Changeset 6652 for trunk/MagicSoft/TDAS-Extractor
- Timestamp:
- 02/21/05 19:24:32 (20 years ago)
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- 1 edited
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trunk/MagicSoft/TDAS-Extractor/MonteCarlo.tex
r6648 r6652 22 22 \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 23 23 high-gain channel has been used. 24 \item The low-gain pulse starts to saturate at already about 200 photo-electrons while in reality, 25 this limit lies at more than 500 photo-electrons for an inner pixel. This is due to the wider low-gain pulse in real conditions. 24 26 \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 25 27 after the high-gain pulse in real conditions. 26 28 \item No switching noise due to the low-gain switch has been simulated. 27 29 \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 31 limit of $0.2\,\mathrm{ns}/\sqrt{12} \approx 0.06\,\mathrm{ns}$. 28 32 \item The total dynamic range of the entire signal transmission chain was set to infinite, thus the detector has been simulated 29 33 to be completely linear. … … 268 272 where $\widehat{T}_{rec}$ is the reconstructed arrival time and $T_{sim}$ the simulated one. 269 273 \par 270 271 272 273 \begin{figure}[htp]%%[t!] 274 Generally, the time resolutions $\Delta T_{\mathrm{MC}}$ are about a factor 1.5 better than those obtained 275 from the calibration (section~\ref{sec:cal:timeres}, figure~\ref{fig:time:dep}). This 276 is understandable since the Monte-Carlo pulses are smaller and 277 further the intrinsic time spread of the photo-multiplier has not been simulated. Moreover, no time resolution offset was 278 simulated, thus the reconstructed time resolutions follow about a $1/\sqrt{N_{\mathrm{phe}}}$\,--\,behaviour over the whole low-gain range. 279 The spline extractors level off in contradiction to what has been found with the calibration pulses. 280 \par 281 In figure~\ref{fig:mc:TimeRes_SlidW}, one can see nicely the effect of the addition of noise to the reconstructed time 282 resolution: While without noise all sliding window extractors with a window size of at least 4~FADC slices show the same time 283 resolution, with added noise, the resolution degrades with larger extraction window sizes. This can be understood by the fact that 284 an 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] 274 287 \centering 275 288 \includegraphics[width=0.49\linewidth]{TimeAndChargePlots/TDAS_TimeRes_SlidW_NoNoise_HiGain.eps}
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