Symmetries of N $$ \mathcal{N} $$ = (1, 0) supergravity backgrounds in six dimensions

Abstract General N $$ \mathcal{N} $$ = (1, 0) supergravity-matter systems in six dimensions may be described using one of the two fully fledged superspace formulations for conformal supergravity: (i) SU(2) superspace; and (ii) conformal superspace. With motivation to develop rigid supersymmetric fie...

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Main Authors: Sergei M. Kuzenko, Ulf Lindström, Emmanouil S. N. Raptakis, Gabriele Tartaglino-Mazzucchelli
Format: Article
Language:English
Published: SpringerOpen 2021-03-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP03(2021)157
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spelling doaj-1d30cca299184f149c2d17e3686363e42021-03-21T12:07:47ZengSpringerOpenJournal of High Energy Physics1029-84792021-03-012021315310.1007/JHEP03(2021)157Symmetries of N $$ \mathcal{N} $$ = (1, 0) supergravity backgrounds in six dimensionsSergei M. Kuzenko0Ulf Lindström1Emmanouil S. N. Raptakis2Gabriele Tartaglino-Mazzucchelli3Department of Physics M013, The University of Western AustraliaDepartment of Physics, Faculty of Arts and Sciences, Middle East Technical UniversityDepartment of Physics M013, The University of Western AustraliaSchool of Mathematics and Physics, University of QueenslandAbstract General N $$ \mathcal{N} $$ = (1, 0) supergravity-matter systems in six dimensions may be described using one of the two fully fledged superspace formulations for conformal supergravity: (i) SU(2) superspace; and (ii) conformal superspace. With motivation to develop rigid supersymmetric field theories in curved space, this paper is devoted to the study of the geometric symmetries of supergravity backgrounds. In particular, we introduce the notion of a conformal Killing spinor superfield ϵ α , which proves to generate extended superconformal transformations. Among its cousins are the conformal Killing vector ξ a and tensor ζ a(n) superfields. The former parametrise conformal isometries of supergravity backgrounds, which in turn yield symmetries of every superconformal field theory. Meanwhile, the conformal Killing tensors of a given background are associated with higher symmetries of the hypermultiplet. By studying the higher symmetries of a non-conformal vector multiplet we introduce the concept of a Killing tensor superfield. We also analyse the problem of computing higher symmetries for the conformal d’Alembertian in curved space and demonstrate that, beyond the first-order case, these operators are defined only on a limited class of backgrounds, including all conformally flat ones.https://doi.org/10.1007/JHEP03(2021)157Extended SupersymmetryHigher Spin SymmetrySupergravity ModelsSuperspaces
collection DOAJ
language English
format Article
sources DOAJ
author Sergei M. Kuzenko
Ulf Lindström
Emmanouil S. N. Raptakis
Gabriele Tartaglino-Mazzucchelli
spellingShingle Sergei M. Kuzenko
Ulf Lindström
Emmanouil S. N. Raptakis
Gabriele Tartaglino-Mazzucchelli
Symmetries of N $$ \mathcal{N} $$ = (1, 0) supergravity backgrounds in six dimensions
Journal of High Energy Physics
Extended Supersymmetry
Higher Spin Symmetry
Supergravity Models
Superspaces
author_facet Sergei M. Kuzenko
Ulf Lindström
Emmanouil S. N. Raptakis
Gabriele Tartaglino-Mazzucchelli
author_sort Sergei M. Kuzenko
title Symmetries of N $$ \mathcal{N} $$ = (1, 0) supergravity backgrounds in six dimensions
title_short Symmetries of N $$ \mathcal{N} $$ = (1, 0) supergravity backgrounds in six dimensions
title_full Symmetries of N $$ \mathcal{N} $$ = (1, 0) supergravity backgrounds in six dimensions
title_fullStr Symmetries of N $$ \mathcal{N} $$ = (1, 0) supergravity backgrounds in six dimensions
title_full_unstemmed Symmetries of N $$ \mathcal{N} $$ = (1, 0) supergravity backgrounds in six dimensions
title_sort symmetries of n $$ \mathcal{n} $$ = (1, 0) supergravity backgrounds in six dimensions
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2021-03-01
description Abstract General N $$ \mathcal{N} $$ = (1, 0) supergravity-matter systems in six dimensions may be described using one of the two fully fledged superspace formulations for conformal supergravity: (i) SU(2) superspace; and (ii) conformal superspace. With motivation to develop rigid supersymmetric field theories in curved space, this paper is devoted to the study of the geometric symmetries of supergravity backgrounds. In particular, we introduce the notion of a conformal Killing spinor superfield ϵ α , which proves to generate extended superconformal transformations. Among its cousins are the conformal Killing vector ξ a and tensor ζ a(n) superfields. The former parametrise conformal isometries of supergravity backgrounds, which in turn yield symmetries of every superconformal field theory. Meanwhile, the conformal Killing tensors of a given background are associated with higher symmetries of the hypermultiplet. By studying the higher symmetries of a non-conformal vector multiplet we introduce the concept of a Killing tensor superfield. We also analyse the problem of computing higher symmetries for the conformal d’Alembertian in curved space and demonstrate that, beyond the first-order case, these operators are defined only on a limited class of backgrounds, including all conformally flat ones.
topic Extended Supersymmetry
Higher Spin Symmetry
Supergravity Models
Superspaces
url https://doi.org/10.1007/JHEP03(2021)157
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AT gabrieletartaglinomazzucchelli symmetriesofnmathcaln10supergravitybackgroundsinsixdimensions
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