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(1,0) superconformal models in six dimensions

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TLDR
In this article, a superconformal model with non-abelian gauge couplings for multiple tensor multiplets was constructed and the model was perturbatively defined only in the spontaneously broken phase with the vev of the tensor multiplet scalars serving as the inverse coupling constants of the Yang-Mills multiplet.
Abstract
We construct six-dimensional (1,0) superconformal models with non-abelian gauge couplings for multiple tensor multiplets. A crucial ingredient in the construction is the introduction of three-form gauge potentials which communicate degrees of freedom between the tensor multiplets and the Yang-Mills multiplet, but do not introduce additional degrees of freedom. Generically these models provide only equations of motions. For a subclass also a Lagrangian formulation exists, however it appears to exhibit indefinite metrics in the kinetic sector. We discuss several examples and analyze the excitation spectra in their supersymmetric vacua. In general, the models are perturbatively defined only in the spontaneously broken phase with the vev of the tensor multiplet scalars serving as the inverse coupling constants of the Yang-Mills multiplet. We briefly discuss the inclusion of hypermultiplets which complete the field content to that of superconformal (2,0) theories.

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All AdS7 solutions of type II supergravity

TL;DR: In this article, a pure spinor approach reminiscent of generalized complex geometry is used to determine uniquely the form of the metric and uxes, up to solving a system of ODEs.
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All AdS_7 solutions of type II supergravity

TL;DR: In this paper, a pure spinor approach reminiscent of generalized complex geometry is used to find supersymmetric solutions of the type AdS_7 x M_3 in type II supergravity.
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Anomaly polynomial of general 6D SCFTs

TL;DR: In this article, the authors describe a method to determine the anomaly polynomials of general 6d N=(2,0) and N=(1-0) SCFTs, in terms of the anomaly matching on their tensor branches.
Journal ArticleDOI

Spinorial geometry, horizons and superconformal symmetry in six dimensions

TL;DR: In this paper, the spinorial geometry method of solving the Killing spinor equations is reviewed as it applies to six-dimensional (1-0) supergravity, and the method is used to identify both the fractions of supersymmetry preserved by and the geometry of all supersymmetric backgrounds.
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Multiple membranes in M-theory

TL;DR: In this article, the authors review developments in the theory of multiple, parallel membranes in M-theory and introduce 3-algebras, leading to distinct classes of 2+1 dimensional theories with varying degrees of supersymmetry.
References
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N=6 superconformal Chern-Simons-matter theories, M2-branes and their gravity duals

TL;DR: In this paper, the authors constructed three dimensional Chern-Simons-matter theories with gauge groups U(N) × U(n) and SU(N), SU(2) × SU (2) which have explicit = 6 superconformal symmetry.
Journal ArticleDOI

Gauge symmetry and supersymmetry of multiple M2-branes

Jonathan Bagger, +1 more
- 07 Mar 2008 - 
TL;DR: In this article, a supersymmetric field theory model for multiple M2-branes based on an algebra with a totally antisymmetric triple product is proposed. But the field is not dynamical.
Journal ArticleDOI

Algebraic structures on parallel M2-branes

Andreas Gustavsson
- 11 Apr 2009 - 
TL;DR: In this article, the authors assume a certain algebraic structure for the low energy theory living on parallel M2 branes, and assume a topological degree-of-freedom field with topological degrees of freedom.

Some Comments On String Dynamics

Edward Witten
TL;DR: In this paper, a self-dual non-critical string appears in Type IIB superstring theory at points in the moduli space where the Type IIA theory has extended gauge symmetry.
Journal ArticleDOI

A Note on the Green - Schwarz Mechanism in Open - String Theories

TL;DR: In this article, the Green-Schwarz mechanism can take a generalized form, resulting from the combined action of all the antisymmetric tensors, and some of their implications for the low-energy effective field theory are pointed out.
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