Abstract

At small AdS radius, the superstring on AdS5 × S5 was conjectured by Maldacena to be equivalent to mathcal{N} = 4 super-Yang-Mills at small ‘t Hooft coupling where thickened Feynman diagrams can be used to compute scattering amplitudes. It was previously shown that the pure spinor worldsheet action of the AdS5 × S5 superstring can be expressed as the sum of a BRST-trivial term and a “B-term” which is antisymmetric in worldsheet derivatives. Using the explicit form of the pure spinor vertex operators, it will be argued here that the free super-Yang-Mills Feynman diagrams are described by the BRST-trivial term where the thickened propagators are the regions of the string worldsheet near the AdS boundary and the holes are the regions near the AdS horizon. Evidence will then be presented that the antisymmetric B-term generates the super-Yang-Mills vertex so that, at small radius and arbitrary genus, the superstring amplitudes correctly reproduce the super-Yang-Mills Feynman diagram expansion.

Highlights

  • includes terms depending on the pure spinor ghosts

  • Using the explicit form of the pure spinor vertex operators, it will be argued here that the free super-Yang-Mills Feynman diagrams are described by the BRST-trivial term where the thickened propagators are the regions of the string worldsheet near the AdS boundary and the holes are the regions near the AdS horizon

  • Feynman diagrams where the Feynman propagators are the regions of the string worldsheet near the AdS boundary and the holes in the Feynman diagram are the regions of the string worldsheet near the AdS horizon

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Summary

N for the non-planar

Yang-Mills, section 4 will compare the B term and the cubic super-Yang-Mills vertex, and the appendix will review the construction of the AdS5 × S5 topological action

Half-BPS vertex operators
General non-BPS vertex operators at small radius
Topological action
Emergence of propagators
Topological amplitudes
Commutators from B terms
Expansion of B
Summary
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