Linear Algebra and Matrix Methods in Econometrics
Total Page:16
File Type:pdf, Size:1020Kb
Load more
Recommended publications
-
Matrix Analysis (Lecture 1)
Matrix Analysis (Lecture 1) Yikun Zhang∗ March 29, 2018 Abstract Linear algebra and matrix analysis have long played a fundamen- tal and indispensable role in fields of science. Many modern research projects in applied science rely heavily on the theory of matrix. Mean- while, matrix analysis and its ramifications are active fields for re- search in their own right. In this course, we aim to study some fun- damental topics in matrix theory, such as eigen-pairs and equivalence relations of matrices, scrutinize the proofs of essential results, and dabble in some up-to-date applications of matrix theory. Our lecture will maintain a cohesive organization with the main stream of Horn's book[1] and complement some necessary background knowledge omit- ted by the textbook sporadically. 1 Introduction We begin our lectures with Chapter 1 of Horn's book[1], which focuses on eigenvalues, eigenvectors, and similarity of matrices. In this lecture, we re- view the concepts of eigenvalues and eigenvectors with which we are familiar in linear algebra, and investigate their connections with coefficients of the characteristic polynomial. Here we first outline the main concepts in Chap- ter 1 (Eigenvalues, Eigenvectors, and Similarity). ∗School of Mathematics, Sun Yat-sen University 1 Matrix Analysis and its Applications, Spring 2018 (L1) Yikun Zhang 1.1 Change of basis and similarity (Page 39-40, 43) Let V be an n-dimensional vector space over the field F, which can be R, C, or even Z(p) (the integers modulo a specified prime number p), and let the list B1 = fv1; v2; :::; vng be a basis for V. -
Matrix-Valued Moment Problems
Matrix-valued moment problems A Thesis Submitted to the Faculty of Drexel University by David P. Kimsey in partial fulfillment of the requirements for the degree of Doctor of Philosophy in Mathematics June 2011 c Copyright 2011 David P. Kimsey. All Rights Reserved. ii Acknowledgments I wish to thank my advisor Professor Hugo J. Woerdeman for being a source of mathematical and professional inspiration. Woerdeman's encouragement and support have been extremely beneficial during my undergraduate and graduate career. Next, I would like to thank Professor Robert P. Boyer for providing a very important men- toring role which guided me toward a career in mathematics. I owe many thanks to L. Richard Duffy for providing encouragement and discussions on fundamental topics. Professor Dmitry Kaliuzhnyi-Verbovetskyi participated in many helpful discussions which helped shape my understanding of several mathematical topics of interest to me. In addition, Professor Anatolii Grinshpan participated in many useful discussions gave lots of encouragement. I wish to thank my Ph.D. defense committee members: Professors Boyer, Lawrence A. Fialkow, Grinshpan, Pawel Hitczenko, and Woerde- man for pointing out any gaps in my understanding as well as typographical mistakes in my thesis. Finally, I wish to acknowledge funding for my research assistantship which was provided by the National Science Foundation, via the grant DMS-0901628. iii Table of Contents Abstract ................................................................................ iv 1. INTRODUCTION ................................................................ -
A Singularly Valuable Decomposition: the SVD of a Matrix Dan Kalman
