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figures/ZH_simulation/array_geometry_beacon_amplitude.png
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figures/ZH_simulation/ba_measure_beacon_phase.py.A74.masked.pdf
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figures/ZH_simulation/signal_to_noise_definition.pdf
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presentations/2022-12-15_group_meeting/2022-12-15_CRHEP.tex
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presentations/2022-12-15_group_meeting/2022-12-15_CRHEP.tex
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\documentclass[showdate=false]{beamer}
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\usepackage[british]{babel}
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\usepackage{amsmath}
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\usepackage{hyperref}
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\usepackage[backend=bibtex,style=trad-plain]{biblatex}
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\usepackage{graphicx}
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\graphicspath{{.}{../../figures/}}
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\usepackage{todo}
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||||||
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\addbibresource{../../../bibliotheca/bibliography.bib}
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||||||
|
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||||||
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% Disable Captions
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||||||
|
\setbeamertemplate{caption}{\raggedright\small\insertcaption\par}
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||||||
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||||||
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% Show Section overview at beginning of section
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||||||
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%\AtBeginSection[]
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||||||
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%{
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||||||
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% \begin{frame}<beamer>{Table of Contents}
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||||||
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% \tableofcontents[currentsection, currentsubsection, sectionstyle=show/shaded, subsectionstyle=hide]
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||||||
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% \end{frame}
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||||||
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%}
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||||||
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||||||
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% no to navigation, yes to frame numbering
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||||||
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\beamertemplatenavigationsymbolsempty
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\setbeamerfont{page number in head/foot}{size=\normalsize}
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\setbeamertemplate{footline}[frame number]
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\title[Beacon Timing]{Enhancing Timing Accuracy using Beacons}
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\date{Dec 15, 2022}
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\author{E.T. de Boone}
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||||||
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\begin{document}
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||||||
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\frame{\titlepage}
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||||||
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||||||
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\begin{frame}{Enhancing time accuracy}
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||||||
|
\begin{block}{}
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||||||
|
Goal: $\sigma_{ij} < 1\mathrm{ns}$
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||||||
|
(enabling Radio Interferometry)
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||||||
|
\end{block}
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||||||
|
|
||||||
|
\begin{block}{Strategy}
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||||||
|
\begin{itemize}
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||||||
|
\item Simulating beacons (both pulse and sine)
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\item Characterising GNSS (GRAND)
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||||||
|
\end{itemize}
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||||||
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\end{block}
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\end{frame}
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||||||
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||||||
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% Antenna Setup
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\section{Beacon}
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|
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||||||
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\begin{frame}{Antenna Setup}
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\begin{block}{}
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Local time $t_i$ due to time delay $t_{\mathrm{d}i}$ and clock skew $\sigma_i$\\
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\end{block}
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\begin{figure}
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\includegraphics[width=0.8\textwidth]{beacon/antenna_setup_two.pdf}
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\end{figure}
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\vskip -2em
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|
\begin{equation*}
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\Delta t'_{12} = t'_1 - t'_2 = \Delta t_{\mathrm{d}12} + \sigma_{12} + (t_0 - t_0)
