DOCSLIB.ORG

1.1. Laplacian Expansion, Cofactor, Adjugate, Inverse Matrix Formula. in This Section, We Generalize the Method That We Used To

Total Page：16

File Type：pdf, Size：1020Kb

Download full-text PDF Read full-text
1.1. Laplacian Expansion, Cofactor, Adjugate, Inverse Matrix Formula. in This Section, We Generalize the Method That We Used To 1. LAPLACIAN EXPANSION 1.1. Laplacian Expansion, Cofactor, Adjugate, Inverse Matrix Formula. In this section, We generalize the method that we used to compute the formula of 2 by 2 and 3 by 3 determinants to n by n matirx, the goal is not to write down the explicite formula, but to make use of it to analyses a method to find the inverse. Definition 1.1.1 The block diagonal matrix is the block matrix with the same partition on rows and columns, such that all non-zero blocks lies on the diagonal cells. Like: 0 1 A1 B .. C @ . A An The following could be viewed as block diagonal matrix with approperate partition 0 1 1 0 1 1 @ 2 5 A = @ 2 5 A 6 7 6 7 The above matrix could be seen as a block diagonal matrix with partition (1; 2) 0 2 3 1 0 2 3 1 B 4 6 C B 4 6 C B C B C B 2 4 7 C B 2 4 7 C B C = B C B 1 2 0 C B 1 2 0 C B C B C @ 3 5 6 A @ 3 5 6 A 6 6 The above matrix could be seen as block diagonal matrix with partition (1; 3; 2) 0 1 3 1 B 2 4 C B C B 5 6 C B C @ 5 A 7 The above matrix is not a block diagonal matrix, as the partition on its columns and rows are not the same Proposition 1.1 The determinant of block diagonal matrix is the product of the determinant of all diagonal blocks. 1 Compute the following determinant: 1 2 3 2 2 3 1 5 Answer: The determinant is just the product of the determinant of diagonal matrices. That is 1 2 3 2 2 3 1 5 1 2 2 3 = 3 2 1 5 = (−4) × 7 = −28 Definition 1.1.2 The block upper triangular matrix is the block matrix with the same partition on rows and columns, such that all non-zero blocks lies on or above the diagonal cells. Like: 0 1 A11 ··· A1n B .. C @ . A Ann Definition 1.1.3 The block lower triangular matrix is the block matrix with the same partition on rows and columns, such that all non-zero blocks lies on or below the diagonal cells. Like: 0 1 A11 B . .. C @ . A An1 ··· An Proposition 1.2 The determinant of block upper triangular matrix or block lower triangular matrix is the product of determinant of blocks of diagonals. 2 Definition 1.1.4 Let M be a n × n square matrix over F , and 1 ≤ i ≤ n, 1 ≤ j ≤ n, then the cofactor of M at i,j is defined to be the determinant of (n − 1) × (n − 1) matrix which is obtained by deleting the ith row and jth column. If we multiply this determinant by (−1)i+j, then the value is called the algebraic cofactor, denoted by Mij, where the M is the notation for original matrix. 0 1 2 2 1 Let M=@ 8 2 8 A, What is M12? −1 2 0 Answer: M12 is got by computing the determinant of cancelling the 1st row and 2nd column, and times (−1)i+j i.e. 1+2 8 8 M12 = (−1) = −8 −1 0 Now we trying to use our method to find the determinant for n × n matirx inductively, and look what we could find. Trying to simplify the determinant of 5×5 matrix into the computation of determinant 4×4 matrix 1 2 2 1 1 2 4 5 4 4 4 6 7 8 6 5 7 1 1 2 6 1 0 0 7 We use our standard method: 3 1 2 2 1 1 2 4 5 4 4 4 6 7 8 6 5 7 1 1 2 6 1 0 0 7 1 2 2 2 4 5 4 4 2 4 5 4 4 2 4 5 4 4 = 4 6 7 8 6 + 4 6 7 8 6 + 4 6 7 8 6 5 7 1 1 2 5 7 1 1 2 5 7 1 1 2 6 1 0 0 7 6 1 0 0 7 6 1 0 0 7 1 1 2 4 