DETERMINANTS Math 121, 11/14/2005 O.Knill
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Lecture # 4 % System of Linear Equations (Cont.)
Lecture # 4 - System of Linear Equations (cont.) In our last lecture, we were starting to apply the Gaussian Elimination Method to our macro model Y = C + 1500 C = 200 + 4 (Y T ) 5 1 T = 100 + 5 Y We de…ned the extended coe¢ cient matrix 1 1 0 1000 [A d] = 2 4 1 4 200 3 5 5 6 7 6 7 6 1 0 1 100 7 6 5 7 4 5 The objective is to use elementary row operations (ERO’s)to transform our system of linear equations into another, simpler system. – Eliminate coe¢ cient for …rst variable (column) from all equations (rows) except …rst equation (row). – Eliminate coe¢ cient for second variable (column) from all equations (rows) except second equation (rows). – Eliminate coe¢ cient for third variable (column) from all equations (rows) except third equation (rows). The objective is to get a system that looks like this: 1 0 0 s1 0 1 0 s2 2 3 0 0 1 s3 4 5 1 Let’suse our example 1 1 0 1500 [A d] = 2 4 1 4 200 3 5 5 6 7 6 7 6 1 0 1 100 7 6 5 7 4 5 Multiply …rst row (equation) by 1 and add it to third row 5 1 1 0 1500 [A d] = 2 4 1 4 200 3 5 5 6 7 6 7 6 0 1 1 400 7 6 5 7 4 5 Multiply …rst row by 4 and add it to row 2 5 1 1 0 1500 [A d] = 2 0 1 4 1400 3 5 5 6 7 6 7 6 0 1 1 400 7 6 5 7 4 5 Add row 2 to row 3 1 1 0 1500 [A d] = 2 0 1 4 1400 3 5 5 6 7 6 7 6 0 0 9 1800 7 6 5 7 4 5 Multiply second row by 5 1 1 0 1500 [A d] = 2 0 1 4 7000 3 6 7 6 7 6 0 0 9 1800 7 6 5 7 4 5 Add row 2 to row 1 1 0 4 8500 [A d] = 2 0 1 4 7000 3 6 7 6 7 6 0 0 9 1800 7 6 5 7 4 5 2 Multiply row 3 by 5 9 1 0 4 8500 [A d] = 2 0 1 4 7000 3 6 7 6 7 6 0 0 1 1000 -
Chapter Four Determinants
Chapter Four Determinants In the first chapter of this book we considered linear systems and we picked out the special case of systems with the same number of equations as unknowns, those of the form T~x = ~b where T is a square matrix. We noted a distinction between two classes of T ’s. While such systems may have a unique solution or no solutions or infinitely many solutions, if a particular T is associated with a unique solution in any system, such as the homogeneous system ~b = ~0, then T is associated with a unique solution for every ~b. We call such a matrix of coefficients ‘nonsingular’. The other kind of T , where every linear system for which it is the matrix of coefficients has either no solution or infinitely many solutions, we call ‘singular’. Through the second and third chapters the value of this distinction has been a theme. For instance, we now know that nonsingularity of an n£n matrix T is equivalent to each of these: ² a system T~x = ~b has a solution, and that solution is unique; ² Gauss-Jordan reduction of T yields an identity matrix; ² the rows of T form a linearly independent set; ² the columns of T form a basis for Rn; ² any map that T represents is an isomorphism; ² an inverse matrix T ¡1 exists. So when we look at a particular square matrix, the question of whether it is nonsingular is one of the first things that we ask. This chapter develops a formula to determine this. (Since we will restrict the discussion to square matrices, in this chapter we will usually simply say ‘matrix’ in place of ‘square matrix’.) More precisely, we will develop infinitely many formulas, one for 1£1 ma- trices, one for 2£2 matrices, etc. -
An Exploration of the Relationship Between Mathematics and Music
