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A unified representation-theoretic approach to special functions, hep-th 9312101, Functional Anal. and its Applic. 28 (1994)

by P I Etingof, A A Kirillov
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Macdonald's Polynomials And Representations Of Quantum Groups

by Pavel I. Etingof, Alexander A. Kirillov, Jr., Er A. Kirillov - Math. Res. Let , 1994
"... this paper we present a formula for Macdonald's polynomials which arises from the representation theory of the quantum group U q (gl n ). This formula expresses Macdonald's polynomials as vector-valued characters -- (weighted) traces of intertwining operators between certain modules over U ..."
Abstract - Cited by 43 (12 self) - Add to MetaCart
this paper we present a formula for Macdonald's polynomials which arises from the representation theory of the quantum group U q (gl n ). This formula expresses Macdonald's polynomials as vector-valued characters -- (weighted) traces of intertwining operators between certain modules over U q (gl n ). This result was announced in [EK]. It is an interesting problem to find relation between this construction and a recent paper of Noumi ([No]) which gives interpretation of Macdonald's polynomials for special values of k as zonal spherical functions on a homogeneous space for a quantum group
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...l n ). This formula expresses Macdonald's polynomials as vector-valued characters -- (weighted) traces of intertwining operators between certain modules over U q (gl n ). This result was announced in =-=[EK]-=-. It is an interesting problem to find relation between this construction and a recent paper of Noumi ([No]) which gives interpretation of Macdonald's polynomials for special values of k as zonal sphe...

On Inner Product In Modular Tensor Categories. II Inner Product On Conformal Blocks.

by Alexander A. Kirillov, Jr. - I & II, math.QA/9508017 and q-alg/9611008 , 1995
"... this paper, we apply the same construction to the MTC coming from the integrable representations of affine Lie algebras or, equivalently, from Wess-ZuminoWitten model of conformal field theory. We briefly recall construction of this category, first suggested by Moore and Seiberg (see [MS1,2]) and la ..."
Abstract - Cited by 43 (0 self) - Add to MetaCart
this paper, we apply the same construction to the MTC coming from the integrable representations of affine Lie algebras or, equivalently, from Wess-ZuminoWitten model of conformal field theory. We briefly recall construction of this category, first suggested by Moore and Seiberg (see [MS1,2]) and later refined by Kazhdan and Lusztig ([KL1--4]) and Finkelberg ([F]) in Section 9. In particular, spaces of homomorphisms in this category are the spaces of conformal blocks of WZW model. Thus, the general theory developed in Section 2 of [K] gives us an inner product on the space of conformal blocks, and so defined inner product is modular invariant. This definition is constructive: we show how it can be rewritten so that it only involves Drinfeld associator, or, equivalently, asymptotics of solutions of Knizhnik-Zamolodchikov equations. Since there are integral formulas for the solutions of KZ equations, this shows that the inner product on the space of conformal blocks can be written explicitly in terms of certain integrals. In the case g = sl 2 these integrals can be calculated (see [V]), using Selberg integral, and the answer is written in terms of \Gamma-functions. Thus, in this case we can write explicit formulas for inner product on the space of conformal blocks. These expressions are 1991 Mathematics Subject Classification. Primary 81R50, 05E35, 18D10; Secondary 57M99

Spherical functions on affine Lie groups

by Pavel I. Etingof, Igor B. Frenkel, Alexander A. Kirillov - Duke Math. J , 1995
"... hep-th 9407047 ..."
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hep-th 9407047

Three formulas for eigenfunctions of integrable Schrödinger operators

by Giovanni Felder, Alexander Varchenko , 1995
"... Abstract. We give three formulas for meromorphic eigenfunctions (scattering states) of Sutherland’s integrable N-body Schrödinger operators and their generalizations. The first is an explicit computation of the Etingof–Kirillov traces of intertwining operators, the second an integral representation ..."
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Abstract. We give three formulas for meromorphic eigenfunctions (scattering states) of Sutherland’s integrable N-body Schrödinger operators and their generalizations. The first is an explicit computation of the Etingof–Kirillov traces of intertwining operators, the second an integral representation of hypergeometric type, and the third of Bethe ansatz type. The last two formulas are degenerations of elliptic formulas obtained previously in connection with the Knizhnik–Zamolodchikov– Bernard equation. The Bethe ansatz formulas in the elliptic case are reviewed and discussed in more detail here: Eigenfunctions are parametrized by a “Hermite–Bethe ” variety, a generalization of the spectral variety of the Lamé operator. We also give the q-deformed version of our first formula. In the scalar slN case, this gives common eigenfunctions of the commuting Macdonald–Rujsenaars difference operators. 1.
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...λ)) eαe−α (1) acting on functions on h with values in U[0]. The Laplacian △ is the operator ∑ ν ∂2 ∂λ2 in terms of coordinates λν = (bν,λ) for any orthonormal ν basis b1,... ,br of h . As remarked in =-=[3]-=-, if g = slN, and U is the symmetric power SpN CN of the defining representation CN , then U[0] is onedimensional and this differential operator reduces to Sutherland’s integrable N-body Schrödinger o...

