updated manual directory
git-svn-id: file:///afs/psi.ch/project/sls_det_software/svn/slsDetectorsPackage@47 08cae9ef-cb74-4d14-b03a-d7ea46f178d7
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manual/manual-calwiz/Advanced.png
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manual/manual-calwiz/Constant_step.png
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manual/manual-calwiz/GUI_Advanced.eps
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manual/manual-calwiz/GUI_ThresholdScan.eps
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manual/manual-calwiz/Makefile
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DESTDIR?=../
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#manual-api manual-calwiz manual-client manual-gui manual-main
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TEX=latex
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MAINTEXS= angularCalibrationHowTo.tex energyCalibrationHowTo.tex
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TEXS=ancCal.tex enCal.tex installation.tex
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DVIS = $(MAINTEXS:.tex=.dvi)
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PSS = $(MAINTEXS:.tex=.ps)
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PDFS = $(MAINTEXS:.tex=.pdf)
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HTMLS = $(MAINTEXS:%.tex=%)
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#destdir?!?!?
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all: $(PDFS) $(HTMLS)
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echo $(PWD)
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echo $(PDFS)
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echo $(HTMLS)
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pdf: $(PDFS)
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html: $(HTMLS)
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$(HTMLS): $(TEXS) $(MAINTEXS)
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latex $@.tex
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latex2html -split 4 $@.tex
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$(shell test -d $(DESTDIR)/html || mkdir -p $(DESTDIR)/html)
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mv $@ $(DESTDIR)/html
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%.dvi : %.tex $(TEXS)
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latex $<
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latex $<
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%.ps : %.dvi
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dvips -o $@ $<
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%.pdf : %.ps
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ps2pdf $< $@
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clean:
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rm -rf *.aux *.log *.toc *.out $(DVIS) $(PSS) $(PDFS) $(HTMLS)
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manual/manual-calwiz/addEnergy.eps
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manual/manual-calwiz/addEnergy.png
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manual/manual-calwiz/ancCal.tex
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In order to convert from strip number to 2$\theta$-angle, an accurate angular calibration of the detector must be performed (for details see the paper Bergamaschi, A. et al. (2010). J. Synchrotron Rad. 17, 653-668). \\
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For this purpose, a series of patterns of a powder standard with symmetric peaks (e.g. silicon) must acquired while shifting the detector by an angular step of the order of about 2\% of the module size. During the measurement, a strong intensity peak (e.g. Si(111)) should pass through the field of view of every module such that it can be used as a reference angular position to perform the calibration of the modules position.\\
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In a first step, the peak is fitted with a Gaussian in order to determine its position $C_{peak}$ in channel number for each of the acquired patterns.\\
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In a second step, for each module $i$, the encoder position $\Theta_e$ is fitted as a function of the peak position $C_{peak}$ according to:
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\begin{equation}\label{eq:angcal}
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\Theta_e=\Theta_o^i-\arctan\Big(\frac{p \cdot (C_{peak}-C_{center}^i)}{R^i}\Big),
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\end{equation}
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where the parameters $\Theta_o^i$ is the angular offset with respect to the diffractometer zero position, $C_{center}^{i}$ is the central channel and $R^i$ is the distance of the module $i$ from the diffractometer center while $p=50~\mu m$ is the strip pitch of the detector. \\
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Finally, the global offset of the detector system is precisely determined by refining a silicon pattern at a well-defined energy (i.e., knowing the position of the peak).
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The same function of equation~\ref{eq:angcal}, with the parameters obtained from the calibration, is used in order to convert from channel number to 2$\theta$-angle.
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The parallax at the borders of the modules due to the thickness of the silicon sensor is a function of the X-ray energy (higher energy X-rays are absorbed deeper inside the sensor) and is of the order of 0.2~mdeg at 12~keV and 0.5~mdeg at 30~keV. \\
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The differences in pixel size due to the different portion of solid angle covered by the strips on the border of the modules and the higher efficiency due to the longer path of the X-rays in the sensor are removed by the flat field correction. This also normalizes additional differences in pixel size between channels which are also present because of mismatches in the strip sensor fabrication and in fluctuations of the channels threshold level.
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Patterns acquired at different detector positions are generally merged together in order to fill the gaps between the modules and correct possibly bad functioning channels. In this procedure the data from different positions which are closer than 4~mdeg (the average pixel size) are averaged and the new position is set to the mean of the positions of the original points.
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The position and width of the peaks results from a fit over several detector channels. Geometrical distortions might disturb this determination mainly because of errors in the angular calibration, fluctuations in the encoder position, variations between channels and parallax effects.\\
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The resolution in locating the peak center and determining its width and integrated intensity has been estimated by acquiring several patterns of a LaB$_6$ sample in a 300~$\mu$m capillary with the detector shifted in 5~mdeg steps between 30.4 and 36.5 degrees. The 16~peaks acquired have been fitted with a Gaussian function plus background and the fluctuations on the fitted parameters have been calculated. The resulting average resolutions are 0.63$\pm$0.06~mdeg for the peak center and 0.22$\pm$0.05~mdeg for the peak Full-Width at Half-Maximum (FWHM) for an average peak FWHM of 27.0$\pm$2.5~mdeg. \\
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These results show that the angular calibration allows a resolution in determining the peaks position and width which is appropriate for structural determination.
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\section{Data acquisition}
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The angular calibration consists in acquiring a set of diffraction patterns of a well known powder standard (e.g. Silicon) at different encoder positions. In order to facilitate the procedure, the sample should not emit fluorescent light and should present relatively symmetric peaks. \\
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During the measurement, a strong intensity peak (e.g. Si(111)) should pass through the field of view of every module such that it can be used as a reference angular position to perform the calibration of the modules position. In general the highest peak will be used for the calibration, but this is not necessary in case there would be e.g. geometrical limitations for shifting the detector. \\ \textbf{Do not forget to properly position the beam stopper if the detector is scanned in front of the direct beam.}\\
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The detector should be shifted of an angular step of the order of about 2\% of the module size, such that about 50 patterns can contribute to the fitting of the 3 parameters necessary for the angular calibration.\\
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All the angular calibration procedure should be acquired using a trimmed detector with the threshold set at half of the X-ray energy (Assuming no fluorescent element in the standard). A flat field should also be acquired in order to precisely correct the data, while the X-ray intensity should be kept lower than about 100~kHz per strip in order to avoid the need for rate corrections.
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A rough angular conversion file starting from a previous calibration or from the geometric characteristics of the mechanics is an advantage. The angular conversion file should contain a line for each module of the detector with its module number $i$, center $C_{center}^{i}$ and error, conversion radius $p/R^i$ and error, offset $\Theta_o^i$ and error:
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\begin{verbatim}
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module 0 center 639.5 +- 0 conversion 6.56E-05 +- 0 offset 0 +- 0
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\end{verbatim}
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Also the \textit{global offset} value of the beamline should be approximately known i.e. the angular position of channel 0 of module 0 when the motor is set at 0. \\
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All the documentation assumes that the detector is oriented in the same direction as the encoder position i.e. large channel number at higher angles (both per module and absolute). If this is not the case, the \textit{angular direction} should be set to -1.
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\subsection{Software}
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For the acquisition ot the data you need to install the slsDetector software package (please refere to separate documentation). The use of the GUI is optional and all operations can be performed also using the text client.\\
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Please make sure that you have edited the \\
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\textit{slsDetectorSoftware/usersFunctions/angleFunction.h} \\
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in order to match the angular conversion for your geometry and \\
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\textit{slsDetectorSoftware/usersFunctions/usersFunctions.cpp} \\
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in order to be able to move the detector and read out its position by using the slsDetector software.
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In the following the command to acquire a dataset for the angular calibration with an exposure time of 1~s, and position shift
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\begin{verbatim}
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#setup angular calibration log mode
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> sls_detector_put angcallog 1
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#set exposure time to 1s
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> sls_detector_put exptime 1.
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#setup threshold scan
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> sls_detector_put scan0script position
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#setup the precision for the scan variable in the file name
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> sls_detector_put scan0prec 2
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#set scan range between 20deg and -60deg, step of -0.1deg
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# (at 12.4 keV the Si(111) peak is at approx 19deg
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> sls_detector_put scan0range 20 -60 -0.1
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#acquire the data
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> sls_detector_acquire
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#unset angular calibration log mode
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> sls_detector_put angcallog 0
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\end{verbatim}
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With the GUI you can obtain the same results by clicking on the \textit{Angular calibration} log button in the advanced tab (see figure~\ref{fig:guiangcallog}) and setting up the motor position scan in the Actions tab (see figure~\ref{fig:guiposscan}). The exposure time should also be set in the measurement tab.
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Additional to the data files, the acquisition will produce a .angcal file containing an header and, for each step of the acquisition, the exect value of the motor position and the file name. \\
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In case you forgot to enable the angcallog flag in the software, you can produce the file with the syntax as follows, assuming that you know the exact values of your encoder for each frame:
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\begin{verbatim}
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type Mythen
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maxmod 32
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nmod 32
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angconv /scratch/angcal20120422/ang.off
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globaloff 5.088
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fineoff 0.0
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angdir 1
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ffdir /scratch/angcal20120422/
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flatfield flatfield_E12keV_T6keV_0.raw
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badchannels /scratch/cal/bad.chans
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19.99998 angcal_S20.00_0
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19.90001 angcal_S19.90_0
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19.79999 angcal_S19.80_0
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19.70002 angcal_S19.70_0
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......
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\end{verbatim}
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\begin{figure}
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\caption{Acquisition GUI window to enable the angular calibration log.} \label{fig:guiangcallog}
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\includegraphics[width=\textwidth]{enable_angcal.eps}
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\end{figure}
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\begin{figure}
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\caption{Acquisition GUI window to setup the motor position scan.} \label{fig:guiposscan}
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\includegraphics[width=\textwidth]{position_scan.eps}
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\end{figure}
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\newpage
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\section{Data analysis}
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The data analysis consists in fitting with a gaussian the selected peak of the powder pattern for each position in order to determine its position is channel number as a function of the encoder position. \\
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In a second step, for each module, the channel vs. encoder curve is fitted in order to extrapolate the three parameters necessary for the angular conversion and the result is written to file
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\subsection{Software}
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The software used for the angular calibration data analysis is based on root (see http://root.cern.ch).\\
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This can be downloaded as binary or installed from sources. The version of the software should not play an important role, but up to now everything has been implemented and tested using version 5.20.
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To start the data analysis simply launch:
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\begin{verbatim}
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> ./angularCalibrationWizard
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\end{verbatim}
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\begin{figure}
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\caption{Overview of the nagular calibration dataset.} \label{fig:setangcal}
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\includegraphics[width=\textwidth]{setupAngcal.eps}
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\end{figure}
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To setup the angular calibration dataset, the .angcal file should be selected (or digited) and the load button should be pressed to confirm. The parameters of the angular calibration are then read to the file and the data loaded for a quick overview (see figure~\ref{fig:setangcal}).\\
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The software assumes that the data files (.raw) and the .encal file are in the same directory.\\
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A 2D color plot will show a rebinned overview of the dataset. The peak to be fitted should be visible as a high intensity diagonal line passing through all the channels.
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\begin{figure}
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\caption{Preview of the fitting of the Si(111) peak for one of the detector positions.} \label{fig:peakfit}
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\includegraphics[width=\textwidth]{peakFit.eps}
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\end{figure}
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For a more detailed view of the data, one can select an angular calibration step from the combo box, select the plot mode (raw data or processed data as a function of channel number, processed angular converted data, flat field data, or again an overview of the whole dataset). \\
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By (right) clicking close to the axis you are able to zoom in/out, set the scale to logarithmic etc.\\
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If the bad channel list, angular conversion file or flat field file are changed compared to the acquisition, they can be reloaded by editing the correspondent text entries and pressing enter.
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In particular, the angular converted data should be checked in order to view the position of the selected peak. In this case, the plot will be zoomed to the angular region slected in the minimum and maximum angle entries. By pressing fit, the fit of the peak in the selected angular range will be shown (see figure~\ref{fig:peakfit}). It is useful to check that it works properly in several positions such that then the sequential fitting on all steps can give good results.
