X-Git-Url: https://hackdaworld.org/gitweb/?p=lectures%2Flatex.git;a=blobdiff_plain;f=posic%2Fthesis%2Fdefects.tex;h=b8a58fbfffb8aa40edbaddbf683056b4a646f168;hp=57809905034c5f0d1efff2895a87fd614224d7d7;hb=bddc8d909e9a701c50ee4f68163343067faf9f69;hpb=9ed87418d6969979b996d6b692ab2e706f1a395f diff --git a/posic/thesis/defects.tex b/posic/thesis/defects.tex index 5780990..b8a58fb 100644 --- a/posic/thesis/defects.tex +++ b/posic/thesis/defects.tex @@ -1181,6 +1181,8 @@ Again, conclusions concerning the probability of formation are drawn by investig Since C$_{\text{s}}$ is unlikely to exhibit a low activation energy for migration the focus is on C$_{\text{i}}$. Pathways starting from the next most favored configuration, i.e. \cs{} located at position 2, into configuration a and b are investigated, which show activation energies above \unit[2.2]{eV} and \unit[2.5]{eV}. The respective barriers and structures are shown in Fig.~\ref{fig:051-xxx}. +Again, the non-magnetic configuration is obtained. +If not forced by the CRT algorithm, the structures beyond \perc{50} displacement of the transition into configuration a would likewise settle into configuration b. \begin{figure}[tp] \begin{center} \includegraphics[width=0.7\textwidth]{comb_mig_051-xxx_conf.ps}