H 2 -matrices with adaptive bases

Size: px
Start display at page:

Download "H 2 -matrices with adaptive bases"

Transcription

1 1 H 2 -matrices with adaptive bases Steffen Börm MPI für Mathematik in den Naturwissenschaften Inselstraße 22 26, Leipzig

2 Problem 2 Goal: Treat certain large dense matrices in linear complexity. Model problem: Discretization of integral operators of the form K[u](x) = κ(x, y)u(y) dy. Ω Discretization: Galerkin method with FE basis (ϕ i ) n i=1 leads to a matrix K R n n with K ij = ϕ i, K[ϕ j ] L 2 = ϕ i (x)κ(x, y)ϕ j (y) dy dx. (1 i, j n) Ω Ω Problem: K is dense. Idea: Use properties of the kernel function to approximate K. Examples: Wavelets, multipole expansion, interpolation.

3 Interpolation 3 Idea: We consider a subdomain τ σ Ω Ω and replace the kernel function κ by an interpolant κ τ,σ (x, y) := k k κ(x τ ν, x σ µ)l τ ν(x)l σ µ(y). (k n) ν=1 µ=1 Result: Local matrix in factorized form K τ,σ ij := ϕ i (x)κ(x, y)ϕ j (y) dy dx = τ k σ k ν=1 µ=1 κ(x τ ν, x σ µ) } {{ } =:Sνµ τ,σ = (V τ S τ,σ (V σ ) ) ij τ ϕ i (x)l τ ν(x) dx τ } {{ } =:Viν τ σ ϕ i (x) κ τ,σ (x, y)ϕ j (y) dy dx ϕ j (y)l σ µ(y) dy σ } {{ } =:Vjµ σ n k n k

4 Local interpolation 4 Problem: Typical kernel functions are not globally smooth. Idea: They are locally smooth outside of the diagonal x = y. Examples: 1/ x y, log x y. Error bound: For m-th order tensor interpolation on axis-parallel boxes B τ τ and B σ σ, we get ( κ τ,σ κ L (B τ B σ ) C apx (m) dist(bτ, B σ ) m ) diam(b τ B σ. ) Rank: m interpolation points per coordinate k = m d. Admissibility: Uniform exponential convergence requires diam(b τ B σ ) 2η dist(b τ, B σ ).

5 Block structure 5 Approach: Split Ω Ω into admissible subdomains and a small remainder. Cluster tree: Hierarchy of subdomains of Ω Nearfield: Small blocks, stored in standard format. Farfield: Admissible blocks, stored in V τ S τ,σ (V σ ) format. Partition: Collection of farand nearfield blocks. Construction of cluster tree and block partition can be accomplished by general algorithms in O(n) operations.

6 Nested bases 6 Goal: Treat the cluster basis (V τ ) τ T efficiently. Idea: For a cluster τ and τ sons(τ) we have L τ ν = k ν =1 L τ ν(x τ ν )Lτ. (1 ν k) ν Nested bases: Consider i τ τ. Setting T τ ν ν := Lτ ν(x τ ν ), we find k V τ iν = τ ϕ i (x)l τ ν(x) dx = ν =1 T τ ν ν τ ϕ i (x)l τ ν (x) dx = (V τ T τ ) iν. Consequence: Store V τ only for leaves and use T τ for all other clusters. Complexity: Storage O(nk), matrixvector O(nk).

7 Orthogonalization 7 Problem: Efficiency depends on the rank k. Can we reduce this rank by eliminating redundant expansion functions? Idea: Orthogonalize columns of V τ. Gram-Schmidt: Find Ṽ τ = V τ Z τ such that (Ṽ τ ) Ṽ τ = I holds. Nested structure: Using P τ with V τ = Ṽ τ P τ, we find V τ = V τ 1 T τ 1 = Ṽ τ 1 P τ 1 T τ 1 = Ṽ τ 1 V τ 2 T τ 2 Ṽ τ 2 P τ 2 T τ 2 Ṽ τ 2 = Ṽ τ V τ Z τ P τ 1 T τ 1, P τ 2 T τ 2 so it is sufficient to orthogonalize a (2k) k matrix. The resulting cluster basis is nested due to Ṽ τ = V τ Z τ = Ṽ τ 1 (P τ 1 T τ 1 Z τ ) = Ṽ τ 1 T τ 1. Ṽ τ 2 (P τ 2 T τ 2 Z τ ) Ṽ τ 2 τ T 2 Result: Complexity O(nk 2 ).

8 Orthogonalization: Simple example 8 Example: Unit sphere, piecewise constant trial and test functions. Interpolation Orthogonalized n Build MVM Mem/n Expl Impl MVM Mem/n H 2 -matrix constructed by cubic interpolation and subsequent orthogonalization, relative error Hardware: SunFire 6800 with 900 MHz UltraSparc IIIcu processors Software: HLib, see

9 Recompression algorithm: Problem 9 Problem: Interpolation does not take into account that a subset of polynomials may be sufficient to approximate the kernel function. Idea: Use local singular value decompositions to find optimal cluster bases Take kernel and geometry into account. Important: Since the cluster bases are nested, the father clusters depend on the son clusters. Consequence: If τ σ is a farfield block and τ sons(τ), we have K τ σ = (V τ S τ,σ (V σ ) ) τ σ = V τ T τ S τ,σ (V σ ), i.e., the choice of V τ its other ancestors. influences all farfield blocks connected to τ or

10 Recompression algorithm: Local problems and recursion 10 Block row: R τ := {σ : τ + τ : τ + σ is admissible}. Goal: Find an orthogonal matrix V τ R τ kτ that maximizes σ R τ (V τ ) K τ σ 2 F. Optimal solution: Use eigenvectors of corresponding Gram matrix. Nested structure: Ensured by bottom-up recursion and projections. Result: Algorithm with complexity O(nk 2 ), truncation error can be controlled directly.

