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Automorphic Forms on GL(2)
Automorphic Forms on GL(2) Herve´ Jacquet and Robert P. Langlands Formerly appeared as volume #114 in the Springer Lecture Notes in Mathematics, 1970, pp. 1-548 Chapter 1 i Table of Contents Introduction ...................................ii Chapter I: Local Theory ..............................1 § 1. Weil representations . 1 § 2. Representations of GL(2,F ) in the non•archimedean case . 12 § 3. The principal series for non•archimedean fields . 46 § 4. Examples of absolutely cuspidal representations . 62 § 5. Representations of GL(2, R) ........................ 77 § 6. Representation of GL(2, C) . 111 § 7. Characters . 121 § 8. Odds and ends . 139 Chapter II: Global Theory ............................152 § 9. The global Hecke algebra . 152 §10. Automorphic forms . 163 §11. Hecke theory . 176 §12. Some extraordinary representations . 203 Chapter III: Quaternion Algebras . 216 §13. Zeta•functions for M(2,F ) . 216 §14. Automorphic forms and quaternion algebras . 239 §15. Some orthogonality relations . 247 §16. An application of the Selberg trace formula . 260 Chapter 1 ii Introduction Two of the best known of Hecke’s achievements are his theory of L•functions with grossen•¨ charakter, which are Dirichlet series which can be represented by Euler products, and his theory of the Euler products, associated to automorphic forms on GL(2). Since a grossencharakter¨ is an automorphic form on GL(1) one is tempted to ask if the Euler products associated to automorphic forms on GL(2) play a role in the theory of numbers similar to that played by the L•functions with grossencharakter.¨ In particular do they bear the same relation to the Artin L•functions associated to two•dimensional representations of a Galois group as the Hecke L•functions bear to the Artin L•functions associated to one•dimensional representations? Although we cannot answer the question definitively one of the principal purposes of these notes is to provide some evidence that the answer is affirmative. -
REPRESENTATION THEORY WEEK 7 1. Characters of GL Kand Sn A
REPRESENTATION THEORY WEEK 7 1. Characters of GLk and Sn A character of an irreducible representation of GLk is a polynomial function con- stant on every conjugacy class. Since the set of diagonalizable matrices is dense in GLk, a character is defined by its values on the subgroup of diagonal matrices in GLk. Thus, one can consider a character as a polynomial function of x1,...,xk. Moreover, a character is a symmetric polynomial of x1,...,xk as the matrices diag (x1,...,xk) and diag xs(1),...,xs(k) are conjugate for any s ∈ Sk. For example, the character of the standard representation in E is equal to x1 + ⊗n n ··· + xk and the character of E is equal to (x1 + ··· + xk) . Let λ = (λ1,...,λk) be such that λ1 ≥ λ2 ≥ ···≥ λk ≥ 0. Let Dλ denote the λj determinant of the k × k-matrix whose i, j entry equals xi . It is clear that Dλ is a skew-symmetric polynomial of x1,...,xk. If ρ = (k − 1,..., 1, 0) then Dρ = i≤j (xi − xj) is the well known Vandermonde determinant. Let Q Dλ+ρ Sλ = . Dρ It is easy to see that Sλ is a symmetric polynomial of x1,...,xk. It is called a Schur λ1 λk polynomial. The leading monomial of Sλ is the x ...xk (if one orders monomials lexicographically) and therefore it is not hard to show that Sλ form a basis in the ring of symmetric polynomials of x1,...,xk. Theorem 1.1. The character of Wλ equals to Sλ. I do not include a proof of this Theorem since it uses beautiful but hard combina- toric. -
Matrix Coefficients and Linearization Formulas for SL(2)
