MATRIX COMPLETION THEOREMS1 SL(2«, R), Although Sp(2, R)
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Modeling, Inference and Clustering for Equivalence Classes of 3-D Orientations Chuanlong Du Iowa State University
Iowa State University Capstones, Theses and Graduate Theses and Dissertations Dissertations 2014 Modeling, inference and clustering for equivalence classes of 3-D orientations Chuanlong Du Iowa State University Follow this and additional works at: https://lib.dr.iastate.edu/etd Part of the Statistics and Probability Commons Recommended Citation Du, Chuanlong, "Modeling, inference and clustering for equivalence classes of 3-D orientations" (2014). Graduate Theses and Dissertations. 13738. https://lib.dr.iastate.edu/etd/13738 This Dissertation is brought to you for free and open access by the Iowa State University Capstones, Theses and Dissertations at Iowa State University Digital Repository. It has been accepted for inclusion in Graduate Theses and Dissertations by an authorized administrator of Iowa State University Digital Repository. For more information, please contact [email protected]. Modeling, inference and clustering for equivalence classes of 3-D orientations by Chuanlong Du A dissertation submitted to the graduate faculty in partial fulfillment of the requirements for the degree of DOCTOR OF PHILOSOPHY Major: Statistics Program of Study Committee: Stephen Vardeman, Co-major Professor Daniel Nordman, Co-major Professor Dan Nettleton Huaiqing Wu Guang Song Iowa State University Ames, Iowa 2014 Copyright c Chuanlong Du, 2014. All rights reserved. ii DEDICATION I would like to dedicate this dissertation to my mother Jinyan Xu. She always encourages me to follow my heart and to seek my dreams. Her words have always inspired me and encouraged me to face difficulties and challenges I came across in my life. I would also like to dedicate this dissertation to my wife Lisha Li without whose support and help I would not have been able to complete this work. -
Unitary Group - Wikipedia
Unitary group - Wikipedia https://en.wikipedia.org/wiki/Unitary_group Unitary group In mathematics, the unitary group of degree n, denoted U( n), is the group of n × n unitary matrices, with the group operation of matrix multiplication. The unitary group is a subgroup of the general linear group GL( n, C). Hyperorthogonal group is an archaic name for the unitary group, especially over finite fields. For the group of unitary matrices with determinant 1, see Special unitary group. In the simple case n = 1, the group U(1) corresponds to the circle group, consisting of all complex numbers with absolute value 1 under multiplication. All the unitary groups contain copies of this group. The unitary group U( n) is a real Lie group of dimension n2. The Lie algebra of U( n) consists of n × n skew-Hermitian matrices, with the Lie bracket given by the commutator. The general unitary group (also called the group of unitary similitudes ) consists of all matrices A such that A∗A is a nonzero multiple of the identity matrix, and is just the product of the unitary group with the group of all positive multiples of the identity matrix. Contents Properties Topology Related groups 2-out-of-3 property Special unitary and projective unitary groups G-structure: almost Hermitian Generalizations Indefinite forms Finite fields Degree-2 separable algebras Algebraic groups Unitary group of a quadratic module Polynomial invariants Classifying space See also Notes References Properties Since the determinant of a unitary matrix is a complex number with norm 1, the determinant gives a group 1 of 7 2/23/2018, 10:13 AM Unitary group - Wikipedia https://en.wikipedia.org/wiki/Unitary_group homomorphism The kernel of this homomorphism is the set of unitary matrices with determinant 1. -
Be the Integral Symplectic Group and S(G) Be the Set of All Positive Integers Which Can Occur As the Order of an Element in G
