m-thesis-documentation/documents/thesis/chapters/conclusion.tex

50 lines
2.5 KiB
TeX
Raw Normal View History

2023-10-31 15:19:29 +01:00
% vim: fdm=marker fmr=<<<,>>>
2022-08-24 17:24:49 +02:00
\documentclass[../thesis.tex]{subfiles}
\graphicspath{
{.}
{../../figures/}
{../../../figures/}
}
2022-07-12 04:20:00 +02:00
\begin{document}
\chapter{Conclusion}
\label{sec:conclusion}
2023-10-31 15:19:29 +01:00
%<<<
2023-10-19 18:25:07 +02:00
Using radio antennas to detect \glspl{UHECR} has received much attention recently.
The \acrlong{Auger} is currently being upgraded to \gls{AugerPrime} incorporating radio detectors with scintillators and water-cherenkov detectors.
Other experiments, such as \gls{GRAND}, plan\Todo{word} to fully rely on radio detection only.
\\
% Timing not enough
Time information in such large observatories is typically distributed using \glspl{GNSS}, reaching up to $10\ns$ accuracy under very good conditions.
2023-10-31 15:19:29 +01:00
For analysis using radio interferometry to be competitive, this timing accuracy needs to be improved towards the $1\ns$ mark.
2023-10-19 18:25:07 +02:00
\\
2023-10-31 15:19:29 +01:00
%>>>
2023-10-19 18:25:07 +02:00
2023-10-31 15:19:29 +01:00
% Beacon introduction %<<<
2023-10-19 18:25:07 +02:00
A viable method to obtain this timing accuracy is to incorporate a beacon transmitter into the array.
2023-10-31 15:19:29 +01:00
This (narrow-band) transmitter sends out a special signal that is picked up by the radio antennas in the array.
With relatively simple techniques, the timing accuracy can be improved to below $1\ns$.
2023-10-19 18:25:07 +02:00
Thus, at a relatively low cost, the (relative) timing of radio arrays can be improved to enable radio interferometry.
\\
2023-10-31 15:19:29 +01:00
%>>>
2023-10-19 18:25:07 +02:00
2023-10-31 15:19:29 +01:00
% Passive Beacon %<<<
2023-10-19 18:25:07 +02:00
In some circumstances, an external transmitter can be used as a beacon.
2023-10-31 15:19:29 +01:00
For example, in \gls{Auger}, a public TV broadcaster emits its signal at $f = 62.75\MHz$.
With the source location and the frequency known, time delays can be calculated and this signal can be used to account for timing errors smaller than $T = 1/f \sim 16\ns$.
Unfortunately, with the \gls{GNSS} timing accuracy estimated in the same order of magnitude and the signal being periodic, the synchronisation of the antennas can be off by an integer amount of periods $T$.
2023-10-19 18:25:07 +02:00
\\
2023-10-31 15:19:29 +01:00
% >>>
2023-10-19 18:25:07 +02:00
2023-10-31 15:19:29 +01:00
% Combined sine beacon + air shower %<<<
2023-10-19 18:25:07 +02:00
Recording an air shower, in addition to such a narrow-band beacon, might provide a method to determine the correct beacon period.
Radio interferometeric analysis of the air shower depends on the coherence of the received signals.
2023-10-31 15:19:29 +01:00
Any synchronicity problems in the radio antennas decrease the coherence and thus the power mapping used to derive properties of the air shower.
With a limited set of periods to test, this power can be maximised while simultaneously inferring the correct beacon period.
2023-10-19 18:25:07 +02:00
\\
2023-10-31 15:19:29 +01:00
The developed method to synchronise can be directly tested at \gls{Auger}, both with data from \gls{AERA} and the upcoming radio detectors from AugerPrime.
% >>>
2022-07-12 04:20:00 +02:00
\end{document}