Accelerating the LOBPCG Method on Gpus Using a Blocked Sparse Matrix Vector Product
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Recursive Approach in Sparse Matrix LU Factorization
51 Recursive approach in sparse matrix LU factorization Jack Dongarra, Victor Eijkhout and the resulting matrix is often guaranteed to be positive Piotr Łuszczek∗ definite or close to it. However, when the linear sys- University of Tennessee, Department of Computer tem matrix is strongly unsymmetric or indefinite, as Science, Knoxville, TN 37996-3450, USA is the case with matrices originating from systems of Tel.: +865 974 8295; Fax: +865 974 8296 ordinary differential equations or the indefinite matri- ces arising from shift-invert techniques in eigenvalue methods, one has to revert to direct methods which are This paper describes a recursive method for the LU factoriza- the focus of this paper. tion of sparse matrices. The recursive formulation of com- In direct methods, Gaussian elimination with partial mon linear algebra codes has been proven very successful in pivoting is performed to find a solution of Eq. (1). Most dense matrix computations. An extension of the recursive commonly, the factored form of A is given by means technique for sparse matrices is presented. Performance re- L U P Q sults given here show that the recursive approach may per- of matrices , , and such that: form comparable to leading software packages for sparse ma- LU = PAQ, (2) trix factorization in terms of execution time, memory usage, and error estimates of the solution. where: – L is a lower triangular matrix with unitary diago- nal, 1. Introduction – U is an upper triangular matrix with arbitrary di- agonal, Typically, a system of linear equations has the form: – P and Q are row and column permutation matri- Ax = b, (1) ces, respectively (each row and column of these matrices contains single a non-zero entry which is A n n A ∈ n×n x where is by real matrix ( R ), and 1, and the following holds: PPT = QQT = I, b n b, x ∈ n and are -dimensional real vectors ( R ). -
Arxiv:1911.09220V2 [Cs.MS] 13 Jul 2020
MFEM: A MODULAR FINITE ELEMENT METHODS LIBRARY ROBERT ANDERSON, JULIAN ANDREJ, ANDREW BARKER, JAMIE BRAMWELL, JEAN- SYLVAIN CAMIER, JAKUB CERVENY, VESELIN DOBREV, YOHANN DUDOUIT, AARON FISHER, TZANIO KOLEV, WILL PAZNER, MARK STOWELL, VLADIMIR TOMOV Lawrence Livermore National Laboratory, Livermore, USA IDO AKKERMAN Delft University of Technology, Netherlands JOHANN DAHM IBM Research { Almaden, Almaden, USA DAVID MEDINA Occalytics, LLC, Houston, USA STEFANO ZAMPINI King Abdullah University of Science and Technology, Thuwal, Saudi Arabia Abstract. MFEM is an open-source, lightweight, flexible and scalable C++ library for modular finite element methods that features arbitrary high-order finite element meshes and spaces, support for a wide variety of dis- cretization approaches and emphasis on usability, portability, and high-performance computing efficiency. MFEM's goal is to provide application scientists with access to cutting-edge algorithms for high-order finite element mesh- ing, discretizations and linear solvers, while enabling researchers to quickly and easily develop and test new algorithms in very general, fully unstructured, high-order, parallel and GPU-accelerated settings. In this paper we describe the underlying algorithms and finite element abstractions provided by MFEM, discuss the software implementation, and illustrate various applications of the library. arXiv:1911.09220v2 [cs.MS] 13 Jul 2020 1. Introduction The Finite Element Method (FEM) is a powerful discretization technique that uses general unstructured grids to approximate the solutions of many partial differential equations (PDEs). It has been exhaustively studied, both theoretically and in practice, in the past several decades [1, 2, 3, 4, 5, 6, 7, 8]. MFEM is an open-source, lightweight, modular and scalable software library for finite elements, featuring arbitrary high-order finite element meshes and spaces, support for a wide variety of discretization approaches and emphasis on usability, portability, and high-performance computing (HPC) efficiency [9]. -
Abstract 1 Introduction
