We demonstrate that the relative ratio of the decays of hidden charm pentaquark-like structure P + c (4380) toD * Λ + c and J/ψp are very different for P + c beingDΣ * c (2520) orD * Σc(2455) molecule states. While the partial width of theDΣ * c (2520) molecule to theD * Λ + c is much larger, by one order of magnitude, than that to the J/ψp, theD * Σc(2455) molecule shows a different pattern. Our analysis shows that theDΣ * c bound state ansatz is more reasonable than theD * Σc one to explain the broad Pc(4380) structure. We suggest to search for the Pc(4380) in theD * Λ + c system, which can be used to disentangle the nature of the P + c (4380) structure. * Among the two observed structures, the existence of the narrow P c (4450), no matter what it is, is affirmative from the data for the J/ψp invariant mass distribution. However, introducing the second structure, the P c (4380), does not seem that necessary since there is still a discrepancy