Compact Matrix Decomposition for Large Sparse Graphs
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On Multigrid Methods for Solving Electromagnetic Scattering Problems
On Multigrid Methods for Solving Electromagnetic Scattering Problems Dissertation zur Erlangung des akademischen Grades eines Doktor der Ingenieurwissenschaften (Dr.-Ing.) der Technischen Fakultat¨ der Christian-Albrechts-Universitat¨ zu Kiel vorgelegt von Simona Gheorghe 2005 1. Gutachter: Prof. Dr.-Ing. L. Klinkenbusch 2. Gutachter: Prof. Dr. U. van Rienen Datum der mundliche¨ Prufung:¨ 20. Jan. 2006 Contents 1 Introductory remarks 3 1.1 General introduction . 3 1.2 Maxwell’s equations . 6 1.3 Boundary conditions . 7 1.3.1 Sommerfeld’s radiation condition . 9 1.4 Scattering problem (Model Problem I) . 10 1.5 Discontinuity in a parallel-plate waveguide (Model Problem II) . 11 1.6 Absorbing-boundary conditions . 12 1.6.1 Global radiation conditions . 13 1.6.2 Local radiation conditions . 18 1.7 Summary . 19 2 Coupling of FEM-BEM 21 2.1 Introduction . 21 2.2 Finite element formulation . 21 2.2.1 Discretization . 26 2.3 Boundary-element formulation . 28 3 4 CONTENTS 2.4 Coupling . 32 3 Iterative solvers for sparse matrices 35 3.1 Introduction . 35 3.2 Classical iterative methods . 36 3.3 Krylov subspace methods . 37 3.3.1 General projection methods . 37 3.3.2 Krylov subspace methods . 39 3.4 Preconditioning . 40 3.4.1 Matrix-based preconditioners . 41 3.4.2 Operator-based preconditioners . 42 3.5 Multigrid . 43 3.5.1 Full Multigrid . 47 4 Numerical results 49 4.1 Coupling between FEM and local/global boundary conditions . 49 4.1.1 Model problem I . 50 4.1.2 Model problem II . 63 4.2 Multigrid . 64 4.2.1 Theoretical considerations regarding the classical multi- grid behavior in the case of an indefinite problem . -
Geometric Polarimetry − Part I: Spinors and Wave States
1 Geometric Polarimetry Part I: Spinors and − Wave States David Bebbington, Laura Carrea, and Ernst Krogager, Member, IEEE Abstract A new approach to polarization algebra is introduced. It exploits the geometric properties of spinors in order to represent wave states consistently in arbitrary directions in three dimensional space. In this first expository paper of an intended series the basic derivation of the spinorial wave state is seen to be geometrically related to the electromagnetic field tensor in the spatio-temporal Fourier domain. Extracting the polarization state from the electromagnetic field requires the introduction of a new element, which enters linearly into the defining relation. We call this element the phase flag and it is this that keeps track of the polarization reference when the coordinate system is changed and provides a phase origin for both wave components. In this way we are able to identify the sphere of three dimensional unit wave vectors with the Poincar´esphere. Index Terms state of polarization, geometry, covariant and contravariant spinors and tensors, bivectors, phase flag, Poincar´esphere. I. INTRODUCTION arXiv:0804.0745v1 [physics.optics] 4 Apr 2008 The development of applications in radar polarimetry has been vigorous over the past decade, and is anticipated to continue with ambitious new spaceborne remote sensing missions (for example TerraSAR-X [1] and TanDEM-X [2]). As technical capabilities increase, and new application areas open up, innovations in data analysis often result. Because polarization data are This work was supported by the Marie Curie Research Training Network AMPER (Contract number HPRN-CT-2002-00205). D. Bebbington and L. -
Sparse Matrices and Iterative Methods
Iterative Methods Sparsity Sparse Matrices and Iterative Methods K. Cooper1 1Department of Mathematics Washington State University 2018 Cooper Washington State University Introduction Iterative Methods Sparsity Iterative Methods Consider the problem of solving Ax = b, where A is n × n. Why would we use an iterative method? I Avoid direct decomposition (LU, QR, Cholesky) I Replace with iterated matrix multiplication 3 I LU is O(n ) flops. 