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\end{equation*}
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\end{frame}
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\begin{frame}{Beacon: Sine: Two traces}
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\begin{equation*}
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t'_i = (\frac{\varphi'_i}{2\pi} + n_i)T = A_i + B_i
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\end{equation*}
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\begin{figure}
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\includegraphics[width=1\textwidth]{beacon/08_beacon_sync_timing_outline.pdf}
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\end{figure}
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|
\begin{align*}
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\Delta t_{ij} &= (A_j + B_j) - (A_i + B_i) + \Delta t_\varphi \\
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&= \Delta A_{ij} + \Delta t_\varphi + k_{ij}T\\
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\end{align*}
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\end{frame}
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\begin{frame}{Beacon: Sine: Two traces: Discrete solutions}
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\begin{figure}
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\includegraphics<1>[width=1\textwidth]{beacon/08_beacon_sync_timing_outline.pdf}
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%\includegraphics<2>[width=1\textwidth]{beacon/08_beacon_sync_synchronised_period_alignment.pdf}
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|
\end{figure}
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|
\begin{figure}
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\includegraphics[width=1\textwidth]{beacon/08_beacon_sync_coherent_sum.pdf}
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\end{figure}
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\end{frame}
|
||||||
|
|
||||||
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\begin{frame}{Simulation}
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\begin{block}{}
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||||||
|
Apply same steps to an airshower simulation:
|
||||||
|
\begin{itemize}
|
||||||
|
\item Add (sine) beacon to each antenna
|
||||||
|
\item Shift clocks
|
||||||
|
\item Measure phase
|
||||||
|
\item Repair clocks for small offset
|
||||||
|
\item Approximate
|
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|
\end{itemize}
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|
\end{block}
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|
\end{frame}
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|
\begin{frame}{}
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\begin{figure}
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\includegraphics<1>[width=1\textwidth]{figs/orig_antenna_geometry.pdf}
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\end{figure}
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|
\end{frame}
|
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|
|
||||||
|
\begin{frame}{Simulation: Phase: Local }
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|
\begin{block}{}
|
||||||
|
@Antenna $i$: measure phase $\varphi_i$ , get $\varphi(\sigma_i) = \varphi_i - \varphi(t_0) - \varphi(t_{\mathrm{d}i})$
|
||||||
|
\end{block}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics<1>[width=1\textwidth]{figs/ba_measure_beacon_phase.py.A63.pdf}
|
||||||
|
\includegraphics<2>[width=1\textwidth]{figs/ba_measure_beacon_phase.py.A63.zoomed.pdf}
|
||||||
|
\includegraphics<3>[width=1\textwidth]{figs/bb_measure_true_phase.py.F0.05153.pdf}
|
||||||
|
\end{figure}
|
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|
\end{frame}
|
||||||
|
|
||||||
|
\begin{frame}{Simulation: Phase: Baseline}
|
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|
\begin{block}{}
|
||||||
|
@Baseline $i,j$: $\Delta \varphi_{ij} = \varphi(\sigma_i) - \varphi(\sigma_j)$ \\
|
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|
|
||||||
|
Minimise matrix:
|
||||||
|
$\left(\begin{matrix}
|
||||||
|
\Delta_{11} & \Delta_{12} & \Delta_{13} & \\
|
||||||
|
\Delta_{21} & \Delta_{22} & \Delta_{23} & \\
|
||||||
|
\Delta_{31} & \Delta_{32} & \Delta_{33} & \\
|
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|
\end{matrix}\right)$
|
||||||
|
\end{block}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics<1>[width=1\textwidth]{figs/bc_baseline_phase_deltas.py.0ns.1.F0.05153.pdf}
|
||||||
|
\includegraphics<2>[width=1\textwidth]{figs/bc_baseline_phase_deltas.py.5ns_gauss1.F0.05153.pdf}
|
||||||
|
\end{figure}
|
||||||
|
\end{frame}
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|
|
||||||
|
\begin{frame}{Simulation: Period $k$}
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||||||
|
\begin{block}{}
|
||||||
|
Interferometry while allowing to shift by $T = 1/f_\mathrm{beacon}$
|
||||||
|
\end{block}
|
||||||
|
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics<1>[width=1\textwidth]{figs/ca_period_from_shower.py.loc12.0-2894.2-7780.1.i5.run2.pdf}
|
||||||
|
\includegraphics<2>[width=1\textwidth]{figs/ca_period_from_shower.py.loc12.0-2894.2-7780.1.i5.run2.zoomed.peak.pdf}
|
||||||
|
\includegraphics<3>[width=1\textwidth]{figs/ca_period_from_shower.py.loc12.0-2894.2-7780.1.i5.run2.zoomed.beacon.pdf}
|
||||||
|
\includegraphics<4>[width=1\textwidth]{figs/bc_period_from_shower.py.maxima.run0.0ns.pdf}
|
||||||
|
\end{figure}
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
\begin{frame}{Interferometry}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics<1>[width=1\textwidth]{figs/reconstruct_5ns.pdf}
|
||||||
|
\includegraphics<2>[width=1\textwidth]{figs/reconstruct_15ns.pdf}
|
||||||
|
\end{figure}
|
||||||
|
\end{frame}
|
||||||
|
\end{document}
|
3
presentations/2022-12-15_group_meeting/README.md
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presentations/2022-12-15_group_meeting/README.md
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||||||
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# Short Presentation on current status (Beacon)
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Mostly to show what I've been doing uptil now.
