Matrix Valued Orthogonal Polynomials Related to Compact Gel'fand Pairs of Rank

Total Page:16

File Type:pdf, Size:1020Kb

Matrix Valued Orthogonal Polynomials Related to Compact Gel'fand Pairs of Rank Matrix valued orthogonal polynomials related to compact Gel'fand pairs of rank one ISBN 978-94-6191-511-5 NUR 921 c 2012 by M.L.A. van Pruijssen. All rights reserved. Matrix valued orthogonal polynomials related to compact Gel'fand pairs of rank one Proefschrift ter verkrijging van de graad van doctor aan de Radboud Universiteit Nijmegen op gezag van de rector magnificus prof. mr. S.C.J.J. Kortmann, volgens besluit van het college van decanen in het openbaar te verdedigen op woensdag 19 december 2012 om 10.30 uur precies door Maarten Leonardus Antonius van Pruijssen geboren op 4 juni 1979 te Oosterhout Promotoren: prof. dr. G.J. Heckman prof. dr. H.T. Koelink Copromotor: dr. P. Rom´an Universidad Nacional de C´ordoba Manuscriptcommissie: prof. dr. M. Brion Universit´ede Grenoble 1 prof. dr. F.A. Gr¨unbaum University of California, Berkeley prof. dr. T.H. Koornwinder Universiteit van Amsterdam prof. dr. N.P. Landsman prof. dr. P.-E. Paradan Universit´eMontpellier 2 Contents 1 Introduction 1 1.1 Orthogonal polynomials . .1 1.2 Realization as matrix coefficients . .4 1.3 The spectral problem . .6 1.4 The general construction in a nutshell . 10 1.5 Applications and further studies . 11 1.6 This dissertation . 12 I The General Framework 15 2 Multiplicity Free Systems 17 2.1 Introduction . 17 2.2 Multiplicity free systems . 21 2.3 Inverting the branching rule . 31 2.4 Module structure . 51 3 Matrix Valued Polynomials 57 3.1 Introduction . 57 3.2 Multiplicity free triples . 58 3.3 Spherical functions . 60 3.3.1 Spherical functions and representations . 60 3.3.2 Recurrence relations for the spherical functions . 63 3.3.3 The space of spherical functions . 65 3.4 Spherical functions restricted to A ...................... 67 3.4.1 Transformation behavior . 67 3.4.2 Orthogonality and recurrence relations . 68 3.4.3 Differential operators . 71 3.5 Spherical polynomials . 74 3.5.1 Spherical polynomials on G ...................... 74 3.5.2 Spherical polynomials restricted to A ................. 76 v Contents 3.6 Full spherical polynomials . 78 3.6.1 Construction . 78 3.6.2 Properties . 78 3.6.3 Comparison to other constructions . 80 II The Example (SU(2) × SU(2); diag) 83 4 MVOPs related to (SU(2) × SU(2); diag), I 85 4.1 Introduction . 85 4.2 Spherical Functions of the pair (SU(2) × SU(2); diag) . 87 4.3 Recurrence Relation for the Spherical Functions . 90 4.4 Restricted Spherical Functions . 94 4.5 The Weight Matrix . 97 4.6 MVOPs associated to (SU(2) × SU(2); diag) . 102 4.6.1 Matrix valued orthogonal polynomials . 102 4.6.2 Polynomials associated to SU(2) × SU(2) . 104 4.6.3 Symmetries of the weight and the matrix polynomials . 104 4.7 Matrix Valued Differential Operators . 107 4.7.1 Symmetric differential operators . 107 4.7.2 Matrix valued differential operators for the polynomials Pn .... 108 4.8 Examples . 112 4.8.1 The case ` = 0; the scalar weight . 112 1 4.8.2 The case ` = 2 ; weight of dimension 2 . 113 4.8.3 Case ` = 1; weight of dimension 3 . 114 4.8.4 Case ` = 3=2; weight of dimension 4 . 118 4.8.5 Case ` = 2; weight of dimension 5 . 120 4.A Transformation formulas . 122 4.B Proof of the symmetry for differential operators . 126 5 MVOPs related to (SU(2) × SU(2); diag), II 131 5.1 Introduction . 131 5.2 LDU-decomposition of the weight . 135 5.3 MVOP as eigenfunctions of DO . 139 5.4 MVOP as MVHGF . 