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Timestamp:
02/18/05 13:58:52 (20 years ago)
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gaug
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  • trunk/MagicSoft/TDAS-Extractor/Criteria.tex

    r6583 r6590  
    9494\subsection{Stability}
    9595
    96 The signal extraction algorithms has to stabelly reconstruct the charge for different types of pules with different intrinsic shapes and backgrounds:
     96The signal extraction algorithms has to reconstruct stably the charge for different types of pulses
     97with different intrinsic pulse shapes and backgrounds:
    9798
    9899\begin{itemize}
     
    102103\end{itemize}
    103104
    104 An important point is the difference between the pulse shapes of the calibration and Cherenkov signals. It has to be ensured that the calibration factor between the reconstructed charge in FADC counts and photo electrons for calibration events can be applied to Cherenkov signals.
     105An important point is the difference between the pulse shapes of the calibration and Cherenkov signals. It has to be ensured that the
     106computed calibration factor between the reconstructed charge in FADC counts and photo electrons for calibration events
     107is valid for signals from Cherenkov photons.
    105108
    106109
    107110\subsection{Applicability for Different Sampling Speeds / No Pulse Shaping.}
    108 The current read-out system of the MAGIC telescope \cite{Magic-DAQ} with 300 MSamples/s is relatively slow compared to the fast pulses of about 2 ns FWHM of Cherenkov pulses. To acquire the pulse shape an artificial pulse shaping to about 6.5 ns FWHM is used. Thereby also more LONS is integrated that acts as noise.
     111The current read-out system of the MAGIC telescope~\cite{Magic-DAQ} with 300~MSamples/s is relatively slow compared to the fast pulses of
     112about 2\,ns FWHM of Cherenkov pulses.
     113To acquire the pulse shape an artificial pulse shaping to about 6.5\,ns FWHM is used. Thereby also more night sky background light
     114is integrated which acts as noise.
    109115
    110116For 2 ns FWHM fast pulses a 2 GSamples/s FADC provides at least 4 sampling points. This permits a reasonable reconstruction of the pulse shape. First prototype tests with fast digitization systems for MAGIC have been successfully conducted \cite{GSamlesFADC}. The signals have been reconstructed within the common MAGIC Mars software framework.
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