Fast and Stable Eigendecomposition of Symmetric Banded Plus Semi-Separable Matrices S
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Periodic Staircase Matrices and Generalized Cluster Structures
PERIODIC STAIRCASE MATRICES AND GENERALIZED CLUSTER STRUCTURES MISHA GEKHTMAN, MICHAEL SHAPIRO, AND ALEK VAINSHTEIN Abstract. As is well-known, cluster transformations in cluster structures of geometric type are often modeled on determinant identities, such as short Pl¨ucker relations, Desnanot–Jacobi identities and their generalizations. We present a construction that plays a similar role in a description of general- ized cluster transformations and discuss its applications to generalized clus- ter structures in GLn compatible with a certain subclass of Belavin–Drinfeld Poisson–Lie brackets, in the Drinfeld double of GLn, and in spaces of periodic difference operators. 1. Introduction Since the discovery of cluster algebras in [4], many important algebraic varieties were shown to support a cluster structure in a sense that the coordinate rings of such variety is isomorphic to a cluster algebra or an upper cluster algebra. Lie theory and representation theory turned out to be a particularly rich source of varieties of this sort including but in no way limited to such examples as Grassmannians [5, 18], double Bruhat cells [1] and strata in flag varieties [15]. In all these examples, cluster transformations that connect distinguished coordinate charts within a ring of regular functions are modeled on three-term relations such as short Pl¨ucker relations, Desnanot–Jacobi identities and their Lie-theoretic generalizations of the kind considered in [3]. This remains true even in the case of exotic cluster structures on GLn considered in [8, 10] where cluster transformations can be obtained by applying Desnanot–Jacobi type identities to certain structured matrices of a size far exceeding n. -
Arxiv:Math/0010243V1
FOUR SHORT STORIES ABOUT TOEPLITZ MATRIX CALCULATIONS THOMAS STROHMER∗ Abstract. The stories told in this paper are dealing with the solution of finite, infinite, and biinfinite Toeplitz-type systems. A crucial role plays the off-diagonal decay behavior of Toeplitz matrices and their inverses. Classical results of Gelfand et al. on commutative Banach algebras yield a general characterization of this decay behavior. We then derive estimates for the approximate solution of (bi)infinite Toeplitz systems by the finite section method, showing that the approximation rate depends only on the decay of the entries of the Toeplitz matrix and its condition number. Furthermore, we give error estimates for the solution of doubly infinite convolution systems by finite circulant systems. Finally, some quantitative results on the construction of preconditioners via circulant embedding are derived, which allow to provide a theoretical explanation for numerical observations made by some researchers in connection with deconvolution problems. Key words. Toeplitz matrix, Laurent operator, decay of inverse matrix, preconditioner, circu- lant matrix, finite section method. AMS subject classifications. 65T10, 42A10, 65D10, 65F10 0. Introduction. Toeplitz-type equations arise in many applications in mathe- matics, signal processing, communications engineering, and statistics. The excellent surveys [4, 17] describe a number of applications and contain a vast list of references. The stories told in this paper are dealing with the (approximate) solution of biinfinite, infinite, and finite hermitian positive definite Toeplitz-type systems. We pay special attention to Toeplitz-type systems with certain decay properties in the sense that the entries of the matrix enjoy a certain decay rate off the diagonal. -
THREE STEPS on an OPEN ROAD Gilbert Strang This Note Describes
