24 research outputs found

    Letter from Senator Dennis DeConcini (D-AZ) to Geraldine Ferraro

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    Letter from Senator Dennis DeConcini (D-AZ) to Geraldine Ferraro. Senator DeConcini attached a letter from a Dutch academic, Dr. C.V. Lafeber. Dr. C.V. Lafeber included a plan for Polish and Dutch foreign policy. Letters have handwritten notes.https://ir.lawnet.fordham.edu/vice_presidential_campaign_correspondence_1984_international/1334/thumbnail.jp

    Roots of Unity: Representations of Quantum Groups

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    Representations of Quantum Groups U_q (g_n), g_n any semi simple Lie algebra of rank n, are constructed from arbitrary representations of rank n-1 quantum groups for q a root of unity. Representations which have the maximal dimension and number of free parameters for irreducible representations arise as special cases.Comment: 23 page

    On Ï„(2)\tau^{(2)}-model in Chiral Potts Model and Cyclic Representation of Quantum Group Uq(sl2)U_q(sl_2)

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    We identify the precise relationship between the five-parameter Ï„(2)\tau^{(2)}-family in the NN-state chiral Potts model and XXZ chains with Uq(sl2)U_q (sl_2)-cyclic representation. By studying the Yang-Baxter relation of the six-vertex model, we discover an one-parameter family of LL-operators in terms of the quantum group Uq(sl2)U_q (sl_2). When NN is odd, the NN-state Ï„(2)\tau^{(2)}-model can be regarded as the XXZ chain of Uq(sl2)U_{\sf q} (sl_2) cyclic representations with qN=1{\sf q}^N=1. The symmetry algebra of the Ï„(2)\tau^{(2)}-model is described by the quantum affine algebra Uq(sl^2)U_{\sf q} (\hat{sl}_2) via the canonical representation. In general for an arbitrary NN, we show that the XXZ chain with a Uq(sl2)U_q (sl_2)-cyclic representation for q2N=1q^{2N}=1 is equivalent to two copies of the same NN-state Ï„(2)\tau^{(2)}-model.Comment: Latex 11 pages; Typos corrected, Minor changes for clearer presentation, References added and updated-Journal versio

    Duality and Symmetry in Chiral Potts Model

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    We discover an Ising-type duality in the general NN-state chiral Potts model, which is the Kramers-Wannier duality of planar Ising model when N=2. This duality relates the spectrum and eigenvectors of one chiral Potts model at a low temperature (of small k′k') to those of another chiral Potts model at a high temperature (of k′−1k'^{-1}). The τ(2)\tau^{(2)}-model and chiral Potts model on the dual lattice are established alongside the dual chiral Potts models. With the aid of this duality relation, we exact a precise relationship between the Onsager-algebra symmetry of a homogeneous superintegrable chiral Potts model and the sl2sl_2-loop-algebra symmetry of its associated spin-N−12\frac{N-1}{2} XXZ chain through the identification of their eigenstates.Comment: Latex 34 pages, 2 figures; Typos and misprints in Journal version are corrected with minor changes in expression of some formula

    Finite Basis Property of S-Ideals of Finite Dimensional Forms

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