to a graph Given an undirected graph G, the most natural matrix associated to it is its adjacency matrix: Definition 4.1 (Adjacency matrix). The adjacency matrix A 2 f0; 1gn×n is defined as ( 1 if fi; jg 2 E; Aij = 0 otherwise. Note that A is always a symmetric matrix with exactly di ones in the i-th row and the i-th column. While A is a natural representation of G when we think of a matrix as a table of numbers used to store information, it is less natural if we think of a matrix as an operator, a linear transformation which acts on vectors. The most natural operator associated with a graph is the diffusion operator, which spreads a quantity supported on any vertex equally onto its neighbors. To introduce the diffusion operator, first consider the degree matrix: Definition 4.2 (Degree matrix). -
Hadamard and Conference Matrices
Hadamard and conference matrices Peter J. Cameron December 2011 with input from Dennis Lin, Will Orrick and Gordon Royle Now det(H) is equal to the volume of the n-dimensional parallelepiped spanned by the rows of H. By assumption, each row has Euclidean length at most n1/2, so that det(H) ≤ nn/2; equality holds if and only if I every entry of H is ±1; > I the rows of H are orthogonal, that is, HH = nI. A matrix attaining the bound is a Hadamard matrix. Hadamard's theorem Let H be an n × n matrix, all of whose entries are at most 1 in modulus. How large can det(H) be? A matrix attaining the bound is a Hadamard matrix. Hadamard's theorem Let H be an n × n matrix, all of whose entries are at most 1 in modulus. How large can det(H) be? Now det(H) is equal to the volume of the n-dimensional parallelepiped spanned by the rows of H. By assumption, each row has Euclidean length at most n1/2, so that det(H) ≤ nn/2; equality holds if and only if I every entry of H is ±1; > I the rows of H are orthogonal, that is, HH = nI. Hadamard's theorem Let H be an n × n matrix, all of whose entries are at most 1 in modulus. How large can det(H) be? Now det(H) is equal to the volume of the n-dimensional parallelepiped spanned by the rows of H. By assumption, each row has Euclidean length at most n1/2, so that det(H) ≤ nn/2; equality holds if and only if I every entry of H is ±1; > I the rows of H are orthogonal, that is, HH = nI. -
MINIMUM DEGREE ENERGY of GRAPHS Dedicated to the Platinum
Electronic Journal of Mathematical Analysis and Applications Vol. 7(2) July 2019, pp. 230-243. ISSN: 2090-729X(online) http://math-frac.org/Journals/EJMAA/ |||||||||||||||||||||||||||||||| MINIMUM DEGREE ENERGY OF GRAPHS B. BASAVANAGOUD AND PRAVEEN JAKKANNAVAR Dedicated to the Platinum Jubilee year of Dr. V. R. Kulli Abstract. Let G be a graph of order n. Then an n × n symmetric matrix is called the minimum degree matrix MD(G) of a graph G, if its (i; j)th entry is minfdi; dj g whenever i 6= j, and zero otherwise, where di and dj are the degrees of ith and jth vertices of G, respectively. In the present work, we obtain the characteristic polynomial of the minimum degree matrix of graphs obtained by some graph operations. In addition, bounds for the largest minimum degree eigenvalue and minimum degree energy of graphs are obtained. 1. Introduction Throughout this paper by a graph G = (V; E) we mean a finite undirected graph without loops and multiple edges of order n and size m. Let V = V (G) and E = E(G) be the vertex set and edge set of G, respectively. The degree dG(v) of a vertex v 2 V (G) is the number of edges incident to it in G. The graph G is r-regular if and only if the degree of each vertex in G is r. Let fv1; v2; :::; vng be the vertices of G and let di = dG(vi). Basic notations and terminologies can be found in [8, 12, 14]. In literature, there are several graph polynomials defined on different graph matrices such as adjacency matrix [8, 12, 14], Laplacian matrix [15], signless Laplacian matrix [9, 18], seidel matrix [5], degree sum matrix [13, 19], distance matrix [1] etc. -
On Sign-Symmetric Signed Graphs∗
ISSN 1855-3966 (printed edn.), ISSN 1855-3974 (electronic edn.) ARS MATHEMATICA CONTEMPORANEA 19 (2020) 83–93 https://doi.org/10.26493/1855-3974.2161.f55 (Also available at http://amc-journal.eu) On sign-symmetric signed graphs∗ Ebrahim Ghorbani Department of Mathematics, K. N. Toosi University of Technology, P.O. Box 16765-3381, Tehran, Iran Willem H. Haemers Department of Econometrics and Operations Research, Tilburg University, Tilburg, The Netherlands Hamid Reza Maimani , Leila Parsaei Majd y Mathematics Section, Department of Basic Sciences, Shahid Rajaee Teacher Training University, P.O. Box 16785-163, Tehran, Iran Received 24 October 2019, accepted 27 March 2020, published online 10 November 2020 Abstract A signed graph is said to be sign-symmetric if it is switching isomorphic to its