(Hessenberg) Eigenvalue-Eigenmatrix Relations∗
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Eigenvalues and Eigenvectors of Tridiagonal Matrices∗
Electronic Journal of Linear Algebra ISSN 1081-3810 A publication of the International Linear Algebra Society Volume 15, pp. 115-133, April 2006 ELA http://math.technion.ac.il/iic/ela EIGENVALUES AND EIGENVECTORS OF TRIDIAGONAL MATRICES∗ SAID KOUACHI† Abstract. This paper is continuation of previous work by the present author, where explicit formulas for the eigenvalues associated with several tridiagonal matrices were given. In this paper the associated eigenvectors are calculated explicitly. As a consequence, a result obtained by Wen- Chyuan Yueh and independently by S. Kouachi, concerning the eigenvalues and in particular the corresponding eigenvectors of tridiagonal matrices, is generalized. Expressions for the eigenvectors are obtained that differ completely from those obtained by Yueh. The techniques used herein are based on theory of recurrent sequences. The entries situated on each of the secondary diagonals are not necessary equal as was the case considered by Yueh. Key words. Eigenvectors, Tridiagonal matrices. AMS subject classifications. 15A18. 1. Introduction. The subject of this paper is diagonalization of tridiagonal matrices. We generalize a result obtained in [5] concerning the eigenvalues and the corresponding eigenvectors of several tridiagonal matrices. We consider tridiagonal matrices of the form −α + bc1 00 ... 0 a1 bc2 0 ... 0 .. .. 0 a2 b . An = , (1) .. .. .. 00. 0 . .. .. .. . cn−1 0 ... ... 0 an−1 −β + b n−1 n−1 ∞ where {aj}j=1 and {cj}j=1 are two finite subsequences of the sequences {aj}j=1 and ∞ {cj}j=1 of the field of complex numbers C, respectively, and α, β and b are complex numbers. We suppose that 2 d1, if j is odd ajcj = 2 j =1, 2, ..., (2) d2, if j is even where d 1 and d2 are complex numbers. -
Parametrizations of K-Nonnegative Matrices
Parametrizations of k-Nonnegative Matrices Anna Brosowsky, Neeraja Kulkarni, Alex Mason, Joe Suk, Ewin Tang∗ October 2, 2017 Abstract Totally nonnegative (positive) matrices are matrices whose minors are all nonnegative (positive). We generalize the notion of total nonnegativity, as follows. A k-nonnegative (resp. k-positive) matrix has all minors of size k or less nonnegative (resp. positive). We give a generating set for the semigroup of k-nonnegative matrices, as well as relations for certain special cases, i.e. the k = n − 1 and k = n − 2 unitriangular cases. In the above two cases, we find that the set of k-nonnegative matrices can be partitioned into cells, analogous to the Bruhat cells of totally nonnegative matrices, based on their factorizations into generators. We will show that these cells, like the Bruhat cells, are homeomorphic to open balls, and we prove some results about the topological structure of the closure of these cells, and in fact, in the latter case, the cells form a Bruhat-like CW complex. We also give a family of minimal k-positivity tests which form sub-cluster algebras of the total positivity test cluster algebra. We describe ways to jump between these tests, and give an alternate description of some tests as double wiring diagrams. 1 Introduction A totally nonnegative (respectively totally positive) matrix is a matrix whose minors are all nonnegative (respectively positive). Total positivity and nonnegativity are well-studied phenomena and arise in areas such as planar networks, combinatorics, dynamics, statistics and probability. The study of total positivity and total nonnegativity admit many varied applications, some of which are explored in “Totally Nonnegative Matrices” by Fallat and Johnson [5]. -
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]. -
QR Decomposition: History and Its Applications
Mathematics & Statistics Auburn University, Alabama, USA QR History Dec 17, 2010 Asymptotic result QR iteration QR decomposition: History and its EE Applications Home Page Title Page Tin-Yau Tam èèèUUUÎÎÎ JJ II J I Page 1 of 37 Æâ§w Go Back fÆêÆÆÆ Full Screen Close email: [email protected] Website: www.auburn.edu/∼tamtiny Quit 1. QR decomposition Recall the QR decomposition of A ∈ GLn(C): QR A = QR History Asymptotic result QR iteration where Q ∈ GLn(C) is unitary and R ∈ GLn(C) is upper ∆ with positive EE diagonal entries. Such decomposition is unique. Set Home Page a(A) := diag (r11, . , rnn) Title Page where A is written in column form JJ II J I A = (a1| · · · |an) Page 2 of 37 Go Back Geometric interpretation of a(A): Full Screen rii is the distance (w.r.t. 2-norm) between ai and span {a1, . , ai−1}, Close i = 2, . , n. Quit Example: 12 −51 4 6/7 −69/175 −58/175 14 21 −14 6 167 −68 = 3/7 158/175 6/175 0 175 −70 . QR −4 24 −41 −2/7 6/35 −33/35 0 0 35 History Asymptotic result QR iteration EE • QR decomposition is the matrix version of the Gram-Schmidt orthonor- Home Page malization process. Title Page JJ II • QR decomposition can be extended to rectangular matrices, i.e., if A ∈ J I m×n with m ≥ n (tall matrix) and full rank, then C Page 3 of 37 A = QR Go Back Full Screen where Q ∈ Cm×n has orthonormal columns and R ∈ Cn×n is upper ∆ Close with positive “diagonal” entries. -
