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
Summary
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].
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