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To automatically fit all positions simply press \textit{Proceed to Modules Calibration} and wait until all steps are fitted. This can take sometime, depending on the number of steps.
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\begin{figure}
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\caption{Window for fitting the angular calibration parameters of a module.} \label{fig:anglefit}
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\includegraphics[width=\textwidth]{angleFit.eps}
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\end{figure}
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In the module calibration window (see figure~\ref{fig:anglefit}), you will be able to fit the channel number to encoder position curve to estimate the three angular calibration parameters for each module.\\
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The entries show the angular calibration parameters used for approximate angular conversion in the previous step of the calibration. These can be edited and will be used as start parameters for the fit.
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By clicking on the check box next to the parameters, the selected parameter will be set and fixed during the fit. Often the center is used as a fix parameter.\\
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It is possible to navigate between modules by using the Previous and Next module buttons. To refit the current module (e.g. after changing one of the parameters) simply re-click on the module number.
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After fitting all modules you can click on the \textit{Write Angular Calibration} button, select the file name to write to and save the calibration angulat calibration data. Please note that the offset of module 0 will always be 0 and the other values will be rescaled to its value. Therefore the global offset of the steup will always need to be specified for a proper angular conversion unless the home of the encoder will not be redifined.
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\section{Setup calibration files}
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To use the generated angular calibration files, using the text client:
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\begin{verbatim}
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sls_detector_put angconv /scratch/ang_new.off
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\end{verbatim}
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while for the GUI the file name should be specified in the configuration file (works also for the text client).
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\end{document}
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manual/manual-calwiz/angleFit.eps
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manual/manual-calwiz/angleFit.png
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manual/manual-calwiz/angularCalibrationHowTo.tex
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\documentclass{article}
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\usepackage{amssymb}
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\usepackage[dvips]{graphicx}
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\usepackage{verbatim}
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\begin{document}
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\title{Angular calibration wizard manual}
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\author{Anna Bergamaschi}
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\date{\today}
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\maketitle
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\section{Introduction}
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\input{ancCal.tex}
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\end{document}
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manual/manual-calwiz/calibrateModule.eps
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manual/manual-calwiz/calibrateModule.png
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manual/manual-calwiz/calibrationWizardsHowTo.tex
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\documentclass{report}
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\usepackage{amssymb}
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\usepackage[dvips]{graphicx}
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\usepackage{verbatim}
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\begin{document}
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||||
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||||
\title{Calibration wizards manual}
|
||||
\author{Anna Bergamaschi}
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\date{\today}
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||||
\maketitle
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\chapter{Installation}
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\input{installation.tex}
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\chapter{Energy calibration}
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%\section{Introduction}
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\input{enCal.tex}
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||||
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\chapter{Angular calibration}
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%\section{Introduction}
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\input{ancCal.tex}
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\end{document}
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manual/manual-calwiz/enCal.tex
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The choice of the level of the comparator threshold plays a very important role in counting systems since it influences the efficiency of the detector as well as its spatial resolution (for details see the paper Bergamaschi, A. et al. (2010). J. Synchrotron Rad. 17, 653-668).
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||||
|
||||
|
||||
Single-photon-counting detectors are sensitive to single photons and the only limitation on the fluctuations of the number of counts is given by the Poisson-like statistics of the X-ray quanta.
|
||||
The digitized signal does not carry any information concerning the energy of the X-rays and all photons with an energy larger than the threshold are counted as one bit. This means that the choice of the correct comparator threshold level is critical in order to obtain good-quality data.\\
|
||||
Figure~\ref{fig:thrscanexpl} shows the expected number of counts as a function of the threshold energy for $N_0$ monochromatic X-rays of energy $E_0$. This is often denominated S-curve and can be interpreted as the integral of the signal spectrum between the threshold level and infinity.
|
||||
The dashed curve represents the behavior of an ideal counting system: nothing is counted for thresholds larger than the photon energy and all the $N_0$ X-rays are counted for thresholds lower than $E_0$.
|
||||
The thick solid line represents the physical curve which also takes into account the electronic noise and the charge sharing between channels.
|
||||
|
||||
The intrinsic noise on the electronic signal is defined by the Equivalent Noise Charge ($ENC$). The $ENC$ describes noise in terms of the charge at the detector input needed to create the same output at the end of the analog chain and is normally expressed in electrons. For silicon sensors, it can be converted into energy units by considering 1~$e^-$=3.6~eV.
|
||||
The value of the $ENC$ normally depends on the shaping settings of the analog chain and increases with shorter shaping times.
|
||||
The resulting electronic signal spectrum is then given by a convolution between the radiation spectrum and the noise i.e., a Gaussian of standard deviation $ENC$.
|
||||
The S-curve for a monochromatic radiation beam is well described by a Gaussian cumulative distribution $D$ with an additional increase at low threshold due to the baseline noise, as shown by the solid thin line.
|
||||
|
||||
Moreover, when a photon is absorbed in the region between two strips of the sensor, the generated charge is partially collected by the two nearest electronic channels. For this reason the physical S-curve is not flat but can be modeled by a decreasing straight line. The number of shared photons $N_S$ is given by the difference between the number of counts and the number of X-rays whose charge is completely collected by the strip (shown by the dotted line).
|
||||
|
||||
The number of counts in the physical case is equal to that in the ideal case for a threshold set at half the photon energy. This defines the optimal threshold level $E_t=E_0/2$.\\
|
||||
The detector response $N$ as a function of the threshold energy $E_t$ is given by the sum of the noise counts $N_n$ and the counts originating from photons $N_\gamma$:
|
||||
\begin{equation}
|
||||
N_\gamma(E_t)=\frac{N_0}{2}\cdot\Big(1+C_s \frac{E_0-2E_t}{E_0}\Big)D \Big(\frac{E_0-E_t}{ENC} \Big), \label{eq:thrscan}
|
||||
\end{equation}
|
||||
where $C_s$ is the fraction of photons which produce a charge cloud which is shared between neighboring strips ($N_s=C_s N_0$).\\
|
||||
By assuming a noise of Gaussian type, and considering its bandwidth limited by the shaping time $\tau_s$, the number of noise counts in the acquisition time $T$ can be approximated as:
|
||||
\begin{equation}
|
||||
N_n(E_t) \sim \frac{T}{\tau_s} D \Big(\frac{-E_t}{ENC} \Big). \label{eq:noisescan}
|
||||
\end{equation}
|
||||
|
||||
The choice of the comparator threshold level $E_t$ influences not only the counting efficiency and noise performances, but also the spatial resolution and the counting statistics of the detector.
|
||||
If the threshold is set at values higher than the ideal value $E_t=E_0/2$, a fraction of the photons absorbed in the sensor in the region between two strips is not counted thus reducing the detector efficiency but improving its spatial resolution (narrower strip size). On the other hand, if the threshold is set at values lower than $E_t$, part of the X-rays absorbed in the region between two strips are counted by both of them, resulting in a deterioration of the spatial resolution of the detector and of the fluctuations on the number of photons because of the increased multiplicity.
|
||||
|
||||
|
||||
Furthermore, the threshold uniformity is particularly critical with regards to fluorescent radiation emitted by the sample under investigation. Since the emission of fluorescent light is isotropic, the data quality will be improved by setting the threshold high enough in order to discard the fluorescence background (see figure~\ref{fig:thrscanfluo}). \\
|
||||
Moreover, setting the threshold too close to the energy of the fluorescent light gives rise to large fluctuations between channels in the number of counts since the threshold sits on the steepest part of the threshold scan curve for the fluorescent background. These differences cannot be corrected by using a flat-field normalization since the fluorescent component is not present in the reference image. For this reason, it is extremely important that the threshold uniformity over the whole detector is optimized. The threshold level must be set at least $\Sigma>3\,ENC$ away from both the fluorescent energy level and the X-ray energy in order to remove the fluorescence background while efficiently count the diffracted photons.
|
||||
|
||||
The comparator threshold is given by a global level which can be set on a module basis and adds to a component which is individually adjustable for each channel. In order to optimize the uniformity of the detector response it is important to properly adjust the threshold for all channels. \\
|
||||
Since both the signal amplification stages and the comparator are linear, it is necessary to calibrate the detector offset $O$ and gain $G$ in order to correctly set its comparator threshold $V_t$ at the desired energy $E_t$:
|
||||
\begin{equation}
|
||||
V_{t}=O+G \cdot E_t.\label{eq:encal}
|
||||
\end{equation}
|
||||
This is initially performed by acquiring measurements while scanning the global threshold using different X-ray energies and calculating the median of the counts at each threshold value for each module $i$. The curves obtained for one of the detector modules at three energies are shown in figure~\ref{fig:modulecalibration}. The experimental data are then fitted according to equation~\ref{eq:thrscan} and for each module a linear relation is found between the X-ray energy and the estimated inflection point, as shown in the inset of figure~\ref{fig:modulecalibration}. The resulting offset $O_i$ and gain $G_i$ are used as a conversion factor between the threshold level and the energy.
|
||||
|
||||
|
||||
\begin{figure}
|
||||
\caption{Expected counts as a function of a threshold energy for a monochromatic beam of energy $E_0$=12~keV. $N_0$=10000 is the number of photons absorbed by the detector during the acquisition time. The dashed line represents the curve in an ideal case without electronic noise and charge sharing, the solid thin line with noise $ENC$=1~keV but without charge sharing and the solid thick line is the physical case with noise and $CS=$22~\% charge sharing. $N_S$ is the number of photons whose charge is shared between neighbouring strips ($CS=\frac{N_S}{N_0}$). The dotted line represents the number of photons whose charge is completely collected by a single strip.}\label{fig:thrscanexpl}
|
||||
\includegraphics[width=\textwidth]{fig4.eps}
|
||||
\end{figure}
|
||||
|
||||
|
||||
|
||||
\begin{figure}
|
||||
\caption{Measured threshold scan at 12.5~keV with the three different settings. In the inset the fit of the experimental data with the expected curve as in function~\ref{eq:thrscan} is shown in the region of the inflection point.} \label{fig:expthrscan}
|
||||
\includegraphics[width=\textwidth]{fig5.eps}
|
||||
\end{figure}
|
||||
|
||||
\begin{figure}
|
||||
\caption{Number of counts as a function of the threshold measured from a sample containing iron ($E_f$=5.9~keV) when using X-rays of energy $E_0$=12~keV. In this case, setting the threshold at $E_0/2$, which is very close to $E_f$, would give $\Delta \sim$10\% counts from the fluorescense background. Therefore the threshold should be set at an intermediate level $E_t$ between the two energy components with a distance of at least $\Sigma>3ENC$ from both $E_f$ and $E_0$.}\label{fig:thrscanfluo}
|
||||
\includegraphics[width=\textwidth]{fig7.eps}
|
||||
\end{figure}
|
||||
Differences in gain and offset are present also between individual channels within a module and therefore the use of threshold equalization techniques (trimming) using the internal 6-bit DAC is needed in order to reduce the threshold dispersion.
|
||||
Since both gain and offset have variations between channels, the optimal trimming should be performed as a function of the threshold energy.
|
||||
Please not that trimming of the channels of the detector should be performed in advanced and is extremely important for a succeful energy calibration of the detector.
|
||||
|
||||
All energy calibration procedures should be applied to a trimmed detector and only an improvement of the existing trimbits can be performed afterwards, since it does not significatively affect the energy calibration.
|
||||
|
||||
|
||||
\begin{figure}
|
||||
\caption{Median of the number of counts as a function of the threshold for X-rays of 12.5, 17.5 and 25~keV for one of the detector modules using \textit{standard} settings. The solid line represents the fit of the experimental points with equation~\ref{eq:thrscan}. In the inset the linear fit between the X-ray energy and the position of the inflection point of the curves is shown.}\label{fig:modulecalibration}
|
||||
\includegraphics[width=\textwidth]{fig8.eps}
|
||||
\end{figure}
|
||||
\newpage
|
||||
|
||||
\section{Data acquisition}
|
||||
|
||||
The energy calibration consists in acquiring threshold scans using the detector at at least 2 (better 3) energies. A monochromatic beam is ideal in this procedure, but beam obtained from some fluorescent sample is also good.\\
|
||||
Please note that the statistic is important to succesfully analyze the data. Normally the exposure time for each step should be chosen in order to achieve at least 1000 counts per step.
