MATH 320 NOTES 4 5.4 Invariant Subspaces and Cayley-Hamilton
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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. -
Solution to Homework 5
Solution to Homework 5 Sec. 5.4 1 0 2. (e) No. Note that A = is in W , but 0 2 0 1 1 0 0 2 T (A) = = 1 0 0 2 1 0 is not in W . Hence, W is not a T -invariant subspace of V . 3. Note that T : V ! V is a linear operator on V . To check that W is a T -invariant subspace of V , we need to know if T (w) 2 W for any w 2 W . (a) Since we have T (0) = 0 2 f0g and T (v) 2 V; so both of f0g and V to be T -invariant subspaces of V . (b) Note that 0 2 N(T ). For any u 2 N(T ), we have T (u) = 0 2 N(T ): Hence, N(T ) is a T -invariant subspace of V . For any v 2 R(T ), as R(T ) ⊂ V , we have v 2 V . So, by definition, T (v) 2 R(T ): Hence, R(T ) is also a T -invariant subspace of V . (c) Note that for any v 2 Eλ, λv is a scalar multiple of v, so λv 2 Eλ as Eλ is a subspace. So we have T (v) = λv 2 Eλ: Hence, Eλ is a T -invariant subspace of V . 4. For any w in W , we know that T (w) is in W as W is a T -invariant subspace of V . Then, by induction, we know that T k(w) is also in W for any k. k Suppose g(T ) = akT + ··· + a1T + a0, we have k g(T )(w) = akT (w) + ··· + a1T (w) + a0(w) 2 W because it is just a linear combination of elements in W . -
Spectral Coupling for Hermitian Matrices
Spectral coupling for Hermitian matrices Franc¸oise Chatelin and M. Monserrat Rincon-Camacho Technical Report TR/PA/16/240 Publications of the Parallel Algorithms Team http://www.cerfacs.fr/algor/publications/ SPECTRAL COUPLING FOR HERMITIAN MATRICES FRANC¸OISE CHATELIN (1);(2) AND M. MONSERRAT RINCON-CAMACHO (1) Cerfacs Tech. Rep. TR/PA/16/240 Abstract. The report presents the information processing that can be performed by a general hermitian matrix when two of its distinct eigenvalues are coupled, such as λ < λ0, instead of λ+λ0 considering only one eigenvalue as traditional spectral theory does. Setting a = 2 = 0 and λ0 λ 6 e = 2− > 0, the information is delivered in geometric form, both metric and trigonometric, associated with various right-angled triangles exhibiting optimality properties quantified as ratios or product of a and e. The potential optimisation has a triple nature which offers two j j e possibilities: in the case λλ0 > 0 they are characterised by a and a e and in the case λλ0 < 0 a j j j j by j j and a e. This nature is revealed by a key generalisation to indefinite matrices over R or e j j C of Gustafson's operator trigonometry. Keywords: Spectral coupling, indefinite symmetric or hermitian matrix, spectral plane, invariant plane, catchvector, antieigenvector, midvector, local optimisation, Euler equation, balance equation, torus in 3D, angle between complex lines. 1. Spectral coupling 1.1. Introduction. In the work we present below, we focus our attention on the coupling of any two distinct real eigenvalues λ < λ0 of a general hermitian or symmetric matrix A, a coupling called spectral coupling. -
Section 18.1-2. in the Next 2-3 Lectures We Will Have a Lightning Introduction to Representations of finite Groups
Section 18.1-2. In the next 2-3 lectures we will have a lightning introduction to representations of finite groups. For any vector space V over a field F , denote by L(V ) the algebra of all linear operators on V , and by GL(V ) the group of invertible linear operators. Note that if dim(V ) = n, then L(V ) = Matn(F ) is isomorphic to the algebra of n×n matrices over F , and GL(V ) = GLn(F ) to its multiplicative group. Definition 1. A linear representation of a set X in a vector space V is a map φ: X ! L(V ), where L(V ) is the set of linear operators on V , the space V is called the space of the rep- resentation. We will often denote the representation of X by (V; φ) or simply by V if the homomorphism φ is clear from the context. If X has any additional structures, we require that the map φ is a homomorphism. For example, a linear representation of a group G is a homomorphism φ: G ! GL(V ). Definition 2. A morphism of representations φ: X ! L(V ) and : X ! L(U) is a linear map T : V ! U, such that (x) ◦ T = T ◦ φ(x) for all x 2 X. In other words, T makes the following diagram commutative φ(x) V / V T T (x) U / U An invertible morphism of two representation is called an isomorphism, and two representa- tions are called isomorphic (or equivalent) if there exists an isomorphism between them. Example. (1) A representation of a one-element set in a vector space V is simply a linear operator on V . -
