\begin{document}$ p, d $\end{document}) reactions. Our study covers 32 sets of angular distribution data of (\begin{document}$ p, d $\end{document}) reactions on four targets and a large range of incident energies (20-200 MeV/nucleon). This study uses two semi-microscopic nucleon OMPs, i.e., Jeukenne, Lejeune, and Mahaux (JLM) [Phys. Rev. C 16, 80 (1977); Phys. Rev. C 58, 1118 (1998)] and CTOM [Phys. Rev. C 94, 034606 (2016)], and a pure microscopic nucleon potential, i.e., WLH [Phys. Rev. Lett. 127, 182502 (2021)]. The results are compared with those using the phenomenological global optical potential KD02 [Nucl. Phys. A 713, 231 (2003)]. We find that the incident energy dependence of spectroscopic factors extracted from (\begin{document}$ p, d $\end{document}) reactions is evidently suppressed when microscopic OMPs are employed for 12C, 28Si, and 40Ca. In addition, spectroscopic factors extracted using the systematic microscopic optical potential CTOM based on the Dirac-Brueckner-Hartree-Fock theory are more in line with the results obtained from (\begin{document}$ e, e'p $\end{document}) measurements, except for 16O and 40Ca at high energies (> 100 MeV), necessitating an exact treatment of double-magic nuclei. The results obtained by using the pure microscopic optical potential, WLH, based on the EFT theory show the same trend as those of CTOM but are generally higher. The JLM potential, which relies on simplified nuclear matter calculations with old-fashioned bare interactions, produces results that are very similar to those of the phenomenological potential KD02. Our results indicate that modern microscopic OMPs are reliable tools for probing the nuclear structure using transfer reactions across a wide energy range."> Systematic investigation of nucleon optical model potentials in (<i>p</i>, <i>d</i>) transfer reactions -
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