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Related papers: A 6D nonabelian $(1,0)$ Theory

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We construct a general nonabelian (1,0) tensor multiplet theory in six dimensions. The gauge field of this (1,0) theory is non-dynamical, and the theory contains a continuous parameter $b$. When $b=1/2$, the (1,0) theory possesses an extra…

High Energy Physics - Theory · Physics 2014-03-25 Fa-Min Chen

We construct a class of nonabelian superconformal (1,0) hypermultiplet theories in six dimensions by introducing an abelian auxiliary field. The gauge fields of this class of theories are non-dynamical, and this class of theories can be…

High Energy Physics - Theory · Physics 2018-01-08 Fa-Min Chen

Using 3-algebras we obtain a nonabelian system of equations that furnish a representation of the (2,0)-supersymmetric tensor multiplet. The on-shell conditions are quite restrictive so that the system can be reduced to five-dimensional…

High Energy Physics - Theory · Physics 2014-11-21 Neil Lambert , Constantinos Papageorgakis

We show that the (1,0) tensor and hypermultiplet supersymmetry variations can be uplifted to loop space. Upon dimensional reduction we make contact with abelian five-dimensional super Yang-Mills, which has a nonabelian generalization that…

High Energy Physics - Theory · Physics 2024-07-23 Dongsu Bak , Andreas Gustavsson

We present an action for a six-dimensional superconformal field theory containing a non-abelian tensor multiplet. All of the ingredients of this action have been available in the literature. We bring these pieces together by choosing the…

High Energy Physics - Theory · Physics 2018-04-06 Christian Saemann , Lennart Schmidt

We compactify the abelian 6d (1,0) tensor multiplet on a circle bundle, thus reducing the theory down to 5d SYM while keeping all the KK modes. This abelian classical field theory, when interpreted suitably, has a nonlocal superconformal…

High Energy Physics - Theory · Physics 2019-02-20 Andreas Gustavsson

We construct six-dimensional superconformal models with non-abelian tensor and hypermultiplets. They describe the field content of (2,0) theories, coupled to (1,0) vector multiplets. The latter are part of the non-abelian gauge structure…

High Energy Physics - Theory · Physics 2015-06-12 Henning Samtleben , Ergin Sezgin , Robert Wimmer

We present a six-dimensional $\mathcal{N}=(1,0)$ supersymmetric higher gauge theory in which self-duality is consistently implemented by physically trivial additional fields. The action contains both $\mathcal{N}=(1,0)$ tensor and vector…

High Energy Physics - Theory · Physics 2021-06-09 Dominik Rist , Christian Saemann , Miro van der Worp

We study six-dimensional N=(1,0) supergravity theories with abelian, as well as non-abelian, gauge group factors. We show that for theories with fewer than nine tensor multiplets, the number of possible combinations of gauge groups -…

High Energy Physics - Theory · Physics 2012-06-13 Daniel S. Park , Washington Taylor

We make the observation that M-brane models defined in terms of 3-algebras can be interpreted as higher gauge theories involving Lie 2-groups. Such gauge theories arise in particular in the description of non-abelian gerbes. This…

High Energy Physics - Theory · Physics 2012-07-10 Sam Palmer , Christian Saemann

We construct gauge theories with a vector-multiplet and hypermultiplets of $(1,0)$ supersymmetry on the six-sphere. The gauge coupling on the sphere depends on the polar angle. This has a natural explanation in terms of the tensor branch of…

High Energy Physics - Theory · Physics 2019-01-09 Usman Naseer

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…

High Energy Physics - Theory · Physics 2015-05-30 Henning Samtleben , Ergin Sezgin , Robert Wimmer

A manifestly invariant renormalization scheme of N=1 nonabelian supersymmetric gauge theories is proposed.

High Energy Physics - Theory · Physics 2009-11-10 A. A. Slavnov , K. V. Stepanyantz

In D=10 N=1 super Yang-Mills theory we give the background breaking a half of supersymmetry. In the background there is a six-dimensional object so called D=10 5-brane.

High Energy Physics - Theory · Physics 2009-10-31 Yoshinori Gotoh , Ikuo Okouchi

We employ the harmonic superspace methods to study a six-dimensional $\mathcal{N}=(1,0)$ supersymmetric gauge theory with higher derivatives coupled to a hypermultiplet in the adjoint representation. By introducing a novel non-minimal…

High Energy Physics - Theory · Physics 2026-05-20 I. L. Buchbinder , A. S. Budekhina , E. A. Ivanov , K. V. Stepanyantz

With the aim to study six-dimensional (2,0) superconformal theories with non-Abelian tensor multiplets we propose a five-dimensional superconformal action with eight supersymmetries for an infinite tower of non-Abelian vector, tensor and…

High Energy Physics - Theory · Physics 2015-06-11 Federico Bonetti , Thomas W. Grimm , Stefan Hohenegger

We consider $6D$, ${\cal N}=(1,1)$ supersymmetric Yang-Mills theory formulated in ${\cal N}=(1,0)$ harmonic superspace and analyze the structure of the two-loop divergences in the hypermultiplet sector. Using the ${\cal N}=(1,0)$ superfield…

High Energy Physics - Theory · Physics 2018-02-01 I. L. Buchbinder , E. A. Ivanov , B. S. Merzlikin , K. V. Stepanyantz

We assume the existence of a background vector field that enables us to make an ansatz for the superconformal transformations for the non-Abelian 6d $(1,0)$ tensor multiplet. Closure of supersymmetry on generators of the conformal algebra,…

High Energy Physics - Theory · Physics 2018-08-15 Andreas Gustavsson

We carry out the N=1 supersymmetrization of a physical non-Abelian tensor with non-trivial consistent couplings in four dimensions. Our system has three multiplets: (i) The usual non-Abelian vector multiplet (VM) (A_\mu{}^I, \lambda^I),…

High Energy Physics - Theory · Physics 2015-06-04 Hitoshi Nishino , Subhash Rajpoot

We exploit the $6D, {\cal N}=(1,0)$ and ${\cal N}=(1,1)$ harmonic superspace approaches to construct the full set of the maximally supersymmetric on-shell invariants of the canonical dimension ${\bf d=12}$ in $6D, \,{\cal N}=(1,1)$…

High Energy Physics - Theory · Physics 2021-08-18 Serafim Buyucli , Evgeny Ivanov
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