Minimal area surfaces in AdS n+1 and Wilson loops

Abstract The AdS/CFT correspondence relates the expectation value of Wilson loops in N $$ \mathcal{N} $$ = 4 SYM to the area of minimal surfaces in AdS 5. In this paper we consider minimal area surfaces in generic Euclidean AdS n+1 using the Pohlmeyer reduction in a similar way as we did previously...

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Main Authors: Yifei He, Changyu Huang, Martin Kruczenski
Format: Article
Language:English
Published: SpringerOpen 2018-02-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP02(2018)027
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spelling doaj-a22ece04e8eb4b519d771de239c6c15f2020-11-24T21:41:28ZengSpringerOpenJournal of High Energy Physics1029-84792018-02-012018212310.1007/JHEP02(2018)027Minimal area surfaces in AdS n+1 and Wilson loopsYifei He0Changyu Huang1Martin Kruczenski2Department of Physics and Astronomy, Purdue UniversityDepartment of Physics and Astronomy, Purdue UniversityDepartment of Physics and Astronomy, Purdue UniversityAbstract The AdS/CFT correspondence relates the expectation value of Wilson loops in N $$ \mathcal{N} $$ = 4 SYM to the area of minimal surfaces in AdS 5. In this paper we consider minimal area surfaces in generic Euclidean AdS n+1 using the Pohlmeyer reduction in a similar way as we did previously in Euclidean AdS 3. As in that case, the main obstacle is to find the correct parameterization of the curve in terms of a conformal parameter. Once that is done, the boundary conditions for the Pohlmeyer fields are obtained in terms of conformal invariants of the curve. After solving the Pohlmeyer equations, the area can be expressed as a boundary integral involving a generalization of the conformal arc-length, curvature and torsion of the curve. Furthermore, one can introduce the λ-deformation symmetry of the contours by a simple change in the conformal invariants. This determines the λ-deformed contours in terms of the solution of a boundary linear problem. In fact the condition that all λ deformed contours are periodic can be used as an alternative to solving the Pohlmeyer equations and is equivalent to imposing the vanishing of an infinite set of conserved charges derived from integrability.http://link.springer.com/article/10.1007/JHEP02(2018)027AdS-CFT CorrespondenceWilson’t Hooft and Polyakov loops
collection DOAJ
language English
format Article
sources DOAJ
author Yifei He
Changyu Huang
Martin Kruczenski
spellingShingle Yifei He
Changyu Huang
Martin Kruczenski
Minimal area surfaces in AdS n+1 and Wilson loops
Journal of High Energy Physics
AdS-CFT Correspondence
Wilson
’t Hooft and Polyakov loops
author_facet Yifei He
Changyu Huang
Martin Kruczenski
author_sort Yifei He
title Minimal area surfaces in AdS n+1 and Wilson loops
title_short Minimal area surfaces in AdS n+1 and Wilson loops
title_full Minimal area surfaces in AdS n+1 and Wilson loops
title_fullStr Minimal area surfaces in AdS n+1 and Wilson loops
title_full_unstemmed Minimal area surfaces in AdS n+1 and Wilson loops
title_sort minimal area surfaces in ads n+1 and wilson loops
publisher SpringerOpen
series Journal of High Energy Physics
issn 1029-8479
publishDate 2018-02-01
description Abstract The AdS/CFT correspondence relates the expectation value of Wilson loops in N $$ \mathcal{N} $$ = 4 SYM to the area of minimal surfaces in AdS 5. In this paper we consider minimal area surfaces in generic Euclidean AdS n+1 using the Pohlmeyer reduction in a similar way as we did previously in Euclidean AdS 3. As in that case, the main obstacle is to find the correct parameterization of the curve in terms of a conformal parameter. Once that is done, the boundary conditions for the Pohlmeyer fields are obtained in terms of conformal invariants of the curve. After solving the Pohlmeyer equations, the area can be expressed as a boundary integral involving a generalization of the conformal arc-length, curvature and torsion of the curve. Furthermore, one can introduce the λ-deformation symmetry of the contours by a simple change in the conformal invariants. This determines the λ-deformed contours in terms of the solution of a boundary linear problem. In fact the condition that all λ deformed contours are periodic can be used as an alternative to solving the Pohlmeyer equations and is equivalent to imposing the vanishing of an infinite set of conserved charges derived from integrability.
topic AdS-CFT Correspondence
Wilson
’t Hooft and Polyakov loops
url http://link.springer.com/article/10.1007/JHEP02(2018)027
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AT changyuhuang minimalareasurfacesinadsn1andwilsonloops
AT martinkruczenski minimalareasurfacesinadsn1andwilsonloops
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