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presentations/2022-12-15_group_meeting/figs/reconstruct_15ns.pdf
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presentations/2022-12-15_group_meeting/figs/reconstruct_15ns.pdf
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presentations/2022-12-15_group_meeting/figs/reconstruct_5ns.pdf
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presentations/2022-12-15_group_meeting/figs/reconstruct_5ns.pdf
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286
presentations/2023-04-13_group_meeting/2023-04-13_CRHEP.tex
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presentations/2023-04-13_group_meeting/2023-04-13_CRHEP.tex
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@ -0,0 +1,286 @@
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\documentclass[showdate=false]{beamer}
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|
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|
\usepackage[british]{babel}
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\usepackage{amsmath}
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\usepackage{hyperref}
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|
\usepackage[backend=bibtex,style=trad-plain]{biblatex}
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|
\usepackage{graphicx}
|
||||||
|
\graphicspath{{.}{../../figures/}}
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\usepackage{todo}
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\usepackage{physics}
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\usepackage{cancel}
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||||||
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||||||
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\addbibresource{../../../bibliotheca/bibliography.bib}
|
||||||
|
|
||||||
|
% Disable Captions
|
||||||
|
\setbeamertemplate{caption}{\raggedright\small\insertcaption\par}
|
||||||
|
|
||||||
|
% Show Section overview at beginning of section
|
||||||
|
%\AtBeginSection[]
|
||||||
|
%{
|
||||||
|
% \begin{frame}<beamer>{Table of Contents}
|
||||||
|
% \tableofcontents[currentsection, currentsubsection, sectionstyle=show/shaded, subsectionstyle=hide]
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||||||
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% \end{frame}
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||||||
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%}
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||||||
|
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||||||
|
% no to navigation, yes to frame numbering
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||||||
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\beamertemplatenavigationsymbolsempty
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\setbeamerfont{page number in head/foot}{size=\normalsize}
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||||||
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\setbeamertemplate{footline}[frame number]
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||||||
|
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||||||
|
\title[Beacon Timing]{Enhancing Timing Accuracy using Beacons}
|
||||||
|
\date{Apr 13, 2023}
|
||||||
|
\author{E.T. de Boone}
|
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||||||
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||||||
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||||||
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\newcommand{\pTrue}{\phi}
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\newcommand{\PTrue}{\Phi}
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\newcommand{\pMeas}{\varphi}
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||||||
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\newcommand{\pTrueEmit}{\pTrue_0}
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\newcommand{\pTrueArriv}{\pTrueArriv'}