Linear Algebra Midterm Exam, April 5, 2007 Write Clearly, with Complete
Mathematics 110 Name: GSI Name: Linear Algebra Midterm Exam, April 5, 2007 Write clearly, with complete sentences, explaining your work. You will be graded on clarity, style, and brevity. If you add false statements to a correct argument, you will lose points. Be sure to put your name and your GSI’s name on every page. 1. Let V and W be finite dimensional vector spaces over a field F . (a) What is the definition of the transpose of a linear transformation T : V → W ? What is the relationship between the rank of T and the rank of its transpose? (No proof is required here.) Answer: The transpose of T is the linear transformation T t: W ∗ → V ∗ sending a functional φ ∈ W ∗ to φ ◦ T ∈ V ∗. It has the same rank as T . (b) Let T be a linear operator on V . What is the definition of a T - invariant subspace of V ? What is the definition of the T -cyclic subspace generated by an element of V ? Answer: A T -invariant subspace of V is a linear subspace W such that T w ∈ W whenever w ∈ W . The T -cyclic subspace of V generated by v is the subspace of V spanned by the set of all T nv for n a natural number. (c) Let F := R, let V be the space of polynomials with coefficients in R, and let T : V → V be the operator sending f to xf 0, where f 0 is the derivative of f. Let W be the T -cyclic subspace of V generated by x2 + 1. -
Cyclic Vectors and Invariant Subspaces for the Backward Shift Operator Annales De L’Institut Fourier, Tome 20, No 1 (1970), P
ANNALES DE L’INSTITUT FOURIER R. G. DOUGLAS H. S. SHAPIRO A. L. SHIELDS Cyclic vectors and invariant subspaces for the backward shift operator Annales de l’institut Fourier, tome 20, no 1 (1970), p. 37-76 <http://www.numdam.org/item?id=AIF_1970__20_1_37_0> © Annales de l’institut Fourier, 1970, tous droits réservés. L’accès aux archives de la revue « Annales de l’institut Fourier » (http://annalif.ujf-grenoble.fr/) implique l’accord avec les conditions gé- nérales d’utilisation (http://www.numdam.org/conditions). Toute utilisa- tion commerciale ou impression systématique est constitutive d’une in- fraction pénale. Toute copie ou impression de ce fichier doit conte- nir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ Ann. Inst. Fourier, Grenoble 20,1 (1970), 37-76 CYCLIC VECTORS AND INVARIANT SUBSPACES FOR THE BACKWARD SHIFT OPERATOR (i) by R. G. DOUGLAS (2), H. S. SHAPIRO and A.L. SHIELDS 1. Introduction. Let T denote the unit circle and D the open unit disk in the complex plane. In [3] Beurling studied the closed invariant subspaces for the operator U which consists of multiplication by the coordinate function on the Hilbert space H2 = H^D). The operator U is called the forward (or right) shift, because the action of U is to transform a given function into one whose sequence of Taylor coefficients is shifted one unit to the right, that is, its action on sequences is U : (flo,^,^,...) ——>(0,flo,fli ,...). Strictly speaking, of course, the multiplication and the right shift operate on the distinct (isometric) Hilbert spaces H2 and /2. -
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proceedings OF the AMERICAN MATHEMATICAL SOCIETY Volume 78, Number 1, January 1980 THE INACCESSIBLE INVARIANT SUBSPACES OF CERTAIN C0 OPERATORS JOHN DAUGHTRY Abstract. We extend the Douglas-Pearcy characterization of the inaccessi- ble invariant subspaces of an operator on a finite-dimensional Hubert space to the cases of algebraic operators and certain C0 operators on any Hubert space. This characterization shows that the inaccessible invariant subspaces for such an operator form a lattice. In contrast to D. Herrero's recent result on hyperinvariant subspaces, we show that quasisimilar operators in the classes under consideration have isomorphic lattices of inaccessible in- variant subspaces. Let H be a complex Hubert space. For T in B(H) (the space of bounded linear operators on H) the set of invariant subspaces for T is given the metric dist(M, N) = ||PM — PN|| where PM (PN) is the orthogonal projection on M (N) and "|| ||" denotes the norm in B(H). An invariant subspace M for T is "cyclic" if there exists x in M such that { T"x) spans M. R. G. Douglas and Carl Pearcy [3] have characterized the isolated invariant subspaces for T in the case of finite-dimensional H (see [9, Chapters 6 and 7], for the linear algebra used in this article): An invariant subspace M for T is isolated if and only if M n M, = {0} or M, for every noncyclic summand M, in the primary decomposition for T. In [1] we showed how to view this result as a sharpening of the previously known conditions for the isolation of a solution to a quadratic matrix equation. -
