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Thesis: Single: use new GridPower figures

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Eric Teunis de Boone 2023-11-03 18:27:00 +01:00
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documents/thesis/chapters/single_sine_interferometry.tex
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@ -430,7 +430,7 @@ Additionally, since the true period shifts are static per event, the evaluation
\end{subfigure} \end{subfigure}
\\ \\
\begin{subfigure}[t]{0.9\textwidth} \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 \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} \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{ \caption{
@ -458,5 +458,43 @@ Additionally, since the true period shifts are static per event, the evaluation
} }
\label{fig:grid_power_time_fixes} \label{fig:grid_power_time_fixes}
\end{figure}%>>> \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} \end{document}