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\newcommand{\pMeasArriv}{\pMeas_0}
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||||||
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\newcommand{\pProp}{\pTrue_d}
|
||||||
|
\newcommand{\pClock}{\pTrue_c}
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||||||
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||||||
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||||||
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||||||
|
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||||||
|
|
||||||
|
|
||||||
|
\begin{document}
|
||||||
|
\frame{\titlepage}
|
||||||
|
|
||||||
|
\begin{frame}{Enhancing time accuracy}
|
||||||
|
\begin{block}{}
|
||||||
|
Goal: $\sigma_{ij} < 1\mathrm{ns}$
|
||||||
|
(enabling Radio Interferometry)
|
||||||
|
\end{block}
|
||||||
|
|
||||||
|
\begin{block}{Strategy}
|
||||||
|
\begin{itemize}
|
||||||
|
\item Simulating beacons (both pulse and sine)
|
||||||
|
\item Characterising GNSS (GRAND)
|
||||||
|
\end{itemize}
|
||||||
|
\end{block}
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
% Antenna Setup
|
||||||
|
\section{Beacon}
|
||||||
|
\begin{frame}{Antenna Setup}
|
||||||
|
\vskip -2em
|
||||||
|
Local antenna time $t'_i$ due to time delay $t_{\mathrm{d}i}$ and clock skew $\sigma_i$
|
||||||
|
\\
|
||||||
|
\small\begin{equation*}
|
||||||
|
t'_i = t_{tx} + t_{\mathrm{d}i} + \sigma_i
|
||||||
|
\end{equation*}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics[width=0.6\textwidth]{beacon/antenna_setup_two.pdf}
|
||||||
|
\end{figure}
|
||||||
|
\vskip -2em
|
||||||
|
\begin{equation*}
|
||||||
|
\Delta t'_{12} = t'_1 - t'_2 = \Delta t_{\mathrm{d}12} + \sigma_{12} + (t_{tx} - t_{tx})
|
||||||
|
\end{equation*}
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
\begin{frame}{Beacon: Sine: Two traces}
|
||||||
|
Required signal: sine (beacon) + single pulse
|
||||||
|
\begin{equation*}
|
||||||
|
t'_i = (\frac{\varphi'_i}{2\pi} + n_i)T = A_i + B_i
|
||||||
|
\end{equation*}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics<1>[width=1\textwidth]{beacon/08_beacon_sync_timing_outline.pdf}
|
||||||
|
\includegraphics<2>[width=1\textwidth]{beacon/08_beacon_sync_synchronised_outline.pdf}
|
||||||
|
\end{figure}
|
||||||
|
\begin{align*}
|
||||||
|
\Delta t'_{ij} &= (A_j + B_j) - (A_i + B_i) + \Delta t'_\varphi \\
|
||||||
|
&= \Delta A_{ij} + \only<1>{\Delta t'_\varphi}\only<2->{\cancel{\Delta t'_\varphi}} + k_{ij}T\\
|
||||||
|
\end{align*}
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
\begin{frame}{Beacon: Sine: Two traces: Discrete solutions}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics<1>[width=1\textwidth]{beacon/08_beacon_sync_synchronised_outline.pdf}
|
||||||
|
\includegraphics<2->[width=1\textwidth]{beacon/08_beacon_sync_synchronised_period_alignment.pdf}
|
||||||
|
\end{figure}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics<-2>[width=1\textwidth]{beacon/08_beacon_sync_coherent_sum.pdf}
|
||||||
|
\end{figure}
|
||||||
|
\only<3>{\begin{equation*}\Delta t'_{ij} = \Delta A_{ij} + \cancel{\Delta t'_\varphi} + \cancel{k_{ij}T} \end{equation*}}
|
||||||
|
\only<3>\vfill
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
\section{Simulations}
|
||||||
|
\begin{frame}{Simulation: Sine}
|
||||||
|
Apply previous steps to an airshower simulation (providing the pulse):
|
||||||
|
\begin{block}{}
|
||||||
|
\begin{itemize}
|
||||||
|
\item Add (sine) beacon to each antenna
|
||||||
|
\item Shift clocks
|
||||||
|
\item Measure phase
|
||||||
|
\item Repair clocks for small offset $\Delta t'_{ij}$
|
||||||
|
\item Iteratively find best $k_{ij}$
|
||||||
|
\end{itemize}
|
||||||
|
\end{block}
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
\begin{frame}{Simulation: Antenna Setup}
|
||||||
|
\begin{columns}
|
||||||
|