negation. Bipartite signed graphs are trivially sign-symmetric. We give new constructions of non- bipartite sign-symmetric signed graphs. Sign-symmetric signed graphs have a symmetric spectrum but not the other way around. We present constructions of signed graphs with symmetric spectra which are not sign-symmetric. This, in particular answers a problem posed by Belardo, Cioaba,˘ Koolen, and Wang in 2018. Keywords: Signed graph, spectrum. Math. Subj. Class. (2020): 05C22, 05C50 1 Introduction Let G be a graph with vertex set V and edge set E. All graphs considered in this paper are undirected, finite, and simple (without loops or multiple edges). A signed graph is a graph in which every edge has been declared positive or negative. In fact, a signed graph Γ is a pair (G; σ), where G = (V; E) is a graph, called the underlying ∗The authors would like to thank the anonymous referees for their helpful comments and suggestions. -
Pretty Good State Transfer in Discrete-Time Quantum Walks
Pretty good state transfer in discrete-time quantum walks Ada Chan and Hanmeng Zhan Department of Mathematics and Statistics, York University, Toronto, ON, Canada fssachan, [email protected] Abstract We establish the theory for pretty good state transfer in discrete- time quantum walks. For a class of walks, we show that pretty good state transfer is characterized by the spectrum of certain Hermitian adjacency matrix of the graph; more specifically, the vertices involved in pretty good state transfer must be m-strongly cospectral relative to this matrix, and the arccosines of its eigenvalues must satisfy some number theoretic conditions. Using normalized adjacency matrices, cyclic covers, and the theory on linear relations between geodetic an- gles, we construct several infinite families of walks that exhibits this phenomenon. 1 Introduction arXiv:2105.03762v1 [math.CO] 8 May 2021 A quantum walk with nice transport properties is desirable in quantum com- putation. For example, Grover's search algorithm [12] is a quantum walk on the looped complete graph, which sends the all-ones vector to a vector that almost \concentrate on" a vertex. In this paper, we study a slightly stronger notion of state transfer, where the target state can be approximated with arbitrary precision. This is called pretty good state transfer. Pretty good state transfer has been extensively studied in continuous-time quantum walks, especially on the paths [9, 22, 1, 5, 21]. However, not much 1 is known for the discrete-time analogues. The biggest difference between these two models is that in a continuous-time quantum walk, the evolution is completely determined by the adjacency or Laplacian matrix of the graph, while in a discrete-time quantum walk, the transition matrix depends on more than just the graph - usually, it is a product of two unitary matrices: U = SC; where S permutes the arcs of the graph, and C, called the coin matrix, send each arc to a linear combination of the outgoing arcs of the same vertex. -
Hadamard Matrices Include
Hadamard and conference matrices Peter J. Cameron University of St Andrews & Queen Mary University of London Mathematics Study Group with input from Rosemary Bailey, Katarzyna Filipiak, Joachim Kunert, Dennis Lin, Augustyn Markiewicz, Will Orrick, Gordon Royle and many happy returns . Happy Birthday, MSG!! Happy Birthday, MSG!! and many happy returns . Now det(H) is equal to the volume of the n-dimensional parallelepiped spanned by the rows of H. By assumption, each row has Euclidean length at most n1/2, so that det(H) ≤ nn/2; equality holds if and only if I every entry of H is ±1; > I the rows of H are orthogonal, that is, HH = nI. A matrix attaining the bound is a Hadamard matrix. This is a nice example of a continuous problem whose solution brings us into discrete mathematics. Hadamard's theorem Let H be an n × n matrix, all of whose entries are at most 1 in modulus. How large can det(H) be? A matrix attaining the bound is a Hadamard matrix. This is a nice example of a continuous problem whose solution brings us into discrete mathematics. Hadamard's theorem Let H be an n × n matrix, all of whose entries are at most 1 in modulus. How large can det(H) be? Now det(H) is equal to the volume of the n-dimensional parallelepiped spanned by the rows of H. By assumption, each row has Euclidean length at most n1/2, so that det(H) ≤ nn/2; equality holds if and only if I every entry of H is ±1; > I the rows of H are orthogonal, that is, HH = nI. -
MATH7502 Topic 6 - Graphs and Networks