|
||||
If this is not possible it is better to reduce the scan range or enlarge the scan step rather than acquiring data with a too low statics.
|
||||
|
||||
With a quick acquisition or threshold scan it is useful to define the range of the scan and the exposure time. It is important to start from a threshold high enough that (almost) all channels of the detector have a negligible number of counts and that the plateau of the S-curve is long enough to correctly estimate the number of photons.
|
||||
|
||||
\subsection{Software}
|
||||
|
||||
For the acquisition ot the data you need to install the slsDetector software package (please refere to separate documentation). The use of the GUI is optional and all operations can be performed also using the text client.\\
|
||||
|
||||
In the following the command to acquire a dataset for the energy calibration with an exposure time of 1~s, and threshold scan range between 200 and 850 with a setp of 1 DAC unit.
|
||||
\begin{verbatim}
|
||||
> sls_detector_put encallog 1 #setup energy calibration
|
||||
> sls_detector_put exptime 1. #set exposure time to 1s
|
||||
> sls_detector_put scan0script threshold #setup threshold scan
|
||||
> sls_detector_put scan0range 200 850 1 #set scan range between 200 and 850, step of 1
|
||||
> sls_detector_acquire #acquire the data
|
||||
> sls_detector_put encallog 0 #unset energy calibration
|
||||
\end{verbatim}
|
||||
|
||||
With the GUI you can obtain the same results by clicking on the \textit{Energy Calibration} log button in the advanced tab (see figure~\ref{fig:guiencallog}) and setting up the threshold scan in the Actions tab (see figure~\ref{fig:guithrscan}). the exposure time should also be set in the measurement tab.
|
||||
|
||||
|
||||
This procedure should be executed at at least 2 (better 3) energies.
|
||||
|
||||
Additional to the data files, the acquisition will produce a .encal file containing an header and, for each step of the acquisition, the threshold value and the file name. \\
|
||||
In case you forgot to enable the encallog flag in the software, you can produce the file with the syntax as follows:
|
||||
\begin{verbatim}
|
||||
settings standard
|
||||
type Mythen+
|
||||
nmod 12
|
||||
modulenumber:0 000
|
||||
modulenumber:1 111
|
||||
modulenumber:2 222
|
||||
modulenumber:3 333
|
||||
modulenumber:4 444
|
||||
modulenumber:5 555
|
||||
modulenumber:6 666
|
||||
modulenumber:7 777
|
||||
modulenumber:8 888
|
||||
modulenumber:9 999
|
||||
modulenumber:10 aaa
|
||||
modulenumber:11 bbb
|
||||
450 standard_12_4keV_S450_0
|
||||
460 standard_12_4keV_S460_0
|
||||
470 standard_12_4keV_S470_0
|
||||
480 standard_12_4keV_S480_0
|
||||
490 standard_12_4keV_S490_0
|
||||
500 standard_12_4keV_S500_0
|
||||
510 standard_12_4keV_S510_0
|
||||
520 standard_12_4keV_S520_0
|
||||
...
|
||||
...
|
||||
\end{verbatim}
|
||||
|
||||
|
||||
|
||||
|
||||
\begin{figure}
|
||||
\caption{Acquisition GUI window to enable the energy calibration log.} \label{fig:guiencallog}
|
||||
\includegraphics[width=\textwidth]{GUI_Advanced.eps}
|
||||
\end{figure}
|
||||
|
||||
\begin{figure}
|
||||
\caption{Acquisition GUI window to setup the threshold scan.} \label{fig:guithrscan}
|
||||
\includegraphics[width=\textwidth]{GUI_ThresholdScan.eps}
|
||||
\end{figure}
|
||||
\newpage
|
||||
|
||||
\section{Data analysis}
|
||||
|
||||
The data analysis consists in fitting the S-curves obtained from the datasets acquired as above and then performing a linear fit between the energy values and the inflection points.
|
||||
|
||||
\subsection{Software}
|
||||
|
||||
The software used for the energy calibration data analysis is based on root (see http://root.cern.ch).\\
|
||||
This can be downloaded as binary or installed from sources. The version of the software should not play an important role, but up to now everything has been implemented and tested using version 5.20.
|
||||
|
||||
To start the data analysis simply launch:
|
||||
\begin{verbatim}
|
||||
> ./energyCalibrationWizard
|
||||
\end{verbatim}
|
||||
|
||||
To add anew energy write the energy value and select (or digit) the name of the .encal file corresponding to that energy (see figure~\ref{fig:addenergy}).\\
|
||||
The software assumes that the data files (.raw) and the .encal file are in the same directory.
|
||||
Press \textit{Preview} and a 2D color plot will be displayed, showing the channel numbers on the X-axis, the threshold on the Y-axis, and the number of counts as a color scale.
|
||||
By (right) clicking close to the axis you are able to zoom in/out, set the scale to logarithmic etc.\\
|
||||
If the plot corresponds to your expectations press \textit{Add to list}. The energy value will be shown in the combo box on top and labels will display the settings of the detector, the number of modules, the number of channels per module and the modules serial numbers.
|
||||
|
||||
Add then all the other energies to the calibration always by editing the energy value and .encal file name, pressing \textit{preview} and \textit{add to list}.\\
|
||||
If the settings, number of modules or serial numbers do not match, you will not be llowed to add the energy.\\
|
||||
By using the \textit{selected energy actions} you can navigate in the combo box with list of energies, view the plots and eventually remove the ones you don't want to use in your calibration.\\
|
||||
Once you have uploaded at least 2 energies, you will be allowed to \textit{proceed to module calibration}.
|
||||
|
||||
|
||||
|
||||
\begin{figure}
|
||||
\caption{Window to add energies to the calibration.} \label{fig:addenergy}
|
||||
\includegraphics[width=\textwidth]{addEnergy.eps}
|
||||
\end{figure}
|
||||
|
||||
In the module calibration window (see figure~\ref{fig:calibratemodule}), you are still able to look at the calibration summary, and eventually return to the previous windown by pressing \textit{Back to energy setup}.\\
|
||||
The canvas will show the plot of the S-curves relative to the median of the selected module, fitted with equation~\ref{eq:thrscan} and the linear fit between the energy values and the fitted inflection points.
|
||||
Normally the points lie on a straight line (although often not perfect), therefore it should be simple to spot if there are problems in the fitting of some of the data.\\
|
||||
If \textit{Manual save} is unclicked, the calibration files will be saved locally, with the extension automatically generated by using the modules serial numbers, every time a linear fit is performed (i.e. if you mess up wiht the linear fit you overwrite a previous good file!). If you click the checkbox, you need to save the calibration by pressing \textit{Write to file} for each module once you are happy with the fit.
|
||||
|
||||
To change the Y scale of the plot, edit the \textit{Counts} entry. After clicking of the energy button (eventually twice) the maximum of the histogram will be set to three times the value.
|
||||
|
||||
To re-fit one energy with modified range or start parameters, you should press the central button with the energy value once the energy is selected. The text color tells you which curve you are referring to.\\
|
||||
|
||||
You should set the range of the fit. In particular the maximum should be limited in order to avoid to enter the noise range (and can be pretty different for the various modules).\\
|
||||
Normally the data are acquired by collecting holes from the detector and therefore the \textit{Invert axis} check button should be ckecked. Uncheck it in case your detector collects electrons (e.g. CdTe, Si n in p)
|
||||
|
||||
You can change the start values of the parameters of the fits by editing the number eneries. The label nearby will show you the actual value of the fitted parameters.\\
|
||||
By checking the checkboxes you can fix the values to the ones you specify.\\
|
||||
Normally it can be useful to fix the pedestal and pedestal slope to 0, unless you have a lot of 3rd armnonics contribution, primary beam background or similar.\\
|
||||
Changing the starting value of the inflection point or of the number of counts can often help the fit to converge.\\
|
||||
Normally it is not very useful to change the starting value for the noise or charge sharing slope.
|
||||
|
||||
The button \textit{Finished} will be enebled only once the calibration files have been generated for all modules.
|
||||
|
||||
|
||||
\begin{figure}
|
||||
\caption{Window to calibrate the modules.} \label{fig:calibratemodule}
|
||||
\includegraphics[width=\textwidth]{calibrateModule.eps}
|
||||
\end{figure}
|
||||
\newpage
|
||||
|
||||
|
||||
\section{Setup calibration files}
|
||||
|
||||
To use the genrated calibration files as default ones, copy them into your default \textit{caldir/settings} renaming them calibration.snxxx, where snxxx is the extension that the genrated files already have, which corresponds to the module serial number.\\
|
||||
Fot this scope, a script as following can be used:
|
||||
\begin{verbatim}
|
||||
for i in $(ls newcal_standard.sn* | awk -F "." '{print $2}'); do \
|
||||
mv newcal_standard.$i caldir/standard/calibration.$i; \
|
||||
done
|
||||
\end{verbatim}
|
||||
|
||||
By reloading the default detector settings, the calibration coefficients will be automatically loaded.
