The Road to Deterministic Matrices with the Restricted Isometry Property
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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. -
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. -
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. -
Arxiv:1205.2081V6 [Math.OC]
THE COMPUTATIONAL COMPLEXITY OF RIP, NSP, AND RELATED CONCEPTS IN COMPRESSED SENSING 1 The Computational Complexity of the Restricted Isometry Property, the Nullspace Property, and Related Concepts in Compressed Sensing Andreas M. Tillmann and Marc E. Pfetsch Abstract This paper deals with the computational complexity of conditions which guarantee that the NP-hard problem of finding the sparsest solution to an underdetermined linear system can be solved by efficient algorithms. In the literature, several such conditions have been introduced. The most well-known ones are the mutual coherence, the restricted isometry property (RIP), and the nullspace property (NSP). While evaluating the mutual coherence of a given matrix is easy, it has been suspected for some time that evaluating RIP and NSP is computationally intractable in general. We confirm these conjectures by showing that for a given matrix A and positive integer k, computing the best constants for which the RIP or NSP hold is, in general, NP-hard. These results are based on the fact that determining the spark of a matrix is NP-hard, which is also established in this paper. Furthermore, we also give several complexity statements about problems related to the above concepts. Index Terms Compressed Sensing, Computational Complexity, Sparse Recovery Conditions I. INTRODUCTION CENTRAL problem in compressed sensing (CS), see, e.g., [1], [2], [3], is the task of finding a sparsest solution to an A underdetermined linear system, i.e., min x s.t. Ax = b, (P ) k k0 0 m n for a given matrix A R × with m n, where x 0 denotes the ℓ0-quasi-norm, i.e., the number of nonzero entries in x. -
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. -
2020 Ural Workshop on Group Theory and Combinatorics
Institute of Natural Sciences and Mathematics of the Ural Federal University named after the first President of Russia B.N.Yeltsin N.N. Krasovskii Institute of Mathematics and Mechanics of the Ural Branch of the Russian Academy of Sciences The Ural Mathematical Center 2020 Ural Workshop on Group Theory and Combinatorics Yekaterinburg – Online, Russia, August 24-30, 2020 Abstracts Yekaterinburg 2020 2020 Ural Workshop on Group Theory and Combinatorics: Abstracts of 2020 Ural Workshop on Group Theory and Combinatorics. Yekaterinburg: N.N. Krasovskii Institute of Mathematics and Mechanics of the Ural Branch of the Russian Academy of Sciences, 2020. DOI Editor in Chief Natalia Maslova Editors Vladislav Kabanov Anatoly Kondrat’ev Managing Editors Nikolai Minigulov Kristina Ilenko Booklet Cover Desiner Natalia Maslova c Institute of Natural Sciences and Mathematics of Ural Federal University named after the first President of Russia B.N.Yeltsin N.N. Krasovskii Institute of Mathematics and Mechanics of the Ural Branch of the Russian Academy of Sciences The Ural Mathematical Center, 2020 2020 Ural Workshop on Group Theory and Combinatorics Conents Contents Conference program 5 Plenary Talks 8 Bailey R. A., Latin cubes . 9 Cameron P. J., From de Bruijn graphs to automorphisms of the shift . 10 Gorshkov I. B., On Thompson’s conjecture for finite simple groups . 11 Ito T., The Weisfeiler–Leman stabilization revisited from the viewpoint of Terwilliger algebras . 12 Ivanov A. A., Densely embedded subgraphs in locally projective graphs . 13 Kabanov V. V., On strongly Deza graphs . 14 Khachay M. Yu., Efficient approximation of vehicle routing problems in metrics of a fixed doubling dimension . -
High-Girth Matrices and Polarization
High-Girth Matrices and Polarization Emmanuel Abbe Yuval Wigderson Prog. in Applied and Computational Math. and EE Dept. Department of Mathematics Princeton University Princeton University Email: [email protected] Email: [email protected] Abstract—The girth of a matrix is the least number of linearly requirement to be asymptotic, requiring rank(A) ∼ girth(A) 1 dependent columns, in contrast to the rank which is the largest when the number of columns in A tends to infinity. If F = F2, number of linearly independent columns. This paper considers the Gilbert-Varshamov bound provides a lower-bound on the the construction of high-girth matrices, whose probabilistic girth maximal girth (conjectured to be tight by some). Namely, is close to their rank. Random matrices can be used to show for a uniformly drawn matrix A with n columns, with high the existence of high-girth matrices. This paper uses a recursive probability, construction based on conditional ranks (inspired by polar codes) to obtain a deterministic and efficient construction of high- girth matrices for arbitrary relative ranks. Interestingly, the rank(A) = nH(girth(A)=n) + o(n); (3) construction is agnostic to the underlying field and applies to both finite and continuous fields with the same binary matrix. The where H is the binary entropy function. construction gives in particular the following: (i) over the binary For F = Fq, the bound in (1) is a restatement of the field, high-girth matrices are equivalent to capacity-achieving Singleton bound for linear codes and expressed in terms of the codes, and our construction turns out to match exactly the BEC co-dimension of the code. -
