diff --git a/documents/thesis/chapters/single_sine_interferometry.tex b/documents/thesis/chapters/single_sine_interferometry.tex
index c4a6aac..93bd57f 100644
--- a/documents/thesis/chapters/single_sine_interferometry.tex
+++ b/documents/thesis/chapters/single_sine_interferometry.tex
@@ -430,7 +430,7 @@ Additionally, since the true period shifts are static per event, the evaluation
 	\end{subfigure}
 	\\
 	\begin{subfigure}[t]{0.9\textwidth}
-		\includegraphics[width=0.45\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X400.repair_all.scale4d.pdf}
+		\includegraphics[width=0.45\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X400.repair_full.scale4d.pdf}
 		\hfill
 		\includegraphics[width=0.46\textwidth]{radio_interferometry/trace_overlap/on-axis/dc_grid_power_time_fixes.py.repair_full.axis.X400.trace_overlap.zoomed.repair_full.pdf}
 		\caption{
@@ -458,5 +458,43 @@ Additionally, since the true period shifts are static per event, the evaluation
 	}
 	\label{fig:grid_power_time_fixes}
 \end{figure}%>>>
+
+\begin{figure}%<<< grid_power:axis:X600
+	\centering
+	\begin{subfigure}[t]{0.9\textwidth}
+		\includegraphics[width=0.45\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X200.repair_full.scale2d.pdf}
+		\hfill
+		\includegraphics[width=0.45\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X200.repair_full.scale02d.pdf}
+		\caption{$X=200\,\mathrm{g/cm^2}$}
+		\label{fig:grid_power:axis:X200}
+	\end{subfigure}
+	\begin{subfigure}[t]{0.9\textwidth}
+		\includegraphics[width=0.45\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X400.repair_full.scale2d.pdf}
+		\hfill
+		\includegraphics[width=0.45\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X400.repair_full.scale02d.pdf}
+		\caption{$X=400\,\mathrm{g/cm^2}$}
+		\label{fig:grid_power:axis:X400}
+	\end{subfigure}
+	\begin{subfigure}[t]{0.9\textwidth}
+		\includegraphics[width=0.45\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X600.repair_full.scale2d.pdf}
+		\hfill
+		\includegraphics[width=0.45\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X600.repair_full.scale02d.pdf}
+		\caption{$X=600\,\mathrm{g/cm^2}$}
+		\label{fig:grid_power:axis:X600}
+	\end{subfigure}
+	\begin{subfigure}[t]{0.9\textwidth}
+		\includegraphics[width=0.45\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X800.repair_full.scale2d.pdf}
+		\hfill
+		\includegraphics[width=0.45\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X800.repair_full.scale02d.pdf}
+		\caption{$X=800\,\mathrm{g/cm^2}$}
+		\label{fig:grid_power:axis:X800}
+	\end{subfigure}
+	\caption{
+		Interferometric power for the fully resolved clocks at four atmospheric depths for an opening angle of $2^\circ$(\textit{left}) and $0.2^\circ$(\textit{right}).
+		The simulation axis is indicated by the red plus, the maximum power is indicated by the blue cross.
+		Except for \subref{fig:grid_power:axis:X800}, the shower axis is resolved within $0.1^\circ$ of the true shower axis.
+	}
+	\label{fig:grid_power:axis}
+\end{figure}
 % >>>
 \end{document}