|
59330
manual/manual-calwiz/enable_angcal.eps
Normal file
BIN
manual/manual-calwiz/eneble_angcal.png
Normal file
After Width: | Height: | Size: 70 KiB |
16
manual/manual-calwiz/energyCalibrationHowTo.tex
Normal file
@ -0,0 +1,16 @@
|
||||
\documentclass{article}
|
||||
\usepackage{amssymb}
|
||||
\usepackage[dvips]{graphicx}
|
||||
\usepackage{verbatim}
|
||||
\begin{document}
|
||||
|
||||
\title{Energy calibration wizard manual}
|
||||
\author{Anna Bergamaschi}
|
||||
\date{\today}
|
||||
\maketitle
|
||||
|
||||
|
||||
\section{Introduction}
|
||||
\input{enCal.tex}
|
||||
\end{document}
|
||||
|
135
manual/manual-calwiz/fig4.eps
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|
||||
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-9 d 10 -9 d 10 -9 d 10 -10 d 10 -10 d 9 -10 d 10 -10 d 10 -10 d 10 -11 d 10 -11 d 9 -11 d 10 -11 d 10 -12 d 10 -12 d 9 -11 d 10 -12 d 10 -12 d 10 -12 d 10 -12 d 9 -13 d 10 -12 d 10 -12 d 10 -12 d s 1616 1605 m 9 -12 d 10 -12 d 10 -12 d 10 -11 d 10
|
||||
-12 d 9 -11 d 10 -11 d 10 -11 d 10 -11 d 9 -11 d 10 -10 d 10 -10 d 10 -10 d 10 -9 d 9 -9 d 10 -9 d 10 -8 d 10 -8 d 9 -8 d 10 -8 d 10 -7 d 10 -6 d 10 -7 d 9 -6 d 10 -6 d 10 -6 d 10 -5 d 9 -5 d 10 -4 d 10 -5 d 10 -4 d 10 -3 d 9 -4 d 10 -3 d 10 -3 d
|
||||
10 -3 d 9 -3 d 10 -2 d 10 -2 d 10 -3 d 10 -1 d 9 -2 d 10 -2 d 10 -1 d 10 -1 d 9 -2 d 10 -1 d 10 -1 d 10 -1 d s 2095 1303 m 10 X s[ 12 12] 0 sd 3 lw 1 1 1 c black[ ] 0 sd 1147 1972 1177 1960 1208 1944 1239 1929 1269 1911 1300 1891 1330 1870 1361
|
||||
1847 1391 1822 1422 1795 1452 1767 1483 1737 1514 1704 1544 1672 1575 1639 1605 1607 1636 1573 1666 1541 1697 1510 1727 1481 1758 1454 1789 1429 1819 1407 1850 1388 1880 1370 1911 1355 1941 1343 1972 1332 2002 1324 2033 1317 2064 1312 2094 1308 32
|
||||
{ m24} R[ 12 12] 0 sd 9 lw 0.95 0.95 0.95 c black 1136 1982 m 10 -4 d 10 -3 d 10 -5 d 10 -4 d 9 -4 d 10 -5 d 10 -5 d 10 -5 d 9 -5 d 10 -5 d 10 -6 d 10 -5 d 10 -6 d 9 -6 d 10 -6 d 10 -6 d 10 -7 d 9 -7 d 10 -7 d 10 -7 d 10 -8 d 10 -7 d 9 -8 d 10 -8 d
|
||||
10 -9 d 10 -8 d 9 -9 d 10 -9 d 10 -9 d 10 -9 d 10 -10 d 9 -9 d 10 -10 d 10 -10 d 10 -10 d 10 -10 d 9 -10 d 10 -11 d 10 -11 d 10 -10 d 9 -11 d 10 -10 d 10 -11 d 10 -11 d 10 -11 d 9 -11 d 10 -10 d 10 -11 d 10 -11 d s 1616 1592 m 9 -10 d 10 -11 d 10
|
||||
-10 d 10 -10 d 10 -10 d 9 -10 d 10 -10 d 10 -10 d 10 -10 d 9 -9 d 10 -9 d 10 -9 d 10 -8 d 10 -9 d 9 -8 d 10 -8 d 10 -7 d 10 -8 d 9 -7 d 10 -7 d 10 -7 d 10 -6 d 10 -7 d 9 -5 d 10 -6 d 10 -6 d 10 -5 d 9 -4 d 10 -5 d 10 -5 d 10 -4 d 10 -4 d 9 -4 d 10
|
||||
-3 d 10 -3 d 10 -4 d 9 -3 d 10 -2 d 10 -3 d 10 -2 d 10 -3 d 9 -2 d 10 -2 d 10 -2 d 10 -1 d 9 -2 d 10 -1 d 10 -2 d 10 -1 d s 2095 1308 m 10 -1 d s[ 4 8] 0 sd 3 lw 1 1 1 c black[ ] 0 sd 1147 2002 1177 1989 1208 1983 1239 1966 1269 1957 1300 1940
|
||||
1330 1925 1361 1904 1391 1886 1422 1863 1452 1834 1483 1804 1514 1767 1544 1731 1575 1686 1605 1646 1636 1597 1666 1556 1697 1511 1727 1473 1758 1436 1789 1405 1819 1381 1850 1358 1880 1343 1911 1329 1941 1321 1972 1313 2002 1311 2033 1306 2064
|
||||
1306 2094 1304 32 { m28} R[ 4 8] 0 sd 9 lw 0.95 0.95 0.95 c black 1136 2004 m 10 -3 d 10 -2 d 10 -3 d 10 -3 d 9 -3 d 10 -3 d 10 -3 d 10 -3 d 9 -4 d 10 -3 d 10 -4 d 10 -3 d 10 -4 d 9 -4 d 10 -4 d 10 -5 d 10 -4 d 9 -5 d 10 -5 d 10 -5 d 10 -6 d 10 -6
|
||||
d 9 -6 d 10 -7 d 10 -7 d 10 -7 d 9 -7 d 10 -9 d 10 -8 d 10 -8 d 10 -10 d 9 -10 d 10 -10 d 10 -10 d 10 -11 d 10 -11 d 9 -11 d 10 -13 d 10 -12 d 10 -13 d 9 -13 d 10 -13 d 10 -14 d 10 -13 d 10 -14 d 9 -15 d 10 -14 d 10 -14 d 10 -14 d s 1616 1625 m 9
|
||||
-15 d 10 -14 d 10 -14 d 10 -14 d 10 -14 d 9 -13 d 10 -14 d 10 -13 d 10 -13 d 9 -12 d 10 -12 d 10 -12 d 10 -11 d 10 -11 d 9 -10 d 10 -11 d 10 -9 d 10 -8 d 9 -9 d 10 -8 d 10 -8 d 10 -7 d 10 -7 d 9 -5 d 10 -6 d 10 -6 d 10 -5 d 9 -4 d 10 -4 d 10 -4 d
|
||||
10 -3 d 10 -3 d 9 -3 d 10 -3 d 10 -2 d 10 -2 d 9 -2 d 10 -2 d 10 -1 d 10 -2 d 10 -1 d 9 -1 d 10 -1 d 10 -1 d 10 X 9 -1 d 10 X 10 -1 d 10 X s 2095 1303 m 10 -1 d s[ ] 0 sd 3 lw 1 1 1 c black 632 2089 645 1978 658 1730 671 1586 684 1490 697 1427 709
|
||||
1390 722 1364 735 1345 748 1334 761 1324 774 1315 787 1309 800 1302 813 1295 826 1289 839 1282 852 1277 865 1270 878 1264 891 1258 904 1251 917 1246 930 1240 943 1234 956 1229 969 1222 982 1216 995 1210 1008 1204 1020 1196 1033 1193 1046 1186 1059
|
||||
1180 1072 1173 1085 1169 1098 1163 1111 1156 1124 1150 1137 1145 1150 1140 1163 1133 1176 1127 1189 1120 1202 1115 1215 1109 1228 1101 1241 1095 1254 1087 1267 1081 50 { m20} R 632 2089 m 13 -111 d 13 -248 d 13 -144 d 13 -96 d 13 -63 d 12 -37 d 13
|
||||
-26 d 13 -19 d 13 -11 d 13 -10 d 13 -9 d 13 -6 d 13 -7 d 13 -7 d 13 -6 d 13 -7 d 13 -5 d 13 -7 d 13 -6 d 13 -6 d 13 -7 d 13 -5 d 13 -6 d 13 -6 d 13 -5 d 13 -7 d 13 -6 d 13 -6 d 13 -6 d 12 -8 d 13 -3 d 13 -7 d 13 -6 d 13 -7 d 13 -4 d 13 -6 d 13 -7 d
|
||||
13 -6 d 13 -5 d 13 -5 d 13 -7 d 13 -6 d 13 -7 d 13 -5 d 13 -6 d 13 -8 d 13 -6 d 13 -8 d 13 -6 d s 1267 1081 1280 1075 1293 1068 1306 1060 1319 1052 1331 1046 1344 1038 1357 1031 1370 1022 1383 1015 1396 1006 1409 998 1422 987 1435 977 1448 966 1461
|
||||
954 1474 941 1487 925 1500 909 1513 890 1526 869 1539 847 1552 823 1565 796 1578 767 1591 735 1604 702 1617 668 1630 634 1642 598 1655 565 1668 532 1681 502 1694 473 1707 448 1720 425 1733 405 1746 389 1759 375 1772 364 1785 355 1798 348 1811 343
|
||||
1824 340 1837 337 1850 335 1863 334 1876 333 1889 332 1902 332 50 { m20} R 1267 1081 m 13 -6 d 13 -7 d 13 -8 d 13 -8 d 12 -6 d 13 -8 d 13 -7 d 13 -9 d 13 -7 d 13 -9 d 13 -8 d 13 -11 d 13 -10 d 13 -11 d 13 -12 d 13 -13 d 13 -16 d 13 -16 d 13 -19 d
|
||||
13 -21 d 13 -22 d 13 -24 d 13 -27 d 13 -29 d 13 -32 d 13 -33 d 13 -34 d 13 -34 d 12 -36 d 13 -33 d 13 -33 d 13 -30 d 13 -29 d 13 -25 d 13 -23 d 13 -20 d 13 -16 d 13 -14 d 13 -11 d 13 -9 d 13 -7 d 13 -5 d 13 -3 d 13 -3 d 13 -2 d 13 -1 d 13 -1 d 13
|
||||
-1 d 13 X s 1902 332 1915 331 1928 331 1941 331 1953 331 1966 331 1979 331 1992 331 2005 331 2018 331 2031 331 2044 331 2057 331 2070 331 2083 331 2096 331 2109 331 2122 331 2135 331 2148 331 20 { m20} R 1902 332 m 13 -1 d 233 X s[ 12 12] 0 sd 1 1
|
||||
1 c black[ ] 0 sd 748 2089 761 1386 774 1361 787 1345 800 1325 813 1319 826 1305 839 1294 852 1286 865 1279 878 1270 891 1263 904 1254 917 1247 930 1242 943 1235 956 1229 969 1223 982 1215 995 1210 1008 1204 1020 1197 1033 1191 1046 1185 1059 1181
|
||||
1072 1174 1085 1168 1098 1161 1111 1155 1124 1148 1137 1142 1150 1136 1163 1130 1176 1124 1189 1116 1202 1110 1215 1104 1228 1097 1241 1091 1254 1083 1267 1076 1280 1069 1293 1061 1306 1054 1319 1046 1331 1038 1344 1030 1357 1022 1370 1011 1383
|
||||
1004 50 { m24} R[ 12 12] 0 sd 748 2089 m 13 -703 d 13 -25 d 13 -16 d 13 -20 d 13 -6 d 13 -14 d 13 -11 d 13 -8 d 13 -7 d 13 -9 d 13 -7 d 13 -9 d 13 -7 d 13 -5 d 13 -7 d 13 -6 d 13 -6 d 13 -8 d 13 -5 d 13 -6 d 12 -7 d 13 -6 d 13 -6 d 13 -4 d 13 -7 d
|
||||
13 -6 d 13 -7 d 13 -6 d 13 -7 d 13 -6 d 13 -6 d 13 -6 d 13 -6 d 13 -8 d 13 -6 d 13 -6 d 13 -7 d 13 -6 d 13 -8 d 13 -7 d 13 -7 d 13 -8 d 13 -7 d 13 -8 d 12 -8 d 13 -8 d 13 -8 d 13 -11 d 13 -7 d s[ ] 0 sd 1383 1004 1396 994 1409 983 1422 972 1435
|
||||
961 1448 949 1461 935 1474 921 1487 903 1500 885 1513 866 1526 845 1539 821 1552 796 1565 769 1578 742 1591 711 1604 681 1617 651 1630 620 1642 589 1655 559 1668 530 1681 503 1694 477 1707 455 1720 434 1733 416 1746 400 1759 386 1772 374 1785 364
|
||||
1798 356 1811 350 1824 345 1837 341 1850 339 1863 336 1876 334 1889 333 1902 332 1915 332 1928 331 1941 331 1953 331 1966 331 1979 331 1992 331 2005 331 2018 331 50 { m24} R[ 12 12] 0 sd 1383 1004 m 13 -10 d 13 -11 d 13 -11 d 13 -11 d 13 -12 d 13
|
||||
-14 d 13 -14 d 13 -18 d 13 -18 d 13 -19 d 13 -21 d 13 -24 d 13 -25 d 13 -27 d 13 -27 d 13 -31 d 13 -30 d 13 -30 d 13 -31 d 12 -31 d 13 -30 d 13 -29 d 13 -27 d 13 -26 d 13 -22 d 13 -21 d 13 -18 d 13 -16 d 13 -14 d 13 -12 d 13 -10 d 13 -8 d 13 -6 d
|
||||
13 -5 d 13 -4 d 13 -2 d 13 -3 d 13 -2 d 13 -1 d 13 -1 d 13 X 13 -1 d 90 X s[ ] 0 sd 2018 331 2031 331 2044 330 2057 330 2070 330 2083 330 2096 330 2109 330 2122 330 2135 330 2148 330 11 { m24} R[ 12 12] 0 sd 2018 331 m 13 X 13 -1 d 104 X s[ 4 8
|
||||
] 0 sd 1 1 1 c black[ ] 0 sd 515 2089 528 2040 541 1779 554 1647 567 1615 580 1504 593 1472 606 1483 619 1425 632 1409 645 1423 658 1386 671 1377 684 1362 697 1374 709 1345 722 1340 735 1340 748 1322 761 1315 774 1314 787 1301 800 1295 813 1295 826
|
||||
1281 839 1278 852 1268 865 1269 878 1256 891 1254 904 1249 917 1240 930 1235 943 1233 956 1228 969 1219 982 1217 995 1210 1008 1206 1020 1197 1033 1197 1046 1185 1059 1184 1072 1178 1085 1171 1098 1167 1111 1157 1124 1158 1137 1146 1150 1144 50 {
|
||||
m28} R[ 4 8] 0 sd 515 2089 m 13 -49 d 13 -261 d 13 -132 d 13 -32 d 13 -111 d 13 -32 d 13 11 d 13 -58 d 13 -16 d 13 14 d 13 -37 d 13 -9 d 13 -15 d 13 12 d 12 -29 d 13 -5 d 13 X 13 -18 d 13 -7 d 13 -1 d 13 -13 d 13 -6 d 13 X 13 -14 d 13 -3 d 13 -10 d
|
||||
13 1 d 13 -13 d 13 -2 d 13 -5 d 13 -9 d 13 -5 d 13 -2 d 13 -5 d 13 -9 d 13 -2 d 13 -7 d 13 -4 d 12 -9 d 13 X 13 -12 d 13 -1 d 13 -6 d 13 -7 d 13 -4 d 13 -10 d 13 1 d 13 -12 d 13 -2 d s[ ] 0 sd 1150 1144 1163 1135 1176 1133 1189 1123 1202 1122 1215
