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
XeiφNÃk k gN
Intermediate NÃ
SUMMARY
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