Spectra of Graphs
Spectra of graphs Andries E. Brouwer Willem H. Haemers 2 Contents 1 Graph spectrum 11 1.1 Matricesassociatedtoagraph . 11 1.2 Thespectrumofagraph ...................... 12 1.2.1 Characteristicpolynomial . 13 1.3 Thespectrumofanundirectedgraph . 13 1.3.1 Regulargraphs ........................ 13 1.3.2 Complements ......................... 14 1.3.3 Walks ............................. 14 1.3.4 Diameter ........................... 14 1.3.5 Spanningtrees ........................ 15 1.3.6 Bipartitegraphs ....................... 16 1.3.7 Connectedness ........................ 16 1.4 Spectrumofsomegraphs . 17 1.4.1 Thecompletegraph . 17 1.4.2 Thecompletebipartitegraph . 17 1.4.3 Thecycle ........................... 18 1.4.4 Thepath ........................... 18 1.4.5 Linegraphs .......................... 18 1.4.6 Cartesianproducts . 19 1.4.7 Kronecker products and bipartite double. 19 1.4.8 Strongproducts ....................... 19 1.4.9 Cayleygraphs......................... 20 1.5 Decompositions............................ 20 1.5.1 Decomposing K10 intoPetersengraphs . 20 1.5.2 Decomposing Kn into complete bipartite graphs . 20 1.6 Automorphisms ........................... 21 1.7 Algebraicconnectivity . 22 1.8 Cospectralgraphs .......................... 22 1.8.1 The4-cube .......................... 23 1.8.2 Seidelswitching. 23 1.8.3 Godsil-McKayswitching. 24 1.8.4 Reconstruction ........................ 24 1.9 Verysmallgraphs .......................... 24 1.10 Exercises ............................... 25 3 4 CONTENTS 2 Linear algebra 29 2.1 -
Equiangular Tight Frames with Simplices and with Full Spark in Rd
ISSN 1995-0802, Lobachevskii Journal of Mathematics, 2021, Vol. 42, No. 1, pp. 154–165. c Pleiades Publishing, Ltd., 2021. Equiangular Tight Frames with Simplices and with Full Spark in Rd S. Ya. Novikov1* (SubmittedbyA.M.Elizarov) 1Samara University, Samara, 443011 Russia Received May 23, 2020; revised August 19, 2020; accepted August 26, 2020 Abstract—An equiangular tight frame (ETF) is an equal norm tight frame with the same sharp angles between the vectors. This work is an attempt to create a brief review with complete proofs and calculations of two directions of research on the equiangular tight frames (ETF): bounds of the spark of the ETF, namely the smallest number of the vectors from ETF that are linearly dependent, and the existence of a regular simplex inside ETF. Tracing these two directions, we go through the case of equality in the Welch estimate, see the connection between RIP (restricted isometry property) and the spark of an ETF,construct a regular simplex using the technique of Naimark complements. We show the connection between equality in the lower estimate of the spark and the presence of a simplex inside ETF. Gram matrix and the matrix of the synthesis operator are calculated for the frame with 10 elements in the space R5. This frame contains a regular simplex and its spark is equal to 4, i.e. is not full. On the other hand you may see an example of the ETF with 6 vectors in R3 without a simplex, but with the spark equal to 4. In such cases the term “full spark” is used, so we have an example of the full spark ETF (FSETF). -
Sixth(A) Edition
A Mathematical Bibliography of Signed and Gain Graphs and Allied Areas Compiled by Thomas Zaslavsky Manuscript prepared with Marge Pratt Department of Mathematical Sciences Binghamton University Binghamton, New York, U.S.A. 13902-6000 E-mail: [email protected] Submitted: March 19, 1998; Accepted: July 20, 1998. Sixth Edition, Revision a 20 July 1998 Mathematical Subject Classifications (1991): Primary 05-02, 05C99; Secondary 05B20, 05B25, 05B35, 05C10, 05C15, 05C20, 05C25, 05C30, 05C35, 05C38, 05C45, 05C50, 05C60, 05C65, 05C70, 05C75, 05C80, 05C85, 05C90, 05E25, 05E30, 06A07, 06A09, 05C10, 15A06, 15A15, 15A39, 15A99, 20B25, 20F55, 34C11, 51D20, 51E20, 52B12, 52B30, 52B40, 52C07, 68Q15, 68Q25, 68Q35, 68R10, 82B20, 82D30, 90A08, 90B10, 90C08, 90C27, 90C35, 90C60, 92D40, 92E10, 92H30, 92J10, 92K10, 94B25. Colleagues: HELP! If you have any suggestions whatever for items to include in this bibliography, or for other changes, please let me hear from you. Thank you. Index A 1 H 48 O 83 V 110 B 8 I 59 P 84 W 111 C 20 J 60 Q 90 X 118 D 28 K 63 R 90 Y 118 E 32 L 71 S 94 Z 115 F 36 M 76 T 104 G 39 N 82 U 109 Preface A signed graph is a graph whose edges are labeled by signs. This is a bibliography of signed graphs and related mathematics. I regard as fundamental the notion of balance of a circuit (sign product equals +, the sign group identity) and the vertex-edge incidence matrix (whose column for a negative edge has two +1's or two −1's, for a positive edge one +1 and one −1, the rest being zero).