167 research outputs found

    Central Extension of the Yangian Double

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    Central extension \DYg of the Double of the Yangian is defined for a simple Lie algebra g{\bf g} with complete proof for g=sl2{\bf g} =sl_2. Basic representations and intertwining operators are constructed for \DY2.Comment: 12 pages, latex, no figure

    Mickelsson algebras and representations of Yangians

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    Unitarity and Complete Reducibility of Certain Modules over Quantized Affine Lie Algebras

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    Let Uq(G^)U_q(\hat{\cal G}) denote the quantized affine Lie algebra and Uq(G(1))U_q({\cal G}^{(1)}) the quantized {\em nontwisted} affine Lie algebra. Let Ofin{\cal O}_{\rm fin} be the category defined in section 3. We show that when the deformation parameter qq is not a root of unit all integrable representations of Uq(G^)U_q(\hat{\cal G}) in the category Ofin{\cal O}_{\rm fin} are completely reducible and that every integrable irreducible highest weight module over Uq(G(1))U_q({\cal G}^{(1)}) corresponding to q>0q>0 is equivalent to a unitary module.Comment: 17 pages (minor errors corrected

    Unified description of quantum affine (super)algebras U_q(A_{1}^{(1)}) and U_q(C(2)^{(2)})

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    We show that the quantum affine algebra U_{q}(A_{1}^{(1)}) and the quantum affine superalgebra U_{q}(C(2)^{(2)}) admit unified description. The difference between them consists in the phase factor which is equal to 1 for U_{q}(A_{1}^{(1)}) and is equal to -1 for U_{q}(C(2)^{(2)}). We present such a description for the construction of Cartan-Weyl generators and their commutation relations, as well for the universal R-matrices.Comment: 16 pages, LaTeX. Talk by V.N. Tolstoy at XIV-th Max Born Symposium "New Symmetries and Integrable Models", Karpacz, September 1999; in press in Proceedings, Ed. World Scientific, 200

    Quantum Affine (Super)Algebras Uq(A1(1))U_q(A_{1}^{(1)}) and Uq(C(2)(2))U_q(C(2)^{(2)})

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    We show that the quantum affine algebra Uq(A1(1))U_{q}(A_{1}^{(1)}) and the quantum affine superalgebra Uq(C(2)(2))U_{q}(C(2)^{(2)}) admit a unified description. The difference between them consists in the phase factor which is equal to 1 for Uq(A1(1))U_{q}(A_{1}^{(1)}) and it is equal to -1 for Uq(C(2)(2))U_{q}(C(2)^{(2)}). We present such a description for the actions of the braid group, for the construction of Cartan-Weyl generators and their commutation relations, as well for the extremal projector and the universal R-matrix. We give also a unified description for the 'new realizations' of these algebras together with explicit calculations of corresponding R-matrices.Comment: 22 pages, LaTe

    Three realizations of quantum affine algebra Uq(A2(2))U_q(A_2^{(2)})

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    In this article we establish explicit isomorphisms between three realizations of quantum twisted affine algebra Uq(A2(2))U_q(A_2^{(2)}): the Drinfeld ("current") realization, the Chevalley realization and the so-called RLLRLL realization, investigated by Faddeev, Reshetikhin and Takhtajan.Comment: 15 page

    Cherednik algebras and Zhelobenko operators

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    We study canonical intertwining operators between induced modules of the trigonometric Cherednik algebra. We demonstrate that these operators correspond to the Zhelobenko operators for the affine Lie algebra of type A. To establish the correspondence, we use the functor of Arakawa, Suzuki and Tsuchiya which maps certain modules of the affine Lie algebra to modules of the Cherednik algebra

    Q-power function over Q-commuting variables and deformed XXX, XXZ chains

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    We find certain functional identities for the Gauss q-power function of a sum of q-commuting variables. Then we use these identities to obtain two-parameter twists of the quantum affine algebra U_q (\hat{sl}_2) and of the Yangian Y(sl_2). We determine the corresponding deformed trigonometric and rational quantum R-matrices, which then are used in the computation of deformed XXX and XXZ Hamiltonians.Comment: LaTeX, 12 page

    Factorization of the Universal R-matrix for Uq(sl^2)U_q(\hat{sl}_2)

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    The factorization of the universal R-matrix corresponding to so called Drinfeld Hopf structure is described on the example of quantum affine algebra Uq(sl^2)U_q(\hat{sl}_2). As a result of factorization procedure we deduce certain differential equations on the factors of the universal R{\cal R}-matrix, which allow to construct uniquely these factors in the integral form.Comment: 28 pages, LaTeX 2.09 using amssym.def and amssym.te
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