Adiabatic Invariants of the Linear Hamiltonian Systems with Periodic Coefficients
JOURNAL OF DIFFERENTIAL EQUATIONS 42, 47-71 (1981) Adiabatic Invariants of the Linear Hamiltonian Systems with Periodic Coefficients MARK LEVI Department of Mathematics, Duke University, Durham, North Carolina 27706 Received November 19, 1980 0. HISTORICAL REMARKS In 1911 Lorentz and Einstein had offered an explanation of the fact that the ratio of energy to the frequency of radiation of an atom remains constant. During the long time intervals separating two quantum jumps an atom is exposed to varying surrounding electromagnetic fields which should supposedly change the ratio. Their explanation was based on the fact that the surrounding field varies extremely slowly with respect to the frequency of oscillations of the atom. The idea can be illstrated by a slightly simpler model-a pendulum (instead of Bohr’s model of an atom) with a slowly changing length (slowly with respect to the frequency of oscillations of the pendulum). As it turns out, the ratio of energy of the pendulum to its frequency changes very little if its length varies slowly enough from one constant value to another; the pendulum “remembers” the ratio, and the slower the change the better the memory. I had learned this interesting historical remark from Wasow [15]. Those parameters of a system which remain nearly constant during a slow change of a system were named by the physicists the adiabatic invariants, the word “adiabatic” indicating that one parameter changes slowly with respect to another-e.g., the length of the pendulum with respect to the phaze of oscillations. Precise definition of the concept will be given in Section 1. -
A Criterion for the Existence of Common Invariant Subspaces Of
Linear Algebra and its Applications 322 (2001) 51–59 www.elsevier.com/locate/laa A criterion for the existence of common invariant subspaces of matricesୋ Michael Tsatsomeros∗ Department of Mathematics and Statistics, University of Regina, Regina, Saskatchewan, Canada S4S 0A2 Received 4 May 1999; accepted 22 June 2000 Submitted by R.A. Brualdi Abstract It is shown that square matrices A and B have a common invariant subspace W of di- mension k > 1 if and only if for some scalar s, A + sI and B + sI are invertible and their kth compounds have a common eigenvector, which is a Grassmann representative for W.The applicability of this criterion and its ability to yield a basis for the common invariant subspace are investigated. © 2001 Elsevier Science Inc. All rights reserved. AMS classification: 15A75; 47A15 Keywords: Invariant subspace; Compound matrix; Decomposable vector; Grassmann space 1. Introduction The lattice of invariant subspaces of a matrix is a well-studied concept with sev- eral applications. In particular, there is substantial information known about matrices having the same invariant subspaces, or having chains of common invariant subspac- es (see [7]). The question of existence of a non-trivial invariant subspace common to two or more matrices is also of interest. It arises, among other places, in the study of irreducibility of decomposable positive linear maps on operator algebras [3]. It also comes up in what might be called Burnside’s theorem, namely that if two square ୋ Research partially supported by NSERC research grant. ∗ Tel.: +306-585-4771; fax: +306-585-4020. E-mail address: [email protected] (M. -
Subspace Polynomials and Cyclic Subspace Codes,” Arxiv:1404.7739, 2014
