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Things You Need to Know About Linear Algebra Math 131 Multivariate
the standard (x; y; z) coordinate three-space. Nota- tions for vectors. Geometric interpretation as vec- tors as displacements as well as vectors as points. Vector addition, the zero vector 0, vector subtrac- Things you need to know about tion, scalar multiplication, their properties, and linear algebra their geometric interpretation. Math 131 Multivariate Calculus We start using these concepts right away. In D Joyce, Spring 2014 chapter 2, we'll begin our study of vector-valued functions, and we'll use the coordinates, vector no- The relation between linear algebra and mul- tation, and the rest of the topics reviewed in this tivariate calculus. We'll spend the first few section. meetings reviewing linear algebra. We'll look at just about everything in chapter 1. Section 1.2. Vectors and equations in R3. Stan- Linear algebra is the study of linear trans- dard basis vectors i; j; k in R3. Parametric equa- formations (also called linear functions) from n- tions for lines. Symmetric form equations for a line dimensional space to m-dimensional space, where in R3. Parametric equations for curves x : R ! R2 m is usually equal to n, and that's often 2 or 3. in the plane, where x(t) = (x(t); y(t)). A linear transformation f : Rn ! Rm is one that We'll use standard basis vectors throughout the preserves addition and scalar multiplication, that course, beginning with chapter 2. We'll study tan- is, f(a + b) = f(a) + f(b), and f(ca) = cf(a). We'll gent lines of curves and tangent planes of surfaces generally use bold face for vectors and for vector- in that chapter and throughout the course. -
Schaum's Outline of Linear Algebra (4Th Edition)
SCHAUM’S SCHAUM’S outlines outlines Linear Algebra Fourth Edition Seymour Lipschutz, Ph.D. Temple University Marc Lars Lipson, Ph.D. University of Virginia Schaum’s Outline Series New York Chicago San Francisco Lisbon London Madrid Mexico City Milan New Delhi San Juan Seoul Singapore Sydney Toronto Copyright © 2009, 2001, 1991, 1968 by The McGraw-Hill Companies, Inc. All rights reserved. Except as permitted under the United States Copyright Act of 1976, no part of this publication may be reproduced or distributed in any form or by any means, or stored in a database or retrieval system, without the prior writ- ten permission of the publisher. ISBN: 978-0-07-154353-8 MHID: 0-07-154353-8 The material in this eBook also appears in the print version of this title: ISBN: 978-0-07-154352-1, MHID: 0-07-154352-X. All trademarks are trademarks of their respective owners. Rather than put a trademark symbol after every occurrence of a trademarked name, we use names in an editorial fashion only, and to the benefit of the trademark owner, with no intention of infringement of the trademark. Where such designations appear in this book, they have been printed with initial caps. McGraw-Hill eBooks are available at special quantity discounts to use as premiums and sales promotions, or for use in corporate training programs. To contact a representative please e-mail us at [email protected]. TERMS OF USE This is a copyrighted work and The McGraw-Hill Companies, Inc. (“McGraw-Hill”) and its licensors reserve all rights in and to the work. -
Determinants Math 122 Calculus III D Joyce, Fall 2012
Determinants Math 122 Calculus III D Joyce, Fall 2012 What they are. A determinant is a value associated to a square array of numbers, that square array being called a square matrix. For example, here are determinants of a general 2 × 2 matrix and a general 3 × 3 matrix. a b = ad − bc: c d a b c d e f = aei + bfg + cdh − ceg − afh − bdi: g h i The determinant of a matrix A is usually denoted jAj or det (A). You can think of the rows of the determinant as being vectors. For the 3×3 matrix above, the vectors are u = (a; b; c), v = (d; e; f), and w = (g; h; i). Then the determinant is a value associated to n vectors in Rn. There's a general definition for n×n determinants. It's a particular signed sum of products of n entries in the matrix where each product is of one entry in each row and column. The two ways you can choose one entry in each row and column of the 2 × 2 matrix give you the two products ad and bc. There are six ways of chosing one entry in each row and column in a 3 × 3 matrix, and generally, there are n! ways in an n × n matrix. Thus, the determinant of a 4 × 4 matrix is the signed sum of 24, which is 4!, terms. In this general definition, half the terms are taken positively and half negatively. In class, we briefly saw how the signs are determined by permutations. -