11 Recompression: Simple example 11 Example: Unit sphere, piecewise constant trial and test functions. Interpolation Recompressed n Build MVM Mem/n Build MVM Mem/n H 2 -matrix constructed by cubic interpolation. Recompression with relative error bound 10 3, maximal rank 16. Hardware: SunFire 6800 with 900 MHz UltraSparc IIIcu processors. Software: HLib, see

12 Recompression: Netgen example 12 Example: Grid Crank shaft of the Netgen package. n Build Mem/n Near/n MVM Rel. error 0.05% 0.07% 0.08% DMem/n

13 Recompression: Netgen geometries and eddy current model 13 Z Z b(v, φ) = Γ Z φ(y), v(x) x Φ(x, y), n(x) dy dx Z φ(y),n(x) x Φ(x, y), v(x) dy dx Γ Γ Γ n Direct MVM Mem/DoF Recompressed MVM Mem/DoF Rel. error

14 Summary 14 H 2 -matrices: Nested structure leads to complexity O(nk) for storage requirements and matrix-vector multiplication. Black box: The approximation is constructed by using only kernel evaluations κ(x τ ν, x σ µ) and works for all asymptotically smooth kernel functions. Recompression: Use O(nk 2 ) algorithm to reduce the rank k, find a quasi-optimal cluster basis adapted to geometry, discretization and kernel function. Work in progress: H 2 -matrix arithmetics, HCA.

15 H 2 -matrix arithmetics 15 Goal: Perform matrix addition and multiplication efficiently. Addition and scaling: For an admissible block τ σ, we have (A + λb) τ σ = V τ (S τ,σ A + λsτ,σ B )(V σ ), so H 2 -matrices form a vector space. Addition and scaling can be performed in O(nk) operations. ( + λ ) Multiplication: Defined recursively. A 11 A 12 B 11 B 12 = A 11B 11 + A 12 B 21 A 11 B 12 + A 12 B 22 A 21 A 22 B 21 B 22 A 21 B 11 + A 22 B 21 A 21 B 12 + A 22 B 22 Use truncation if product does not match prescribed format.

16 H 2 -matrix multiplication I 16 := Situation: Let A = V τ S τ,ϱ A (V ϱ ), B not admissible. Compute best approximation of AB in the form C = V τ S τ,σ C (V σ ). Orthogonality: If V τ and V σ are orthogonal: S τ,σ C = (V τ ) ABV σ = (V τ ) V τ S τ,ϱ A (V ϱ ) BV σ = S τ,ϱ A (V ϱ ) BV σ. }{{} =: S ϱ,σ B Problem: Computing (V ϱ ) BV σ directly is too expensive. Idea: Prepare S ϱ,σ B := (V ϱ ) BV σ in advance. Matrix forward transformation: Since the cluster bases are nested, all matrices can be prepared in O(nk3 ) operations. S ϱ,σ B

17 H 2 -matrix multiplication II 17 := Situation: Let A = V τ S τ,ϱ A (V ϱ ) and B = V ϱ S ϱ,σ B (V σ ). Advantage: The product AB already has the factorized form AB = V τ S τ,ϱ A (V ϱ ) V ϱ S ϱ,σ B (V σ ) = V τ (S τ,ϱ A Sϱ,σ B )(V σ ). Problem: Converting AB directly to the format of C will lead to inacceptable complexity. S τ,σ C Idea: Store result in multiplication is complete. := S τ,ϱ A Sϱ,σ B and distribute after the Matrix backward transformation: Since the cluster bases are nested, all matrices can be distributed in O(nk3 ) operations. S τ,σ C

18 H 2 -matrix multiplication III 18 := Situation: Let B = V ϱ S ϱ,σ B (V σ ). Approach: Split B and proceed by recursion: B ϱ σ = V ϱ T ϱ S ϱ,σ B (T σ ) (V σ ). }{{} =: bs ϱ,σ B Complexity: Only O(Cspn) 2 such splitting operations are required Complexity O(Cspnk 2 3 ). Result: The best approximation C of AB in a prescribed H 2 -matrix format can be computed in O(C 2 spnk 3 ) operations.

19 H 2 -matrix multiplication: Fixed structure 19 Example: Discretized double layer potential on the unit sphere K, approximate KK. n Build C sp H 2 -MVM H 2 -MMM H-MMM Error < Important: Here, the result matrix is projected to the same cluster bases and the same block structure as K. Question: Can we reduce the error by using adapted cluster bases?

20 H 2 -matrix multiplication: Adapted structure 20 Modification: Choose cluster bases for result matrix adaptively to improve the precision. n C sp Old MMM Error New basis New MMM Error Advantage: Precision significantly improved, computation time only slightly increased. Current work: Improve the efficiency of the construction of adapted cluster bases.

21 Hybrid Cross Approximation 21 Problem: For each admissble block V τ S τ,σ (V σ ) of the H 2 -matrix, the kernel function κ has to be evaluated in m 2d points. Very time-consuming if high precision is required. Approach: Apply adaptive cross approximation to the coefficient matrices S τ,σ to find rank k representation S τ,σ X τ,σ (Y τ,σ ). Result: Only m d k m 2d kernel evaluations required to approximate coefficient matrix S τ,σ. Important: ACA is only applied to coefficient matrices. Construction still linear in n, no problems with quadrature. m Std 24.1s 64.7s 160.8s 399.2s HCA 22.3s 49.2s 90.0s 222.7s

22 Conclusion 22 H 2 -matrices: Data-sparse approximation of certain dense matrices with linear complexity in the number of degrees of freedom. Adaptive cluster bases: Find quasi-optimal expansion systems for arbitrary matrices. In the case of integral operators, point evaluations of the kernel function are sufficient to construct efficient and reliable H 2 -matrix approximations. H 2 -matrix arithmetics: Approximate A + λb and AB in O(nk 2 ) and O(nk 3 ) operations. Next goal: Approximate A 1 and LU. HCA: Reduce the number of kernel evaluations required to construct the H 2 -matrix. Software: HLib package for hierarchical matrices and H 2 -matrices, including applications to elliptic PDEs and integral equations.

23 Interpolation vs. Multipole 23 Construction: Pointwise evaluation and integrals of polynomials. Tν t ν = L t ν(x t ν ), S t,s νµ = κ(x t ν, x s µ), Viν t = ϕ i (x)l t ν(x) dx. Interpolation Multipole - Rank k = p d + Rank k = p d 1 - Low frequencies only + Low and high frequencies + General kernels - Special kernels only + Anisotropic clusters - Spherical clusters only Γ Goal: Reduce rank for interpolation without sacrificing precision.

