931 research outputs found

    M2-Branes in N=3 Harmonic Superspace

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    We give a brief account of the recently proposed N=3 superfield formulation of the N=6, 3D superconformal theory of Aharony et al (ABJM) describing a low-energy limit of the system of multiple M2-branes on the AdS_4 x S^7/Z_k background. This formulation is given in harmonic N=3 superspace and reveals a number of surprising new features. In particular, the sextic scalar potential of ABJM arises at the on-shell component level as the result of eliminating appropriate auxiliary fields, while there is no any explicit superpotential at the off-shell superfield level.Comment: 9 pages, Talk at the Conference "Selected Topics in Mathematical and Particle Physics", In Honor of the 70-th Birthday of Jiri Niederle, Prague, 5 - 7 May 2009; the version published in the proceeding

    Harmonic Superfields in N=4 Supersymmetric Quantum Mechanics

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    This is a brief survey of applications of the harmonic superspace methods to the models of N=4 supersymmetric quantum mechanics (SQM). The main focus is on a recent progress in constructing SQM models with couplings to the background non-Abelian gauge fields. Besides reviewing and systemizing the relevant results, we present some new examples and make clarifying comments

    Quaternion-K\"ahler N=4 Supersymmetric Mechanics

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    Using the N=4, 1D harmonic superspace approach, we construct a new type of N=4 supersymmetric mechanics involving 4n-dimensional Quaternion-K\"ahler (QK) 1D sigma models as the bosonic core. The basic ingredients of our construction are {\it local} N=4, 1D supersymmetry realized by the appropriate transformations in 1D harmonic superspace, the general N=4, 1D superfield vielbein and a set of 2(n+1) analytic "matter" superfields representing (n+1) off-shell supermultiplets (4, 4, 0). Both superfield and component actions are given for the simplest QK models with the manifolds \mathbb{H}H^n = Sp(1,n)/[Sp(1) x Sp(n)] and \mathbb{H}P^n = Sp(1+n)/[Sp(1) x Sp(n)] as the bosonic targets. For the general case the relevant superfield action and constraints on the (4, 4, 0) "matter" superfields are presented. Further generalizations are briefly discussed.Comment: further minor corrections in eqs. (2.21), (4.24) and (A9

    Higher Spins from Nonlinear Realizations of OSp(18)OSp(1|8)

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    We exhibit surprising relations between higher spin theory and nonlinear realizations of the supergroup OSp(18)OSp(1|8), a minimal superconformal extension of N=1, 4D supersymmetry with tensorial charges. We construct a realization of OSp(18)OSp(1|8) on the coset supermanifold OSp(18)/SL(4,R)OSp(1|8)/SL(4,R) which involves the tensorial superspace R(104)R^{(10|4)} and Goldstone superfields given on it. The covariant superfield equation encompassing the component ones for all integer and half-integer massless higher spins amounts to the vanishing of covariant spinor derivatives of the suitable Goldstone superfields, and, via Maurer-Cartan equations, to the vanishing of SL(4,R)SL(4,R) supercurvature in odd directions of R(104)R^{(10|4)}. Aiming at higher spin extension of the Ogievetsky-Sokatchev formulation of N=1 supergravity, we generalize the notion of N=1 chirality and construct first examples of invariant superfield actions involving a non-trivial interaction. Some other potential implications of OSp(18)OSp(1|8) in the proposed setting are briefly outlined.Comment: LaTeX, 13 pages. Minor, mostly typographic corrections. Version which appears in Physics Letters

    OSp(4|2) Superconformal Mechanics

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    A new superconformal mechanics with OSp(4|2) symmetry is obtained by gauging the U(1) isometry of a superfield model. It is the one-particle case of the new N=4 super Calogero model recently proposed in arXiv:0812.4276 [hep-th]. Classical and quantum generators of the osp(4|2) superalgebra are constructed on physical states. As opposed to other realizations of N=4 superconformal algebras, all supertranslation generators are linear in the odd variables, similarly to the N=2 case. The bosonic sector of the component action is standard one-particle (dilatonic) conformal mechanics accompanied by an SU(2)/U(1) Wess-Zumino term, which gives rise to a fuzzy sphere upon quantization. The strength of the conformal potential is quantized.Comment: 1+20 pages, v2: typos fixed, for publication in JHE

    From N=4\mathcal{N}{=}\,4 Galilean superparticle to three-dimensional non-relativistic N=4\mathcal{N}{=}\,4 superfields

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    We consider the general N=4,\mathcal{N}{=}\,4, d=3d{=}\,3 Galilean superalgebra with arbitrary central charges and study its dynamical realizations. Using the nonlinear realization techniques, we introduce a class of actions for N=4\mathcal{N}{=}\,4 three-dimensional non-relativistic superparticle, such that they are linear in the central charge Maurer-Cartan one-forms. As a prerequisite to the quantization, we analyze the phase space constraints structure of our model for various choices of the central charges. The first class constraints generate gauge transformations, involving fermionic κ\kappa-gauge transformations. The quantization of the model gives rise to the collection of free N=4\mathcal{N}{=}\,4, d=3d{=}\,3 Galilean superfields, which can be further employed, e.g., for description of three-dimensional non-relativistic N=4\mathcal{N}{=}\,4 supersymmetric theories.Comment: 1 + 39 pages; v2: minor corrections in few formulas and many language corrections without any impact on the results; one reference and two footnotes adde

    Resolutions of mesh algebras: periodicity and Calabi-Yau dimensions

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    A triangulated category is said to be Calabi-Yau of dimension d if the dth power of its suspension is a Serre functor. We determine which stable categories of self-injective algebras A of finite representation type are Calabi-Yau and compute their Calabi-Yau dimensions. We achieve this by studying the minimal projective resolution of the stable Auslander algebra of A over its enveloping algebra, and use covering theory to reduce to (generalized) preprojective algebras of Dynkin graphs. We also describe how this problem can be approached by realizing the stable categories in question as orbit categories of the bounded derived categories of hereditary algebras.Comment: Final version. To appear in Math.
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