AdS4/CFT3 for unprotected operators

Abstract We consider the four-point function of the lowest scalar in the stress-energy tensor multiplet in N=8 $$ \mathcal{N}=8 $$ ABJ(M) theory [1, 2]. At large central charge c T ∼ N 3/2, this correlator is given by the corresponding holographic correlation function in 11d supergravity on AdS 4 ×...

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Main Author: Shai M. Chester
Format: Article
Language:English
Published: SpringerOpen 2018-07-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP07(2018)030
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author Shai M. Chester
author_facet Shai M. Chester
author_sort Shai M. Chester
collection DOAJ
description Abstract We consider the four-point function of the lowest scalar in the stress-energy tensor multiplet in N=8 $$ \mathcal{N}=8 $$ ABJ(M) theory [1, 2]. At large central charge c T ∼ N 3/2, this correlator is given by the corresponding holographic correlation function in 11d supergravity on AdS 4 × S 7. We use Mellin space techniques to compute the leading 1/c T correction to anomalous dimensions and OPE coefficients of operators that appear in this holographic correlator. For half and quarter-BPS operators, we find exact agreement with previously computed localization results. For the other BPS and non-BPS operators, our results match the N=8 $$ \mathcal{N}=8 $$ numerical bootstrap for ABJ(M) at large c T , which provides a precise check of unprotected observables in AdS/CFT.
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spelling doaj.art-e98a185e28a2455a8f232991873d2ce42022-12-21T19:38:59ZengSpringerOpenJournal of High Energy Physics1029-84792018-07-012018712210.1007/JHEP07(2018)030AdS4/CFT3 for unprotected operatorsShai M. Chester0Joseph Henry Laboratories, Princeton UniversityAbstract We consider the four-point function of the lowest scalar in the stress-energy tensor multiplet in N=8 $$ \mathcal{N}=8 $$ ABJ(M) theory [1, 2]. At large central charge c T ∼ N 3/2, this correlator is given by the corresponding holographic correlation function in 11d supergravity on AdS 4 × S 7. We use Mellin space techniques to compute the leading 1/c T correction to anomalous dimensions and OPE coefficients of operators that appear in this holographic correlator. For half and quarter-BPS operators, we find exact agreement with previously computed localization results. For the other BPS and non-BPS operators, our results match the N=8 $$ \mathcal{N}=8 $$ numerical bootstrap for ABJ(M) at large c T , which provides a precise check of unprotected observables in AdS/CFT.http://link.springer.com/article/10.1007/JHEP07(2018)030AdS-CFT CorrespondenceConformal Field TheoryM-Theory
spellingShingle Shai M. Chester
AdS4/CFT3 for unprotected operators
Journal of High Energy Physics
AdS-CFT Correspondence
Conformal Field Theory
M-Theory
title AdS4/CFT3 for unprotected operators
title_full AdS4/CFT3 for unprotected operators
title_fullStr AdS4/CFT3 for unprotected operators
title_full_unstemmed AdS4/CFT3 for unprotected operators
title_short AdS4/CFT3 for unprotected operators
title_sort ads4 cft3 for unprotected operators
topic AdS-CFT Correspondence
Conformal Field Theory
M-Theory
url http://link.springer.com/article/10.1007/JHEP07(2018)030
work_keys_str_mv AT shaimchester ads4cft3forunprotectedoperators