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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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 |
work_keys_str_mv |
AT sergeimkuzenko symmetriesofnmathcaln10supergravitybackgroundsinsixdimensions AT ulflindstrom symmetriesofnmathcaln10supergravitybackgroundsinsixdimensions AT emmanouilsnraptakis symmetriesofnmathcaln10supergravitybackgroundsinsixdimensions AT gabrieletartaglinomazzucchelli symmetriesofnmathcaln10supergravitybackgroundsinsixdimensions |
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