1,193 research outputs found

    The exponential map for representations of Up,q(gl(2))U_{p,q}(gl(2))

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    For the quantum group GLp,q(2)GL_{p,q}(2) and the corresponding quantum algebra Up,q(gl(2))U_{p,q}(gl(2)) Fronsdal and Galindo explicitly constructed the so-called universal TT-matrix. In a previous paper we showed how this universal TT-matrix can be used to exponentiate representations from the quantum algebra to get representations (left comodules) for the quantum group. Here, further properties of the universal TT-matrix are illustrated. In particular, it is shown how to obtain comodules of the quantum algebra by exponentiating modules of the quantum group. Also the relation with the universal RR-matrix is discussed.Comment: LaTeX-file, 7 pages. Submitted for the Proceedings of the 4th International Colloquium ``Quantum Groups and Integrable Systems,'' Prague, 22-24 June 199

    The quantum superalgebra Uq[osp(1/2n)]U_q[osp(1/2n)]: deformed para-Bose operators and root of unity representations

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    We recall the relation between the Lie superalgebra osp(1/2n)osp(1/2n) and para-Bose operators. The quantum superalgebra Uq[osp(1/2n)]U_q[osp(1/2n)], defined as usual in terms of its Chevalley generators, is shown to be isomorphic to an associative algebra generated by so-called pre-oscillator operators satisfying a number of relations. From these relations, and the analogue with the non-deformed case, one can interpret these pre-oscillator operators as deformed para-Bose operators. Some consequences for Uq[osp(1/2n)]U_q[osp(1/2n)] (Cartan-Weyl basis, Poincar\'e-Birkhoff-Witt basis) and its Hopf subalgebra Uq[gl(n)]U_q[gl(n)] are pointed out. Finally, using a realization in terms of ``qq-commuting'' qq-bosons, we construct an irreducible finite-dimensional unitary Fock representation of Uq[osp(1/2n)]U_q[osp(1/2n)] and its decomposition in terms of Uq[gl(n)]U_q[gl(n)] representations when qq is a root of unity.Comment: 15 pages, LaTeX (latex twice), no figure

    Unitarizable Representations of the Deformed Para-Bose Superalgebra Uq[osp(1/2)] at Roots of 1

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    The unitarizable irreps of the deformed para-Bose superalgebra pBqpB_q, which is isomorphic to Uq[osp(1/2)]U_q[osp(1/2)], are classified at qq being root of 1. New finite-dimensional irreps of Uq[osp(1/2)]U_q[osp(1/2)] are found. Explicit expressions for the matrix elements are written down.Comment: 19 pages, PlainTe

    Dynamics in a noncommutative phase space

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    Dynamics has been generalized to a noncommutative phase space. The noncommuting phase space is taken to be invariant under the quantum group GLq,p(2)GL_{q,p}(2). The qq-deformed differential calculus on the phase space is formulated and using this, both the Hamiltonian and Lagrangian forms of dynamics have been constructed. In contrast to earlier forms of qq-dynamics, our formalism has the advantage of preserving the conventional symmetries such as rotational or Lorentz invariance.Comment: LaTeX-twice, 16 page

    Real Space Renormalization Group Study of the S=1/2 XXZ Chains with Fibonacci Exchange Modulation

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    Ground state properties of the S=1/2 antiferromagnetic XXZ chain with Fibonacci exchange modulation are studied using the real space renormalization group method for strong modulation. The quantum dynamical critical behavior with a new universality class is predicted in the isotropic case. Combining our results with the weak coupling renormalization group results by Vidal et al., the ground state phase diagram is obtained.Comment: 9 pages, 9 figure

    Quantum critical behavior of disordered itinerant ferromagnets

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    The quantum ferromagnetic transition at zero temperature in disordered itinerant electron systems is considered. Nonmagnetic quenched disorder leads to diffusive electron dynamics that induces an effective long-range interaction between the spin or order parameter fluctuations of the form r^{2-2d}, with d the spatial dimension. This leads to unusual scaling behavior at the quantum critical point, which is determined exactly. In three-dimensional systems the quantum critical exponents are substantially different from their finite temperature counterparts, a difference that should be easily observable. Experiments to check these predictions are proposed.Comment: 14pp., REVTeX, 3 eps figs, final version as publishe
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