\begin{document}$ c\bar{c} $\end{document}) pair production number in proton-nucleus (pA) collisions, the correlation between different \begin{document}$ c\bar{c} $\end{document} pairs is negligible, which makes the Schrödinger equation viable for tracking the evolution of only one \begin{document}$ c\bar{c} $\end{document} pair. We employ the time-dependent Schrödinger equation with an in-medium \begin{document}$ c\bar{c} $\end{document} potential to study the evolution of charmonium wave functions in a hydrodynamic-like QCD medium produced in pA collisions. We explore different parametrizations of real and imaginary parts of the \begin{document}$ c\bar{c} $\end{document} potential and calculate the nuclear modification factors (\begin{document}$R_{pA}$\end{document}) of \begin{document}$ J/\psi $\end{document} and \begin{document}$ \psi(2S) $\end{document} in \begin{document}$ \sqrt{s_{NN}}=5.02 $\end{document} TeV energy p-Pb collisions at the Large Hadron Collider (LHC). Comparing strong and weak screening scenarios with experimental data in this approach, we arrive at the conclusion that color screening is weak at temperatures close to the deconfined phase transition. Moreover, the imaginary part of the potential is crucial in describing the experimental data, which is consistent with widely studied semi-classical approaches, where dissociation rates are essential."> Investigating color screening in proton-nucleus collisions with complex potentials -
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