Implementation in ScaLAPACK of Divide-and-Conquer Algorithms for Banded and Tridiagonal Linear Systems A. Cleary Department of Computer Science University of Tennessee J. Dongarra Department of Computer Science University of Tennessee Mathematical Sciences Section Oak Ridge National Laboratory Abstract Described hereare the design and implementation of a family of algorithms for a variety of classes of narrow ly banded linear systems. The classes of matrices include symmetric and positive de - nite, nonsymmetric but diagonal ly dominant, and general nonsymmetric; and, al l these types are addressed for both general band and tridiagonal matrices. The family of algorithms captures the general avor of existing divide-and-conquer algorithms for banded matrices in that they have three distinct phases, the rst and last of which arecompletely paral lel, and the second of which is the par- al lel bottleneck. The algorithms have been modi ed so that they have the desirable property that they are the same mathematical ly as existing factorizations Cholesky, Gaussian elimination of suitably reordered matrices. This approach represents a departure in the nonsymmetric case from existing methods, but has the practical bene ts of a smal ler and more easily hand led reduced system. All codes implement a block odd-even reduction for the reduced system that al lows the algorithm to scale far better than existing codes that use variants of sequential solution methods for the reduced system. A cross section of results is displayed that supports the predicted performance results for the algo- rithms. Comparison with existing dense-type methods shows that for areas of the problem parameter space with low bandwidth and/or high number of processors, the family of algorithms described here is superior. -
Overview of Iterative Linear System Solver Packages
Overview of Iterative Linear System Solver Packages Victor Eijkhout July, 1998 Abstract Description and comparison of several packages for the iterative solu- tion of linear systems of equations. 1 1 Intro duction There are several freely available packages for the iterative solution of linear systems of equations, typically derived from partial di erential equation prob- lems. In this rep ort I will give a brief description of a numberofpackages, and giveaninventory of their features and de ning characteristics. The most imp ortant features of the packages are which iterative metho ds and preconditioners supply; the most relevant de ning characteristics are the interface they present to the user's data structures, and their implementation language. 2 2 Discussion Iterative metho ds are sub ject to several design decisions that a ect ease of use of the software and the resulting p erformance. In this section I will give a global discussion of the issues involved, and how certain p oints are addressed in the packages under review. 2.1 Preconditioners A go o d preconditioner is necessary for the convergence of iterative metho ds as the problem to b e solved b ecomes more dicult. Go o d preconditioners are hard to design, and this esp ecially holds true in the case of parallel pro cessing. Here is a short inventory of the various kinds of preconditioners found in the packages reviewed. 2.1.1 Ab out incomplete factorisation preconditioners Incomplete factorisations are among the most successful preconditioners devel- op ed for single-pro cessor computers. Unfortunately, since they are implicit in nature, they cannot immediately b e used on parallel architectures. -
Krylov Subspaces
Lab 1 Krylov Subspaces Lab Objective: Discuss simple Krylov Subspace Methods for finding eigenvalues and show some interesting applications. One of the biggest difficulties in computational linear algebra is the amount of memory needed to store a large matrix and the amount of time needed to read its entries. Methods using Krylov subspaces avoid this difficulty by studying how a matrix acts on vectors, making it unnecessary in many cases to create the matrix itself. More specifically, we can construct a Krylov subspace just by knowing how a linear transformation acts on vectors, and with these subspaces we can closely approximate eigenvalues of the transformation and solutions to associated linear systems. The Arnoldi iteration is an algorithm for finding an orthonormal basis of a Krylov subspace. Its outputs can also be used to approximate the eigenvalues of the original matrix. The Arnoldi Iteration The order-N Krylov subspace of A generated by x is 2 n−1 Kn(A; x) = spanfx;Ax;A x;:::;A xg: If the vectors fx;Ax;A2x;:::;An−1xg are linearly independent, then they form a basis for Kn(A; x). However, this basis is usually far from orthogonal, and hence computations using this basis will likely be ill-conditioned. One way to find an orthonormal basis for Kn(A; x) would be to use the modi- fied Gram-Schmidt algorithm from Lab TODO on the set fx;Ax;A2x;:::;An−1xg. More efficiently, the Arnold iteration integrates the creation of fx;Ax;A2x;:::;An−1xg with the modified Gram-Schmidt algorithm, returning an orthonormal basis for Kn(A; x). -