141 5.5 Three-term recurrence relation . 145 5.6 MVOP related to Gegenbauer and Racah . 149 5.7 Group theoretic interpretation . 156 5.7.1 Group theoretic setting of the MVOPs . 156 5.7.2 Calculation of the Casimir operators . 159 5.A Proof of Theorem 5.2.1 . 165 5.B Moments . 168 vi Contents Bibliography 169 Index 177 Samenvatting 179 Dankwoord 181 Curriculum Vitae 183 vii Chapter 1 Introduction In this dissertation we present a construction of matrix valued polynomials in one vari- able, with special properties, out of matrix coefficients on certain compact groups. The construction generalizes the theory that relates Jacobi polynomials to certain matrix co- efficients on compact groups. In the present chapter we motivate the research in this dissertation and we give an outline of the results. To this end, we discuss in Sections 1.1 and 1.2 the notion of matrix valued orthogonal polynomials and how their simplest examples, the scalar valued orthogonal polynomials, are related to matrix coefficients on compact Lie groups. Once the definitions and notations are fixed we can formulate the research goal. In Section 1.3 we discuss a spectral problem in the theory of Lie groups. In Section 1.4 we indicate that for the solutions of the spectral problem there is a general framework of certain functions, whose structure is determined by a family of matrix valued orthogonal polynomials. In Section 1.5 we discuss the use of this construction and some of the open questions. We close this chapter with an overview of the contents of the various chapters in Section 1.6. 1.1 Orthogonal polynomials 1.1.1. Let I = (a; b) ⊂ R be an interval, possibly unbounded. Let w : I ! R be a non- R negative integrable function satisfying I w(x)dx > 0, where dx is the Lebesgue measure R n and suppose that the moments are finite, i.e. I jx jw(x)dx < 1 for all n 2 N. Define the inner product h·; ·iw on the space of complex valued continuous functions on I by Z hf; hiw = f(x)h(x)w(x)dx: I A sequence of orthogonal polynomials on I with respect to h·; ·iw is a sequence fpd : d 2 Ng with pd(x) 2 C[x] of degree d satisfying hpd; pd0 iw = cdδd;d0 , with cd 2 R a positive number. A family of orthogonal polynomials satisfies a three term recurrence relation, i.e. there 1 Chapter 1. Introduction are sequences of complex numbers fad : d 2 Ng; fbd : d 2 Ng and fcd : d 2 Ng with the ad 6= 0 for which the functional equation xpd(x) = adpd+1(x) + bdpd(x) + cdpd−1(x) (1.1) holds on I. Conversely, given a three term recurrence relation (1.1) one can construct a sequence of polynomials fpd(x): d 2 Ng. Favard's theorem gives sufficient conditions on the coefficients ad; bd and cd to guarantee the existence of a positive Borel measure µ so that fpd(x): d 2 Ng is a sequence of orthogonal polynomials with respect to µ. See e.g. [Chi78] for an introduction to the theory of orthogonal polynomials. The classical orthogonal polynomials of Hermite, Laguerre and Jacobi are also eigen- functions of a second order differential operator that is symmetric with respect to h·; ·iw and Bochner showed that this additional property characterizes them among all the fam- ilies of orthogonal polynomials. 