One-loop free energy of tensionless type IIB string in AdS5×S5

Abstract Considering the zero ’t Hooft coupling limit of N = 4 $$ \mathcal{N}=4 $$ super-Yang-Mills theory, the exact spectrum of all single-trace operators can be accessed in terms of the underlying so(2, 4) character. This makes it possible in turn to compute the one-loop free energy of the tensio...

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Main Authors: Jin-Beom Bae, Euihun Joung, Shailesh Lal
Format: Article
Language:English
Published: SpringerOpen 2017-06-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP06(2017)155
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spelling doaj-46e9d856bf49428caf7a97dd67bd17512020-11-25T01:40:29ZengSpringerOpenJournal of High Energy Physics1029-84792017-06-012017611610.1007/JHEP06(2017)155One-loop free energy of tensionless type IIB string in AdS5×S5Jin-Beom Bae0Euihun Joung1Shailesh Lal2Korea Institute for Advanced StudyDepartment of Physics and Research Institute of Basic Science, Kyung Hee UniversityLPTHE — UMR 7589, UPMC Paris 06, Sorbonne UniversitésAbstract Considering the zero ’t Hooft coupling limit of N = 4 $$ \mathcal{N}=4 $$ super-Yang-Mills theory, the exact spectrum of all single-trace operators can be accessed in terms of the underlying so(2, 4) character. This makes it possible in turn to compute the one-loop free energy of the tensionless type IIB string theory in AdS5×S5 background, with help of the recently developed method of character integral representation of zeta function (CIRZ). We calcu-late first the one-loop free energy of the string states in the (p − 1)-th Regge trajectory and find the result to be p times the free energy of a single N = 4 $$ \mathcal{N}=4 $$ Maxwell multiplet. The full one-loop free energy is hence proportional to the divergent series ∑ p = 2 ∞ p $$ {\displaystyle {\sum}_{p=2}^{{}_{\infty }}p} $$ . The divergence arises as a result of interrupting the regularization procedure in an intermediate stage. With a reorganization of states, we extract the finite part of free energy after summing over the Regge trajectories. This way gives us a finite result which is minus of the free energy of the N = 4 $$ \mathcal{N}=4 $$ multiplet. Hence, this bulk one-loop result matches the −1 term in the N 2 − 1 factor of the boundary result.http://link.springer.com/article/10.1007/JHEP06(2017)1551/N ExpansionAdS-CFT CorrespondenceHigher Spin GravityHigher Spin Symmetry
collection DOAJ
language English
format Article
sources DOAJ
author Jin-Beom Bae
Euihun Joung
Shailesh Lal
spellingShingle Jin-Beom Bae
Euihun Joung
Shailesh Lal
One-loop free energy of tensionless type IIB string in AdS5×S5
Journal of High Energy Physics
1/N Expansion
AdS-CFT Correspondence
Higher Spin Gravity
Higher Spin Symmetry
author_facet Jin-Beom Bae
Euihun Joung
Shailesh Lal
author_sort Jin-Beom Bae
title One-loop free energy of tensionless type IIB string in AdS5×S5
title_short One-loop free energy of tensionless type IIB string in AdS5×S5
title_full One-loop free energy of tensionless type IIB string in AdS5×S5
title_fullStr One-loop free energy of tensionless type IIB string in AdS5×S5
title_full_unstemmed One-loop free energy of tensionless type IIB string in AdS5×S5
title_sort one-loop free energy of tensionless type iib string in ads5×s5
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2017-06-01
description Abstract Considering the zero ’t Hooft coupling limit of N = 4 $$ \mathcal{N}=4 $$ super-Yang-Mills theory, the exact spectrum of all single-trace operators can be accessed in terms of the underlying so(2, 4) character. This makes it possible in turn to compute the one-loop free energy of the tensionless type IIB string theory in AdS5×S5 background, with help of the recently developed method of character integral representation of zeta function (CIRZ). We calcu-late first the one-loop free energy of the string states in the (p − 1)-th Regge trajectory and find the result to be p times the free energy of a single N = 4 $$ \mathcal{N}=4 $$ Maxwell multiplet. The full one-loop free energy is hence proportional to the divergent series ∑ p = 2 ∞ p $$ {\displaystyle {\sum}_{p=2}^{{}_{\infty }}p} $$ . The divergence arises as a result of interrupting the regularization procedure in an intermediate stage. With a reorganization of states, we extract the finite part of free energy after summing over the Regge trajectories. This way gives us a finite result which is minus of the free energy of the N = 4 $$ \mathcal{N}=4 $$ multiplet. Hence, this bulk one-loop result matches the −1 term in the N 2 − 1 factor of the boundary result.
topic 1/N Expansion
AdS-CFT Correspondence
Higher Spin Gravity
Higher Spin Symmetry
url http://link.springer.com/article/10.1007/JHEP06(2017)155
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AT euihunjoung oneloopfreeenergyoftensionlesstypeiibstringinads5s5
AT shaileshlal oneloopfreeenergyoftensionlesstypeiibstringinads5s5
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