Fast evaluation of boundary integral operators arising from an eddy current problem. MPI MIS Leipzig

Fast evaluation of boundary integral operators arising from an eddy current problem. MPI MIS Leipzig 1 Fast evaluation of boundary integral operators arising from an eddy current problem Steffen Börm MPI MIS Leipzig Jörg Ostrowski ETH Zürich Induction heating 2 Induction heating: Time harmonic eddy current

More information

für Mathematik in den Naturwissenschaften Leipzig

für Mathematik in den Naturwissenschaften Leipzig Max-Planck-Institut für Mathematik in den Naturwissenschaften Leipzig Approximation of integral operators by H 2 -matrices with adaptive bases (revised version: December 2004) by Steffen Börm Preprint

More information

Max-Planck-Institut fur Mathematik in den Naturwissenschaften Leipzig H 2 -matrix approximation of integral operators by interpolation by Wolfgang Hackbusch and Steen Borm Preprint no.: 04 200 H 2 -Matrix

More information

APPROXIMATING GAUSSIAN PROCESSES

APPROXIMATING GAUSSIAN PROCESSES 1 / 23 APPROXIMATING GAUSSIAN PROCESSES WITH H 2 -MATRICES Steffen Börm 1 Jochen Garcke 2 1 Christian-Albrechts-Universität zu Kiel 2 Universität Bonn and Fraunhofer SCAI 2 / 23 OUTLINE 1 GAUSSIAN PROCESSES

More information

Hierarchical Matrices. Jon Cockayne April 18, 2017

Hierarchical Matrices. Jon Cockayne April 18, 2017 Hierarchical Matrices Jon Cockayne April 18, 2017 1 Sources Introduction to Hierarchical Matrices with Applications [Börm et al., 2003] 2 Sources Introduction to Hierarchical Matrices with Applications

More information

Karhunen-Loève Approximation of Random Fields Using Hierarchical Matrix Techniques

Karhunen-Loève Approximation of Random Fields Using Hierarchical Matrix Techniques Institut für Numerische Mathematik und Optimierung Karhunen-Loève Approximation of Random Fields Using Hierarchical Matrix Techniques Oliver Ernst Computational Methods with Applications Harrachov, CR,

More information

für Mathematik in den Naturwissenschaften Leipzig

für Mathematik in den Naturwissenschaften Leipzig Max-Planck-Institut für Mathematik in den Naturwissenschaften Leipzig Introduction to Hierarchical Matrices with Applications by Steffen Börm, Lars Grasedyck, and Wolfgang Hackbusch Preprint no.: 18 2002

More information

Hierarchical matrix techniques for low and high frequency Helmholtz problems

Hierarchical matrix techniques for low and high frequency Helmholtz problems Hierarchical matrix techniques for low and high frequency Helmholtz problems Lehel Banjai Wolfgang Hackbusch 12th December 2006 Abstract In this paper, we discuss the application of hierarchical matrix

More information

Math 671: Tensor Train decomposition methods

Math 671: Tensor Train decomposition methods Math 671: Eduardo Corona 1 1 University of Michigan at Ann Arbor December 8, 2016 Table of Contents 1 Preliminaries and goal 2 Unfolding matrices for tensorized arrays The Tensor Train decomposition 3

More information

Fast matrix algebra for dense matrices with rank-deficient off-diagonal blocks

Fast matrix algebra for dense matrices with rank-deficient off-diagonal blocks CHAPTER 2 Fast matrix algebra for dense matrices with rank-deficient off-diagonal blocks Chapter summary: The chapter describes techniques for rapidly performing algebraic operations on dense matrices

More information

Max-Planck-Institut für Mathematik in den Naturwissenschaften Leipzig

Max-Planck-Institut für Mathematik in den Naturwissenschaften Leipzig Max-Planck-Institut für Mathematik in den Naturwissenschaften Leipzig Hierarchical matrices and the High-Frequency Fast Multipole Method for the Helmholtz Equation with Decay revised version: March 014)

More information

THE H 2 -matrix is a general mathematical framework [1],

THE H 2 -matrix is a general mathematical framework [1], Accuracy Directly Controlled Fast Direct Solutions of General H -Matrices and ts Application to Electrically Large ntegral-equation-based Electromagnetic Analysis Miaomiao Ma, Student Member, EEE, and

More information

MULTI-LAYER HIERARCHICAL STRUCTURES AND FACTORIZATIONS

MULTI-LAYER HIERARCHICAL STRUCTURES AND FACTORIZATIONS MULTI-LAYER HIERARCHICAL STRUCTURES AND FACTORIZATIONS JIANLIN XIA Abstract. We propose multi-layer hierarchically semiseparable MHS structures for the fast factorizations of dense matrices arising from

More information

Hybrid Cross Approximation for the Electric Field Integral Equation

Hybrid Cross Approximation for the Electric Field Integral Equation Progress In Electromagnetics Research M, Vol. 75, 79 90, 2018 Hybrid Cross Approximation for the Electric Field Integral Equation Priscillia Daquin, Ronan Perrussel, and Jean-René Poirier * Abstract The

More information

An H-LU Based Direct Finite Element Solver Accelerated by Nested Dissection for Large-scale Modeling of ICs and Packages

An H-LU Based Direct Finite Element Solver Accelerated by Nested Dissection for Large-scale Modeling of ICs and Packages PIERS ONLINE, VOL. 6, NO. 7, 2010 679 An H-LU Based Direct Finite Element Solver Accelerated by Nested Dissection for Large-scale Modeling of ICs and Packages Haixin Liu and Dan Jiao School of Electrical

More information

Theory and implementation of H-matrix based iterative and direct solvers for Helmholtz and elastodynamic oscillatory kernels

Theory and implementation of H-matrix based iterative and direct solvers for Helmholtz and elastodynamic oscillatory kernels Theory and implementation of H-matrix based iterative and direct solvers for Helmholtz and elastodynamic oscillatory kernels Stéphanie Chaillat, Luca Desiderio, Patrick Ciarlet To cite this version: Stéphanie

More information

Fast Multipole BEM for Structural Acoustics Simulation

Fast Multipole BEM for Structural Acoustics Simulation Fast Boundary Element Methods in Industrial Applications Fast Multipole BEM for Structural Acoustics Simulation Matthias Fischer and Lothar Gaul Institut A für Mechanik, Universität Stuttgart, Germany