An Exploration of the Relationship between Mathematics and Music Shah, Saloni 2010 MIMS EPrint: 2010.103 Manchester Institute for Mathematical Sciences School of Mathematics The University of Manchester Reports available from: http://eprints.maths.manchester.ac.uk/ And by contacting: The MIMS Secretary School of Mathematics The University of Manchester Manchester, M13 9PL, UK ISSN 1749-9097 An Exploration of ! Relation"ip Between Ma#ematics and Music MATH30000, 3rd Year Project Saloni Shah, ID 7177223 University of Manchester May 2010 Project Supervisor: Professor Roger Plymen ! 1 TABLE OF CONTENTS Preface! 3 1.0 Music and Mathematics: An Introduction to their Relationship! 6 2.0 Historical Connections Between Mathematics and Music! 9 2.1 Music Theorists and Mathematicians: Are they one in the same?! 9 2.2 Why are mathematicians so fascinated by music theory?! 15 3.0 The Mathematics of Music! 19 3.1 Pythagoras and the Theory of Music Intervals! 19 3.2 The Move Away From Pythagorean Scales! 29 3.3 Rameau Adds to the Discovery of Pythagoras! 32 3.4 Music and Fibonacci! 36 3.5 Circle of Fifths! 42 4.0 Messiaen: The Mathematics of his Musical Language! 45 4.1 Modes of Limited Transposition! 51 4.2 Non-retrogradable Rhythms! 58 5.0 Religious Symbolism and Mathematics in Music! 64 5.1 Numbers are God"s Tools! 65 5.2 Religious Symbolism and Numbers in Bach"s Music! 67 5.3 Messiaen"s Use of Mathematical Ideas to Convey Religious Ones! 73 6.0 Musical Mathematics: The Artistic Aspect of Mathematics! 76 6.1 Mathematics as Art! 78 6.2 Mathematical Periods! 81 6.3 Mathematics Periods vs. -
Determinants
Determinants §1. Prerequisites 1) Every row operation can be achieved by pre-multiplying (left-multiplying) by an invertible matrix E called the elementary matrix for that operation. The matrix E is obtained by applying the ¡ row operation to the appropriate identity matrix. The matrix E is also denoted by Aij c ¡ , Mi c , or Pij, respectively, for the operations add c times row j to i operation, multiply row i by c, and permute rows i and j, respectively. 2) The Row Reduction Theorem asserts that every matrix A can be row reduced to a unique row echelon reduced matrix R. In matrix form: There is a unique row reduced matrix R and some 1 £ £ £ ¤ ¢ ¢ ¢ ¢ ¢ elementary Ei with Ep ¢ E1A R, or equivalently, A F1 FpR where Fi Ei are also elemen- tary. 3) A matrix A determines a linear transformation: It takes vectors x and gives vectors Ax. §2. Restrictions All matrices must be square. Determinants are not defined for non-square matrices. §3. Motivation Determinants determine whether a matrix has an inverse. They give areas and play a crucial role in the change of variables formula in multivariable calculus. ¡ ¥ ¡ Let’s compute the area of the parallelogram determined by vectors a ¥ b and c d . See Figure 1. c a (a+c, b+d) b b (c, d) c d d c (a, b) b b (0, 0) a c Figure 1. 1 1 ¡ ¦ ¡ § ¡ § ¡ § £ ¦ ¦ ¦ § § § £ § The area is a ¦ c b d 2 2ab 2 2cd 2bc ab ad cb cd ab cd 2bc ad bc. Tentative definition: The determinant of a 2 by 2 matrix is ¨ a b a b £ § det £ ad bc © c d c d which is the “signed” area of the parallelogram with sides determine by the rows of the matrix. -
18.703 Modern Algebra, Permutation Groups
5. Permutation groups Definition 5.1. Let S be a set. A permutation of S is simply a bijection f : S −! S. Lemma 5.2. Let S be a set. (1) Let f and g be two permutations of S. Then the composition of f and g is a permutation of S. (2) Let f be a permutation of S. Then the inverse of f is a permu tation of S. Proof. Well-known. D Lemma 5.3. Let S be a set. The set of all permutations, under the operation of composition of permutations, forms a group A(S). Proof. (5.2) implies that the set of permutations is closed under com position of functions. We check the three axioms for a group. We already proved that composition of functions is associative. Let i: S −! S be the identity function from S to S. Let f be a permutation of S. Clearly f ◦ i = i ◦ f = f. Thus i acts as an identity. Let f be a permutation of S. Then the inverse g of f is a permutation of S by (5.2) and f ◦ g = g ◦ f = i, by definition. Thus inverses exist and G is a group. D Lemma 5.4. Let S be a finite set with n elements. Then A(S) has n! elements. Proof. Well-known. D Definition 5.5. The group Sn is the set of permutations of the first n natural numbers. We want a convenient way to represent an element of Sn. The first way, is to write an element σ of Sn as a matrix. -
