Product Cosines of Angles between Subspaces

Size: px
Start display at page:

Download "Product Cosines of Angles between Subspaces"

Transcription

1 Product Cosines of Anges between Subspaces Jianming Miao and Adi Ben-Israe Juy, 993 Dedicated to Professor C.R. Rao on his 75th birthday Let Abstract cos{l,m} : i cos θ i, denote the product of the cosines of the principa anges {θ i } between the subspaces L and M. The n direction cosines of an r-dimensiona subspace L are the numbers {cos{l,ir n r J} : J Q r,n } where Q r,n : the set of increasing sequences of r eements from {,...,n}, and IR n J : {x x k IR n : x k 0 for k J}. The basic decomposition of a inear operator A : IR n IR m, with ranka r > 0, is A cos {RA,IR m I } cos {RA T,IR n J}B IJ, I IA J J A a convex combination of nonsinguar inear operators B IJ : IR n J IR n I. Here IA : {I Q r,m : ranka I r}, and J A : {J Q r,n : ranka J r}. The product cosines are reated to the matrix voume, defined as the product of its nonzero singuar vaues. The Moore-Penrose inverse A is characterized as having the minima voume among a {,}- inverses of A. Indeed, if G is a {,}-inverse of A, with range RG T and nu-space NG S then vo A vo G cos{t,ra T } cos{s,na T }. Key words: Principa anges. Singuar vaues. Voume. Generaized Inverses. RUTCOR-Rutgers Center for Operations Research, Rutgers University, P.O. Box 506, New Brunswick, NJ

2 Introduction. Notation We use the notation and terminoogy of [] and [5]. In particuar:..a The voume of A IR m n r is voa : where σ i are the nonzero singuar vaues of A. 0, if r 0, r σ i, if r > 0, i..b Let L, M be subspaces in IR n, and dim L dim M m. Then the principa anges between L and M, 0 θ θ θ π.. are defined by cos θ i : <x i, y i > x i y i max { <x, y> x y : x L, x x k, y M, y y k,, k,...,i },.3 where are the corresponding pairs of principa vectors...c x i, y i L M, i,...,,.4 The product of principa sines, and the product of principa cosines, are denoted by sin{l, M} : sinθ sin θ,.5 cos{l, M} : cos θ cos θ..6 Note that.5 and.6 are just notation, and not ordinary trigonometrica functions. In particuar, sin {L, M} + cos {L, M}...D Let Q r,n denote the set of increasing sequences of r eements from {,...,n}. For A IR m n r we denote by IA : {I Q r,m : ranka I r},.7..e J A : {J Q r,n : ranka J r}..8 The basic subspaces of dimension r of IR n n are the subspaces r which, for r, reduce to the n coordinate ines. Resuts IR n J : {x x k IR n : x k 0 if k J}, J Q r,n,.9 IR n {j} : {x x k IR n : x k 0 if k j}, j,...,n..0 This paper studies reations between the voume function, principa anges and generaized inverses. In we study the direction cosines cos {L,IR n J } of a subspace L. The basic decomposition of inear operators IR n IR m is given in 3. In 4 we prove reated extrema properties of the Moore Penrose. The Moore Penrose inverse A is of minima voume among the {, }-inverses of A.

3 Direction cosines Let L be a ine in IR n passing through the origin, spanned by the vector j. The direction cosines of L are the n cosines {cos {L,IR n {j}} : j,...,n}. of the non-obtuse anges between L and the n coordinate axes. The direction cosines are the modui of the cosines of the anges between and the unit vectors {e j : j,...,n} and satisfy cos {L,IR n {j} } cos {, e j },. n cos {L,IR n {j} }..3 j For any ine M through the origin, spanned by the vector m m j, n cos {L, M} cos {,m} cos {, e j } cos {m, e j } j n cos {,e j } cos {m, e j }.4 j n j cos{l,ir n {j} } cos{m, IRn {j} }, with equaity in.4 if and ony if cos {, e j } and cos {m,e j } have the same signs for a j, or equivaenty, sign j sign m j, j,...,n..5 The anaogous resuts for genera subspaces of IR n are given beow. First the anaog of the identity.3. Theorem Let L be a subspace of IR n, diml > 0 and et r {,...,n}. Then r n r cos {L,IR n J}, if r n n r n n r, if r < n.6 Proof: Let r. For any J {j,,j r } Q r,n, et P : e j,,e jr IR n r denote the matrix with coumns e j, j J. Let the coumns of Q IR n form an orthonorma basis for L. Then cos {L,IR n J} σi P T Q, by [5, Lemma ] i detq T J Q J detq T K Q K, K Q,n K J

4 where σ i P T Q are singuar vaues of P T Q. Therefore cos {L,IR n J} K Q,n K J r n r n r n r detq T K Q K, K Q,n detq T K Q K, n detq T Q, r n r n,.7 where the second equaity foows that for each term detq T K Q K, K Q,n, it appears in the summation r n r exacty n times. The resut for r < is obtained from.7 using the fact that the nonzero principa anges between L and M are the same as the nonzero principa anges between L and M, [5, Theorem 3]. Therefore if r <, We see from.6 that cos {L,IR n J} J Q n r,n cos {L, IR n J} n r n n n r n. n cos {L,IR n J}.8 ony if r diml or r n. The specia case r diml gives the identity.3. The foowing theorem gives the anaog of inequaity.4 for equi-dimensiona subspaces. Theorem If L and M are subspaces of IR n of dimension r, then cos {L, M} cos{l,ir n J} cos{m, IR n J}..9 Proof: Let the coumns of E and F be orthonorma bases for L and M respectivey. Then cos {L, M} dete T F, by [5, Theorem 5], det EJ F T J, dete J detf J, cos{l,ir n J} cos{m, IR n J}, by [5, Coroary ]..0 3

