The Square Root Function of a Matrix
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Regular Linear Systems on Cp1 and Their Monodromy Groups V.P
Astérisque V. P. KOSTOV Regular linear systems onCP1 and their monodromy groups Astérisque, tome 222 (1994), p. 259-283 <http://www.numdam.org/item?id=AST_1994__222__259_0> © Société mathématique de France, 1994, tous droits réservés. L’accès aux archives de la collection « Astérisque » (http://smf4.emath.fr/ Publications/Asterisque/) implique l’accord avec les conditions générales d’uti- lisation (http://www.numdam.org/conditions). Toute utilisation commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ REGULAR LINEAR SYSTEMS ON CP1 AND THEIR MONODROMY GROUPS V.P. KOSTOV 1. INTRODUCTION 1.1 A meromorphic linear system of differential equations on CP1 can be pre sented in the form X = A(t)X (1) where A{t) is a meromorphic on CP1 n x n matrix function, " • " = d/dt. Denote its poles ai,... ,ap+i, p > 1. We consider the dependent variable X to be also n x n-matrix. Definition. System (1) is called fuchsian if all the poles of the matrix- function A(t) axe of first order. Definition. System (1) is called regular at the pole a,j if in its neighbour hood the solutions of the system are of moderate growth rate, i.e. IW-a^l^Odt-a^), Ni E R, j = 1,...., p + 1 Here || • || denotes an arbitrary norm in gl(n, C) and we consider a restriction of the solution to a sector with vertex at ctj and of a sufficiently small radius, i.e. -
The Rational and Jordan Forms Linear Algebra Notes
The Rational and Jordan Forms Linear Algebra Notes Satya Mandal November 5, 2005 1 Cyclic Subspaces In a given context, a "cyclic thing" is an one generated "thing". For example, a cyclic groups is a one generated group. Likewise, a module M over a ring R is said to be a cyclic module if M is one generated or M = Rm for some m 2 M: We do not use the expression "cyclic vector spaces" because one generated vector spaces are zero or one dimensional vector spaces. 1.1 (De¯nition and Facts) Suppose V is a vector space over a ¯eld F; with ¯nite dim V = n: Fix a linear operator T 2 L(V; V ): 1. Write R = F[T ] = ff(T ) : f(X) 2 F[X]g L(V; V )g: Then R = F[T ]g is a commutative ring. (We did considered this ring in last chapter in the proof of Caley-Hamilton Theorem.) 2. Now V acquires R¡module structure with scalar multiplication as fol- lows: Define f(T )v = f(T )(v) 2 V 8 f(T ) 2 F[T ]; v 2 V: 3. For an element v 2 V de¯ne Z(v; T ) = F[T ]v = ff(T )v : f(T ) 2 Rg: 1 Note that Z(v; T ) is the cyclic R¡submodule generated by v: (I like the notation F[T ]v, the textbook uses the notation Z(v; T ).) We say, Z(v; T ) is the T ¡cyclic subspace generated by v: 4. If V = Z(v; T ) = F[T ]v; we say that that V is a T ¡cyclic space, and v is called the T ¡cyclic generator of V: (Here, I di®er a little from the textbook.) 5. -
MAT247 Algebra II Assignment 5 Solutions
MAT247 Algebra II Assignment 5 Solutions 1. Find the Jordan canonical form and a Jordan basis for the map or matrix given in each part below. (a) Let V be the real vector space spanned by the polynomials xiyj (in two variables) with i + j ≤ 3. Let T : V V be the map Dx + Dy, where Dx and Dy respectively denote 2 differentiation with respect to x and y. (Thus, Dx(xy) = y and Dy(xy ) = 2xy.) 0 1 1 1 1 1 ! B0 1 2 1 C (b) A = B C over Q @0 0 1 -1A 0 0 0 2 Solution: (a) The operator T is nilpotent so its characterictic polynomial splits and its only eigenvalue is zero and K0 = V. We have Im(T) = spanf1; x; y; x2; xy; y2g; Im(T 2) = spanf1; x; yg Im(T 3) = spanf1g T 4 = 0: Thus the longest cycle for eigenvalue zero has length 4. Moreover, since the number of cycles of length at least r is given by dim(Im(T r-1)) - dim(Im(T r)), the number of cycles of lengths at least 4, 3, 2, 1 is respectively 1, 2, 3, and 4. Thus the number of cycles of lengths 4,3,2,1 is respectively 1,1,1,1. Denoting the r × r Jordan block with λ on the diagonal by Jλ,r, the Jordan canonical form is thus 0 1 J0;4 B J0;3 C J = B C : @ J0;2 A J0;1 We now proceed to find a corresponding Jordan basis, i.e. -