\begin{column}{0.5\textwidth}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics[width=\textwidth]{ZH_simulation/tx_array_geometry.png}
|
||||||
|
\end{figure}
|
||||||
|
\end{column}
|
||||||
|
\hfill
|
||||||
|
\begin{column}{0.45\textwidth}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics[width=\textwidth]{ZH_simulation/array_geometry_beacon_amplitude.png}
|
||||||
|
\end{figure}
|
||||||
|
\end{column}
|
||||||
|
\end{columns}
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
\begin{frame}{Simulation: Measure Local Phase}
|
||||||
|
\begin{block}{}
|
||||||
|
@Antenna $i$: measure phase $\varphi_i$ using DTFT, get $\varphi(\sigma_i) = \varphi_i - \varphi(t_0) - \varphi(t_{\mathrm{d}i})$
|
||||||
|
\end{block}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics<1>[width=0.8\textwidth]{ZH_simulation/ba_measure_beacon_phase.py.A74.no_mask.pdf}
|
||||||
|
\includegraphics<2>[width=0.8\textwidth]{ZH_simulation/ba_measure_beacon_phase.py.A74.masked.pdf}
|
||||||
|
\end{figure}
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
\begin{frame}{Simulation: Phase measurement}
|
||||||
|
Beacon frequency: $51.53~\mathrm{MHz}$
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics<1>[width=0.8\textwidth]{ZH_simulation/bd_antenna_phase_deltas.py.phase.residuals.c5_b_N4096_noise1e1.pdf}
|
||||||
|
\includegraphics<2>[width=0.45\textwidth]{ZH_simulation/bd_antenna_phase_deltas.py.phase.residuals.c5_b_N4096_noise1e1.pdf}
|
||||||
|
\hfill
|
||||||
|
\includegraphics<2>[width=0.45\textwidth]{ZH_simulation/bd_antenna_phase_deltas.py.phase.residuals.c5_b_N4096_noise1e3.pdf}
|
||||||
|
\\
|
||||||
|
\vspace{0.5cm}
|
||||||
|
\includegraphics<2>[width=0.45\textwidth]{ZH_simulation/bd_antenna_phase_deltas.py.phase.residuals.c5_b_N4096_noise1e4.pdf}
|
||||||
|
\hfill
|
||||||
|
\includegraphics<2>[width=0.45\textwidth]{ZH_simulation/bd_antenna_phase_deltas.py.phase.residuals.c5_b_N4096_noise1e5.pdf}
|
||||||
|
\end{figure}
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
\begin{frame}{Simulation: Signal to Noise}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics[width=0.8\textwidth]{beacon/time_res_vs_snr.pdf}
|
||||||
|
\end{figure}
|
||||||
|
\begin{columns}
|
||||||
|
\begin{column}{0.3\textwidth}
|
||||||
|
\end{column}
|
||||||
|
\begin{column}{0.7\textwidth}
|
||||||
|
\tiny\begin{equation*}
|
||||||
|
p_\PTrue(\pTrue; s, \sigma) =
|
||||||
|
\frac{ e^{-\left(\frac{s^2}{2\sigma^2}\right)} }{ 2 \pi }
|
||||||
|
+
|
||||||
|
\sqrt{\frac{1}{2\pi}}
|
||||||
|
\frac{s}{\sigma}
|
||||||
|
e^{-\left( \frac{s^2}{2\sigma^2}\sin^2{\pTrue} \right)}
|
||||||
|
\frac{\left(
|
||||||
|
1 + \erf{ \frac{s \cos{\pTrue}}{\sqrt{2} \sigma }}
|
||||||
|
\right)}{2}
|
||||||
|
\cos{\pTrue}
|
||||||
|
\end{equation*}
|
||||||
|
|
||||||
|
\tiny{Random Phasor Sum: ``Statistical Optics'', J. Goodman}
|
||||||
|
\end{column}
|
||||||
|
\end{columns}
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
|
||||||
|
\begin{frame}{Simulation: Phase: Baseline}
|
||||||
|
\begin{block}{Correction to previous talk: modifies global phase only}
|
||||||
|
@Baseline $i,j$: $\Delta \varphi_{ij} = \varphi(\sigma_i) - \varphi(\sigma_j)$ \\
|
||||||
|
|
||||||
|
Minimise matrix:
|
||||||
|
\tiny$\left(\begin{matrix}
|
||||||
|
\Delta_{11} & \Delta_{12} & \Delta_{13} & \\
|
||||||
|
\Delta_{21} & \Delta_{22} & \Delta_{23} & \\
|
||||||
|
\Delta_{31} & \Delta_{32} & \Delta_{33} & \\
|
||||||
|
\end{matrix}\right)$
|
||||||
|
\end{block}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics<1>[width=0.8\textwidth]{ZH_simulation/bc_baseline_phase_deltas.py.residuals.c5_b_N4096_noise1e3.pdf}
|
||||||
|
\end{figure}
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
\begin{frame}{Simulation: Period $k_i$}
|
||||||
|
\small{
|
||||||
|
Interferometry while allowing to shift by $T = 1/f_\mathrm{beacon}$
|
||||||
|
\\
|
||||||
|
Iterative process: \\
|
||||||
|
\; Scan positions finding the best $\{k_i\}$ set, then zoom in on strongest.
