Abstract

We investigate the possibility of studying the strange hidden-charm pentaquark state $P_{cs}(4459)$ by photon-induced reactions on a proton target in an effective Lagrangian approach. The production process is described by the $t$-channel $K^{-}$ exchange, the $u$-channel $\Lambda$ exchange, the contract term, and the $s$- channel nucleon pole. Our theoretical approach is based on the assumption that $P_{cs}(4459)$ with $J^{P}=1/2^{-}$ or $J^{P}=3/2^{-}$ can be interpreted as a molecule composed of $\bar{D}^{*}\Xi_c$. Using the coupling constants of the $P^{J^P}_{cs}$ to $\gamma{}\Lambda$ and $K^{-}p$ channels obtained from molecule picture of the $P^{J^{P}}_{cs}(4459)$, the total cross-sections of the process $\gamma{}p\to{}P^{J^P}_{cs}K^{+}$ is evaluated. Our calculation indicates that the cross-section for $\gamma{}p\to{}P^{1/2^{-}}_{cs}K^{+}$ and $\gamma{}p\to{}P^{3/2^{-}}_{cs}K^{+}$ are of the order of 10.0 pb and 5.0 pb, respectively. In addition, we compute the cross-section by assuming $P_{cs}(4459)$ as a compact pentaquark and find it is quite different from the results of $\bar{D}^{*}\Xi_c$ molecule. Those results can be measured in future experiments, such as the Electron-Ion Collider in China and the United States. And can be used to test the nature of the $P_{cs}$.

Highlights

  • In the past few decades, more and more hadronic exotic states were observed following the accumulation of the precise data in high energy experiments [1]

  • The production process is described by the t-channel K− exchange, the u-channel Λ exchange, the contract term, and the s- channel nucleon pole

  • The results show that the total cross section for Pcs production for JP 1⁄4 1=2− is larger than for JP 1⁄4 3=2−

Read more

Summary

INTRODUCTION

In the past few decades, more and more hadronic exotic states were observed following the accumulation of the precise data in high energy experiments [1]. We proposed that a pure D ÃΞc molecular state with mass about 4459 and JP 1⁄4 1=2− could exist, and it mainly decays to DΞ0c final state. Its properties, such as the spectroscopy and the decay width, can be well explained in the context of the multiquark state [11,12,13] with the conclusion that the Pcsð4459Þ can be assigned as hidden charm compact pentaquark state with JP 1⁄4 1=2− or JP 1⁄4 3=2−. The Appendix contains technical details to compute the partial decay widths of Pcs → γΛ and Pcs → K−P reactions

Pcs production as D ÃΞc molecule
Pcs production as compact pentaquark
RESULTS
SUMMARY
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call