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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...
Autores principales: | , |
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Lenguaje: | eng |
Publicado: |
1998
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Materias: | |
Acceso en línea: | https://dx.doi.org/10.1016/S0370-2693(99)00446-3 http://cds.cern.ch/record/374089 |
_version_ | 1780893224407138304 |
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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. |
id | cern-374089 |
institution | Organización Europea para la Investigación Nuclear |
language | eng |
publishDate | 1998 |
record_format | invenio |
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 |
work_keys_str_mv | AT anselmid subleadingcorrectionsandcentralchargesintheadscftcorrespondence AT kehagiasa subleadingcorrectionsandcentralchargesintheadscftcorrespondence |