|
||||||
|
}
|
||||||
|
|
||||||
|
\only<1-4>{\begin{figure}
|
||||||
|
\includegraphics<1>[width=0.8\textwidth]{ZH_simulation/findks/ca_period_from_shower.py.run0.i5.loc8.0-2795.4-7816.0.pdf}
|
||||||
|
\includegraphics<2>[width=0.8\textwidth]{ZH_simulation/findks/ca_period_from_shower.py.run0.i99.loc8.0-2795.4-7816.0.pdf}
|
||||||
|
\includegraphics<3>[width=0.8\textwidth]{ZH_simulation/findks/ca_period_from_shower.py.maxima.run0.pdf}
|
||||||
|
\includegraphics<4>[width=0.8\textwidth]{ZH_simulation/findks/ca_period_from_shower.py.reconstruction.run0.power.pdf}
|
||||||
|
\end{figure}}
|
||||||
|
\only<5>{\begin{figure}
|
||||||
|
\includegraphics[width=0.45\textwidth]{ZH_simulation/findks/ca_period_from_shower.py.maxima.run0.pdf}
|
||||||
|
\hfill
|
||||||
|
\includegraphics[width=0.45\textwidth]{ZH_simulation/findks/ca_period_from_shower.py.reconstruction.run0.power.pdf}
|
||||||
|
\vspace{0.5cm}
|
||||||
|
\includegraphics[width=0.45\textwidth]{ZH_simulation/findks/ca_period_from_shower.py.maxima.run1.pdf}
|
||||||
|
\hfill
|
||||||
|
\includegraphics[width=0.45\textwidth]{ZH_simulation/findks/ca_period_from_shower.py.reconstruction.run1.power.pdf}
|
||||||
|
\end{figure}}
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
\begin{frame}{Simulation: Effects of Corrections}
|
||||||
|
Found both phase and period differences
|
||||||
|
\visible<2->{\begin{figure}
|
||||||
|
\includegraphics[width=0.45\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X400.repair_none.scale4d.pdf}
|
||||||
|
\hfill
|
||||||
|
\includegraphics[width=0.45\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X400.repair_phases.scale4d.pdf}
|
||||||
|
\vspace{0.5cm}
|
||||||
|
\includegraphics[width=0.45\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X400.repair_all.scale4d.pdf}
|
||||||
|
\hfill
|
||||||
|
\includegraphics[width=0.45\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X400.no_offset.scale4d.pdf}
|
||||||
|
\end{figure}}
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
\begin{frame}{Simulation Conclusions}
|
||||||
|
\begin{columns}
|
||||||
|
\begin{column}{0.5\textwidth}
|
||||||
|
\begin{itemize}
|
||||||
|
\item (Single) Sine beacon:\\
|
||||||
|
$\sigma < 1\mathrm{ns}$ from $\mathrm{SNR} > 3$\\
|
||||||
|
depends on beacon period.