Inverse Problems and Imaging doi:10.3934/ipi.2013.7.961 Volume 7, No. 3, 2013, 961{966 THREE STEPS ON AN OPEN ROAD Gilbert Strang Massachusetts Institute of Technology Cambridge, MA 02139, USA Abstract. This note describes three recent factorizations of banded invertible infinite matrices 1. If A has a banded inverse : A=BC with block{diagonal factors B and C. 2. Permutations factor into a shift times N < 2w tridiagonal permutations. 3. A = LP U with lower triangular L, permutation P , upper triangular U. We include examples and references and outlines of proofs. This note describes three small steps in the factorization of banded matrices. It is written to encourage others to go further in this direction (and related directions). At some point the problems will become deeper and more difficult, especially for doubly infinite matrices. Our main point is that matrices need not be Toeplitz or block Toeplitz for progress to be possible. An important theory is already established [2, 9, 10, 13-16] for non-Toeplitz \band-dominated operators". The Fredholm index plays a key role, and the second small step below (taken jointly with Marko Lindner) computes that index in the special case of permutation matrices. Recall that banded Toeplitz matrices lead to Laurent polynomials. If the scalars or matrices a−w; : : : ; a0; : : : ; aw lie along the diagonals, the polynomial is A(z) = P k akz and the bandwidth is w. The required index is in this case a winding number of det A(z). Factorization into A+(z)A−(z) is a classical problem solved by Plemelj [12] and Gohberg [6-7]. -
Arxiv:2004.05118V1 [Math.RT]
GENERALIZED CLUSTER STRUCTURES RELATED TO THE DRINFELD DOUBLE OF GLn MISHA GEKHTMAN, MICHAEL SHAPIRO, AND ALEK VAINSHTEIN Abstract. We prove that the regular generalized cluster structure on the Drinfeld double of GLn constructed in [9] is complete and compatible with the standard Poisson–Lie structure on the double. Moreover, we show that for n = 4 this structure is distinct from a previously known regular generalized cluster structure on the Drinfeld double, even though they have the same compatible Poisson structure and the same collection of frozen variables. Further, we prove that the regular generalized cluster structure on band periodic matrices constructed in [9] possesses similar compatibility and completeness properties. 1. Introduction In [6, 8] we constructed an initial seed Σn for a complete generalized cluster D structure GCn in the ring of regular functions on the Drinfeld double D(GLn) and proved that this structure is compatible with the standard Poisson–Lie structure on D(GLn). In [9, Section 4] we constructed a different seed Σ¯ n for a regular D D generalized cluster structure GCn on D(GLn). In this note we prove that GCn D shares all the properties of GCn : it is complete and compatible with the standard Poisson–Lie structure on D(GLn). Moreover, we prove that the seeds Σ¯ 4(X, Y ) and T T Σ4(Y ,X ) are not mutationally equivalent. In this way we provide an explicit example of two different regular complete generalized cluster structures on the same variety with the same compatible Poisson structure and the same collection of frozen D variables. -
Solving Systems of Linear Equations by Gaussian Elimination
Chapter 3 Solving Systems of Linear Equations By Gaussian Elimination 3.1 Mathematical Preliminaries In this chapter we consider the problem of computing the solution of a system of n linear equations in n unknowns. The scalar form of that system is as follows: a11x1 +a12x2 +... +... +a1nxn = b1 a x +a x +... +... +a x = b (S) 8 21 1 22 2 2n n 2 > ... ... ... ... ... <> an1x1 +an2x2 +... +... +annxn = bn > Written in matrix:> form, (S) is equivalent to: (3.1) Ax = b, where the coefficient square matrix A Rn,n, and the column vectors x, b n,1 n 2 2 R ⇠= R . Specifically, a11 a12 ... ... a1n a21 a22 ... ... a2n A = 0 1 ... ... ... ... ... B a a ... ... a C B n1 n2 nn C @ A 93 94 N. Nassif and D. Fayyad x1 b1 x2 b2 x = 0 1 and b = 0 1 . ... ... B x C B b C B n C B n C @ A @ A We assume that the basic linear algebra property for systems of linear equa- tions like (3.1) are satisfied. Specifically: Proposition 3.1. The following statements are equivalent: 1. System (3.1) has a unique solution. 2. det(A) =0. 6 3. A is invertible. In this chapter, our objective is to present the basic ideas of a linear system solver. It consists of two main procedures allowing to solve efficiently (3.1). 1. The first, referred to as Gauss elimination (or reduction) reduces (3.1) into an equivalent system of linear equations, which matrix is upper triangular. Specifically one shows in section 4 that Ax = b Ux = c, () where c Rn and U Rn,n is given by: 2 2 u11 u12 .. -
