On the near-threshold $\bar pp$ invariant mass spectrum measured in $J/\psi$ and $\psi'$ decays

TL;DR

This paper analyzes the near-threshold enhancement in the antiproton-proton invariant mass spectrum from $J/ar{p}p$ decays, attributing it to final-state interactions, and demonstrates that existing models can reproduce experimental data.

Contribution

It provides a systematic analysis of the $ar pp$ invariant mass spectrum using chiral effective field theory and phenomenological models, revealing the potential existence of a $ar NN$ bound state.

Findings

The $ar pp$ FSI can explain the observed spectrum enhancements.

The isospin-1 $^1S_0$ channel interaction suggests a possible $ar NN$ bound state.

Both recent and older models successfully reproduce experimental data.

Abstract

A systematic analysis of the near-threshold enhancement in the $\bar pp$ invariant mass spectrum seen in the decay reactions $J/\psi \to x \bar pp$ and $\psi (3686) \to x \bar pp$ $(x = \gamma,\, \omega,\, \rho,\, \pi,\, \eta)$ is presented. The enhancement is assumed to be due to the $\bar NN$ final-state interaction (FSI) and the pertinent FSI effects are evaluated in an approach that is based on the distorted-wave Born approximation. For the $\bar NN$ interaction a recent potential derived within chiral effective field theory and fitted to results of a partial-wave analysis of $\bar pp$ scattering data is considered and, in addition, an older phenomenological model constructed by the J\"ulich group. It is shown that the near-threshold spectrum observed in various decay reactions can be reproduced simultaneously and consistently by our treatment of the $\bar pp$ FSI. It turns out that the interaction in the isospin-1 $^1S_0$ channel required for the description of the $J/\psi \to \gamma \bar pp$ decay predicts a $\bar NN$ bound state.