|
||||||
|
\vspace{1cm}
|
||||||
|
\item Pulsed beacon:\\
|
||||||
|
(small) ongoing work\\
|
||||||
|
while writing thesis.
|
||||||
|
\end{itemize}
|
||||||
|
\end{column}
|
||||||
|
\begin{column}{0.5\textwidth}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics[width=1.1\textwidth]{beacon/time_res_vs_snr.pdf}
|
||||||
|
\end{figure}
|
||||||
|
\end{column}
|
||||||
|
\end{columns}
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
\begin{frame}{Simulation: Effects of Corrections (fullsize)}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics<+>[width=\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X400.repair_none.scale4d.pdf}
|
||||||
|
\includegraphics<+>[width=\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X400.repair_phases.scale4d.pdf}
|
||||||
|
\includegraphics<+>[width=\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X400.repair_all.scale4d.pdf}
|
||||||
|
\includegraphics<+>[width=\textwidth]{radio_interferometry/dc_grid_power_time_fixes.py.X400.no_offset.scale4d.pdf}
|
||||||
|
\end{figure}
|
||||||
|
\end{frame}
|
||||||
|
|
||||||
|
\begin{frame}{Signal to Noise definition}
|
||||||
|
\begin{figure}
|
||||||
|
\includegraphics[width=\textwidth]{ZH_simulation/signal_to_noise_definition.pdf}
|
||||||
|
\end{figure}
|
||||||
|
\end{frame}
|
||||||
|
\end{document}
|
24
presentations/2023-04-13_group_meeting/Makefile
Normal file
24
presentations/2023-04-13_group_meeting/Makefile
Normal file
|
@ -0,0 +1,24 @@
|
||||||
|
# vim:ft=make
|
||||||
|
-include config.mk
|
||||||
|
|
||||||
|
.PHONY: all clean dist-clean
|
||||||
|
|
||||||
|
### Variables
|
||||||
|
MAIN_SRC ?= main.tex
|
||||||
|
TEXENGINE ?= latexmk --pdf
|
||||||
|
|
||||||
|
MAIN_TARGET = $(patsubst %.tex,%.pdf,$(MAIN_SRC))
|
||||||
|
|
||||||
|
### Targets
|
||||||
|
all: $(MAIN_TARGET)
|
||||||
|
|
||||||
|
dist: all clean
|
||||||
|
|
||||||
|
$(MAIN_TARGET): $(MAIN_SRC)
|
||||||
|
$(TEXENGINE) $^
|
||||||
|
|
||||||
|
dist-clean: clean
|
||||||
|
@rm -vf *.pdf *.eps *.dvi *.ps
|
||||||
|
|
||||||
|
clean:
|
||||||
|
@rm -vf *.dat *.log *.out *.aux *.nav *.snm *.toc *.vrb *~ *.fls *.fdb_latexmk *-blx.bib *.bbl *.blg *.run.xml
|
14
presentations/2023-04-13_group_meeting/README.md
Normal file
14
presentations/2023-04-13_group_meeting/README.md
Normal file
|
@ -0,0 +1,14 @@
|
||||||
|
# Short Presentation on current status (Beacon)
|
||||||
|
|
||||||
|
Mostly to show what I've been doing uptil now.
|
||||||
|
|
||||||
|
Recap Sine Beacon
|
||||||
|
DTFT
|
||||||
|
Deviation Minimisation was poorly explained (and doesn't work)
|
||||||
|
|
||||||
|
!! 150MHz in addition to 50MHz simulation
|
||||||
|
|
||||||
|
Maybe Pulsed beacon scheme if time allows
|
||||||
|
|
||||||
|
|
||||||
|
|
1
presentations/2023-04-13_group_meeting/config.mk
Normal file
1
presentations/2023-04-13_group_meeting/config.mk
Normal file
|
@ -0,0 +1 @@
|
||||||
|
MAIN_SRC=2023-04-13_CRHEP.tex
|
Loading…
Reference in a new issue