A Singularly Valuable Decomposition: The SVD of a Matrix Dan Kalman Dan Kalman is an assistant professor at American University in Washington, DC. From 1985 to 1993 he worked as an applied mathematician in the aerospace industry. It was during that period that he first learned about the SVD and its applications. He is very happy to be teaching again and is avidly following all the discussions and presentations about the teaching of linear algebra. Every teacher of linear algebra should be familiar with the matrix singular value deco~??positiolz(or SVD). It has interesting and attractive algebraic properties, and conveys important geometrical and theoretical insights about linear transformations. The close connection between the SVD and the well-known theo1-j~of diagonalization for sylnmetric matrices makes the topic immediately accessible to linear algebra teachers and, indeed, a natural extension of what these teachers already know. At the same time, the SVD has fundamental importance in several different applications of linear algebra. Gilbert Strang was aware of these facts when he introduced the SVD in his now classical text [22, p. 1421, obselving that "it is not nearly as famous as it should be." Golub and Van Loan ascribe a central significance to the SVD in their defini- tive explication of numerical matrix methods [8, p, xivl, stating that "perhaps the most recurring theme in the book is the practical and theoretical value" of the SVD. Additional evidence of the SVD's significance is its central role in a number of re- cent papers in :Matlgenzatics ivlagazine and the Atnericalz Mathematical ilironthly; for example, [2, 3, 17, 231. -
SUPPLEMENTARY MATERIAL: I. Fitting of the Hessian Matrix
Supplementary Material (ESI) for PCCP This journal is © the Owner Societies 2010 1 SUPPLEMENTARY MATERIAL: I. Fitting of the Hessian matrix In the fitting of the Hessian matrix elements as functions of the reaction coordinate, one can take advantage of symmetry. The non-diagonal elements may be written in the form of numerical derivatives as E(Δα, Δβ ) − E(Δα,−Δβ ) − E(−Δα, Δβ ) + E(−Δα,−Δβ ) H (α, β ) = . (S1) 4δ 2 Here, α and β label any of the 15 atomic coordinates in {Cx, Cy, …, H4z}, E(Δα,Δβ) denotes the DFT energy of CH4 interacting with Ni(111) with a small displacement along α and β, and δ the small displacement used in the second order differencing. For example, the H(Cx,Cy) (or H(Cy,Cx)) is 0, since E(ΔCx ,ΔC y ) = E(ΔC x ,−ΔC y ) and E(−ΔCx ,ΔC y ) = E(−ΔCx ,−ΔC y ) . From Eq.S1, one can deduce the symmetry properties of H of methane interacting with Ni(111) in a geometry belonging to the Cs symmetry (Fig. 1 in the paper): (1) there are always 18 zero elements in the lower triangle of the Hessian matrix (see Fig. S1), (2) the main block matrices A, B and F (see Fig. S1) can be split up in six 3×3 sub-blocks, namely A1, A2 , B1, B2, F1 and F2, in which the absolute values of all the corresponding elements in the sub-blocks corresponding to each other are numerically identical to each other except for the sign of their off-diagonal elements, (3) the triangular matrices E1 and E2 are also numerically the same except for the sign of their off-diagonal terms, (4) the 1 Supplementary Material (ESI) for PCCP This journal is © the Owner Societies 2010 2 block D is a unique block and its off-diagonal terms differ only from each other in their sign. -
EUCLIDEAN DISTANCE MATRIX COMPLETION PROBLEMS June 6
EUCLIDEAN DISTANCE MATRIX COMPLETION PROBLEMS HAW-REN FANG∗ AND DIANNE P. O’LEARY† June 6, 2010 Abstract. A Euclidean distance matrix is one in which the (i, j) entry specifies the squared distance between particle i and particle j. Given a partially-specified symmetric matrix A with zero diagonal, the Euclidean distance matrix completion problem (EDMCP) is to determine the unspecified entries to make A a Euclidean distance matrix. We survey three different approaches to solving the EDMCP. We advocate expressing the EDMCP as a nonconvex optimization problem using the particle positions as variables and solving using a modified Newton or quasi-Newton method. To avoid local minima, we develop a randomized initial- ization technique that involves a nonlinear version of the classical multidimensional scaling, and a dimensionality relaxation scheme with optional weighting. Our experiments show that the method easily solves the artificial problems introduced by Mor´e and Wu. It also solves the 12 much more difficult protein fragment problems introduced by Hen- drickson, and the 6 larger protein problems introduced by Grooms, Lewis, and Trosset. Key words. distance geometry, Euclidean distance matrices, global optimization, dimensional- ity relaxation, modified Cholesky factorizations, molecular conformation AMS subject classifications. 49M15, 65K05, 90C26, 92E10 1. Introduction. Given the distances between each pair of n particles in Rr, n r, it is easy to determine the relative positions of the particles. In many applications,≥ though, we are given only some of the distances and we would like to determine the missing distances and thus the particle positions. We focus in this paper on algorithms to solve this distance completion problem. -
