Abstract

In this work, we propose that there exists a moving triangle singularity in the $\ensuremath{\psi}(2S)\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{K}^{+}{K}^{\ensuremath{-}}$ process, whose position can vary from 1.158 to 1.181 GeV in the invariant mass spectrum of ${K}^{+}{K}^{\ensuremath{-}}$. After a precise analysis on this process, it turns out that after doing some cuts on ${m}_{{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}}$, experiments do have the opportunity to observe this triangle singularity. In addition, when changing the cuts on ${m}_{{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}}$, the movement of the predicted triangle singularity can also be observed. Thus, we suggest future experiments, especially Super Tau-Charm Facility (STCF), to do an analysis on the $\ensuremath{\psi}(2S)\ensuremath{\rightarrow}{\ensuremath{\pi}}^{+}{\ensuremath{\pi}}^{\ensuremath{-}}{K}^{+}{K}^{\ensuremath{-}}$ process to verify our prediction.

Highlights

  • In the past decades, the triangle singularity that proposed by L

  • In recent years, with the discoveries of a series of exotic states such as Zc [9–15], Pc [16,17] and X(2900) [18,19], many researches on triangle singularity have been carried out [2–6,8,20–57], which imply that these exotic states can be related to some specific triangle singularities

  • By using the triangle singularity produced by the kaon loop, they successfully explained the peak of a1ð1420Þ without introducing the Breit-Wigner structure

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Summary

INTRODUCTION

The triangle singularity that proposed by L. [59] proposed that it is very possible for experiments to detect a pure triangle singularity in the ψð2SÞ → ppη process, where the triangle loop is composed by J=ψ, η and proton. Under this situation, the position of the triangle singularity is 80 MeV above the J=ψη threshold. If we fix the value of mCD in the permitted kinematical range, due to the triangle singularity there will be a peak structure in the invariant mass spectrum of ðE; FÞ and the peak position can be solved exactly from Eqs.

MAIN DECAY MECHANISMS OF ψð2SÞ → π + π − K + K − PROCESS
Determining the coupling constants
The signal of triangle singularity
The possibility of observing this triangle singularity in the ψð2SÞ → π + π − K + K − process
How to detect the triangle singularity in the ψð2SÞ → π + π − K + K − process in experiments
SUMMARY
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