\begin{document}$^{9,10,11,13,14}{\rm{C}}$\end{document} projectiles were predicted using the obtained \begin{document}$^{12}{\rm{C}}$\end{document} and \begin{document}$^{9}{\rm{Be}}$\end{document} global optical model potentials, respectively. The predictions were analyzed in detail by comparison with the available experimental data. The results indicate that the \begin{document}$^{12}{\rm{C}}$\end{document} and \begin{document}$^{9}{\rm{Be}}$\end{document} global optical model potentials provide a satisfactory description of the elastic scattering data for the reactions induced by the \begin{document}$^{9,10,11,13}{\rm{C}}$\end{document}. For the neutron-rich carbon isotope \begin{document}$^{14}{\rm{C}}$\end{document}, the elastic scattering can be well described by changing the real part radius parameter of the \begin{document}$^{12}{\rm{C}}$\end{document} global optical model potential. Possible physical explanations for the observed differences are further discussed."> Description of elastic scattering induced by the unstable nuclei <sup>9,10,11,13,14</sup>C -
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