QUADRATIC FORMS and DEFINITE MATRICES 1.1. Definition of A
QUADRATIC FORMS AND DEFINITE MATRICES 1. DEFINITION AND CLASSIFICATION OF QUADRATIC FORMS 1.1. Definition of a quadratic form. Let A denote an n x n symmetric matrix with real entries and let x denote an n x 1 column vector. Then Q = x’Ax is said to be a quadratic form. Note that a11 ··· a1n . x1 Q = x´Ax =(x1...xn) . xn an1 ··· ann P a1ixi . =(x1,x2, ··· ,xn) . P anixi 2 (1) = a11x1 + a12x1x2 + ... + a1nx1xn 2 + a21x2x1 + a22x2 + ... + a2nx2xn + ... + ... + ... 2 + an1xnx1 + an2xnx2 + ... + annxn = Pi ≤ j aij xi xj For example, consider the matrix 12 A = 21 and the vector x. Q is given by 0 12x1 Q = x Ax =[x1 x2] 21 x2 x1 =[x1 +2x2 2 x1 + x2 ] x2 2 2 = x1 +2x1 x2 +2x1 x2 + x2 2 2 = x1 +4x1 x2 + x2 1.2. Classification of the quadratic form Q = x0Ax: A quadratic form is said to be: a: negative definite: Q<0 when x =06 b: negative semidefinite: Q ≤ 0 for all x and Q =0for some x =06 c: positive definite: Q>0 when x =06 d: positive semidefinite: Q ≥ 0 for all x and Q = 0 for some x =06 e: indefinite: Q>0 for some x and Q<0 for some other x Date: September 14, 2004. 1 2 QUADRATIC FORMS AND DEFINITE MATRICES Consider as an example the 3x3 diagonal matrix D below and a general 3 element vector x. 100 D = 020 004 The general quadratic form is given by 100 x1 0 Q = x Ax =[x1 x2 x3] 020 x2 004 x3 x1 =[x 2 x 4 x ] x2 1 2 3 x3 2 2 2 = x1 +2x2 +4x3 Note that for any real vector x =06 , that Q will be positive, because the square of any number is positive, the coefficients of the squared terms are positive and the sum of positive numbers is always positive. -
Removing External Degrees of Freedom from Transition State
Removing External Degrees of Freedom from Transition State Search Methods using Quaternions Marko Melander1,2*, Kari Laasonen1,2, Hannes Jónsson3,4 1) COMP Centre of Excellence, Aalto University, FI-00076 Aalto, Finland 2) Department of Chemistry, Aalto University, FI-00076 Aalto, Finland 3) Department of Applied Physics, Aalto University, FI-00076 Aalto, Finland 4) Faculty of Physical Sciences, University of Iceland, 107 Reykjavík, Iceland 1 ABSTRACT In finite systems, such as nanoparticles and gas-phase molecules, calculations of minimum energy paths (MEP) connecting initial and final states of transitions as well as searches for saddle points are complicated by the presence of external degrees of freedom, such as overall translation and rotation. A method based on quaternion algebra for removing the external degrees of freedom is described here and applied in calculations using two commonly used methods: the nudged elastic band (NEB) method for finding minimum energy paths and DIMER method for finding the minimum mode in minimum mode following searches of first order saddle points. With the quaternion approach, fewer images in the NEB are needed to represent MEPs accurately. In both NEB and DIMER calculations of finite systems, the number of iterations required to reach convergence is significantly reduced. The algorithms have been implemented in the Atomic Simulation Environment (ASE) open source software. Keywords: Nudged Elastic Band, DIMER, quaternion, saddle point, transition. 2 1. INTRODUCTION Chemical reactions, diffusion events and configurational changes of molecules are transitions from some initial arrangement of the atoms to another, from an initial state minimum on the energy surface to a final state minimum. -
Linear Algebra Review James Chuang