5 4 4 2 4 5 4 4 + 4 6 7 8 6 + 4 6 7 8 6 5 7 1 1 2 5 7 1 1 2 6 1 0 0 7 6 1 0 0 7 1 2 2 2 4 5 4 4 4 2 5 4 4 5 2 4 4 4 = 4 6 7 8 6 − 6 4 7 8 6 + 7 4 6 8 6 5 7 1 1 2 7 5 1 1 2 1 5 7 1 2 6 1 0 0 7 1 6 0 0 7 0 6 1 0 7 1 1 4 2 4 5 4 4 2 4 5 4 − 8 4 6 7 6 + 6 4 6 7 8 1 5 7 1 2 2 5 7 1 1 0 6 1 0 7 7 6 1 0 0 4 5 4 4 2 5 4 4 2 4 4 4 6 7 8 6 4 7 8 6 4 6 8 6 = 1 × − 2 × + 2 × 7 1 1 2 5 1 1 2 5 7 1 2 1 0 0 7 6 0 0 7 6 1 0 7 2 4 5 4 2 4 5 4 4 6 7 6 4 6 7 8 −1 × + 1 × 5 7 1 2 5 7 1 1 6 1 0 7 6 1 0 0 As you can see, in the expansion, we expanded out the all the entry of the first row, and left with the determinant of numbers that in the different row and column with the entry, with the sign alternating, that exactly the first row times the cofactor corresponds to first row. To conclude, we now have the Laplacian Expansion: 4 Definition 1.1.5 Suppose A is a square matrix, then we can expand A by any row or any column. namely Row expansion: det(A) = ai1Ai1 + ai2Ai2 + ··· + ainAin Column expansion: det(A) = a1iA1i + a2iA2i + ··· + aniAni (Please keep in mind to change the sign, as the term appeared on the formula means algebraic cofac- tors) Expand the following matrix by the second row 6 8 9 2 4 1 1 2 5 8 9 6 9 6 8 = −2 × + 4 × − 1 × 2 5 1 5 1 2 Expand the following matrix by the second column 6 8 9 2 4 1 1 2 5 6 9 2 1 2 6 = −4 × + 8 × − 2 × 1 5 1 5 1 9 As you can see, the method we used above can inductively give the formula, but what is more than that is the following observation: What if I change the coefficient of each corfactor by the entry of other row? Then in the previous example it would be the laplacian expansion of the determinant: In the expansion of 6 8 9 2 4 1 1 2 5 8 9 6 9 6 8 = −2 × + 4 × − 1 × 2 5 1 5 1 2 Now if we change the coefficient by the corresponding entries of other lines, that is 5 8 9 6 9 6 8 −1 × + 2 × − 5 × 2 5 1 5 1 2 What the value would be? as you can see, the line that we expanded only determined the coefficient in front of each algebraic cofacter, not appear in any of the cofacter . if we change the coefficient, the only change is the line that we expand by. 6 8 9 8 9 6 9 6 8 −1 × + 2 × − 5 × = −1 −2 −5 = 0 2 5 1 5 1 2 1 2 5 we get the last equation because the second row is scalar multiple of the third row Proposition 1.3 The othogonal property of cofactor: let A = mataijnn be a matirx, r = 0 1 k Al1 B Al2 C a a ··· a cl = B C k1 k2 kn be any row of A, and B . C be the cofactor of some row. then @ . A Aln l rkc = 0 if k 6= l l rkc = detA if k = l At this point, we can make the propersition: Now we construct a matrix, namely, Adjugate Matrix of A, it is constructed by putting Aij in the j’th row and i’th column(remember the order). Then with the adjugate matrix, we have the following property: Proposition 1.4 ∗ ∗ let A = (aij)1≤i≤n be a matirx, we define A = (Aji)1≤j≤n to be the adjunct matrix, then A A = 1≤j≤n 1≤i≤n det(A)In Then if the determinant is not 0, simply divide the adjugate matrix by determinant, we can get the inverse Proposition 1.5 ∗ let A = (aij)1≤i≤n be a matirx, we define A = (Aji)1≤j≤n to be the adjunct matrix, then 1≤j≤n 1≤i≤n −1 A = (Aji)1≤j≤n 1≤i≤n 0 2 4 6 1 Find the inverse of @ 1 3 4 A 6 7 2 Answer: 6 0 2 4 6 1 @ 1 3 4 A 6 7 2 0 1 3 4 4 6 4 6 − B 7 2 7 2 3 4 C B C 1 B 1 4 2 6 2 6 C = B − − C 6 2 6 2 1 4 2 4 6 B C B C 1 3 4 1 3 2 4 2 4 @ A − 6 7 2 6 7 6 7 1 3 0 −22 34 −2 1 1 = − 64 @ 22 −32 −2 A −11 10 2 7.