FINITE ORDER ELEMENTS IN THE INTEGRAL SYMPLECTIC GROUP KUMAR BALASUBRAMANIAN, M. RAM MURTY, AND KARAM DEO SHANKHADHAR Abstract For g 2 N, let G = Sp(2g; Z) be the integral symplectic group and S(g) be the set of all positive integers which can occur as the order of an element in G. In this paper, we show that S(g) is a bounded subset of R for all positive integers g. We also study the growth of the functions f(g) = jS(g)j, and h(g) = maxfm 2 N j m 2 S(g)g and show that they have at least exponential growth. 1. Introduction Given a group G and a positive integer m 2 N, it is natural to ask if there exists k 2 G such that o(k) = m, where o(k) denotes the order of the element k. In this paper, we make some observations about the collection of positive integers which can occur as orders of elements in G = Sp(2g; Z). Before we proceed further we set up some notations and briefly mention the questions studied in this paper. Let G = Sp(2g; Z) be the group of all 2g × 2g matrices with integral entries satisfying > A JA = J 0 I where A> is the transpose of the matrix A and J = g g . −Ig 0g α1 αk Throughout we write m = p1 : : : pk , where pi is a prime and αi > 0 for all i 2 f1; 2; : : : ; kg. We also assume that the primes pi are such that pi < pi+1 for 1 ≤ i < k. -
Sometimes Only Square Matrices Can Be Diagonalized 19
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 52, October 1975 SOMETIMESONLY SQUARE MATRICESCAN BE DIAGONALIZED LAWRENCE S. LEVY ABSTRACT. It is proved that every SQUARE matrix over a serial ring is equivalent to some diagonal matrix, even though there are rectangular matri- ces over these rings which cannot be diagonalized. Two matrices A and B over a ring R are equivalent if B - PAQ for in- vertible matrices P and Q over R- Following R. B. Warfield, we will call a module serial if its submodules are totally ordered by inclusion; and we will call a ring R serial it R is a direct sum of serial left modules, and also a direct sum of serial right mod- ules. When R is artinian, these become the generalized uniserial rings of Nakayama LE-GJ- Note that, in serial rings, finitely generated ideals do not have to be principal; for example, let R be any full ring of lower triangular matrices over a field. Moreover, it is well known (and easily proved) that if aR + bR is a nonprincipal right ideal in any ring, the 1x2 matrix [a b] is not equivalent to a diagonal matrix. Thus serial rings do not have the property that every rectangular matrix can be diagonalized. 1. Background. Serial rings are clearly semiperfect (P/radR is semisim- ple artinian and idempotents can be lifted modulo radP). (1.1) Every indecomposable projective module over a semiperfect ring R is S eR for some primitive idempotent e of R. (See [M].) A double-headed arrow -» will denote an "onto" homomorphism. -
The Classical Groups and Domains 1. the Disk, Upper Half-Plane, SL 2(R
(June 8, 2018) The Classical Groups and Domains Paul Garrett [email protected] http:=/www.math.umn.edu/egarrett/ The complex unit disk D = fz 2 C : jzj < 1g has four families of generalizations to bounded open subsets in Cn with groups acting transitively upon them. Such domains, defined more precisely below, are bounded symmetric domains. First, we recall some standard facts about the unit disk, the upper half-plane, the ambient complex projective line, and corresponding groups acting by linear fractional (M¨obius)transformations. Happily, many of the higher- dimensional bounded symmetric domains behave in a manner that is a simple extension of this simplest case. 1. The disk, upper half-plane, SL2(R), and U(1; 1) 2. Classical groups over C and over R 3. The four families of self-adjoint cones 4. The four families of classical domains 5. Harish-Chandra's and Borel's realization of domains 1. The disk, upper half-plane, SL2(R), and U(1; 1) The group a b GL ( ) = f : a; b; c; d 2 ; ad − bc 6= 0g 2 C c d C acts on the extended complex plane C [ 1 by linear fractional transformations a b az + b (z) = c d cz + d with the traditional natural convention about arithmetic with 1. But we can be more precise, in a form helpful for higher-dimensional cases: introduce homogeneous coordinates for the complex projective line P1, by defining P1 to be a set of cosets u 1 = f : not both u; v are 0g= × = 2 − f0g = × P v C C C where C× acts by scalar multiplication. -