|
||||
1111 1228 1108 1241 1103 1254 1091 1267 1088 1280 1077 1293 1076 1306 1063 1319 1059 1331 1050 1344 1044 1357 1034 1370 1031 1383 1019 1396 1014 1409 1006 1422 996 1435 989 1448 976 1461 971 1474 955 1487 947 1500 931 1513 917 1526 897 1539 881
|
||||
1552 859 1565 832 1578 804 1591 770 1604 736 1617 694 1630 657 1642 612 1655 573 1668 531 1681 496 1694 461 1707 432 1720 409 1733 388 1746 374 1759 362 1772 354 1785 346 50 { m28} R[ 4 8] 0 sd 1150 1144 m 13 -9 d 13 -2 d 13 -10 d 13 -1 d 13 -11 d
|
||||
13 -3 d 13 -5 d 13 -12 d 13 -3 d 13 -11 d 13 -1 d 13 -13 d 13 -4 d 12 -9 d 13 -6 d 13 -10 d 13 -3 d 13 -12 d 13 -5 d 13 -8 d 13 -10 d 13 -7 d 13 -13 d 13 -5 d 13 -16 d 13 -8 d 13 -16 d 13 -14 d 13 -20 d 13 -16 d 13 -22 d 13 -27 d 13 -28 d 13 -34 d
|
||||
13 -34 d 13 -42 d 13 -37 d 12 -45 d 13 -39 d 13 -42 d 13 -35 d 13 -35 d 13 -29 d 13 -23 d 13 -21 d 13 -14 d 13 -12 d 13 -8 d 13 -8 d s[ ] 0 sd 1785 346 1798 345 1811 340 1824 340 1837 338 1850 337 1863 337 1876 335 1889 336 1902 335 1915 335 1928
|
||||
335 1941 335 1953 334 1966 335 1979 335 1992 334 2005 334 2018 334 2031 334 2044 333 2057 334 2070 333 2083 333 2096 333 2109 333 2122 333 2135 333 2148 333 29 { m28} R[ 4 8] 0 sd 1785 346 m 13 -1 d 13 -5 d 13 X 13 -2 d 13 -1 d 13 X 13 -2 d 13 1 d
|
||||
13 -1 d 39 X 12 -1 d 13 1 d 13 X 13 -1 d 39 X 13 -1 d 13 1 d 13 -1 d 78 X s[ ] 0 sd 6 lw 1 1 1 c 680 440 454 440 bf black 454 440 m 680 X s 1134 440 m 440 Y s 1134 880 m -680 X s 454 880 m -440 Y s
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gsave 2268 2199 0 0 C 470 798 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (Settings) show NC gr
|
||||
gsave 2268 2199 0 0 C 621 678 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (standard) show NC gr 3 lw 479 715 m 119 X s 539 715 m20
|
||||
gsave 2268 2199 0 0 C 621 567 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (fast) show NC gr [ 12 12] 0 sd 479 605 m 119 X s[ ] 0 sd 539 605 m24[ 12 12] 0 sd
|
||||
gsave 2268 2199 0 0 C 621 470 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (highgain) show NC gr [ 4 8] 0 sd 479 495 m 119 X s[ ] 0 sd 539 495 m28[ 4 8] 0 sd
|
||||
gr gr
|
||||
showpage
|
||||
end
|
||||
%%EOF
|
103
manual/manual-calwiz/fig7.eps
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newpath gsave .25 .25 scale gsave 0 0 t black[ ] 0 sd 6 lw 1 1 1 c 2268 2256 0 0 bf black 3 lw 1 1 1 c 1814 1806 340 338 bf black 1814 1806 340 338 bl 1 1 1 c 1814 1806 340 338 bf black 1814 1806 340 338 bl 1 1 1 c black /w 24
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|
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m2} R 955 1457 963 1451 972 1445 980 1434 989 1427 997 1421 1006 1405 1014 1400 1023 1385 1031 1373 1040 1368 1048 1356 1057 1345 1065 1331 1073 1324 1082 1310 1090 1304 1099 1291 1107 1278 1116 1268 1124 1256 1133 1248 1141 1240 1150 1231 1158
|
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1222 1167 1208 1175 1204 1184 1197 1192 1186 1201 1185 1209 1177 1218 1172 1226 1163 1235 1152 1243 1155 1251 1147 1260 1142 1268 1137 1277 1133 1285 1132 1294 1123 1302 1124 1311 1118 1319 1113 1328 1109 1336 1103 1345 1100 1353 1094 1362 1095
|
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1370 1092 50 { m2} R 1370 1092 1379 1088 1387 1085 1396 1079 1404 1073 1413 1064 1421 1063 1430 1058 1438 1054 1446 1053 1455 1048 1463 1043 1472 1038 1480 1034 1489 1032 1497 1026 1506 1020 1514 1018 1523 1009 1531 1007 1540 998 1548 994 1557 989
|
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1565 983 1574 976 1582 966 1591 960 1599 951 1608 943 1616 935 1624 929 1633 915 1641 903 1650 893 1658 882 1667 869 1675 856 1684 846 1692 832 1701 814 1709 798 1718 779 1726 763 1735 745 1743 725 1752 704 1760 682 1769 661 1777 638 1786 619 50 {
|
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m2} R 1786 619 1794 597 1803 579 1811 558 1819 536 1828 518 1836 500 1845 483 1853 467 1862 453 1870 438 1879 426 1887 415 1896 404 1904 394 1913 386 1921 378 1930 372 1938 367 1947 362 1955 359 1964 356 1972 352 1981 350 1989 348 1997 347 2006 345
|
||||
2014 344 2023 343 2031 343 2040 343 2048 342 2057 342 2065 342 2074 341 2082 341 2091 341 2099 341 2108 341 2116 341 2125 341 2133 341 2142 341 2150 341 44 { m2} R 9 lw 0.95 0.95 0.95 c black 715 1630 m 15 -9 d 14 -9 d 14 -9 d 15 -9 d 14 -9 d 15 -9
|
||||
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|
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|
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|
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-28 Y s 828 393 m -55 Y s 888 366 m -28 Y s 948 366 m -28 Y s 1008 366 m -28 Y s 1068 393 m -55 Y s 1129 366 m -28 Y s 1189 366 m -28 Y s 1249 366 m -28 Y s 1309 393 m -55 Y s 1369 366 m -28 Y s 1429 366 m -28 Y s 1489 366 m -28 Y s 1549 393 m -55
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||||
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||||
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||||
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|
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|
||||
367 654 m -27 X s 395 699 m -55 X s 367 745 m -27 X s 367 790 m -27 X s 367 835 m -27 X s 395 880 m -55 X s 367 925 m -27 X s 367 970 m -27 X s 367 1015 m -27 X s 395 1061 m -55 X s 367 1106 m -27 X s 367 1151 m -27 X s 367 1196 m -27 X s 395 1241
|
||||
m -55 X s 367 1286 m -27 X s 367 1331 m -27 X s 367 1376 m -27 X s 395 1422 m -55 X s 367 1467 m -27 X s 367 1512 m -27 X s 367 1557 m -27 X s 395 1602 m -55 X s 367 1647 m -27 X s 367 1692 m -27 X s 367 1737 m -27 X s 395 1783 m -55 X s 367 1828 m
|
||||
-27 X s 367 1873 m -27 X s 367 1918 m -27 X s 395 1963 m -55 X s 367 2008 m -27 X s 367 2053 m -27 X s 367 2098 m -27 X s 395 2144 m -55 X s
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|
||||
-8 d 14 -8 d 14 -8 d 15 -8 d 14 -8 d 15 -8 d 14 -8 d 15 -8 d 14 -7 d 14 -8 d 15 -8 d 14 -8 d 15 -8 d 14 -8 d 14 -8 d 15 -8 d 14 -8 d 15 -8 d 14 -7 d 15 -8 d 14 -8 d 14 -8 d 15 -8 d 14 -8 d 15 -8 d 14 -8 d 15 -8 d 14 -7 d 14 -8 d 15 -8 d 14 -8 d 15
|
||||
-8 d 14 -8 d 14 -8 d 15 -8 d 14 -8 d 15 -8 d s 1422 1062 m 14 -7 d 15 -8 d 14 -8 d 14 -8 d 15 -8 d 14 -9 d 15 -8 d 14 -9 d 15 -9 d 14 -10 d 14 -10 d 15 -11 d 14 -13 d 15 -14 d 14 -16 d 14 -18 d 15 -21 d 14 -23 d 15 -26 d 14 -29 d 15 -31 d 14 -33 d
|
||||
14 -35 d 15 -36 d 14 -36 d 15 -36 d 14 -35 d 15 -32 d 14 -31 d 14 -27 d 15 -24 d 14 -21 d 15 -18 d 14 -15 d 14 -12 d 15 -9 d 14 -7 d 15 -5 d 14 -4 d 15 -3 d 14 -2 d 14 -2 d 15 -1 d 14 X 15 -1 d 57 X s 2128 341 m 15 X s[ 4 8] 0 sd 6 lw 1068 338 m
|
||||
993 Y s 1429 338 m 720 Y s 1789 338 m 281 Y s[ 12 16 4 16] 0 sd 347 1331 m 721 X s 347 1256 m 721 X s
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||||
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||||
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||||
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|
||||
gsave 2268 2256 0 0 C 1044 1360 t 0 r /Helvetica-Bold findfont 104.36 sf 0 0 m (E) show NC gr [ ] 0 sd 1068 519 m 361 X s 1397 537 m 32 -18 d -32 -18 d s 1100 501 m -32 18 d 32 18 d s 1429 519 m 360 X s 1758 537 m 31 -18 d -31 -18 d s 1461 501 m
|
||||
-32 18 d 32 18 d s
|
||||
gsave 2268 2256 0 0 C 1247 564 t 0 r /Symbol findfont 104.36 sf 0 0 m (S) show NC gr
|
||||
gsave 2268 2256 0 0 C 1608 564 t 0 r /Symbol findfont 104.36 sf 0 0 m (S) show NC gr 588 1331 m -75 Y s 597 1272 m -9 -16 d -9 16 d s 579 1315 m 9 16 d 9 -16 d s
|
||||
gsave 2268 2256 0 0 C 609 1269 t 0 r /Symbol findfont 84.6163 sf 0 0 m (D) show NC gr
|
||||
gr gr
|
||||
showpage
|
||||
end
|
||||
%%EOF
|
146
manual/manual-calwiz/fig8.eps
Normal file
@ -0,0 +1,146 @@
|
||||
%!PS-Adobe-2.0 EPSF-2.0
|
||||
%%BoundingBox: 0 0 567 550
|
||||
%%Title: /afs/psi.ch/user/b/bergamaschi/root_macros/paper/moduleCalibration.eps: c1_n3
|
||||
%%Creator: ROOT Version 5.20/00
|
||||
%%CreationDate: Tue Feb 24 16:20:36 2009
|
||||
%%EndComments
|
||||
%%BeginProlog
|
||||
80 dict begin
|
||||
/s {stroke} def /l {lineto} def /m {moveto} def /t {translate} def
|
||||
/sw {stringwidth} def /r {rotate} def /rl {roll} def /R {repeat} def
|
||||
/d {rlineto} def /rm {rmoveto} def /gr {grestore} def /f {eofill} def
|
||||
/c {setrgbcolor} def /black {0 setgray} def /sd {setdash} def
|
||||
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|
||||
/box {m dup 0 exch d exch 0 d 0 exch neg d cl} def
|
||||
/NC{systemdict begin initclip end}def/C{NC box clip newpath}def
|
||||
/bl {box s} def /bf {box f} def /Y { 0 exch d} def /X { 0 d} def
|
||||
/mp {newpath /y exch def /x exch def} def
|
||||
/side {[w .77 mul w .23 mul] .385 w mul sd w 0 l currentpoint t -144 r} def
|
||||
/mr {mp x y w2 0 360 arc} def /m24 {mr s} def /m20 {mr f} def
|
||||
/mb {mp x y w2 add m w2 neg 0 d 0 w neg d w 0 d 0 w d cl} def
|
||||
/mt {mp x y w2 add m w2 neg w neg d w 0 d cl} def
|
||||
/m21 {mb f} def /m25 {mb s} def /m22 {mt f} def /m26{mt s} def
|
||||
/m23 {mp x y w2 sub m w2 w d w neg 0 d cl f} def
|
||||