MFEM: a Modular Finite Element Methods Library
MFEM: A Modular Finite Element Methods Library Robert Anderson1, Andrew Barker1, Jamie Bramwell1, Jakub Cerveny2, Johann Dahm3, Veselin Dobrev1,YohannDudouit1, Aaron Fisher1,TzanioKolev1,MarkStowell1,and Vladimir Tomov1 1Lawrence Livermore National Laboratory 2University of West Bohemia 3IBM Research July 2, 2018 Abstract MFEM is a free, lightweight, flexible and scalable C++ library for modular finite element methods that features arbitrary high-order finite element meshes and spaces, support for a wide variety of discretization approaches and emphasis on usability, portability, and high-performance computing efficiency. Its mission is to provide application scientists with access to cutting-edge algorithms for high-order finite element meshing, discretizations and linear solvers. MFEM also enables researchers to quickly and easily develop and test new algorithms in very general, fully unstructured, high-order, parallel settings. In this paper we describe the underlying algorithms and finite element abstractions provided by MFEM, discuss the software implementation, and illustrate various applications of the library. Contents 1 Introduction 3 2 Overview of the Finite Element Method 4 3Meshes 9 3.1 Conforming Meshes . 10 3.2 Non-Conforming Meshes . 11 3.3 NURBS Meshes . 12 3.4 Parallel Meshes . 12 3.5 Supported Input and Output Formats . 13 1 4 Finite Element Spaces 13 4.1 FiniteElements....................................... 14 4.2 DiscretedeRhamComplex ................................ 16 4.3 High-OrderSpaces ..................................... 17 4.4 Visualization . 18 5 Finite Element Operators 18 5.1 DiscretizationMethods................................... 18 5.2 FiniteElementLinearSystems . 19 5.3 Operator Decomposition . 23 5.4 High-Order Partial Assembly . 25 6 High-Performance Computing 27 6.1 Parallel Meshes, Spaces, and Operators . 27 6.2 Scalable Linear Solvers . -
Over-Scalapack.Pdf
1 2 The Situation: Parallel scienti c applications are typically Overview of ScaLAPACK written from scratch, or manually adapted from sequen- tial programs Jack Dongarra using simple SPMD mo del in Fortran or C Computer Science Department UniversityofTennessee with explicit message passing primitives and Mathematical Sciences Section Which means Oak Ridge National Lab oratory similar comp onents are co ded over and over again, co des are dicult to develop and maintain http://w ww .ne tl ib. org /ut k/p e opl e/J ackDo ngarra.html debugging particularly unpleasant... dicult to reuse comp onents not really designed for long-term software solution 3 4 What should math software lo ok like? The NetSolve Client Many more p ossibilities than shared memory Virtual Software Library Multiplicityofinterfaces ! Ease of use Possible approaches { Minimum change to status quo Programming interfaces Message passing and ob ject oriented { Reusable templates { requires sophisticated user Cinterface FORTRAN interface { Problem solving environments Integrated systems a la Matlab, Mathematica use with heterogeneous platform Interactiveinterfaces { Computational server, like netlib/xnetlib f2c Non-graphic interfaces Some users want high p erf., access to details {MATLAB interface Others sacri ce sp eed to hide details { UNIX-Shell interface Not enough p enetration of libraries into hardest appli- Graphic interfaces cations on vector machines { TK/TCL interface Need to lo ok at applications and rethink mathematical software { HotJava Browser -
Limited Memory Block Krylov Subspace Optimization for Computing Dominant Singular Value Decompositions
