Hidden charm pentaquark states in a diquark model

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 I J(P) = 1/2(3/2(-)), the P-c(4457)(+) state could be explained as a hidden charm pentaquark state with I J(P) = 1/2(5/2(-)), and the P-cs (4459)(+) state could be explained as a hidden charm pentaquark state with I J(P) = 0(1/2(-)) or 0(3/2(-)). 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.

Automated summary

The mass spectrum of hidden charm pentaquark states is calculated using an effective Hamiltonian with interactions dependent on spin, color, and flavor. The results explain certain states and predict the masses of others, while also discussing potential decay channels.