Linear Algebra Handbook
CS419 Linear Algebra January 7, 2021 1 What do we need to know? By the end of this booklet, you should know all the linear algebra you need for CS419. More specifically, you'll understand: • Vector spaces (the important ones, at least) • Dirac (bra-ket) notation and why it's quite nice to use • Linear combinations, linearly independent sets, spanning sets and basis sets • Matrices and linear transformations (they're the same thing) • Changing basis • Inner products and norms • Unitary operations • Tensor products • Why we care about linear algebra 2 Vector Spaces In quantum computing, the `vectors' we'll be working with are going to be made up of complex numbers1. A vector space, V , over C is a set of vectors with the vital property2 that αu + βv 2 V for all α; β 2 C and u; v 2 V . Intuitively, this means we can add together and scale up vectors in V, and we know the result is still in V. Our vectors are going to be lists of n complex numbers, v 2 Cn, and Cn will be our most important vector space. Note we can just as easily define vector spaces over R, the set of real numbers. Over the course of this module, we'll see the reasons3 we use C, but for all this linear algebra, we can stick with R as everyone is happier with real numbers. Rest assured for the entire module, every time you see something like \Consider a vector space V ", this vector space will be Rn or Cn for some n 2 N. -
Lecture 6 — Generalized Eigenspaces & Generalized Weight
18.745 Introduction to Lie Algebras September 28, 2010 Lecture 6 | Generalized Eigenspaces & Generalized Weight Spaces Prof. Victor Kac Scribe: Andrew Geng and Wenzhe Wei Definition 6.1. Let A be a linear operator on a vector space V over field F and let λ 2 F, then the subspace N Vλ = fv j (A − λI) v = 0 for some positive integer Ng is called a generalized eigenspace of A with eigenvalue λ. Note that the eigenspace of A with eigenvalue λ is a subspace of Vλ. Example 6.1. A is a nilpotent operator if and only if V = V0. Proposition 6.1. Let A be a linear operator on a finite dimensional vector space V over an alge- braically closed field F, and let λ1; :::; λs be all eigenvalues of A, n1; n2; :::; ns be their multiplicities. Then one has the generalized eigenspace decomposition: s M V = Vλi where dim Vλi = ni i=1 Proof. By the Jordan normal form of A in some basis e1; e2; :::en. Its matrix is of the following form: 0 1 Jλ1 B Jλ C A = B 2 C B .. C @ . A ; Jλn where Jλi is an ni × ni matrix with λi on the diagonal, 0 or 1 in each entry just above the diagonal, and 0 everywhere else. Let Vλ1 = spanfe1; e2; :::; en1 g;Vλ2 = spanfen1+1; :::; en1+n2 g; :::; so that Jλi acts on Vλi . i.e. Vλi are A-invariant and Aj = λ I + N , N nilpotent. Vλi i ni i i From the above discussion, we obtain the following decomposition of the operator A, called the classical Jordan decomposition A = As + An where As is the operator which in the basis above is the diagonal part of A, and An is the rest (An = A − As). -
Span, Linear Independence and Basis Rank and Nullity
Remarks for Exam 2 in Linear Algebra Span, linear independence and basis The span of a set of vectors is the set of all linear combinations of the vectors. A set of vectors is linearly independent if the only solution to c1v1 + ::: + ckvk = 0 is ci = 0 for all i. Given a set of vectors, you can determine if they are linearly independent by writing the vectors as the columns of the matrix A, and solving Ax = 0. If there are any non-zero solutions, then the vectors are linearly dependent. If the only solution is x = 0, then they are linearly independent. A basis for a subspace S of Rn is a set of vectors that spans S and is linearly independent. There are many bases, but every basis must have exactly k = dim(S) vectors. A spanning set in S must contain at least k vectors, and a linearly independent set in S can contain at most k vectors. A spanning set in S with exactly k vectors is a basis. A linearly independent set in S with exactly k vectors is a basis. Rank and nullity The span of the rows of matrix A is the row space of A. The span of the columns of A is the column space C(A). The row and column spaces always have the same dimension, called the rank of A. Let r = rank(A). Then r is the maximal number of linearly independent row vectors, and the maximal number of linearly independent column vectors. So if r < n then the columns are linearly dependent; if r < m then the rows are linearly dependent. -
Calculus and Differential Equations II
