Abstract

In this work, we report on a theoretical study of possible pentaquark states $\Lambda^0_b(5912)$ and $\Lambda^0_b(5920)$ in the $\gamma{}p\to{}\Lambda_b^{0(*)}B^+$ reactions within an effective Lagrangian approach. In addition to the contributions from the $s$-channel nucleon pole and $t$-channel $\bar{B}^{{*}-}$ exchange, the contact term contribution are also included. Our theoretical approach is based on the chiral unitary theory where the $\Lambda^0_b(5912)$ and $\Lambda^0_b(5920)$ resonances are dynamically generated. Within the coupling constants of the $\Lambda^0_b(5912)$ and $\Lambda^0_b(5920)$ to $\bar{B}p$ and $\bar{B}^{*}p$ channels obtained from chiral unitary theory, the total and differential cross sections of the $\gamma{}p\to{}\Lambda_b^{0(*)}B^+$ are evaluated. Our calculation indicates that the cross section for $\gamma{}p\to{}\Lambda_b^{0}(5912)B^{+}$ and $\gamma{}p\to{}\Lambda_b^{0}(5920)B^{+}$ reactions are of the order of 0.0164 nb and 0.00527 nb,respectively. If measured in future experiments, such as Electron-Ion Collider in China (EicC) or US(US-EIC), the predicted total cross sections and specific features of the angular distributions can be used to test the (molecular) nature of the $\Lambda^0_b(5912)$ and $\Lambda^0_b(5920)$ that they may be pentaquark states.

Highlights

  • Thanks to the experimental progress in the sector of heavy baryons in the past decade, many heavy baryons that cannot be ascribed to three-quark configurations have been reported [1]

  • Within the coupling constants of the Λ0bð5912Þ and Λ0bð5920Þ to Bp and B Ãp channels obtained from chiral unitary theory, the total and differential cross sections of the γp → Λ0bðÃÞBþ are evaluated

  • The mechanism including the t channel mediated by the exchange of B Ã mesons, the contact term, and the s channel where nucleon is considered as an intermediate state

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Summary

INTRODUCTION

Thanks to the experimental progress in the sector of heavy baryons in the past decade, many heavy baryons that cannot be ascribed to three-quark configurations have been reported [1]. A new possible strange hidden charm pentaquark Pcsð4459Þ was observed by the LHCb Collaboration with udscccomponent in the Ξ−b → J=ψΛK− process [3]. These findings stirred an active discussion on the structure of these states. It is easy to confirm that the new Pc [Pcð4312Þ, Pcð4440Þ, and Pcð4450Þ] and Pcsð4459Þ contain at least five valence quarks according to the quark components of decay model J=ψp and J=ψΛ [2,3] They are perfect candidates of hidden-charm pentaquark states. III, the numerical result of the γp → Λ0bðÃÞBþ will be given, followed by discussions and conclusions in the last section

THEORETICAL FORMALISM
RESULTS
SUMMARY

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