Norms of Zonal Spherical Functions and Fourier Series on Compact Symmetric Spaces
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On the Stability of a Class of Functional Equations
Journal of Inequalities in Pure and Applied Mathematics ON THE STABILITY OF A CLASS OF FUNCTIONAL EQUATIONS volume 4, issue 5, article 104, BELAID BOUIKHALENE 2003. Département de Mathématiques et Informatique Received 20 July, 2003; Faculté des Sciences BP 133, accepted 24 October, 2003. 14000 Kénitra, Morocco. Communicated by: K. Nikodem EMail: [email protected] Abstract Contents JJ II J I Home Page Go Back Close c 2000 Victoria University ISSN (electronic): 1443-5756 Quit 098-03 Abstract In this paper, we study the Baker’s superstability for the following functional equation Z X −1 (E (K)) f(xkϕ(y)k )dωK (k) = |Φ|f(x)f(y), x, y ∈ G ϕ∈Φ K where G is a locally compact group, K is a compact subgroup of G, ωK is the normalized Haar measure of K, Φ is a finite group of K-invariant morphisms of On the Stability of A Class of G and f is a continuous complex-valued function on G satisfying the Kannap- Functional Equations pan type condition, for all x, y, z ∈ G Belaid Bouikhalene Z Z Z Z −1 −1 −1 −1 (*) f(zkxk hyh )dωK (k)dωK (h)= f(zkyk hxh )dωK (k)dωK (h). K K K K Title Page We treat examples and give some applications. Contents 2000 Mathematics Subject Classification: 39B72. Key words: Functional equation, Stability, Superstability, Central function, Gelfand JJ II pairs. The author would like to greatly thank the referee for his helpful comments and re- J I marks. Go Back Contents Close 1 Introduction, Notations and Preliminaries ............... -
Arxiv:1902.09497V5 [Math.DS]
GELFAND PAIRS ADMIT AN IWASAWA DECOMPOSITION NICOLAS MONOD Abstract. Every Gelfand pair (G,K) admits a decomposition G = KP , where P<G is an amenable subgroup. In particular, the Furstenberg boundary of G is homogeneous. Applications include the complete classification of non-positively curved Gelfand pairs, relying on earlier joint work with Caprace, as well as a canonical family of pure spherical functions in the sense of Gelfand–Godement for general Gelfand pairs. Let G be a locally compact group. The space M b(G) of bounded measures on G is an algebra for convolution, which is simply the push-forward of the multiplication map G × G → G. Definition. Let K<G be a compact subgroup. The pair (G,K) is a Gelfand pair if the algebra M b(G)K,K of bi-K-invariant measures is commutative. This definition, rooted in Gelfand’s 1950 work [14], is often given in terms of algebras of func- tions [12]. This is equivalent, by an approximation argument in the narrow topology, but has the inelegance of requiring the choice (and existence) of a Haar measure on G. Examples of Gelfand pairs include notably all connected semi-simple Lie groups G with finite center, where K is a maximal compact subgroup. Other examples are provided by their analogues over local fields [18], and non-linear examples include automorphism groups of trees [23],[2]. All these “classical” examples also have in common another very useful property: they admit a co-compact amenable subgroup P<G. In the semi-simple case, P is a minimal parabolic subgroup. -
Q-KRAWTCHOUK POLYNOMIALS AS SPHERICAL FUNCTIONS on the HECKE ALGEBRA of TYPE B
TRANSACTIONS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 352, Number 10, Pages 4789{4813 S 0002-9947(00)02588-5 Article electronically published on April 21, 2000 q-KRAWTCHOUK POLYNOMIALS AS SPHERICAL FUNCTIONS ON THE HECKE ALGEBRA OF TYPE B H. T. KOELINK Abstract. The Hecke algebra for the hyperoctahedral group contains the Hecke algebra for the symmetric group as a subalgebra. Inducing the index representation of the subalgebra gives a Hecke algebra module, which splits multiplicity free. The corresponding zonal spherical functions are calculated in terms of q-Krawtchouk polynomials using the quantised enveloping algebra for sl(2; C). The result covers a number of previously established interpretations of (q-)Krawtchouk polynomials on the hyperoctahedral group, finite groups of Lie type, hypergroups and the quantum SU(2) group. 