Load more

Recommended publications
  • Linear Algebra: Example Sheet 2 of 4
    Michaelmas Term 2014 SJW Linear Algebra: Example Sheet 2 of 4 1. (Another proof of the row rank column rank equality.) Let A be an m × n matrix of (column) rank r. Show that r is the least integer for which A factorises as A = BC with B 2 Matm;r(F) and C 2 Matr;n(F). Using the fact that (BC)T = CT BT , deduce that the (column) rank of AT equals r. 2. Write down the three types of elementary matrices and find their inverses. Show that an n × n matrix A is invertible if and only if it can be written as a product of elementary matrices. Use this method to find the inverse of 0 1 −1 0 1 @ 0 0 1 A : 0 3 −1 3. Let A and B be n × n matrices over a field F . Show that the 2n × 2n matrix IB IB C = can be transformed into D = −A 0 0 AB by elementary row operations (which you should specify). By considering the determinants of C and D, obtain another proof that det AB = det A det B. 4. (i) Let V be a non-trivial real vector space of finite dimension. Show that there are no endomorphisms α; β of V with αβ − βα = idV . (ii) Let V be the space of infinitely differentiable functions R ! R. Find endomorphisms α; β of V which do satisfy αβ − βα = idV . 5. Find the eigenvalues and give bases for the eigenspaces of the following complex matrices: 0 1 1 0 1 0 1 1 −1 1 0 1 1 −1 1 @ 0 3 −2 A ; @ 0 3 −2 A ; @ −1 3 −1 A : 0 1 0 0 1 0 −1 1 1 The second and third matrices commute; find a basis with respect to which they are both diagonal.
    [Show full text]
  • 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
    [Show full text]
  • A New Algorithm to Obtain the Adjugate Matrix Using CUBLAS on GPU González, H.E., Carmona, L., J.J
    ISSN: 2277-3754 ISO 9001:2008 Certified International Journal of Engineering and Innovative Technology (IJEIT) Volume 7, Issue 4, October 2017 A New Algorithm to Obtain the Adjugate Matrix using CUBLAS on GPU González, H.E., Carmona, L., J.J. Information Technology Department, ININ-ITTLA Information Technology Department, ININ proved to be the best option for most practical applications. Abstract— In this paper a parallel code for obtain the Adjugate The new transformation proposed here can be obtained from Matrix with real coefficients are used. We postulate a new linear it. Next, we briefly review this topic. transformation in matrix product form and we apply this linear transformation to an augmented matrix (A|I) by means of both a minimum and a complete pivoting strategies, then we obtain the II. LU-MATRICIAL DECOMPOSITION WITH GT. Adjugate matrix. Furthermore, if we apply this new linear NOTATION AND DEFINITIONS transformation and the above pivot strategy to a augmented The problem of solving a linear system of equations matrix (A|b), we obtain a Cramer’s solution of the linear system of Ax b is central to the field of matrix computation. There are equations. That new algorithm present an O n3 computational several ways to perform the elimination process necessary for complexity when n . We use subroutines of CUBLAS 2nd A, b R its matrix triangulation. We will focus on the Doolittle-Gauss rd and 3 levels in double precision and we obtain correct numeric elimination method: the algorithm of choice when A is square, results. dense, and un-structured. nxn Index Terms—Adjoint matrix, Adjugate matrix, Cramer’s Let us assume that AR is nonsingular and that we rule, CUBLAS, GPU.