The Symplectic Group
Sp(n), THE SYMPLECTIC GROUP CONNIE FAN 1. Introduction t ¯ 1.1. Definition. Sp(n)= (n, H)= A Mn(H) A A = I is the symplectic group. O { 2 | } 1.2. Example. Sp(1) = z M1(H) z =1 { 2 || | } = z = a + ib + jc + kd a2 + b2 + c2 + d2 =1 { | } 3 ⇠= S 2. The Lie Algebra sp(n) t ¯ 2.1. Definition. AmatrixA Mn(H)isskew-symplecticif A + A =0. 2 t ¯ 2.2. Definition. sp(n)= A Mn(H) A + A =0 is the Lie algebra of Sp(n) with commutator bracket [A,B]{ 2 = AB -| BA. } Proof. This was proven in class. ⇤ 2.3. Fact. sp(n) is a real vector space. Proof. Let A, B sp(n)anda, b R 2 2 (aA + bB)+taA + bB = a(A + tA¯)+b(B + tB¯)=0 ⇤ 1 2.4. Fact. The dimension of sp(n)is(2n +1)n. Proof. Let A sp(n). 2 a11 + ib11 + jc11 + kd11 a12 + ib12 + jc12 + kd12 ... a1n + ib1n + jc1n + kd1n . A = . .. 0 . 1 an1 + ibn1 + jcn1 + kdn1 an2 + ibn2 + jcn2 + kdn2 ... ann + ibnn + jcnn + kdnn @ A Then A + tA¯ = 2a11 (a12 + a21)+i(b12 b21)+j(c12 c21)+k(d12 d21) ... (a1n + an1)+i(b1n bn1)+j(c1n cn1)+k(d1n dn1) − − − − − − (a21 + a12)+i(b21 b12)+j(c21 c12)+k(d21 d12)2a22 ... (a2n + an2)+i(b2n bn2)+j(c2n cn2)+k(d2n dn2) − − − − − − 0 . 1 . .. B . C B C B(a1n + an1)+i(b1n bn1)+j(c1n cn1)+k(d1n dn1) ... 2ann C @ − − − A t 2 A + A¯ =0,so: axx =0, x 0degreesoffreedom 8 ! n(n 1) − axy = ayx,x= y 2 degrees of freedom − 6 !n(n 1) − bxy = byx,x= y 2 degrees of freedom 6 ! n(n 1) − cxy = cyx,x= y 2 degrees of freedom 6 ! n(n 1) − dxy = dyx,x= y 2 degrees of freedom b ,c ,d unrestricted,6 ! x 3n degrees of freedom xx xx xx 8 ! In total, dim(sp(n)) = 2n2 + n = n(2n +1) ⇤ 2.5. -
The Intersection of Some Classical Equivalence Classes of Matrices Mark Alan Mills Iowa State University
Iowa State University Capstones, Theses and Retrospective Theses and Dissertations Dissertations 1999 The intersection of some classical equivalence classes of matrices Mark Alan Mills Iowa State University Follow this and additional works at: https://lib.dr.iastate.edu/rtd Part of the Mathematics Commons Recommended Citation Mills, Mark Alan, "The intersection of some classical equivalence classes of matrices " (1999). Retrospective Theses and Dissertations. 12153. https://lib.dr.iastate.edu/rtd/12153 This Dissertation is brought to you for free and open access by the Iowa State University Capstones, Theses and Dissertations at Iowa State University Digital Repository. It has been accepted for inclusion in Retrospective Theses and Dissertations by an authorized administrator of Iowa State University Digital Repository. For more information, please contact [email protected]. INFORMATION TO USERS This manuscript has been reproduced from the microfilm master. UMI films the text directly fi'om the original or copy submitted. Thus, some thesis and dissertation copies are in typewriter face, while others may be from any type of computer printer. The quality of this reproduction is dependent upon the quality of the copy submitted. Broken or indistinct print, colored or poor quality illustrations and photographs, print bleedthrough, substandard margins, and improper alignment can adversely affect reproduction. In the unlikely event that the author did not send UMI a complete manuscript and there are missing pages, these will be noted. Also, if unauthorized copyright material had to be removed, a note will indicate the deletion. Oversize materials (e.g., maps, drawings, charts) are reproduced by sectioning the original, beginning at the upper left-hand comer and continuing firom left to right in equal sections with small overlaps. -
Differential Topology: Exercise Sheet 3
