Thesis+Figure: Split Cable Measurements at 50MHz

documents/thesis/chapters/grand_characterisation.tex

@@ -68,7 +68,7 @@ Both the \gls{ADC} and the filterchains introduce systematic delays.
 Since each channel corresponds to a polarisation, it is important that relative systematic delays between the channels can be accounted for.
 \\
 
-\begin{figure}[h]
+\begin{figure}
 	\centering
 	\includegraphics[width=0.4\textwidth]{grand/setup/channel-delay-setup.pdf}
 	\caption{
@@ -115,12 +115,36 @@ However, because it is symmetric for both setups, this does not affect the measu
 		\label{fig:split-cable:waveform}
 	\end{subfigure}
 	\caption{
-		Waveforms of the sine wave measured in the ``forward'' setup and the phase shift between the channels.
+		Waveforms of the sine wave measured in the ``forward'' setup and their spectra near the testing frequency of $50\MHz$..
-		The sine wave was emitted at $50\MHz$ at $200\;\mathrm{mVpp}$.
+		The sine wave was emitted at $200\;\mathrm{mVpp}$.
 	}
 	\label{fig:grand:signal}
 \end{figure}% >>>
 
+\begin{figure}% <<< fig:grand:phaseshift
+	\centering
+	\includegraphics[width=0.47\textwidth]{grand/split-cable/sine-sweep/ch2ch4fig8-histogram.50.pdf}
+	\caption{
+		Histogram of the measured phase shifts in Figure~\ref{fig:grand:phaseshift:measruement}.
+	}
+	\label{fig:grand:phaseshift}
+\end{figure}% >>>
+
+\begin{figure}% <<< fig:grand:phaseshift:measurements
+	\centering
+	\begin{subfigure}{0.47\textwidth}
+		\includegraphics[width=0.47\textwidth]{grand/split-cable/sine-sweep/ch2ch4fig9-measurements.forward.50.pdf}
+	\end{subfigure}
+	\hfill
+	\begin{subfigure}{0.47\textwidth}
+		\includegraphics[width=0.47\textwidth]{grand/split-cable/sine-sweep/ch2ch4fig9-measurements.backward.50.pdf}
+	\end{subfigure}
+	\caption{
+		The measured phase shifts at $50\MHz$ converted to a time delay.
+	}
+	\label{fig:grand:phaseshift}
+\end{figure}
+
 %\begin{figure}% <<<<
 %	\centering
 %	\begin{subfigure}{0.45\textwidth}

documents/thesis/chapters/single_sine_interferometry.tex

@@ -190,7 +190,6 @@ Of course, a gaussian white noise component is introduced to the waveform as a s
 		The green dashed lines indicate the measured beacon parameters.
 		The amplitude spectrum clearly shows a strong component at roughly $50\MHz$.
 		The phase spectrum of the original waveform shows the typical behaviour for a short pulse.
-		\protect\Todo{ft amplitude airshower x1000}
 	}
 	\label{fig:single:proton}
 \end{figure}% >>>
@@ -211,7 +210,7 @@ Since the beacon can be recorded for much longer than the air shower signal, we
 The remaining waveform is fed into a \gls{DTFT} \eqref{eq:fourier:dtft} to measure the beacon's phase $\pMeas$ and amplitude.
 Note that due to explicitly including a time axis in a \gls{DTFT}, a number of samples can be omitted without introducing artifacts.
 \\
-With the obtained beacon parameters, the air shower signal is in turn reconstructed by subtracting the beacon from the full waveform in the time domain.\Todo{cite GAP note?}
+With the obtained beacon parameters, the air shower signal is in turn reconstructed by subtracting the beacon from the full waveform in the time domain.
 \\
 The small clock defect $\tClockPhase$ is then finally calculated from the beacon's phase $\pMeas$ by subtracting the phase introduced by the propagation from the beacon transmitter.
 \\
@@ -284,7 +283,7 @@ Afterwards, a new grid zooms in on the power maximum and the process is repeated
 	\begin{subfigure}[t]{0.45\textwidth}
 		\includegraphics[width=\textwidth]{ZH_simulation/findks/ca_period_from_shower.py.reconstruction.run0.power.pdf}
 		\caption{
-			Power measurement with the $k$s belonging to the overall maximum of the amplitude maxima.
+			Power measurement with the $k$'s belonging to the overall maximum of the amplitude maxima.
 		}
 		\label{fig:findks:reconstruction}
 	\end{subfigure}
@@ -308,7 +307,7 @@ Afterwards, a new grid zooms in on the power maximum and the process is repeated
 	\begin{subfigure}[t]{0.45\textwidth}
 		\includegraphics[width=\textwidth]{ZH_simulation/findks/ca_period_from_shower.py.maxima.run2.pdf}
 		\caption{
-			Final test grid obtaining the same $k$ as Figure~\ref{fig:findks:maxima:zoomed}.
+			Final test grid obtaining the same $k$'s as Figure~\ref{fig:findks:maxima:zoomed}.
 		}
 		\label{fig:findks:maxima:zoomed2}
 	\end{subfigure}
@@ -476,7 +475,6 @@ Additionally, since the true period shifts are static per event, evaluating the
 		their effect on (\textit{right}) the alignment of the waveforms at the true axis
 			and (\textit{left}) the interferometric power near the simulation axis (red plus).
 		The maximum power is indicated by the blue cross.
-%		\protect\Todo{x-axis relative to reference waveform, remove titles, no SNR}
 	}
 	\label{fig:grid_power_time_fixes}
 \end{figure}%>>>