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Motivated by the successful interpretation of these observed $P_c$ and$P_{cs}$ states under the meson-baryon molecular picture, we systematicallyinvestigate the possible hidden-charm molecular pentaquark states with triplestrangeness which is due to the $\Omega_{c}^{(*)}\bar{D}_s^{(*)}$ interactions.We perform a dynamical calculation of the possible hidden-charm molecularpentaquarks with triple strangeness by the one-boson-exchange model, where the$S$-$D$ wave mixing effect and the coupled channel effect are taken intoaccount in our calculation. Our results suggest that the $\Omega_{c}\bar D_s^*$state with $J^P={3}/{2}^{-}$ and the $\Omega_{c}^{*}\bar D_s^*$ state with$J^P={5}/{2}^{-}$ can be recommended as the candidates of the hidden-charmmolecular pentaquark with triple strangeness. Furthermore, we discuss thetwo-body hidden-charm strong decay behaviors of these possible hidden-charmmolecular pentaquarks with triple strangeness by adopting the quark-interchangemodel. These predictions are expected to be tested at the LHCb, which can be asa potential research issue with more accumulated experimental data in nearfuture.

Hidden-charm pentaquarks with triple strangeness due to the $\Omega_{c}^{(*)}\bar{D}_s^{(*)}$ interactions

Hidden-charm pentaquarks with triple strangeness due to the $\Omega_{c}^{()}\bar{D}_s^{()}$ interactions