More information

The Conjugate Gradient Method

The Conjugate Gradient Method The Conjugate Gradient Method Classical Iterations We have a problem, We assume that the matrix comes from a discretization of a PDE. The best and most popular model problem is, The matrix will be as large

More information

COMPARED to other computational electromagnetic

COMPARED to other computational electromagnetic IEEE TRANSACTIONS ON MICROWAVE THEORY AND TECHNIQUES, VOL. 58, NO. 12, DECEMBER 2010 3697 Existence of -Matrix Representations of the Inverse Finite-Element Matrix of Electrodynamic Problems and -Based

More information

Lecture 1: Center for Uncertainty Quantification. Alexander Litvinenko. Computation of Karhunen-Loeve Expansion:

Lecture 1: Center for Uncertainty Quantification. Alexander Litvinenko. Computation of Karhunen-Loeve Expansion: tifica Lecture 1: Computation of Karhunen-Loeve Expansion: Alexander Litvinenko http://sri-uq.kaust.edu.sa/ Stochastic PDEs We consider div(κ(x, ω) u) = f (x, ω) in G, u = 0 on G, with stochastic coefficients

More information

Fast Structured Spectral Methods

Fast Structured Spectral Methods Spectral methods HSS structures Fast algorithms Conclusion Fast Structured Spectral Methods Yingwei Wang Department of Mathematics, Purdue University Joint work with Prof Jie Shen and Prof Jianlin Xia

More information

A Fast N-Body Solver for the Poisson(-Boltzmann) Equation

A Fast N-Body Solver for the Poisson(-Boltzmann) Equation A Fast N-Body Solver for the Poisson(-Boltzmann) Equation Robert D. Skeel Departments of Computer Science (and Mathematics) Purdue University http://bionum.cs.purdue.edu/2008december.pdf 1 Thesis Poisson(-Boltzmann)

More information

An Introduction to Hierachical (H ) Rank and TT Rank of Tensors with Examples

An Introduction to Hierachical (H ) Rank and TT Rank of Tensors with Examples An Introduction to Hierachical (H ) Rank and TT Rank of Tensors with Examples Lars Grasedyck and Wolfgang Hackbusch Bericht Nr. 329 August 2011 Key words: MSC: hierarchical Tucker tensor rank tensor approximation

More information

Numerical Solutions to Partial Differential Equations

Numerical Solutions to Partial Differential Equations Numerical Solutions to Partial Differential Equations Zhiping Li LMAM and School of Mathematical Sciences Peking University Numerical Methods for Partial Differential Equations Finite Difference Methods

More information

Lecture 8: Boundary Integral Equations

Lecture 8: Boundary Integral Equations CBMS Conference on Fast Direct Solvers Dartmouth College June 23 June 27, 2014 Lecture 8: Boundary Integral Equations Gunnar Martinsson The University of Colorado at Boulder Research support by: Consider

More information

Teil 2: Hierarchische Matrizen

Teil 2: Hierarchische Matrizen Teil 2: Hierarchische Matrizen Mario Bebendorf, Universität Leipzig bebendorf@math.uni-leipzig.de Bebendorf, Mario (Univ. Leipzig) Kompaktkurs lineare GS und H-Matrizen 24. 2. April 2 1 / 1 1 1 2 1 2 2

More information

Master Thesis Literature Review: Efficiency Improvement for Panel Codes. TU Delft MARIN

Master Thesis Literature Review: Efficiency Improvement for Panel Codes. TU Delft MARIN Master Thesis Literature Review: Efficiency Improvement for Panel Codes TU Delft MARIN Elisa Ang Yun Mei Student Number: 4420888 1-27-2015 CONTENTS 1 Introduction... 1 1.1 Problem Statement... 1 1.2 Current

More information

Contents. Preface... xi. Introduction...

Contents. Preface... xi. Introduction... Contents Preface... xi Introduction... xv Chapter 1. Computer Architectures... 1 1.1. Different types of parallelism... 1 1.1.1. Overlap, concurrency and parallelism... 1 1.1.2. Temporal and spatial parallelism

More information

Contents. Preface to the Third Edition (2007) Preface to the Second Edition (1992) Preface to the First Edition (1985) License and Legal Information

Contents. Preface to the Third Edition (2007) Preface to the Second Edition (1992) Preface to the First Edition (1985) License and Legal Information Contents Preface to the Third Edition (2007) Preface to the Second Edition (1992) Preface to the First Edition (1985) License and Legal Information xi xiv xvii xix 1 Preliminaries 1 1.0 Introduction.............................

More information

Wavelets in Scattering Calculations

Wavelets in Scattering Calculations Wavelets in Scattering Calculations W. P., Brian M. Kessler, Gerald L. Payne polyzou@uiowa.edu The University of Iowa Wavelets in Scattering Calculations p.1/43 What are Wavelets? Orthonormal basis functions.

More information

Experiences with Model Reduction and Interpolation

Experiences with Model Reduction and Interpolation Experiences with Model Reduction and Interpolation Paul Constantine Stanford University, Sandia National Laboratories Qiqi Wang (MIT) David Gleich (Purdue) Emory University March 7, 2012 Joe Ruthruff (SNL)

More information

4. Numerical Quadrature. Where analytical abilities end... continued

4. Numerical Quadrature. Where analytical abilities end... continued 4. Numerical Quadrature Where analytical abilities end... continued Where analytical abilities end... continued, November 30, 22 1 4.3. Extrapolation Increasing the Order Using Linear Combinations Once

More information

Numerical methods for PDEs FEM convergence, error estimates, piecewise polynomials

Numerical methods for PDEs FEM convergence, error estimates, piecewise polynomials Platzhalter für Bild, Bild auf Titelfolie hinter das Logo einsetzen Numerical methods for PDEs FEM convergence, error estimates, piecewise polynomials Dr. Noemi Friedman Contents of the course Fundamentals

More information

Math 671: Tensor Train decomposition methods II

Math 671: Tensor Train decomposition methods II Math 671: Tensor Train decomposition methods II Eduardo Corona 1 1 University of Michigan at Ann Arbor December 13, 2016 Table of Contents 1 What we ve talked about so far: 2 The Tensor Train decomposition

