Precision matching of circular Wilson loops and strings in AdS 5 × S 5

Abstract Previous attempts to match the exact N=4 $$ \mathcal{N}=4 $$ super Yang-Mills expression for the expectation value of the 12 $$ \frac{1}{2} $$-BPS circular Wilson loop with the semiclassical AdS 5 × S 5 string theory prediction were not successful at the first subleading order. There was a...

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Main Authors: Daniel Medina-Rincon, Arkady A. Tseytlin, Konstantin Zarembo
Format: Article
Language:English
Published: SpringerOpen 2018-05-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP05(2018)199
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spelling doaj-fac011ce97c647cf95dee241947a619d2020-11-25T00:27:30ZengSpringerOpenJournal of High Energy Physics1029-84792018-05-012018511710.1007/JHEP05(2018)199Precision matching of circular Wilson loops and strings in AdS 5 × S 5Daniel Medina-Rincon0Arkady A. Tseytlin1Konstantin Zarembo2Nordita, KTH Royal Institute of Technology and Stockholm UniversityBlackett Laboratory, Imperial CollegeNordita, KTH Royal Institute of Technology and Stockholm UniversityAbstract Previous attempts to match the exact N=4 $$ \mathcal{N}=4 $$ super Yang-Mills expression for the expectation value of the 12 $$ \frac{1}{2} $$-BPS circular Wilson loop with the semiclassical AdS 5 × S 5 string theory prediction were not successful at the first subleading order. There was a missing prefactor ∼ λ −3/4 which could be attributed to the unknown normalization of the string path integral measure. Here we resolve this problem by computing the ratio of the string partition functions corresponding to the circular Wilson loop and the special 14 $$ \frac{1}{4} $$ supersymmetric latitude Wilson loop. The fact that the latter has a trivial expectation value in the gauge theory allows us to relate the prefactor to the contribution of the three zero modes of the “transverse” fluctuation operator in the 5-sphere directions.http://link.springer.com/article/10.1007/JHEP05(2018)199AdS-CFT CorrespondenceWilson, ’t Hooft and Polyakov loops
collection DOAJ
language English
format Article
sources DOAJ
author Daniel Medina-Rincon
Arkady A. Tseytlin
Konstantin Zarembo
spellingShingle Daniel Medina-Rincon
Arkady A. Tseytlin
Konstantin Zarembo
Precision matching of circular Wilson loops and strings in AdS 5 × S 5
Journal of High Energy Physics
AdS-CFT Correspondence
Wilson, ’t Hooft and Polyakov loops
author_facet Daniel Medina-Rincon
Arkady A. Tseytlin
Konstantin Zarembo
author_sort Daniel Medina-Rincon
title Precision matching of circular Wilson loops and strings in AdS 5 × S 5
title_short Precision matching of circular Wilson loops and strings in AdS 5 × S 5
title_full Precision matching of circular Wilson loops and strings in AdS 5 × S 5
title_fullStr Precision matching of circular Wilson loops and strings in AdS 5 × S 5
title_full_unstemmed Precision matching of circular Wilson loops and strings in AdS 5 × S 5
title_sort precision matching of circular wilson loops and strings in ads 5 × s 5
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2018-05-01
description Abstract Previous attempts to match the exact N=4 $$ \mathcal{N}=4 $$ super Yang-Mills expression for the expectation value of the 12 $$ \frac{1}{2} $$-BPS circular Wilson loop with the semiclassical AdS 5 × S 5 string theory prediction were not successful at the first subleading order. There was a missing prefactor ∼ λ −3/4 which could be attributed to the unknown normalization of the string path integral measure. Here we resolve this problem by computing the ratio of the string partition functions corresponding to the circular Wilson loop and the special 14 $$ \frac{1}{4} $$ supersymmetric latitude Wilson loop. The fact that the latter has a trivial expectation value in the gauge theory allows us to relate the prefactor to the contribution of the three zero modes of the “transverse” fluctuation operator in the 5-sphere directions.
topic AdS-CFT Correspondence
Wilson, ’t Hooft and Polyakov loops
url http://link.springer.com/article/10.1007/JHEP05(2018)199
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