Abstract
The mass spectrum of hidden charm pentaquark states composed of two diquarks and an antiquark are calculated by use of an effective Hamiltonian which includes explicitly the spin, color, and flavor dependent interactions. The results show that the \(P_c(4312)^+\) and \(P_c(4440)^+\) states could be explained as hidden charm pentaquark states with isospin and spin-parity \(IJ^P=1/2\left( 3/2^-\right) \), the \(P_c(4457)^+\) state could be explained as a hidden charm pentaquark state with \(IJ^P=1/2\left( 5/2^-\right) \), and the \(P_{cs}(4459)^+\) state could be explained as a hidden charm pentaquark state with \(IJ^P=0\left( 1/2^-\right) \) or \(0\left( 3/2^-\right) \). Predications for the masses of other possible pentaquark states are also given, and the possible decay channels of these hidden charm pentaquark states are discussed.
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Data Availability Statement
This manuscript has no associated data or the data will not be deposited. [Authors’ comment: All data generated during this study are already contained in this published paper.]
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Acknowledgements
This work is partially supported by the National Natural Science Foundation of China under Grants Nos. 11475181, 11635009, and 12075018, the Fundamental Research Funds for the Central Universities, and the Key Research Program of Frontier Sciences of the Chinese Academy of Sciences under Grant No. Y7292610K1.
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Communicated by Eulogio Oset
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Shi, PP., Huang, F. & Wang, WL. Hidden charm pentaquark states in a diquark model. Eur. Phys. J. A 57, 237 (2021). https://doi.org/10.1140/epja/s10050-021-00542-4
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DOI: https://doi.org/10.1140/epja/s10050-021-00542-4