More information

LECTURE NOTES ELEMENTARY NUMERICAL METHODS. Eusebius Doedel

LECTURE NOTES ELEMENTARY NUMERICAL METHODS. Eusebius Doedel LECTURE NOTES on ELEMENTARY NUMERICAL METHODS Eusebius Doedel TABLE OF CONTENTS Vector and Matrix Norms 1 Banach Lemma 20 The Numerical Solution of Linear Systems 25 Gauss Elimination 25 Operation Count

More information

An Adaptive Hierarchical Matrix on Point Iterative Poisson Solver

An Adaptive Hierarchical Matrix on Point Iterative Poisson Solver Malaysian Journal of Mathematical Sciences 10(3): 369 382 (2016) MALAYSIAN JOURNAL OF MATHEMATICAL SCIENCES Journal homepage: http://einspem.upm.edu.my/journal An Adaptive Hierarchical Matrix on Point

More information

Fast Numerical Methods for Stochastic Computations

Fast Numerical Methods for Stochastic Computations Fast AreviewbyDongbinXiu May 16 th,2013 Outline Motivation 1 Motivation 2 3 4 5 Example: Burgers Equation Let us consider the Burger s equation: u t + uu x = νu xx, x [ 1, 1] u( 1) =1 u(1) = 1 Example:

More information

A New Scheme for the Tensor Representation

A New Scheme for the Tensor Representation J Fourier Anal Appl (2009) 15: 706 722 DOI 10.1007/s00041-009-9094-9 A New Scheme for the Tensor Representation W. Hackbusch S. Kühn Received: 18 December 2008 / Revised: 29 June 2009 / Published online:

More information

A High-Order Galerkin Solver for the Poisson Problem on the Surface of the Cubed Sphere

A High-Order Galerkin Solver for the Poisson Problem on the Surface of the Cubed Sphere A High-Order Galerkin Solver for the Poisson Problem on the Surface of the Cubed Sphere Michael Levy University of Colorado at Boulder Department of Applied Mathematics August 10, 2007 Outline 1 Background

More information

Practical Linear Algebra: A Geometry Toolbox

Practical Linear Algebra: A Geometry Toolbox Practical Linear Algebra: A Geometry Toolbox Third edition Chapter 12: Gauss for Linear Systems Gerald Farin & Dianne Hansford CRC Press, Taylor & Francis Group, An A K Peters Book www.farinhansford.com/books/pla

More information

PARTIAL DIFFERENTIAL EQUATIONS

PARTIAL DIFFERENTIAL EQUATIONS MATHEMATICAL METHODS PARTIAL DIFFERENTIAL EQUATIONS I YEAR B.Tech By Mr. Y. Prabhaker Reddy Asst. Professor of Mathematics Guru Nanak Engineering College Ibrahimpatnam, Hyderabad. SYLLABUS OF MATHEMATICAL

More information

Lecture 9 Approximations of Laplace s Equation, Finite Element Method. Mathématiques appliquées (MATH0504-1) B. Dewals, C.

Lecture 9 Approximations of Laplace s Equation, Finite Element Method. Mathématiques appliquées (MATH0504-1) B. Dewals, C. Lecture 9 Approximations of Laplace s Equation, Finite Element Method Mathématiques appliquées (MATH54-1) B. Dewals, C. Geuzaine V1.2 23/11/218 1 Learning objectives of this lecture Apply the finite difference

More information

MATHEMATICAL METHODS INTERPOLATION

MATHEMATICAL METHODS INTERPOLATION MATHEMATICAL METHODS INTERPOLATION I YEAR BTech By Mr Y Prabhaker Reddy Asst Professor of Mathematics Guru Nanak Engineering College Ibrahimpatnam, Hyderabad SYLLABUS OF MATHEMATICAL METHODS (as per JNTU

More information

Preliminary Examination, Numerical Analysis, August 2016

Preliminary Examination, Numerical Analysis, August 2016 Preliminary Examination, Numerical Analysis, August 2016 Instructions: This exam is closed books and notes. The time allowed is three hours and you need to work on any three out of questions 1-4 and any

More information

Adaptive Finite Element Methods Lecture Notes Winter Term 2017/18. R. Verfürth. Fakultät für Mathematik, Ruhr-Universität Bochum

Adaptive Finite Element Methods Lecture Notes Winter Term 2017/18. R. Verfürth. Fakultät für Mathematik, Ruhr-Universität Bochum Adaptive Finite Element Methods Lecture Notes Winter Term 2017/18 R. Verfürth Fakultät für Mathematik, Ruhr-Universität Bochum Contents Chapter I. Introduction 7 I.1. Motivation 7 I.2. Sobolev and finite

More information

Applied/Numerical Analysis Qualifying Exam

Applied/Numerical Analysis Qualifying Exam Applied/Numerical Analysis Qualifying Exam August 9, 212 Cover Sheet Applied Analysis Part Policy on misprints: The qualifying exam committee tries to proofread exams as carefully as possible. Nevertheless,

More information

Part IB Numerical Analysis

Part IB Numerical Analysis Part IB Numerical Analysis Definitions Based on lectures by G. Moore Notes taken by Dexter Chua Lent 206 These notes are not endorsed by the lecturers, and I have modified them (often significantly) after

More information

Solving an Elliptic PDE Eigenvalue Problem via Automated Multi-Level Substructuring and Hierarchical Matrices

Solving an Elliptic PDE Eigenvalue Problem via Automated Multi-Level Substructuring and Hierarchical Matrices Solving an Elliptic PDE Eigenvalue Problem via Automated Multi-Level Substructuring and Hierarchical Matrices Peter Gerds and Lars Grasedyck Bericht Nr. 30 März 2014 Key words: automated multi-level substructuring,

More information

The Lanczos and conjugate gradient algorithms

The Lanczos and conjugate gradient algorithms The Lanczos and conjugate gradient algorithms Gérard MEURANT October, 2008 1 The Lanczos algorithm 2 The Lanczos algorithm in finite precision 3 The nonsymmetric Lanczos algorithm 4 The Golub Kahan bidiagonalization