5 The proof shows that equaity hods in.9 if and ony if sign det E J sign det F J, J Q r,n,. or equivaenty, corresponding Pücker coordinates of L and M have the same signs. 3 The basic decomposition of inear operators A inear operator A : IR n IR m of ranka r > 0 can be written as a convex combination A I IA J J A det A IJ vo A A JI 3. where A JI is an m n matrix with the inverse of the J, Ith submatrix of A in position I, J and zeros esewhere, see [, Theorem 6.]. Each A JI is a one-to-one mapping of IRn J onto IRn I. The operator A of rank r is therefore a convex combination of nonsinguar operators between basic subspaces of dimension r. The representation 3. is caed a basic decomposition of A. We interpret the convex weights det A IJ /vo A of 3. in terms of direction cosines as foows. Theorem 3 If A is a inear operator : IR n IR m of ranka r > 0, then there exist inear operators {B IJ : I IA, J J A} such that B IJ : IR n J IR m I is one-to-one and onto, NB IJ IR n J, and A I IA J J A cos {RA, IR m I } cos {RA T, IR n J} B IJ. 3. Proof: Let A CR 3.3 be a fu rank factorization of A, and appy 3. to C and R separatey, to get A I IC det C I vo C C I J J R det R J vo R R J 3.4 We reca cos{ra, IR m I } deta IJ voa J, 3.5 for any J J A, see [5, Coroary ]. Then 3. foows from 3.4 and 3.5 since IA IC, RA RC, J A J R, RA T RR T and A R C. It foows from [] that the basic decomposition of A has the same convex weights as 3., A I IA J J A cos {RA, IR m I } cos {RA T, IR n J} Â IJ, 3.6 here A IJ is the I, J th submatrix of A, and denote padding with zeros. 4

6 R n R m T RA R n J A B IJ R m I RA Figure : A inear operator A : IR n IR m and one of the basic operators B IJ The foowing exampe shows that the basic decomposition 3. of A may not be unique even if we fix the convex weights. 0 Exampe Let A. The basic decomposition of A is given by 3. as 0 A with basic operators B {,},{,} 5 0 0, B {,},{,3} 0 0, B {,},{,3} However A can aso be expressed as A with the same convex weights, but different basic operators. Note that the above two expressions aso have the same corresponding minors det det det det det det 3. 4 Extrema voumes of {, }-inverses Let A be a inear operator : IR n IR m of rank r, range RA and nu space NA. The {, }-inverses of A are the operators G : IR m IR n satisfying AGA A and GAG G. 4. The set of a {, }-inverses of A is denoted by A{, }. For any two subspaces S and T such that IR n NA T, IR m RA S 4. 5

7 R n NA R m T NA T RA T G A RA S Figure : A {, }-inverse G of A with range T and nu-space S there is a unique {, }-inverse G of A, with RG T, NG S, 4.3 see Figure. In particuar, if S NA T and T RA T then G is the Moore-Penrose inverse A. The voume of A is vo A vo A. 4.4 Theorem 4 Let G be a {, }-inverse of A with range RG T and nu space NG S. Then vog Proof: The rank of G is r, since G A{, }. Let G EPF, voa cos{t, RA T } cos{s, NA T }. 4.5 E, F T IR n r r, P IR r r r, 4.6 be a fu rank factorization of G, where E, F T have orthonorma coumns. Then It foows from 4. that Therefore RG RE T, NG NF S. 4.7 PFCRE I r. 4.8 P RE FC, 4.9 and vog vo Evo Pvo F,, by 4.9 detre detfc vo Rcos{RE, RR T } vo Ccos{RF T, by [5, Theorem 5], RC} voa cos{t, RA T } cos{s, by 4.4, RA} voa cos{t, RA T } cos{s, NA T, by [5, Theorem 3]. } 4.0 6

8 Coroary The Moore-Penrose inverse A is of minima voume among a {, }-inverses of A. Proof: If T RA T or S NA T then the denominator in 4.5 is <. Remark. vog is unbounded in A{, }, athough cos{s, NA T } 0 vioates AGA A, cos{t, RA T } 0 vioates GAG G. References [] S.N. Afriat, Orthogona and obique projectors and the characteristics of pairs of vector spaces, Proc. Cambridge Phi. Soc , [] A. Ben-Israe, A voume associated with m n matrices, Lin. Ageb. and its App. 6799, 87- [3] A. Ben-Israe and T.N.E. Grevie, Generaized Inverses: Theory and Appications, Wiey-Interscience, 974 [4] H. Hoteing, Reations between two sets of variates, Biometrika 8935, [5] J. Miao and A. Ben-Israe, On principa anges between subspaces in IR n, Lin. Ageb. and its App. 799,

2M2. Fourier Series Prof Bill Lionheart

2M2. Fourier Series Prof Bill Lionheart M. Fourier Series Prof Bi Lionheart 1. The Fourier series of the periodic function f(x) with period has the form f(x) = a 0 + ( a n cos πnx + b n sin πnx ). Here the rea numbers a n, b n are caed the Fourier

More information

Fitting affine and orthogonal transformations between two sets of points

Fitting affine and orthogonal transformations between two sets of points Mathematica Communications 9(2004), 27-34 27 Fitting affine and orthogona transformations between two sets of points Hemuth Späth Abstract. Let two point sets P and Q be given in R n. We determine a transation

More information

Week 6 Lectures, Math 6451, Tanveer

Week 6 Lectures, Math 6451, Tanveer Fourier Series Week 6 Lectures, Math 645, Tanveer In the context of separation of variabe to find soutions of PDEs, we encountered or and in other cases f(x = f(x = a 0 + f(x = a 0 + b n sin nπx { a n

More information

Restricted weak type on maximal linear and multilinear integral maps.

