Possible charmed-strange molecular pentaquarks in quark delocalization color screening model

Abstract

Inspired by the states $T_{c\bar{s}0}^a(2900{)}^0$ and $T_{c\bar{s}0}^a(2900{)}^{++}$ reported by the LHCb Collaboration, we carry out a systematical investigation of the charm-strange pentaquark system using resonance group method in the quark delocalization color screening model. The present results predict the existence of some bound states and resonance states with support from the study of the mass spectrum and the decay properties. Both ${\Sigma }_c^{\ast }{K}^{\ast }$ with $I(J^P)=\frac{1}{2}({\frac{5}{2}}^{-})$ and $\Delta D_s^{\ast }$ with $I(J^P)=\frac{3}{2}({\frac{5}{2}}^{-})$ are bounded by channel coupling calculation. Moreover, the resonance state ${\Sigma }_c{K}^{\ast }$ with $I(J^P)=\frac{1}{2}({\frac{1}{2}}^{-})$ and $I(J^P)=\frac{1}{2}({\frac{3}{2}}^{-})$ are available in QDCSM, the masses and the total decay widths of which are ($R^{\prime }=3342\sim 3346$ MeV, ${\Gamma }_{Total}=25.5$ MeV) and ($R^{\prime }=3333$ MeV, ${\Gamma }_{Total}=3.3$ MeV), respectively. In addition, the resonance state $\Delta D_s^{\ast }$ with $I(J^P)=\frac{3}{2}({\frac{1}{2}}^{-})$ is also obtained, the mass and the decay width of this state are 3343 MeV and 0.01 MeV, respectively. These predicted new exotic states may provide new ideas for experimental searches and we sincerely expect more experimental and theoretical research to verify and understand the charm-strange pentaquark states in the future.