this is for holding javascript data
Alfredo A. Correa edited Even_today_the_inclusion_of__.tex
almost 8 years ago
Commit id: a00ff21517e91b93d7e85b4b082f73efe2ccb1d4
deletions | additions
diff --git a/Even_today_the_inclusion_of__.tex b/Even_today_the_inclusion_of__.tex
index 93ca797..880b16f 100644
--- a/Even_today_the_inclusion_of__.tex
+++ b/Even_today_the_inclusion_of__.tex
...
%It is an attractive method because it is both self-consistency and non-perturbative \cite{Kohn_1965} allowing for an atomistic \emph{ab initio} description at a reasonable computational cost for simulation cells below a few hundred atoms. Alternatively, time dependent tight-binding have been proposed as well to overcome some size limitations \cite{Mason_2012} at the price of additional approximations.
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 affects the interatomic forces relative to the adiabatic outcome. Recently Schleife \emph{et al.} \cite{Schleife_2015} have calculated the electronic stopping power ($S_\text{e}$) by $\mathrm{H}$ and $\mathrm{He}$ projectile including
TDDFT non-adiabatic electron dynamics and found that off-channeling trajectories along with the inclusion of semicore electrons enhance $S_\text{e}$,
finally resulting
in much better agreement with the \textsc{Srim}
experimental and modeled data \cite{Ziegler_2010}.
\textsc{Srim} \cite{Ziegler_2010} also 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 $\mathrm{Cu}$.
%