Changeset 6419 for trunk/MagicSoft
- Timestamp:
- 02/12/05 20:03:05 (20 years ago)
- Location:
- trunk/MagicSoft/TDAS-Extractor
- Files:
-
- 6 edited
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Calibration.tex (modified) (2 diffs)
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Changelog (modified) (1 diff)
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PheVsCharge-14.eps (modified) (1 diff)
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PheVsCharge-20.eps (modified) (1 diff)
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PheVsCharge-25.eps (modified) (1 diff)
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PheVsCharge-30.eps (modified) (5 diffs)
Legend:
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trunk/MagicSoft/TDAS-Extractor/Calibration.tex
r6417 r6419 382 382 \par 383 383 384 \subsection{Linearity Tests} 385 386 In this section, we test the lineary of the extractors. As the photo-multiplier and the subsequent 384 %%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%%% 385 386 \subsection{Linearity \label{sec:calibration:linearity}} 387 388 \begin{figure}[htp] 389 \centering 390 \includegraphics[width=0.75\linewidth]{PheVsCharge-3.eps} 391 \caption{Conversion factor $c_{phe}$ for two exemplary inner pixels (upper plots) 392 and two exemplary outer ones (lower plots) obtained with the extractor 393 {\textit{MExtractFixedWindow}} on a window size of 6 high-gain and 6 low-gain slices 394 (extractor \#3). } 395 \label{fig:linear:phevscharge3} 396 \end{figure} 397 398 In this section, we test the lineary of the conversion factors FADC counts to photo-electrons: 399 400 \begin{equation} 401 c_{phe} =\ <Phe> / <\widehat{S}> 402 \end{equation} 403 404 As the photo-multiplier and the subsequent 387 405 optical transmission devices~\cite{david} is a linear device over a 388 406 wide dynamic range, the number of photo-electrons per charge has to remain constant over the tested … … 395 413 separate TDAS~\cite{tdas-calibration}. 396 414 397 398 \begin{figure}[htp] 399 \centering 400 \includegraphics[width=0.95\linewidth]{PheVsCharge-3.eps} 401 \caption{Example of a the development of the conversion factor FADC counts to photo-electrons for two 402 exemplary inner pixels (upper plots) and two exemplary outer ones (lower plots). 403 A fixed window extractor on a window size of 6 high-gain and 6 low-gain slices has been used (extractor \#3). } 404 \label{fig:linear:phevscharge3} 405 \end{figure} 406 407 \begin{figure}[htp] 408 \centering 409 \includegraphics[width=0.95\linewidth]{PheVsCharge-8.eps} 410 \caption{Example of a the development of the conversion factor FADC counts to photo-electrons for two 411 exemplary inner pixels (upper plots) and two exemplary outer ones (lower plots). 412 A fixed window spline extractor on a window size of 6 high-gain and 6 low-gain slices has been used 413 (extractor \#8). } 415 \par 416 Figure~\ref{fig:linear:phevscharge3} shows the conversion factor $c_{phe}$ 417 obtained for different light intensities 418 and colours for two exemplary inner and two exemplary outer pixels using a fixed window on 419 6 FADC slices. One can clearly see the difference 420 between the high-gain ($<$100\ phes) and the low-gain ($>$100\ phes) region and 421 a rather good stability of $c_{phe}$ for each region separately, except for the highest intensities 422 ($>$400\ phes). We conclude 423 that the fixed window extractor \#3 is a linear extractor for both high-gain and low-gain regions, 424 separately below a signal of about 300 photo-elecrons. 425 \par 426 427 \begin{figure}[htp] 428 \centering 429 \includegraphics[width=0.75\linewidth]{PheVsCharge-8.eps} 430 \caption{Conversion factor $c_{phe}$ for two exemplary inner pixels (upper plots) 431 and two exemplary outer ones (lower plots) obtained with the extractor 432 {\textit{MExtractFixedWindowSpline}} 433 on a window size of 6 high-gain and 6 low-gain slices (extractor \#8). } 414 434 \label{fig:linear:phevscharge8} 415 435 \end{figure} 416 436 417 \begin{figure}[htp] 418 \centering 419 \includegraphics[width=0.95\linewidth]{PheVsCharge-14.eps} 420 \caption{Example of a the development of the conversion factor FADC counts to photo-electrons for two 421 exemplary inner pixels (upper plots) and two exemplary outer ones (lower plots). 