Jordan Decomposition for Differential Operators Samuel Weatherhog Bsc Hons I, BE Hons IIA
Jordan Decomposition for Differential Operators Samuel Weatherhog BSc Hons I, BE Hons IIA A thesis submitted for the degree of Master of Philosophy at The University of Queensland in 2017 School of Mathematics and Physics i Abstract One of the most well-known theorems of linear algebra states that every linear operator on a complex vector space has a Jordan decomposition. There are now numerous ways to prove this theorem, how- ever a standard method of proof relies on the existence of an eigenvector. Given a finite-dimensional, complex vector space V , every linear operator T : V ! V has an eigenvector (i.e. a v 2 V such that (T − λI)v = 0 for some λ 2 C). If we are lucky, V may have a basis consisting of eigenvectors of T , in which case, T is diagonalisable. Unfortunately this is not always the case. However, by relaxing the condition (T − λI)v = 0 to the weaker condition (T − λI)nv = 0 for some n 2 N, we can always obtain a basis of generalised eigenvectors. In fact, there is a canonical decomposition of V into generalised eigenspaces and this is essentially the Jordan decomposition. The topic of this thesis is an analogous theorem for differential operators. The existence of a Jordan decomposition in this setting was first proved by Turrittin following work of Hukuhara in the one- dimensional case. Subsequently, Levelt proved uniqueness and provided a more conceptual proof of the original result. As a corollary, Levelt showed that every differential operator has an eigenvector. He also noted that this was a strange chain of logic: in the linear setting, the existence of an eigen- vector is a much easier result and is in fact used to obtain the Jordan decomposition. -
(VI.E) Jordan Normal Form
(VI.E) Jordan Normal Form Set V = Cn and let T : V ! V be any linear transformation, with distinct eigenvalues s1,..., sm. In the last lecture we showed that V decomposes into stable eigenspaces for T : s s V = W1 ⊕ · · · ⊕ Wm = ker (T − s1I) ⊕ · · · ⊕ ker (T − smI). Let B = fB1,..., Bmg be a basis for V subordinate to this direct sum and set B = [T j ] , so that k Wk Bk [T]B = diagfB1,..., Bmg. Each Bk has only sk as eigenvalue. In the event that A = [T]eˆ is s diagonalizable, or equivalently ker (T − skI) = ker(T − skI) for all k , B is an eigenbasis and [T]B is a diagonal matrix diagf s1,..., s1 ;...; sm,..., sm g. | {z } | {z } d1=dim W1 dm=dim Wm Otherwise we must perform further surgery on the Bk ’s separately, in order to transform the blocks Bk (and so the entire matrix for T ) into the “simplest possible” form. The attentive reader will have noticed above that I have written T − skI in place of skI − T . This is a strategic move: when deal- ing with characteristic polynomials it is far more convenient to write det(lI − A) to produce a monic polynomial. On the other hand, as you’ll see now, it is better to work on the individual Wk with the nilpotent transformation T j − s I =: N . Wk k k Decomposition of the Stable Eigenspaces (Take 1). Let’s briefly omit subscripts and consider T : W ! W with one eigenvalue s , dim W = d , B a basis for W and [T]B = B. -
MA251 Algebra I: Advanced Linear Algebra Revision Guide