1 Subspace Polynomials and Cyclic Subspace Codes Eli Ben-Sasson† Tuvi Etzion∗ Ariel Gabizon† Netanel Raviv∗ Abstract Subspace codes have received an increasing interest recently due to their application in error-correction for random network coding. In particular, cyclic subspace codes are possible candidates for large codes with efficient encoding and decoding algorithms. In this paper we consider such cyclic codes and provide constructions of optimal codes for which their codewords do not have full orbits. We further introduce a new way to represent subspace codes by a class of polynomials called subspace polynomials. We present some constructions of such codes which are cyclic and analyze their parameters. I. INTRODUCTION F F∗ , F N F F Let q be the finite field of size q, and let q q \{0}. For n ∈ denote by qn the field extension of degree n of q which may be seen as the vector space of dimension n over Fq. By abuse of notation, we will not distinguish between these two concepts. Given a non-negative integer k ≤ n, the set of all k-dimensional subspaces of Fqn forms a Grassmannian space (Grassmannian in short) over Fq, which is denoted by Gq (n, k). The size of Gq (n, k) is given by the well-known Gaussian n coefficient . The set of all subspaces of F n is called the projective space of order over F [9] and is denoted by . k q q n q Pq(n) The set Pq(n) is endowed with the metric d(U, V ) = dim U + dim V − 2 dim(U ∩ V ). -
The Semi-Simplicity Manifold of Arbitrary Operators
THE SEMI-SIMPLICITY MANIFOLD OF ARBITRARY OPERATORS BY SHMUEL KANTOROVITZ(i) Introduction. In finite dimensional complex Euclidian space, any linear operator has a unique maximal invariant subspace on which it is semi-simple. It is easily described by means of the Jordan decomposition theorem. The main result of this paper (Theorem 2.1) is a generalization of this fact to infinite di- mensional reflexive Banach space, for arbitrary bounded operators T with real spectrum. Our description of the "semi-simplicity manifold" for T is entirely analytic and basis-free, and seems therefore to be a quite natural candidate for such generalizations to infinite dimension. A similar generalization to infinite dimension of the concepts of Jordan cells and Weyr characteristic will be presented elsewhere. The theory is motivated and illustrated by examples in §3. Notations. The following notations are fixed throughout this paper, and will be used without further explanation. R: the field of real numbers. C : the field of complex numbers. âd : the sigma-algebra of all Borel subsets of R. C(R) : the space of all continuous complex valued functions on R. L"(R) : the usual Lebesgue spaces on R (p = 1). j : integration over R. /: the Fourier transform of / e L1(R). X : an arbitrary complex Banach space. X*: the conjugate of X. B(X) : the Banach algebra of all bounded linear operators acting on X. I : the identity operator on X. | • | : the original norms on X, X* and B(X) (new norms, to be defined, will be denoted by double bars). | • \y, | • |œ: the L\R) andL™^) norms (respectively). -
The Common Invariant Subspace Problem
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector Linear Algebra and its Applications 384 (2004) 1–7 www.elsevier.com/locate/laa The common invariant subspace problem: an approach via Gröbner bases Donu Arapura a, Chris Peterson b,∗ aDepartment of Mathematics, Purdue University, West Lafayette, IN 47907, USA bDepartment of Mathematics, Colorado State University, Fort Collins, CO 80523, USA Received 24 March 2003; accepted 17 November 2003 Submitted by R.A. Brualdi Abstract Let A be an n × n matrix. It is a relatively simple process to construct a homogeneous ideal (generated by quadrics) whose associated projective variety parametrizes the one-dimensional invariant subspaces of A. Given a finite collection of n × n matrices, one can similarly con- struct a homogeneous ideal (again generated by quadrics) whose associated projective variety parametrizes the one-dimensional subspaces which are invariant subspaces for every member of the collection. Gröbner basis techniques then provide a finite, rational algorithm to deter- mine how many points are on this variety. In other words, a finite, rational algorithm is given to determine both the existence and quantity of common one-dimensional invariant subspaces to a set of matrices. This is then extended, for each d, to an algorithm to determine both the existence and quantity of common d-dimensional invariant subspaces to a set of matrices. © 2004 Published by Elsevier Inc. Keywords: Eigenvector; Invariant subspace; Grassmann variety; Gröbner basis; Algorithm 1. Introduction Let A and B be two n × n matrices. In 1984, Dan Shemesh gave a very nice procedure for constructing the maximal A, B invariant subspace, N,onwhichA and B commute.