Calculus and Differential Equations II MATH 250 B Linear systems of differential equations Linear systems of differential equations Calculus and Differential Equations II Second order autonomous linear systems We are mostly interested with2 × 2 first order autonomous systems of the form x0 = a x + b y y 0 = c x + d y where x and y are functions of t and a, b, c, and d are real constants. Such a system may be re-written in matrix form as d x x a b = M ; M = : dt y y c d The purpose of this section is to classify the dynamics of the solutions of the above system, in terms of the properties of the matrix M. Linear systems of differential equations Calculus and Differential Equations II Existence and uniqueness (general statement) Consider a linear system of the form dY = M(t)Y + F (t); dt where Y and F (t) are n × 1 column vectors, and M(t) is an n × n matrix whose entries may depend on t. Existence and uniqueness theorem: If the entries of the matrix M(t) and of the vector F (t) are continuous on some open interval I containing t0, then the initial value problem dY = M(t)Y + F (t); Y (t ) = Y dt 0 0 has a unique solution on I . In particular, this means that trajectories in the phase space do not cross. Linear systems of differential equations Calculus and Differential Equations II General solution The general solution to Y 0 = M(t)Y + F (t) reads Y (t) = C1 Y1(t) + C2 Y2(t) + ··· + Cn Yn(t) + Yp(t); = U(t) C + Yp(t); where 0 Yp(t) is a particular solution to Y = M(t)Y + F (t). -
SUPPLEMENT on EIGENVALUES and EIGENVECTORS We Give
SUPPLEMENT ON EIGENVALUES AND EIGENVECTORS We give some extra material on repeated eigenvalues and complex eigenvalues. 1. REPEATED EIGENVALUES AND GENERALIZED EIGENVECTORS For repeated eigenvalues, it is not always the case that there are enough eigenvectors. Let A be an n × n real matrix, with characteristic polynomial m1 mk pA(λ) = (λ1 − λ) ··· (λk − λ) with λ j 6= λ` for j 6= `. Use the following notation for the eigenspace, E(λ j ) = {v : (A − λ j I)v = 0 }. We also define the generalized eigenspace for the eigenvalue λ j by gen m j E (λ j ) = {w : (A − λ j I) w = 0 }, where m j is the multiplicity of the eigenvalue. A vector in E(λ j ) is called a generalized eigenvector. The following is a extension of theorem 7 in the book. 0 m1 mk Theorem (7 ). Let A be an n × n matrix with characteristic polynomial pA(λ) = (λ1 − λ) ··· (λk − λ) , where λ j 6= λ` for j 6= `. Then, the following hold. gen (a) dim(E(λ j )) ≤ m j and dim(E (λ j )) = m j for 1 ≤ j ≤ k. If λ j is complex, then these dimensions are as subspaces of Cn. gen n (b) If B j is a basis for E (λ j ) for 1 ≤ j ≤ k, then B1 ∪ · · · ∪ Bk is a basis of C , i.e., there is always a basis of generalized eigenvectors for all the eigenvalues. If the eigenvalues are all real all the vectors are real, then this gives a basis of Rn. (c) Assume A is a real matrix and all its eigenvalues are real. -
MATH 532: Linear Algebra Chapter 4: Vector Spaces
MATH 532: Linear Algebra Chapter 4: Vector Spaces Greg Fasshauer Department of Applied Mathematics Illinois Institute of Technology Spring 2015 [email protected] MATH 532 1 Outline 1 Spaces and Subspaces 2 Four Fundamental Subspaces 3 Linear Independence 4 Bases and Dimension 5 More About Rank 6 Classical Least Squares 7 Kriging as best linear unbiased predictor [email protected] MATH 532 2 Spaces and Subspaces Outline 1 Spaces and Subspaces 2 Four Fundamental Subspaces 3 Linear Independence 4 Bases and Dimension 5 More About Rank 6 Classical Least Squares 7 Kriging as best linear unbiased predictor [email protected] MATH 532 3 Spaces and Subspaces Spaces and Subspaces While the discussion of vector spaces can be rather dry and abstract, they are an essential tool for describing the world we work in, and to understand many practically relevant consequences. After all, linear algebra is pretty much the workhorse of modern applied mathematics. Moreover, many concepts we discuss now for traditional “vectors” apply also to vector spaces of functions, which form the foundation of functional analysis. [email protected] MATH 532 4 Spaces and Subspaces Vector Space Definition A set V of elements (vectors) is called a vector space (or linear space) over the scalar field F if (A1) x + y 2 V for any x; y 2 V (M1) αx 2 V for every α 2 F and (closed under addition), x 2 V (closed under scalar (A2) (x + y) + z = x + (y + z) for all multiplication), x; y; z 2 V, (M2) (αβ)x = α(βx) for all αβ 2 F, (A3) x + y = y + x for all x; y 2 V, x 2 V, (A4) There exists a zero vector 0 2 V (M3) α(x + y) = αx + αy for all α 2 F, such that x + 0 = x for every x; y 2 V, x 2 V, (M4) (α + β)x = αx + βx for all (A5) For every x 2 V there is a α; β 2 F, x 2 V, negative (−x) 2 V such that (M5)1 x = x for all x 2 V. -