MA251 Algebra I: Advanced Linear Algebra Revision Guide Written by David McCormick ii MA251 Algebra I: Advanced Linear Algebra Contents 1 Change of Basis 1 2 The Jordan Canonical Form 1 2.1 Eigenvalues and Eigenvectors . 1 2.2 Minimal Polynomials . 2 2.3 Jordan Chains, Jordan Blocks and Jordan Bases . 3 2.4 Computing the Jordan Canonical Form . 4 2.5 Exponentiation of a Matrix . 6 2.6 Powers of a Matrix . 7 3 Bilinear Maps and Quadratic Forms 8 3.1 Definitions . 8 3.2 Change of Variable under the General Linear Group . 9 3.3 Change of Variable under the Orthogonal Group . 10 3.4 Unitary, Hermitian and Normal Matrices . 11 4 Finitely Generated Abelian Groups 12 4.1 Generators and Cyclic Groups . 13 4.2 Subgroups and Cosets . 13 4.3 Quotient Groups and the First Isomorphism Theorem . 14 4.4 Abelian Groups and Matrices Over Z .............................. 15 Introduction This revision guide for MA251 Algebra I: Advanced Linear Algebra has been designed as an aid to revision, not a substitute for it. While it may seem that the module is impenetrably hard, there's nothing in Algebra I to be scared of. The underlying theme is normal forms for matrices, and so while there is some theory you have to learn, most of the module is about doing computations. (After all, this is mathematics, not philosophy.) Finding books for this module is hard. My personal favourite book on linear algebra is sadly out-of- print and bizarrely not in the library, but if you can find a copy of Evar Nering's \Linear Algebra and Matrix Theory" then it's well worth it (though it doesn't cover the abelian groups section of the course). -
On the M-Th Roots of a Complex Matrix
The Electronic Journal of Linear Algebra ISSN 1081-3810 A publication of the International Linear Algebra Society Volume 9, pp. 32-41, April 2002 ELA http://math.technion.ac.il/iic/ela ON THE mth ROOTS OF A COMPLEX MATRIX∗ PANAYIOTIS J. PSARRAKOS† Abstract. If an n × n complex matrix A is nonsingular, then for everyinteger m>1,Ahas an mth root B, i.e., Bm = A. In this paper, we present a new simple proof for the Jordan canonical form of the root B. Moreover, a necessaryand sufficient condition for the existence of mth roots of a singular complex matrix A is obtained. This condition is in terms of the dimensions of the null spaces of the powers Ak (k =0, 1, 2,...). Key words. Ascent sequence, eigenvalue, eigenvector, Jordan matrix, matrix root. AMS subject classifications. 15A18, 15A21, 15A22, 47A56 1. Introduction and preliminaries. Let Mn be the algebra of all n × n complex matrices and let A ∈Mn. For an integer m>1, amatrix B ∈Mn is called an mth root of A if Bm = A.IfthematrixA is nonsingular, then it always has an mth root B. This root is not unique and its Jordan structure is related to k the Jordan structure of A [2, pp. 231-234]. In particular, (λ − µ0) is an elementary m k divisor of B if and only if (λ − µ0 ) is an elementary divisor of A.IfA is a singular complex matrix, then it may have no mth roots. For example, there is no matrix 01 B such that B2 = . As a consequence, the problem of characterizing the 00 singular matrices, which have mth roots, is of interest [1], [2]. -
Newton's Method for the Matrix Square Root*
MATHEMATICS OF COMPUTATION VOLUME 46, NUMBER 174 APRIL 1986, PAGES 537-549 Newton's Method for the Matrix Square Root* By Nicholas J. Higham Abstract. One approach to computing a square root of a matrix A is to apply Newton's method to the quadratic matrix equation F( X) = X2 - A =0. Two widely-quoted matrix square root iterations obtained by rewriting this Newton iteration are shown to have excellent mathematical convergence properties. However, by means of a perturbation analysis and supportive numerical examples, it is shown that these simplified iterations are numerically unstable. A further variant of Newton's method for the matrix square root, recently proposed in the literature, is shown to be, for practical purposes, numerically stable. 