Abstract

We revisit from a modern bootstrap perspective the longstanding problem of solving QCD in the large NN limit. We derive universal bounds on the effective field theory of massless pions by imposing the full set of positivity constraints that follow from 2→22 \to 2 scattering. Some features of our exclusion plots have intriguing connections with hadronic phenomenology. The exclusion boundary exhibits a sharp kink, raising the tantalizing scenario that large NN QCD may sit at this kink. We critically examine this possibility, developing in the process a partial analytic understanding of the geometry of the bounds.

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