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Subleading Corrections and Central Charges in the AdS/CFT Correspondence

We explore subleading contributions to the two basic central charges c and a of four-dimensional conformal field theories in the AdS/CFT scheme. In particular we probe subleading corrections to the difference c-a from the string-theory side. In the N=4 CFT, c-a vanish identically consistently with t...

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Detalles Bibliográficos
Autores principales: Anselmi, D., Kehagias, A.
Lenguaje:eng
Publicado: 1998
Materias:
Acceso en línea:https://dx.doi.org/10.1016/S0370-2693(99)00446-3
http://cds.cern.ch/record/374089
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author Anselmi, D.
Kehagias, A.
author_facet Anselmi, D.
Kehagias, A.
author_sort Anselmi, D.
collection CERN
description We explore subleading contributions to the two basic central charges c and a of four-dimensional conformal field theories in the AdS/CFT scheme. In particular we probe subleading corrections to the difference c-a from the string-theory side. In the N=4 CFT, c-a vanish identically consistently with the string-theory expectations. However, for N=1 and N=2 CFTs, the U_R(1) anomaly, which is proportional to c-a, is subleading in the large N limit for theories in the AdS/CFT context and one expects string one-loop R^2 and B terms as coming from the R^4 terms. Similar considerations apply to the U_R(1)^3 anomaly which is, however, subleading only for N=2 theories. As a result, a string one-loop term B \wedge F \wedge F should exist in the low energy effective action of the N=4 five-dimensional supergravity. The U_R(1)^3 term is leading for the N=1 CFT and it is indeed present in the N=2 five-dimensional supergravity.
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institution Organización Europea para la Investigación Nuclear
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spelling cern-3740892023-03-14T20:10:59Zdoi:10.1016/S0370-2693(99)00446-3http://cds.cern.ch/record/374089engAnselmi, D.Kehagias, A.Subleading Corrections and Central Charges in the AdS/CFT CorrespondenceParticle Physics - TheoryWe explore subleading contributions to the two basic central charges c and a of four-dimensional conformal field theories in the AdS/CFT scheme. In particular we probe subleading corrections to the difference c-a from the string-theory side. In the N=4 CFT, c-a vanish identically consistently with the string-theory expectations. However, for N=1 and N=2 CFTs, the U_R(1) anomaly, which is proportional to c-a, is subleading in the large N limit for theories in the AdS/CFT context and one expects string one-loop R^2 and B terms as coming from the R^4 terms. Similar considerations apply to the U_R(1)^3 anomaly which is, however, subleading only for N=2 theories. As a result, a string one-loop term B \wedge F \wedge F should exist in the low energy effective action of the N=4 five-dimensional supergravity. The U_R(1)^3 term is leading for the N=1 CFT and it is indeed present in the N=2 five-dimensional supergravity.We explore subleading contributions to the two basic central charges c and a of four-dimensional conformal field theories in the AdS/CFT scheme. In particular we probe subleading corrections to the difference c-a from the string-theory side. In the N=4 CFT, c-a vanish identically consistently with the string-theory expectations. However, for N=1 and N=2 CFTs, the U_R(1) anomaly, which is proportional to c-a, is subleading in the large N limit for theories in the AdS/CFT context and one expects string one-loop R^2 and B \wedge R \wedge R terms in the low energy effective action. We identify these terms as coming from the R^4 terms. Similar considerations apply to the U_R(1)^3 anomaly which is, however, subleading only for N=2 theories. As a result, a string one-loop term B \wedge F \wedge F should exist in the low energy effective action of the N=4 five-dimensional supergravity. The U_R(1)^3 term is leading for the N=1 CFT and it is indeed present in the N=2 five-dimensional supergravity.We explore subleading contributions to the two basic central charges c and a of four-dimensional conformal field theories in the AdS/CFT scheme. In particular we probe subleading corrections to the difference c − a from the string-theory side. In the N =4 CFT, c − a vanish identically consistently with the string-theory expectations. However, for N =1 and N =2 CFTs, the U R (1) anomaly, which is proportional to c − a , is subleading in the large N limit for theories in the AdS/CFT context and one expects string one-loop R 2 and B ∧ R ∧ R terms in the low energy effective action. We identify these terms as coming from the R 4 terms. Similar considerations apply to the U R (1) 3 anomaly which is, however, subleading only for N =2 theories. As a result, a string one-loop term B ∧ F ∧ F should exist in the low energy effective action of the N =4 five-dimensional supergravity. The U R (1) 3 term is leading for the N =1 CFT and it is indeed present in the N =2 five-dimensional supergravity.hep-th/9812092CERN-TH-98-394CERN-TH-98-394oai:cds.cern.ch:3740891998-12-11
spellingShingle Particle Physics - Theory
Anselmi, D.
Kehagias, A.
Subleading Corrections and Central Charges in the AdS/CFT Correspondence
title Subleading Corrections and Central Charges in the AdS/CFT Correspondence
title_full Subleading Corrections and Central Charges in the AdS/CFT Correspondence
title_fullStr Subleading Corrections and Central Charges in the AdS/CFT Correspondence
title_full_unstemmed Subleading Corrections and Central Charges in the AdS/CFT Correspondence
title_short Subleading Corrections and Central Charges in the AdS/CFT Correspondence
title_sort subleading corrections and central charges in the ads/cft correspondence
topic Particle Physics - Theory
url https://dx.doi.org/10.1016/S0370-2693(99)00446-3
http://cds.cern.ch/record/374089
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