Restricted weak type on maximal linear and multilinear integral maps. Restricted weak type on maxima inear and mutiinear integra maps. Oscar Basco Abstract It is shown that mutiinear operators of the form T (f 1,..., f k )(x) = R K(x, y n 1,..., y k )f 1 (y 1 )...f k (y

More information

JENSEN S OPERATOR INEQUALITY FOR FUNCTIONS OF SEVERAL VARIABLES

JENSEN S OPERATOR INEQUALITY FOR FUNCTIONS OF SEVERAL VARIABLES PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Voume 128, Number 7, Pages 2075 2084 S 0002-99390005371-5 Artice eectronicay pubished on February 16, 2000 JENSEN S OPERATOR INEQUALITY FOR FUNCTIONS OF

More information

Math 124B January 17, 2012

Math 124B January 17, 2012 Math 124B January 17, 212 Viktor Grigoryan 3 Fu Fourier series We saw in previous ectures how the Dirichet and Neumann boundary conditions ead to respectivey sine and cosine Fourier series of the initia

More information

ORTHOGONAL MULTI-WAVELETS FROM MATRIX FACTORIZATION

ORTHOGONAL MULTI-WAVELETS FROM MATRIX FACTORIZATION J. Korean Math. Soc. 46 2009, No. 2, pp. 281 294 ORHOGONAL MLI-WAVELES FROM MARIX FACORIZAION Hongying Xiao Abstract. Accuracy of the scaing function is very crucia in waveet theory, or correspondingy,

More information

Homogeneity properties of subadditive functions

Homogeneity properties of subadditive functions Annaes Mathematicae et Informaticae 32 2005 pp. 89 20. Homogeneity properties of subadditive functions Pá Burai and Árpád Száz Institute of Mathematics, University of Debrecen e-mai: buraip@math.kte.hu

More information

Generalized Bell polynomials and the combinatorics of Poisson central moments

Generalized Bell polynomials and the combinatorics of Poisson central moments Generaized Be poynomias and the combinatorics of Poisson centra moments Nicoas Privaut Division of Mathematica Sciences Schoo of Physica and Mathematica Sciences Nanyang Technoogica University SPMS-MAS-05-43,

More information

Course 2BA1, Section 11: Periodic Functions and Fourier Series

Course 2BA1, Section 11: Periodic Functions and Fourier Series Course BA, 8 9 Section : Periodic Functions and Fourier Series David R. Wikins Copyright c David R. Wikins 9 Contents Periodic Functions and Fourier Series 74. Fourier Series of Even and Odd Functions...........

More information

221B Lecture Notes Notes on Spherical Bessel Functions

221B Lecture Notes Notes on Spherical Bessel Functions Definitions B Lecture Notes Notes on Spherica Besse Functions We woud ike to sove the free Schrödinger equation [ h d r R(r) = h k R(r). () m r dr r m R(r) is the radia wave function ψ( x) = R(r)Y m (θ,

More information

(f) is called a nearly holomorphic modular form of weight k + 2r as in [5].

(f) is called a nearly holomorphic modular form of weight k + 2r as in [5]. PRODUCTS OF NEARLY HOLOMORPHIC EIGENFORMS JEFFREY BEYERL, KEVIN JAMES, CATHERINE TRENTACOSTE, AND HUI XUE Abstract. We prove that the product of two neary hoomorphic Hece eigenforms is again a Hece eigenform

More information

Problem set 6 The Perron Frobenius theorem.

Problem set 6 The Perron Frobenius theorem. Probem set 6 The Perron Frobenius theorem. Math 22a4 Oct 2 204, Due Oct.28 In a future probem set I want to discuss some criteria which aow us to concude that that the ground state of a sef-adjoint operator

More information

Row Space and Column Space of a Matrix

Row Space and Column Space of a Matrix Row Space and Column Space of a Matrix 1/18 Summary: To a m n matrix A = (a ij ), we can naturally associate subspaces of K n and of K m, called the row space of A and the column space of A, respectively.

More information

Partial permutation decoding for MacDonald codes

Partial permutation decoding for MacDonald codes Partia permutation decoding for MacDonad codes J.D. Key Department of Mathematics and Appied Mathematics University of the Western Cape 7535 Bevie, South Africa P. Seneviratne Department of Mathematics

More information

Statistics for Applications. Chapter 7: Regression 1/43

Statistics for Applications. Chapter 7: Regression 1/43 Statistics for Appications Chapter 7: Regression 1/43 Heuristics of the inear regression (1) Consider a coud of i.i.d. random points (X i,y i ),i =1,...,n : 2/43 Heuristics of the inear regression (2)

More information

The Symmetric and Antipersymmetric Solutions of the Matrix Equation A 1 X 1 B 1 + A 2 X 2 B A l X l B l = C and Its Optimal Approximation

The Symmetric and Antipersymmetric Solutions of the Matrix Equation A 1 X 1 B 1 + A 2 X 2 B A l X l B l = C and Its Optimal Approximation The Symmetric Antipersymmetric Soutions of the Matrix Equation A 1 X 1 B 1 + A 2 X 2 B 2 + + A X B C Its Optima Approximation Ying Zhang Member IAENG Abstract A matrix A (a ij) R n n is said to be symmetric

More information

linearly indepedent eigenvectors as the multiplicity of the root, but in general there may be no more than one. For further discussion, assume matrice

linearly indepedent eigenvectors as the multiplicity of the root, but in general there may be no more than one. For further discussion, assume matrice 3. Eigenvalues and Eigenvectors, Spectral Representation 3.. Eigenvalues and Eigenvectors A vector ' is eigenvector of a matrix K, if K' is parallel to ' and ' 6, i.e., K' k' k is the eigenvalue. If is

More information

MAT 167: Advanced Linear Algebra

MAT 167: Advanced Linear Algebra < Proem 1 (15 pts) MAT 167: Advanced Linear Agera Fina Exam Soutions (a) (5 pts) State the definition of a unitary matrix and expain the difference etween an orthogona matrix and an unitary matrix. Soution:

More information

Primal and dual active-set methods for convex quadratic programming

Primal and dual active-set methods for convex quadratic programming Math. Program., Ser. A 216) 159:469 58 DOI 1.17/s117-15-966-2 FULL LENGTH PAPER Prima and dua active-set methods for convex quadratic programming Anders Forsgren 1 Phiip E. Gi 2 Eizabeth Wong 2 Received:

More information

arxiv: v1 [math.fa] 23 Aug 2018

arxiv: v1 [math.fa] 23 Aug 2018 An Exact Upper Bound on the L p Lebesgue Constant and The -Rényi Entropy Power Inequaity for Integer Vaued Random Variabes arxiv:808.0773v [math.fa] 3 Aug 08 Peng Xu, Mokshay Madiman, James Mebourne Abstract

More information

Factorizations of Invertible Symmetric Matrices over Polynomial Rings with Involution

Factorizations of Invertible Symmetric Matrices over Polynomial Rings with Involution Goba Journa of Pure and Appied Matheatics ISSN 0973-1768 Voue 13 Nuber 10 (017) pp 7073-7080 Research India Pubications http://wwwripubicationco Factorizations of Invertibe Syetric Matrices over Poynoia

