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Eigenvalues of Euclidean Distance Matrices and Rs-Majorization on R2
Archive of SID 46th Annual Iranian Mathematics Conference 25-28 August 2015 Yazd University 2 Talk Eigenvalues of Euclidean distance matrices and rs-majorization on R pp.: 1{4 Eigenvalues of Euclidean Distance Matrices and rs-majorization on R2 Asma Ilkhanizadeh Manesh∗ Department of Pure Mathematics, Vali-e-Asr University of Rafsanjan Alemeh Sheikh Hoseini Department of Pure Mathematics, Shahid Bahonar University of Kerman Abstract Let D1 and D2 be two Euclidean distance matrices (EDMs) with correspond- ing positive semidefinite matrices B1 and B2 respectively. Suppose that λ(A) = ((λ(A)) )n is the vector of eigenvalues of a matrix A such that (λ(A)) ... i i=1 1 ≥ ≥ (λ(A))n. In this paper, the relation between the eigenvalues of EDMs and those of the 2 corresponding positive semidefinite matrices respect to rs, on R will be investigated. ≺ Keywords: Euclidean distance matrices, Rs-majorization. Mathematics Subject Classification [2010]: 34B15, 76A10 1 Introduction An n n nonnegative and symmetric matrix D = (d2 ) with zero diagonal elements is × ij called a predistance matrix. A predistance matrix D is called Euclidean or a Euclidean distance matrix (EDM) if there exist a positive integer r and a set of n points p1, . , pn r 2 2 { } such that p1, . , pn R and d = pi pj (i, j = 1, . , n), where . denotes the ∈ ij k − k k k usual Euclidean norm. The smallest value of r that satisfies the above condition is called the embedding dimension. As is well known, a predistance matrix D is Euclidean if and 1 1 t only if the matrix B = − P DP with P = I ee , where I is the n n identity matrix, 2 n − n n × and e is the vector of all ones, is positive semidefinite matrix. -
Quantum Information
Quantum Information J. A. Jones Michaelmas Term 2010 Contents 1 Dirac Notation 3 1.1 Hilbert Space . 3 1.2 Dirac notation . 4 1.3 Operators . 5 1.4 Vectors and matrices . 6 1.5 Eigenvalues and eigenvectors . 8 1.6 Hermitian operators . 9 1.7 Commutators . 10 1.8 Unitary operators . 11 1.9 Operator exponentials . 11 1.10 Physical systems . 12 1.11 Time-dependent Hamiltonians . 13 1.12 Global phases . 13 2 Quantum bits and quantum gates 15 2.1 The Bloch sphere . 16 2.2 Density matrices . 16 2.3 Propagators and Pauli matrices . 18 2.4 Quantum logic gates . 18 2.5 Gate notation . 21 2.6 Quantum networks . 21 2.7 Initialization and measurement . 23 2.8 Experimental methods . 24 3 An atom in a laser field 25 3.1 Time-dependent systems . 25 3.2 Sudden jumps . 26 3.3 Oscillating fields . 27 3.4 Time-dependent perturbation theory . 29 3.5 Rabi flopping and Fermi's Golden Rule . 30 3.6 Raman transitions . 32 3.7 Rabi flopping as a quantum gate . 32 3.8 Ramsey fringes . 33 3.9 Measurement and initialisation . 34 1 CONTENTS 2 4 Spins in magnetic fields 35 4.1 The nuclear spin Hamiltonian . 35 4.2 The rotating frame . 36 4.3 On-resonance excitation . 38 4.4 Excitation phases . 38 4.5 Off-resonance excitation . 39 4.6 Practicalities . 40 4.7 The vector model . 40 4.8 Spin echoes . 41 4.9 Measurement and initialisation . 42 5 Photon techniques 43 5.1 Spatial encoding . -
Boundary Value Problems on Weighted Paths
Introduction and basic concepts BVP on weighted paths Bibliography Boundary value problems on a weighted path Angeles Carmona, Andr´esM. Encinas and Silvia Gago Depart. Matem`aticaAplicada 3, UPC, Barcelona, SPAIN Midsummer Combinatorial Workshop XIX Prague, July 29th - August 3rd, 2013 MCW 2013, A. Carmona, A.M. Encinas and S.Gago Boundary value problems on a weighted path Introduction and basic concepts BVP on weighted paths Bibliography Outline of the talk Notations and definitions Weighted graphs and matrices Schr¨odingerequations Boundary value problems on weighted graphs Green matrix of the BVP Boundary Value Problems on paths Paths with constant potential Orthogonal polynomials Schr¨odingermatrix of the weighted path associated to orthogonal polynomials Two-side Boundary Value Problems