The Spectra of Large Toeplitz Band Matrices with A
MATHEMATICS OF COMPUTATION Volume 72, Number 243, Pages 1329{1348 S 0025-5718(03)01505-9 Article electronically published on February 3, 2003 THESPECTRAOFLARGETOEPLITZBANDMATRICES WITH A RANDOMLY PERTURBED ENTRY A. BOTTCHER,¨ M. EMBREE, AND V. I. SOKOLOV Abstract. (j;k) This paper is concerned with the union spΩ Tn(a) of all possible spectra that may emerge when perturbing a large n n Toeplitz band matrix × Tn(a)inthe(j; k) site by a number randomly chosen from some set Ω. The main results give descriptive bounds and, in several interesting situations, even (j;k) provide complete identifications of the limit of sp Tn(a)asn .Also Ω !1 discussed are the cases of small and large sets Ω as well as the \discontinuity of (j;k) the infinite volume case", which means that in general spΩ Tn(a)doesnot converge to something close to sp(j;k) T (a)asn ,whereT (a)isthecor- Ω !1 responding infinite Toeplitz matrix. Illustrations are provided for tridiagonal Toeplitz matrices, a notable special case. 1. Introduction and main results For a complex-valued continuous function a on the complex unit circle T,the infinite Toeplitz matrix T (a) and the finite Toeplitz matrices Tn(a) are defined by n T (a)=(aj k)j;k1 =1 and Tn(a)=(aj k)j;k=1; − − where a` is the `th Fourier coefficient of a, 2π 1 iθ i`θ a` = a(e )e− dθ; ` Z: 2π 2 Z0 Here, we restrict our attention to the case where a is a trigonometric polynomial, a , implying that at most a finite number of the Fourier coefficients are nonzero; equivalently,2P T (a) is a banded matrix. -
Conversion of Sparse Matrix to Band Matrix Using an Fpga For
CONVERSION OF SPARSE MATRIX TO BAND MATRIX USING AN FPGA FOR HIGH-PERFORMANCE COMPUTING by Anjani Chaudhary, M.S. A thesis submitted to the Graduate Council of Texas State University in partial fulfillment of the requirements for the degree of Master of Science with a Major in Engineering December 2020 Committee Members: Semih Aslan, Chair Shuying Sun William A Stapleton COPYRIGHT by Anjani Chaudhary 2020 FAIR USE AND AUTHOR’S PERMISSION STATEMENT Fair Use This work is protected by the Copyright Laws of the United States (Public Law 94-553, section 107). Consistent with fair use as defined in the Copyright Laws, brief quotations from this material are allowed with proper acknowledgement. Use of this material for financial gain without the author’s express written permission is not allowed. Duplication Permission As the copyright holder of this work, I, Anjani Chaudhary, authorize duplication of this work, in whole or in part, for educational or scholarly purposes only. ACKNOWLEDGEMENTS Throughout my research and report writing process, I am grateful to receive support and suggestions from the following people. I would like to thank my supervisor and chair, Dr. Semih Aslan, Associate Professor, Ingram School of Engineering, for his time, support, encouragement, and patience, without which I would not have made it. My committee members Dr. Bill Stapleton, Associate Professor, Ingram School of Engineering, and Dr. Shuying Sun, Associate Professor, Department of Mathematics, for their essential guidance throughout the research and my graduate advisor, Dr. Vishu Viswanathan, for providing the opportunity and valuable suggestions which helped me to come one more step closer to my goal. -
Copyrighted Material