More information

Lecture Note 3: Stationary Iterative Methods

Lecture Note 3: Stationary Iterative Methods MATH 5330: Computationa Methods of Linear Agebra Lecture Note 3: Stationary Iterative Methods Xianyi Zeng Department of Mathematica Sciences, UTEP Stationary Iterative Methods The Gaussian eimination (or

More information

Volume 13, MAIN ARTICLES

Volume 13, MAIN ARTICLES Voume 13, 2009 1 MAIN ARTICLES THE BASIC BVPs OF THE THEORY OF ELASTIC BINARY MIXTURES FOR A HALF-PLANE WITH CURVILINEAR CUTS Bitsadze L. I. Vekua Institute of Appied Mathematics of Iv. Javakhishvii Tbiisi

More information

(a) If A is a 3 by 4 matrix, what does this tell us about its nullspace? Solution: dim N(A) 1, since rank(a) 3. Ax =

(a) If A is a 3 by 4 matrix, what does this tell us about its nullspace? Solution: dim N(A) 1, since rank(a) 3. Ax = . (5 points) (a) If A is a 3 by 4 matrix, what does this tell us about its nullspace? dim N(A), since rank(a) 3. (b) If we also know that Ax = has no solution, what do we know about the rank of A? C(A)

More information

LECTURE NOTES 8 THE TRACELESS SYMMETRIC TENSOR EXPANSION AND STANDARD SPHERICAL HARMONICS

LECTURE NOTES 8 THE TRACELESS SYMMETRIC TENSOR EXPANSION AND STANDARD SPHERICAL HARMONICS MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Physics 8.07: Eectromagnetism II October, 202 Prof. Aan Guth LECTURE NOTES 8 THE TRACELESS SYMMETRIC TENSOR EXPANSION AND STANDARD SPHERICAL HARMONICS

More information

Algorithms to Compute Bases and the Rank of a Matrix

Algorithms to Compute Bases and the Rank of a Matrix Algorithms to Compute Bases and the Rank of a Matrix Subspaces associated to a matrix Suppose that A is an m n matrix The row space of A is the subspace of R n spanned by the rows of A The column space

More information

UNIFORM CONVERGENCE OF MULTIPLIER CONVERGENT SERIES

UNIFORM CONVERGENCE OF MULTIPLIER CONVERGENT SERIES royecciones Vo. 26, N o 1, pp. 27-35, May 2007. Universidad Catóica de Norte Antofagasta - Chie UNIFORM CONVERGENCE OF MULTILIER CONVERGENT SERIES CHARLES SWARTZ NEW MEXICO STATE UNIVERSITY Received :

More information

Alberto Maydeu Olivares Instituto de Empresa Marketing Dept. C/Maria de Molina Madrid Spain

Alberto Maydeu Olivares Instituto de Empresa Marketing Dept. C/Maria de Molina Madrid Spain CORRECTIONS TO CLASSICAL PROCEDURES FOR ESTIMATING THURSTONE S CASE V MODEL FOR RANKING DATA Aberto Maydeu Oivares Instituto de Empresa Marketing Dept. C/Maria de Moina -5 28006 Madrid Spain Aberto.Maydeu@ie.edu

More information

The state vectors j, m transform in rotations like D(R) j, m = m j, m j, m D(R) j, m. m m (R) = j, m exp. where. d (j) m m (β) j, m exp ij )

The state vectors j, m transform in rotations like D(R) j, m = m j, m j, m D(R) j, m. m m (R) = j, m exp. where. d (j) m m (β) j, m exp ij ) Anguar momentum agebra It is easy to see that the operat J J x J x + J y J y + J z J z commutes with the operats J x, J y and J z, [J, J i ] 0 We choose the component J z and denote the common eigenstate

More information

Equality: Two matrices A and B are equal, i.e., A = B if A and B have the same order and the entries of A and B are the same.

Equality: Two matrices A and B are equal, i.e., A = B if A and B have the same order and the entries of A and B are the same. Introduction Matrix Operations Matrix: An m n matrix A is an m-by-n array of scalars from a field (for example real numbers) of the form a a a n a a a n A a m a m a mn The order (or size) of A is m n (read

More information

On Some Basic Properties of Geometric Real Sequences

On Some Basic Properties of Geometric Real Sequences On Some Basic Properties of eometric Rea Sequences Khirod Boruah Research Schoar, Department of Mathematics, Rajiv andhi University Rono His, Doimukh-791112, Arunacha Pradesh, India Abstract Objective

More information

Distributed average consensus: Beyond the realm of linearity

Distributed average consensus: Beyond the realm of linearity Distributed average consensus: Beyond the ream of inearity Usman A. Khan, Soummya Kar, and José M. F. Moura Department of Eectrica and Computer Engineering Carnegie Meon University 5 Forbes Ave, Pittsburgh,

More information

MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES

MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES MATH 172: MOTIVATION FOR FOURIER SERIES: SEPARATION OF VARIABLES Separation of variabes is a method to sove certain PDEs which have a warped product structure. First, on R n, a inear PDE of order m is

More information

arxiv: v3 [math.ac] 7 Dec 2009

arxiv: v3 [math.ac] 7 Dec 2009 SUPERTROPICAL MATRIX ALGEBRA II: SOLVING TROPICAL EQUATIONS ZUR IZHAKIAN AND LOUIS ROWEN arxiv:0902.2159v3 [math.ac] 7 Dec 2009 Abstract. We continue the study of matrices over a supertropica agebra, proving

More information

CS229 Lecture notes. Andrew Ng

CS229 Lecture notes. Andrew Ng CS229 Lecture notes Andrew Ng Part IX The EM agorithm In the previous set of notes, we taked about the EM agorithm as appied to fitting a mixture of Gaussians. In this set of notes, we give a broader view

More information

Lecture 4 Orthonormal vectors and QR factorization

Lecture 4 Orthonormal vectors and QR factorization Orthonormal vectors and QR factorization 4 1 Lecture 4 Orthonormal vectors and QR factorization EE263 Autumn 2004 orthonormal vectors Gram-Schmidt procedure, QR factorization orthogonal decomposition induced