in weighted paths MCW 2013, A. Carmona, A.M. Encinas and S.Gago Boundary value problems on a weighted path Introduction and basic concepts Schr¨odingerequations BVP on weighted paths Definition of BVP Bibliography Weighted graphs A weighted graphΓ=( V ; E; c) is composed by: V is a set of elements called vertices. E is a set of elements called edges. c : V × V −! [0; 1) is an application named conductance associated to the edges. u, v are adjacent, u ∼ v iff c(u; v) = cuv 6= 0. X The degree of a vertex u is du = cuv . v2V c34 u4 u1 c12 u2 c23 u3 c45 c35 c27 u5 c56 u7 c67 u6 MCW 2013, A. Carmona, A.M. Encinas and S.Gago Boundary value problems on a weighted path Introduction and basic concepts Schr¨odingerequations BVP on weighted paths Definition of BVP Bibliography Matrices associated with graphs Definition The weighted Laplacian matrix of a weighted graph Γ is defined as di if i = j; (L)ij = −cij if i 6= j: c34 u4 u c u c u 1 12 2 23 3 0 d1 −c12 0 0 0 0 0 1 c B −c12 d2 −c23 0 0 0 −c27 C 45 B C c B 0 −c23 d3 −c34 −c35 0 0 C 35 B C c27 L = B 0 0 −c34 d4 −c45 0 0 C B C u5 B 0 0 −c35 −c45 d5 −c56 0 C c56 @ 0 0 0 0 −c56 d6 −c67 A 0 −c27 0 0 0 −c67 d7 u7 c67 u6 MCW 2013, A. -
Polynomial Approximation Algorithms for Belief Matrix Maintenance in Identity Management
Polynomial Approximation Algorithms for Belief Matrix Maintenance in Identity Management Hamsa Balakrishnan, Inseok Hwang, Claire J. Tomlin Dept. of Aeronautics and Astronautics, Stanford University, CA 94305 hamsa,ishwang,[email protected] Abstract— Updating probabilistic belief matrices as new might be constrained to some prespecified (but not doubly- observations arrive, in the presence of noise, is a critical part stochastic) row and column sums. This paper addresses the of many algorithms for target tracking in sensor networks. problem of updating belief matrices by scaling in the face These updates have to be carried out while preserving sum constraints, arising for example, from probabilities. This paper of uncertainty in the system and the observations. addresses the problem of updating belief matrices to satisfy For example, consider the case of the belief matrix for a sum constraints using scaling algorithms. We show that the system with three objects (labelled 1, 2 and 3). Suppose convergence behavior of the Sinkhorn scaling process, used that, at some instant, we are unsure about their identities for scaling belief matrices, can vary dramatically depending (tagged X, Y and Z) completely, and our belief matrix is on whether the prior unscaled matrix is exactly scalable or only almost scalable. We give an efficient polynomial-time algo- a 3 × 3 matrix with every element equal to 1/3. Let us rithm based on the maximum-flow algorithm that determines suppose the we receive additional information that object whether a given matrix is exactly scalable, thus determining 3 is definitely Z. Then our prior, but constraint violating the convergence properties of the Sinkhorn scaling process. -
MATH 237 Differential Equations and Computer Methods
Queen’s University Mathematics and Engineering and Mathematics and Statistics MATH 237 Differential Equations and Computer Methods Supplemental Course Notes Serdar Y¨uksel November 19, 2010 This document is a collection of supplemental lecture notes used for Math 237: Differential Equations and Computer Methods. Serdar Y¨uksel Contents 1 Introduction to Differential Equations 7 1.1 Introduction: ................................... ....... 7 1.2 Classification of Differential Equations . ............... 7 1.2.1 OrdinaryDifferentialEquations. .......... 8 1.2.2 PartialDifferentialEquations . .......... 8 1.2.3 Homogeneous Differential Equations . .......... 8 1.2.4 N-thorderDifferentialEquations . ......... 8 1.2.5 LinearDifferentialEquations . ......... 8 1.3 Solutions of Differential equations . .............. 9 1.4 DirectionFields................................. ........ 10 1.5 Fundamental Questions on First-Order Differential Equations............... 10 2 First-Order Ordinary Differential Equations 11 2.1 ExactDifferentialEquations. ........... 11 2.2 MethodofIntegratingFactors. ........... 12 2.3 SeparableDifferentialEquations . ............ 13 2.4 Differential Equations with Homogenous Coefficients . ................ 13 2.5 First-Order Linear Differential Equations . .............. 14 2.6 Applications.................................... ....... 14 3 Higher-Order Ordinary Linear Differential Equations 15 3.1 Higher-OrderDifferentialEquations . ............ 15 3.1.1 LinearIndependence . ...... 16 3.1.2 WronskianofasetofSolutions . ........ 16 3.1.3 Non-HomogeneousProblem -
