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Algebraic integrability of Schrödinger operators and representations of Lie algebras (1994)

by P Etingof, K Styrkas
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Exchange dynamical quantum groups

by P. Etingof, A. Varchenko - Comm. Math. Phys , 1999
"... Abstract. For any simple Lie algebra g and any complex number q which is not zero or a nontrivial root of unity, we construct a dynamical quantum group (Hopf algebroid), whose representation theory is essentially the same as the representation theory of the quantum group Uq(g). This dynamical quantu ..."
Abstract - Cited by 43 (9 self) - Add to MetaCart
Abstract. For any simple Lie algebra g and any complex number q which is not zero or a nontrivial root of unity, we construct a dynamical quantum group (Hopf algebroid), whose representation theory is essentially the same as the representation theory of the quantum group Uq(g). This dynamical quantum group is obtained from the fusion and exchange relations between intertwining operators in representation theory of Uq(g), and is an algebraic structure standing behind these relations. 1.
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...< aiv, biv ∗ > if JV, ∗ V (λ) = ∑ ai ⊗bi. Let ρ ∈ h ∗ be the half sum of positive roots. Lemma 29. For A = U(g ) and any V, W ∈ O0, we have JV,W(tρ) → 1 when t ∈ C and t tends to infinity. Proof : In =-=[ES1]-=-, the intertwining operator Φ v (λ) was computed in terms of the Shapovalov form (formula (3-5) in [ES1]). From formula (3-5) in [ES1] it is easy to obtain the following asymptotic expansion of Φ v (λ...

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
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... has the form (1.3) (RV (Y1)ψ)(h) = δ(h) −1 ( ∆h − ∑ eαfα 2 sinh 2 ) − 〈ρ, ρ〉 (ψ(h)δ(h)), h ∈ t (〈α, h〉/2) α∈R + where ∆h is the Laplace operator on h, and ψ(h) = ˜ ψ(e h ), ˜ ψ ∈ F V (K). (iii) ([E],=-=[ES]-=-) Set (1.4) Ψ(h) = Tr|Nλ (Φeh ∑ 〈λ,h〉 ) = e α∈Q + Tr| Nλ[λ−α](Φ)e −〈α,h〉 . This series absolutely converges in the region {h ∈ h : Re〈α, h〉 > 0, α ∈ R + }, and its sum takes values in V ∗ [0] and is a...

Hypergeometric solutions of trigonometric KZ equations satisfy dynamical difference equations

by Y. Markov, A. Varchenko - Adv. Math
"... {yavmar, anv} @ email.unc.edu Abstract. The trigonometric KZ equations associated to a Lie algebra g depend on a parameter λ ∈ h where h ⊂ g is a Cartan subalgebra. A system of dynamical difference equations with respect to λ compatible with the KZ equations is introduced in [TV]. We prove that the ..."
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{yavmar, anv} @ email.unc.edu Abstract. The trigonometric KZ equations associated to a Lie algebra g depend on a parameter λ ∈ h where h ⊂ g is a Cartan subalgebra. A system of dynamical difference equations with respect to λ compatible with the KZ equations is introduced in [TV]. We prove that the standard hypergeometric solutions of the trigonometric KZ equations associated to slN also satisfy the dynamical difference equations.
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...k (λ)ea−k 21 e k 31e b−k 32 vλ ⊗ e b−m 32 e m 31e a−m 21 vλ. Finaly, given v ∈ V , there is a unique singular vector, sing(vλ ⊗v), in Mλ ⊗V of the form sing(vλ ⊗ v) = vλ ⊗ v + {lower order terms}. In =-=[ESt]-=- the vector sing(vλ ⊗ v) is given in terms of the inverse of the Shapovalov form. As a corollary we get sing(vλ ⊗ v) = = ∞∑ a,b=0 ∞∑ a,b=0 ∑ min(a,b) m,k=0 ∑ min(a,b) m,k=0 (−1) a+b B a,b m,k (λ)eb−m ...