More information

SUPPLEMENTARY MATERIAL TO INNOVATED SCALABLE EFFICIENT ESTIMATION IN ULTRA-LARGE GAUSSIAN GRAPHICAL MODELS

SUPPLEMENTARY MATERIAL TO INNOVATED SCALABLE EFFICIENT ESTIMATION IN ULTRA-LARGE GAUSSIAN GRAPHICAL MODELS ISEE 1 SUPPLEMENTARY MATERIAL TO INNOVATED SCALABLE EFFICIENT ESTIMATION IN ULTRA-LARGE GAUSSIAN GRAPHICAL MODELS By Yingying Fan and Jinchi Lv University of Southern Caifornia This Suppementary Materia

More information

PRIME TWISTS OF ELLIPTIC CURVES

PRIME TWISTS OF ELLIPTIC CURVES PRIME TWISTS OF ELLIPTIC CURVES DANIEL KRIZ AND CHAO LI Abstract. For certain eiptic curves E/Q with E(Q)[2] = Z/2Z, we prove a criterion for prime twists of E to have anaytic rank 0 or 1, based on a mod

More information

THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE

THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE THE THREE POINT STEINER PROBLEM ON THE FLAT TORUS: THE MINIMAL LUNE CASE KATIE L. MAY AND MELISSA A. MITCHELL Abstract. We show how to identify the minima path network connecting three fixed points on

More information

arxiv:math/ v2 [math.ag] 12 Jul 2006

arxiv:math/ v2 [math.ag] 12 Jul 2006 GRASSMANNIANS AND REPRESENTATIONS arxiv:math/0507482v2 [math.ag] 12 Ju 2006 DAN EDIDIN AND CHRISTOPHER A. FRANCISCO Abstract. In this note we use Bott-Bore-Wei theory to compute cohomoogy of interesting

More information

On the Number of Limit Cycles for Discontinuous Generalized Liénard Polynomial Differential Systems

On the Number of Limit Cycles for Discontinuous Generalized Liénard Polynomial Differential Systems Internationa Journa of Bifurcation and Chaos Vo. 25 No. 10 2015 1550131 10 pages c Word Scientific Pubishing Company DOI: 10.112/S02181271550131X On the Number of Limit Cyces for Discontinuous Generaized

More information

Strauss PDEs 2e: Section Exercise 1 Page 1 of 7

Strauss PDEs 2e: Section Exercise 1 Page 1 of 7 Strauss PDEs 2e: Section 4.3 - Exercise 1 Page 1 of 7 Exercise 1 Find the eigenvaues graphicay for the boundary conditions X(0) = 0, X () + ax() = 0. Assume that a 0. Soution The aim here is to determine

More information

BALANCING REGULAR MATRIX PENCILS

BALANCING REGULAR MATRIX PENCILS BALANCING REGULAR MATRIX PENCILS DAMIEN LEMONNIER AND PAUL VAN DOOREN Abstract. In this paper we present a new diagona baancing technique for reguar matrix pencis λb A, which aims at reducing the sensitivity

More information

Maejo International Journal of Science and Technology

Maejo International Journal of Science and Technology Fu Paper Maejo Internationa Journa of Science and Technoogy ISSN 1905-7873 Avaiabe onine at www.mijst.mju.ac.th A study on Lucas difference sequence spaces (, ) (, ) and Murat Karakas * and Ayse Metin

More information

(This is a sample cover image for this issue. The actual cover is not yet available at this time.)

(This is a sample cover image for this issue. The actual cover is not yet available at this time.) (This is a sampe cover image for this issue The actua cover is not yet avaiabe at this time) This artice appeared in a journa pubished by Esevier The attached copy is furnished to the author for interna

More information

Math Bootcamp An p-dimensional vector is p numbers put together. Written as. x 1 x =. x p

Math Bootcamp An p-dimensional vector is p numbers put together. Written as. x 1 x =. x p Math Bootcamp 2012 1 Review of matrix algebra 1.1 Vectors and rules of operations An p-dimensional vector is p numbers put together. Written as x 1 x =. x p. When p = 1, this represents a point in the

More information

Lecture 6: Moderately Large Deflection Theory of Beams

Lecture 6: Moderately Large Deflection Theory of Beams Structura Mechanics 2.8 Lecture 6 Semester Yr Lecture 6: Moderatey Large Defection Theory of Beams 6.1 Genera Formuation Compare to the cassica theory of beams with infinitesima deformation, the moderatey

More information

CONGRUENCES. 1. History

CONGRUENCES. 1. History CONGRUENCES HAO BILLY LEE Abstract. These are notes I created for a seminar tak, foowing the papers of On the -adic Representations and Congruences for Coefficients of Moduar Forms by Swinnerton-Dyer and

More information

4 1-D Boundary Value Problems Heat Equation

4 1-D Boundary Value Problems Heat Equation 4 -D Boundary Vaue Probems Heat Equation The main purpose of this chapter is to study boundary vaue probems for the heat equation on a finite rod a x b. u t (x, t = ku xx (x, t, a < x < b, t > u(x, = ϕ(x

More information

The Group Structure on a Smooth Tropical Cubic

The Group Structure on a Smooth Tropical Cubic The Group Structure on a Smooth Tropica Cubic Ethan Lake Apri 20, 2015 Abstract Just as in in cassica agebraic geometry, it is possibe to define a group aw on a smooth tropica cubic curve. In this note,

More information

2. Linear algebra. matrices and vectors. linear equations. range and nullspace of matrices. function of vectors, gradient and Hessian

2. Linear algebra. matrices and vectors. linear equations. range and nullspace of matrices. function of vectors, gradient and Hessian FE661 - Statistical Methods for Financial Engineering 2. Linear algebra Jitkomut Songsiri matrices and vectors linear equations range and nullspace of matrices function of vectors, gradient and Hessian

More information

2018 Fall 2210Q Section 013 Midterm Exam II Solution

2018 Fall 2210Q Section 013 Midterm Exam II Solution 08 Fall 0Q Section 0 Midterm Exam II Solution True or False questions points 0 0 points) ) Let A be an n n matrix. If the equation Ax b has at least one solution for each b R n, then the solution is unique

