Observation of Two New N* Peaks in J/psi -> $p pi^- \bar n$ and $\bar p\pi^+n$ Decays

TL;DR

This study reports the first direct observation of two new N* resonance peaks at 1360 MeV and 2030 MeV in J/psi decays, providing insights into nucleon excited states and the missing resonance problem.

Contribution

The paper presents the first direct detection of the N*(1440) and a high-mass N* peak above 2 GeV in J/psi decays, clarifying nucleon resonance spectrum.

Findings

Observation of N*(1440) at 1358 MeV with specific width

Discovery of a new N* peak at 2068 MeV

Enhanced understanding of N* resonance spectrum

Abstract

The $\pi N$ system in decays of $J/\psi\to\bar NN\pi$ is limited to be isospin 1/2 by isospin conservation. This provides a big advantage in studying $N^*\to \pi N$ compared with $\pi N$ and $\gamma N$ experiments which mix isospin 1/2 and 3/2 for the $\pi N$ system. Using 58 million $J/\psi$ decays collected with the Beijing Electron Positron Collider, more than 100 thousand $J/\psi \to p \pi^- \bar n + c.c.$ events are obtained. Besides two well known $N^*$ peaks at 1500 MeV and 1670 MeV, there are two new, clear $N^*$ peaks in the $p\pi$ invariant mass spectrum around 1360 MeV and 2030 MeV. They are the first direct observation of the $N^*(1440)$ peak and a long-sought "missing" $N^*$ peak above 2 GeV in the $\pi N$ invariant mass spectrum. A simple Breit-Wigner fit gives the mass and width for the $N^*(1440)$ peak as $1358\pm 6 \pm 16$ MeV and $179\pm 26\pm 50$ MeV, and for the new $N^*$ peak above 2 GeV as $2068\pm 3^{+15}_{-40}$ MeV and $165\pm 14\pm 40$ MeV, respectively.