1. Introduction The hyperoctahedral group is the finite group of signed permutations, and it con- tains the permutation group as a subgroup. The functions on the hyperoctahedral group, which are left and right invariant with respect to the permutation group, are spherical functions. The zonal spherical functions are the spherical functions which are contained in an irreducible subrepresentation of the group algebra under the left regular representation. The zonal spherical functions are known in terms of finite discrete orthogonal polynomials, the so-called symmetric Krawtchouk poly- nomials. This result goes back to Vere-Jones in the beginning of the seventies, and is also contained in the work of Delsarte on coding theory; see [9] for information and references. There are also group theoretic interpretations of q-Krawtchouk polynomials. Here q-Krawtchouk polynomials are q-analogues of the Krawtchouk polynomials in the sense that for q tending to one we recover the Krawtchouk polynomials. -
A Localization Argument for Characters of Reductive Lie Groups: an Introduction and Examples Matvei Libine
This is page 375 Printer: Opaque this A localization argument for characters of reductive Lie groups: an introduction and examples Matvei Libine In Honor of Jacques Carmona ABSTRACT In this article I describe my recent geometric localization argument dealing with actions of noncompact groups which provides a geometric bridge between two entirely different character formulas for reductive Lie groups and answers the question posed in [Sch]. A corresponding problem in the compact group setting was solved by N. Berline, E. Getzler and M. Vergne in [BGV] by an application of the theory of equivariant forms and, particularly, the fixed point integral localization formula. This localization argument seems to be the first successful attempt in the direction of build- ing a similar theory for integrals of differential forms, equivariant with respect to actions of noncompact groups. I will explain how the argument works in the SL(2, R) case, where the key ideas are not obstructed by technical details and where it becomes clear how it extends to the general case. The general argument appears in [L]. Ihavemade every effort to present this article so that it is widely accessible. Also, although characteristic cycles of sheaves is mentioned, I do not assume that the reader is familiar with this notion. 1 Introduction For motivation, let us start with the case of a compact group. Thus we consider a connected compact group K and a maximal torus T ⊂ K . Let kR and tR denote the Lie algebras of K and T respectively, and k, t be their complexified Lie algebras. Let π be a finite-dimensional representation of K , that is π is a group homomorphism K → Aut(V ). -
NOTES on the WEYL CHARACTER FORMULA the Aim of These Notes
NOTES ON THE WEYL CHARACTER FORMULA The aim of these notes is to give a self-contained algebraic proof of the Weyl Character Formula. The necessary background results on modules for sl2(C) and complex semisimple Lie algebras are outlined in the first two sections. Some technical details are left to the exercises at the end; solutions are provided when the exercise is needed for the proof. 1. Representations of sl2(C) Define ! ! ! 1 0 0 1 0 0 h = ; e = ; f = 0 −1 0 0 1 0 2 and note that hh; e; fi = sl2(C). Let u; v be the canonical basis of E = C . Then each Symd E is irreducible with ud spanning the highest-weight space d of weight d and, up to isomorphism, Sym E is the unique irreducible sl2(C)- module with highest weight d. (See Exercises 1.1 and 1.2.) The diagram below shows the actions of h, e and f on the canonical basis of Symd E: loops show the action of h, arrows to the right show the action of e, arrow to the left show the action of f. d−2c−2 d−2c d−2c+2 d−c+1 d−c d−c−1 i • j * • j * • ) c−1 ud−c−1vc+1 c ud−cvc c+1 ud−c+1vc−1 In particular (a) the eigenvalues of h on Symd E are −d; −d + 2; : : : ; d − 2; d and each h-eigenspace is 1-dimensional, (b) if w 2 Symd E and h · w = (d − 2c)w then f · e · w = c(d − c + 1)w. -