More information

Parallel-Axis Theorem

Parallel-Axis Theorem Parae-Axis Theorem In the previous exampes, the axis of rotation coincided with the axis of symmetry of the object For an arbitrary axis, the paraeaxis theorem often simpifies cacuations The theorem states

More information

SEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l

SEMINAR 2. PENDULUMS. V = mgl cos θ. (2) L = T V = 1 2 ml2 θ2 + mgl cos θ, (3) d dt ml2 θ2 + mgl sin θ = 0, (4) θ + g l Probem 7. Simpe Penduum SEMINAR. PENDULUMS A simpe penduum means a mass m suspended by a string weightess rigid rod of ength so that it can swing in a pane. The y-axis is directed down, x-axis is directed

More information

The second maximal and minimal Kirchhoff indices of unicyclic graphs 1

The second maximal and minimal Kirchhoff indices of unicyclic graphs 1 MATCH Communications in Mathematica and in Computer Chemistry MATCH Commun. Math. Comput. Chem. 61 (009) 683-695 ISSN 0340-653 The second maxima and minima Kirchhoff indices of unicycic graphs 1 Wei Zhang,

More information

An explicit Jordan Decomposition of Companion matrices

An explicit Jordan Decomposition of Companion matrices An expicit Jordan Decomposition of Companion matrices Fermín S V Bazán Departamento de Matemática CFM UFSC 88040-900 Forianópois SC E-mai: fermin@mtmufscbr S Gratton CERFACS 42 Av Gaspard Coriois 31057

More information

C. Fourier Sine Series Overview

C. Fourier Sine Series Overview 12 PHILIP D. LOEWEN C. Fourier Sine Series Overview Let some constant > be given. The symboic form of the FSS Eigenvaue probem combines an ordinary differentia equation (ODE) on the interva (, ) with a

More information

Control of Synchronization for Multi-Agent Systems in Acceleration Motion with Additional Analysis of Formation Control

Control of Synchronization for Multi-Agent Systems in Acceleration Motion with Additional Analysis of Formation Control 2 American Contro Conference on O'Farre Street San Francisco CA USA June 29 - Juy 2 Contro of Synchronization for uti-agent Systems in Acceeration otion with Additiona Anaysis of Formation Contro Haopeng

More information

Discrete Bernoulli s Formula and its Applications Arising from Generalized Difference Operator

Discrete Bernoulli s Formula and its Applications Arising from Generalized Difference Operator Int. Journa of Math. Anaysis, Vo. 7, 2013, no. 5, 229-240 Discrete Bernoui s Formua and its Appications Arising from Generaized Difference Operator G. Britto Antony Xavier 1 Department of Mathematics,

More information

A NOTE ON QUASI-STATIONARY DISTRIBUTIONS OF BIRTH-DEATH PROCESSES AND THE SIS LOGISTIC EPIDEMIC

A NOTE ON QUASI-STATIONARY DISTRIBUTIONS OF BIRTH-DEATH PROCESSES AND THE SIS LOGISTIC EPIDEMIC (January 8, 2003) A NOTE ON QUASI-STATIONARY DISTRIBUTIONS OF BIRTH-DEATH PROCESSES AND THE SIS LOGISTIC EPIDEMIC DAMIAN CLANCY, University of Liverpoo PHILIP K. POLLETT, University of Queensand Abstract

More information

The arc is the only chainable continuum admitting a mean

The arc is the only chainable continuum admitting a mean The arc is the ony chainabe continuum admitting a mean Aejandro Ianes and Hugo Vianueva September 4, 26 Abstract Let X be a metric continuum. A mean on X is a continuous function : X X! X such that for

More information

A Brief Introduction to Markov Chains and Hidden Markov Models

A Brief Introduction to Markov Chains and Hidden Markov Models A Brief Introduction to Markov Chains and Hidden Markov Modes Aen B MacKenzie Notes for December 1, 3, &8, 2015 Discrete-Time Markov Chains You may reca that when we first introduced random processes,

More information

Investigation on spectrum of the adjacency matrix and Laplacian matrix of graph G l

Investigation on spectrum of the adjacency matrix and Laplacian matrix of graph G l Investigation on spectrum of the adjacency matrix and Lapacian matrix of graph G SHUHUA YIN Computer Science and Information Technoogy Coege Zhejiang Wani University Ningbo 3500 PEOPLE S REPUBLIC OF CHINA

More information

Forces of Friction. through a viscous medium, there will be a resistance to the motion. and its environment

Forces of Friction. through a viscous medium, there will be a resistance to the motion. and its environment Forces of Friction When an object is in motion on a surface or through a viscous medium, there wi be a resistance to the motion This is due to the interactions between the object and its environment This

More information

Assignment 7 Due Tuessday, March 29, 2016

Assignment 7 Due Tuessday, March 29, 2016 Math 45 / AMCS 55 Dr. DeTurck Assignment 7 Due Tuessday, March 9, 6 Topics for this week Convergence of Fourier series; Lapace s equation and harmonic functions: basic properties, compuations on rectanges

More information

THE REACHABILITY CONES OF ESSENTIALLY NONNEGATIVE MATRICES

THE REACHABILITY CONES OF ESSENTIALLY NONNEGATIVE MATRICES THE REACHABILITY CONES OF ESSENTIALLY NONNEGATIVE MATRICES by Michae Neumann Department of Mathematics, University of Connecticut, Storrs, CT 06269 3009 and Ronad J. Stern Department of Mathematics, Concordia

More information

PRESENTING QUEER SCHUR SUPERALGEBRAS

PRESENTING QUEER SCHUR SUPERALGEBRAS PRESENTING QUEER SCHUR SUPERALGEBRAS JIE DU AND JINKUI WAN Abstract. Associated to the two types of finite dimensiona simpe superagebras, there are the genera inear Lie superagebra and the queer Lie superagebra.