Matrix Coefficients and Linearization Formulas for SL(2) Robert W. Donley, Jr. (Queensborough Community College) November 17, 2017 Robert W. Donley, Jr. (Queensborough CommunityMatrix College) Coefficients and Linearization Formulas for SL(2)November 17, 2017 1 / 43 Goals of Talk 1 Review of last talk 2 Special Functions 3 Matrix Coefficients 4 Physics Background 5 Matrix calculator for cm;n;k (i; j) (Vanishing of cm;n;k (i; j) at certain parameters) Robert W. Donley, Jr. (Queensborough CommunityMatrix College) Coefficients and Linearization Formulas for SL(2)November 17, 2017 2 / 43 References 1 Andrews, Askey, and Roy, Special Functions (big red book) 2 Vilenkin, Special Functions and the Theory of Group Representations (big purple book) 3 Beiser, Concepts of Modern Physics, 4th edition 4 Donley and Kim, "A rational theory of Clebsch-Gordan coefficients,” preprint. Available on arXiv Robert W. Donley, Jr. (Queensborough CommunityMatrix College) Coefficients and Linearization Formulas for SL(2)November 17, 2017 3 / 43 Review of Last Talk X = SL(2; C)=T n ≥ 0 : V (2n) highest weight space for highest weight 2n, dim(V (2n)) = 2n + 1 ∼ X C[SL(2; C)=T ] = V (2n) n2N T X C[SL(2; C)=T ] = C f2n n2N f2n is called a zonal spherical function of type 2n: That is, T · f2n = f2n: Robert W. Donley, Jr. (Queensborough CommunityMatrix College) Coefficients and Linearization Formulas for SL(2)November 17, 2017 4 / 43 Linearization Formula 1) Weight 0 : t · (f2m f2n) = (t · f2m)(t · f2n) = f2m f2n min(m;n) ∼ P 2) f2m f2n 2 V (2m) ⊗ V (2n) = V (2m + 2n − 2k) k=0 (Clebsch-Gordan decomposition) That is, f2m f2n is also spherical and a finite sum of zonal spherical functions. -
An Introduction to Lie Groups and Lie Algebras
This page intentionally left blank CAMBRIDGE STUDIES IN ADVANCED MATHEMATICS 113 EDITORIAL BOARD b. bollobás, w. fulton, a. katok, f. kirwan, p. sarnak, b. simon, b. totaro An Introduction to Lie Groups and Lie Algebras With roots in the nineteenth century, Lie theory has since found many and varied applications in mathematics and mathematical physics, to the point where it is now regarded as a classical branch of mathematics in its own right. This graduate text focuses on the study of semisimple Lie algebras, developing the necessary theory along the way. The material covered ranges from basic definitions of Lie groups, to the theory of root systems, and classification of finite-dimensional representations of semisimple Lie algebras. Written in an informal style, this is a contemporary introduction to the subject which emphasizes the main concepts of the proofs and outlines the necessary technical details, allowing the material to be conveyed concisely. Based on a lecture course given by the author at the State University of New York at Stony Brook, the book includes numerous exercises and worked examples and is ideal for graduate courses on Lie groups and Lie algebras. CAMBRIDGE STUDIES IN ADVANCED MATHEMATICS All the titles listed below can be obtained from good booksellers or from Cambridge University Press. For a complete series listing visit: http://www.cambridge.org/series/ sSeries.asp?code=CSAM Already published 60 M. P. Brodmann & R. Y. Sharp Local cohomology 61 J. D. Dixon et al. Analytic pro-p groups 62 R. Stanley Enumerative combinatorics II 63 R. M. Dudley Uniform central limit theorems 64 J. -
Math.GR] 21 Jul 2017 01-00357
TWISTED BURNSIDE-FROBENIUS THEORY FOR ENDOMORPHISMS OF POLYCYCLIC GROUPS ALEXANDER FEL’SHTYN AND EVGENIJ TROITSKY Abstract. Let R(ϕ) be the number of ϕ-conjugacy (or Reidemeister) classes of an endo- morphism ϕ of a group G. We prove for several classes of groups (including polycyclic) that the number R(ϕ) is equal to the number of fixed points of the induced map of an appropriate subspace of the unitary dual space G, when R(ϕ) < ∞. Applying the result to iterations of ϕ we obtain Gauss congruences for Reidemeister numbers. b In contrast with the case of automorphisms, studied previously, we have a plenty of examples having the above finiteness condition, even among groups with R∞ property. Introduction The Reidemeister number or ϕ-conjugacy number of an endomorphism ϕ of a group G is the number of its Reidemeister or ϕ-conjugacy classes, defined by the equivalence g ∼ xgϕ(x−1). The interest in twisted conjugacy relations has its origins, in particular, in the Nielsen- Reidemeister fixed point theory (see, e.g. [29, 30, 6]), in Arthur-Selberg theory (see, e.g. [42, 1]), Algebraic Geometry (see, e.g. [27]), and Galois cohomology (see, e.g. [41]). In representation theory twisted conjugacy probably occurs first in [23] (see, e.g. [44, 37]). An important problem in the field is to identify the Reidemeister numbers with numbers of fixed points on an appropriate space in a way respecting iterations. This opens possibility of obtaining congruences for Reidemeister numbers and other important information. For the role of the above “appropriate space” typically some versions of unitary dual can be taken. -