2 I . matrix-vector multiplication is O(n )... I so if we can get convergence in e.g. log(n), iteration might be faster. Cooper Washington State University Introduction Iterative Methods Sparsity Jacobi, GS, SOR Some old methods: I Jacobi is easily parallelized. I . but converges extremely slowly. I Gauss-Seidel/SOR converge faster. I . but cannot be effectively parallelized. I Only Jacobi really takes advantage of sparsity. Cooper Washington State University Introduction Iterative Methods Sparsity Sparsity When a matrix is sparse (many more zero entries than nonzero), then typically the number of nonzero entries is O(n), so matrix-vector multiplication becomes an O(n) operation. This makes iterative methods very attractive. It does not help direct solves as much because of the problem of fill-in, but we note that there are specialized solvers to minimize fill-in. Cooper Washington State University Introduction Iterative Methods Sparsity Krylov Subspace Methods A class of methods that converge in n iterations (in exact arithmetic). We hope that they arrive at a solution that is “close enough” in fewer iterations. Often these work much better than the classic methods. They are more readily parallelized, and take full advantage of sparsity. -
Scalable Stochastic Kriging with Markovian Covariances
Scalable Stochastic Kriging with Markovian Covariances Liang Ding and Xiaowei Zhang∗ Department of Industrial Engineering and Decision Analytics The Hong Kong University of Science and Technology, Clear Water Bay, Hong Kong Abstract Stochastic kriging is a popular technique for simulation metamodeling due to its flexibility and analytical tractability. Its computational bottleneck is the inversion of a covariance matrix, which takes O(n3) time in general and becomes prohibitive for large n, where n is the number of design points. Moreover, the covariance matrix is often ill-conditioned for large n, and thus the inversion is prone to numerical instability, resulting in erroneous parameter estimation and prediction. These two numerical issues preclude the use of stochastic kriging at a large scale. This paper presents a novel approach to address them. We construct a class of covariance functions, called Markovian covariance functions (MCFs), which have two properties: (i) the associated covariance matrices can be inverted analytically, and (ii) the inverse matrices are sparse. With the use of MCFs, the inversion-related computational time is reduced to O(n2) in general, and can be further reduced by orders of magnitude with additional assumptions on the simulation errors and design points. The analytical invertibility also enhance the numerical stability dramatically. The key in our approach is that we identify a general functional form of covariance functions that can induce sparsity in the corresponding inverse matrices. We also establish a connection between MCFs and linear ordinary differential equations. Such a connection provides a flexible, principled approach to constructing a wide class of MCFs. Extensive numerical experiments demonstrate that stochastic kriging with MCFs can handle large-scale problems in an both computationally efficient and numerically stable manner. -
A Fast Method for Computing the Inverse of Symmetric Block Arrowhead Matrices
Appl. Math. Inf. Sci. 9, No. 2L, 319-324 (2015) 319 Applied Mathematics & Information Sciences An International Journal http://dx.doi.org/10.12785/amis/092L06 A Fast Method for Computing the Inverse of Symmetric Block Arrowhead Matrices Waldemar Hołubowski1, Dariusz Kurzyk1,∗ and Tomasz Trawi´nski2 1 Institute of Mathematics, Silesian University of Technology, Kaszubska 23, Gliwice 44–100, Poland 2 Mechatronics Division, Silesian University of Technology, Akademicka 10a, Gliwice 44–100, Poland Received: 6 Jul. 2014, Revised: 7 Oct. 2014, Accepted: 8 Oct. 2014 Published online: 1 Apr. 2015 Abstract: We propose an effective method to find the inverse of symmetric block arrowhead matrices which often appear in areas of applied science and engineering such as head-positioning systems of hard disk drives or kinematic chains of industrial robots. Block arrowhead matrices can be considered as generalisation of arrowhead matrices occurring in physical problems and engineering. The proposed method is based on LDLT decomposition and we show that the inversion of the large block arrowhead matrices can be more effective when one uses our method. Numerical results are