1.1.2. Among the generalizations of the theory of orthogonal polynomials is the theory of matrix valued orthogonal polynomials in one variable. Matrix valued polynomials are elements in C[x] ⊗ End(V ) where V is a finite dimensional complex vector space. The space C[x] ⊗ End(V ) is a bimodule over the matrix algebra End(V ). The Hermitian adjoint of A 2 End(V ) is denoted by A∗. Let I = (a; b) ⊂ R be an interval, possibly unbounded. A matrix weight W on I is an End(V )-valued function for which all its matrix entries are integrable functions such that W (x) is positive definite almost everywhere on I. Suppose that W has finite moments, R n i.e., that I jxj jWi;j(x)jdx < 1 for all i; j and all n 2 N, where the integration is entry wise. Define the pairing h·; ·iW : C[x] ⊗ End(V ) × C[x] ⊗ End(V ) ! End(V ) R ∗ by hP; QiW = I P (x) W (x)Q(x)dx. The pairing h·; ·iW is called an End(V )-valued inner product, i.e. it has the following properties. •h P; QS + RT iW = hP; QiW S + hP; RiW T for all S; T 2 End(V ) and all P; Q; R 2 C[x] ⊗ End(V ), ∗ •h P; QiW = hQ; P iW for all P; Q 2 C[x] ⊗ End(V ), •h P; P iW ≥ 0 for all P 2 C[x] ⊗ End(V ), i.e. hP; P iW is positive semi-definite. If hP; P iW = 0 then P = 0. The right End(V )-module C[x]⊗End(V ) with the pairing h·; ·iW is called a pre-Hilbert module, see e.g. [Lan95] and [RW98]. A family fPd : d 2 Ng with Pd 2 C[x] ⊗ End(V ) is called a family of matrix valued orthogonal polynomials for h·; ·iW if (i) deg Pd = d, (ii) the leading coefficient of Pd is non-singular and (iii) hPd;Pd0 iW = Sdδd;d0 with Sd 2 End(V ). Note that Sd is positive definite. The existence of a family of matrix valued orthogonal polynomials for a given matrix weight W (x) is proved in e.g. [GT07, Prop. 2.4], by a generalization of the Gram-Schmidt orthogonalization. 2 1.1. Orthogonal polynomials An important property of a family of matrix valued orthogonal polynomials is that they satisfy a three term recurrence relation, i.e. there are sequences fAd : d 2 Ng; fBd : d 2 Ng and fCd : d 2 Ng in End(V ) with the Ad invertible, such that xPd(x) = Pd+1(x)Ad + Pd(x)Bd + Pd−1(x)Cd holds on I.
Recommended publications
  • The Theory of Induced Representations in Field Theory
    QMW{PH{95{? hep-th/yymmnnn The Theory of Induced Representations in Field Theory Jose´ M. Figueroa-O'Farrill ABSTRACT These are some notes on Mackey's theory of induced representations. They are based on lectures at the ITP in Stony Brook in the Spring of 1987. They were intended as an exercise in the theory of homogeneous spaces (as principal bundles). They were never meant for distribution. x1 Introduction The theory of group representations is by no means a closed chapter in mathematics. Although for some large classes of groups all representations are more or less completely classified, this is not the case for all groups. The theory of induced representations is a method of obtaining representations of a topological group starting from a representation of a subgroup. The classic example and one of fundamental importance in physics is the Wigner construc- tion of representations of the Poincar´egroup. Later Mackey systematized this construction and made it applicable to a large class of groups. The method of induced representations appears geometrically very natural when expressed in the context of (homogeneous) vector bundles over a coset manifold. In fact, the representation of a group G induced from a represen- tation of a subgroup H will be decomposed as a \direct integral" indexed by the elements of the space of cosets G=H. The induced representation of G will be carried by the completion of a suitable subspace of the space of sections through a given vector bundle over G=H. In x2 we review the basic notions about coset manifolds emphasizing their connections with principal fibre bundles.
    [Show full text]
  • 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.