Polynomials and Hankel Matrices
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Polynomials and Hankel Matrices Miroslav Fiedler Czechoslovak Academy of Sciences Institute of Mathematics iitnci 25 115 67 Praha 1, Czechoslovakia Submitted by V. Ptak ABSTRACT Compatibility of a Hankel n X n matrix W and a polynomial f of degree m, m < n, is defined. If m = n, compatibility means that HC’ = CfH where Cf is the companion matrix of f With a suitable generalization of Cr, this theorem is gener- alized to the case that m < n. INTRODUCTION By a Hankel matrix [S] we shall mean a square complex matrix which has, if of order n, the form ( ai +k), i, k = 0,. , n - 1. If H = (~y~+~) is a singular n X n Hankel matrix, the H-polynomial (Pi of H was defined 131 as the greatest common divisor of the determinants of all (r + 1) x (r + 1) submatrices~of the matrix where r is the rank of H. In other words, (Pi is that polynomial for which the nX(n+l)matrix I, 0 0 0 %fb) 0 i 0 0 0 1 LINEAR ALGEBRA AND ITS APPLICATIONS 66:235-248(1985) 235 ‘F’Elsevier Science Publishing Co., Inc., 1985 52 Vanderbilt Ave., New York, NY 10017 0024.3795/85/$3.30 236 MIROSLAV FIEDLER is the Smith normal form [6] of H,. It has also been shown [3] that qN is a (nonzero) polynomial of degree at most T. It is known [4] that to a nonsingular n X n Hankel matrix H = ((Y~+~)a linear pencil of polynomials of degree at most n can be assigned as follows: f(x) = fo + f,x + . -
Explicit Inverse of a Tridiagonal (P, R)–Toeplitz Matrix
Explicit inverse of a tridiagonal (p; r){Toeplitz matrix A.M. Encinas, M.J. Jim´enez Departament de Matemtiques Universitat Politcnica de Catalunya Abstract Tridiagonal matrices appears in many contexts in pure and applied mathematics, so the study of the inverse of these matrices becomes of specific interest. In recent years the invertibility of nonsingular tridiagonal matrices has been quite investigated in different fields, not only from the theoretical point of view (either in the framework of linear algebra or in the ambit of numerical analysis), but also due to applications, for instance in the study of sound propagation problems or certain quantum oscillators. However, explicit inverses are known only in a few cases, in particular when the tridiagonal matrix has constant diagonals or the coefficients of these diagonals are subjected to some restrictions like the tridiagonal p{Toeplitz matrices [7], such that their three diagonals are formed by p{periodic sequences. The recent formulae for the inversion of tridiagonal p{Toeplitz matrices are based, more o less directly, on the solution of second order linear difference equations, although most of them use a cumbersome formulation, that in fact don not take into account the periodicity of the coefficients. This contribution presents the explicit inverse of a tridiagonal matrix (p; r){Toeplitz, which diagonal coefficients are in a more general class of sequences than periodic ones, that we have called quasi{periodic sequences. A tridiagonal matrix A = (aij) of order n + 2 is called (p; r){Toeplitz if there exists m 2 N0 such that n + 2 = mp and ai+p;j+p = raij; i; j = 0;:::; (m − 1)p: Equivalently, A is a (p; r){Toeplitz matrix iff k ai+kp;j+kp = r aij; i; j = 0; : : : ; p; k = 0; : : : ; m − 1: We have developed a technique that reduces any linear second order difference equation with periodic or quasi-periodic coefficients to a difference equation of the same kind but with constant coefficients [3]. -
Etna the Block Hessenberg Process for Matrix