Representation Theory
M392C NOTES: REPRESENTATION THEORY ARUN DEBRAY MAY 14, 2017 These notes were taken in UT Austin's M392C (Representation Theory) class in Spring 2017, taught by Sam Gunningham. I live-TEXed them using vim, so there may be typos; please send questions, comments, complaints, and corrections to [email protected]. Thanks to Kartik Chitturi, Adrian Clough, Tom Gannon, Nathan Guermond, Sam Gunningham, Jay Hathaway, and Surya Raghavendran for correcting a few errors. Contents 1. Lie groups and smooth actions: 1/18/172 2. Representation theory of compact groups: 1/20/174 3. Operations on representations: 1/23/176 4. Complete reducibility: 1/25/178 5. Some examples: 1/27/17 10 6. Matrix coefficients and characters: 1/30/17 12 7. The Peter-Weyl theorem: 2/1/17 13 8. Character tables: 2/3/17 15 9. The character theory of SU(2): 2/6/17 17 10. Representation theory of Lie groups: 2/8/17 19 11. Lie algebras: 2/10/17 20 12. The adjoint representations: 2/13/17 22 13. Representations of Lie algebras: 2/15/17 24 14. The representation theory of sl2(C): 2/17/17 25 15. Solvable and nilpotent Lie algebras: 2/20/17 27 16. Semisimple Lie algebras: 2/22/17 29 17. Invariant bilinear forms on Lie algebras: 2/24/17 31 18. Classical Lie groups and Lie algebras: 2/27/17 32 19. Roots and root spaces: 3/1/17 34 20. Properties of roots: 3/3/17 36 21. Root systems: 3/6/17 37 22. Dynkin diagrams: 3/8/17 39 23. -
Schur Orthogonality Relations and Invariant Sesquilinear Forms
PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 130, Number 4, Pages 1211{1219 S 0002-9939(01)06227-X Article electronically published on August 29, 2001 SCHUR ORTHOGONALITY RELATIONS AND INVARIANT SESQUILINEAR FORMS ROBERT W. DONLEY, JR. (Communicated by Rebecca Herb) Abstract. Important connections between the representation theory of a compact group G and L2(G) are summarized by the Schur orthogonality relations. The first part of this work is to generalize these relations to all finite-dimensional representations of a connected semisimple Lie group G: The second part establishes a general framework in the case of unitary representa- tions (π, V ) of a separable locally compact group. The key step is to identify the matrix coefficient space with a dense subset of the Hilbert-Schmidt endo- morphisms on V . 0. Introduction For a connected compact Lie group G, the Peter-Weyl Theorem [PW] provides an explicit decomposition of L2(G) in terms of the representation theory of G.Each irreducible representation occurs in L2(G) with multiplicity equal to its dimension. The set of all irreducible representations are parametrized in the Theorem of the Highest Weight. To convert representations into functions, one forms the set of matrix coefficients. To undo this correspondence, the Schur orthogonality relations express the L2{inner product in terms of the unitary structure of the irreducible representations. 0 Theorem 0.1 (Schur). Fix irreducible unitary representations (π, V π), (π0;Vπ ) of G.Then Z ( 1 h 0ih 0i ∼ 0 0 0 0 u; u v; v if π = π ; hπ(g)u; vihπ (g)u ;v i dg = dπ 0 otherwise, G π 0 0 π0 where u; v are in V ;u;v are in V ;dgis normalized Haar measure, and dπ is the dimension of V π. -
Block Matrices in Linear Algebra