Kobe University Repository : Kernel
Kobe University Repository : Kernel タイトル Zonal spherical functions on the quantum homogeneous space Title SUq(n+1)/SUq(n) 著者 Noumi, Masatoshi / Yamada, Hirofumi / Mimachi, Katsuhisa Author(s) 掲載誌・巻号・ページ Proceedings of the Japan Academy. Ser. A, Mathematical Citation sciences,65(6):169-171 刊行日 1989-06 Issue date 資源タイプ Journal Article / 学術雑誌論文 Resource Type 版区分 publisher Resource Version 権利 Rights DOI 10.3792/pjaa.65.169 JaLCDOI URL http://www.lib.kobe-u.ac.jp/handle_kernel/90003238 PDF issue: 2021-10-01 No. 6] Proc. Japan Acad., 65, Ser. A (1989) 169 Zonal Spherical Functions on the Quantum Homogeneous Space SU (n + 1 )/SU (n) By Masatoshi NOUMI,*) Hirofumi YAMADA,**) and Katsuhisa :M:IMACHI***) (Communicated by Shokichi IYANA,GA, M. ff.A., June. 13, 1989) In this note, we give an explicit expression to the zonal spherical func- tions on the quantum homogeneous space SU(n + 1)/SU(n). Details of the following arguments as well as the representation theory of the quantum group SU(n+ 1) will be presented in our forthcoming paper [3]. Through- out this note, we fix a non-zero real number q. 1. Following [4], we first make a brief review on the definition of the quantum groups SLy(n+ 1; C) and its real form SUb(n+ 1). The coordinate ring A(SL,(n+ 1; C)) of SLy(n+ 1; C) is the C-algebra A=C[x,; O_i, ]_n] defined by the "canonical generators" x, (Oi, ]n) and the following fundamental relations" (1.1) xixj=qxx, xixj=qxx or O_i]_n, O_k_n, (1.2) xx=xxt, xx--qxxj=xtx--q-lxx or Oi]_n, Okl_n and (1.3) det-- 1. -
Arxiv:Math/9512225V1
SOME REMARKS ON THE CONSTRUCTION OF QUANTUM SYMMETRIC SPACES Mathijs S. Dijkhuizen Department of Mathematics, Faculty of Science, Kobe University, Rokko, Kobe 657, Japan 31 May 1995 Abstract. We present a general survey of some recent developments regarding the construction of compact quantum symmetric spaces and the analysis of their zonal spherical functions in terms of q-orthogonal polynomials. In particular, we define a one-parameter family of two-sided coideals in Uq(gl(n, C)) and express the zonal spherical functions on the corresponding quantum projective spaces as Askey-Wilson polynomials containing two continuous and one discrete parameter. 0. Introduction In this paper, we discuss some recent progress in the analysis of compact quantum symmetric spaces and their zonal spherical functions. It is our aim to present a more or less coherent overview of a number of quantum analogues of symmetric spaces that have recently been studied. We shall try to emphasize those aspects of the theory that distinguish quantum symmetric spaces from their classical counterparts. It was recognized not long after the introduction of quantum groups by Drinfeld [Dr], Jimbo [J1], and Woronowicz [Wo], that the quantization of symmetric spaces was far from straightforward. We discuss some of the main problems that came up. First of all, there was the, at first sight rather annoying, lack of interesting quan- tum subgroups. Let us mention, for instance, the well-known fact that there is no analogue of SO(n) inside the quantum group SUq(n). A major step forward in overcoming this hurdle was made by Koornwinder [K2], who was able to construct a quantum analogue of the classical 2-sphere SU(2)/SO(2) and express the zonal arXiv:math/9512225v1 [math.QA] 21 Dec 1995 spherical functions as a subclass of Askey-Wilson polynomials by exploiting the notion of a twisted primive element in the quantized universal enveloping algebra q(sl(2, C)). -
Noncommutative Fourier Transform for the Lorentz Group Via the Duflo Map