presented in the examples. Keywords: matrix inversion, block arrowhead matrices, LDLT decomposition, mechatronic systems 1 Introduction thermal and many others. Considered subsystems are highly differentiated, hence formulation of uniform and simple mathematical model describing their static and A square matrix which has entries equal zero except for dynamic states becomes problematic. The process of its main diagonal, a one row and a column, is called the preparing a proper mathematical model is often based on arrowhead matrix. Wide area of applications causes that the formulation of the equations associated with this type of matrices is popular subject of research related Lagrangian formalism [9], which is a convenient way to with mathematics, physics or engineering, such as describe the equations of mechanical, electromechanical computing spectral decomposition [1], solving inverse and other components. -
Chapter 7 Iterative Methods for Large Sparse Linear Systems
Chapter 7 Iterative methods for large sparse linear systems In this chapter we revisit the problem of solving linear systems of equations, but now in the context of large sparse systems. The price to pay for the direct methods based on matrix factorization is that the factors of a sparse matrix may not be sparse, so that for large sparse systems the memory cost make direct methods too expensive, in memory and in execution time. Instead we introduce iterative methods, for which matrix sparsity is exploited to develop fast algorithms with a low memory footprint. 7.1 Sparse matrix algebra Large sparse matrices We say that the matrix A Rn is large if n is large, and that A is sparse if most of the elements are2 zero. If a matrix is not sparse, we say that the matrix is dense. Whereas for a dense matrix the number of nonzero elements is (n2), for a sparse matrix it is only (n), which has obvious implicationsO for the memory footprint and efficiencyO for algorithms that exploit the sparsity of a matrix. AdiagonalmatrixisasparsematrixA =(aij), for which aij =0for all i = j,andadiagonalmatrixcanbegeneralizedtoabanded matrix, 6 for which there exists a number p,thebandwidth,suchthataij =0forall i<j p or i>j+ p.Forexample,atridiagonal matrix A is a banded − 59 CHAPTER 7. ITERATIVE METHODS FOR LARGE SPARSE 60 LINEAR SYSTEMS matrix with p =1, xx0000 xxx000 20 xxx003 A = , (7.1) 600xxx07 6 7 6000xxx7 6 7 60000xx7 6 7 where x represents a nonzero4 element. 5 Compressed row storage The compressed row storage (CRS) format is a data structure for efficient represention of a sparse matrix by three arrays, containing the nonzero values, the respective column indices, and the extents of the rows. -
Structured Factorizations in Scalar Product Spaces
STRUCTURED FACTORIZATIONS IN SCALAR PRODUCT SPACES D. STEVEN MACKEY¤, NILOUFER MACKEYy , AND FRANC»OISE TISSEURz Abstract. Let A belong to an automorphism group, Lie algebra or Jordan algebra of a scalar product. When A is factored, to what extent do the factors inherit structure from A? We answer this question for the principal matrix square root, the matrix sign decomposition, and the polar decomposition. For general A, we give a simple derivation and characterization of a particular generalized polar decomposition, and we relate it to other such decompositions in the literature. Finally, we study eigendecompositions and structured singular value decompositions, considering in particular the structure in eigenvalues, eigenvectors and singular values that persists across a wide range of scalar products. A key feature of our analysis is the identi¯cation of two particular classes of scalar products, termed unitary and orthosymmetric, which serve to unify assumptions for the existence of structured factorizations. A variety of di®erent characterizations of these scalar product classes is given. Key words. automorphism group, Lie group, Lie algebra, Jordan algebra, bilinear form, sesquilinear form, scalar product, inde¯nite inner product, orthosymmetric, adjoint, factorization, symplectic, Hamiltonian, pseudo-orthogonal, polar decomposition, matrix sign function, matrix square root, generalized polar decomposition, eigenvalues, eigenvectors, singular values, structure preservation. AMS subject classi¯cations. 15A18, 15A21, 15A23, 15A57, -
