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Related papers: NB BLG model in N=8 superfields

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We give a brief review of Bagger-Lambert-Gustavsson (BLG) model, with emphasis on its version invariant under the volume preserving diffeomorphisms (SDiff3) symmetry. We describe the on-shell superfield formulation of this SDiff3 BLG model…

High Energy Physics - Theory · Physics 2010-04-14 Igor A. Bandos

We reformulate the Bagger-Lambert-Gustavsson model using an N=8 superspace, thus making the full supersymmetry manifest. The formulation is based on appropriate "pure spinor wave functions" for the Chern-Simons and matter multiplets. The…

High Energy Physics - Theory · Physics 2009-12-07 Martin Cederwall

This paper is concerned with the problem of coupling the N=8 superconformal Bagger-Lambert-Gustavsson (BLG) theory to N=8 conformal supergravity in three dimensions. We start by constructing the on-shell N=8 conformal supergravity in three…

High Energy Physics - Theory · Physics 2009-11-13 Ulf Gran , Bengt E. W. Nilsson

We consider three-dimensional maximally superconformal Bagger-Lambert-Gustavsson (BLG) theory and its topologically gauged version (constructed recently in arXiv:0809.4478 [hep-th]) in the light-cone gauge. After eliminating the entire…

High Energy Physics - Theory · Physics 2010-01-05 Bengt E. W. Nilsson

We construct some examples of D=3, N=4 GW theory and N=5 superconformal Chern-Simons matter theory by using the covariantly constant curvature of a quaternionic-Kahler manifold to construct the symplectic 3-algebra in the theories.…

High Energy Physics - Theory · Physics 2012-03-30 Fa-Min Chen

We present a Lagrangian formulation for ${\cal N}=8$ superconformal field theories in three spacetime dimensions that is general enough to encompass infinite-dimensional gauge algebras that generally go beyond Lie algebras. To this end we…

High Energy Physics - Theory · Physics 2019-05-01 Olaf Hohm , Henning Samtleben

We elaborate on the suggestion made in arXiv:0806.3498 that the 3d \N=8 superconformal SU(N) Chern-Simons-matter theory of Lorentzian Bagger-Lambert-Gustavson type (L-BLG) can be obtained by a scaling limit (involving sending the level k to…

High Energy Physics - Theory · Physics 2009-02-20 E. Antonyan , A. A. Tseytlin

We use superalgebras to realize the 3-algebras used to construct N=6, 8 Chern-Simons-matter (CSM) theories. We demonstrate that the superalgebra realization of the 3-algebras provides a unified framework for classifying the gauge groups of…

High Energy Physics - Theory · Physics 2012-03-30 Fa-Min Chen

Recently it was proposed that the Bagger-Lambert-Gustavsson theory with Nambu-Poisson structure describes an M5-brane in a three-form flux background. In this paper we investigate the superalgebra associated with this theory. We derive the…

High Energy Physics - Theory · Physics 2010-05-12 Andrew M. Low

Maximally supersymmetric mass deformation of the Bagger-Lambert-Gustavsson (BLG) theory corresponds to a {non-central} extension of the d=3 N=8 Poincare superalgebra (allowed in three dimensions). We obtain its light-cone superspace…

High Energy Physics - Theory · Physics 2014-11-21 Dmitry V. Belyaev

The light-cone superspace version of the d=3, N=8 superconformal theory of Bagger, Lambert and Gustavsson (BLG) is obtained as a solution to constraints imposed by OSp(2,2|8) superalgebra. The Hamiltonian of the theory is shown to be a…

High Energy Physics - Theory · Physics 2010-05-07 Dmitry Belyaev , Lars Brink , Sung-Soo Kim , Pierre Ramond

Based on the realization of three-algebras in terms of algebra of matrices and four-brackets [arXiv:0807.1570] we present the notion of u(N)-based extended three-algebras, which for N=2 reproduces the Bagger-Lambert three-algebra. Using…

High Energy Physics - Theory · Physics 2009-01-22 M. M. Sheikh-Jabbari

The recently formulated Bagger-Lambert-Gustavsson (BLG) theory in three dimensions is described in terms of a constrained chiral superfield in light-cone superspace. We discuss the use of Superconformal symmetry to determine the form of its…

High Energy Physics - Theory · Physics 2010-02-16 Pierre Ramond

The Bagger-Lambert-Gustavsson theory is coupled to an off-shell D=3, N=8 conformal supergravity background. Local transformation laws of the conformal supergravity multiplet are obtained from those of the D=4, N=8 SO(8) gauged supergravity.…

High Energy Physics - Theory · Physics 2015-06-05 M. Nishimura , Y. Tanii

We show that an infinite family of N=6 d=3 superconformal Chern-Simons-matter theories has hidden N=8 superconformal symmetry and hidden parity on the quantum level. This family of theories is different from the one found by Aharony,…

High Energy Physics - Theory · Physics 2015-05-27 Denis Bashkirov , Anton Kapustin

We consider dimensional reduction of the Bagger-Lambert-Gustavsson theory to a zero-dimensional 3-Lie algebra model and construct various stable solutions corresponding to quantized Nambu-Poisson manifolds. A recently proposed Higgs…

High Energy Physics - Theory · Physics 2011-04-21 Joshua DeBellis , Christian Saemann , Richard J. Szabo

A Lagrangian description of a maximally supersymmetric conformal field theory in three dimensions was constructed recently by Bagger and Lambert (BL). The BL theory has SO(4) gauge symmetry and contains scalar and spinor fields that…

High Energy Physics - Theory · Physics 2009-07-09 Miguel A. Bandres , Arthur E. Lipstein , John H. Schwarz

We generalize the suggestion presented in arXiv:0806.3498 that the 3d N=8 superconformal SU(N) Chern-Simons-matter theory of Lorentzian Bagger-Lambert-Gustavson type (L-BLG) can be obtained through the scaling limit from N=6 superconformal…

High Energy Physics - Theory · Physics 2009-05-01 J. Kluson

We show that the N=8 superconformal Bagger-Lambert theory based on the Lorentzian 3-algebra can be derived by taking a certain scaling limit of the recently proposed N=6 superconformal U(N)xU(N) Chern-Simons-matter theories at level (k,…

High Energy Physics - Theory · Physics 2008-12-18 Yoshinori Honma , Satoshi Iso , Yoske Sumitomo , Sen Zhang

We present a systematic analysis of the N=8 superspace constraints in three space-time dimensions. The general coupling between vector and scalar supermultiplets is encoded in an SO(8) tensor W_{AB} which is a function of the matter fields…

High Energy Physics - Theory · Physics 2010-03-17 Henning Samtleben , Robert Wimmer
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