    [Show full text]
  • Field of U-Invariants of Adjoint Representation of the Group GL (N, K)
    Field of U-invariants of adjoint representation of the group GL(n,K) K.A.Vyatkina A.N.Panov ∗ It is known that the field of invariants of an arbitrary unitriangular group is rational (see [1]). In this paper for adjoint representation of the group GL(n,K) we present the algebraically system of generators of the field of U-invariants. Note that the algorithm for calculating generators of the field of invariants of an arbitrary rational representation of an unipotent group was presented in [2, Chapter 1]. The invariants was constructed using induction on the length of Jordan-H¨older series. In our case the length is equal to n2; that is why it is difficult to apply the algorithm. −1 Let us consider the adjoint representation AdgA = gAg of the group GL(n,K), where K is a field of zero characteristic, on the algebra of matri- ces M = Mat(n,K). The adjoint representation determines the representation −1 ρg on K[M] (resp. K(M)) by formula ρgf(A)= f(g Ag). Let U be the subgroup of upper triangular matrices in GL(n,K) with units on the diagonal. A polynomial (rational function) f on M is called an U- invariant, if ρuf = f for every u ∈ U. The set of U-invariant rational functions K(M)U is a subfield of K(M). Let {xi,j} be a system of standard coordinate functions on M. Construct a X X∗ ∗ X X∗ X∗ X matrix = (xij). Let = (xij) be its adjugate matrix, · = · = det X · E. Denote by Jk the left lower corner minor of order k of the matrix X.
    [Show full text]
  • Formalizing the Matrix Inversion Based on the Adjugate Matrix in HOL4 Liming Li, Zhiping Shi, Yong Guan, Jie Zhang, Hongxing Wei
    Formalizing the Matrix Inversion Based on the Adjugate Matrix in HOL4 Liming Li, Zhiping Shi, Yong Guan, Jie Zhang, Hongxing Wei To cite this version: Liming Li, Zhiping Shi, Yong Guan, Jie Zhang, Hongxing Wei. Formalizing the Matrix Inversion Based on the Adjugate Matrix in HOL4. 8th International Conference on Intelligent Information Processing (IIP), Oct 2014, Hangzhou, China. pp.178-186, 10.1007/978-3-662-44980-6_20. hal-01383331 HAL Id: hal-01383331 https://hal.inria.fr/hal-01383331 Submitted on 18 Oct 2016 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Distributed under a Creative Commons Attribution| 4.0 International License Formalizing the Matrix Inversion Based on the Adjugate Matrix in HOL4 Liming LI1, Zhiping SHI1?, Yong GUAN1, Jie ZHANG2, and Hongxing WEI3 1 Beijing Key Laboratory of Electronic System Reliability Technology, Capital Normal University, Beijing 100048, China [email protected], [email protected] 2 College of Information Science & Technology, Beijing University of Chemical Technology, Beijing 100029, China 3 School of Mechanical Engineering and Automation, Beihang University, Beijing 100083, China Abstract. This paper presents the formalization of the matrix inversion based on the adjugate matrix in the HOL4 system.
    [Show full text]
  • Linearized Polynomials Over Finite Fields Revisited
    Linearized polynomials over finite fields revisited∗ Baofeng Wu,† Zhuojun Liu‡ Abstract We give new characterizations of the algebra Ln(Fqn ) formed by all linearized polynomials over the finite field Fqn after briefly sur- veying some known ones. One isomorphism we construct is between ∨ L F n F F n n( q ) and the composition algebra qn ⊗Fq q . The other iso- morphism we construct is between Ln(Fqn ) and the so-called Dickson matrix algebra Dn(Fqn ). We also further study the relations between a linearized polynomial and its associated Dickson matrix, generalizing a well-known criterion of Dickson on linearized permutation polyno- mials. Adjugate polynomial of a linearized polynomial is then intro- duced, and connections between them are discussed. Both of the new characterizations can bring us more simple approaches to establish a special form of representations of linearized polynomials proposed re- cently by several authors. Structure of the subalgebra Ln(Fqm ) which are formed by all linearized polynomials over a subfield Fqm of Fqn where m|n are also described. Keywords Linearized polynomial; Composition algebra; Dickson arXiv:1211.5475v2 [math.RA] 1 Jan 2013 matrix algebra; Representation. ∗Partially supported by National Basic Research Program of China (2011CB302400). †Key Laboratory of Mathematics Mechanization, AMSS, Chinese Academy of Sciences, Beijing 100190, China. Email: [email protected] ‡Key Laboratory of Mathematics Mechanization, AMSS, Chinese Academy of Sciences, Beijing 100190, China. Email: [email protected] 1 1 Introduction n Let Fq and Fqn be the finite fields with q and q elements respectively, where q is a prime or a prime power.
