N $$ \mathcal{N} $$ = 2 CFT3’s from N $$ \mathcal{N} $$ = 4 gauged supergravity
Abstract We use holography and four-dimensional N $$ \mathcal{N} $$ = 4 gauged supergravity to collect evidence for a large class of interconnected three-dimensional N $$ \mathcal{N} $$ = 2 conformal field theories. On the gravity side, we construct a one-parameter family of ISO(3) × ISO(3) gaugings...
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Format: | Article |
Language: | English |
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SpringerOpen
2023-06-01
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Series: | Journal of High Energy Physics |
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Online Access: | https://doi.org/10.1007/JHEP06(2023)068 |
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author | Miguel Chamorro-Burgos Adolfo Guarino Colin Sterckx |
author_facet | Miguel Chamorro-Burgos Adolfo Guarino Colin Sterckx |
author_sort | Miguel Chamorro-Burgos |
collection | DOAJ |
description | Abstract We use holography and four-dimensional N $$ \mathcal{N} $$ = 4 gauged supergravity to collect evidence for a large class of interconnected three-dimensional N $$ \mathcal{N} $$ = 2 conformal field theories. On the gravity side, we construct a one-parameter family of ISO(3) × ISO(3) gaugings of half-maximal supergravity containing a rich structure of N $$ \mathcal{N} $$ = 2 AdS4 solutions at fixed radius. By looking at excitations around these AdS4 solutions, the spectrum of low lying operators in the dual N $$ \mathcal{N} $$ = 2 CFT3’s is computed and further arranged into 𝔬𝔰(2|4) supermultiplets. Upon suitable removal of gauge redundancies, we identify the Zamolodchikov metric on the conformal manifold dual to the AdS4 moduli space, and recover previous results in the S-fold literature. Two special points of N $$ \mathcal{N} $$ = 4 supersymmetry enhancement occur. While one describes an S-fold CFT3 dual to a non-geometric type IIB twisted compactification, the string-theoretic realisation of the other, if any, is still lacking. |
first_indexed | 2024-03-11T22:20:11Z |
format | Article |
id | doaj.art-acd635b208334e21a73f085ba1ca263a |
institution | Directory Open Access Journal |
issn | 1029-8479 |
language | English |
last_indexed | 2024-03-11T22:20:11Z |
publishDate | 2023-06-01 |
publisher | SpringerOpen |
record_format | Article |
series | Journal of High Energy Physics |
spelling | doaj.art-acd635b208334e21a73f085ba1ca263a2023-09-24T11:06:52ZengSpringerOpenJournal of High Energy Physics1029-84792023-06-012023613910.1007/JHEP06(2023)068N $$ \mathcal{N} $$ = 2 CFT3’s from N $$ \mathcal{N} $$ = 4 gauged supergravityMiguel Chamorro-Burgos0Adolfo Guarino1Colin Sterckx2Departamento de Física, Universidad de OviedoDepartamento de Física, Universidad de OviedoUniversité Libre de Bruxelles (ULB) and International Solvay Institutes, Service de Physique Théorique et MathématiqueAbstract We use holography and four-dimensional N $$ \mathcal{N} $$ = 4 gauged supergravity to collect evidence for a large class of interconnected three-dimensional N $$ \mathcal{N} $$ = 2 conformal field theories. On the gravity side, we construct a one-parameter family of ISO(3) × ISO(3) gaugings of half-maximal supergravity containing a rich structure of N $$ \mathcal{N} $$ = 2 AdS4 solutions at fixed radius. By looking at excitations around these AdS4 solutions, the spectrum of low lying operators in the dual N $$ \mathcal{N} $$ = 2 CFT3’s is computed and further arranged into 𝔬𝔰(2|4) supermultiplets. Upon suitable removal of gauge redundancies, we identify the Zamolodchikov metric on the conformal manifold dual to the AdS4 moduli space, and recover previous results in the S-fold literature. Two special points of N $$ \mathcal{N} $$ = 4 supersymmetry enhancement occur. While one describes an S-fold CFT3 dual to a non-geometric type IIB twisted compactification, the string-theoretic realisation of the other, if any, is still lacking.https://doi.org/10.1007/JHEP06(2023)068Supergravity ModelsSuperstring VacuaAdS-CFT CorrespondenceExtended Supersymmetry |
spellingShingle | Miguel Chamorro-Burgos Adolfo Guarino Colin Sterckx N $$ \mathcal{N} $$ = 2 CFT3’s from N $$ \mathcal{N} $$ = 4 gauged supergravity Journal of High Energy Physics Supergravity Models Superstring Vacua AdS-CFT Correspondence Extended Supersymmetry |
title | N $$ \mathcal{N} $$ = 2 CFT3’s from N $$ \mathcal{N} $$ = 4 gauged supergravity |
title_full | N $$ \mathcal{N} $$ = 2 CFT3’s from N $$ \mathcal{N} $$ = 4 gauged supergravity |
title_fullStr | N $$ \mathcal{N} $$ = 2 CFT3’s from N $$ \mathcal{N} $$ = 4 gauged supergravity |
title_full_unstemmed | N $$ \mathcal{N} $$ = 2 CFT3’s from N $$ \mathcal{N} $$ = 4 gauged supergravity |
title_short | N $$ \mathcal{N} $$ = 2 CFT3’s from N $$ \mathcal{N} $$ = 4 gauged supergravity |
title_sort | n mathcal n 2 cft3 s from n mathcal n 4 gauged supergravity |
topic | Supergravity Models Superstring Vacua AdS-CFT Correspondence Extended Supersymmetry |
url | https://doi.org/10.1007/JHEP06(2023)068 |
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