Prof. Dr. M. Wolf WS 2018/19 M. Heinze Sheet 3 Differential Topology: Exercise Sheet 3 Exercises (for Nov. 21th and 22th) 3.1 Smooth maps Prove the following: (a) A map f : M ! N between smooth manifolds (M; A); (N; B) is smooth if and only if for all x 2 M there are pairs (U; φ) 2 A; (V; ) 2 B such that x 2 U, f(U) ⊂ V and ◦ f ◦ φ−1 : φ(U) ! (V ) is smooth. (b) Compositions of smooth maps between subsets of smooth manifolds are smooth. Solution: (a) As the charts of a smooth structure cover the manifold the above property is certainly necessary for smoothness of f : M ! N. To show that it is also sufficient, consider two arbitrary charts U;~ φ~ 2 A and V;~ ~ 2 B. We need to prove that the map ~ ◦ f ◦ φ~−1 : φ~(U~) ! ~(V~ ) is smooth. Therefore consider an arbitrary y 2 φ~(U~) such that there is some x 2 M such that x = φ~−1(y). By assumption there are charts (U; φ) 2 A; (V; ) 2 B such that x 2 U, −1 f(U) ⊂ V and ◦ f ◦ φ : φ(U) ! (V ) is smooth. Now we choose U0;V0 such ~ ~ that x 2 U0 ⊂ U \ U and f(x) 2 V0 ⊂ V \ V and therefore we can write ~ ~−1 ~ −1 −1 ~−1 ◦ f ◦ φ j = ◦ ◦ ◦ f ◦ φ ◦ φ ◦ φ : (1) φ~(U0) As a composition of smooth maps, we showed that ~ ◦ f ◦ φ~−1j is smooth. As φ~(U0) x 2 M was chosen arbitrarily we proved that ~ ◦ f ◦ φ~−1 is a smooth map. -
A Review of Matrix Scaling and Sinkhorn's Normal Form for Matrices
A review of matrix scaling and Sinkhorn’s normal form for matrices and positive maps Martin Idel∗ Zentrum Mathematik, M5, Technische Universität München, 85748 Garching Abstract Given a nonnegative matrix A, can you find diagonal matrices D1, D2 such that D1 AD2 is doubly stochastic? The answer to this question is known as Sinkhorn’s theorem. It has been proved with a wide variety of methods, each presenting a variety of possible generalisations. Recently, generalisations such as to positive maps between matrix algebras have become more and more interesting for applications. This text gives a review of over 70 years of matrix scaling. The focus lies on the mathematical landscape surrounding the problem and its solution as well as the generalisation to positive maps and contains hardly any nontrivial unpublished results. Contents 1. Introduction3 2. Notation and Preliminaries4 3. Different approaches to equivalence scaling5 3.1. Historical remarks . .6 3.2. The logarithmic barrier function . .8 3.3. Nonlinear Perron-Frobenius theory . 12 3.4. Entropy optimisation . 14 3.5. Convex programming and dual problems . 17 3.6. Topological (non-constructive) approaches . 20 arXiv:1609.06349v1 [math.RA] 20 Sep 2016 3.7. Other ideas . 21 3.7.1. Geometric proofs . 22 3.7.2. Other direct convergence proofs . 23 ∗[email protected] 1 4. Equivalence scaling 24 5. Other scalings 27 5.1. Matrix balancing . 27 5.2. DAD scaling . 29 5.3. Matrix Apportionment . 33 5.4. More general matrix scalings . 33 6. Generalised approaches 35 6.1. Direct multidimensional scaling . 35 6.2. Log-linear models and matrices as vectors . -
Math 623: Matrix Analysis Final Exam Preparation
Mike O'Sullivan Department of Mathematics San Diego State University Spring 2013 Math 623: Matrix Analysis Final Exam Preparation The final exam has two parts, which I intend to each take one hour. Part one is on the material covered since the last exam: Determinants; normal, Hermitian and positive definite matrices; positive matrices and Perron's theorem. The problems will all be very similar to the ones in my notes, or in the accompanying list. For part two, you will write an essay on what I see as the fundamental theme of the course, the four equivalence relations on matrices: matrix equivalence, similarity, unitary equivalence and unitary similarity (See p. 41 in Horn 2nd Ed. He calls matrix equivalence simply \equivalence."). Imagine you are writing for a fellow master's student. Your goal is to explain to them the key ideas. Matrix equivalence: (1) Define it. (2) Explain the relationship with abstract linear transformations and change of basis. (3) We found a simple set of representatives for the equivalence classes: identify them and sketch the proof. Similarity: (1) Define it. (2) Explain the relationship with abstract linear transformations and change of basis. (3) We found a set of representatives for the equivalence classes using Jordan matrices. State the Jordan theorem. (4) The proof of the Jordan theorem can be broken into two parts: (1) writing the ambient space as a direct sum of generalized eigenspaces, (2) classifying nilpotent matrices. Sketch the proof of each. Explain the role of invariant spaces. Unitary equivalence (1) Define it. (2) Explain the relationship with abstract inner product spaces and change of basis. -