MATH7502 Topic 6 - Graphs and Networks October 18, 2019 Group ID fbb0bfdc-79d6-44ad-8100-05067b9a0cf9 Chris Lam 41735613 Anthony North 46139896 Stuart Norvill 42938019 Lee Phillips 43908587 Minh Tram Julien Tran 44536389 Tutor Chris Raymond (P03 Tuesday 4pm) 1 [ ]: using Pkg; Pkg.add(["LightGraphs", "GraphPlot", "Laplacians","Colors"]); using LinearAlgebra; using LightGraphs, GraphPlot, Laplacians,Colors; 0.1 Graphs and Networks Take for example, a sample directed graph: [2]: # creating the above directed graph let edges = [(1, 2), (1, 3), (2,4), (3, 2), (3, 5), (4, 5), (4, 6), (5, 2), (5, 6)] global graph = DiGraph(Edge.(edges)) end [2]: {6, 9} directed simple Int64 graph 2 0.2 Incidence matrix • shows the relationship between nodes (columns) via edges (rows) • edges are connected by exactly two nodes (duh), with direction indicated by the sign of each row in the edge column – a value of 1 at A12 indicates that edge 1 is directed towards node 1, or node 2 is the destination node for edge 1 • edge rows sum to 0 and constant column vectors c(1, ... , 1) are in the nullspace • cannot represent self-loops (nodes connected to themselves) Using Strang’s definition in the LALFD book, a graph consists of nodes defined as columns n and edges m as rows between the nodes. An Incidence Matrix A is m × n. For the above sample directed graph, we can generate its incidence matrix. [3]: # create an incidence matrix from a directed graph function create_incidence(graph::DiGraph) M = zeros(Int, ne(graph), nv(graph)) # each edge maps to a row in the incidence -
Two One-Parameter Special Geometries
Two One-Parameter Special Geometries Volker Braun1, Philip Candelas2 and Xenia de la Ossa2 1Elsenstrasse 35 12435 Berlin Germany 2Mathematical Institute University of Oxford Radcliffe Observatory Quarter Woodstock Road Oxford OX2 6GG, UK arXiv:1512.08367v1 [hep-th] 28 Dec 2015 Abstract The special geometries of two recently discovered Calabi-Yau threefolds with h11 = 1 are analyzed in detail. These correspond to the 'minimal three-generation' manifolds with h21 = 4 and the `24-cell' threefolds with h21 = 1. It turns out that the one- dimensional complex structure moduli spaces for these manifolds are both very similar and surprisingly complicated. Both have 6 hyperconifold points and, in addition, there are singularities of the Picard-Fuchs equation where the threefold is smooth but the Yukawa coupling vanishes. Their fundamental periods are the generating functions of lattice walks, and we use this fact to explain why the singularities are all at real values of the complex structure. Contents 1 Introduction 1 2 The Special Geometry of the (4,1)-Manifold 6 2.1 Fundamental Period . .6 2.2 Picard-Fuchs Differential Equation . .8 2.3 Integral Homology Basis and the Prepotential . 11 2.4 The Yukawa coupling . 16 3 The Special Geometry of the (1,1)-Manifold(s) 17 3.1 The Picard-Fuchs Operator . 17 3.2 Monodromy . 19 3.3 Prepotential . 22 3.4 Integral Homology Basis . 23 3.5 Instanton Numbers . 24 3.6 Cross Ratios . 25 4 Lattice Walks 27 4.1 Spectral Considerations . 27 4.2 Square Lattice . 28 1. Introduction Detailed descriptions of special geometries are known only in relatively few cases. -
On D. G. Higman's Note on Regular 3-Graphs
Also available at http://amc.imfm.si ISSN 1855-3966 (printed edn.), ISSN 1855-3974 (electronic edn.) ARS MATHEMATICA CONTEMPORANEA 6 (2013) 99–115 On D. G. Higman’s note on regular 3-graphs Daniel Kalmanovich Department of Mathematics Ben-Gurion University of the Negev 84105 Beer Sheva, Israel Received 17 October 2011, accepted 25 April 2012, published online 4 June 2012 Abstract We introduce the notion of a t-graph and prove that regular 3-graphs are equivalent to cyclic antipodal 3-fold covers of a complete graph. This generalizes the equivalence of regular two-graphs and Taylor graphs. As a consequence, an equivalence between cyclic antipodal distance regular graphs of diameter 3 and certain rank 6 commutative association schemes is proved. New examples of regular 3-graphs are presented. Keywords: Antipodal graph, association scheme, distance regular graph of diameter 3, Godsil- Hensel matrix, group ring, Taylor graph, two-graph. Math. Subj. Class.: 05E30, 05B20, 05E18 1 Introduction This paper is mainly a clarification of [6] — a short draft written by Donald Higman in 1994, entitled “A note on regular 3-graphs”. The considered generalization of two-graphs was introduced by D. G. Higman in [5]. As in the famous correspondence between two-graphs and switching classes of simple graphs, t-graphs are interpreted as equivalence classes of an appropriate switching relation defined on weights, which play the role of simple graphs. In his note Higman uses certain association schemes to characterize regular 3-graphs and to obtain feasibility conditions for their parameters. Specifically, he provides a graph theoretic interpretation of a weight and from the resulted graph he constructs a rank 4 symmetric association scheme and a rank 6 fission of it.