Electronic Transactions on Numerical Analysis. Volume 46, pp. 460–473, 2017. ETNA Kent State University and c Copyright 2017, Kent State University. Johann Radon Institute (RICAM) ISSN 1068–9613. THE BLOCK HESSENBERG PROCESS FOR MATRIX EQUATIONS∗ M. ADDAMy, M. HEYOUNIy, AND H. SADOKz Abstract. In the present paper, we first introduce a block variant of the Hessenberg process and discuss its properties. Then, we show how to apply the block Hessenberg process in order to solve linear systems with multiple right-hand sides. More precisely, we define the block CMRH method for solving linear systems that share the same coefficient matrix. We also show how to apply this process for solving discrete Sylvester matrix equations. Finally, numerical comparisons are provided in order to compare the proposed new algorithms with other existing methods. Key words. Block Krylov subspace methods, Hessenberg process, Arnoldi process, CMRH, GMRES, low-rank matrix equations. AMS subject classifications. 65F10, 65F30 1. Introduction. In this work, we are first interested in solving s systems of linear equations with the same coefficient matrix and different right-hand sides of the form (1.1) A x(i) = y(i); 1 ≤ i ≤ s; where A is a large and sparse n × n real matrix, y(i) is a real column vector of length n, and s n. Such linear systems arise in numerous applications in computational science and engineering such as wave propagation phenomena, quantum chromodynamics, and dynamics of structures [5, 9, 36, 39]. When n is small, it is well known that the solution of (1.1) can be computed by a direct method such as LU or Cholesky factorization. -
Determinant Formulas and Cofactors
Determinant formulas and cofactors Now that we know the properties of the determinant, it’s time to learn some (rather messy) formulas for computing it. Formula for the determinant We know that the determinant has the following three properties: 1. det I = 1 2. Exchanging rows reverses the sign of the determinant. 3. The determinant is linear in each row separately. Last class we listed seven consequences of these properties. We can use these ten properties to find a formula for the determinant of a 2 by 2 matrix: � � � � � � � a b � � a 0 � � 0 b � � � = � � + � � � c d � � c d � � c d � � � � � � � � � � a 0 � � a 0 � � 0 b � � 0 b � = � � + � � + � � + � � � c 0 � � 0 d � � c 0 � � 0 d � = 0 + ad + (−cb) + 0 = ad − bc. By applying property 3 to separate the individual entries of each row we could get a formula for any other square matrix. However, for a 3 by 3 matrix we’ll have to add the determinants of twenty seven different matrices! Many of those determinants are zero. The non-zero pieces are: � � � � � � � � � a a a � � a 0 0 � � a 0 0 � � 0 a 0 � � 11 12 13 � � 11 � � 11 � � 12 � � a21 a22 a23 � = � 0 a22 0 � + � 0 0 a23 � + � a21 0 0 � � � � � � � � � � a31 a32 a33 � � 0 0 a33 � � 0 a32 0 � � 0 0 a33 � � � � � � � � 0 a 0 � � 0 0 a � � 0 0 a � � 12 � � 13 � � 13 � + � 0 0 a23 � + � a21 0 0 � + � 0 a22 0 � � � � � � � � a31 0 0 � � 0 a32 0 � � a31 0 0 � = a11 a22a33 − a11a23 a33 − a12a21a33 +a12a23a31 + a13 a21a32 − a13a22a31. Each of the non-zero pieces has one entry from each row in each column, as in a permutation matrix. -
Mathematische Annalen Digital Object Identifier (DOI) 10.1007/S002080100153
Math. Ann. (2001) Mathematische Annalen Digital Object Identifier (DOI) 10.1007/s002080100153 Pfaff τ-functions M. Adler · T. Shiota · P. van Moerbeke Received: 20 September 1999 / Published online: ♣ – © Springer-Verlag 2001 Consider the two-dimensional Toda lattice, with certain skew-symmetric initial condition, which is preserved along the locus s =−t of the space of time variables. Restricting the solution to s =−t, we obtain another hierarchy called Pfaff lattice, which has its own tau function, being equal to the square root of the restriction of 2D-Toda tau function. We study its bilinear and Fay identities, W and Virasoro symmetries, relation to symmetric and symplectic matrix integrals and quasiperiodic solutions. 0. Introduction Consider the set of equations ∂m∞ n ∂m∞ n = Λ m∞ , =−m∞(Λ ) ,n= 1, 2,..., (0.1) ∂tn ∂sn on infinite matrices m∞ = m∞(t, s) = (µi,j (t, s))0≤i,j<∞ , M. Adler∗ Department of Mathematics, Brandeis University, Waltham, MA 02454–9110, USA (e-mail: [email protected]) T. Shiota∗∗ Department of Mathematics, Kyoto University, Kyoto 606–8502, Japan (e-mail: [email protected]) P. van Moerbeke∗∗∗ Department of Mathematics, Universit´e de Louvain, 1348 Louvain-la-Neuve, Belgium Brandeis University, Waltham, MA 02454–9110, USA (e-mail: [email protected] and @math.brandeis.edu) ∗ The support of a National Science Foundation grant # DMS-98-4-50790 is gratefully ac- knowledged. ∗∗ The support of Japanese ministry of education’s grant-in-aid for scientific research, and the hospitality of the University of Louvain and Brandeis University are gratefully acknowledged. -
The Unsymmetric Eigenvalue Problem
