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In studying the role of ion-solid interactions in $\mathrm{H^+ + Al}$, Correa \emph{et al.} \cite{Correa_2012} have shown that the electronic excitations affect the interatomic forces relative to the adiabatic outcome.   Recently, Schleife \emph{et al.} \cite{Schleife_2015} have calculated the electronic stopping power ($S_\text{e}$) of $\mathrm{H}$ and $\mathrm{He}$ projectiles including   TDDFT non-adiabatic electron dynamics and found that off-channeling trajectories \emph{along with} the inclusion of semicore electrons enhance $S_\text{e}$, resulting in much better agreement with the \textsc{Srim} experimental and modeled data \cite{Ziegler_2010} in a wide range of energies.   \textsc{Srim} \cite{Ziegler_2010} provides both a fitted model for electronic stopping as well as a large set of experimental points.  In this case we concentrate in a metal with a richer electronic band structure around the Fermi energy, such as $\mathrm{Cu}$.