Phase transition of anti-symmetric Wilson loops in N=4 $$ \mathcal{N}=4 $$ SYM

Abstract We will argue that the 1/2 BPS Wilson loops in the anti-symmetric representations in the N=4 $$ \mathcal{N}=4 $$ super Yang-Mills (SYM) theory exhibit a phase transition at some critical value of the ’t Hooft coupling of order N 2. In the matrix model computation of Wilson loop expectation...

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Main Author: Kazumi Okuyama
Format: Article
Language:English
Published: SpringerOpen 2017-12-01
Series:Journal of High Energy Physics
Subjects:
Online Access:http://link.springer.com/article/10.1007/JHEP12(2017)125
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author Kazumi Okuyama
author_facet Kazumi Okuyama
author_sort Kazumi Okuyama
collection DOAJ
description Abstract We will argue that the 1/2 BPS Wilson loops in the anti-symmetric representations in the N=4 $$ \mathcal{N}=4 $$ super Yang-Mills (SYM) theory exhibit a phase transition at some critical value of the ’t Hooft coupling of order N 2. In the matrix model computation of Wilson loop expectation values, this phase transition corresponds to the transition between the one-cut phase and the two-cut phase. It turns out that the one-cut phase is smoothly connected to the small ’t Hooft coupling regime and the 1/N corrections of Wilson loops in this phase can be systematically computed from the topological recursion in the Gaussian matrix model.
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spelling doaj.art-9db4eeb3ad3048009974881d04bd49a92022-12-22T02:56:04ZengSpringerOpenJournal of High Energy Physics1029-84792017-12-0120171212410.1007/JHEP12(2017)125Phase transition of anti-symmetric Wilson loops in N=4 $$ \mathcal{N}=4 $$ SYMKazumi Okuyama0Department of Physics, Shinshu UniversityAbstract We will argue that the 1/2 BPS Wilson loops in the anti-symmetric representations in the N=4 $$ \mathcal{N}=4 $$ super Yang-Mills (SYM) theory exhibit a phase transition at some critical value of the ’t Hooft coupling of order N 2. In the matrix model computation of Wilson loop expectation values, this phase transition corresponds to the transition between the one-cut phase and the two-cut phase. It turns out that the one-cut phase is smoothly connected to the small ’t Hooft coupling regime and the 1/N corrections of Wilson loops in this phase can be systematically computed from the topological recursion in the Gaussian matrix model.http://link.springer.com/article/10.1007/JHEP12(2017)125AdS-CFT CorrespondenceWilson,’t Hooft and Polyakov loops1/N ExpansionMatrix Models
spellingShingle Kazumi Okuyama
Phase transition of anti-symmetric Wilson loops in N=4 $$ \mathcal{N}=4 $$ SYM
Journal of High Energy Physics
AdS-CFT Correspondence
Wilson,’t Hooft and Polyakov loops
1/N Expansion
Matrix Models
title Phase transition of anti-symmetric Wilson loops in N=4 $$ \mathcal{N}=4 $$ SYM
title_full Phase transition of anti-symmetric Wilson loops in N=4 $$ \mathcal{N}=4 $$ SYM
title_fullStr Phase transition of anti-symmetric Wilson loops in N=4 $$ \mathcal{N}=4 $$ SYM
title_full_unstemmed Phase transition of anti-symmetric Wilson loops in N=4 $$ \mathcal{N}=4 $$ SYM
title_short Phase transition of anti-symmetric Wilson loops in N=4 $$ \mathcal{N}=4 $$ SYM
title_sort phase transition of anti symmetric wilson loops in n 4 mathcal n 4 sym
topic AdS-CFT Correspondence
Wilson,’t Hooft and Polyakov loops
1/N Expansion
Matrix Models
url http://link.springer.com/article/10.1007/JHEP12(2017)125
work_keys_str_mv AT kazumiokuyama phasetransitionofantisymmetricwilsonloopsinn4mathcaln4sym