Revisiting extremal couplings in AdS/CFT

Abstract We consider an effective theory of massive scalar fields on a fixed AdS d+1 background with a cubic extremal interaction among them. A bulk coupling is called extremal whenever the corresponding conformal dimension of any of the dual CFT d operators matches the sum of all the others. For cu...

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Main Authors: Alejandra Castro, Pedro J. Martinez
Format: Article
Language:English
Published: SpringerOpen 2024-12-01
Series:Journal of High Energy Physics
Subjects:
Online Access:https://doi.org/10.1007/JHEP12(2024)157
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author Alejandra Castro
Pedro J. Martinez
author_facet Alejandra Castro
Pedro J. Martinez
author_sort Alejandra Castro
collection DOAJ
description Abstract We consider an effective theory of massive scalar fields on a fixed AdS d+1 background with a cubic extremal interaction among them. A bulk coupling is called extremal whenever the corresponding conformal dimension of any of the dual CFT d operators matches the sum of all the others. For cubic bulk couplings, this is ∆ i + ∆ j = ∆ k . These bulk interactions are often disregarded in the literature since they do not appear in traditional models of AdS/CFT. Turning them on yields a divergent vertex in the dual CFT, and here we show that these divergences can be regulated. Once renormalized, we demonstrate that this coupling introduces non-trivial mixing between single- and double-trace operators, and we compute the anomalous dimensions of the corrected operators to leading order in perturbation theory.
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spelling doaj-art-746b2326eb924ac1b3cb8d610398741b2025-01-05T12:05:56ZengSpringerOpenJournal of High Energy Physics1029-84792024-12-0120241213310.1007/JHEP12(2024)157Revisiting extremal couplings in AdS/CFTAlejandra Castro0Pedro J. Martinez1Department of Applied Mathematics and Theoretical Physics, University of CambridgeInstituto de Física La Plata — CONICET, Universidad Nacional de La PlataAbstract We consider an effective theory of massive scalar fields on a fixed AdS d+1 background with a cubic extremal interaction among them. A bulk coupling is called extremal whenever the corresponding conformal dimension of any of the dual CFT d operators matches the sum of all the others. For cubic bulk couplings, this is ∆ i + ∆ j = ∆ k . These bulk interactions are often disregarded in the literature since they do not appear in traditional models of AdS/CFT. Turning them on yields a divergent vertex in the dual CFT, and here we show that these divergences can be regulated. Once renormalized, we demonstrate that this coupling introduces non-trivial mixing between single- and double-trace operators, and we compute the anomalous dimensions of the corrected operators to leading order in perturbation theory.https://doi.org/10.1007/JHEP12(2024)157AdS-CFT CorrespondenceGauge-Gravity Correspondence
spellingShingle Alejandra Castro
Pedro J. Martinez
Revisiting extremal couplings in AdS/CFT
Journal of High Energy Physics
AdS-CFT Correspondence
Gauge-Gravity Correspondence
title Revisiting extremal couplings in AdS/CFT
title_full Revisiting extremal couplings in AdS/CFT
title_fullStr Revisiting extremal couplings in AdS/CFT
title_full_unstemmed Revisiting extremal couplings in AdS/CFT
title_short Revisiting extremal couplings in AdS/CFT
title_sort revisiting extremal couplings in ads cft
topic AdS-CFT Correspondence
Gauge-Gravity Correspondence
url https://doi.org/10.1007/JHEP12(2024)157
work_keys_str_mv AT alejandracastro revisitingextremalcouplingsinadscft
AT pedrojmartinez revisitingextremalcouplingsinadscft