More information

FINITE-DIMENSIONAL LINEAR ALGEBRA

FINITE-DIMENSIONAL LINEAR ALGEBRA DISCRETE MATHEMATICS AND ITS APPLICATIONS Series Editor KENNETH H ROSEN FINITE-DIMENSIONAL LINEAR ALGEBRA Mark S Gockenbach Michigan Technological University Houghton, USA CRC Press Taylor & Francis Croup

More information

Lecture 6. Numerical methods. Approximation of functions

Lecture 6. Numerical methods. Approximation of functions Lecture 6 Numerical methods Approximation of functions Lecture 6 OUTLINE 1. Approximation and interpolation 2. Least-square method basis functions design matrix residual weighted least squares normal equation

More information

für Mathematik in den Naturwissenschaften Leipzig

für Mathematik in den Naturwissenschaften Leipzig ŠܹÈÐ Ò ¹ÁÒ Ø ØÙØ für Mathematik in den Naturwissenschaften Leipzig Nonlinear multigrid for the solution of large scale Riccati equations in low-rank and H-matrix format (revised version: May 2007) by

More information

A Hybrid Method for the Wave Equation. beilina

A Hybrid Method for the Wave Equation.   beilina A Hybrid Method for the Wave Equation http://www.math.unibas.ch/ beilina 1 The mathematical model The model problem is the wave equation 2 u t 2 = (a 2 u) + f, x Ω R 3, t > 0, (1) u(x, 0) = 0, x Ω, (2)

More information

Lecture 1: Introduction to low-rank tensor representation/approximation. Center for Uncertainty Quantification. Alexander Litvinenko

Lecture 1: Introduction to low-rank tensor representation/approximation. Center for Uncertainty Quantification. Alexander Litvinenko tifica Lecture 1: Introduction to low-rank tensor representation/approximation Alexander Litvinenko http://sri-uq.kaust.edu.sa/ KAUST Figure : KAUST campus, 5 years old, approx. 7000 people (include 1400

More information

Chapter Two: Numerical Methods for Elliptic PDEs. 1 Finite Difference Methods for Elliptic PDEs

Chapter Two: Numerical Methods for Elliptic PDEs. 1 Finite Difference Methods for Elliptic PDEs Chapter Two: Numerical Methods for Elliptic PDEs Finite Difference Methods for Elliptic PDEs.. Finite difference scheme. We consider a simple example u := subject to Dirichlet boundary conditions ( ) u

More information

Tensor-Product Representation of Operators and Functions (7 introductory lectures) Boris N. Khoromskij

Tensor-Product Representation of Operators and Functions (7 introductory lectures) Boris N. Khoromskij 1 Everything should be made as simple as possible, but not simpler. A. Einstein (1879-1955) Tensor-Product Representation of Operators and Functions (7 introductory lectures) Boris N. Khoromskij University

More information

Fast Direct Methods for Gaussian Processes

Fast Direct Methods for Gaussian Processes Fast Direct Methods for Gaussian Processes Mike O Neil Departments of Mathematics New York University oneil@cims.nyu.edu December 12, 2015 1 Collaborators This is joint work with: Siva Ambikasaran Dan

More information

Accuracy, Precision and Efficiency in Sparse Grids

Accuracy, Precision and Efficiency in Sparse Grids John, Information Technology Department, Virginia Tech.... http://people.sc.fsu.edu/ jburkardt/presentations/ sandia 2009.pdf... Computer Science Research Institute, Sandia National Laboratory, 23 July

More information

Applied Linear Algebra in Geoscience Using MATLAB

Applied Linear Algebra in Geoscience Using MATLAB Applied Linear Algebra in Geoscience Using MATLAB Contents Getting Started Creating Arrays Mathematical Operations with Arrays Using Script Files and Managing Data Two-Dimensional Plots Programming in

More information

Recurrence Relations and Fast Algorithms

Recurrence Relations and Fast Algorithms Recurrence Relations and Fast Algorithms Mark Tygert Research Report YALEU/DCS/RR-343 December 29, 2005 Abstract We construct fast algorithms for decomposing into and reconstructing from linear combinations

More information

MODEL REDUCTION BY A CROSS-GRAMIAN APPROACH FOR DATA-SPARSE SYSTEMS

MODEL REDUCTION BY A CROSS-GRAMIAN APPROACH FOR DATA-SPARSE SYSTEMS MODEL REDUCTION BY A CROSS-GRAMIAN APPROACH FOR DATA-SPARSE SYSTEMS Ulrike Baur joint work with Peter Benner Mathematics in Industry and Technology Faculty of Mathematics Chemnitz University of Technology

More information

Scientific Computing with Case Studies SIAM Press, Lecture Notes for Unit VII Sparse Matrix

Scientific Computing with Case Studies SIAM Press, Lecture Notes for Unit VII Sparse Matrix Scientific Computing with Case Studies SIAM Press, 2009 http://www.cs.umd.edu/users/oleary/sccswebpage Lecture Notes for Unit VII Sparse Matrix Computations Part 1: Direct Methods Dianne P. O Leary c 2008

More information

Pascal s Triangle on a Budget. Accuracy, Precision and Efficiency in Sparse Grids

Pascal s Triangle on a Budget. Accuracy, Precision and Efficiency in Sparse Grids Covering : Accuracy, Precision and Efficiency in Sparse Grids https://people.sc.fsu.edu/ jburkardt/presentations/auburn 2009.pdf... John Interdisciplinary Center for Applied Mathematics & Information Technology

More information

1. Structured representation of high-order tensors revisited. 2. Multi-linear algebra (MLA) with Kronecker-product data.

1. Structured representation of high-order tensors revisited. 2. Multi-linear algebra (MLA) with Kronecker-product data. Lect. 4. Toward MLA in tensor-product formats B. Khoromskij, Leipzig 2007(L4) 1 Contents of Lecture 4 1. Structured representation of high-order tensors revisited. - Tucker model. - Canonical (PARAFAC)

More information

Stabilization and Acceleration of Algebraic Multigrid Method

Stabilization and Acceleration of Algebraic Multigrid Method Stabilization and Acceleration of Algebraic Multigrid Method Recursive Projection Algorithm A. Jemcov J.P. Maruszewski Fluent Inc. October 24, 2006 Outline 1 Need for Algorithm Stabilization and Acceleration

More information

Numerical methods for PDEs FEM convergence, error estimates, piecewise polynomials