422 A fixed window peak search extractor on a window size of 6 high-gain and 6 low-gain slices has been used 437 Figure~\ref{fig:linear:phevscharge8} shows the conversion factors using an integrated spline over 438 a fixed window of 7 FADC slices. There is a rather stability in 439 the high-gain region ($<$100\ phes), but the low-gain region fluctuates a lot, especially for the two 440 outer pixels. We conclude that the fixed window spline extractor has a bad linearity 441 and is not robust in the low-gain extraction. 442 \par 443 444 \begin{figure}[htp] 445 \centering 446 \includegraphics[width=0.75\linewidth]{PheVsCharge-14.eps} 447 \caption{Conversion factor $c_{phe}$ for two exemplary inner pixels (upper plots) 448 and two exemplary outer ones (lower plots) obtained with the extractor 449 {\textit{MExtractFixedWindowPeakSearch}} on a window size of 6 high-gain and 6 low-gain slices 423 450 (extractor \#14). } 424 451 \label{fig:linear:phevscharge14} 425 452 \end{figure} 426 453 427 \begin{figure}[htp] 428 \centering 429 \includegraphics[width=0.95\linewidth]{PheVsCharge-20.eps} 454 Figure~\ref{fig:linear:phevscharge14} shows the conversion factors using a fixed window obtained with 455 a global peak search over the camera. A similiar result the fixed window is obtained where there is 456 stability up to about 300 photo-electrons. We conclude 457 that the fixed window peak search extractor \#14 is linear for both high-gain and low-gain regions, 458 separately, below a signal of about 300 photo-elecrons. 459 \par 460 461 462 \begin{figure}[htp] 463 \centering 464 \includegraphics[width=0.75\linewidth]{PheVsCharge-20.eps} 430 465 \caption{Example of a the development of the conversion factor FADC counts to photo-electrons for two 431 exemplary inner pixels (upper plots) and two exemplary outer ones (lower plots) .432 A sliding window extractor on a window size of 6 high-gain and 6 low-gain slices has been used 433 (extractor \#20). }466 exemplary inner pixels (upper plots) and two exemplary outer ones (lower plots) obtained with the extractor 467 {\textit{MExtractTimeAndChargeSlidingWindow}} 468 on a window size of 6 high-gain and 6 low-gain slices (extractor \#20). } 434 469 \label{fig:linear:phevscharge20} 435 470 \end{figure} 436 471 437 \begin{figure}[htp] 438 \centering 439 \includegraphics[width=0.95\linewidth]{PheVsCharge-25.eps} 440 \caption{Example of a the development of the conversion factor FADC counts to photo-electrons for two 441 exemplary inner pixels (upper plots) and two exemplary outer ones (lower plots). 442 An integrating spline extractor on a sliding window and a window size of 2 high-gain and 3 low-gain slices 443 has been used (extractor \#25). } 472 Figure~\ref{fig:linear:phevscharge20} shows the conversion factors using a sliding fixed window. 473 A much higher dynamic range is obtained mainting stability up to further than 500 photo-electrons. 474 \par 475 476 477 478 \begin{figure}[htp] 479 \centering 480 \includegraphics[width=0.75\linewidth]{PheVsCharge-25.eps} 481 \caption{Conversion factor $c_{phe}$ for two exemplary inner pixels (upper plots) 482 and two exemplary outer ones (lower plots) obtained with the extractor 483 {\textit{MExtractTimeAndChargeSpline}} with window size of 2 high-gain and 3 low-gain slices 484 (extractor \#25). } 444 485 \label{fig:linear:phevscharge25} 445 486 \end{figure} 446 487 447 \begin{figure}[htp] 448 \centering 449 \includegraphics[width=0.95\linewidth]{PheVsCharge-27.eps} 450 \caption{Example of a the development of the conversion factor FADC counts to photo-electrons for two 451 exemplary inner pixels (upper plots) and two exemplary outer ones (lower plots). 