PHYSICAL REVIEW D 99, 106005 (2019) Noncommutative Fourier transform for the Lorentz group via the Duflo map Daniele Oriti Max Planck Institute for Gravitational Physics (Albert Einstein Institute), Am Mühlenberg 1, 14476 Potsdam-Golm, Germany and Arnold-Sommerfeld-Center for Theoretical Physics, Ludwig-Maximilians-Universität, Theresienstrasse 37, D-80333 München, Germany, EU Giacomo Rosati INFN, Sezione di Cagliari, Cittadella Universitaria, 09042 Monserrato, Italy (Received 11 February 2019; published 13 May 2019) We defined a noncommutative algebra representation for quantum systems whose phase space is the cotangent bundle of the Lorentz group, and the noncommutative Fourier transform ensuring the unitary equivalence with the standard group representation. Our construction is from first principles in the sense that all structures are derived from the choice of quantization map for the classical system, the Duflo quantization map. DOI: 10.1103/PhysRevD.99.106005 I. INTRODUCTION of (noncommutative) Fourier transform to establish the (unitary) equivalence between this new representation and Physical systems whose configuration or phase space is the one based on L2 functions on the group configura- endowed with a curved geometry include, for example, tion space. point particles on curved spacetimes and rotor models in The standard way of dealing with this issue is indeed to condensed matter theory, and they present specific math- renounce to a representation that makes direct use ematical challenges in addition to their physical interest. of the noncommutative Lie algebra variables, and to use In particular, many important results have been obtained in instead a representation in terms of irreducible representa- the case in which their domain spaces can be identified tions of the Lie group, i.e., to resort to spectral decom- with (Abelian) group manifolds or their associated homo- position as the proper analogue of the traditional Fourier geneous spaces. -
Title: Algebraic Group Representations, and Related Topics a Lecture by Len Scott, Mcconnell/Bernard Professor of Mathemtics, the University of Virginia
Title: Algebraic group representations, and related topics a lecture by Len Scott, McConnell/Bernard Professor of Mathemtics, The University of Virginia. Abstract: This lecture will survey the theory of algebraic group representations in positive characteristic, with some attention to its historical development, and its relationship to the theory of finite group representations. Other topics of a Lie-theoretic nature will also be discussed in this context, including at least brief mention of characteristic 0 infinite dimensional Lie algebra representations in both the classical and affine cases, quantum groups, perverse sheaves, and rings of differential operators. Much of the focus will be on irreducible representations, but some attention will be given to other classes of indecomposable representations, and there will be some discussion of homological issues, as time permits. CHAPTER VI Linear Algebraic Groups in the 20th Century The interest in linear algebraic groups was revived in the 1940s by C. Chevalley and E. Kolchin. The most salient features of their contributions are outlined in Chapter VII and VIII. Even though they are put there to suit the broader context, I shall as a rule refer to those chapters, rather than repeat their contents. Some of it will be recalled, however, mainly to round out a narrative which will also take into account, more than there, the work of other authors. §1. Linear algebraic groups in characteristic zero. Replicas 1.1. As we saw in Chapter V, §4, Ludwig Maurer thoroughly analyzed the properties of the Lie algebra of a complex linear algebraic group. This was Cheval ey's starting point. -
MAT 449 : Representation Theory
MAT 449 : Representation theory Sophie Morel December 17, 2018 Contents I Representations of topological groups5 I.1 Topological groups . .5 I.2 Haar measures . .9 I.3 Representations . 17 I.3.1 Continuous representations . 17 I.3.2 Unitary representations . 20 I.3.3 Cyclic representations . 24 I.3.4 Schur’s lemma . 25 I.3.5 Finite-dimensional representations . 27 I.4 The convolution product and the group algebra . 28 I.4.1 Convolution on L1(G) and the group algebra of G ............ 28 I.4.2 Representations of G vs representations of L1(G) ............. 33 I.4.3 Convolution on other Lp spaces . 39 II Some Gelfand theory 43 II.1 Banach algebras . 43 II.1.1 Spectrum of an element . 43 II.1.2 The Gelfand-Mazur theorem . 47 II.2 Spectrum of a Banach algebra . 48 II.3 C∗-algebras and the Gelfand-Naimark theorem . 