PRIMUS Problems, Resources, and Issues in Mathematics Undergraduate Studies ISSN: 1051-1970 (Print) 1935-4053 (Online) Journal homepage: https://www.tandfonline.com/loi/upri20 Block Matrices in Linear Algebra Stephan Ramon Garcia & Roger A. Horn To cite this article: Stephan Ramon Garcia & Roger A. Horn (2020) Block Matrices in Linear Algebra, PRIMUS, 30:3, 285-306, DOI: 10.1080/10511970.2019.1567214 To link to this article: https://doi.org/10.1080/10511970.2019.1567214 Accepted author version posted online: 05 Feb 2019. Published online: 13 May 2019. Submit your article to this journal Article views: 86 View related articles View Crossmark data Full Terms & Conditions of access and use can be found at https://www.tandfonline.com/action/journalInformation?journalCode=upri20 PRIMUS, 30(3): 285–306, 2020 Copyright # Taylor & Francis Group, LLC ISSN: 1051-1970 print / 1935-4053 online DOI: 10.1080/10511970.2019.1567214 Block Matrices in Linear Algebra Stephan Ramon Garcia and Roger A. Horn Abstract: Linear algebra is best done with block matrices. As evidence in sup- port of this thesis, we present numerous examples suitable for classroom presentation. Keywords: Matrix, matrix multiplication, block matrix, Kronecker product, rank, eigenvalues 1. INTRODUCTION This paper is addressed to instructors of a first course in linear algebra, who need not be specialists in the field. We aim to convince the reader that linear algebra is best done with block matrices. In particular, flexible thinking about the process of matrix multiplication can reveal concise proofs of important theorems and expose new results. Viewing linear algebra from a block-matrix perspective gives an instructor access to use- ful techniques, exercises, and examples. -
UNIVERSALLY OPTIMAL MATRICES and FIELD INDEPENDENCE of the MINIMUM RANK of a GRAPH 1. Introduction. the Minimum Rank Problem Is
Electronic Journal of Linear Algebra ISSN 1081-3810 A publication of the International Linear Algebra Society Volume 18, pp. 403-419, July 2009 ELA http://math.technion.ac.il/iic/ela UNIVERSALLY OPTIMAL MATRICES AND FIELD INDEPENDENCE OF THE MINIMUM RANK OF A GRAPH∗ LUZ M. DEALBA†, JASON GROUT‡,LESLIEHOGBEN§, RANA MIKKELSON‡, AND KAELA RASMUSSEN‡ Abstract. The minimum rank of a simple graph G over a field F is the smallest possible rank among all symmetric matrices over F whose (i, j)th entry (for i = j) isnonzero whenever {i, j} isan edge in G and is zero otherwise. A universally optimal matrix is defined to be an integer matrix A such that every off-diagonal entry of A is0, 1, or −1, and for all fields F , the rank of A isthe minimum rank over F of its graph. Universally optimal matrices are used to establish field independence of minimum rank for numerousgraphs. Examplesare alsoprovided verifying lack of field independence for other graphs. Key words. Minimum rank, Universally optimal matrix, Field independent, Symmetric matrix, Rank, Graph, Matrix. AMS subject classifications. 05C50, 15A03. 1. Introduction. The minimum rank problem is, for a given graph G and field F , to determine the smallest possible rank among symmetric matrices over F whose off-diagonal pattern of zero-nonzero entries is described by G. Most work on minimum rank has been on the real minimum rank problem. See [10] for a survey of known results and discussion of the motivation for the minimum rank problem; an extensive bibliography is also provided there. Catalogs of minimum rank and other parameters for families of graphs [15] and small graphs [16] were developed at the AIM workshop “Spectra of families of matrices described by graphs, digraphs, and sign patterns” [2] and are available on-line; these catalogs are updated routinely. -
Visualizing Finite Field of Order P 2 Through Matrices
Global Journal of Science Frontier Research: F Mathematics and Decision Sciences Volume 16 Issue 1 Version 1.0 Year 2016 Type : Double Blind Peer Reviewed International Research Journal Publisher: Global Journals Inc. (USA) Online ISSN: 2249 -4626 & Print ISSN: 0975-5896 Visualizing Finite Field of Order p2 through Matrices By S. K. Pandey Sardar Patel University of Police, India Abstract- In this article we consider finite field of order p2 (p ≠ 2). We provide matrix representation of finite field of order at most p2 = 121. However this article provides a technique to yield matrix field of order p2 for every prime p > 2 . Keywords: finite field, matrix field, Galois field. GJSFR-F Classification : MSC 2010: 12E20 VisualizingFiniteFieldofOrderp2throughMatrices