Numerical methods for PDEs FEM convergence, error estimates, piecewise polynomials Platzhalter für Bild, Bild auf Titelfolie hinter das Logo einsetzen Numerical methods for PDEs FEM convergence, error estimates, piecewise polynomials Dr. Noemi Friedman Contents of the course Fundamentals

More information

homogeneous 71 hyperplane 10 hyperplane 34 hyperplane 69 identity map 171 identity map 186 identity map 206 identity matrix 110 identity matrix 45

homogeneous 71 hyperplane 10 hyperplane 34 hyperplane 69 identity map 171 identity map 186 identity map 206 identity matrix 110 identity matrix 45 address 12 adjoint matrix 118 alternating 112 alternating 203 angle 159 angle 33 angle 60 area 120 associative 180 augmented matrix 11 axes 5 Axiom of Choice 153 basis 178 basis 210 basis 74 basis test

More information

The Fast Multipole Method and other Fast Summation Techniques

The Fast Multipole Method and other Fast Summation Techniques The Fast Multipole Method and other Fast Summation Techniques Gunnar Martinsson The University of Colorado at Boulder (The factor of 1/2π is suppressed.) Problem definition: Consider the task of evaluation

More information

SOLVING SPARSE LINEAR SYSTEMS OF EQUATIONS. Chao Yang Computational Research Division Lawrence Berkeley National Laboratory Berkeley, CA, USA

SOLVING SPARSE LINEAR SYSTEMS OF EQUATIONS. Chao Yang Computational Research Division Lawrence Berkeley National Laboratory Berkeley, CA, USA 1 SOLVING SPARSE LINEAR SYSTEMS OF EQUATIONS Chao Yang Computational Research Division Lawrence Berkeley National Laboratory Berkeley, CA, USA 2 OUTLINE Sparse matrix storage format Basic factorization

More information

Numerical Methods for Partial Differential Equations

Numerical Methods for Partial Differential Equations Numerical Methods for Partial Differential Equations Steffen Börm Compiled July 12, 2018, 12:01 All rights reserved. Contents 1. Introduction 5 2. Finite difference methods 7 2.1. Potential equation.............................

More information

Application of the LLL Algorithm in Sphere Decoding

Application of the LLL Algorithm in Sphere Decoding Application of the LLL Algorithm in Sphere Decoding Sanzheng Qiao Department of Computing and Software McMaster University August 20, 2008 Outline 1 Introduction Application Integer Least Squares 2 Sphere

More information

Scientific Computing I

Scientific Computing I Scientific Computing I Module 8: An Introduction to Finite Element Methods Tobias Neckel Winter 2013/2014 Module 8: An Introduction to Finite Element Methods, Winter 2013/2014 1 Part I: Introduction to

More information

A Recursive Trust-Region Method for Non-Convex Constrained Minimization

A Recursive Trust-Region Method for Non-Convex Constrained Minimization A Recursive Trust-Region Method for Non-Convex Constrained Minimization Christian Groß 1 and Rolf Krause 1 Institute for Numerical Simulation, University of Bonn. {gross,krause}@ins.uni-bonn.de 1 Introduction

More information

Sparse BLAS-3 Reduction

Sparse BLAS-3 Reduction Sparse BLAS-3 Reduction to Banded Upper Triangular (Spar3Bnd) Gary Howell, HPC/OIT NC State University gary howell@ncsu.edu Sparse BLAS-3 Reduction p.1/27 Acknowledgements James Demmel, Gene Golub, Franc

More information

A fast randomized algorithm for computing a Hierarchically Semi-Separable representation of a matrix

A fast randomized algorithm for computing a Hierarchically Semi-Separable representation of a matrix A fast randomized algorithm for computing a Hierarchically Semi-Separable representation of a matrix P.G. Martinsson, Department of Applied Mathematics, University of Colorado at Boulder Abstract: Randomized

More information

Solving Boundary Value Problems (with Gaussians)

Solving Boundary Value Problems (with Gaussians) What is a boundary value problem? Solving Boundary Value Problems (with Gaussians) Definition A differential equation with constraints on the boundary Michael McCourt Division Argonne National Laboratory

More information

Fast Multipole Methods for The Laplace Equation. Outline

Fast Multipole Methods for The Laplace Equation. Outline Fast Multipole Methods for The Laplace Equation Ramani Duraiswami Nail Gumerov Outline 3D Laplace equation and Coulomb potentials Multipole and local expansions Special functions Legendre polynomials Associated

More information

Conjugate Gradient Method

Conjugate Gradient Method Conjugate Gradient Method direct and indirect methods positive definite linear systems Krylov sequence spectral analysis of Krylov sequence preconditioning Prof. S. Boyd, EE364b, Stanford University Three

More information

INFINITE ELEMENT METHODS FOR HELMHOLTZ EQUATION PROBLEMS ON UNBOUNDED DOMAINS

INFINITE ELEMENT METHODS FOR HELMHOLTZ EQUATION PROBLEMS ON UNBOUNDED DOMAINS INFINITE ELEMENT METHODS FOR HELMHOLTZ EQUATION PROBLEMS ON UNBOUNDED DOMAINS Michael Newman Department of Aerospace Engineering Texas A&M University 34 TAMU 744D H.R. Bright Building College Station,

More information

Domain Decomposition Preconditioners for Spectral Nédélec Elements in Two and Three Dimensions

Domain Decomposition Preconditioners for Spectral Nédélec Elements in Two and Three Dimensions Domain Decomposition Preconditioners for Spectral Nédélec Elements in Two and Three Dimensions Bernhard Hientzsch Courant Institute of Mathematical Sciences, New York University, 51 Mercer Street, New

More information

Chapter 1: The Finite Element Method

Chapter 1: The Finite Element Method Chapter 1: The Finite Element Method Michael Hanke Read: Strang, p 428 436 A Model Problem Mathematical Models, Analysis and Simulation, Part Applications: u = fx), < x < 1 u) = u1) = D) axial deformation

More information

Numerical Solutions to Partial Differential Equations

Numerical Solutions to Partial Differential Equations Numerical Solutions to Partial Differential Equations Zhiping Li LMAM and School of Mathematical Sciences Peking University The Residual and Error of Finite Element Solutions Mixed BVP of Poisson Equation