    [Show full text]
  • REPRESENTATION THEORY. WEEK 4 1. Induced Modules Let B ⊂ a Be
    REPRESENTATION THEORY. WEEK 4 VERA SERGANOVA 1. Induced modules Let B ⊂ A be rings and M be a B-module. Then one can construct induced A module IndB M = A ⊗B M as the quotient of a free abelian group with generators from A × M by relations (a1 + a2) × m − a1 × m − a2 × m, a × (m1 + m2) − a × m1 − a × m2, ab × m − a × bm, and A acts on A ⊗B M by left multiplication. Note that j : M → A ⊗B M defined by j (m) = 1 ⊗ m is a homomorphism of B-modules. Lemma 1.1. Let N be an A-module, then for ϕ ∈ HomB (M, N) there exists a unique ψ ∈ HomA (A ⊗B M, N) such that ψ ◦ j = ϕ. Proof. Clearly, ψ must satisfy the relation ψ (a ⊗ m)= aψ (1 ⊗ m)= aϕ (m) . It is trivial to check that ψ is well defined. Exercise. Prove that for any B-module M there exists a unique A-module satisfying the conditions of Lemma 1.1. Corollary 1.2. (Frobenius reciprocity.) For any B-module M and A-module N there is an isomorphism of abelian groups ∼ HomB (M, N) = HomA (A ⊗B M, N) . F Example. Let k ⊂ F be a field extension. Then induction Indk is an exact functor from the category of vector spaces over k to the category of vector spaces over F , in the sense that the short exact sequence 0 → V1 → V2 → V3 → 0 becomes an exact sequence 0 → F ⊗k V1⊗→ F ⊗k V2 → F ⊗k V3 → 0. Date: September 27, 2005.
    [Show full text]
  • Representations of Finite Groups’ Iordan Ganev 13 August 2012 Eugene, Oregon
    Notes for ‘Representations of Finite Groups’ Iordan Ganev 13 August 2012 Eugene, Oregon Contents 1 Introduction 2 2 Functions on finite sets 2 3 The group algebra C[G] 4 4 Induced representations 5 5 The Hecke algebra H(G; K) 7 6 Characters and the Frobenius character formula 9 7 Exercises 12 1 1 Introduction The following notes were written in preparation for the first talk of a week-long workshop on categorical representation theory. We focus on basic constructions in the representation theory of finite groups. The participants are likely familiar with much of the material in this talk; we hope that this review provides perspectives that will precipitate a better understanding of later talks of the workshop. 2 Functions on finite sets Let X be a finite set of size n. Let C[X] denote the vector space of complex-valued functions on X. In what follows, C[X] will be endowed with various algebra structures, depending on the nature of X. The simplest algebra structure is pointwise multiplication, and in this case we can identify C[X] with the algebra C × C × · · · × C (n times). To emphasize pointwise multiplication, we write (C[X], ptwise). A C[X]-module is the same as X-graded vector space, or a vector bundle on X. To see this, let V be a C[X]-module and let δx 2 C[X] denote the delta function at x. Observe that δ if x = y δ · δ = x x y 0 if x 6= y It follows that each δx acts as a projection onto a subspace Vx of V and Vx \ Vy = 0 if x 6= y.
    [Show full text]
  • Representation Theory with a Perspective from Category Theory
    Representation Theory with a Perspective from Category Theory Joshua Wong Mentor: Saad Slaoui 1 Contents 1 Introduction3 2 Representations of Finite Groups4 2.1 Basic Definitions.................................4 2.2 Character Theory.................................7 3 Frobenius Reciprocity8 4 A View from Category Theory 10 4.1 A Note on Tensor Products........................... 10 4.2 Adjunction.................................... 10 4.3 Restriction and extension of scalars....................... 12 5 Acknowledgements 14 2 1 Introduction Oftentimes, it is better to understand an algebraic structure by representing its elements as maps on another space. For example, Cayley's Theorem tells us that every finite group is isomorphic to a subgroup of some symmetric group. In particular, representing groups as linear maps on some vector space allows us to translate group theory problems to linear algebra problems. In this paper, we will go over some introductory representation theory, which will allow us to reach an interesting result known as Frobenius Reciprocity. Afterwards, we will examine Frobenius Reciprocity from the perspective of category theory. 3 2 Representations of Finite Groups 2.1 Basic Definitions Definition 2.1.1 (Representation). A representation of a group G on a finite-dimensional vector space is a homomorphism φ : G ! GL(V ) where GL(V ) is the group of invertible linear endomorphisms on V . The degree of the representation is defined to be the dimension of the underlying vector space. Note that some people refer to V as the representation of G if it is clear what the underlying homomorphism is. Furthermore, if it is clear what the representation is from context, we will use g instead of φ(g).
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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.
    [Show full text]
  • 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 ).
    [Show full text]
  • 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.
    [Show full text]