/m27 {mp x y w2 add m w3 neg w2 neg d w3 w2 neg d w3 w2 d cl s} def
|
||||
/m28 {mp x w2 sub y w2 sub w3 add m w3 0 d 0 w3 neg d w3 0 d 0 w3 d w3 0 d 0 w3 d w3 neg 0 d 0 w3 d w3 neg 0 d
|
||||
0 w3 neg d w3 neg 0 d cl s } def
|
||||
/m29 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t
|
||||
4 {side} repeat cl fill gr} def
|
||||
/m30 {mp gsave x w2 sub y w2 add w3 sub m currentpoint t
|
||||
4 {side} repeat cl s gr} def
|
||||
/m31 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d x w2 sub y w2 add m w w neg d x w2 sub y w2
|
||||
sub m w w d s} def
|
||||
/m2 {mp x y w2 sub m 0 w d x w2 sub y m w 0 d s} def
|
||||
/m5 {mp x w2 sub y w2 sub m w w d x w2 sub y w2 add m w w neg d s} def
|
||||
/reEncode {exch findfont dup length dict begin {1 index /FID eq {pop pop} {def} ifelse } forall /Encoding exch def currentdict end dup /FontName get exch definefont pop } def [/Times-Bold /Times-Italic /Times-BoldItalic /Helvetica
|
||||
/Helvetica-Oblique /Helvetica-Bold /Helvetica-BoldOblique /Courier /Courier-Oblique /Courier-Bold /Courier-BoldOblique /Times-Roman /AvantGarde-Book /AvantGarde-BookOblique /AvantGarde-Demi /AvantGarde-DemiOblique /Bookman-Demi
|
||||
/Bookman-DemiItalic /Bookman-Light /Bookman-LightItalic /Helvetica-Narrow /Helvetica-Narrow-Bold /Helvetica-Narrow-BoldOblique /Helvetica-Narrow-Oblique /NewCenturySchlbk-Roman /NewCenturySchlbk-Bold
|
||||
/NewCenturySchlbk-BoldItalic /NewCenturySchlbk-Italic /Palatino-Bold /Palatino-BoldItalic /Palatino-Italic /Palatino-Roman ] {ISOLatin1Encoding reEncode } forall
|
||||
/oshow {gsave [] 0 sd true charpath stroke gr} def
|
||||
/stwn { /fs exch def /fn exch def /text exch def fn findfont fs sf
|
||||
text sw pop xs add /xs exch def} def
|
||||
/stwb { /fs exch def /fn exch def /nbas exch def /textf exch deftextf length /tlen exch def nbas tlen gt {/nbas tlendef} iffn findfont fs sf textf dup length nbas sub nbas getinterval sw
|
||||
pop neg xs add /xs exch def} def
|
||||
%%EndProlog
|
||||
%%BeginSetup
|
||||
%%EndSetup
|
||||
newpath gsave .25 .25 scale gsave 0 0 t black[ ] 0 sd 6 lw 1 1 1 c 2268 2199 0 0 bf black 3 lw 1 1 1 c 1814 1759 340 330 bf black 1814 1759 340 330 bl 1 1 1 c 1814 1759 340 330 bf black 1814 1759 340 330 bl 1 1 1 c black 340 330 m 1814 X s 6 lw
|
||||
340 330 m 1814 X s
|
||||
gsave 2268 2199 0 0 C 1279 123 t 0 r /Helvetica-Bold findfont 102.56 sf 0 0 m (Threshold \(DACu\)) show NC gr 340 383 m -53 Y s 392 356 m -26 Y s 444 356 m -26 Y s 496 356 m -26 Y s 547 356 m -26 Y s 599 383 m -53 Y s 651 356 m -26 Y s 703 356 m
|
||||
-26 Y s 755 356 m -26 Y s 807 356 m -26 Y s 858 383 m -53 Y s 910 356 m -26 Y s 962 356 m -26 Y s 1014 356 m -26 Y s 1066 356 m -26 Y s 1118 383 m -53 Y s 1169 356 m -26 Y s 1221 356 m -26 Y s 1273 356 m -26 Y s 1325 356 m -26 Y s 1377 383 m -53 Y
|
||||
s 1429 356 m -26 Y s 1480 356 m -26 Y s 1532 356 m -26 Y s 1584 356 m -26 Y s 1636 383 m -53 Y s 1688 356 m -26 Y s 1740 356 m -26 Y s 1791 356 m -26 Y s 1843 356 m -26 Y s 1895 383 m -53 Y s 1947 356 m -26 Y s 1999 356 m -26 Y s 2051 356 m -26 Y s
|
||||
2102 356 m -26 Y s 2154 383 m -53 Y s
|
||||
gsave 2268 2199 0 0 C 271 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (400) show NC gr
|
||||
gsave 2268 2199 0 0 C 530 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (450) show NC gr
|
||||
gsave 2268 2199 0 0 C 789 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (500) show NC gr
|
||||
gsave 2268 2199 0 0 C 1048 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (550) show NC gr
|
||||
gsave 2268 2199 0 0 C 1308 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (600) show NC gr
|
||||
gsave 2268 2199 0 0 C 1567 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (650) show NC gr
|
||||
gsave 2268 2199 0 0 C 1826 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (700) show NC gr
|
||||
gsave 2268 2199 0 0 C 2085 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (750) show NC gr 340 330 m 1759 Y s
|
||||
gsave 2268 2199 0 0 C 100 1439 t 90 r /Helvetica-Bold findfont 102.56 sf 0 0 m (Counts \(A.U.\)) show NC gr 395 330 m -55 X s 367 374 m -27 X s 367 418 m -27 X s 367 462 m -27 X s 395 506 m -55 X s 367 550 m -27 X s 367 594 m -27 X s 367 638 m
|
||||
-27 X s 395 682 m -55 X s 367 726 m -27 X s 367 770 m -27 X s 367 814 m -27 X s 395 858 m -55 X s 367 902 m -27 X s 367 946 m -27 X s 367 990 m -27 X s 395 1034 m -55 X s 367 1078 m -27 X s 367 1122 m -27 X s 367 1166 m -27 X s 395 1210 m -55 X s
|
||||
367 1254 m -27 X s 367 1298 m -27 X s 367 1342 m -27 X s 395 1386 m -55 X s 367 1430 m -27 X s 367 1474 m -27 X s 367 1518 m -27 X s 395 1562 m -55 X s 367 1606 m -27 X s 367 1650 m -27 X s 367 1693 m -27 X s 395 1737 m -55 X s 367 1781 m -27 X s
|
||||
367 1825 m -27 X s 367 1869 m -27 X s 395 1913 m -55 X s 367 1957 m -27 X s 367 2001 m -27 X s 367 2045 m -27 X s 395 2089 m -55 X s
|
||||
gsave 2268 2199 0 0 C 285 293 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (0) show NC gr
|
||||
gsave 2268 2199 0 0 C 194 470 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (200) show NC gr
|
||||
gsave 2268 2199 0 0 C 194 647 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (400) show NC gr
|
||||
gsave 2268 2199 0 0 C 194 823 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (600) show NC gr
|
||||
gsave 2268 2199 0 0 C 194 997 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (800) show NC gr
|
||||
gsave 2268 2199 0 0 C 145 1174 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (1000) show NC gr
|
||||
gsave 2268 2199 0 0 C 145 1350 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (1200) show NC gr
|
||||
gsave 2268 2199 0 0 C 145 1527 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (1400) show NC gr
|
||||
gsave 2268 2199 0 0 C 145 1701 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (1600) show NC gr
|
||||
gsave 2268 2199 0 0 C 145 1877 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (1800) show NC gr
|
||||
gsave 2268 2199 0 0 C 145 2054 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (2000) show NC gr 3 lw 1 1 1 c black /w 24 def /w2 {w 2 div} def /w3 {w 3 div} def 858 330 864 330 869 330 874 330 879 330 884 330 889 330 895 330 900 330 905 330 910
|
||||
330 915 330 920 330 926 330 931 330 936 330 941 330 946 330 951 330 957 330 962 330 967 330 972 330 977 330 982 330 988 330 993 330 998 330 1003 330 1008 330 1013 330 1019 330 1024 330 1029 330 1034 330 1039 330 1044 330 1050 330 1055 330 1060 330
|
||||
1065 330 1070 330 1075 330 1081 330 1086 330 1091 330 1096 330 1101 330 1106 330 1112 330 50 { m26} R 1112 330 1117 330 1122 330 1127 330 1132 330 1137 330 1143 330 1148 330 1153 330 1158 330 1163 330 1168 330 1174 330 1179 330 1184 330 1189 330
|
||||
1194 330 1199 330 1205 330 1210 330 1215 330 1220 330 1225 331 1230 331 1236 331 1241 331 1246 331 1251 331 1256 331 1261 331 1267 331 1272 331 1277 331 1282 331 1287 331 1292 331 1298 332 1303 332 1308 332 1313 333 1318 334 1323 335 1329 336 1334
|
||||
338 1339 340 1344 343 1349 346 1354 349 1360 354 1365 360 50 { m26} R 1365 360 1370 366 1375 374 1380 383 1385 393 1391 405 1396 418 1401 433 1406 448 1411 464 1416 483 1422 501 1427 524 1432 545 1437 568 1442 591 1447 613 1453 635 1458 661 1463
|
||||
685 1468 706 1473 728 1478 751 1484 771 1489 790 1494 810 1499 827 1504 844 1509 859 1515 874 1520 887 1525 900 1530 911 1535 922 1540 932 1546 943 1551 951 1556 960 1561 969 1566 977 1571 985 1577 991 1582 998 1587 1004 1592 1010 1597 1016 1602
|
||||
1022 1608 1028 1613 1034 1618 1038 50 { m26} R 1618 1038 1623 1044 1628 1048 1633 1054 1639 1059 1644 1063 1649 1068 1654 1072 1659 1078 1664 1082 1670 1086 1675 1092 1680 1096 1685 1102 1690 1106 1695 1110 1701 1115 1706 1118 1711 1124 1716 1128
|
||||
1721 1133 1726 1137 1732 1141 1737 1145 1742 1149 1747 1153 1752 1160 1757 1162 1763 1167 1768 1169 1773 1173 1778 1177 1783 1182 1788 1186 1794 1190 1799 1195 1804 1199 1809 1202 1814 1206 1819 1210 1825 1215 1830 1217 1835 1222 1840 1226 1845
|
||||
1231 1850 1235 1856 1238 1861 1243 1866 1249 1871 1251 50 { m26} R 1871 1251 1876 1256 1881 1259 1887 1263 1892 1267 1897 1272 1902 1277 1907 1279 1912 1285 1918 1290 1923 1292 1928 1298 1933 1302 1938 1305 1943 1312 1949 1316 1954 1320 1959 1325
|
||||
1964 1330 1969 1333 1974 1338 1980 1345 1985 1351 1990 1357 1995 1363 2000 1372 2005 1384 2011 1397 2016 1419 2021 1441 2026 1473 2031 1519 2036 1584 2042 1680 2047 1822 2052 2020 2057 2089 37 { m26} R 2150 2089 m26 9 lw 0.95 0.95 0.95 c black 782
|
||||
330 m 434 X 16 1 d 48 X 16 1 d 16 1 d 16 4 d 16 7 d 17 12 d 16 21 d 16 32 d 16 45 d 16 58 d 16 68 d 16 73 d 16 74 d 16 68 d 16 58 d 16 47 d 16 37 d 16 28 d 16 22 d s 1569 987 m 16 18 d 17 16 d 16 14 d 16 15 d 16 14 d 16 13 d 16 14 d 16 14 d 16 14 d
|
||||
16 14 d 16 14 d 16 14 d 16 13 d 16 14 d 16 14 d 16 14 d 17 14 d 16 14 d 16 13 d 16 14 d 16 14 d 16 14 d 16 14 d s[ 12 12] 0 sd 3 lw 1447 330 m 283 Y s[ ] 0 sd 1447 613 m20[ 12 12] 0 sd[ ] 0 sd 1 1 1 c black 864 330 889 330 900 330 905 330 910 330
|
||||
