54 research outputs found

    Bimodule structure of the mixed tensor product over Uqsℓ(2∣1)U_{q} s\ell(2|1) and quantum walled Brauer algebra

    Full text link
    We study a mixed tensor product 3⊗m⊗3‾⊗n\mathbf{3}^{\otimes m} \otimes \mathbf{\overline{3}}^{\otimes n} of the three-dimensional fundamental representations of the Hopf algebra Uqsℓ(2∣1)U_{q} s\ell(2|1), whenever qq is not a root of unity. Formulas for the decomposition of tensor products of any simple and projective Uqsℓ(2∣1)U_{q} s\ell(2|1)-module with the generating modules 3\mathbf{3} and 3‾\mathbf{\overline{3}} are obtained. The centralizer of Uqsℓ(2∣1)U_{q} s\ell(2|1) on the chain is calculated. It is shown to be the quotient Xm,n\mathscr{X}_{m,n} of the quantum walled Brauer algebra. The structure of projective modules over Xm,n\mathscr{X}_{m,n} is written down explicitly. It is known that the walled Brauer algebras form an infinite tower. We have calculated the corresponding restriction functors on simple and projective modules over Xm,n\mathscr{X}_{m,n}. This result forms a crucial step in decomposition of the mixed tensor product as a bimodule over Xm,n⊠Uqsℓ(2∣1)\mathscr{X}_{m,n}\boxtimes U_{q} s\ell(2|1). We give an explicit bimodule structure for all m,nm,n.Comment: 43 pages, 5 figure

    BRST Formalism and Zero Locus Reduction

    Get PDF
    In the BRST quantization of gauge theories, the zero locus ZQZ_Q of the BRST differential QQ carries an (anti)bracket whose parity is opposite to that of the fundamental bracket. We show that the on-shell BFV/BV gauge symmetries are in a 1:1 correspondence with Hamiltonian vector fields on ZQZ_Q, and observables of the BRST theory are in a 1:1 correspondence with characteristic functions of the bracket on ZQZ_Q. By reduction to the zero locus, we obtain relations between bracket operations and differentials arising in different complexes (the Gerstenhaber, Schouten, Berezin-Kirillov, and Sklyanin brackets); the equation ensuring the existence of a nilpotent vector field on the reduced manifold can be the classical Yang-Baxter equation. We also generalize our constructions to the bi-QP-manifolds which from the BRST theory viewpoint corresponds to the BRST-anti-BRST-symmetric quantization.Comment: 21 pages, latex2e, several modifications have been made, main content remains unchange
    • …
    corecore