Strictly as per the compliance and regulations of : © 2016. S. K. Pandey. This is a research/review paper, distributed under the terms of the Creative Commons Attribution- Noncommercial 3.0 Unported License http://creativecommons.org/licenses/by-nc/3.0/), permitting all non commercial use, distribution, and reproduction in any medium, provided the original work is properly cited. Ref Visualizing Finite Field of Order p2 through Matrices 2016 r ea Y S. K. Pandey 271 Abstract- In this article we consider finite field of order 2 (pp ≠ 2). We provide matrix representation of finite field of order at most p2 =121 . However this article provides a technique to yield matrix field of order p2 for every prime p > 2 . V I Keywords: finite field, matrix field, Galois field. ue ersion I s s MSCS2010: 12E20. I I. Intro duction XVI There is a finite field of order pn for every positive prime p and positive integer n . -
Matrix Theory States Ecd Eef = X (D = (3) E)Ecf
Tensor spaces { the basics S. Gill Williamson Abstract We present the basic concepts of tensor products of vectors spaces, ex- ploiting the special properties of vector spaces as opposed to more gen- eral modules. Introduction (1), Basic multilinear algebra (2), Tensor products of vector spaces (3), Tensor products of matrices (4), Inner products on tensor spaces (5), Direct sums and tensor products (6), Background concepts and notation (7), Discussion and acknowledge- ments (8). This material draws upon [Mar73] and relates to subsequent work [Mar75]. 1. Introduction a We start with an example. Let x = ( b ) 2 M2;1 and y = ( c d ) 2 M1;2 where Mm;n denotes the m × n matrices over the real numbers, R. The set of matrices Mm;n forms a vector space under matrix addition and multiplication by real numbers, R. The dimension of this vector space is mn. We write dim(Mm;n) = mn: arXiv:1510.02428v1 [math.AC] 8 Oct 2015 ac ad Define a function ν(x; y) = xy = bc bd 2 M2;2 (matrix product of x and y). The function ν has domain V1 × V2 where V1 = M2;1 and V2 = M1;2 are vector spaces of dimension, dim(Vi) = 2, i = 1; 2. The range of ν is the vector space P = M2;2 which has dim(P ) = 4: The function ν is bilinear in the following sense: (1.1) ν(r1x1 + r2x2; y) = r1ν(x1; y) + r2ν(x2; y) (1.2) ν(x; r1y1 + r2y2) = r1ν(x; y1) + r2ν(x; y2) for any r1; r2 2 R; x; x1; x2 2 V1; and y; y1; y2 2 V2: We denote the set of all such bilinear functions by M(V1;V2 : P ). -
Matrices, Jordan Normal Forms, and Spectral Radius Theory∗
Matrices, Jordan Normal Forms, and Spectral Radius Theory∗ René Thiemann and Akihisa Yamada February 23, 2021 Abstract Matrix interpretations are useful as measure functions in termina- tion proving. In order to use these interpretations also for complexity analysis, the growth rate of matrix powers has to examined. Here, we formalized an important result of spectral radius theory, namely that the growth rate is polynomially bounded if and only if the spectral radius of a matrix is at most one. To formally prove this result we first studied the growth rates of matrices in Jordan normal form, and prove the result that every com- plex matrix has a Jordan normal form by means of two algorithms: we first convert matrices into similar ones via Schur decomposition, and then apply a second algorithm which converts an upper-triangular matrix into Jordan normal form. We further showed uniqueness of Jordan normal forms which then gives rise to a modular algorithm to compute individual blocks of a Jordan normal form. The whole development is based on a new abstract type for matri- ces, which is also executable by a suitable setup of the code generator. It completely subsumes our former AFP-entry on executable matri- ces [6], and its main advantage is its close connection to the HMA- representation which allowed us to easily adapt existing proofs on de- terminants. All the results have been applied to improve CeTA [7, 1], our certifier to validate termination and complexity proof certificates. Contents 1 Introduction 4 2 Missing Ring 5 3 Missing Permutations 9 3.1 Instantiations ..........................