915 330 920 330 926 330 931 330 936 330 941 330 946 330 951 330 957 330 962 330 967 330 972 331 977 331 982 331 988 331 993 331 998 332 1003 333 1008 333 1013 335 1019 336 1024 338 1029 340 1034 342 1039 345 1044 349 1050 353 1055 359 1060 366 1065
|
||||
373 1070 382 1075 391 1081 402 1086 413 1091 428 1096 442 1101 456 1106 474 1112 493 1117 511 1122 532 1127 552 1132 571 1137 593 1143 614 50 { m27} R 1143 614 1148 634 1153 659 1158 677 1163 697 1168 717 1174 738 1179 757 1184 773 1189 788 1194
|
||||
802 1199 820 1205 830 1210 842 1215 856 1220 870 1225 879 1230 888 1236 896 1241 904 1246 909 1251 918 1256 924 1261 930 1267 936 1272 942 1277 950 1282 955 1287 963 1292 968 1298 972 1303 974 1308 979 1313 985 1318 987 1323 991 1329 995 1334 1000
|
||||
1339 1004 1344 1011 1349 1012 1354 1016 1360 1020 1365 1024 1370 1026 1375 1032 1380 1038 1385 1040 1391 1045 1396 1046 50 { m27} R 1396 1046 1401 1051 1406 1053 1411 1056 1416 1055 1422 1058 1427 1063 1432 1067 1437 1073 1442 1073 1447 1080 1453
|
||||
1083 1458 1084 1463 1090 1468 1095 1473 1098 1478 1099 1484 1104 1489 1111 1494 1113 1499 1118 1504 1118 1509 1122 1515 1123 1520 1126 1525 1129 1530 1133 1535 1136 1540 1138 1546 1140 1551 1142 1556 1149 1561 1150 1566 1152 1571 1157 1577 1161
|
||||
1582 1161 1587 1164 1592 1169 1597 1172 1602 1174 1608 1176 1613 1178 1618 1180 1623 1183 1628 1184 1633 1190 1639 1190 1644 1195 1649 1196 50 { m27} R 1649 1196 1654 1196 1659 1205 1664 1206 1670 1210 1675 1214 1680 1217 1685 1222 1690 1221 1695
|
||||
1225 1701 1228 1706 1234 1711 1236 1716 1240 1721 1242 1726 1242 1732 1247 1737 1250 1742 1252 1747 1256 1752 1256 1757 1258 1763 1267 1768 1268 1773 1270 1778 1276 1783 1277 1788 1275 1794 1282 1799 1286 1804 1287 1809 1285 1814 1289 1819 1297
|
||||
1825 1299 1830 1302 1835 1306 1840 1311 1845 1311 1850 1309 1856 1313 1861 1319 1866 1321 1871 1321 1876 1322 1881 1327 1887 1328 1892 1331 1897 1337 1902 1343 50 { m27} R 1902 1343 1907 1350 1912 1351 1918 1354 1923 1362 1928 1359 1933 1365 1938
|
||||
1366 1943 1371 1949 1370 1954 1377 1959 1382 1964 1384 1969 1389 1974 1392 1980 1401 1985 1401 1990 1412 1995 1417 2000 1432 2005 1448 2011 1465 2016 1491 2021 1535 2026 1589 2031 1673 2036 1806 2042 2003 2047 2089 29 { m27} R 2150 2089 m27 9 lw
|
||||
0.95 0.95 0.95 c black 348 330 m 601 X 16 1 d 15 X 16 1 d 16 3 d 16 5 d 16 10 d 15 16 d 16 24 d 16 35 d 16 46 d 16 57 d s 1123 528 m 16 64 d 15 67 d 16 66 d 16 59 d 16 51 d 16 40 d 15 32 d 16 24 d 16 18 d 16 14 d 16 12 d 15 11 d 16 10 d 16 10 d 16
|
||||
10 d 16 10 d 15 10 d 16 10 d 16 9 d 16 10 d 16 10 d 16 10 d 15 10 d 16 10 d 16 9 d 16 10 d 16 10 d 15 10 d 16 10 d 16 9 d 16 10 d 16 10 d 15 10 d 16 10 d 16 9 d 16 10 d 16 10 d 15 10 d 16 10 d 16 10 d 16 9 d 16 10 d 16 10 d 15 10 d 16 10 d 16 9 d
|
||||
16 10 d 16 10 d 15 10 d s 1897 1350 m 16 10 d s[ 12 12] 0 sd 3 lw 1140 330 m 284 Y s[ ] 0 sd 1140 614 m20[ 12 12] 0 sd[ ] 0 sd 1 1 1 c black 516 331 521 331 526 331 531 331 537 332 542 332 547 334 552 334 557 335 562 336 568 339 573 341 578 343
|
||||
583 347 588 351 594 356 599 361 604 367 609 374 614 383 619 391 625 400 630 411 635 423 640 439 645 450 650 465 656 482 661 498 666 516 671 537 676 550 681 569 687 591 692 608 697 628 702 645 707 663 712 681 718 698 723 711 728 727 733 743 738 757
|
||||
743 769 749 784 754 795 759 807 764 817 769 826 50 { m28} R 769 826 774 837 780 843 785 854 790 863 795 870 800 875 805 881 811 887 816 896 821 903 826 903 831 912 837 914 842 920 847 924 852 928 857 933 862 936 868 941 873 946 878 948 883 952 888
|
||||
956 893 961 899 964 904 968 909 970 914 972 919 973 924 977 930 981 935 987 940 992 945 994 950 998 955 999 961 1002 966 1004 971 1009 976 1008 981 1009 986 1012 992 1016 997 1020 1002 1025 1007 1029 1012 1034 1017 1035 1023 1037 50 { m28} R 1023
|
||||
1037 1028 1037 1033 1044 1038 1042 1043 1048 1048 1057 1054 1060 1059 1064 1064 1068 1069 1067 1074 1066 1080 1067 1085 1071 1090 1071 1095 1073 1100 1074 1105 1079 1111 1080 1116 1080 1121 1085 1126 1087 1131 1092 1136 1094 1142 1095 1147 1098
|
||||
1152 1099 1157 1100 1162 1106 1167 1106 1173 1111 1178 1111 1183 1115 1188 1117 1193 1119 1198 1119 1204 1120 1209 1122 1214 1122 1219 1128 1224 1128 1229 1128 1235 1132 1240 1136 1245 1140 1250 1142 1255 1142 1260 1148 1266 1149 1271 1151 1276
|
||||
1149 50 { m28} R 1276 1149 1281 1154 1286 1154 1292 1153 1297 1160 1302 1159 1307 1162 1312 1163 1317 1164 1323 1169 1328 1168 1333 1170 1338 1175 1343 1174 1348 1180 1354 1178 1359 1178 1364 1179 1369 1181 1374 1183 1379 1186 1385 1189 1390 1190
|
||||
1395 1197 1400 1199 1405 1201 1410 1201 1416 1200 1421 1202 1426 1207 1431 1207 1436 1212 1441 1212 1447 1210 1452 1213 1457 1217 1462 1217 1467 1222 1472 1224 1478 1226 1483 1229 1488 1234 1493 1232 1498 1234 1503 1233 1509 1237 1514 1239 1519
|
||||
1240 1524 1242 1529 1245 50 { m28} R 1529 1245 1535 1250 1540 1253 1545 1255 1550 1261 1555 1266 1560 1267 1566 1270 1571 1272 1576 1276 1581 1275 1586 1276 1591 1276 1597 1279 1602 1283 1607 1282 1612 1286 1617 1292 1622 1295 1628 1295 1633 1296
|
||||
1638 1297 1643 1297 1648 1292 1653 1297 1659 1296 1664 1303 1669 1304 1674 1303 1679 1304 1684 1302 1690 1308 1695 1307 1700 1313 1705 1320 1710 1320 1715 1314 1721 1313 1726 1322 1731 1328 1736 1329 1741 1338 1747 1338 1752 1340 1757 1341 1762
|
||||
1341 1767 1343 1772 1343 1778 1343 1783 1347 50 { m28} R 1783 1347 1788 1355 1793 1354 1798 1365 1803 1362 1809 1370 1814 1372 1819 1367 1824 1376 1829 1377 1834 1382 1840 1379 1845 1384 1850 1386 1855 1386 1860 1392 1865 1399 1871 1399 1876 1400
|
||||
1881 1403 1886 1407 1891 1411 1896 1416 1902 1416 1907 1419 1912 1425 1917 1429 1922 1431 1927 1437 1933 1440 1938 1442 1943 1441 1948 1446 1953 1447 1958 1448 1964 1457 1969 1464 1974 1470 1979 1483 1984 1493 1990 1507 1995 1520 2000 1537 2005
|
||||
1565 2010 1602 2015 1665 2021 1761 2026 1901 2031 2089 49 { m28} R 2150 2089 m28 9 lw 0.95 0.95 0.95 c black 348 330 m 155 X 16 1 d 16 1 d 15 3 d 16 5 d 15 8 d 16 12 d 15 19 d 16 26 d 15 35 d 16 44 d 15 51 d 16 56 d 16 59 d 15 57 d 16 53 d 15 46 d
|
||||
16 39 d 15 31 d 16 24 d 15 18 d 16 14 d 16 11 d 15 9 d 16 8 d 15 7 d 16 8 d 15 7 d 16 7 d 15 6 d 16 7 d 15 7 d 16 7 d 16 7 d 15 7 d 16 7 d 15 7 d 16 7 d 15 6 d 16 7 d s 1110 1064 m 15 7 d 16 7 d 16 7 d 15 7 d 16 7 d 15 7 d 16 7 d 15 7 d 16 6 d 15 7
|
||||
d 16 7 d 15 7 d 16 7 d 16 7 d 15 7 d 16 7 d 15 7 d 16 6 d 15 7 d 16 7 d 15 7 d 16 7 d 16 7 d 15 7 d 16 7 d 15 7 d 16 6 d 15 7 d 16 7 d 15 7 d 16 7 d 15 7 d 16 7 d 16 7 d 15 7 d 16 7 d 15 6 d 16 7 d 15 7 d 16 7 d 15 7 d 16 7 d 16 7 d 15 7 d 16 7 d
|
||||
15 6 d 16 7 d 15 7 d 16 7 d s 1872 1402 m 15 7 d s[ 12 12] 0 sd 3 lw 693 330 m 278 Y s[ ] 0 sd 693 608 m20[ 12 12] 0 sd[ ] 0 sd 6 lw 1 1 1 c 1088 725 386 1320 bf black 3 lw 1 1 1 c 947 631 516 1407 bf black 947 631 516 1407 bl 1 1 1 c 947 631 516
|
||||
1407 bf black 947 631 516 1407 bl 6 lw 516 1407 m 947 X s
|
||||
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|
||||
1416 m -9 Y s 750 1426 m -19 Y s 779 1416 m -9 Y s 807 1416 m -9 Y s 835 1416 m -9 Y s 863 1426 m -19 Y s 891 1416 m -9 Y s 920 1416 m -9 Y s 948 1416 m -9 Y s 976 1426 m -19 Y s 1004 1416 m -9 Y s 1032 1416 m -9 Y s 1061 1416 m -9 Y s 1089 1426 m
|
||||
-19 Y s 1117 1416 m -9 Y s 1145 1416 m -9 Y s 1173 1416 m -9 Y s 1202 1426 m -19 Y s 1230 1416 m -9 Y s 1258 1416 m -9 Y s 1286 1416 m -9 Y s 1314 1426 m -19 Y s 1343 1416 m -9 Y s 1371 1416 m -9 Y s 1399 1416 m -9 Y s 1427 1426 m -19 Y s 525 1426
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|
||||
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|
||||
gsave 1088 725 386 1320 C 467 1812 t 0 r /Helvetica-Bold findfont 25.7167 sf 0 0 m (600) show NC gr
|
||||
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|
||||
-4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 8 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 8 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4
|
||||
d 7 -4 d 8 -4 d 7 -4 d 7 -4 d 7 -4 d s 1015 1660 m 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 8 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 8 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7
|
||||
-4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 8 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d 7 -4 d s 1361 1464 m 7 -4 d s 6 lw 1 1 1 c 454 440 1587 440 bf black
|
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|
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|
||||
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|
||||
gr gr
|
||||
showpage
|
||||
end
|
||||
%%EOF
|
18
manual/manual-calwiz/installation.tex
Normal file
@ -0,0 +1,18 @@
|
||||
The calibration wizards are based on the \textit{Root} software developed at CERN.\\
|
||||
To install it, simply download it from the url \textit{http://root.cern.ch}.\\
|
||||
You can either download the binaries for your system or install from source (which is time consuming, but possibly more stable).\\
|
||||
The development and debugging of the wizards have been done using the root version 5.20, but it should be working also with newer versions.
