mirror of
https://gitlab.science.ru.nl/mthesis-edeboone/m.internship-documentation.git
synced 2024-11-22 07:03:30 +01:00
Thesis: change sectioning Single Sine
This commit is contained in:
parent
cc1657e893
commit
06d49890ed
1 changed files with 5 additions and 4 deletions
|
@ -116,9 +116,10 @@ Of course, a limit on the number of periods is required to prevent over-optimisa
|
||||||
In general, they can be constrained using estimates of the accuracy of other timing mechanisms (see below).
|
In general, they can be constrained using estimates of the accuracy of other timing mechanisms (see below).
|
||||||
\\
|
\\
|
||||||
With a restricted set of allowed period shifts, we can alternate optimising the calibration signal's origin and optimising the set of period time delays of the array.
|
With a restricted set of allowed period shifts, we can alternate optimising the calibration signal's origin and optimising the set of period time delays of the array.
|
||||||
|
\\
|
||||||
% >>>
|
% >>>
|
||||||
|
|
||||||
\section{Lifting the Period Degeneracy with an Air Shower}% <<<
|
%\section{Lifting the Period Degeneracy with an Air Shower}% <<<
|
||||||
% <<<<
|
% <<<<
|
||||||
% Airshower gives t0
|
% Airshower gives t0
|
||||||
In the case of radio detection of air showers, the very signal of the air shower itself can be used as the calibration signal.
|
In the case of radio detection of air showers, the very signal of the air shower itself can be used as the calibration signal.
|
||||||
|
@ -128,7 +129,7 @@ The best period defects must thus be recovered from a single event.
|
||||||
When doing the interferometric analysis for a sine beacon synchronised array, waveforms can only be delayed by an integer amount of periods, thereby giving discrete solutions to maximising the interferometric signal.
|
When doing the interferometric analysis for a sine beacon synchronised array, waveforms can only be delayed by an integer amount of periods, thereby giving discrete solutions to maximising the interferometric signal.
|
||||||
\Todo{add size of shower at plane vs period defects in meters}
|
\Todo{add size of shower at plane vs period defects in meters}
|
||||||
|
|
||||||
\subsection{Air Shower simulation}
|
\section{Air Shower simulation}
|
||||||
% simulation of proton E15 on 10x10 antenna
|
% simulation of proton E15 on 10x10 antenna
|
||||||
To test the idea of combining a single sine beacon with an air shower, we simulated a set of recordings of a single air shower that also contains a beacon signal.
|
To test the idea of combining a single sine beacon with an air shower, we simulated a set of recordings of a single air shower that also contains a beacon signal.
|
||||||
\footnote{\url{https://gitlab.science.ru.nl/mthesis-edeboone/m-thesis-introduction/-/tree/main/airshower_beacon_simulation}}
|
\footnote{\url{https://gitlab.science.ru.nl/mthesis-edeboone/m-thesis-introduction/-/tree/main/airshower_beacon_simulation}}
|
||||||
|
@ -230,7 +231,7 @@ Shifting the waveforms to remove these small clocks defects, we are left with re
|
||||||
\end{figure}%>>>
|
\end{figure}%>>>
|
||||||
|
|
||||||
% >>>>
|
% >>>>
|
||||||
\subsection{\textit{k}-finding} % <<<
|
\section{\textit{k}-finding} % <<<
|
||||||
|
|
||||||
% unknown origin of air shower signal
|
% unknown origin of air shower signal
|
||||||
Up until now, the shower axis and thus the origin of the air shower signal have not been resolved.
|
Up until now, the shower axis and thus the origin of the air shower signal have not been resolved.
|
||||||
|
@ -331,7 +332,7 @@ Afterwards, a new grid zooms in on the power maximum and the process is repeated
|
||||||
|
|
||||||
\clearpage
|
\clearpage
|
||||||
%\phantomsection
|
%\phantomsection
|
||||||
\subsection{Strategy / Result} %<<<
|
\section{Strategy / Result} %<<<
|
||||||
|
|
||||||
Figure~\ref{fig:grid_power_time_fixes} shows the effect of the various synchronisation stages on both the alignment of the air shower waveforms, and the interferometric power measurement near the true shower axis.
|
Figure~\ref{fig:grid_power_time_fixes} shows the effect of the various synchronisation stages on both the alignment of the air shower waveforms, and the interferometric power measurement near the true shower axis.
|
||||||
Phase synchronising the antennas gives a small increase in observed power, while further aligning the periods after the optimisation process significantly enhances this power.
|
Phase synchronising the antennas gives a small increase in observed power, while further aligning the periods after the optimisation process significantly enhances this power.
|
||||||
|
|
Loading…
Reference in a new issue