Permutation Group and Determinants (Dated: September 16, 2021)
Permutation group and determinants (Dated: September 16, 2021) 1 I. SYMMETRIES OF MANY-PARTICLE FUNCTIONS Since electrons are fermions, the electronic wave functions have to be antisymmetric. This chapter will show how to achieve this goal. The notion of antisymmetry is related to permutations of electrons’ coordinates. Therefore we will start with the discussion of the permutation group and then introduce the permutation-group-based definition of determinant, the zeroth-order approximation to the wave function in theory of many fermions. This definition, in contrast to that based on the Laplace expansion, relates clearly to properties of fermionic wave functions. The determinant gives an N-particle wave function built from a set of N one-particle waves functions and is called Slater’s determinant. II. PERMUTATION (SYMMETRIC) GROUP Definition of permutation group: The permutation group, known also under the name of symmetric group, is the group of all operations on a set of N distinct objects that order the objects in all possible ways. The group is denoted as SN (we will show that this is a group below). We will call these operations permutations and denote them by symbols σi. For a set consisting of numbers 1, 2, :::, N, the permutation σi orders these numbers in such a way that k is at jth position. Often a better way of looking at permutations is to say that permutations are all mappings of the set 1, 2, :::, N onto itself: σi(k) = j, where j has to go over all elements. Number of permutations: The number of permutations is N! Indeed, we can first place each object at positions 1, so there are N possible placements. -
2014 CBK Linear Algebra Honors.Pdf
PETERS TOWNSHIP SCHOOL DISTRICT CORE BODY OF KNOWLEDGE LINEAR ALGEBRA HONORS GRADE 12 For each of the sections that follow, students may be required to analyze, recall, explain, interpret, apply, or evaluate the particular concept being taught. Course Description This college level mathematics course will cover linear algebra and matrix theory emphasizing topics useful in other disciplines such as physics and engineering. Key topics include solving systems of equations, evaluating vector spaces, performing linear transformations and matrix representations. Linear Algebra Honors is designed for the extremely capable student who has completed one year of calculus. Systems of Linear Equations Categorize a linear equation in n variables Formulate a parametric representation of solution set Assess a system of linear equations to determine if it is consistent or inconsistent Apply concepts to use back-substitution and Guassian elimination to solve a system of linear equations Investigate the size of a matrix and write an augmented or coefficient matrix from a system of linear equations Apply concepts to use matrices and Guass-Jordan elimination to solve a system of linear equations Solve a homogenous system of linear equations Design, setup and solve a system of equations to fit a polynomial function to a set of data points Design, set up and solve a system of equations to represent a network Matrices Categorize matrices as equal Construct a sum matrix Construct a product matrix Assess two matrices as compatible Apply matrix multiplication -
Section 2.4–2.5 Partitioned Matrices and LU Factorization
