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Timestamp:
02/21/05 19:24:32 (20 years ago)
Author:
gaug
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  • trunk/MagicSoft/TDAS-Extractor/MonteCarlo.tex

    r6648 r6652  
    2222\item The low-gain pulse is not yet simulated with the correct pulse width, but instead the same pulse shape as the one of the
    2323high-gain channel has been used.
     24\item The low-gain pulse starts to saturate at already about 200 photo-electrons while in reality,
     25this limit lies at more than 500 photo-electrons for an inner pixel. This is due to the wider low-gain pulse in real conditions.
    2426\item The low-gain pulse is delayed by only 15 FADC slices in the Monte-Carlo simulations, while it arrives about 16.5 FADC slices
    2527after the high-gain pulse in real conditions.
    2628\item No switching noise due to the low-gain switch has been simulated.
    2729\item The intrinsic transit time spread of the photo-multipliers has not been simulated.
     30\item The pulses have been simulated in steps of 0.2\,ns before digitization. There is thus an artificial numerial time resolution
     31limit of $0.2\,\mathrm{ns}/\sqrt{12} \approx 0.06\,\mathrm{ns}$.
    2832\item The total dynamic range of the entire signal transmission chain was set to infinite, thus the detector has been simulated
    2933to be completely linear.
     
    268272where $\widehat{T}_{rec}$ is the reconstructed arrival time and $T_{sim}$ the simulated one.
    269273\par
    270 
    271 
    272 
    273 \begin{figure}[htp]%%[t!]
     274Generally, the time resolutions $\Delta T_{\mathrm{MC}}$ are about  a factor 1.5 better than those obtained
     275from the calibration (section~\ref{sec:cal:timeres}, figure~\ref{fig:time:dep}). This
     276 is understandable since the Monte-Carlo pulses are smaller and
     277further the intrinsic time spread of the photo-multiplier has not been simulated. Moreover, no time resolution offset was
     278simulated, thus the reconstructed time resolutions follow about a $1/\sqrt{N_{\mathrm{phe}}}$\,--\,behaviour over the whole low-gain range.
     279The spline extractors level off in contradiction to what has been found with the calibration pulses.
     280\par
     281In figure~\ref{fig:mc:TimeRes_SlidW}, one can see nicely the effect of the addition of noise to the reconstructed time
     282resolution: While without noise all sliding window extractors with a window size of at least 4~FADC slices show the same time
     283resolution, with added noise, the resolution degrades with larger extraction window sizes. This can be understood by the fact that
     284an extractor covers the whole pulse if integrating at least 4~FADC slices and each additional slice can only be affected by the noise.
     285
     286\begin{figure}[htp]
    274287\centering
    275288  \includegraphics[width=0.49\linewidth]{TimeAndChargePlots/TDAS_TimeRes_SlidW_NoNoise_HiGain.eps}
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