Kobe University Repository : Kernel

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. The symbol det stands for the quantum determinant (1.4) det= (--q)Z(Xo(oX...x, aSn+ where S/ is the permutation group o the set {0, 1,..., n} and, or each a e S+1, l(a) denotes the number o pairs (i, ]) with Oi]n and a(i) a(]). This algebra A has the structure of a Hop algebra, endowed with the coproduct z" A-A(R)A and the counit " A-+C satisfying (1.5) (x)- xxj and e(x)=/j or Oi, ]n. k=0 Moreover, there exists a unique conjugate linear anti-homomorphism aa*" A-+A such that (1.6) x*..-S(x) or O<i,_ ]<n_ with respect to the antipode S" A-A o A. Together with this *-opera- tion, the Hopf algebra A=A(SL(n/I;C)) defines the *-Hopf algebra A(SU(n/ 1)). In what ollows, we denote by G the quantum group SU(n+ 1) and by K the quantum subgroup SU,(n) o G=SU(n+I). Denote by y (0i, *) Department of Mathematics, Sophia University. **) Department of Mathematics, Tokyo Metropolitan University. ***) Department of Mathematics, Nagoya University. 170 M. NOUMI, H. YAMADA, and K. MIMACHI [Vol. 65 (A), ]<_n) the canonical generators for the coordinate ring A(K). Embedding of K into G is then specialized by the C-algebra epimorphism A(G)-- A(K) such that " (1.7) K(x)=yj, K(x,)=l and 7CK(Xin)---7K(Xnj)---O for Oi, ]<n. 2. For a given dominant integral weight A--20z0+'-. +2,-e,- (0 ..,_,0), there exists unique irreducible right A(G)-comodule V with highest weight A. We denote by A the undmental weight e0+'" +_ or lkn. As representation of K=SU(n), V can be decom- posed into irreducible components. It turns out that V has trivial rep- resentation o K as an irreducible component if and only if the highest weight A is o the orm A 1A,- man or some l, m e N and that the trivial representation may appear with multiplicity one. Such a representation V is said to be of class 1 relative to K. If V is o class 1, it can be decomposed into the form (2.) V=CvoV as an A(K)-comodule, where v0 is a K-fixed vector of V. Let {v, ..., v_} be a C-basis or V (N=dimc V) and deflate the matrix elements w of the representation V by (2.2) Re(v)= vw or 0]N. i=0 Here R" VVA(G) is the structure mapping of the right A(G)- comodule V. Then the matrix element Woo does not depend on the choice o v0, ..., v_ and is bi-K-invariant in the sense that (2.3) R(woo)=Wol and L(Woo)=lwoo, where R=(idz)o and L We call woo the zonal spherical function o V relative to K. We introduce the notation of quantum r-minor determinants. Let I and J be two subsets of {0, 1,..., n} with I=J=r. Arrange the ele- ments o I and J in the increasing order" I-{io,...,i_} (Oio... i_n) und J=[]o, ", ]-} (0]o... ]_n). We define the quantum r-minor determinant by (3.) ?o:.._ x__ If I {0, 1, r--1}, we use the abbreviation $=. To investigate spherical functions, we give a geometric realization of V (cf. [3]). Let A=A,o+A,+ Az_ (;0'" Z> 0) be a dominant integral weight. Let J=(J0, "J-) be a sequence of non-empty subsets of {0, 1, .., n} with Js=Z for 0sk. We call J a column strict plane partition of shape A if the following conditions are satisfied" (3.2) Is= {]0,,,..., L,_,,)c{o, 1,..., ],,<]+,, and The irreducible representation of V can be realized as a right sub-A(G)- No. 6] Zonal Spherical Functions 171 comodule as (3.3) V-- CsA(G), J where the sum is taken over the set of all column strict plane partitions of shape A and (3.4) i J=(J, J_). s--o""" _ ., It is seen that these vectors are linearly independent and that they orm a C-basis or right A(G)-comodule. Note that the product of minor de- terminants (3.5) 0...,o-''' $0...,_- gives the highest weight vector of V. We remark that V is identified with the vector space of all left relative B_-invariants in A(SL(n/ 1; C)) with respect to the character corresponding to A, where B_ is the Borel subgroup "of lower triangular matrices" (see [3]). I A=IA.,+mA (1, m e N), the .spherical representation V contains K-fixed vector 01...n-lira (3 6) v0 (,) ($0 .n-l] By using algebraic properties of quantum minor determinants, we can determine explicitly the zonal spherical function of V in terms of basic hypergeometric series (3.7) a, b. q, z " (a; q)(b q) z, (a; q)= [-[ (1--aqO. c Theorem. Let VA be the representation of G--SUq(n/ 1) with highest weight A=lAl+mAn (1, m e N). Then the zonal spherical function w--Woo of VA relative to K=SUq(n) is expressed by a basic hypergeometric series in z--1 Xo...n_f::01--.n-1 as follows" q(/) q,qz (3.8) w=(xn)-(q-''q ifl_m, and q-' q(+) (3.9) q2' q2z ($ .n-l] if <m w=?,( q2n ) The above polynomials in z are so-called-little q-Jacobi polynomials. As for zonal spherical functions, Theorem generalizes a result of [1, 2]. References 1 T. Masuda et .al.: Representations of quantum groups and a q-analogue of or- thogonal polynomials. C. R. Acad. Sci. Paris, Srie I, 307, 559-564 (1988). 2 : Representations of the quantum group SUq(2) and the little q-Jacobi poly- nomials (preprint). 3 M. Noumi, H. Yamada, and K. Mimachi: Representations of the quantum group GLq(n +1; C) (in preparation). 4 N. Yu. Reshetikhin, L. A. Takhtajan, and L. D. Faddeev: Quantization of Lie groups and Lie algebras (to appear in Algebra and Analysis) (in Russian)..

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