Abstract

In this work, the triangle singularity mechanism is investigated in the $\psi(2S) \to p \bar{p} \eta / p \bar{p} \pi^0$ process. The triangle loop composed by $J/\psi$, $\eta$ and $p$ has a singularity in the physical kinematic range for the $\psi(2S) \to p \bar{p} \eta / p \bar{p} \pi^0$ process, and it would generate a very narrow peak in the invariant mass spectrum of $p\eta (\pi)$ around $1.56387$ GeV, which is far away from both the threshold and relative resonances. In these processes, all the involved vertices are constrained by the experimental data. Thus, we can make a precise model independent prediction here. It turns out that the peak in the $p\eta$ invariant mass spectrum is visible, while it is very small in the $p\pi^0$ invariant mass spectrum. We expect this effect shown in $p \bar{p} \eta$ final state can be observed by the Beijing Spectrometer (BESIII) and Super Tau-Charm Facility (STCF) in the future.

Highlights

  • The concept of triangle singularity is first proposed by L

  • We propose to detect a pure triangle singularity effect in the pη=pπ0 invariant mass spectrum in the ψð2SÞ → ppη=ppπ0 process with the triangle loop composed by J=ψ, η, and p

  • We need to prove our previous arguments that the form factor F ðq; m; ΛÞ and Nð1650Þ in ppη channel will not affect the height of triangle singularity too much

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Summary

INTRODUCTION

The concept of triangle singularity is first proposed by L. [3,4,5,6,7] by considering the triangle singularity produced in the KK KÃ loop. Particle A first decays into two particles 1 and 2. From Coleman-Norton theorem, we can see that the triangle singularity is a pure kinematical effect. Such an effect from the triangle loop is model independent and can be computed theoretically once all the vertices are known.

Published by the American Physical Society
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Intermediate NÃ
SUMMARY

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