Precision spectroscopy and higher spin symmetry in the ABJM model

被引:0
作者
Massimo Bianchi
Rubik Poghossian
Marine Samsonyan
机构
[1] Università di Roma “Tor Vergata”,Dipartimento di Fisica
[2] I.N.F.N. Sezione di Roma “Tor Vergata”,Physics Department, Theory Unit
[3] CERN,undefined
[4] Yerevan Physics Institute,undefined
来源
Journal of High Energy Physics | / 2010卷
关键词
AdS-CFT Correspondence; M-Theory;
D O I
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摘要
We revisit Kaluza-Klein compactification of 11-d supergravity on \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ {{{{S^7}}} \left/ {{{\mathbb{Z}_k}}} \right.} $\end{document} using group theory techniques that may find application in other flux vacua with internal coset spaces. Among the SO(2) neutral states, we identify marginal deformations and fields that couple to the recently discussed world-sheet instanton of Type IIA on \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ \mathbb{C}{\mathbb{P}^3} $\end{document}. We also discuss charged states, dual to monopole operators, and the \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ {\mathbb{Z}_k} $\end{document} projection of the Osp(8|4) singleton and its tensor products. In particular, we show that the doubleton spectrum may account for \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$ \mathcal{N} = 6 $\end{document} higher spin symmetry enhancement in the limit of vanishing ’t Hooft coupling in the boundary Chern-Simons theory.
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