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\documentclass [../thesis.tex] { subfiles}
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\begin { document}
\chapter { Conclusion}
\label { sec:conclusion}
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%<<<
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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.
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% 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.
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For analysis using radio interferometry to be competitive, this timing accuracy needs to be improved towards the $ 1 \ns $ mark.
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%>>>
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% Beacon introduction %<<<
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A viable method to obtain this timing accuracy is to incorporate a beacon transmitter into the array.
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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 $ .
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Thus, at a relatively low cost, the (relative) timing of radio arrays can be improved to enable radio interferometry.
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%>>>
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% Passive Beacon %<<<
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In some circumstances, an external transmitter can be used as a beacon.
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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 $ .
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% >>>
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% Combined sine beacon + air shower %<<<
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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.
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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.
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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.
% >>>
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\end { document}