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Alfredo A. Correa edited figures/plot-stopping8/caption.tex
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\label{fig:stopping_power} (color online). The stopping power ($S_\text{e}$) vs. projectile velocity $v$: for a channeling trajectory (red lines) and for off-channeling trajectory (blue crosses). The black continuous lines refers to the nominal tabulated results from the \text{Srim} database for electronic stopping power \cite{Ziegler_2010}. The gray dots refers to the \textsc{Srim} experimental database contained therein \cite{Copper_Stop}. (Lowest velocity experimental point is at $v = \sim 0.2~\mathrm{a.u.}$).
The error bars of the off-channeling trajectory is shown by the blue lines.
(Error bars in channeling trajectories is smaller than the points.)
Open circles and open squares shows data of Cantero \emph{et al.} \cite{Cantero_2009} and Markin \emph{et al.} \cite{Markin_2009} respectively.
%The optimized density we obtain for the Cu crystal is $8.96~\mathrm{g/cm^3}$ and the available experimental density of Cu was $8.92~\mathrm{g/cm^3}$.% are smaller than the calculated value (of point size).%
%Proton in Copper Stopping Power: The stopping power ($S_\text{e}$) vs. projectile velocity $v$: for a channeling trajectory (with experimental density-red lines), for a channeling trajectory (with low density-blue dots). The black continuous lines refers to the nominal tabulated results from the \text{Srim} database for electronic stopping power\cite{Ziegler_2010}. The gray dots refers to the \textsc{Srim} experimental database contained therein http://www.srim.org/SRIM/SRIMPICS/STOP01/STOP0129.gif.(Lowest velocity experimental point is at $v = \sim 0.2~\mathrm{a.u.}$.) The error bars (darkgreen crosses) are smaller than the calculated value (of point size).%