1. Introduction. A square root of an n X n matrix A with complex elements, A e C"x", is a solution X e C"*" of the quadratic matrix equation (1.1) F(X) = X2-A=0. A natural approach to computing a square root of A is to apply Newton's method to (1.1). For a general function G: CXn -* Cx", Newton's method for the solution of G(X) = 0 is specified by an initial approximation X0 and the recurrence (see [14, p. 140], for example) (1.2) Xk+l = Xk-G'{XkylG{Xk), fc = 0,1,2,..., where G' denotes the Fréchet derivative of G. Identifying F(X+ H) = X2 - A +(XH + HX) + H2 with the Taylor series for F we see that F'(X) is a linear operator, F'(X): Cx" ^ C"x", defined by F'(X)H= XH+ HX. -
Sensitivity and Stability Analysis of Nonlinear Kalman Filters with Application to Aircraft Attitude Estimation
Graduate Theses, Dissertations, and Problem Reports 2013 Sensitivity and stability analysis of nonlinear Kalman filters with application to aircraft attitude estimation Matthew Brandon Rhudy West Virginia University Follow this and additional works at: https://researchrepository.wvu.edu/etd Recommended Citation Rhudy, Matthew Brandon, "Sensitivity and stability analysis of nonlinear Kalman filters with application ot aircraft attitude estimation" (2013). Graduate Theses, Dissertations, and Problem Reports. 3659. https://researchrepository.wvu.edu/etd/3659 This Dissertation is protected by copyright and/or related rights. It has been brought to you by the The Research Repository @ WVU with permission from the rights-holder(s). You are free to use this Dissertation in any way that is permitted by the copyright and related rights legislation that applies to your use. For other uses you must obtain permission from the rights-holder(s) directly, unless additional rights are indicated by a Creative Commons license in the record and/ or on the work itself. This Dissertation has been accepted for inclusion in WVU Graduate Theses, Dissertations, and Problem Reports collection by an authorized administrator of The Research Repository @ WVU. For more information, please contact [email protected]. SENSITIVITY AND STABILITY ANALYSIS OF NONLINEAR KALMAN FILTERS WITH APPLICATION TO AIRCRAFT ATTITUDE ESTIMATION by Matthew Brandon Rhudy Dissertation submitted to the Benjamin M. Statler College of Engineering and Mineral Resources at West Virginia University in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Aerospace Engineering Approved by Dr. Yu Gu, Committee Chairperson Dr. John Christian Dr. Gary Morris Dr. Marcello Napolitano Dr. Powsiri Klinkhachorn Department of Mechanical and Aerospace Engineering Morgantown, West Virginia 2013 Keywords: Attitude Estimation, Extended Kalman Filter, GPS/INS Sensor Fusion, Stochastic Stability Copyright 2013, Matthew B. -
Matlib: Matrix Functions for Teaching and Learning Linear Algebra and Multivariate Statistics
Package ‘matlib’ August 21, 2021 Type Package Title Matrix Functions for Teaching and Learning Linear Algebra and Multivariate Statistics Version 0.9.5 Date 2021-08-10 Maintainer Michael Friendly <[email protected]> Description A collection of matrix functions for teaching and learning matrix linear algebra as used in multivariate statistical methods. These functions are mainly for tutorial purposes in learning matrix algebra ideas using R. In some cases, functions are provided for concepts available elsewhere in R, but where the function call or name is not obvious. In other cases, functions are provided to show or demonstrate an algorithm. In addition, a collection of functions are provided for drawing vector diagrams in 2D and 3D. License GPL (>= 2) Language en-US URL https://github.com/friendly/matlib BugReports https://github.com/friendly/matlib/issues LazyData TRUE Suggests knitr, rglwidget, rmarkdown, carData, webshot2, markdown Additional_repositories https://dmurdoch.github.io/drat Imports xtable, MASS, rgl, car, methods VignetteBuilder knitr RoxygenNote 7.1.1 Encoding UTF-8 NeedsCompilation no Author Michael Friendly [aut, cre] (<https://orcid.org/0000-0002-3237-0941>), John Fox [aut], Phil Chalmers [aut], Georges Monette [ctb], Gaston Sanchez [ctb] 1 2 R topics documented: Repository CRAN Date/Publication 2021-08-21 15:40:02 UTC R topics documented: adjoint . .3 angle . .4 arc..............................................5 arrows3d . .6 buildTmat . .8 cholesky . .9 circle3d . 