Linear algebra review James Chuang December 15, 2016 Contents 2.1 vector-vector products ............................................... 1 2.2 matrix-vector products ............................................... 2 2.3 matrix-matrix products ............................................... 4 3.2 the transpose .................................................... 5 3.3 symmetric matrices ................................................. 5 3.4 the trace ....................................................... 6 3.5 norms ........................................................ 6 3.6 linear independence and rank ............................................ 7 3.7 the inverse ...................................................... 7 3.8 orthogonal matrices ................................................. 8 3.9 range and nullspace of a matrix ........................................... 8 3.10 the determinant ................................................... 9 3.11 quadratic forms and positive semidefinite matrices ................................ 10 3.12 eigenvalues and eigenvectors ........................................... 11 3.13 eigenvalues and eigenvectors of symmetric matrices ............................... 12 4.1 the gradient ..................................................... 13 4.2 the Hessian ..................................................... 14 4.3 gradients and hessians of linear and quadratic functions ............................. 15 4.5 gradients of the determinant ............................................ 16 4.6 eigenvalues -
An Introduction to the HESSIAN
An introduction to the HESSIAN 2nd Edition Photograph of Ludwig Otto Hesse (1811-1874), circa 1860 https://upload.wikimedia.org/wikipedia/commons/6/65/Ludwig_Otto_Hesse.jpg See page for author [Public domain], via Wikimedia Commons I. As the students of the first two years of mathematical analysis well know, the Wronskian, Jacobian and Hessian are the names of three determinants and matrixes, which were invented in the nineteenth century, to make life easy to the mathematicians and to provide nightmares to the students of mathematics. II. I don’t know how the Hessian came to the mind of Ludwig Otto Hesse (1811-1874), a quiet professor father of nine children, who was born in Koenigsberg (I think that Koenigsberg gave birth to a disproportionate 1 number of famous men). It is possible that he was studying the problem of finding maxima, minima and other anomalous points on a bi-dimensional surface. (An alternative hypothesis will be presented in section X. ) While pursuing such study, in one variable, one first looks for the points where the first derivative is zero (if it exists at all), and then examines the second derivative at each of those points, to find out its “quality”, whether it is a maximum, a minimum, or an inflection point. The variety of anomalies on a bi-dimensional surface is larger than for a one dimensional line, and one needs to employ more powerful mathematical instruments. Still, also in two dimensions one starts by looking for points where the two first partial derivatives, with respect to x and with respect to y respectively, exist and are both zero. -
Linear Algebra Primer
Linear Algebra Review Linear Algebra Primer Slides by Juan Carlos Niebles*, Ranjay Krishna* and Maxime Voisin *Stanford Vision and Learning Lab 27 - Sep - 2018 Another, very in-depth linear algebra review from CS229 is available here: http://cs229.stanford.edu/section/cs229-linalg.pdf And a video discussion of linear algebra from EE263 is here (lectures 3 and 4): https://see.stanford.edu/Course/EE263 1 Stanford University Outline Linear Algebra Review • Vectors and matrices – Basic Matrix Operations – Determinants, norms, trace – Special Matrices • Transformation Matrices – Homogeneous coordinates – Translation • Matrix inverse 27 - • Matrix rank Sep - • Eigenvalues and Eigenvectors 2018 • Matrix Calculus 2 Stanford University Outline Vectors and matrices are just Linear Algebra Review • Vectors and matrices collections of ordered numbers – Basic Matrix Operations that represent