Abstract

Stimulated by the $P_{cs}(4459)$ reported by the LHCb Collaboration, we perform a single $\Xi_c\bar{D}^*$ channel and a coupled $\Xi_c\bar{D}^*/\Xi_c^*\bar{D}/\Xi_c^{\prime}\bar{D}^*/\Xi_c^*\bar{D}^*$ channel analysis by using a one-boson-exchange model. Our results indicate that the newly $P_{cs}(4459)$ cannot be a pure $\Xi_c\bar{D}^*$ molecular state, but a coupled $\Xi_c\bar{D}^*/\Xi_c^*\bar{D}/\Xi_c^{\prime}\bar{D}^*/\Xi_c^*\bar{D}^*$ bound state with $I(J^P)=0(3/2^-)$, where the $\Xi_c\bar{D}^*$ and $\Xi_c^*\bar{D}$ components are dominant. Meanwhile, we find the interactions from the $\Xi_c^{\prime}\bar{D}^*$ system with $0(1/2^-)$, the $\Xi_c^{*}\bar{D}$ system with $1(3/2^-)$, and the $\Xi_c^{*}\bar{D}^*$ system with $1(1/2^-)$ are strongly attractive, where one can expect possible strange hidden-charm molecular or resonant structures near the these thresholds with the assigned quantum numbers.

Highlights

  • INTRODUCTIONIn 2019, the LHCb collaboration updated the observations in the Λ0b → J=ψpK− process by using more data [1], they discovered a new narrow pentaquark state, Pcð4312Þþ, and found that the Pcð4450Þ reported previously [2] consists of two narrow overlapping peaks, Pcð4440Þþ and Pcð4457Þþ

  • In 2019, the LHCb collaboration updated the observations in the Λ0b → J=ψpK− process by using more data [1], they discovered a new narrow pentaquark state, Pcð4312Þþ, and found that the Pcð4450Þ reported previously [2] consists of two narrow overlapping peaks, Pcð4440Þþ and Pcð4457Þþ.The discovery of Pc states has sparked an enormous interest in the study of multiquark systems and exotic hadrons

  • We find the interactions from the Ξ0cD Ã system with 0ð1=2−Þ, the ΞÃcDsystem with 1ð3=2−Þ, and the ΞÃcD Ã system with 1ð1=2−Þ are strongly attractive, where one can expect possible strange hidden-charm molecular or resonant structures near these thresholds with the assigned quantum numbers

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Summary

INTRODUCTION

In 2019, the LHCb collaboration updated the observations in the Λ0b → J=ψpK− process by using more data [1], they discovered a new narrow pentaquark state, Pcð4312Þþ, and found that the Pcð4450Þ reported previously [2] consists of two narrow overlapping peaks, Pcð4440Þþ and Pcð4457Þþ. The masses of the Pc states are close to the thresholds of a charmed baryon and an anticharmed meson, which is the main reason why the hadronic molecular state assignments to them were proposed. Since its mass is just below the ΞcD Ã threshold with around 19 MeV, whether the newly Pcsð4459Þ can be explained as a strange hidden-charm ΞcD Ã molecule is open to discussion [33,34,35], i.e., Chen et al.’s results supported the Pcsð4459Þ as the ΞcD Ã molecule of either JP 1⁄4 1=2− or 3=2− after adopting the QCD sum rules [33].

ONE-BOSON-EXCHANGE EFFECTIVE POTENTIALS
BÃ6μ i þ λpSgffiffiV 2
Findings
SUMMARY
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