More information

NOTES FOR LINEAR ALGEBRA 133

NOTES FOR LINEAR ALGEBRA 133 NOTES FOR LINEAR ALGEBRA 33 William J Anderson McGill University These are not official notes for Math 33 identical to the notes projected in class They are intended for Anderson s section 4, and are 2

More information

The DMP Inverse for Rectangular Matrices

The DMP Inverse for Rectangular Matrices Filomat 31:19 (2017, 6015 6019 https://doi.org/10.2298/fil1719015m Published by Faculty of Sciences Mathematics, University of Niš, Serbia Available at: http://.pmf.ni.ac.rs/filomat The DMP Inverse for

More information

AFormula for N-Row Macdonald Polynomials

AFormula for N-Row Macdonald Polynomials Journa of Agebraic Combinatorics, 21, 111 13, 25 c 25 Springer Science + Business Media, Inc. Manufactured in The Netherands. AFormua for N-Row Macdonad Poynomias ELLISON-ANNE WILLIAMS North Caroina State

More information

Consistent initial values for DAE systems in circuit simulation D. Estevez Schwarz Abstract One of the diculties of the numerical integration methods

Consistent initial values for DAE systems in circuit simulation D. Estevez Schwarz Abstract One of the diculties of the numerical integration methods Consistent initia vaues for DAE systems in circuit simuation D. Estevez Schwarz Abstract One of the dicuties of the numerica integration methods for dierentia-agebraic equations (DAEs) is computing consistent

More information

Supplementary Appendix (not for publication) for: The Value of Network Information

Supplementary Appendix (not for publication) for: The Value of Network Information Suppementary Appendix not for pubication for: The Vaue of Network Information Itay P. Fainmesser and Andrea Gaeotti September 6, 03 This appendix incudes the proof of Proposition from the paper "The Vaue

More information

Two-Stage Least Squares as Minimum Distance

Two-Stage Least Squares as Minimum Distance Two-Stage Least Squares as Minimum Distance Frank Windmeijer Discussion Paper 17 / 683 7 June 2017 Department of Economics University of Bristo Priory Road Compex Bristo BS8 1TU United Kingdom Two-Stage

More information

Akaike Information Criterion for ANOVA Model with a Simple Order Restriction

Akaike Information Criterion for ANOVA Model with a Simple Order Restriction Akaike Information Criterion for ANOVA Mode with a Simpe Order Restriction Yu Inatsu * Department of Mathematics, Graduate Schoo of Science, Hiroshima University ABSTRACT In this paper, we consider Akaike

More information

WAVELET LINEAR ESTIMATION FOR DERIVATIVES OF A DENSITY FROM OBSERVATIONS OF MIXTURES WITH VARYING MIXING PROPORTIONS. B. L. S.

WAVELET LINEAR ESTIMATION FOR DERIVATIVES OF A DENSITY FROM OBSERVATIONS OF MIXTURES WITH VARYING MIXING PROPORTIONS. B. L. S. Indian J. Pure App. Math., 41(1): 275-291, February 2010 c Indian Nationa Science Academy WAVELET LINEAR ESTIMATION FOR DERIVATIVES OF A DENSITY FROM OBSERVATIONS OF MIXTURES WITH VARYING MIXING PROPORTIONS

More information

An Extension of Almost Sure Central Limit Theorem for Order Statistics

An Extension of Almost Sure Central Limit Theorem for Order Statistics An Extension of Amost Sure Centra Limit Theorem for Order Statistics T. Bin, P. Zuoxiang & S. Nadarajah First version: 6 December 2007 Research Report No. 9, 2007, Probabiity Statistics Group Schoo of

More information

Math 215 HW #9 Solutions

Math 215 HW #9 Solutions Math 5 HW #9 Solutions. Problem 4.4.. If A is a 5 by 5 matrix with all a ij, then det A. Volumes or the big formula or pivots should give some upper bound on the determinant. Answer: Let v i be the ith

More information

ANALOG OF HEAT EQUATION FOR GAUSSIAN MEASURE OF A BALL IN HILBERT SPACE GYULA PAP

ANALOG OF HEAT EQUATION FOR GAUSSIAN MEASURE OF A BALL IN HILBERT SPACE GYULA PAP ANALOG OF HEAT EQUATION FOR GAUSSIAN MEASURE OF A BALL IN HILBERT SPACE GYULA PAP ABSTRACT. If µ is a Gaussian measure on a Hibert space with mean a and covariance operator T, and r is a} fixed positive

More information

ASummaryofGaussianProcesses Coryn A.L. Bailer-Jones

ASummaryofGaussianProcesses Coryn A.L. Bailer-Jones ASummaryofGaussianProcesses Coryn A.L. Baier-Jones Cavendish Laboratory University of Cambridge caj@mrao.cam.ac.uk Introduction A genera prediction probem can be posed as foows. We consider that the variabe

More information

Jackson 4.10 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell

Jackson 4.10 Homework Problem Solution Dr. Christopher S. Baird University of Massachusetts Lowell Jackson 4.10 Homework Probem Soution Dr. Christopher S. Baird University of Massachusetts Lowe PROBLEM: Two concentric conducting spheres of inner and outer radii a and b, respectivey, carry charges ±.

More information

LECTURE NOTES 9 TRACELESS SYMMETRIC TENSOR APPROACH TO LEGENDRE POLYNOMIALS AND SPHERICAL HARMONICS

LECTURE NOTES 9 TRACELESS SYMMETRIC TENSOR APPROACH TO LEGENDRE POLYNOMIALS AND SPHERICAL HARMONICS MASSACHUSETTS INSTITUTE OF TECHNOLOGY Physics Department Physics 8.07: Eectromagnetism II October 7, 202 Prof. Aan Guth LECTURE NOTES 9 TRACELESS SYMMETRIC TENSOR APPROACH TO LEGENDRE POLYNOMIALS AND SPHERICAL

More information

~ g-inverses are indeed an integral part of linear algebra and should be treated as such even at an elementary level.