Hamiltonian and Symplectic Symmetries: an Introduction
BULLETIN (New Series) OF THE AMERICAN MATHEMATICAL SOCIETY Volume 54, Number 3, July 2017, Pages 383–436 http://dx.doi.org/10.1090/bull/1572 Article electronically published on March 6, 2017 HAMILTONIAN AND SYMPLECTIC SYMMETRIES: AN INTRODUCTION ALVARO´ PELAYO In memory of Professor J.J. Duistermaat (1942–2010) Abstract. Classical mechanical systems are modeled by a symplectic mani- fold (M,ω), and their symmetries are encoded in the action of a Lie group G on M by diffeomorphisms which preserve ω. These actions, which are called sym- plectic, have been studied in the past forty years, following the works of Atiyah, Delzant, Duistermaat, Guillemin, Heckman, Kostant, Souriau, and Sternberg in the 1970s and 1980s on symplectic actions of compact Abelian Lie groups that are, in addition, of Hamiltonian type, i.e., they also satisfy Hamilton’s equations. Since then a number of connections with combinatorics, finite- dimensional integrable Hamiltonian systems, more general symplectic actions, and topology have flourished. In this paper we review classical and recent re- sults on Hamiltonian and non-Hamiltonian symplectic group actions roughly starting from the results of these authors. This paper also serves as a quick introduction to the basics of symplectic geometry. 1. Introduction Symplectic geometry is concerned with the study of a notion of signed area, rather than length, distance, or volume. It can be, as we will see, less intuitive than Euclidean or metric geometry and it is taking mathematicians many years to understand its intricacies (which is work in progress). The word “symplectic” goes back to the 1946 book [164] by Hermann Weyl (1885–1955) on classical groups. -
Symplectic Group and Heisenberg Group in P-Adic Quantum Mechanics
SYMPLECTIC GROUP AND HEISENBERG GROUP IN p-ADIC QUANTUM MECHANICS SEN HU & ZHI HU ABSTRACT. This paper treats mathematically some problems in p-adic quantum mechanics. We first deal with p-adic symplectic group corresponding to the symmetry on the classical phase space. By the filtrations of isotropic subspaces and almost self-dual lattices in the p-adic symplectic vector space, we explicitly give the expressions of parabolic subgroups, maximal compact subgroups and corresponding Iwasawa decompositions of some symplectic groups. For a triple of Lagrangian subspaces, we associated it with a quadratic form whose Hasse invariant is calculated. Next we study the various equivalent realizations of unique irreducible and admissible representation of p-adic Heisenberg group. For the Schrödinger representation, we can define Weyl operator and its kernel function, while for the induced representations from the characters of maximal abelian subgroups of Heisenberg group generated by the isotropic subspaces or self-dual lattice in the p-adic symplectic vector space, we calculate the Maslov index defined via the intertwining operators corresponding to the representation transformation operators in quantum mechanics. CONTENTS 1. Introduction 1 2. Brief Review of p-adic Analysis 2 3. p-adic Symplectic Group 3 3.1. Isotropic subspaces and parabolic subgroups 3 3.2. Lagrangian subspaces and quadratic forms 4 3.3. Latices and maximal compact subgroups 6 4. p-adic Heisenberg Group 8 4.1. Schrödinger representations and Weyl operators 8 4.2. Induced representations and Maslov indices 11 References 14 1. INTRODUCTION It seems that there is no prior reason for opposing the fascinating idea that at the very small (Planck) scale the geometry of the spacetime should be non-Archimedean.