ABJ theory in the higher spin limit

被引:0
|
作者
Shinji Hirano
Masazumi Honda
Kazumi Okuyama
Masaki Shigemori
机构
[1] University of the Witwatersrand,School of Physics and Mandelstam Institute for Theoretical Physics, and DST
[2] Harish-Chandra Research Institute,NRF Centre of Excellence in Mathematical and Statistical Sciences (CoE
[3] Shinshu University,MaSS)
[4] Kyoto University,Department of Physics
[5] Kyoto University,Yukawa Institute for Theoretical Physics
[6] Weizmann Institute of Science,Hakubi Center
来源
Journal of High Energy Physics | / 2016卷
关键词
AdS-CFT Correspondence; Chern-Simons Theories; Higher Spin Gravity; Supersymmetric gauge theory;
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学科分类号
摘要
We study the conjecture made by Chang, Minwalla, Sharma, and Yin on the duality between the N=6\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \mathcal{N}=6 $$\end{document} Vasiliev higher spin theory on AdS4 and the N=6\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \mathcal{N}=6 $$\end{document} Chern-Simons-matter theory, so-called ABJ theory, with gauge group U(N) × U(N + M). Building on our earlier results on the ABJ partition function, we develop the systematic 1/M expansion, corresponding to the weak coupling expansion in the higher spin theory, and compare the leading 1/M correction, with our proposed prescription, to the one-loop free energy of the N=6\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$ \mathcal{N}=6 $$\end{document} Vasiliev theory. We find an agreement between the two sides up to an ambiguity that appears in the bulk one-loop calculation.
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