The breakdown of resummed perturbation theory at high energies

Calculations of high-energy processes involving the production of a large number of particles in weakly-coupled quantum field theories have previously signaled the need for novel non-perturbative behavior or even new physical phenomena. In some scenarios, already tree-level computations may enter the regime of large-order perturbation theory and therefore require a careful investigation. We demonstrate that in scalar quantum field theories with a unique global minimum, where suitably resummed perturbative expansions are expected to capture all relevant physical effects, perturbation theory may still suffer from severe shortcomings in the high-energy regime. As an example, we consider the computation of multiparticle threshold amplitudes of the form 1 -> n in phi(6) theory with a positive mass term, and show that they may violate unitarity of the quantum theory for large n, even after the resummation of all leading-n quantum corrections. We further argue that this is a generic feature of scalar field theories with higher-order self-interactions beyond phi(4), thereby rendering the latter unique with respect to its high-energy behavior.

Automated summary

Using resummed perturbative expansions in scalar quantum field theories with a unique global minimum may still lead to severe shortcomings in the high-energy regime, as demonstrated in the computation of multiparticle threshold amplitudes.