Limited Memory Block Krylov Subspace Optimization for Computing Dominant Singular Value Decompositions Xin Liu∗ Zaiwen Weny Yin Zhangz March 22, 2012 Abstract In many data-intensive applications, the use of principal component analysis (PCA) and other related techniques is ubiquitous for dimension reduction, data mining or other transformational purposes. Such transformations often require efficiently, reliably and accurately computing dominant singular value de- compositions (SVDs) of large unstructured matrices. In this paper, we propose and study a subspace optimization technique to significantly accelerate the classic simultaneous iteration method. We analyze the convergence of the proposed algorithm, and numerically compare it with several state-of-the-art SVD solvers under the MATLAB environment. Extensive computational results show that on a wide range of large unstructured matrices, the proposed algorithm can often provide improved efficiency or robustness over existing algorithms. Keywords. subspace optimization, dominant singular value decomposition, Krylov subspace, eigen- value decomposition 1 Introduction Singular value decomposition (SVD) is a fundamental and enormously useful tool in matrix computations, such as determining the pseudo-inverse, the range or null space, or the rank of a matrix, solving regular or total least squares data fitting problems, or computing low-rank approximations to a matrix, just to mention a few. The need for computing SVDs also frequently arises from diverse fields in statistics, signal processing, data mining or compression, and from various dimension-reduction models of large-scale dynamic systems. Usually, instead of acquiring all the singular values and vectors of a matrix, it suffices to compute a set of dominant (i.e., the largest) singular values and their corresponding singular vectors in order to obtain the most valuable and relevant information about the underlying dataset or system. -
XAMG: a Library for Solving Linear Systems with Multiple Right-Hand
XAMG: A library for solving linear systems with multiple right-hand side vectors B. Krasnopolsky∗, A. Medvedev∗∗ Institute of Mechanics, Lomonosov Moscow State University, 119192 Moscow, Michurinsky ave. 1, Russia Abstract This paper presents the XAMG library for solving large sparse systems of linear algebraic equations with multiple right-hand side vectors. The library specializes but is not limited to the solution of linear systems obtained from the discretization of elliptic differential equations. A corresponding set of numerical methods includes Krylov subspace, algebraic multigrid, Jacobi, Gauss-Seidel, and Chebyshev iterative methods. The parallelization is im- plemented with MPI+POSIX shared memory hybrid programming model, which introduces a three-level hierarchical decomposition using the corre- sponding per-level synchronization and communication primitives. The code contains a number of optimizations, including the multilevel data segmen- tation, compression of indices, mixed-precision floating-point calculations, arXiv:2103.07329v1 [cs.MS] 12 Mar 2021 vector status flags, and others. The XAMG library uses the program code of the well-known hypre library to construct the multigrid matrix hierar- chy. The XAMG’s own implementation for the solve phase of the iterative methods provides up to a twofold speedup compared to hypre for the tests ∗E-mail address: [email protected] ∗∗E-mail address: [email protected] Preprint submitted to Elsevier March 15, 2021 performed. Additionally, XAMG provides extended functionality to solve systems with multiple right-hand side vectors. Keywords: systems of linear algebraic equations, Krylov subspace iterative methods, algebraic multigrid method, multiple right-hand sides, hybrid programming model, MPI+POSIX shared memory Nr. -
Power Method and Krylov Subspaces
Power method and Krylov subspaces Introduction When calculating an eigenvalue of a matrix A using the power method, one starts with an initial random vector b and then computes iteratively the sequence Ab, A2b,...,An−1b normalising and storing the result in b on each iteration. The sequence converges to the eigenvector of the largest eigenvalue of A. The set of vectors 2 n−1 Kn = b, Ab, A b,...,A b , (1) where n < rank(A), is called the order-n Krylov matrix, and the subspace spanned by these vectors is called the order-n Krylov subspace. The vectors are not orthogonal but can be made so e.g. by Gram-Schmidt orthogonalisation. For the same reason that An−1b approximates the dominant eigenvector one can expect that the other orthogonalised vectors approximate the eigenvectors of the n largest eigenvalues. Krylov subspaces are the basis of several successful iterative methods in numerical linear algebra, in particular: Arnoldi and Lanczos methods for finding one (or a few) eigenvalues of a matrix; and GMRES (Generalised Minimum RESidual) method for solving systems of linear equations. These methods are particularly suitable for large sparse matrices as they avoid