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Stimulated by the $P_{cs}(4459)$ reported by the LHCb Collaboration, weperform a single $\Xi_c\bar{D}^*$ channel and a coupled$\Xi_c\bar{D}^*/\Xi_c^*\bar{D}/\Xi_c^{\prime}\bar{D}^*/\Xi_c^*\bar{D}^*$channel analysis by using a one-boson-exchange model. Our results indicate thatthe newly $P_{cs}(4459)$ cannot be a pure $\Xi_c\bar{D}^*$ molecular state, buta coupled$\Xi_c\bar{D}^*/\Xi_c^*\bar{D}/\Xi_c^{\prime}\bar{D}^*/\Xi_c^*\bar{D}^*$ boundstate with $I(J^P)=0(3/2^-)$, where the $\Xi_c\bar{D}^*$ and $\Xi_c^*\bar{D}$components are dominant. Meanwhile, we find the interactions from the$\Xi_c^{\prime}\bar{D}^*$ system with $0(1/2^-)$, the $\Xi_c^{*}\bar{D}$ systemwith $1(3/2^-)$, and the $\Xi_c^{*}\bar{D}^*$ system with $1(1/2^-)$ arestrongly attractive, where one can expect possible strange hidden-charmmolecular or resonant structures near the these thresholds with the assignedquantum numbers.

Can the newly $P_{cs}(4459)$ be a strange hidden-charm $\Xi_c\bar{D}^{*}$ molecular pentaquarks?