On The Affine Analogue Of Jack's And Macdonald's Polynomials

by Pavel I. Etingof, Alexander A. Kirillov, Jr. - DUKE MATH J , 1994
"... ..."
Abstract - Cited by 24 (4 self) - Add to MetaCart
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Algebraic integrability of Schrödinger operators and representations of Lie algebras

by Pavel Etingof, Konstantin Styrkas , 1994
"... hep-th 9403135 ..."
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hep-th 9403135

Representation-Theoretic Proof Of The Inner Product And Symmetry Identities For Macdonald's Polynomials

by Pavel I. Etingof, Alexander A. Kirillov, Jr. - Compositio Math , 1996
"... This paper is a continuation of our papers [EK1, EK2]. In [EK2] we showed that for the root system An\Gamma1 one can obtain Macdonald's polynomials -- a new interesting class of symmetric functions recently defined by I. Macdonald [M1] -- as weighted traces of intertwining operators between cer ..."
Abstract - Cited by 12 (1 self) - Add to MetaCart
This paper is a continuation of our papers [EK1, EK2]. In [EK2] we showed that for the root system An\Gamma1 one can obtain Macdonald's polynomials -- a new interesting class of symmetric functions recently defined by I. Macdonald [M1] -- as weighted traces of intertwining operators between certain finite-dimensional representations of U q sl n . The main goal of the present paper is to use this construction to give a representation-theoretic proof of Macdonald's inner product and symmetry identities for the root system An\Gamma1 . Macdonald's inner product identities (see [M2]) have been proved by combinatorial methods by Macdonald (unpublished) for the root system An\Gamma1 and by Cherednik in the general case; symmetry identities for the root system An\Gamma1 have also been proved by Macdonald ([Macdonald, private communication]). The paper is organized as follows. In Section 1 we briefly list the basic definitions. In Section 2 we define Macdonald's polynomials P and recall the construction of

Central Elements For Quantum Affine Algebras And Affine Macdonald's Operators

by Pavel I. Etingof, N Zwe
"... We describe a generalization of Drinfeld's description of the center of a quantum group to the case of quantum affine algebras. We use the obtained central elements to construct the affine analogue of Macdonald's difference operators. ..."
Abstract - Cited by 7 (2 self) - Add to MetaCart
We describe a generalization of Drinfeld's description of the center of a quantum group to the case of quantum affine algebras. We use the obtained central elements to construct the affine analogue of Macdonald's difference operators.
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...r where (Tif)(x1,... ,xn) =f(x1,... ,q 2 xi,... ,xn), t is a formal variable, and r =1,... ,n− 1. Macdonald proved [M] that these operators are pairwise commutative: [M r ,M s ]=0,1≤ r, s ≤ n − 1. In =-=[EK1]-=-,[EK2] it was shown how to obtain Macdonald operators from central elements of the quantum group Uq(g), where g = sln. This was done as follows. 3.2. Recall that fundamental representations of Uq(g) a...

Integral formulas for wave functions of quantum many-body problems and representations of gln

by Pavel Etingof
"... hep-th 9405038 We derive explicit integral formulas for eigenfunctions of quantum integrals of the Calogero-Sutherland-Moser operator with trigonometric interaction potential. In particular, we derive explicit formulas for Jack’s symmetric functions. To obtain such formulas, we use the representatio ..."
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hep-th 9405038 We derive explicit integral formulas for eigenfunctions of quantum integrals of the Calogero-Sutherland-Moser operator with trigonometric interaction potential. In particular, we derive explicit formulas for Jack’s symmetric functions. To obtain such formulas, we use the representation of these eigenfunctions by means of traces of intertwining operators between certain modules over the Lie algebra gln, and the realization of these modules on functions of many variables.
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...e of such intertwiner, which is our main result (Theorem 2.2). As a corollary, we get an explicit integral representation of Jack’s symmetric functions. It follows from Theorem 2.2 and the results of =-=[EK1]-=-,[EK2]. 1. Trace representation of wave functions The Hamiltonian of the quantum n-body problem on the line is (1.1) H = n∑ ∂2 ∂x i=1 2 i − C ∑ U(xi − xj), i<j where U is some potential function, and ...

Cental elements for quantum affine . . .

by Pavel I. Etingof , 1994
"... We describe a generalization of Drinfeld’s description of the center of a quantum group to the case of quantum affine algebras. We use the obtained central elements to construct the affine analogue of Macdonald’s difference operators. ..."
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We describe a generalization of Drinfeld’s description of the center of a quantum group to the case of quantum affine algebras. We use the obtained central elements to construct the affine analogue of Macdonald’s difference operators.
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