m-thesis-documentation/presentations/2022-02-03_group_meeting/2022-02-03_group_meeting.tex

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\documentclass[showdate=false]{beamer}
\usepackage[british]{babel}
\usepackage{amsmath}
\usepackage{hyperref}
\usepackage[backend=bibtex,style=trad-plain]{biblatex}
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\graphicspath{{.}{../../figures/}}
\addbibresource{../../../bibliotheca/bibliography.bib}
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\AtBeginSection[]
{
\begin{frame}<beamer>{Table of Contents}
\tableofcontents[currentsection, currentsubsection, sectionstyle=show/shaded, subsectionstyle=hide]
\end{frame}
}
% no to navigation, yes to frame numbering
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\title[Timing Accuracy]{Timing Accuracy in Air Shower Detectors}
\date{February 10, 2022}
\author{E.T. de Boone}
\begin{document}
\frame{\titlepage}
\section{Timing Mechanisms in Detectors}
\begin{frame}{Timing Mechanisms}
\begin{block}{Why improve timing accuracy?}
\begin{itemize}
\item Better statistics (narrow down direction of air showers)
\item Interferometry
\end{itemize}
\end{block}
\begin{block}{Strategy}
\begin{itemize}
\item Simulations for synchronisation techniques
\item Characterising current methods
\end{itemize}
\end{block}
\end{frame}
\begin{frame}{Characterising current methods}
\begin{block}{Current Timing Methods}
\begin{itemize}
\item GNSS (online)
\item Beacon (offline)
\end{itemize}
\end{block}
\vspace{2em}
\begin{itemize}
\item GPS Accuracy $\leq 30 \mathrm{ns}$ for $95$\% time (often better)
\item Total time accuracy in the order of 5 -- 10~ns
\item More accurate reference timing needed to characterise/improve current mechanisms.
\end{itemize}
\end{frame}
%%%%%%%%%%%%%
\subsection{Beacon}
\begin{frame}{Timing Mechanisms: Beacon}
\begin{itemize}
\item Beating between frequency signals indicate timing
\item PA: located in physics band $\mapsto$ offline analysis, \\
corrects for GPS drift.
\item different frequency responses for antenna models and directions
\end{itemize}
\begin{columns}
\begin{column}{.5\textwidth}
\begin{figure}
\includegraphics[width=\textwidth]{beacon/auger/1512.02216.figure2.beacon_beat.png}
\caption{
\cite{PierreAuger:2015aqe}
Four beacon frequencies beating at PA.
}
\end{figure}
\end{column}
\begin{column}{.5\textwidth}
\begin{figure}
\includegraphics[width=\textwidth]{beacon/auger/1512.02216.figure4.ads-b.png}
%\caption{
% \cite{PierreAuger:2015aqe}
% ADS-B and signal intercepts.
%}
\end{figure}
\end{column}
\end{columns}
\end{frame}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\section{Experimental Setup: White Rabbit}
\subsection[PTP]{Precision Time Protocol}
\begin{frame}{Precision Time Protocol}
\begin{itemize}
\item Time synchronisation over (long) distance between (multiple) nodes
\end{itemize}
\begin{figure}
\includegraphics[width=0.4\textwidth]{white-rabbit/protocol/ptpMSGs-color.pdf}
\caption{
\cite{WRPTP}
Precision Time Protocol messages.
}
\end{figure}
\end{frame}
%%%%%%%%%%%%%
\subsection[WR]{White Rabbit}
\begin{frame}{White Rabbit}
\begin{columns}
\begin{column}{.5\textwidth}
White Rabbit:
\begin{itemize}
\item SyncE (common oscillator)
\item PTP (synchronisation)
\end{itemize}
\vspace{2em}
Factors:
\begin{itemize}
\item device ($\Delta_{txm}$, $\Delta_{rxs}$, ...)
\item link ($\delta_{ms}$, ...)