JWST600-IND JWST600-Penney September 28, 2015 7:40 Printer Name: Trim: 6.125in × 9.25in INDEX Additive property of determinants, 244 Cofactor expansion, 240 Argument of a complex number, 297 Column space, 76 Column vector, 2 Band matrix, 407 Complementary vector, 319 Band width, 407 Complex eigenvalue, 302 Basis Complex eigenvector, 302 chain, 438 Complex linear transformation, 304 coordinate matrix for a basis, 217 Complex matrices, 301 coordinate transformation, 223 Complex number definition, 104 argument, 297 normalization, 315 conjugate, 302 ordered, 216 Complex vector space, 303 orthonormal, 315 Conjugate of a complex number, 302 point transformation, 223 Consumption matrix, 198 standard Coordinate matrix, 217 M(m,n), 119 Coordinates n, 119 coordinate vector, 216 Rn, 118 coordinate matrix for a basis, 217 COPYRIGHTEDcoordinate MATERIAL vector, 216 Cn, 302 point matrix, 217 Chain basis, 438 point transformation, 223 Characteristic polynomial, 275 Cramer’s rule, 265 Coefficient matrix, 75 Current, 41 Linear Algebra: Ideas and Applications, Fourth Edition. Richard C. Penney. © 2016 John Wiley & Sons, Inc. Published 2016 by John Wiley & Sons, Inc. Companion website: www.wiley.com/go/penney/linearalgebra 487 JWST600-IND JWST600-Penney September 28, 2015 7:40 Printer Name: Trim: 6.125in × 9.25in 488 INDEX Data compression, 349 Haar function, 346 Determinant Hermitian additive property, 244 adjoint, 412 cofactor expansion, 240 symmetric, 414 Cramer’s rule, 265 Hermitian, orthogonal, 413 inverse matrix, 267 Homogeneous system, 80 Laplace -
Arxiv:2009.05100V2
THE COMPLETE POSITIVITY OF SYMMETRIC TRIDIAGONAL AND PENTADIAGONAL MATRICES LEI CAO 1,2, DARIAN MCLAREN 3, AND SARAH PLOSKER 3 Abstract. We provide a decomposition that is sufficient in showing when a symmetric tridiagonal matrix A is completely positive. Our decomposition can be applied to a wide range of matrices. We give alternate proofs for a number of related results found in the literature in a simple, straightforward manner. We show that the cp-rank of any irreducible tridiagonal doubly stochastic matrix is equal to its rank. We then consider symmetric pentadiagonal matrices, proving some analogous results, and providing two different decom- positions sufficient for complete positivity. We illustrate our constructions with a number of examples. 1. Preliminaries All matrices herein will be real-valued. Let A be an n n symmetric tridiagonal matrix: × a1 b1 b1 a2 b2 . .. .. .. . A = .. .. .. . bn 3 an 2 bn 2 − − − bn 2 an 1 bn 1 − − − bn 1 an − We are often interested in the case where A is also doubly stochastic, in which case we have ai = 1 bi 1 bi for i = 1, 2,...,n, with the convention that b0 = bn = 0. It is easy to see that− if a− tridiagonal− matrix is doubly stochastic, it must be symmetric, so the additional hypothesis of symmetry can be dropped in that case. We are interested in positivity conditions for symmetric tridiagonal and pentadiagonal matrices. A stronger condition than positive semidefiniteness, known as complete positivity, arXiv:2009.05100v2 [math.CO] 10 Mar 2021 has applications in a variety of areas of study, including block designs, maximin efficiency- robust tests, modelling DNA evolution, and more [5, Chapter 2], as well as recent use in mathematical optimization and quantum information theory (see [14] and the references therein). -
NAG Library Chapter Contents F16 – NAG Interface to BLAS F16 Chapter Introduction
F16 – NAG Interface to BLAS Contents – F16 NAG Library Chapter Contents f16 – NAG Interface to BLAS f16 Chapter Introduction Function Mark of Name Introduction Purpose f16dbc 7 nag_iload Broadcast scalar into integer vector f16dlc 9 nag_isum Sum elements of integer vector f16dnc 9 nag_imax_val Maximum value and location, integer vector f16dpc 9 nag_imin_val Minimum value and location, integer vector f16dqc 9 nag_iamax_val Maximum absolute value and location, integer vector f16drc 9 nag_iamin_val Minimum absolute value and location, integer vector f16eac 24 nag_ddot Dot product of two vectors, allows scaling and