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Alfredo A. Correa edited For_the_off_channeling_trajectory__.tex
almost 8 years ago
Commit id: 4e3ba9f9024e7ea5c3a28ee9ed4e2e2ce1535439
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In Fig.~\ref{fig:fit_off_channel}, the sharp peaks show when the proton is in the vicinity of a host $\mathrm{Cu}$ atom during an off-channeling trajectory,
while the smaller peaks and flatter regions indicate that the proton is not very close to any host atom.
To obtain the $S_\text{e}$ we compute the slopes of the curves by a linear fit of the form $y = a + bx$ (black solid lines) using our data from $x > 5~a_0$ (to eliminate the transient region)
up to a given maximum position of $x$ determined by minimizing reentrancy in the periodic supercell into the initial position.
The slope ($b$) gives the electronic stopping for this off-channeling case.
%We have displayed the procedure used in obtaining the electronic stopping for the off-channeling trajectory case in Figure \ref{fig:fit_off_channel}.%