52 II.4 The spectral theorem . 55 III The Gelfand-Raikov theorem 59 III.1 L1(G) ....................................... 59 III.2 Functions of positive type . 59 III.3 Functions of positive type and irreducible representations . 65 III.4 The convex set P1 ................................. 68 III.5 The Gelfand-Raikov theorem . 73 IV The Peter-Weyl theorem 75 IV.1 Compact operators . 75 IV.2 Semisimplicity of unitary representations of compact groups . 77 IV.3 Matrix coefficients . 80 IV.4 The Peter-Weyl theorem . 86 IV.5 Characters . 87 3 Contents IV.6 The Fourier transform . 90 IV.7 Characters and Fourier transforms . 93 V Gelfand pairs 97 V.1 Invariant and bi-invariant functions . -
Arxiv:1810.00775V1 [Math-Ph] 1 Oct 2018 .Introduction 1
Modular structures and extended-modular-group-structures after Hecke pairs Orchidea Maria Lecian Comenius University in Bratislava, Faculty of Mathematics, Physics and Informatics, Department of Theoretical Physics and Physics Education- KTFDF, Mlynsk´aDolina F2, 842 48, Bratislava, Slovakia; Sapienza University of Rome, Faculty of Civil and Industrial Engineering, DICEA- Department of Civil, Constructional and Environmental Engineering, Via Eudossiana, 18- 00184 Rome, Italy. E-mail: [email protected]; [email protected] Abstract. The simplices and the complexes arsing form the grading of the fundamental (desymmetrized) domain of arithmetical groups and non-arithmetical groups, as well as their extended (symmetrized) ones are described also for oriented manifolds in dim > 2. The conditions for the definition of fibers are summarized after Hamiltonian analysis, the latters can in some cases be reduced to those for sections for graded groups, such as the Picard groups and the Vinberg group.The cases for which modular structures rather than modular-group- structure measures can be analyzed for non-arithmetic groups, i.e. also in the cases for which Gelfand triples (rigged spaces) have to be substituted by Hecke couples, as, for Hecke groups, the existence of intertwining operators after the calculation of the second commutator within the Haar measures for the operators of the correspondingly-generated C∗ algebras is straightforward. The results hold also for (also non-abstract) groups with measures on (manifold) boundaries. The Poincar´e invariance of the representation of Wigner-Bargmann (spin 1/2) particles is analyzed within the Fock-space interaction representation. The well-posed-ness of initial conditions and boundary ones for the connected (families of) equations is discussed. -
A Recursive Formula for Characters of Simple Lie Algebras
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Elsevier - Publisher Connector JOURNAL OF ALGEBRA 137, 126-144 (1991) A Recursive Formula for Characters of Simple Lie Algebras STEVEN N. KASS* Centre de recherches mathkmatiques, UniversitP de MontrPal C. P. 6128, &cc. “A”, MontrPal, Qutbec, Canada H3C 357 Communicated by Robert Steinberg Received July 20, 1988; accepted July 18, 1989 In 1964, Antoine and Speiser published succinct and elegant formulae for the characters of the irreducible highest weight modules for the Lie algebras A, and B,. (The result for A, may have been known as early as 1957.) These can be derived from a recursive formula for characters valid for all simple complex Kac-Moody Lie algebras for which the Weyl-Kac character formula holds. 0 1991 Academic Press. Inc. 1. INTRODUCTION To avoid the encumbrance of technicalities, we present the results first for simple finite-dimensional Lie algebras over C. We use the following notation, generally following Humphreys [H]. Let L be a finite-dimensional complex simple Lie algebra of rank 1. We denote by H a Cartan subalgebra of L, by ai (1 Q i < I) a choice of simple roots, by Q the integral lattice they generate, and by R, R+, and R- the root system, positive roots, and negative roots with respect to H and the ai, respectively. Let A be the weight lattice for L, and li (1~ i,< I) the fundamental weights corresponding to the choice of simple roots. The set of dominant weights will be denoted A +.