Algebraic Integrability Of Macdonald Operators And Representations Of Quantum Groups

by Pavel Etingof, Konstantin Styrkas
"... In this paper we construct examples of commutative rings of difference operators with matrix coefficients from representation theory of quantum groups, generalizing the results of our previous paper [ES] to the q-deformed case. A generalized Baker-Akhiezer function \Psi is realized as a matrix ch ..."
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In this paper we construct examples of commutative rings of difference operators with matrix coefficients from representation theory of quantum groups, generalizing the results of our previous paper [ES] to the q-deformed case. A generalized Baker-Akhiezer function \Psi is realized as a matrix character of a Verma module and is a common eigenfunction for a commutative ring of difference operators.
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...sion / 1 (; x) = 2ffl \Delta / (0) 1 (; x) +O(ffl 2 ) where / (0) 1 (; x) = e x (e x \Gamma e \Gammax ) 2 `s\Gamma e x + e \Gammax e x \Gamma e \Gammax ' is the /-function for the classical case (cf. =-=[ES]-=-). The difference operators become M 1 = 2 + ffl 2 (D 2 + 4) +O(ffl 3 ) M 0 = \Gamma2 + ffl 2 (3D 2 + 8) + 4ffl 3 (D 3 + 1) +O(ffl 4 ); where commuting differential operators D 2 ; D 3 are equal D 2 =...

Multicomponent Calogero model of BN-type confined in harmonic potential Phys

by Takashi Yamamoto - Lett , 1995
"... A new one-dimensional model, the multicomponent Calogero model of BNtype confined in the harmonic potential, is introduced. The Lax pair of this model is determined, and then a set of functionally independent conserved operators are constructed. Moreover, the energy spectrums of the above model are ..."
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A new one-dimensional model, the multicomponent Calogero model of BNtype confined in the harmonic potential, is introduced. The Lax pair of this model is determined, and then a set of functionally independent conserved operators are constructed. Moreover, the energy spectrums of the above model are obtained by three different methods. Typeset using REVTEX
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...k ⎦ . (54) Also, the discritization [7,8,29,30] of the BN-CSC model and the BCN-SS model can be constructed. 4 The integrability of this model (with λ ′ 1 = 0) has been studied by Etingof and Styrkas =-=[27]-=- in terms of the representation theory of the Lie algebras. See also [18,28]. 5 Using the identity sin 2x = 2sin xcos x, we rewrote the term 1/sin 2 (π/L)2qj. 12The models which were introduced in th...

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 ..."
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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&apos;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&apos;s inner product and symmetry identities for the root system An\Gamma1 . Macdonald&apos;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&apos;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&apos;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&apos;s difference operators.

Norms of logarithmic primaries of Virasoro algebra

by Shintarou Yanagida
"... ar ..."
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...(r,s)∈Z2>0, 1≤rs≤n [ lim h→hr,s(t) Nr,s(t, h) h− hr,s(t) ]−1 fn−rs(t, hr,s(t) + rs) h− hr,s(t) . (1.25) Actually, one can obtain this formula by considering the Jantzen filtration (see [27], [14] and =-=[10]-=-) on M(c, h) and by some calculation on Kn. Thus from the comparison of (1.24) and (1.25), the verification of the conjecture (1.23) is reduced to the conjecture (1.20). However, it seems that the jus...

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.

The Fine Structure Of Translation Functors

by Karen Günzl , 1999
"... Let E be a simple finite-dimensional representation of a semisimple Lie algebra with extremal weight # and let 0 #= e # E# . Let M(#) be the Verma module with highest weight # and 0 #= v# # M(#)# . We investigate the projection of e# v# # E# M(#) on the central character #(# + #). This is ..."
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Let E be a simple finite-dimensional representation of a semisimple Lie algebra with extremal weight # and let 0 #= e # E# . Let M(#) be the Verma module with highest weight # and 0 #= v# # M(#)# . We investigate the projection of e# v# # E# M(#) on the central character #(# + #). This is a rational function in # and we calculate its poles and zeros. We then apply this result in order to compare translation functors.
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