something: location in space, speed, pixel brightness, – Determinants, norms, trace etc. We’ll define some common – Special Matrices uses and standard operations on • Transformation Matrices them. – Homogeneous coordinates – Translation • Matrix inverse 27 - • Matrix rank Sep - • Eigenvalues and Eigenvectors 2018 • Matrix Calculus 3 Stanford University Vector Linear Algebra Review • A column vector where • A row vector where 27 - Sep - 2018 denotes the transpose operation 4 Stanford University Vector • We’ll default to column vectors in this class Linear Algebra Review 27 - Sep - • You’ll want to keep track of the orientation of your 2018 vectors when programming in python 5 Stanford University Some vectors have a geometric interpretation, others don’t… Linear Algebra Review • Other vectors don’t have a • Some vectors have a geometric interpretation: geometric – Vectors can represent any kind of interpretation: 27 data (pixels, gradients at an - – Points are just vectors image keypoint, etc) Sep - from the origin. -
Lecture 11: Maxima and Minima
LECTURE 11 Maxima and Minima n n Definition 11.1. Let f : R → R be a real-valued function of several variables. A point xo ∈ R is called a local minimum of f if there is a neighborhood U of xo such that f(x) ≥ f(xo) for all x ∈ U. n A point xo ∈ R is called a local maxmum of f if there is a neighborhood U of xo such that f(x) ≤ f(xo) for all x ∈ U . n A point xo ∈ R is called a local extremum if it is either a local minimum or a local maximum. Definition 11.2. Let f : Rn → R be a real-valued function of several variables. A critical point of f is a point xo where ∇f(xo)=0. If a critical point is not also a local extremum then it is called a saddle point. n Theorem 11.3. Suppose U is an open subset of R , f : U → R is differentiable, and xo is a local extremum. Then ∇f(xo)=0 i.e., xo is a critical point of f. Proof. Suppose xo is an extremum of f. Then there exists a neighborhood N of xo such that either f(x) ≥ f (xo) , for all x ∈ N or f(x) ≤ f (xo) , for all x ∈ NR. n Let σ : I ⊂ R → R be any smooth path such that σ(0) = xo. Since σ is in particular continuous, there must be a subinterval IN of I containing 0 such that σ(t) ∈ N,for all t ∈ IN . But then if we define h(t) ≡ f (σ(t)) we see that since σ(t)liesinNfor all t ∈ IN , we must have either h(t)=f(σ(t)) ≥ f (xo)=h(0) , for all t ∈ IN or h(t)=f(σ(t)) ≤ f (xo)=h(0) , for all t ∈ IN . -
Arxiv:1805.04488V5 [Math.NA]
GENERALIZED STANDARD TRIPLES FOR ALGEBRAIC LINEARIZATIONS OF MATRIX POLYNOMIALS∗ EUNICE Y. S. CHAN†, ROBERT M. CORLESS‡, AND LEILI RAFIEE SEVYERI§ Abstract. We define generalized standard triples X, Y , and L(z) = zC1 − C0, where L(z) is a linearization of a regular n×n −1 −1 matrix polynomial P (z) ∈ C [z], in order to use the representation X(zC1 − C0) Y = P (z) which holds except when z is an eigenvalue of P . This representation can be used in constructing so-called algebraic linearizations for matrix polynomials of the form H(z) = zA(z)B(z)+ C ∈ Cn×n[z] from generalized standard triples of A(z) and B(z). This can be done even if A(z) and B(z) are expressed in differing polynomial bases. Our main theorem is that X can be expressed using ℓ the coefficients of the expression 1 = Pk=0 ekφk(z) in terms of the relevant polynomial basis. For convenience, we tabulate generalized standard triples for orthogonal polynomial bases, the monomial basis, and Newton interpolational bases; for the Bernstein basis; for Lagrange interpolational bases; and for Hermite interpolational bases. We account for the possibility of common similarity transformations. Key words. Standard triple, regular matrix polynomial, polynomial bases, companion matrix, colleague matrix, comrade matrix, algebraic linearization, linearization of matrix polynomials. AMS subject classifications. 65F15, 15A22, 65D05 1. Introduction. A matrix polynomial P (z) ∈ Fm×n[z] is a polynomial in the variable z with coef- ficients that are m by n matrices with entries from the field F. We will use F = C, the field of complex k numbers, in this paper.