The Exponential of a Matrix
5-28-2012 The Exponential of a Matrix The solution to the exponential growth equation dx kt = kx is given by x = c e . dt 0 It is natural to ask whether you can solve a constant coefficient linear system ′ ~x = A~x in a similar way. If a solution to the system is to have the same form as the growth equation solution, it should look like At ~x = e ~x0. The first thing I need to do is to make sense of the matrix exponential eAt. The Taylor series for ez is ∞ n z z e = . n! n=0 X It converges absolutely for all z. It A is an n × n matrix with real entries, define ∞ n n At t A e = . n! n=0 X The powers An make sense, since A is a square matrix. It is possible to show that this series converges for all t and every matrix A. Differentiating the series term-by-term, ∞ ∞ ∞ ∞ n−1 n n−1 n n−1 n−1 m m d At t A t A t A t A At e = n = = A = A = Ae . dt n! (n − 1)! (n − 1)! m! n=0 n=1 n=1 m=0 X X X X At ′ This shows that e solves the differential equation ~x = A~x. The initial condition vector ~x(0) = ~x0 yields the particular solution At ~x = e ~x0. This works, because e0·A = I (by setting t = 0 in the power series). Another familiar property of ordinary exponentials holds for the matrix exponential: If A and B com- mute (that is, AB = BA), then A B A B e e = e + . -
On the Eigenvalues of Euclidean Distance Matrices
“main” — 2008/10/13 — 23:12 — page 237 — #1 Volume 27, N. 3, pp. 237–250, 2008 Copyright © 2008 SBMAC ISSN 0101-8205 www.scielo.br/cam On the eigenvalues of Euclidean distance matrices A.Y. ALFAKIH∗ Department of Mathematics and Statistics University of Windsor, Windsor, Ontario N9B 3P4, Canada E-mail: [email protected] Abstract. In this paper, the notion of equitable partitions (EP) is used to study the eigenvalues of Euclidean distance matrices (EDMs). In particular, EP is used to obtain the characteristic poly- nomials of regular EDMs and non-spherical centrally symmetric EDMs. The paper also presents methods for constructing cospectral EDMs and EDMs with exactly three distinct eigenvalues. Mathematical subject classification: 51K05, 15A18, 05C50. Key words: Euclidean distance matrices, eigenvalues, equitable partitions, characteristic poly- nomial. 1 Introduction ( ) An n ×n nonzero matrix D = di j is called a Euclidean distance matrix (EDM) 1, 2,..., n r if there exist points p p p in some Euclidean space < such that i j 2 , ,..., , di j = ||p − p || for all i j = 1 n where || || denotes the Euclidean norm. i , ,..., Let p , i ∈ N = {1 2 n}, be the set of points that generate an EDM π π ( , ,..., ) D. An m-partition of D is an ordered sequence = N1 N2 Nm of ,..., nonempty disjoint subsets of N whose union is N. The subsets N1 Nm are called the cells of the partition. The n-partition of D where each cell consists #760/08. Received: 07/IV/08. Accepted: 17/VI/08. ∗Research supported by the Natural Sciences and Engineering Research Council of Canada and MITACS. -
Smith Normal Formal of Distance Matrix of Block Graphs∗†
