NLSM $\subset$ Tr$(\phi^3)$

TL;DR

This paper reveals that the Tr(Φ^3) scalar theory secretly encodes all-loop amplitudes of the Non-linear Sigma Model (NLSM), establishing a novel connection via a specific kinematic shift that reproduces pion-like amplitudes and their properties.

Contribution

The work uncovers a hidden relationship between Tr(Φ^3) theory and NLSM amplitudes through a unique kinematic shift, providing new insights into their structural connection and on-shell properties.

Findings

NLSM amplitudes are obtained from Tr(Φ^3) amplitudes by a specific kinematic shift.

The shifted kinematics produce amplitudes with spontaneous symmetry breaking and Goldstone bosons.

The correspondence reproduces Adler zero and on-shell residues, confirming the physical consistency.

Abstract

Scattering amplitudes for the simplest theory of colored scalar particles - the Tr($\Phi^3$) theory - have recently been the subject of active investigations. In this letter we describe an unanticipated wider implication of this work: the Tr($\Phi^3$) theory secretly contains Non-linear Sigma Model (NLSM) amplitudes to all loop orders. The NLSM amplitudes are obtained from Tr$(\Phi^3)$ amplitudes by a unique shift of kinematic variables. We show that this shifted kinematics produces amplitudes for a cubic theory with a linear term in potential, with extrema spontaneously breaking $U(N) \to U(N-k) \times U(k)$. The Goldstone amplitudes for this theory coincide with those of pions in the $U(N) \times U(N) \to U(N)$ chiral Lagrangian to all orders in the planar limit. We also give a purely on-shell understanding of this correspondence, showing integrands defined by the kinematic shifts have the correct residues on poles and appropriately produce the Adler zero. Finally, we discuss how similar kinematic shifts produce certain infinite classes of mixed amplitudes of pions and Tr($\Phi^3$) scalars, most of which are not interpretable from the Lagrangian description.