484 research outputs found

    Bethe Equation of τ(2)\tau^{(2)}-model and Eigenvalues of Finite-size Transfer Matrix of Chiral Potts Model with Alternating Rapidities

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    We establish the Bethe equation of the τ(2)\tau^{(2)}-model in the NN-state chiral Potts model (including the degenerate selfdual cases) with alternating vertical rapidities. The eigenvalues of a finite-size transfer matrix of the chiral Potts model are computed by use of functional relations. The significance of the "alternating superintegrable" case of the chiral Potts model is discussed, and the degeneracy of τ(2)\tau^{(2)}-model found as in the homogeneous superintegrable chiral Potts model.Comment: Latex 25 pages; Typos corrected, Minor changes for clearer presentation, References added-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 kk') to those of another chiral Potts model at a high temperature (of k1k'^{-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-N12\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

    On τ(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 τ(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 τ(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 τ(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 τ(2)\tau^{(2)}-model.Comment: Latex 11 pages; Typos corrected, Minor changes for clearer presentation, References added and updated-Journal versio

    The Q-operator and Functional Relations of the Eight-vertex Model at Root-of-unity η=2mKN\eta = \frac{2m K}{N} for odd N

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    Following Baxter's method of producing Q_{72}-operator, we construct the Q-operator of the root-of-unity eight-vertex model for the crossing parameter η=2mKN\eta = \frac{2m K}{N} with odd NN where Q_{72} does not exist. We use this new Q-operator to study the functional relations in the Fabricius-McCoy comparison between the root-of-unity eight-vertex model and the superintegrable N-state chiral Potts model. By the compatibility of the constructed Q-operator with the structure of Baxter's eight-vertex (solid-on-solid) SOS model, we verify the set of functional relations of the root-of-unity eight-vertex model using the explicit form of the Q-operator and fusion weights of SOS model.Comment: Latex 28 page; Typos corrected, minor changes in presentation, References added and updated-Journal versio

    The Q-operator for Root-of-Unity Symmetry in Six Vertex Model

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    We construct the explicit QQ-operator incorporated with the sl2sl_2-loop-algebra symmetry of the six-vertex model at roots of unity. The functional relations involving the QQ-operator, the six-vertex transfer matrix and fusion matrices are derived from the Bethe equation, parallel to the Onsager-algebra-symmetry discussion in the superintegrable NN-state chiral Potts model. We show that the whole set of functional equations is valid for the QQ-operator. Direct calculations in certain cases are also given here for clearer illustration about the nature of the QQ-operator in the symmetry study of root-of-unity six-vertex model from the functional-relation aspect.Comment: Latex 26 Pages; Typos and small errors corrected, Some explanations added for clearer presentation, References updated-Journal version with modified labelling of sections and formula

    The Onsager Algebra Symmetry of τ(j)\tau^{(j)}-matrices in the Superintegrable Chiral Potts Model

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    We demonstrate that the τ(j)\tau^{(j)}-matrices in the superintegrable chiral Potts model possess the Onsager algebra symmetry for their degenerate eigenvalues. The Fabricius-McCoy comparison of functional relations of the eight-vertex model for roots of unity and the superintegrable chiral Potts model has been carefully analyzed by identifying equivalent terms in the corresponding equations, by which we extract the conjectured relation of QQ-operators and all fusion matrices in the eight-vertex model corresponding to the TT^T\hat{T}-relation in the chiral Potts model.Comment: Latex 21 pages; Typos added, References update

    Individuals' Use of Care While Uninsured: Effects of Time Since Episode Inception and Episode Length

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    Few studies have addressed how use of care may vary over the course of an episode of being uninsured or across uninsured episodes of varying duration. This research models the probability that an uninsured individual has (a) any medical expenditures or charges, and (b) any office-based visit during each month of an uninsured episode. We find that the ultimate length of an individual's episode of being uninsured bears relatively little on individuals' use of healthcare in any particular month and that the probability of health care utilization rises during the first year of the episode, with more use in the second six months of the year compared to the first six months.

    CHIP Expansions to Higher-Income Children in Three States: Profiles of Eligibility and Insurance Coverage

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    Summarizes findings on how changes in eligibility rules for children's public health insurance programs affected 2002-09 coverage rates and the number of uninsured children in Illinois, Pennsylvania, and Washington. Compares results by scope of reform

    Take-Up of Public Insurance and Crowd-out of Private Insurance Under Recent CHIP Expansions to Higher Income Children

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    We analyze the effects of states’ expansions of CHIP eligibility to children in higher income families during 2002-2009 on take-up of public coverage, crowd-out of private coverage, and rates of uninsurance. Our results indicate these expansions were associated with limited uptake of public coverage and only a two percentage point reduction in the uninsurance rate among these children. Because not all of the take-up of public insurance among eligible children is accounted for by children who transfer from being uninsured to having public insurance, our results suggest that there may be some crowd-out of private insurance coverage; the upper bound crowd-out rate we calculate is 46 percent.

    Fusion Operators in the Generalized τ(2)\tau^{(2)}-model and Root-of-unity Symmetry of the XXZ Spin Chain of Higher Spin

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    We construct the fusion operators in the generalized τ(2)\tau^{(2)}-model using the fused LL-operators, and verify the fusion relations with the truncation identity. The algebraic Bethe ansatz discussion is conducted on two special classes of τ(2)\tau^{(2)} which include the superintegrable chiral Potts model. We then perform the parallel discussion on the XXZ spin chain at roots of unity, and demonstrate that the sl2sl_2-loop-algebra symmetry exists for the root-of-unity XXZ spin chain with a higher spin, where the evaluation parameters for the symmetry algebra are identified by the explicit Fabricius-McCoy current for the Bethe states. Parallels are also drawn to the comparison with the superintegrable chiral Potts model.Comment: Latex 33 Pages; Typos and errors corrected, New improved version by adding explanations for better presentation. Terminology in the content and the title refined. References added and updated-Journal versio
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