~ g-inverses are indeed an integral part of linear algebra and should be treated as such even at an elementary level. Existence of Generalized Inverse: Ten Proofs and Some Remarks R B Bapat Introduction The theory of g-inverses has seen a substantial growth over the past few decades. It is an area of great theoretical

More information

u(x) s.t. px w x 0 Denote the solution to this problem by ˆx(p, x). In order to obtain ˆx we may simply solve the standard problem max x 0

u(x) s.t. px w x 0 Denote the solution to this problem by ˆx(p, x). In order to obtain ˆx we may simply solve the standard problem max x 0 Bocconi University PhD in Economics - Microeconomics I Prof M Messner Probem Set 4 - Soution Probem : If an individua has an endowment instead of a monetary income his weath depends on price eves In particuar,

More information

Integrating Factor Methods as Exponential Integrators

Integrating Factor Methods as Exponential Integrators Integrating Factor Methods as Exponentia Integrators Borisav V. Minchev Department of Mathematica Science, NTNU, 7491 Trondheim, Norway Borko.Minchev@ii.uib.no Abstract. Recenty a ot of effort has been

More information

Lecture Summaries for Linear Algebra M51A

Lecture Summaries for Linear Algebra M51A These lecture summaries may also be viewed online by clicking the L icon at the top right of any lecture screen. Lecture Summaries for Linear Algebra M51A refers to the section in the textbook. Lecture

More information

Chapter 1. Matrix Algebra

Chapter 1. Matrix Algebra ST4233, Linear Models, Semester 1 2008-2009 Chapter 1. Matrix Algebra 1 Matrix and vector notation Definition 1.1 A matrix is a rectangular or square array of numbers of variables. We use uppercase boldface

More information

Math113: Linear Algebra. Beifang Chen

Math113: Linear Algebra. Beifang Chen Math3: Linear Algebra Beifang Chen Spring 26 Contents Systems of Linear Equations 3 Systems of Linear Equations 3 Linear Systems 3 2 Geometric Interpretation 3 3 Matrices of Linear Systems 4 4 Elementary

More information

Theory of Generalized k-difference Operator and Its Application in Number Theory

Theory of Generalized k-difference Operator and Its Application in Number Theory Internationa Journa of Mathematica Anaysis Vo. 9, 2015, no. 19, 955-964 HIKARI Ltd, www.m-hiari.com http://dx.doi.org/10.12988/ijma.2015.5389 Theory of Generaized -Difference Operator and Its Appication

More information

Online Appendices for The Economics of Nationalism (Xiaohuan Lan and Ben Li)

Online Appendices for The Economics of Nationalism (Xiaohuan Lan and Ben Li) Onine Appendices for The Economics of Nationaism Xiaohuan Lan and Ben Li) A. Derivation of inequaities 9) and 10) Consider Home without oss of generaity. Denote gobaized and ungobaized by g and ng, respectivey.

More information

THE PARTITION FUNCTION AND HECKE OPERATORS

THE PARTITION FUNCTION AND HECKE OPERATORS THE PARTITION FUNCTION AND HECKE OPERATORS KEN ONO Abstract. The theory of congruences for the partition function p(n depends heaviy on the properties of haf-integra weight Hecke operators. The subject

More information

$, (2.1) n="# #. (2.2)

$, (2.1) n=# #. (2.2) Chapter. Eectrostatic II Notes: Most of the materia presented in this chapter is taken from Jackson, Chap.,, and 4, and Di Bartoo, Chap... Mathematica Considerations.. The Fourier series and the Fourier

More information

On formulas for moments of the Wishart distributions as weighted generating functions of matchings

On formulas for moments of the Wishart distributions as weighted generating functions of matchings FPSAC 2010, San Francisco, USA DMTCS proc. AN, 2010, 821 832 On formuas for moments of the Wishart distributions as weighted generating functions of matchings Yasuhide NUMATA 1,3 and Satoshi KURIKI 2,3

More information

Powers of Ideals: Primary Decompositions, Artin-Rees Lemma and Regularity

Powers of Ideals: Primary Decompositions, Artin-Rees Lemma and Regularity Powers of Ideas: Primary Decompositions, Artin-Rees Lemma and Reguarity Irena Swanson Department of Mathematica Sciences, New Mexico State University, Las Cruces, NM 88003-8001 (e-mai: iswanson@nmsu.edu)

More information

Physics 116C Helmholtz s and Laplace s Equations in Spherical Polar Coordinates: Spherical Harmonics and Spherical Bessel Functions

Physics 116C Helmholtz s and Laplace s Equations in Spherical Polar Coordinates: Spherical Harmonics and Spherical Bessel Functions Physics 116C Hemhotz s an Lapace s Equations in Spherica Poar Coorinates: Spherica Harmonics an Spherica Besse Functions Peter Young Date: October 28, 2013) I. HELMHOLTZ S EQUATION As iscusse in cass,

More information

Global Optimality Principles for Polynomial Optimization Problems over Box or Bivalent Constraints by Separable Polynomial Approximations

Global Optimality Principles for Polynomial Optimization Problems over Box or Bivalent Constraints by Separable Polynomial Approximations Goba Optimaity Principes for Poynomia Optimization Probems over Box or Bivaent Constraints by Separabe Poynomia Approximations V. Jeyakumar, G. Li and S. Srisatkunarajah Revised Version II: December 23,

More information

The values of the generalized matrix functions of 3 3 matrices

The values of the generalized matrix functions of 3 3 matrices Hiroshima Math. J. 45 (205), 8 The vaues of the generaized matrix functions of matrices Ryo Tabata (Received Juy 25, 20) (Revised October 25, 20) Abstract. When A is a positive semi-definite Hermitian

More information

Linear algebra for computational statistics

Linear algebra for computational statistics University of Seoul May 3, 2018 Vector and Matrix Notation Denote 2-dimensional data array (n p matrix) by X. Denote the element in the ith row and the jth column of X by x ij or (X) ij. Denote by X j

More information

Analysis of Emerson s Multiple Model Interpolation Estimation Algorithms: The MIMO Case

Analysis of Emerson s Multiple Model Interpolation Estimation Algorithms: The MIMO Case Technica Report PC-04-00 Anaysis of Emerson s Mutipe Mode Interpoation Estimation Agorithms: The MIMO Case João P. Hespanha Dae E. Seborg University of Caifornia, Santa Barbara February 0, 004 Anaysis

More information

6 Wave Equation on an Interval: Separation of Variables

6 Wave Equation on an Interval: Separation of Variables 6 Wave Equation on an Interva: Separation of Variabes 6.1 Dirichet Boundary Conditions Ref: Strauss, Chapter 4 We now use the separation of variabes technique to study the wave equation on a finite interva.

More information