A Parallel Solver for Graph Laplacians
A Parallel Solver for Graph Laplacians Tristan Konolige Jed Brown University of Colorado Boulder University of Colorado Boulder [email protected] ABSTRACT low energy components while maintaining coarse grid sparsity. We Problems from graph drawing, spectral clustering, network ow also develop a parallel algorithm for nding and eliminating low and graph partitioning can all be expressed in terms of graph Lapla- degree vertices, a technique introduced for a sequential multigrid cian matrices. ere are a variety of practical approaches to solving algorithm by Livne and Brandt [22], that is important for irregular these problems in serial. However, as problem sizes increase and graphs. single core speeds stagnate, parallelism is essential to solve such While matrices can be distributed using a vertex partition (a problems quickly. We present an unsmoothed aggregation multi- 1D/row distribution) for PDE problems, this leads to unacceptable grid method for solving graph Laplacians in a distributed memory load imbalance for irregular graphs. We represent matrices using a seing. We introduce new parallel aggregation and low degree elim- 2D distribution (a partition of the edges) that maintains load balance ination algorithms targeted specically at irregular degree graphs. for parallel scaling [11]. Many algorithms that are practical for 1D ese algorithms are expressed in terms of sparse matrix-vector distributions are not feasible for more general distributions. Our products using generalized sum and product operations. is for- new parallel algorithms are distribution agnostic. mulation is amenable to linear algebra using arbitrary distributions and allows us to operate on a 2D sparse matrix distribution, which 2 BACKGROUND is necessary for parallel scalability. -
Solving Linear Systems: Iterative Methods and Sparse Systems
Solving Linear Systems: Iterative Methods and Sparse Systems COS 323 Last time • Linear system: Ax = b • Singular and ill-conditioned systems • Gaussian Elimination: A general purpose method – Naïve Gauss (no pivoting) – Gauss with partial and full pivoting – Asymptotic analysis: O(n3) • Triangular systems and LU decomposition • Special matrices and algorithms: – Symmetric positive definite: Cholesky decomposition – Tridiagonal matrices • Singularity detection and condition numbers Today: Methods for large and sparse systems • Rank-one updating with Sherman-Morrison • Iterative refinement • Fixed-point and stationary methods – Introduction – Iterative refinement as a stationary method – Gauss-Seidel and Jacobi methods – Successive over-relaxation (SOR) • Solving a system as an optimization problem • Representing sparse systems Problems with large systems • Gaussian elimination, LU decomposition (factoring step) take O(n3) • Expensive for big systems! • Can get by more easily with special matrices – Cholesky decomposition: for symmetric positive definite A; still O(n3) but halves storage and operations – Band-diagonal: O(n) storage and operations • What if A is big? (And not diagonal?) Special Example: Cyclic Tridiagonal • Interesting extension: cyclic tridiagonal • Could derive yet another special case algorithm, but there’s a better way Updating Inverse • Suppose we have some fast way of finding A-1 for some matrix A • Now A changes in a special way: A* = A + uvT for some n×1 vectors u and v • Goal: find a fast way of computing (A*)-1 -
Linear Algebra - Part II Projection, Eigendecomposition, SVD
Linear Algebra - Part II Projection, Eigendecomposition, SVD (Adapted from Punit Shah's slides) 2019 Linear Algebra, Part II 2019 1 / 22 Brief Review from Part 1 Matrix Multiplication is a linear tranformation. Symmetric Matrix: A = AT Orthogonal Matrix: AT A = AAT = I and A−1 = AT L2 Norm: s X 2 jjxjj2 = xi i Linear Algebra, Part II 2019 2 / 22 Angle Between Vectors Dot product of two vectors can be written in terms of their L2 norms and the angle θ between them. T a b = jjajj2jjbjj2 cos(θ) Linear Algebra, Part II 2019 3 / 22 Cosine Similarity Cosine between two vectors is a measure of their similarity: a · b cos(θ) = jjajj jjbjj Orthogonal Vectors: Two vectors a and b are orthogonal to each other if a · b = 0. Linear