    [Show full text]
  • Arxiv:2012.03523V3 [Math.NT] 16 May 2021 Favne Cetfi Optn Eerh(SR Spr Ft of Part (CM4)
    WRONSKIAN´ ALGEBRA AND BROADHURST–ROBERTS QUADRATIC RELATIONS YAJUN ZHOU To the memory of Dr. W (1986–2020) ABSTRACT. Throughalgebraicmanipulationson Wronskian´ matrices whose entries are reducible to Bessel moments, we present a new analytic proof of the quadratic relations conjectured by Broadhurst and Roberts, along with some generalizations. In the Wronskian´ framework, we reinterpret the de Rham intersection pairing through polynomial coefficients in Vanhove’s differential operators, and compute the Betti inter- section pairing via linear sum rules for on-shell and off-shell Feynman diagrams at threshold momenta. From the ideal generated by Broadhurst–Roberts quadratic relations, we derive new non-linear sum rules for on-shell Feynman diagrams, including an infinite family of determinant identities that are compatible with Deligne’s conjectures for critical values of motivic L-functions. CONTENTS 1. Introduction 1 2. W algebra 5 2.1. Wronskian´ matrices and Vanhove operators 5 2.2. Block diagonalization of on-shell Wronskian´ matrices 8 2.3. Sumrulesforon-shellandoff-shellBesselmoments 11 3. W⋆ algebra 20 3.1. Cofactors of Wronskians´ 21 3.2. Threshold behavior of Wronskian´ cofactors 24 3.3. Quadratic relations for off-shell Bessel moments 30 4. Broadhurst–Roberts quadratic relations 37 4.1. Quadratic relations for on-shell Bessel moments 37 4.2. Arithmetic applications to Feynman diagrams 43 4.3. Alternative representations of de Rham matrices 49 References 53 arXiv:2012.03523v3 [math.NT] 16 May 2021 Date: May 18, 2021. Keywords: Bessel moments, Feynman integrals, Wronskian´ matrices, Bernoulli numbers Subject Classification (AMS 2020): 11B68, 33C10, 34M35 (Primary) 81T18, 81T40 (Secondary) * This research was supported in part by the Applied Mathematics Program within the Department of Energy (DOE) Office of Advanced Scientific Computing Research (ASCR) as part of the Collaboratory on Mathematics for Mesoscopic Modeling of Materials (CM4).