Ann. of Appl. Math. 32:1(2016); 20-29 SMITH NORMAL FORMAL OF DISTANCE MATRIX OF BLOCK GRAPHS∗y Jing Chen1;2,z Yaoping Hou2 (1. The Center of Discrete Math., Fuzhou University, Fujian 350003, PR China; 2. School of Math., Hunan First Normal University, Hunan 410205, PR China) Abstract A connected graph, whose blocks are all cliques (of possibly varying sizes), is called a block graph. Let D(G) be its distance matrix. In this note, we prove that the Smith normal form of D(G) is independent of the interconnection way of blocks and give an explicit expression for the Smith normal form in the case that all cliques have the same size, which generalize the results on determinants. Keywords block graph; distance matrix; Smith normal form 2000 Mathematics Subject Classification 05C50 1 Introduction Let G be a connected graph (or strong connected digraph) with vertex set f1; 2; ··· ; ng. The distance matrix D(G) is an n × n matrix in which di;j = d(i; j) denotes the distance from vertex i to vertex j: Like the adjacency matrix and Lapla- cian matrix of a graph, D(G) is also an integer matrix and there are many results on distance matrices and their applications. For distance matrices, Graham and Pollack [10] proved a remarkable result that gives a formula of the determinant of the distance matrix of a tree depend- ing only on the number n of vertices of the tree. The determinant is given by det D = (−1)n−1(n − 1)2n−2: This result has attracted much interest in algebraic graph theory. -
Variants of the Graph Laplacian with Applications in Machine Learning
Variants of the Graph Laplacian with Applications in Machine Learning Sven Kurras Dissertation zur Erlangung des Grades des Doktors der Naturwissenschaften (Dr. rer. nat.) im Fachbereich Informatik der Fakult¨at f¨urMathematik, Informatik und Naturwissenschaften der Universit¨atHamburg Hamburg, Oktober 2016 Diese Promotion wurde gef¨ordertdurch die Deutsche Forschungsgemeinschaft, Forschergruppe 1735 \Structural Inference in Statistics: Adaptation and Efficiency”. Betreuung der Promotion durch: Prof. Dr. Ulrike von Luxburg Tag der Disputation: 22. M¨arz2017 Vorsitzender des Pr¨ufungsausschusses: Prof. Dr. Matthias Rarey 1. Gutachterin: Prof. Dr. Ulrike von Luxburg 2. Gutachter: Prof. Dr. Wolfgang Menzel Zusammenfassung In s¨amtlichen Lebensbereichen finden sich Graphen. Zum Beispiel verbringen Menschen viel Zeit mit der Kantentraversierung des Internet-Graphen. Weitere Beispiele f¨urGraphen sind soziale Netzwerke, ¨offentlicher Nahverkehr, Molek¨ule, Finanztransaktionen, Fischernetze, Familienstammb¨aume,sowie der Graph, in dem alle Paare nat¨urlicher Zahlen gleicher Quersumme durch eine Kante verbunden sind. Graphen k¨onnendurch ihre Adjazenzmatrix W repr¨asentiert werden. Dar¨uber hinaus existiert eine Vielzahl alternativer Graphmatrizen. Viele strukturelle Eigenschaften von Graphen, beispielsweise ihre Kreisfreiheit, Anzahl Spannb¨aume,oder Random Walk Hitting Times, spiegeln sich auf die ein oder andere Weise in algebraischen Eigenschaften ihrer Graphmatrizen wider. Diese grundlegende Verflechtung erlaubt das Studium von Graphen unter Verwendung s¨amtlicher Resultate der Linearen Algebra, angewandt auf Graphmatrizen. Spektrale Graphentheorie studiert Graphen insbesondere anhand der Eigenwerte und Eigenvektoren ihrer Graphmatrizen. Dabei ist vor allem die Laplace-Matrix L = D − W von Bedeutung, aber es gibt derer viele Varianten, zum Beispiel die normalisierte Laplacian, die vorzeichenlose Laplacian und die Diplacian. Die meisten Varianten basieren auf einer \syntaktisch kleinen" Anderung¨ von L, etwa D +W anstelle von D −W . -
![Arxiv:1803.06211V1 [Math.NA] 16 Mar 2018](https://docslib.b-cdn.net/cover/2225/arxiv-1803-06211v1-math-na-16-mar-2018-382225.webp)
Arxiv:1803.06211V1 [Math.NA] 16 Mar 2018
A NUMERICAL MODEL FOR THE CONSTRUCTION OF FINITE BLASCHKE PRODUCTS WITH PREASSIGNED DISTINCT CRITICAL POINTS CHRISTER GLADER AND RAY PORN¨ Abstract. We present a numerical model for determining a finite Blaschke product of degree n + 1 having n preassigned distinct critical points z1; : : : ; zn in the complex (open) unit disk D. The Blaschke product is uniquely determined up to postcomposition with conformal automor- phisms of D. The proposed method is based on the construction of a sparse nonlinear system where the data dependency is isolated to two vectors and on a certain transformation of the critical points. The effi- ciency and accuracy of the method is illustrated in several examples. 