Widely applied to both light and heavy meson decay and standing as one of the most successful strong decay models is the \(^{3}P_{0}\) model, in which \(q\bar{q}\) pair production is the dominant mechanism. In the present, we use the bound-state corrected version of the \(^{3}P_{0}\), called the C\(^{3}P_{0}\) model, to calculate the decay widths of the charmonium \(J^{PC}=1^{--}\) states, nominally \(J/\psi\), \(\psi (2S)\), \(\psi (3770)\), \(\psi (4040)\), \(\psi (4160)\), \(\psi (4415)\) and \(\psi (4660)\) to several common channels.