Changeset 6519


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Timestamp:
02/16/05 14:16:05 (20 years ago)
Author:
gaug
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  • trunk/MagicSoft/TDAS-Extractor/Calibration.tex

    r6517 r6519  
    116116\item The reconstructed mean number of photo-electrons lies 4.5 sigma outside
    117117the distribution of photo-electrons obtained with the inner or outer pixels in the camera, respectively.
    118 This criterium cuts out pixels channels with apparently deviating (hardware) behaviour compared to
     118This criterium cuts out channels with apparently deviating (hardware) behaviour compared to
    119119the rest of the camera readout\footnote{This criteria is not applied any more in the standard analysis,
    120 although here, we kept using it}.
     120although we kept using it here}.
    121121\item All pixels with reconstructed negative mean signal or with a
    122122mean numbers of photo-electrons smaller than one. Pixels with a negative pedestal RMS subtracted
     
    128128\end{enumerate}
    129129
    130 Moreover, the number of events are counted which have been reconstructed outside a 5 sigma region
     130Moreover, the number of events are counted which have been reconstructed outside a 5$\sigma$ region
    131131from the mean signal. These events are called ``outliers''. Figure~\ref{fig:outlier} shows a typical
    132 outlier obtained with the digital filter applied to a low-gain signal and figure~\ref{fig:unsuited:all}
     132outlier obtained with the digital filter applied on a low-gain signal, and figure~\ref{fig:unsuited:all}
    133133shows the average number of all excluded pixels and outliers obtained from all 19 calibration configurations.
    134134One can already see that the largest window sizes yield a high number of un-calibrated pixels, mostly
     
    162162and~\ref{fig:unsuited:23ledsblue} show the resulting numbers of un-calibrated pixels and events for
    163163different colours and intensities. Because there is a strong anti-correlation between the number of
    164 excluded channels and the number of outliers per event, we have chosen to show these numbers together.
     164excluded pixels and the number of outliers per event, we have chosen to show these numbers together.
    165165
    166166\par
     
    198198One can see that in general, big extraction windows raise the
    199199number of un-calibrated pixels and are thus less stable. Especially for the very low-intensity
    200 \textit{\bf 1Led\,UV}-pulse, the big extraction windows summing 8 or more slices, cannot calibrate more
    201 than 50\%
    202 of the inner pixels (fig.~\ref{fig:unsuited:1leduv}). This is an expected behavior since big windows
    203 add up more noise which in turn makes the search for the small signal more difficult.
     200\textit{\bf 1\,Led\,UV}-pulse, the big extraction windows -- summing 8 or more slices -- cannot calibrate more
     201than 50\% of the inner pixels (fig.~\ref{fig:unsuited:1leduv}).
     202This is an expected behavior since big windows
     203sum up more noise which in turn makes the search for the small signal more difficult.
    204204\par
    205205In general, one can also find that all ``sliding window''-algorithms (extractors \#17-32) discard
    206206less pixels than the corresponding ``fixed window''-ones (extractors \#1--16). The digital filter with
    207207the correct weights (extractors \#30-33) discards the least number of pixels and is also robust against
    208 slight modifications of its weights (extractors \#28--30). The robustness gets lost when the high-gain and
    209 low-gain weights are inverted (extractors \#31--39, see fig.~\ref{fig:unsuited:23ledsblue}).
     208slight modifications of its weights (extractors \#28--30).
    210209\par
    211210Also the ``spline'' algorithms on small 
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