Math 2280 - Lecture 23
Math 2280 - Lecture 23 Dylan Zwick Fall 2013 In our last lecture we dealt with solutions to the system: ′ x = Ax where A is an n × n matrix with n distinct eigenvalues. As promised, today we will deal with the question of what happens if we have less than n distinct eigenvalues, which is what happens if any of the roots of the characteristic polynomial are repeated. This lecture corresponds with section 5.4 of the textbook, and the as- signed problems from that section are: Section 5.4 - 1, 8, 15, 25, 33 The Case of an Order 2 Root Let’s start with the case an an order 2 root.1 So, our eigenvalue equation has a repeated root, λ, of multiplicity 2. There are two ways this can go. The first possibility is that we have two distinct (linearly independent) eigenvectors associated with the eigen- value λ. In this case, all is good, and we just use these two eigenvectors to create two distinct solutions. 1Admittedly, not one of Sherlock Holmes’s more popular mysteries. 1 Example - Find a general solution to the system: 9 4 0 ′ x = −6 −1 0 x 6 4 3 Solution - The characteristic equation of the matrix A is: |A − λI| = (5 − λ)(3 − λ)2. So, A has the distinct eigenvalue λ1 = 5 and the repeated eigenvalue λ2 =3 of multiplicity 2. For the eigenvalue λ1 =5 the eigenvector equation is: 4 4 0 a 0 (A − 5I)v = −6 −6 0 b = 0 6 4 −2 c 0 which has as an eigenvector 1 v1 = −1 . -
23. Eigenvalues and Eigenvectors
23. Eigenvalues and Eigenvectors 11/17/20 Eigenvalues and eigenvectors have a variety of uses. They allow us to solve linear difference and differential equations. For many non-linear equations, they inform us about the long-run behavior of the system. They are also useful for defining functions of matrices. 23.1 Eigenvalues We start with eigenvalues. Eigenvalues and Spectrum. Let A be an m m matrix. An eigenvalue (characteristic value, proper value) of A is a number λ so that× A λI is singular. The spectrum of A, σ(A)= {eigenvalues of A}.− Sometimes it’s possible to find eigenvalues by inspection of the matrix. ◮ Example 23.1.1: Some Eigenvalues. Suppose 1 0 2 1 A = , B = . 0 2 1 2 Here it is pretty obvious that subtracting either I or 2I from A yields a singular matrix. As for matrix B, notice that subtracting I leaves us with two identical columns (and rows), so 1 is an eigenvalue. Less obvious is the fact that subtracting 3I leaves us with linearly independent columns (and rows), so 3 is also an eigenvalue. We’ll see in a moment that 2 2 matrices have at most two eigenvalues, so we have determined the spectrum of each:× σ(A)= {1, 2} and σ(B)= {1, 3}. ◭ 2 MATH METHODS 23.2 Finding Eigenvalues: 2 2 × We have several ways to determine whether a matrix is singular. One method is to check the determinant. It is zero if and only the matrix is singular. That means we can find the eigenvalues by solving the equation det(A λI)=0. -
Chapter 2: Linear Algebra User's Manual
Preprint typeset in JHEP style - HYPER VERSION Chapter 2: Linear Algebra User's Manual Gregory W. Moore Abstract: An overview of some of the finer points of linear algebra usually omitted in physics courses. May 3, 2021 -TOC- Contents 1. Introduction 5 2. Basic Definitions Of Algebraic Structures: Rings, Fields, Modules, Vec- tor Spaces, And Algebras 6 2.1 Rings 6 2.2 Fields 7 2.2.1 Finite Fields 8 2.3 Modules 8 2.4 Vector Spaces 9 2.5 Algebras 10 3. Linear Transformations 14 4. Basis And Dimension 16 4.1 Linear Independence 16 4.2 Free Modules 16 4.3 Vector Spaces 17 4.4 Linear Operators And Matrices 20 4.5 Determinant And Trace 23 5. New Vector Spaces from Old Ones 24 5.1 Direct sum 24 5.2 Quotient Space 28 5.3 Tensor Product 30 5.4 Dual Space 34 6. Tensor spaces 38 6.1 Totally Symmetric And Antisymmetric Tensors 39 6.2 Algebraic structures associated with tensors 44 6.2.1 An Approach To Noncommutative Geometry 47 7. Kernel, Image, and Cokernel 47 7.1 The index of a linear operator 50 8. A Taste of Homological Algebra 51 8.1 The Euler-Poincar´eprinciple 54 8.2 Chain maps and chain homotopies 55 8.3 Exact sequences of complexes 56 8.4 Left- and right-exactness 56 { 1 { 9. Relations Between Real, Complex, And Quaternionic Vector Spaces 59 9.1 Complex structure on a real vector space 59 9.2 Real Structure On A Complex Vector Space 64 9.2.1 Complex Conjugate Of A Complex Vector Space 66 9.2.2 Complexification 67 9.3 The Quaternions 69 9.4 Quaternionic Structure On A Real Vector Space 79 9.5 Quaternionic Structure On Complex Vector Space 79 9.5.1 Complex Structure On Quaternionic Vector Space 81 9.5.2 Summary 81 9.6 Spaces Of Real, Complex, Quaternionic Structures 81 10.