From 09f8d77a2eb77809de207180f94fe4cb88899546 Mon Sep 17 00:00:00 2001 From: Eric Teunis de Boone Date: Fri, 3 Nov 2023 18:27:00 +0100 Subject: [PATCH] Thesis: Single: use new GridPower figures --- .../chapters/single_sine_interferometry.tex | 40 ++++++++++++++++++- 1 file changed, 39 insertions(+), 1 deletion(-) 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}