We revisit hidden-charm pentaquark states P_c(4380) and P_c(4450) using the method of QCD sum rules by requiring the pole contribution to be greater than or equal to 30% in order to better that the one-pole parametriz...We revisit hidden-charm pentaquark states P_c(4380) and P_c(4450) using the method of QCD sum rules by requiring the pole contribution to be greater than or equal to 30% in order to better that the one-pole parametrization is valid. We find two mixing currents, and our results suggest that P_c(4380) and P_c(4450) can be identified as hiddencharm pentaquark states having J^P= 3/2^-and 5/2^+, respectively. However, there still exist other possible spin-parity assignments, such as J^P = 3/2^+ and J^P = 5/2^-, which must be clarified in further theoretical and experimental studies.展开更多
基金Supported by National Natural Science Foundation of China(11722540,11261130311)Fundamental Research Funds for the Central UniversitiesFoundation for Young Talents in College of Anhui Province(gxyq2018103)
文摘We revisit hidden-charm pentaquark states P_c(4380) and P_c(4450) using the method of QCD sum rules by requiring the pole contribution to be greater than or equal to 30% in order to better that the one-pole parametrization is valid. We find two mixing currents, and our results suggest that P_c(4380) and P_c(4450) can be identified as hiddencharm pentaquark states having J^P= 3/2^-and 5/2^+, respectively. However, there still exist other possible spin-parity assignments, such as J^P = 3/2^+ and J^P = 5/2^-, which must be clarified in further theoretical and experimental studies.