accumulation. f16ecc 7 nag_daxpby Real weighted vector addition f16ehc 9 nag_dwaxpby Real weighted vector addition preserving input f16elc 9 nag_dsum Sum elements of real vector f16fbc 7 nag_dload Broadcast scalar into real vector f16gcc 24 nag_zaxpby Complex weighted vector addition f16ghc 9 nag_zwaxpby Complex weighted vector addition preserving input f16glc 9 nag_zsum Sum elements of complex vector f16hbc 7 nag_zload Broadcast scalar into complex vector f16jnc 9 nag_dmax_val Maximum value and location, real vector f16jpc 9 nag_dmin_val Minimum value and location, real vector f16jqc 9 nag_damax_val Maximum absolute value and location, real vector f16jrc 9 nag_damin_val Minimum absolute value and location, real vector f16jsc 9 nag_zamax_val Maximum absolute value and location, complex vector f16jtc 9 nag_zamin_val Minimum absolute value and location, complex vector f16pac 8 nag_dgemv Matrix-vector product, real rectangular matrix -
THE EFFECTIVE POTENTIAL of an M-MATRIX Marcel Filoche, Svitlana Mayboroda, Terence Tao
THE EFFECTIVE POTENTIAL OF AN M-MATRIX Marcel Filoche, Svitlana Mayboroda, Terence Tao To cite this version: Marcel Filoche, Svitlana Mayboroda, Terence Tao. THE EFFECTIVE POTENTIAL OF AN M- MATRIX. 2021. hal-03189307 HAL Id: hal-03189307 https://hal.archives-ouvertes.fr/hal-03189307 Preprint submitted on 3 Apr 2021 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. THE EFFECTIVE POTENTIAL OF AN M-MATRIX MARCEL FILOCHE, SVITLANA MAYBORODA, AND TERENCE TAO Abstract. In the presence of a confining potential V, the eigenfunctions of a con- tinuous Schrodinger¨ operator −∆ + V decay exponentially with the rate governed by the part of V which is above the corresponding eigenvalue; this can be quan- tified by a method of Agmon. Analogous localization properties can also be es- tablished for the eigenvectors of a discrete Schrodinger¨ matrix. This note shows, perhaps surprisingly, that one can replace a discrete Schrodinger¨ matrix by any real symmetric Z-matrix and still obtain eigenvector localization estimates. In the case of a real symmetric non-singular M-matrix A (which is a situation that arises in several contexts, including random matrix theory and statistical physics), the landscape function u = A−11 plays the role of an effective potential of localiza- tion. -
Inverse Eigenvalue Problems Involving Multiple Spectra
Inverse eigenvalue problems involving multiple spectra G.M.L. Gladwell Department of Civil Engineering University of Waterloo Waterloo, Ontario, Canada N2L 3G1 [email protected] URL: http://www.civil.uwaterloo.ca/ggladwell Abstract If A Mn, its spectrum is denoted by σ(A).IfA is oscillatory (O) then σ(A∈) is positive and discrete, the submatrix A[r +1,...,n] is O and itsspectrumisdenotedbyσr(A). Itisknownthatthereisaunique symmetric tridiagonal O matrix with given, positive, strictly interlacing spectra σ0, σ1. It is shown that there is not necessarily a pentadiagonal O matrix with given, positive strictly interlacing spectra σ0, σ1, σ2, but that there is a family of such matrices with positive strictly interlacing spectra σ0, σ1. The concept of inner total positivity (ITP) is introduced, and it is shown that an ITP matrix may be reduced to ITP band form, or filled in to become TP. These reductions and filling-in procedures are used to construct ITP matrices with given multiple common spectra. 1Introduction My interest in inverse eigenvalue problems (IEP) stems from the fact that they appear in inverse vibration problems, see [7]. In these problems the matrices that appear are usually symmetric; in this paper we shall often assume that the matrices are symmetric: A Sn. ∈ If A Sn, its eigenvalues are real; we denote its spectrum by σ(A)= ∈ λ1, λ2,...,λn ,whereλ1 λ2 λn. The direct problem of finding σ{(A) from A is} well understood.≤ At≤ fi···rst≤ sight it appears that inverse eigenvalue T problems are trivial: every A Sn with spectrum σ(A) has the form Q Q ∈ ∧ where Q is orthogonal and = diag(λ1, λ2,...,λn).