|
||||
|
||||
After installing the root software, edit your .bashrc file to define the ROOTSYS enviroment variable, and add the binaries and libraries to your path, e.g.:
|
||||
\begin{verbatim}
|
||||
export ROOTSYS=/usr/local/root_sl5_32bit
|
||||
export LD_LIBRARY_PATH=$ROOTSYS/lib:$LD_LIBRARY_PATH
|
||||
export PATH=$ROOTSYS/bin:$PATH
|
||||
\end{verbatim}
|
||||
|
||||
Then enter the calibrationWizards directory and compile:
|
||||
\begin{verbatim}
|
||||
make clean && make
|
||||
\end{verbatim}
|
||||
|
||||
The two executables \textit{energyCalibrationWizard} and \textit{angularCalibrationWizard} should be generated, together with some documentation in pdf format inside the \textit{manual} directory.
|
69497
manual/manual-calwiz/peakFit.eps
Normal file
BIN
manual/manual-calwiz/peakFit.png
Normal file
After Width: | Height: | Size: 64 KiB |
59330
manual/manual-calwiz/position_scan.eps
Normal file
BIN
manual/manual-calwiz/position_scan.png
Normal file
After Width: | Height: | Size: 69 KiB |
69497
manual/manual-calwiz/setupAngcal.eps
Normal file
BIN
manual/manual-calwiz/setupAngcal.png
Normal file
After Width: | Height: | Size: 264 KiB |
135
manual/manual-calwiz/spectrum_expl.eps
Normal file
@ -0,0 +1,135 @@
|
||||
%!PS-Adobe-2.0 EPSF-2.0
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||||
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||||
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|
||||
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|
||||
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|
||||
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||||
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||||
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|
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|
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79 /greaterequal 80 /braceleft 81 /braceright 82 /radical
|
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|
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88 /multiply 89 /percent 90 /infinity 48 /circlemultiply 49 /circleplus
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|
||||
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|
||||
103 /union 104 /propersuperset 105 /reflexsuperset 106 /notsubset 107 /propersubset 108 /reflexsubset 109 /element 110 /notelement 111 /gradient 112 /logicaland 113 /logicalor 114 /arrowdblboth 115 /arrowdblleft 116 /arrowdblup 117 /arrowdblright
|
||||
118 /arrowdbldown 119 /ampersand 120 /omega1 121 /similar 122 /aleph ] def
|
||||
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||||
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|
||||
/stwn { /fs exch def /fn exch def /text exch def fn findfont fs sf
|
||||
text sw pop xs add /xs exch def} def
|
||||
/stwb { /fs exch def /fn exch def /nbas exch def /textf exch deftextf length /tlen exch def nbas tlen gt {/nbas tlendef} iffn findfont fs sf textf dup length nbas sub nbas getinterval sw
|
||||
pop neg xs add /xs exch def} def
|
||||
%%EndProlog
|
||||
%%BeginSetup
|
||||
%%EndSetup
|
||||
newpath gsave .25 .25 scale gsave 0 0 t black[ ] 0 sd 3 lw 1 1 1 c 2268 2199 0 0 bf black 1 1 1 c 1814 1761 345 330 bf black 1814 1761 345 330 bl 1 1 1 c 1814 1761 345 330 bf black 1814 1761 345 330 bl 9 lw 0.95 0.95 0.95 c black 354 1681 m 18
|
||||
-4 d 18 -3 d 18 -3 d 18 -4 d 19 -3 d 18 -4 d 18 -3 d 18 -4 d 18 -3 d 18 -3 d 18 -4 d 19 -3 d 18 -4 d 18 -3 d 18 -4 d 18 -3 d 18 -3 d 18 -4 d 19 -3 d 18 -4 d 18 -3 d 18 -4 d 18 -3 d 18 -3 d 18 -4 d 19 -3 d 18 -4 d 18 -3 d 18 -4 d 18 -4 d 18 -4 d 19
|
||||
-5 d 18 -8 d 18 -10 d 18 -14 d 18 -19 d 18 -24 d 18 -30 d 19 -33 d 18 -34 d 18 -32 d 18 -29 d 18 -24 d 18 -18 d 18 -13 d 19 -9 d 18 -6 d 18 -5 d 18 -3 d s 1243 1257 m 18 -3 d 18 -3 d 18 -3 d 19 -2 d 18 -3 d 18 -3 d 18 -4 d 18 -4 d 18 -7 d 18 -10 d
|
||||
19 -18 d 18 -29 d 18 -43 d 18 -60 d 18 -79 d 18 -94 d 19 -104 d 18 -104 d 18 -97 d 18 -82 d 18 -63 d 18 -46 d 18 -29 d 19 -18 d 18 -10 d 18 -5 d 18 -2 d 18 -1 d 18 X 18 -1 d 345 X s 2132 330 m 18 X s 3 lw 345 330 m 1814 X s
|
||||
gsave 2268 2199 0 0 C 1658 162 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (Energy \(keV\)) show NC gr 345 383 m -53 Y s 405 357 m -27 Y s 466 357 m -27 Y s 526 357 m -27 Y s 587 357 m -27 Y s 647 383 m -53 Y s 708 357 m -27 Y s 768 357 m -27
|
||||
Y s 829 357 m -27 Y s 889 357 m -27 Y s 950 383 m -53 Y s 1010 357 m -27 Y s 1071 357 m -27 Y s 1131 357 m -27 Y s 1192 357 m -27 Y s 1252 383 m -53 Y s 1313 357 m -27 Y s 1373 357 m -27 Y s 1434 357 m -27 Y s 1494 357 m -27 Y s 1555 383 m -53 Y s
|
||||
1615 357 m -27 Y s 1676 357 m -27 Y s 1736 357 m -27 Y s 1797 357 m -27 Y s 1857 383 m -53 Y s 1917 357 m -27 Y s 1978 357 m -27 Y s 2038 357 m -27 Y s 2099 357 m -27 Y s 2159 383 m -53 Y s
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||||
gsave 2268 2199 0 0 C 322 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (0) show NC gr
|
||||
gsave 2268 2199 0 0 C 624 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (5) show NC gr
|
||||
gsave 2268 2199 0 0 C 903 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (10) show NC gr
|
||||
gsave 2268 2199 0 0 C 1205 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (15) show NC gr
|
||||
gsave 2268 2199 0 0 C 1507 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (20) show NC gr
|
||||
gsave 2268 2199 0 0 C 1809 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (25) show NC gr
|
||||
gsave 2268 2199 0 0 C 2114 251 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (30) show NC gr 345 330 m 1761 Y s
|
||||
gsave 2268 2199 0 0 C 105 1809 t 90 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (Counts) show NC gr 399 330 m -54 X s 372 374 m -27 X s 372 419 m -27 X s 372 463 m -27 X s 399 507 m -54 X s 372 551 m -27 X s 372 595 m -27 X s 372 639 m -27 X s
|
||||
399 683 m -54 X s 372 727 m -27 X s 372 771 m -27 X s 372 815 m -27 X s 399 859 m -54 X s 372 903 m -27 X s 372 947 m -27 X s 372 991 m -27 X s 399 1035 m -54 X s 372 1079 m -27 X s 372 1123 m -27 X s 372 1167 m -27 X s 399 1211 m -54 X s 372 1255
|
||||
m -27 X s 372 1299 m -27 X s 372 1343 m -27 X s 399 1387 m -54 X s 372 1431 m -27 X s 372 1475 m -27 X s 372 1519 m -27 X s 399 1563 m -54 X s 372 1607 m -27 X s 372 1651 m -27 X s 372 1695 m -27 X s 399 1739 m -54 X s 372 1783 m -27 X s 372 1827 m
|
||||
-27 X s 372 1871 m -27 X s 399 1915 m -54 X s 372 1959 m -27 X s 372 2003 m -27 X s 372 2047 m -27 X s 399 2091 m -54 X s
|
||||
gsave 2268 2199 0 0 C 291 293 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (0) show NC gr
|
||||
gsave 2268 2199 0 0 C 151 470 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (2000) show NC gr
|
||||
gsave 2268 2199 0 0 C 151 647 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (4000) show NC gr
|
||||
gsave 2268 2199 0 0 C 151 823 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (6000) show NC gr
|
||||
gsave 2268 2199 0 0 C 151 1000 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (8000) show NC gr
|
||||
gsave 2268 2199 0 0 C 105 1174 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (10000) show NC gr
|
||||
gsave 2268 2199 0 0 C 105 1350 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (12000) show NC gr
|
||||
gsave 2268 2199 0 0 C 105 1527 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (14000) show NC gr
|
||||
gsave 2268 2199 0 0 C 105 1704 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (16000) show NC gr
|
||||
gsave 2268 2199 0 0 C 105 1880 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (18000) show NC gr
|
||||
gsave 2268 2199 0 0 C 105 2054 t 0 r /Helvetica-Bold findfont 82.6178 sf 0 0 m (20000) show NC gr [ 12 12] 0 sd 6 lw 1555 330 m 441 Y s 1071 330 m 1083 Y s[ 4 8] 0 sd 1313 330 m 916 Y s
|
||||
gsave 2268 2199 0 0 C 1624 752 t 0 r /Helvetica-Bold findfont 68.3734 sf 0 0 m (0) show NC gr
|
||||
gsave 2268 2199 0 0 C 1558 781 t 0 r /Helvetica-Bold findfont 102.56 sf 0 0 m (E) show NC gr
|
||||
gsave 2268 2199 0 0 C 1140 1396 t 0 r /Helvetica-Bold findfont 68.3734 sf 0 0 m (f) show NC gr
|
||||
gsave 2268 2199 0 0 C 1074 1424 t 0 r /Helvetica-Bold findfont 102.56 sf 0 0 m (E) show NC gr
|
||||
gsave 2268 2199 0 0 C 1336 1262 t 0 r /Helvetica-Bold findfont 68.3734 sf 0 0 m (t) show NC gr
|
||||
gsave 2268 2199 0 0 C 1271 1291 t 0 r /Helvetica-Bold findfont 102.56 sf 0 0 m (E) show NC gr [ ] 0 sd 1071 595 m 242 X s 1281 613 m 32 -18 d -32 -19 d s 1102 576 m -31 19 d 31 18 d s 1313 595 m 242 X s 1523 613 m 32 -18 d -32 -19 d s 1344 576 m
|
||||
-31 19 d 31 18 d s
|
||||
gsave 2268 2199 0 0 C 1159 613 t 0 r /Symbol findfont 102.56 sf 0 0 m (S) show NC gr
|
||||
gsave 2268 2199 0 0 C 1402 613 t 0 r /Symbol findfont 102.56 sf 0 0 m (S) show NC gr
|
||||
gr gr
|
||||
showpage
|
||||
end
|
||||
%%EOF
|