Algebra, Part II 2019 4 / 22 Vector Projection ^ b Given two vectors a and b, let b = jjbjj be the unit vector in the direction of b. ^ Then a1 = a1 · b is the orthogonal projection of a onto a straight line parallel to b, where b a = jjajj cos(θ) = a · b^ = a · 1 jjbjj Image taken from wikipedia. Linear Algebra, Part II 2019 5 / 22 Diagonal Matrix Diagonal matrix has mostly zeros with non-zero entries only in the diagonal, e.g. identity matrix. A square diagonal matrix with diagonal elements given by entries of vector v is denoted: diag(v) Multiplying vector x by a diagonal matrix is efficient: diag(v)x = v x is the entrywise product. Inverting a square diagonal matrix is efficient: 1 1 diag(v)−1 = diag [ ;:::; ]T v1 vn Linear Algebra, Part II 2019 6 / 22 Determinant Determinant of a square matrix is a mapping to a scalar. -
Unit 6: Matrix Decomposition
Unit 6: Matrix decomposition Juan Luis Melero and Eduardo Eyras October 2018 1 Contents 1 Matrix decomposition3 1.1 Definitions.............................3 2 Singular Value Decomposition6 3 Exercises 13 4 R practical 15 4.1 SVD................................ 15 2 1 Matrix decomposition 1.1 Definitions Matrix decomposition consists in transforming a matrix into a product of other matrices. Matrix diagonalization is a special case of decomposition and is also called diagonal (eigen) decomposition of a matrix. Definition: there is a diagonal decomposition of a square matrix A if we can write A = UDU −1 Where: • D is a diagonal matrix • The diagonal elements of D are the eigenvalues of A • Vector columns of U are the eigenvectors of A. For symmetric matrices there is a special decomposition: Definition: given a symmetric matrix A (i.e. AT = A), there is a unique decomposition of the form A = UDU T Where • U is an orthonormal matrix • Vector columns of U are the unit-norm orthogonal eigenvectors of A • D is a diagonal matrix formed by the eigenvalues of A This special decomposition is known as spectral decomposition. Definition: An orthonormal matrix is a square matrix whose columns and row vectors are orthogonal unit vectors (orthonormal vectors). Orthonormal matrices have the property that their transposed matrix is the inverse matrix. 3 Proposition: if a matrix Q is orthonormal, then QT = Q−1 Proof: consider the row vectors in a matrix Q: 0 1 u1 B . C T u j ::: ju Q = @ . A and Q = 1 n un 0 1 0 1 0 1 u1 hu1; u1i ::: hu1; uni 1 ::: 0 T B . -
High Performance Selected Inversion Methods for Sparse Matrices
High performance selected inversion methods for sparse matrices Direct and stochastic approaches to selected inversion Doctoral Dissertation submitted to the Faculty of Informatics of the Università della Svizzera italiana in partial fulfillment of the requirements for the degree of Doctor of Philosophy presented by Fabio Verbosio under the supervision of Olaf Schenk February 2019 Dissertation Committee Illia Horenko Università della Svizzera italiana, Switzerland Igor Pivkin Università della Svizzera italiana, Switzerland Matthias Bollhöfer Technische Universität Braunschweig, Germany Laura Grigori INRIA Paris, France Dissertation accepted on 25 February 2019 Research Advisor PhD Program Director Olaf Schenk Walter Binder i I certify that except where due acknowledgement has been given, the work presented in this thesis is that of the author alone; the work has not been sub- mitted previously, in whole or in part, to qualify for any other academic award; and the content of the thesis is the result of work which has been carried out since the official commencement date of the approved research program. Fabio Verbosio Lugano, 25 February 2019 ii To my whole family. In its broadest sense. iii iv Le conoscenze matematiche sono proposizioni costruite dal nostro intelletto in modo da funzionare sempre come vere, o perché sono innate o perché la matematica è stata inventata prima delle altre scienze. E la biblioteca è stata costruita da una mente umana che pensa in modo matematico, perché senza matematica non fai labirinti. Umberto Eco, “Il nome della rosa” v vi Abstract The explicit evaluation of selected entries of the inverse of a given sparse ma- trix is an important process in various application fields and is gaining visibility in recent years.