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Alfredo A. Correa edited A_snapshot_of_the_distribution__.tex
almost 8 years ago
Commit id: 56bcdd7dbe6a922ca8b1376b8b63da4d1257a3db
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A snapshot of the
distribution redistribution of the charge density as a function of time for the simulation is shown in Fig.~\ref{fig:snapshot_copper}. At $t = 0~\text{attoseconds}$ (see Fig.~\ref{fig:snapshot_copper}a) the $\mathrm{H^+}$ interacts with the neighboring $\mathrm{Cu}$ atoms charge density where some electron density is acquired.
Elongated wake tails are characteristic of projectiles traveling at or above the Fermi
velocity\cite{Tehada_1980}. velocity\cite{Tehada_1980}, in turn this affects the forces exerted on the neighboring atoms.
%As $\mathrm{H^+}$ moves further through the $\mathrm{Cu}$ atoms it acquires substantial electron densities from the adjacent $\mathrm{Cu}$ atoms as shown in Fig.~\ref{fig:snapshot_copper}b for $t = 91.65~\text{attoseconds}$.
%As $\mathrm{H^+}$ travels through the $\mathrm{Cu}$ crystal more electron density is acquired from the neighboring atoms as seen at $t = 91.65~\text{attoseconds}$.