More information

Matrix assembly by low rank tensor approximation

Matrix assembly by low rank tensor approximation Matrix assembly by low rank tensor approximation Felix Scholz 13.02.2017 References Angelos Mantzaflaris, Bert Juettler, Boris Khoromskij, and Ulrich Langer. Matrix generation in isogeometric analysis

More information

Scientific Computing: An Introductory Survey

Scientific Computing: An Introductory Survey Scientific Computing: An Introductory Survey Chapter 7 Interpolation Prof. Michael T. Heath Department of Computer Science University of Illinois at Urbana-Champaign Copyright c 2002. Reproduction permitted

More information

Applied Linear Algebra in Geoscience Using MATLAB

Applied Linear Algebra in Geoscience Using MATLAB Applied Linear Algebra in Geoscience Using MATLAB Contents Getting Started Creating Arrays Mathematical Operations with Arrays Using Script Files and Managing Data Two-Dimensional Plots Programming in

More information

ACM/CMS 107 Linear Analysis & Applications Fall 2017 Assignment 2: PDEs and Finite Element Methods Due: 7th November 2017

ACM/CMS 107 Linear Analysis & Applications Fall 2017 Assignment 2: PDEs and Finite Element Methods Due: 7th November 2017 ACM/CMS 17 Linear Analysis & Applications Fall 217 Assignment 2: PDEs and Finite Element Methods Due: 7th November 217 For this assignment the following MATLAB code will be required: Introduction http://wwwmdunloporg/cms17/assignment2zip

More information

CS 450 Numerical Analysis. Chapter 8: Numerical Integration and Differentiation

CS 450 Numerical Analysis. Chapter 8: Numerical Integration and Differentiation Lecture slides based on the textbook Scientific Computing: An Introductory Survey by Michael T. Heath, copyright c 2018 by the Society for Industrial and Applied Mathematics. http://www.siam.org/books/cl80

More information

Preface to the Second Edition. Preface to the First Edition

Preface to the Second Edition. Preface to the First Edition n page v Preface to the Second Edition Preface to the First Edition xiii xvii 1 Background in Linear Algebra 1 1.1 Matrices................................. 1 1.2 Square Matrices and Eigenvalues....................

More information

Fast Nyström Methods for Parabolic Boundary Integral Equations

Fast Nyström Methods for Parabolic Boundary Integral Equations Fast Nyström Methods for Parabolic Boundary Integral Equations Johannes Tausch Abstract Time dependence in parabolic boundary integral operators appears in form of an integral over the previous time evolution

More information

Hierarchical Parallel Solution of Stochastic Systems

Hierarchical Parallel Solution of Stochastic Systems Hierarchical Parallel Solution of Stochastic Systems Second M.I.T. Conference on Computational Fluid and Solid Mechanics Contents: Simple Model of Stochastic Flow Stochastic Galerkin Scheme Resulting Equations

More information

Course Notes: Week 1

Course Notes: Week 1 Course Notes: Week 1 Math 270C: Applied Numerical Linear Algebra 1 Lecture 1: Introduction (3/28/11) We will focus on iterative methods for solving linear systems of equations (and some discussion of eigenvalues

More information

3.1 Interpolation and the Lagrange Polynomial

3.1 Interpolation and the Lagrange Polynomial MATH 4073 Chapter 3 Interpolation and Polynomial Approximation Fall 2003 1 Consider a sample x x 0 x 1 x n y y 0 y 1 y n. Can we get a function out of discrete data above that gives a reasonable estimate

More information

Hierarchical Matrices in Computations of Electron Dynamics

Hierarchical Matrices in Computations of Electron Dynamics Hierarchical Matrices in Computations of Electron Dynamics Othmar Koch Christopher Ede Gerald Jordan Armin Scrinzi July 20, 2009 Abstract We discuss the approximation of the meanfield terms appearing in

More information

Numerical Methods I Orthogonal Polynomials

Numerical Methods I Orthogonal Polynomials Numerical Methods I Orthogonal Polynomials Aleksandar Donev Courant Institute, NYU 1 donev@courant.nyu.edu 1 Course G63.2010.001 / G22.2420-001, Fall 2010 Nov. 4th and 11th, 2010 A. Donev (Courant Institute)

More information

Class notes: Approximation

Class notes: Approximation Class notes: Approximation Introduction Vector spaces, linear independence, subspace The goal of Numerical Analysis is to compute approximations We want to approximate eg numbers in R or C vectors in R

More information

Fixed point iteration and root finding

Fixed point iteration and root finding Fixed point iteration and root finding The sign function is defined as x > 0 sign(x) = 0 x = 0 x < 0. It can be evaluated via an iteration which is useful for some problems. One such iteration is given

More information

FastMMLib: a generic Fast Multipole Method library. Eric DARRIGRAND. IRMAR Université de Rennes 1

FastMMLib: a generic Fast Multipole Method library. Eric DARRIGRAND. IRMAR Université de Rennes 1 FastMMLib: a generic Fast Multipole Method library Eric DARRIGRAND joint work with Yvon LAFRANCHE IRMAR Université de Rennes 1 Outline Introduction to FMM Historically SVD principle A first example of

More information

Lecture 8: Fast Linear Solvers (Part 7)

Lecture 8: Fast Linear Solvers (Part 7) Lecture 8: Fast Linear Solvers (Part 7) 1 Modified Gram-Schmidt Process with Reorthogonalization Test Reorthogonalization If Av k 2 + δ v k+1 2 = Av k 2 to working precision. δ = 10 3 2 Householder Arnoldi

More information

AMS526: Numerical Analysis I (Numerical Linear Algebra for Computational and Data Sciences)

AMS526: Numerical Analysis I (Numerical Linear Algebra for Computational and Data Sciences) AMS526: Numerical Analysis I (Numerical Linear Algebra for Computational and Data Sciences) Lecture 19: Computing the SVD; Sparse Linear Systems Xiangmin Jiao Stony Brook University Xiangmin Jiao Numerical

More information

Directional Field. Xiao-Ming Fu

Directional Field. Xiao-Ming Fu Directional Field Xiao-Ming Fu Outlines Introduction Discretization Representation Objectives and Constraints Outlines Introduction Discretization Representation Objectives and Constraints Definition Spatially-varying

More information