\end{itemize}
\begin{figure}
\makebox[\textwidth][c]{\includegraphics[width=1.1\textwidth]{white-rabbit/protocol/delaymodel.pdf}}
%\caption{\small From \cite{WRPTP}}.
\end{figure}
\end{column}
\begin{column}{.5\textwidth}
\begin{figure}
\makebox[\textwidth][c]{\includegraphics[width=1.1\textwidth]{white-rabbit/protocol/wrptpMSGs_1.pdf}}
%\caption{From \cite{WRPTP}}.
\end{figure}
\end{column}
\end{columns}
\end{frame}
\begin{frame}{White Rabbit}
\begin{figure}
\centering
\includegraphics<1>[width=0.8\textwidth]{gnss/phase-delocked-gps-white-rabbit-setup-colored.pdf}
\includegraphics<2>[width=0.8\textwidth]{gnss/phase-locked-gps-white-rabbit-setup-colored.pdf}
\end{figure}
\end{frame}
%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%
\section{Fourier and Phase information}
\begin{frame}{(Discrete) Fourier and Phase}
\begin{equation*}
\hspace{-2em}
u(t) = \exp(i2\pi ft + \phi_t) \xrightarrow{\mathrm{Fourier\; Transform}} f', \phi_f
\end{equation*}
\begin{block}{Discrete Fourier Transform}
\begin{equation*}
N_\mathrm{required} := f_\mathrm{sample\_rate} / f_\mathrm{signal}
\end{equation*}
\begin{equation*}
f_\mathrm{Nyquist} = \frac{1}{2} f_\mathrm{sample\_rate}
\end{equation*}
\end{block}
\includegraphics[width=\textwidth]{fourier/02-fourier_phase-f_max_showcase.pdf}
\end{frame}
%%%%%%%%%%%%%
\subsection{Phase reconstruction}
\begin{frame}{Phase reconstruction?}
\begin{block}{}
\begin{equation*}
u(t) = \exp(2i\pi ft + \phi_t)
\end{equation*}
\end{block}
\begin{figure}
\makebox[\textwidth][c]{\includegraphics[width=1.4\textwidth]{fourier/02-fourier_phase-phi_f_vs_phi_t.pdf}}%
\end{figure}
\begin{block}{}
Phase reconstruction is easy if sample rate ``correct''
\end{block}
\end{frame}
%%%%%%%%%%%%%
\begin{frame}{Phase reconstruction?}
\begin{block}{}
What if sample rate ``incorrect''? \\
\end{block}
\begin{block}<2->{}
$\rightarrow$ Linear interpolation ({\small $f_\mathrm{signal}$, $f_\mathrm{max}$, $f_\mathrm{submax}$, $\phi_\mathrm{max}$ and $\phi_\mathrm{submax}$})
\end{block}
\vspace{2em}
\begin{figure}
\makebox[\textwidth][c]{
\includegraphics<1-2>[width=1.4\textwidth]{fourier/02-fourier_phase-phi_f_vs_f_max_increasing_N_samples.pdf}
\includegraphics<3>[width=1.3\textwidth]{fourier/02-fourier_phase-phase_reconstruction-unfolded.pdf}
\includegraphics<4>[width=1.3\textwidth]{fourier/02-fourier_phase-phase_reconstruction-unfolded-zoomed.pdf}
}%
\end{figure}
\end{frame}
%%%%%%%%%%%%%
\subsection{Without interpolation?}
\begin{frame}{Without interpolation? (Coming)}
\begin{figure}
\makebox[\textwidth][c]{\includegraphics[width=1.3\textwidth]{fourier/02-fourier_phase-relative_amplitudes_vs_N_samples_absolute.pdf}}\\%
\makebox[\textwidth][c]{\includegraphics[width=1.3\textwidth]{fourier/02-fourier_phase-relative_amplitudes_vs_N_samples_power.pdf}}\\%
\end{figure}
\end{frame}
%%%%%%%%%%%%%
\section*{References}
\begin{frame}{References}
\printbibliography
\end{frame}
\end{document}