    [Show full text]
  • Lecture 5: Matrix Operations: Inverse
    Lecture 5: Matrix Operations: Inverse • Inverse of a matrix • Computation of inverse using co-factor matrix • Properties of the inverse of a matrix • Inverse of special matrices • Unit Matrix • Diagonal Matrix • Orthogonal Matrix • Lower/Upper Triangular Matrices 1 Matrix Inverse • Inverse of a matrix can only be defined for square matrices. • Inverse of a square matrix exists only if the determinant of that matrix is non-zero. • Inverse matrix of 퐴 is noted as 퐴−1. • 퐴퐴−1 = 퐴−1퐴 = 퐼 • Example: 2 −1 0 1 • 퐴 = , 퐴−1 = , 1 0 −1 2 2 −1 0 1 0 1 2 −1 1 0 • 퐴퐴−1 = = 퐴−1퐴 = = 1 0 −1 2 −1 2 1 0 0 1 2 Inverse of a 3 x 3 matrix (using cofactor matrix) • Calculating the inverse of a 3 × 3 matrix is: • Compute the matrix of minors for A. • Compute the cofactor matrix by alternating + and – signs. • Compute the adjugate matrix by taking a transpose of cofactor matrix. • Divide all elements in the adjugate matrix by determinant of matrix 퐴. 1 퐴−1 = 푎푑푗(퐴) det(퐴) 3 Inverse of a 3 x 3 matrix (using cofactor matrix) 3 0 2 퐴 = 2 0 −2 0 1 1 0 −2 2 −2 2 0 1 1 0 1 0 1 2 2 2 0 2 3 2 3 0 Matrix of Minors = = −2 3 3 1 1 0 1 0 1 0 2 3 2 3 0 0 −10 0 0 −2 2 −2 2 0 2 2 2 1 −1 1 2 −2 2 Cofactor of A (퐂) = −2 3 3 .∗ −1 1 −1 = 2 3 −3 0 −10 0 1 −1 1 0 10 0 2 2 0 adj A = CT = −2 3 10 2 −3 0 2 2 0 0.2 0.2 0 1 1 A-1 = ∗ adj A = −2 3 10 = −0.2 0.3 1 |퐴| 10 2 −3 0 0.2 −0.3 0 4 Properties of Inverse of a Matrix • (A-1)-1 = A • (AB)-1 = B-1A-1 • (kA)-1 = k-1A-1 where k is a non-zero scalar.
    [Show full text]
  • Contents 2 Matrices and Systems of Linear Equations
    Business Math II (part 2) : Matrices and Systems of Linear Equations (by Evan Dummit, 2019, v. 1.00) Contents 2 Matrices and Systems of Linear Equations 1 2.1 Systems of Linear Equations . 1 2.1.1 Elimination, Matrix Formulation . 2 2.1.2 Row-Echelon Form and Reduced Row-Echelon Form . 4 2.1.3 Gaussian Elimination . 6 2.2 Matrix Operations: Addition and Multiplication . 8 2.3 Determinants and Inverses . 11 2.3.1 The Inverse of a Matrix . 11 2.3.2 The Determinant of a Matrix . 13 2.3.3 Cofactor Expansions and the Adjugate . 16 2.3.4 Matrices and Systems of Linear Equations, Revisited . 18 2 Matrices and Systems of Linear Equations In this chapter, we will discuss the problem of solving systems of linear equations, reformulate the problem using matrices, and then give the general procedure for solving such systems. We will then study basic matrix operations (addition and multiplication) and discuss the inverse of a matrix and how it relates to another quantity known as the determinant. We will then revisit systems of linear equations after reformulating them in the language of matrices. 2.1 Systems of Linear Equations • Our motivating problem is to study the solutions to a system of linear equations, such as the system x + 3x = 5 1 2 : 3x1 + x2 = −1 ◦ Recall that a linear equation is an equation of the form a1x1 + a2x2 + ··· + anxn = b, for some constants a1; : : : an; b, and variables x1; : : : ; xn. ◦ When we seek to nd the solutions to a system of linear equations, this means nding all possible values of the variables such that all equations are satised simultaneously.
    [Show full text]
  • Lecture No. 6
    Preliminaries: linear algebra State-space models System interconnections Control Theory (035188) lecture no. 6 Leonid Mirkin Faculty of Mechanical Engineering Technion | IIT Preliminaries: linear algebra State-space models System interconnections Outline Preliminaries: linear algebra State-space models System interconnections in terms of state-space realizations Preliminaries: linear algebra State-space models System interconnections Outline Preliminaries: linear algebra State-space models System interconnections in terms of state-space realizations Preliminaries: linear algebra State-space models System interconnections Linear algebra, notation and terminology A matrix A Rn×m is an n m table of real numbers, 2 × 2 3 a a a m 11 12 ··· 1 6 a21 a22 a1m 7 A = 6 . ··· . 7 = [aij ]; 4 . 5 · an an anm 1 2 ··· accompanied by their manipulation rules (addition, multiplication, etc). The number of linearly independent rows (or columns) in A is called its rank and denoted rank A. A matrix A Rn×m is said to 2 have full row (column) rank if rank A = n (rank A = m) − be square if n = m, tall if n > m, and fat if n < m − be diagonal (A = diag ai ) if it is square and aij = 0 whenever i = j − f g 6 be lower (upper) triangular if aij = 0 whenever i > j (i < j) − 0 0 be symmetric if A = A , where the transpose A = [aji ] − · The identity matrix I = diag 1 Rn×n (if the dimension is clear, just I ). n · It is a convention that ·A0 = I fforg every2 nonzero square A. Preliminaries: linear algebra State-space models System interconnections Block matrices n×m P P Let A R and let i=1 ni = n and i=1 mi = n for some ni ; mi N.
