Octagons II: Strong Coupling

Abstract

The octagon function is the fundamental building block yielding correlation functions of four large BPS operators in N=4 super Yang-Mills theory at any value of the 't Hooft coupling and at any genus order. Here we compute the octagon at strong coupling, and discuss various interesting limits and implications, both at the planar and non-planar level.

arXiv comment43 pages, 14 figures, comments welcome

References in corpus (13)

• Thermodynamic Bubble Ansatz
• Y-system for Scattering Amplitudes
• Structure Constants and Integrable Bootstrap in Planar N=4 SYM Theory
• Higher-spin correlators
• Bootstrapping the simplest correlator in planar N = 4 SYM at all loops
• Quantum folded string and integrability: from finite size effects to Konishi dimension
• Correlation functions of three heavy operators - the AdS contribution
• On the collinear limit of scattering amplitudes at strong coupling
• Determinant formula for the octagon form factor in $\mathcal{N}$=4 SYM
• Exact null octagon
• Octagons I: Combinatorics and Non-Planar Resummations
• Clustering and the Three-Point Function
• χ-Systems for Correlation Functions

Cited by in corpus (7)

• Exact null octagon
• Octagon at finite coupling
• Large $p$ explorations. From SUGRA to big STRINGS in Mellin space
• Octagons I: Combinatorics and Non-Planar Resummations
• Stampedes I: Fishnet OPE and Octagon Bootstrap with Nonzero Bridges
• Pentagon OPE resummation in N=4 SYM: hexagons with one effective particle contribution
• Three-Point Functions in ABJM and Bethe Ansatz