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We present a constructive derivation of all four-point tree-level holographic correlators for eleven dimensional supergravity on $AdS_7 \times S^4$.
1905
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1906
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1910
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C. Sleight and M. Taronna, “The Unique Polyakov Blocks,” arXiv:1912.07998 [hep-th]
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L. F. Alday and X. Zhou, “Simplicity of AdS Supergravity at One Loop,” arXiv:1912.02663 [hep-th]
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R. Corrado, B. Florea, and R. McNees, “Correlation functions of operators and Wilson surfaces in the d = 6, (0,2) theory in the large N limit,” Phys. Rev
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M. Nirschl and H. Osborn, “Superconformal Ward identities and their solution,” Nucl. Phys. B
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J. Penedones, “Writing CFT correlation functions as AdS scattering amplitudes,” JHEP
2017
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2017
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2017
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L. Rastelli and X. Zhou, “Holographic Four-Point Functions in the (2, 0) Theory,” JHEP
2018
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X. Zhou, “On Superconformal Four-Point Mellin Amplitudes in Dimension d > 2 d>2 ,” JHEP
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2011
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2015
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2016
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Cubic vertices for s k s_{k} have been obtained in the literature [ 16 , 17 ] . Other vertices such as the general quartic vertices have not been worked out. By contrast, the general quartic vertices in A d S 5 × S 5 AdS_{5}\times S^{5} were obtained in [ Arutyunov:1999fb
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The first visible long operator exchanged has conformal twist 𝔱 = 2 m a x { k 1 + k 3 , k 2 + k 4 } + 4 \mathfrak{t}=2\mathop{max}\displaylimits\{k_{1}+k_{3},k_{2}+k_{4}\}+4 , and corresponds to a double pole at u = 𝔱 u=\mathfrak{t} in the integrand of ( 13
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This corresponds to a special choice of contact terms for exchange diagrams
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2018
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2018
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2018
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