Magnetic dipole moments of the ${\mathrm{\Omega }}_c(3185{)}^0$ and ${\mathrm{\Omega }}_c(3327{)}^0$ states from molecular perspective

In this paper we study the magnetic dipole moments of the newly discovered ${\mathrm{\Omega }}_c(3185{)}^0$ and ${\mathrm{\Omega }}_c(3327{)}^0$, assuming that ${\mathrm{\Omega }}_c(3185{)}^0$ and ${\mathrm{\Omega }}_c(3327{)}^0$ are $S$-wave $D\mathrm{\Xi }$ and $D^{\ast }\mathrm{\Xi }$ molecular pentaquark states, respectively. Together with these states, the magnetic dipole moments of possible $D_s\mathrm{\Xi }$, $D_s^{\ast }\mathrm{\Xi }$, $D{\mathrm{\Xi }}^{\ast }$, and $D_s{\mathrm{\Xi }}^{\ast }$ pentaquark states are also studied. The magnetic dipole moments of these singly-charmed pentaquarks are estimated within the framework of the QCD light cone sum rules utilizing the photon distribution amplitudes. In the search for the properties of singly-charmed molecular pentaquark states, the results obtained for the magnetic dipole moments can be useful.