The role of triangle singularity in isospin breaking process $J/\psi \to \Lambda \bar{\Lambda }\pi$ and the possible evidence of ${\Sigma }^{\ast }({\frac{1}{2}}^{-})$ states

Abstract

In this study, the impact of triangle singularity is investigated in the isospin-breaking process $J/\psi \to \Lambda \bar{\Lambda }\pi$. The triangle singularity is found to play a significant role in the process, resulting in the creation of a resonance-like structure around 1.4 GeV in the $\Lambda \pi (\bar{\Lambda }\pi )$ invariant mass spectrum. To amplify the impact of this triangle singularity, the presence of two ${\Sigma }^{\ast }({\frac{1}{2}}^{-})$ states around 1.4 GeV and 1.6 GeV is essential, yet these states have not been definitively identified in the current baryon spectrum. We recommend that experiments, particularly the Beijing Spectrometer (BESIII) and the future Super Tau-Charm Factory (STCF), to investigate the process $J/\psi \to \Lambda \bar{\Lambda }\pi$ to offer direct evidences for our predicted triangle singularity and additional evidence regarding the $\Sigma ({\frac{1}{2}}^{-})$ states.

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Cited by in corpus (1)

• The odd-parity strange baryons $\Sigma ({\frac{1}{2}}^{-})$ below 1.8 GeV with Hamiltonian effective field theory