X-Git-Url: https://hackdaworld.org/gitweb/?p=lectures%2Flatex.git;a=blobdiff_plain;f=posic%2Fthesis%2Fdefects.tex;fp=posic%2Fthesis%2Fdefects.tex;h=ac2228801f04972435f3465986db5cde8697e170;hp=c0acc816889018b9d9c6fee2a57daa31b63c64b7;hb=6821480ec78fa84077694a42dac10bf5f39ced33;hpb=b015eabfb0306ead1d94cb6c0e505806aca2798e

diff --git a/posic/thesis/defects.tex b/posic/thesis/defects.tex
index c0acc81..ac22288 100644
--- a/posic/thesis/defects.tex
+++ b/posic/thesis/defects.tex
@@ -1275,7 +1275,7 @@ Resulting binding energies of a C$_{\text{i}}$ DB and a nearby vacancy are liste
 \end{figure}
 Figure~\ref{fig:defects:comb_db_06} shows the associated configurations.
 All investigated structures are preferred compared to isolated, largely separated defects.
-In contrast to C$_{\text{s}}$ this is also valid for positions along \hkl[1 1 0] resulting in an entirely attractive interaction between defects of these types.
+In contrast to C$_{\text{s}}$, this is also valid for positions along \hkl[1 1 0] resulting in an entirely attractive interaction between defects of these types.
 Even for the largest possible distance (R) achieved in the calculations of the periodic supercell a binding energy as low as \unit[-0.31]{eV} is observed.
 The creation of a vacancy at position 1 results in a configuration of substitutional C on a Si lattice site and no other remaining defects.
 The \ci{} DB atom moves to position 1 where the vacancy is created and the \si{} DB atom recaptures the DB lattice site.