488 research outputs found

    Invariant Differential Operators for Non-Compact Lie Groups: the Sp(n,R) Case

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    In the present paper we continue the project of systematic construction of invariant differential operators on the example of the non-compact algebras sp(n,R), in detail for n=6. Our choice of these algebras is motivated by the fact that they belong to a narrow class of algebras, which we call 'conformal Lie algebras', which have very similar properties to the conformal algebras of Minkowski space-time. We give the main multiplets and the main reduced multiplets of indecomposable elementary representations for n=6, including the necessary data for all relevant invariant differential operators. In fact, this gives by reduction also the cases for n<6, since the main multiplet for fixed n coincides with one reduced case for n+1.Comment: Latex2e, 27 pages, 8 figures. arXiv admin note: substantial text overlap with arXiv:0812.2690, arXiv:0812.265

    Atypical Representations of Uq(sl(N))U_{q}(sl(N)) at Roots of Unity

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    We show how to adapt the Gelfand-Zetlin basis for describing the atypical representation of Uq(sl(N)){\cal U}_{\displaystyle{q}}(sl(N)) when qq is root of unity. The explicit construction of atypical representation is presented in details for N=3N=3.Comment: 18 pages, Tex-file and 2 figures. Uuencoded, compressed and tared archive of plain tex file and postscript figure file. Upon uudecoding, uncompressing and taring, tex the file atypique.te

    Explicit Character Formulae for Positive Energy UIRs of D=4 Conformal Supersymmetry

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    This paper continues the project of constructing the character formulae for the positive energy unitary irreducible representations of the N-extended D=4 conformal superalgebras su(2,2/N). In the first paper we gave the bare characters which represent the defining odd entries of the characters. Now we give the full explicit character formulae for N=1 and for several important examples for N=2 and N=4.Comment: 48 pages, TeX with Harvmac, overlap in preliminaries with arXiv:hep-th/0406154; some comments and references adde

    Positive Energy Representations, Holomorphic Discrete Series and Finite-Dimensional Irreps

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    Let G be a semi-simple non-compact Lie group with unitary lowest/highest weight representations. We consider explicitly the relation between three types of representations of G: positive energy (unitary lowest weight)representations, (holomorphic) discrete series representations and non-unitary finite-dimensional irreps. We consider mainly the conformal groups SO(n,2) treating in full detail the cases n=1,3,4.Comment: 28 pages, TEX with Harvmac using amssym.def, amssym.tex, epsf.tex; v2: new texts in Sections 1 & 3, new refs; v3: added 5 figures; v4: small correction

    Duality for the Jordanian Matrix Quantum Group GLg,h(2)GL_{g,h}(2)

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    We find the Hopf algebra Ug,hU_{g,h} dual to the Jordanian matrix quantum group GLg,h(2)GL_{g,h}(2). As an algebra it depends only on the sum of the two parameters and is split in two subalgebras: Ug,hU'_{g,h} (with three generators) and U(Z)U(Z) (with one generator). The subalgebra U(Z)U(Z) is a central Hopf subalgebra of Ug,hU_{g,h}. The subalgebra Ug,hU'_{g,h} is not a Hopf subalgebra and its coalgebra structure depends on both parameters. We discuss also two one-parameter special cases: g=hg =h and g=hg=-h. The subalgebra Uh,hU'_{h,h} is a Hopf algebra and coincides with the algebra introduced by Ohn as the dual of SLh(2)SL_h(2). The subalgebra Uh,hU'_{-h,h} is isomorphic to U(sl(2))U(sl(2)) as an algebra but has a nontrivial coalgebra structure and again is not a Hopf subalgebra of Uh,hU_{-h,h}.Comment: plain TeX with harvmac, 16 pages, added Appendix implementing the ACC nonlinear ma

    Invariant Differential Operators and Characters of the AdS_4 Algebra

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    The aim of this paper is to apply systematically to AdS_4 some modern tools in the representation theory of Lie algebras which are easily generalised to the supersymmetric and quantum group settings and necessary for applications to string theory and integrable models. Here we introduce the necessary representations of the AdS_4 algebra and group. We give explicitly all singular (null) vectors of the reducible AdS_4 Verma modules. These are used to obtain the AdS_4 invariant differential operators. Using this we display a new structure - a diagram involving four partially equivalent reducible representations one of which contains all finite-dimensional irreps of the AdS_4 algebra. We study in more detail the cases involving UIRs, in particular, the Di and the Rac singletons, and the massless UIRs. In the massless case we discover the structure of sets of 2s_0-1 conserved currents for each spin s_0 UIR, s_0=1,3/2,... All massless cases are contained in a one-parameter subfamily of the quartet diagrams mentioned above, the parameter being the spin s_0. Further we give the classification of the so(5,C) irreps presented in a diagramatic way which makes easy the derivation of all character formulae. The paper concludes with a speculation on the possible applications of the character formulae to integrable models.Comment: 30 pages, 4 figures, TEX-harvmac with input files: amssym.def, amssym.tex, epsf.tex; version 2 1 reference added; v3: minor corrections; v.4: minor corrections, v.5: minor corrections to conform with version in J. Phys. A: Math. Gen; v.6.: small correction and addition in subsections 4.1 & 4.

    qq-Trinomial identities

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    We obtain connection coefficients between qq-binomial and qq-trinomial coefficients. Using these, one can transform qq-binomial identities into a qq-trinomial identities and back again. To demonstrate the usefulness of this procedure we rederive some known trinomial identities related to partition theory and prove many of the conjectures of Berkovich, McCoy and Pearce, which have recently arisen in their study of the ϕ2,1\phi_{2,1} and ϕ1,5\phi_{1,5} perturbations of minimal conformal field theory.Comment: 21 pages, AMSLate
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