AdS8 solutions in type II supergravity

Abstract We find non-supersymmetric AdS8 solutions of type IIA supergravity. The internal space is topologically an S 2 with a U(1) isometry. The only non-zero flux is F 0; an O8 sourcing it is present at the equator of the S 2. The warping function and dilaton are non-constant. It is also possible...

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Main Authors: Clay Córdova, G. Bruno De Luca, Alessandro Tomasiello
Format: Article
Language:English
Published: SpringerOpen 2019-07-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP07(2019)127
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author Clay Córdova
G. Bruno De Luca
Alessandro Tomasiello
author_facet Clay Córdova
G. Bruno De Luca
Alessandro Tomasiello
author_sort Clay Córdova
collection DOAJ
description Abstract We find non-supersymmetric AdS8 solutions of type IIA supergravity. The internal space is topologically an S 2 with a U(1) isometry. The only non-zero flux is F 0; an O8 sourcing it is present at the equator of the S 2. The warping function and dilaton are non-constant. It is also possible to add D8-branes on top of the O8. Possible destabilizing brane bubbles (whose presence would be suggested by the weak-gravity conjecture) are either absent or collapsing. Our solutions are candidate holographic duals to unitary interacting CFTs in seven dimensions with exceptional global symmetry. We also present analogous non-supersymmetric AdS d solutions for general d which are supported only by F 0.
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spelling doaj.art-065aaeeaa84b40e0a0983a02ad88ab0a2022-12-21T19:17:05ZengSpringerOpenJournal of High Energy Physics1029-84792019-07-012019712410.1007/JHEP07(2019)127AdS8 solutions in type II supergravityClay Córdova0G. Bruno De Luca1Alessandro Tomasiello2School of Natural Sciences, Institute for Advanced StudyDipartimento di Fisica, Università di Milano-BicoccaDipartimento di Fisica, Università di Milano-BicoccaAbstract We find non-supersymmetric AdS8 solutions of type IIA supergravity. The internal space is topologically an S 2 with a U(1) isometry. The only non-zero flux is F 0; an O8 sourcing it is present at the equator of the S 2. The warping function and dilaton are non-constant. It is also possible to add D8-branes on top of the O8. Possible destabilizing brane bubbles (whose presence would be suggested by the weak-gravity conjecture) are either absent or collapsing. Our solutions are candidate holographic duals to unitary interacting CFTs in seven dimensions with exceptional global symmetry. We also present analogous non-supersymmetric AdS d solutions for general d which are supported only by F 0.http://link.springer.com/article/10.1007/JHEP07(2019)127AdS-CFT CorrespondenceFlux compactificationsSupergravity Models
spellingShingle Clay Córdova
G. Bruno De Luca
Alessandro Tomasiello
AdS8 solutions in type II supergravity
Journal of High Energy Physics
AdS-CFT Correspondence
Flux compactifications
Supergravity Models
title AdS8 solutions in type II supergravity
title_full AdS8 solutions in type II supergravity
title_fullStr AdS8 solutions in type II supergravity
title_full_unstemmed AdS8 solutions in type II supergravity
title_short AdS8 solutions in type II supergravity
title_sort ads8 solutions in type ii supergravity
topic AdS-CFT Correspondence
Flux compactifications
Supergravity Models
url http://link.springer.com/article/10.1007/JHEP07(2019)127
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AT gbrunodeluca ads8solutionsintypeiisupergravity
AT alessandrotomasiello ads8solutionsintypeiisupergravity