Section 2.4{2.5 Partitioned Matrices and LU Factorization Gexin Yu [email protected] College of William and Mary Gexin Yu [email protected] Section 2.4{2.5 Partitioned Matrices and LU Factorization One approach to simplify the computation is to partition a matrix into blocks. 2 3 0 −1 5 9 −2 3 Ex: A = 4 −5 2 4 0 −3 1 5. −8 −6 3 1 7 −4 This partition can also be written as the following 2 × 3 block matrix: A A A A = 11 12 13 A21 A22 A23 3 0 −1 In the block form, we have blocks A = and so on. 11 −5 2 4 partition matrices into blocks In real world problems, systems can have huge numbers of equations and un-knowns. Standard computation techniques are inefficient in such cases, so we need to develop techniques which exploit the internal structure of the matrices. In most cases, the matrices of interest have lots of zeros. Gexin Yu [email protected] Section 2.4{2.5 Partitioned Matrices and LU Factorization 2 3 0 −1 5 9 −2 3 Ex: A = 4 −5 2 4 0 −3 1 5. −8 −6 3 1 7 −4 This partition can also be written as the following 2 × 3 block matrix: A A A A = 11 12 13 A21 A22 A23 3 0 −1 In the block form, we have blocks A = and so on. 11 −5 2 4 partition matrices into blocks In real world problems, systems can have huge numbers of equations and un-knowns. -
Linear Algebra and Matrix Theory
Linear Algebra and Matrix Theory Chapter 1 - Linear Systems, Matrices and Determinants This is a very brief outline of some basic definitions and theorems of linear algebra. We will assume that you know elementary facts such as how to add two matrices, how to multiply a matrix by a number, how to multiply two matrices, what an identity matrix is, and what a solution of a linear system of equations is. Hardly any of the theorems will be proved. More complete treatments may be found in the following references. 1. References (1) S. Friedberg, A. Insel and L. Spence, Linear Algebra, Prentice-Hall. (2) M. Golubitsky and M. Dellnitz, Linear Algebra and Differential Equa- tions Using Matlab, Brooks-Cole. (3) K. Hoffman and R. Kunze, Linear Algebra, Prentice-Hall. (4) P. Lancaster and M. Tismenetsky, The Theory of Matrices, Aca- demic Press. 1 2 2. Linear Systems of Equations and Gaussian Elimination The solutions, if any, of a linear system of equations (2.1) a11x1 + a12x2 + ··· + a1nxn = b1 a21x1 + a22x2 + ··· + a2nxn = b2 . am1x1 + am2x2 + ··· + amnxn = bm may be found by Gaussian elimination. The permitted steps are as follows. (1) Both sides of any equation may be multiplied by the same nonzero constant. (2) Any two equations may be interchanged. (3) Any multiple of one equation may be added to another equation. Instead of working with the symbols for the variables (the xi), it is eas- ier to place the coefficients (the aij) and the forcing terms (the bi) in a rectangular array called the augmented matrix of the system. a11 a12 . -
The Mathematics Major's Handbook
The Mathematics Major’s Handbook (updated Spring 2016) Mathematics Faculty and Their Areas of Expertise Jennifer Bowen Abstract Algebra, Nonassociative Rings and Algebras, Jordan Algebras James Hartman Linear Algebra, Magic Matrices, Involutions, (on leave) Statistics, Operator Theory Robert Kelvey Combinatorial and Geometric Group Theory Matthew Moynihan Abstract Algebra, Combinatorics, Permutation Enumeration R. Drew Pasteur Differential Equations, Mathematics in Biology/Medicine, Sports Data Analysis Pamela Pierce Real Analysis, Functions of Generalized Bounded Variation, Convergence of Fourier Series, Undergraduate Mathematics Education, Preparation of Pre-service Teachers John Ramsay Topology, Algebraic Topology, Operations Research OndˇrejZindulka Real Analysis, Fractal geometry, Geometric Measure Theory, Set Theory 1 2 Contents 1 Mission Statement and Learning Goals 5 1.1 Mathematics Department Mission Statement . 5 1.2 Learning Goals for the Mathematics Major . 5 2 Curriculum 8 3 Requirements for the Major 9 3.1 Recommended Timeline for the Mathematics Major . 10 3.2 Requirements for the Double Major . 10 3.3 Requirements for Teaching Licensure in Mathematics . 11 3.4 Requirements for the Minor . 11 4 Off-Campus Study in Mathematics 12 5 Senior Independent Study 13 5.1 Mathematics I.S. Student/Advisor Guidelines . 13 5.2 Project Topics . 13 5.3 Project Submissions . 14 5.3.1 Project Proposal . 14 5.3.2 Project Research . 14 5.3.3 Annotated Bibliography . 14 5.3.4 Thesis Outline . 15 5.3.5 Completed Chapters . 15 5.3.6 Digitial I.S. Document . 15 5.3.7 Poster . 15 5.3.8 Document Submission and oral presentation schedule . 15 6 Independent Study Assessment Guide 21 7 Further Learning Opportunities 23 7.1 At Wooster . -
