Changeset 6538 for trunk/MagicSoft/TDAS-Extractor
- Timestamp:
- 02/16/05 17:11:21 (20 years ago)
- Location:
- trunk/MagicSoft/TDAS-Extractor
- Files:
-
- 3 edited
Legend:
- Unmodified
- Added
- Removed
-
trunk/MagicSoft/TDAS-Extractor/Algorithms.tex
r6495 r6538 883 883 \item SetWeightsFile(``calibration\_weights\_blue.dat''); 884 884 \item SetWeightsFile(``calibration\_weights4\_blue.dat''); 885 \item SetWeightsFile(``cosmic\_weights\_logain6.dat'');886 \item SetWeightsFile(``cosmic\_weights\_logain4.dat'');887 \item SetWeightsFile(``calibration\_weights\_UV\_logaintest.dat'');888 \item SetWeightsFile(``calibration\_weights4\_UV\_logaintest.dat'');889 \item SetWeightsFile(``calibration\_weights\_blue\_logaintest.dat'');890 \item SetWeightsFile(``calibration\_weights4\_blue\_logaintest.dat'');891 885 \suspend{enumerate} 892 886 \item[MExtractTimeAndChargeDigitalFilterPeakSearch]: with the following initialization: … … 902 896 \end{description} 903 897 904 Note that the extractors \#34 through \#39 are used only to test the stability of the extraction against905 changes in the pulse-shape.906 907 898 References: \cite{OF77,OF94}. 908 899 -
trunk/MagicSoft/TDAS-Extractor/Calibration.tex
r6534 r6538 459 459 Figure~\ref{fig:linear:phevscharge23} shows the conversion factors using the amplitude-extracting spline 460 460 (extractor \#23). 461 Here, the linearity is worse than in the previous samples. A very clear difference between high-gain and461 Here, the linearity worse than in the previous sample. A very clear difference between high-gain and 462 462 low-gain regions can be seen as well as a bigger general spread in conversion factors. In order to investigate 463 463 if there is a common, systematic effect of the extractor, we show the averaged conversion factors over all 464 inner and outer pixels in figure~\ref{fig:linear:phevschargearea23}. Both characteristics are maintained ,464 inner and outer pixels in figure~\ref{fig:linear:phevschargearea23}. Both characteristics are maintained 465 465 there. Although the differences between high-gain and low-gain can be easily corrected for, we conclude 466 466 that extractor \#23 is still unstable against the linearity tests. … … 488 488 in conversion factors is smaller. 489 489 Figure~\ref{fig:linear:phevschargearea24} shows already rather good stability except for the two 490 lowest intensity pulses in green and blue. We conclude that extractor \#24 is still not toostable, but490 lowest intensity pulses in green and blue. We conclude that extractor \#24 is still un-stable, but 491 491 preferable to amplitude extractor. 492 492 \par … … 509 509 \end{figure} 510 510 511 Looking at figure~\ref{fig:linear:phevscharge25}, one can see that raising the integration window by511 Looking at figure~\ref{fig:linear:phevscharge25}, one can see that raising the integration window 512 512 to two effective FADC slices in the high-gain and three effective FADC slices in the low-gain 513 (extractor \#25), the stability is completely resumed, except for that 514 there seems to be a small systematic increase of the conversion factor in the low-gain range. This effect 515 is not significant in figure~\ref{fig:linear:phevschargearea25}, however it can be seen in five out of the 516 six tested channels of figure~\ref{fig:linear:phevscharge25}. We conclude that extractor \#25 is 517 almost as stable as the fixed window extractors. 513 (extractor \#25), the stability is completely resumed, except for 514 a small systematic increase of the conversion factor in the low-gain range. This effect 515 is not very significant, however it can be seen in five out of the 516 six tested channels. We conclude that extractor \#25 is almost as stable as the fixed window extractors. 518 517 \par 519 518 … … 535 534 \end{figure} 536 535 537 Figure~\ref{fig:linear:phevscharge30} showsthe conversion factors using a digital filter,538 applied on 6 FADC slices with weights calculated from the UV-calibration pulse.539 One can see that many blue and greencalibration pulses at low and intermediate intensity fall540 out of the linear region, moreover there is a lso a systematic offset betweenhigh-gain and low-gain region.541 It seems that the digital filter does not pass this test if the pulse form changes slightlyfrom the536 Figure~\ref{fig:linear:phevscharge30} and~\ref{fig:linear:phevscharge31} show the conversion factors using a digital filter, 537 applied on 6 FADC slices and respectively 4 FADC slices with weights calculated from the UV-calibration pulse. 538 One can see that one or two blue calibration pulses at low and intermediate intensity fall 539 out of the linear region, moreover there is a small systematic offset between the high-gain and low-gain region. 540 It seems that the digital filter does not pass this test if the pulse form changes for more than 2\,ns from the 542 541 expected one. The effect is not as problematic as it may appear here, because the actual calibration 543 542 will not calculate the number of photo-electrons (with the F-Factor method) for every signal intensity. -
trunk/MagicSoft/TDAS-Extractor/Results.tex
r6533 r6538 46 46 \hline 47 47 23 & Spline Amplitude & \ok & \no & \no & \ok & \ok & \ok & \no & \no & \ok \\ 48 24 & Splne Int. (1,1.5) & \ok & \ok & \ok & \ok & \ok & \best & \ok & \ ok& \no \\48 24 & Splne Int. (1,1.5) & \ok & \ok & \ok & \ok & \ok & \best & \ok & \no & \no \\ 49 49 25 & Spline Int. (2,3) & \ok &\ok & \best&\ok & \ok & \best & \ok & \ok & \no \\ 50 50 26 & Spline Int. (4,6) & \ok &\ok & \ok & \ok & \ok & \best & \ok & \ok & \no \\ 51 51 27 & Spline Int. (6,9) & \no &\best& \ok & \ok & \ok & \best & \ok & \ok & \no \\ 52 52 \hline 53 28 & Dig. Filt. (6,6) & \ok &\ok & & \ok & \ok & \ok & \ok & \ok & \ok \\ 54 29 & Dig. Filt. (4,4) & \best &\ok & & \ok & \ok & \best& \ok & \ok & \ok \\ 55 30 & Dig. Filt. Pk S. (4,6) & & & & & & & & & \ok \\ 53 28 & Dig. Filt. (6,6) & \ok &\ok & \ok & \ok & \ok & \ok & \ok & \ok & \ok \\ 54 29 & Dig. Filt. (4,4) & \best &\ok & \ok & \ok & \ok & \best& \ok & \ok & \ok \\ 56 55 \hline 57 56 \hline
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