1. Introduction A finite Blaschke product of degree n is a rational function of the form n Y z − αj (1.1) B(z) = c ; c; α 2 ; jcj = 1; jα j < 1 ; 1 − α z j C j j=1 j which thereby has all its zeros in the open unit disc D, all poles outside the closed unit disc D and constant modulus jB(z)j = 1 on the unit circle T. The overbar in (1.1) and in the sequel stands for complex conjugation. The finite Blaschke products of degree n form a subset of the rational functions of degree n which are unimodular on T. These functions are given by all fractions n ~ a0 + a1 z + ::: + an z (1.2) B(z) = n ; a0; :::; an 2 C : an + an−1 z + ::: + a0 z An irreducible rational function of form (1.2) is a finite Blaschke product when all its zeros are in D. -
The Exponential Function for Matrices
The exponential function for matrices Matrix exponentials provide a concise way of describing the solutions to systems of homoge- neous linear differential equations that parallels the use of ordinary exponentials to solve simple differential equations of the form y0 = λ y. For square matrices the exponential function can be defined by the same sort of infinite series used in calculus courses, but some work is needed in order to justify the construction of such an infinite sum. Therefore we begin with some material needed to prove that certain infinite sums of matrices can be defined in a mathematically sound manner and have reasonable properties. Limits and infinite series of matrices Limits of vector valued sequences in Rn can be defined and manipulated much like limits of scalar valued sequences, the key adjustment being that distances between real numbers that are expressed in the form js−tj are replaced by distances between vectors expressed in the form jx−yj. 1 Similarly, one can talk about convergence of a vector valued infinite series n=0 vn in terms of n the convergence of the sequence of partial sums sn = i=0 vk. As in the case of ordinary infinite series, the best form of convergence is absolute convergence, which correspondsP to the convergence 1 P of the real valued infinite series jvnj with nonnegative terms. A fundamental theorem states n=0 1 that a vector valued infinite series converges if the auxiliary series jvnj does, and there is P n=0 a generalization of the standard M-test: If jvnj ≤ Mn for all n where Mn converges, then P n vn also converges. -
Approximating the Exponential from a Lie Algebra to a Lie Group
MATHEMATICS OF COMPUTATION Volume 69, Number 232, Pages 1457{1480 S 0025-5718(00)01223-0 Article electronically published on March 15, 2000 APPROXIMATING THE EXPONENTIAL FROM A LIE ALGEBRA TO A LIE GROUP ELENA CELLEDONI AND ARIEH ISERLES 0 Abstract. Consider a differential equation y = A(t; y)y; y(0) = y0 with + y0 2 GandA : R × G ! g,whereg is a Lie algebra of the matricial Lie group G. Every B 2 g canbemappedtoGbythematrixexponentialmap exp (tB)witht 2 R. Most numerical methods for solving ordinary differential equations (ODEs) on Lie groups are based on the idea of representing the approximation yn of + the exact solution y(tn), tn 2 R , by means of exact exponentials of suitable elements of the Lie algebra, applied to the initial value y0. This ensures that yn 2 G. When the exponential is difficult to compute exactly, as is the case when the dimension is large, an approximation of exp (tB) plays an important role in the numerical solution of ODEs on Lie groups. In some cases rational or poly- nomial approximants are unsuitable and we consider alternative techniques, whereby exp (tB) is approximated by a product of simpler exponentials. In this paper we present some ideas based on the use of the Strang splitting for the approximation of matrix exponentials. Several cases of g and G are considered, in tandem with general theory. Order conditions are discussed, and a number of numerical experiments conclude the paper. 1. Introduction Consider the differential equation (1.1) y0 = A(t; y)y; y(0) 2 G; with A : R+ × G ! g; where G is a matricial Lie group and g is the underlying Lie algebra.