Jim Lambers CME 335 Spring Quarter 2010-11 Lecture 4 Supplemental Notes The Unsymmetric Eigenvalue Problem Properties and Decompositions Let A be an n × n matrix. A nonzero vector x is called an eigenvector of A if there exists a scalar λ such that Ax = λx: The scalar λ is called an eigenvalue of A, and we say that x is an eigenvector of A corresponding to λ. We see that an eigenvector of A is a vector for which matrix-vector multiplication with A is equivalent to scalar multiplication by λ. We say that a nonzero vector y is a left eigenvector of A if there exists a scalar λ such that λyH = yH A: The superscript H refers to the Hermitian transpose, which includes transposition and complex conjugation. That is, for any matrix A, AH = AT . An eigenvector of A, as defined above, is sometimes called a right eigenvector of A, to distinguish from a left eigenvector. It can be seen that if y is a left eigenvector of A with eigenvalue λ, then y is also a right eigenvector of AH , with eigenvalue λ. Because x is nonzero, it follows that if x is an eigenvector of A, then the matrix A − λI is singular, where λ is the corresponding eigenvalue. Therefore, λ satisfies the equation det(A − λI) = 0: The expression det(A−λI) is a polynomial of degree n in λ, and therefore is called the characteristic polynomial of A (eigenvalues are sometimes called characteristic values). It follows from the fact that the eigenvalues of A are the roots of the characteristic polynomial that A has n eigenvalues, which can repeat, and can also be complex, even if A is real. -
Computing the Jordan Structure of an Eigenvalue∗
SIAM J. MATRIX ANAL.APPL. c 2017 Society for Industrial and Applied Mathematics Vol. 38, No. 3, pp. 949{966 COMPUTING THE JORDAN STRUCTURE OF AN EIGENVALUE∗ NICOLA MASTRONARDIy AND PAUL VAN DOORENz Abstract. In this paper we revisit the problem of finding an orthogonal similarity transformation that puts an n × n matrix A in a block upper-triangular form that reveals its Jordan structure at a particular eigenvalue λ0. The obtained form in fact reveals the dimensions of the null spaces of i (A − λ0I) at that eigenvalue via the sizes of the leading diagonal blocks, and from this the Jordan structure at λ0 is then easily recovered. The method starts from a Hessenberg form that already reveals several properties of the Jordan structure of A. It then updates the Hessenberg form in an efficient way to transform it to a block-triangular form in O(mn2) floating point operations, where m is the total multiplicity of the eigenvalue. The method only uses orthogonal transformations and is backward stable. We illustrate the method with a number of numerical examples. Key words. Jordan structure, staircase form, Hessenberg form AMS subject classifications. 65F15, 65F25 DOI. 10.1137/16M1083098 1. Introduction. Finding the eigenvalues and their corresponding Jordan struc- ture of a matrix A is one of the most studied problems in numerical linear algebra. This structure plays an important role in the solution of explicit differential equations, which can be modeled as n×n (1.1) λx(t) = Ax(t); x(0) = x0;A 2 R ; where λ stands for the differential operator. -
11.5 Reduction of a General Matrix to Hessenberg Form
482 Chapter 11. Eigensystems is equivalent to the 2n 2n real problem × A B u u − =λ (11.4.2) BA·v v T T Note that the 2n 2n matrix in (11.4.2) is symmetric: A = A and B = B visit website http://www.nr.com or call 1-800-872-7423 (North America only),or send email to [email protected] (outside North America). readable files (including this one) to any servercomputer, is strictly prohibited. To order Numerical Recipes books,diskettes, or CDROMs Permission is granted for internet users to make one paper copy their own personal use. Further reproduction, or any copying of machine- Copyright (C) 1988-1992 by Cambridge University Press.Programs Numerical Recipes Software. Sample page from NUMERICAL RECIPES IN C: THE ART OF SCIENTIFIC COMPUTING (ISBN 0-521-43108-5) if C is Hermitian.× − Corresponding to a given eigenvalue λ, the vector v (11.4.3) −u is also an eigenvector, as you can verify by writing out the two matrix equa- tions implied by (11.4.2). Thus if λ1,λ2,...,λn are the eigenvalues of C, then the 2n eigenvalues of the augmented problem (11.4.2) are λ1,λ1,λ2,λ2,..., λn,λn; each, in other words, is repeated twice. The eigenvectors are pairs of the form u + iv and i(u + iv); that is, they are the same up to an inessential phase. Thus we solve the augmented problem (11.4.2), and choose one eigenvalue and eigenvector from each pair. These give the eigenvalues and eigenvectors of the original matrix C.