matrix-matrix opera- tions but rather multiply vectors by matrices and work with the resulting vectors and matrices in Krylov subspaces of modest sizes. Arnoldi iteration Arnoldi iteration is an algorithm where the order-n orthogonalised Krylov matrix Qn of a matrix A is built using stabilised Gram-Schmidt process: • start with a set Q = {q1} of one random normalised vector q1 • repeat for k =2 to n : – make a new vector qk = Aqk−1 † – orthogonalise qk to all vectors qi ∈ Q storing qi qk → hi,k−1 – normalise qk storing qk → hk,k−1 – add qk to the set Q By construction the matrix Hn made of the elements hjk is an upper Hessenberg matrix, h1,1 h1,2 h1,3 ··· h1,n h2,1 h2,2 h2,3 ··· h2,n 0 h3,2 h3,3 ··· h3,n Hn = , (2) . -
Present and Future Leadership Computers at OLCF
Present and Future Leadership Computers at OLCF Buddy Bland OLCF Project Director Presented at: SC’14 November 17-21, 2014 New Orleans ORNL is managed by UT-Battelle for the US Department of Energy Oak Ridge Leadership Computing Facility (OLCF) Mission: Deploy and operate the computational resources required to tackle global challenges Providing world-leading computational and data resources and specialized services for the most computationally intensive problems Providing stable hardware/software path of increasing scale to maximize productive applications development Providing the resources to investigate otherwise inaccessible systems at every scale: from galaxy formation to supernovae to earth systems to automobiles to nanomaterials With our partners, deliver transforming discoveries in materials, biology, climate, energy technologies, and basic science SC’14 Summit - Bland 2 Our Science requires that we continue to advance OLCF’s computational capability over the next decade on the roadmap to Exascale. Since clock-rate scaling ended in 2003, HPC Titan and beyond deliver hierarchical parallelism with performance has been achieved through increased very powerful nodes. MPI plus thread level parallelism parallelism. Jaguar scaled to 300,000 cores. through OpenACC or OpenMP plus vectors OLCF5: 5-10x Summit Summit: 5-10x Titan ~20 MW Titan: 27 PF Hybrid GPU/CPU Jaguar: 2.3 PF Hybrid GPU/CPU 10 MW Multi-core CPU 9 MW CORAL System 7 MW 2010 2012 2017 2022 3 SC’14 Summit - Bland Today’s Leadership System - Titan Hybrid CPU/GPU architecture, Hierarchical Parallelism Vendors: Cray™ / NVIDIA™ • 27 PF peak • 18,688 Compute nodes, each with – 1.45 TF peak – NVIDIA Kepler™ GPU - 1,311 GF • 6 GB GDDR5 memory – AMD Opteron™- 141 GF • 32 GB DDR3 memory – PCIe2 link between GPU and CPU • Cray Gemini 3-D Torus Interconnect • 32 PB / 1 TB/s Lustre® file system 4 SC’14 Summit - Bland Scientific Progress at all Scales Fusion Energy Liquid Crystal Film Stability A Princeton Plasma Physics Laboratory ORNL Postdoctoral fellow Trung Nguyen team led by C.S. -
Solving Symmetric Semi-Definite (Ill-Conditioned)
Solving Symmetric Semi-definite (ill-conditioned) Generalized Eigenvalue Problems Zhaojun Bai University of California, Davis Berkeley, August 19, 2016 Symmetric definite generalized eigenvalue problem I Symmetric definite generalized eigenvalue problem Ax = λBx where AT = A and BT = B > 0 I Eigen-decomposition AX = BXΛ where Λ = diag(λ1; λ2; : : : ; λn) X = (x1; x2; : : : ; xn) XT BX = I: I Assume λ1 ≤ λ2 ≤ · · · ≤ λn LAPACK solvers I LAPACK routines xSYGV, xSYGVD, xSYGVX are based on the following algorithm (Wilkinson'65): 1. compute the Cholesky factorization B = GGT 2. compute C = G−1AG−T 3. compute symmetric eigen-decomposition QT CQ = Λ 4. set X = G−T Q I xSYGV[D,X] could be numerically unstable if B is ill-conditioned: −1 jλbi − λij . p(n)(kB k2kAk2 + cond(B)jλbij) · and −1 1=2 kB k2kAk2(cond(B)) + cond(B)jλbij θ(xbi; xi) . p(n) · specgapi I User's choice between the inversion of ill-conditioned Cholesky decomposition and the QZ algorithm that destroys symmetry Algorithms to address the ill-conditioning 1. Fix-Heiberger'72 (Parlett'80): explicit reduction 2. Chang-Chung Chang'74: SQZ method (QZ by Moler and Stewart'73) 3. Bunse-Gerstner'84: MDR method 4. Chandrasekaran'00: \proper pivoting scheme" 5. Davies-Higham-Tisseur'01: Cholesky+Jacobi 6. Working notes by Kahan'11 and Moler'14 This talk Three approaches: 1. A LAPACK-style implementation of Fix-Heiberger algorithm 2. An algebraic reformulation 3. Locally accelerated block preconditioned steepest descent (LABPSD) This talk Three approaches: 1. A LAPACK-style implementation of Fix-Heiberger algorithm Status: beta-release 2.