10 class . 11 cofactor . 11 cone3d . 12 corner . 13 Det.............................................. 14 echelon . 15 Eigen . 16 gaussianElimination . 17 Ginv............................................. 18 GramSchmidt . 20 gsorth . 21 Inverse............................................ 22 J............................................... 23 len.............................................. 23 LU.............................................. 24 matlib . 25 matrix2latex . 27 minor . 27 MoorePenrose . -
Similar Matrices and Jordan Form
Similar matrices and Jordan form We’ve nearly covered the entire heart of linear algebra – once we’ve finished singular value decompositions we’ll have seen all the most central topics. AT A is positive definite A matrix is positive definite if xT Ax > 0 for all x 6= 0. This is a very important class of matrices; positive definite matrices appear in the form of AT A when computing least squares solutions. In many situations, a rectangular matrix is multiplied by its transpose to get a square matrix. Given a symmetric positive definite matrix A, is its inverse also symmet ric and positive definite? Yes, because if the (positive) eigenvalues of A are −1 l1, l2, · · · ld then the eigenvalues 1/l1, 1/l2, · · · 1/ld of A are also positive. If A and B are positive definite, is A + B positive definite? We don’t know much about the eigenvalues of A + B, but we can use the property xT Ax > 0 and xT Bx > 0 to show that xT(A + B)x > 0 for x 6= 0 and so A + B is also positive definite. Now suppose A is a rectangular (m by n) matrix. A is almost certainly not symmetric, but AT A is square and symmetric. Is AT A positive definite? We’d rather not try to find the eigenvalues or the pivots of this matrix, so we ask when xT AT Ax is positive. Simplifying xT AT Ax is just a matter of moving parentheses: xT (AT A)x = (Ax)T (Ax) = jAxj2 ≥ 0. -
MATH. 513. JORDAN FORM Let A1,...,Ak Be Square Matrices of Size
MATH. 513. JORDAN FORM Let A1,...,Ak be square matrices of size n1, . , nk, respectively with entries in a field F . We define the matrix A1 ⊕ ... ⊕ Ak of size n = n1 + ... + nk as the block matrix A1 0 0 ... 0 0 A2 0 ... 0 . . 0 ...... 0 Ak It is called the direct sum of the matrices A1,...,Ak. A matrix of the form λ 1 0 ... 0 0 λ 1 ... 0 . . 0 . λ 1 0 ...... 0 λ is called a Jordan block. If k is its size, it is denoted by Jk(λ). A direct sum J = Jk1 ⊕ ... ⊕ Jkr (λr) of Jordan blocks is called a Jordan matrix. Theorem. Let T : V → V be a linear operator in a finite-dimensional vector space over a field F . Assume that the characteristic polynomial of T is a product of linear polynimials. Then there exists a basis E in V such that [T ]E is a Jordan matrix. Corollary. Let A ∈ Mn(F ). Assume that its characteristic polynomial is a product of linear polynomials. Then there exists a Jordan matrix J and an invertible matrix C such that A = CJC−1. Notice that the Jordan matrix J (which is called a Jordan form of A) is not defined uniquely. For example, we can permute its Jordan blocks. Otherwise the matrix J is defined uniquely (see Problem 7). On the other hand, there are many choices for C. We have seen this already in the diagonalization process. What is good about it? We have, as in the case when A is diagonalizable, AN = CJ N C−1.