Universal Invariant and Equivariant Graph Neural Networks
Universal Invariant and Equivariant Graph Neural Networks Nicolas Keriven Gabriel Peyré École Normale Supérieure CNRS and École Normale Supérieure Paris, France Paris, France [email protected] [email protected] Abstract Graph Neural Networks (GNN) come in many flavors, but should always be either invariant (permutation of the nodes of the input graph does not affect the output) or equivariant (permutation of the input permutes the output). In this paper, we consider a specific class of invariant and equivariant networks, for which we prove new universality theorems. More precisely, we consider networks with a single hidden layer, obtained by summing channels formed by applying an equivariant linear operator, a pointwise non-linearity, and either an invariant or equivariant linear output layer. Recently, Maron et al. (2019b) showed that by allowing higher- order tensorization inside the network, universal invariant GNNs can be obtained. As a first contribution, we propose an alternative proof of this result, which relies on the Stone-Weierstrass theorem for algebra of real-valued functions. Our main contribution is then an extension of this result to the equivariant case, which appears in many practical applications but has been less studied from a theoretical point of view. The proof relies on a new generalized Stone-Weierstrass theorem for algebra of equivariant functions, which is of independent interest. Additionally, unlike many previous works that consider a fixed number of nodes, our results show that a GNN defined by a single set of parameters can approximate uniformly well a function defined on graphs of varying size. 1 Introduction Designing Neural Networks (NN) to exhibit some invariance or equivariance to group operations is a central problem in machine learning (Shawe-Taylor, 1993). -
Laplace Expansion of the Determinant
Geometria Lingotto. LeLing12: More on determinants. Contents: ¯ • Laplace expansion of the determinant. • Cross product and generalisations. • Rank and determinant: minors. • The characteristic polynomial. Recommended exercises: Geoling 14. ¯ Laplace expansion of the determinant The expansion of Laplace allows to reduce the computation of an n × n determinant to that of n (n − 1) × (n − 1) determinants. The formula, expanded with respect to the ith row (where A = (aij)), is: i+1 i+n det(A) = (−1) ai1det(Ai1) + ··· + (−1) aindet(Ain) where Aij is the (n − 1) × (n − 1) matrix obtained by erasing the row i and the column j from A. With respect to the j th column it is: j+1 j+n det(A) = (−1) a1jdet(A1j) + ··· + (−1) anjdet(Anj) Example 0.1. We do it with respect to the first row below. 1 2 1 4 1 3 1 3 4 3 4 1 = 1 − 2 + 1 = (4 − 6) − 2(3 − 5) + (3:6 − 5:4) = 0 6 1 5 1 5 6 5 6 1 The proof of the expansion along the first row is as follows. The determinant's linearity, proved in the previous set of notes, implies 0 1 Ej n BA C X B 2C det(A) = a1j det B . C j=1 @ . A An Ingegneria dell'Autoveicolo, LeLing12 1 Geometria Geometria Lingotto. where Ej is the canonical basis of the rows, i.e. Ej is zero except at position j where there is 1. Thus we have to calculate the determinants 0 0 ··· 0 1 0 0 ··· 0 a a ··· a a a ······ a 21 22 2(j−1) 2j 2(j+1) 2n .