    [Show full text]
  • 1111: Linear Algebra I
    1111: Linear Algebra I Dr. Vladimir Dotsenko (Vlad) Michaelmas Term 2015 Dr. Vladimir Dotsenko (Vlad) 1111: Linear Algebra I Michaelmas Term 2015 1 / 10 Row expansion of the determinant Our next goal is to prove the following formula: i1 i2 in det(A) = ai1C + ai2C + ··· + ainC ; in other words, if we multiply each element of the i-th row of A by its cofactor and add results, the number we obtain is equal to det(A). Let us first handle the case i = 1. In this case, once we write the corresponding minors with signs, the formula reads 11 12 n+1 1n det(A) = a11A - a12A + ··· + (-1) a1nA : Let us examine the formula for det(A). It is a sum of terms corresponding to pick n elements representing each row and each column of A. In particular, it involves picking an element from the first row. This can be one of the elements a11; a12;:::; a1n. What remains, after we picked the element a1k , is to pick other elements; now we have to avoid the row 1 and the column k. This means that the elements we need to pick are precisely those involved in the determinant A1k , and we just need to check that the signs match. Dr. Vladimir Dotsenko (Vlad) 1111: Linear Algebra I Michaelmas Term 2015 2 / 10 Row expansion of the determinant 1 In fact, it is quite easy to keep track of all signs. The column in the k two-row notation does not add inversions in the first row, and adds k - 1 inversions in the second row, since k appears before 1; 2;:::; k - 1.
    [Show full text]
  • Arxiv:1912.06967V1 [Math.RA] 15 Dec 2019 Values Faui Eigenvector Unit a of Ler Teacher
    MORE ON THE EIGENVECTORS-FROM-EIGENVALUES IDENTITY MALGORZATA STAWISKA Abstract. Using the notion of a higher adjugate of a matrix, we generalize the eigenvector-eigenvalue formula surveyed in [4] to arbitrary square matrices over C and their possibly multiple eigenvalues. 2010 Mathematics Subject Classification. 15A15, 15A24, 15A75 Keywords: Matrices, characteristic polynomial, eigenvalues, eigenvec- tors, adjugates. Dedication: To the memory of Witold Kleiner (1929-2018), my linear algebra teacher. 1. Introduction Very recently the following relation between eigenvectors and eigen- values of a Hermitian matrix (called “the eigenvector-eigenvalue iden- tity”) gained attention: Theorem 1.1. ([4]) If A is an n × n Hermitian matrix with eigen- values λ1(A), ..., λn(A) and i, j = 1, ..., n, then the jth component vi,j of a unit eigenvector vi associated to the eigenvalue λi(A) is related to the eigenvalues λ1(Mj), ..., λn−1(Mj) of the minor Mj of A formed by removing the jth row and column by the formula n n−1 2 |vi,j| Y (λi(A) − λk(A)) = Y(λi(A) − λk(Mj)). arXiv:1912.06967v1 [math.RA] 15 Dec 2019 k=1;k=6 i k=1 The survey paper ([4]) presents several proofs and some generaliza- tions of this identity, along with its many variants encountered in the modern literature, while also commenting on some sociology-of-science aspects of its jump in popularity. It should be pointed out that for sym- metric matrices over R this formula was established already in 1834 by Carl Gustav Jacob Jacobi as formula 30 in his paper [9] (in the process of proving that every real quadratic form has an orthogonal diagonal- ization).
    [Show full text]