452 An integrating spline extractor on a sliding window and a window size of 6 high-gain and 7 low-gain slices 453 has been used (extractor \#27). } 454 \label{fig:linear:phevscharge27} 455 \end{figure} 456 457 \begin{figure}[htp] 458 \centering 459 \includegraphics[width=0.95\linewidth]{PheVsCharge-30.eps} 460 \caption{Example of a the development of the conversion factor FADC counts to photo-electrons for two 461 exemplary inner pixels (upper plots) and two exemplary outer ones (lower plots). 462 A digital filter extractor on a window size of 6 high-gain and 6 low-gain slices has been used 463 with UV-weights (extractor \#30). } 488 Figure~\ref{fig:linear:phevscharge25} shows the conversion factors using a sliding spline 489 extractor with an integration window of 2 FADC slices in the high-gain and 3 FADC slices in the 490 low-gain. The increase of integration window in the low-gain seems to lead to an systematic 491 increase in the conversion factor above 200 photo-electrons. If one uses this extractor, probably this 492 effect will have to be corrected for. 493 494 \par 495 496 \begin{figure}[htp] 497 \centering 498 \includegraphics[width=0.75\linewidth]{PheVsCharge-30.eps} 499 \caption{Conversion factor $c_{phe}$ for two exemplary inner pixels (upper plots) 500 and two exemplary outer ones (lower plots) obtained with the extractor 501 {\textit{MExtractTimeAndChargeDigitalFilter}} 502 using a window size of 6 high-gain and 6 low-gain slices with UV-weights (extractor \#30). } 464 503 \label{fig:linear:phevscharge30} 465 504 \end{figure} 466 505 467 \begin{figure}[htp] 468 \centering 469 \includegraphics[width=0.95\linewidth]{PheVsCharge-31.eps} 470 \caption{Example of a the development of the conversion factor FADC counts to photo-electrons for two 471 exemplary inner pixels (upper plots) and two exemplary outer ones (lower plots). 472 A digital filter extractor on a window size of 4 high-gain and 4 low-gain slices has been used 473 (extractor \#31). } 506 Figure~\ref{fig:linear:phevscharge30} shows the conversion factors using a digital filter applied on 6 FADC slices with weights calculated from 507 the UV-calibration pulse. 508 One can see that all calibration blue and green calibration pulses at low and intermediate intensity fall 509 out of the linear region, moreover there seems to be 510 a systematic offset between high-gain and low-gain. These offsets have to corrected for in any way, however the loss of stability against the 511 exact pulse form in the high-gain is more problematic. 512 513 \par 514 515 \begin{figure}[htp] 516 \centering 517 \includegraphics[width=0.75\linewidth]{PheVsCharge-31.eps} 518 \caption{Conversion factor $c_{phe}$ for two exemplary inner pixels (upper plots) 519 and two exemplary outer ones (lower plots) obtained with the extractor 520 {\textit{MExtractTimeAndChargeDigitalFilter}} using a window size of 521 4 high-gain and 4 low-gain slices (extractor \#31). } 474 522 \label{fig:linear:phevscharge31} 475 523 \end{figure} -
trunk/MagicSoft/TDAS-Extractor/Changelog
r6374 r6419 22 22 2004/02/10: Markus Gaug 23 23 * Pedetal.tex: Updated figures and text 24 * Calibration.tex: moved text from Performance.tex into this file and 25 updated figures and text 24 26 25 27 2004/02/03: Markus Gaug -
trunk/MagicSoft/TDAS-Extractor/PheVsCharge-14.eps
r5908 r6419 3 3 %%Title: ./linearplots/PheVsCharge-14.eps: Conversion Factor vs. Charges 4 4 %%Creator: ROOT Version 3.10/02 5 %%CreationDate: Tue Jan 18 18:09:3820055 %%CreationDate: Sat Feb 12 12:38:40 2005 6 6 %%EndComments 7 7 %%BeginProlog -
trunk/MagicSoft/TDAS-Extractor/PheVsCharge-20.eps
r5908 r6419 3 3 %%Title: ./linearplots/PheVsCharge-20.eps: Conversion Factor vs. Charges 4 4 %%Creator: ROOT Version 3.10/02 5 %%CreationDate: Tue Jan 18 18:09:5120055 %%CreationDate: Sat Feb 12 12:39:07 2005 6 6 %%EndComments 7 7 %%BeginProlog -
trunk/MagicSoft/TDAS-Extractor/PheVsCharge-25.eps
r5908 r6419 3 3 %%Title: ./linearplots/PheVsCharge-25.eps: Conversion Factor vs. Charges 4 4 %%Creator: ROOT Version 3.10/02 5 %%CreationDate: Tue Jan 18 18:10:0520055 %%CreationDate: Sat Feb 12 12:42:02 2005 6 6 %%EndComments 7 7 %%BeginProlog -
trunk/MagicSoft/TDAS-Extractor/PheVsCharge-30.eps
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