How to extract PN spectra of a point-like source and associated matrices using the SAS GUI

Introduction This thread describes how to extract the spectrum of a point-like source observed with the PN cameras using the SAS Graphical User Interface (GUI) Expected Outcome The final outcome of this thread is the standard suite of spectral products required by spectral analysis packages such as XSPEC: A source+background (commonly referred to as "source") spectrum A background spectrum A redistribution matrix (commonly referred to as a "RMF" file) An effective area vector (commonly referred to as an "ARF" file) SAS Tasks to be Used arfgen backscale rmfgen specgroup xmmselect Prerequisites SAS Startup Thread How to reprocess ODFs to generate calibrated and concatenated EPIC event lists Thread Useful Links This thread makes use of the image display software ds9. Caveats

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Procedure

This thread contains a step-by-step recipe to extract PN spectra of a point-like source observed in Imaging mode and to create the associated response matrices, starting from a calibrated, concatenated event list (either produced with epproc or available as PPS product; here it bears the file name PN.evt). The content of this thread is the same as the thread to extract pn spectra for point-like sources (command-line version). Here, however, the extraction of scientific products is being done using the SAS task xmmselect. This is a user-friendly, graphical interface to the SAS extractor (evselect), which allows you to create a wide range of scientific products (images and pseudo-images, time series, spectra, histograms), and screen the data prior to any product accumulations. xmmselect takes advantage of the full integration between SAS and plotting tools such as grace and ds9, to define data selection regions on a 1-D (light curve) or 2-D (image) plane.

1. Set up your SAS environment (following the SAS startup Thread)
2. If necessary, create a PN cleaned and filtered for particle background event file for your observation (see the How to filter EPIC event lists for flaring particle background Thread). Lets assume that a filtered file has been created, with name: PNclean.fits
3. Start xmmselect
   
    xmmselect table=PNclean.fits &
   
   First a window pops-up, asking if you wish to visualise the "[...] selection expression [...]" corresponding to "[...] data subspace information [...]". In practise, xmmselect is asking you if you wish to see the data screening expression, which was employed to generate the event list. The answer to this question does not affect the following steps.
   
   The xmmselect call pops-up a window as shown in Fig.1.
   
   
   
   Fig.1: The main xmmselect window
   
   In this window, we identify:
   • a data screening widget (top)
   • a data column panel (middle)
   • the buttons 1D region and 2D region, which allow to translate selection expression defined in a grace or ds9 window, respectively, into proper selectlib expressions
   • "action" buttons (bottom)
4. Extract an image (sky coordinates in this example; extraction in detector - DET[XY] - coordinates is possible as well, and may be preferable for some specific scientific needs).
This is accomplished by:


• in the data screening widget:
  
  • use #XMMEA_EP && (FLAG==0)
  • use (PATTERN<=4)
  • use (PI in [300:10000])
• clicking the square check-box besides X and Y in the data column xmmselect panel
• click on Image
• go to the Image sub-panel in the evselect window (see Fig.5)
• change at least the file name in the imageset window (e.g. to PNimage.fits)
• click Run




Fig.5: The Image panel in the evselect window

xmmselect will automatically launch a ds9 window on the created image


5. Select the region, from which the spectrum shall be accumulated, using the Regions/Shape/Circle in ds9 (see Fig.6)
   
   
   
   Fig.6: ds9 main window. A circular region (green circle) has been defined using the highlighted menu.


6. Propagate the selected region into the xmmselect data screening panel, by clicking the 2D region button


7. Extract a source spectrum, using all the selection expressions defined so far, and restricting the patterns to single and doubles:
   
   
   • click the radio button close to PI in the data column xmmselect panel
   • click OGIP Spectrum
   • go to the Spectrum sub-panel in the evselect window (see Fig.7)
   • define the binning parameters:
     • withspectrumset active
     • spectrumset=PNsource_spectrum.fits
     • spectralbinsize=5
     • withspecranges active
     • specchannelmin=0
     • specchannelmax=20479
   • click Run
   
   
   
   
   Fig.7: The Spectrum panel in the evselect window


8. Extract a background spectrum using the same steps 5. to 7. above. Have a look at the "EPIC status of calibration and data analysis" document (XMM-SOC-CAL-TN-0018) for latest recommendations on how to select source and background regions. In the following, we assume that the background is extracted from a source-free region at the same distance to the readout node (RAWY position) as the source region. So if your source is at line 150 on CCD 4, you should aim to select background from around line 150 on a neighbouring CCD to ensure similar low-energy noise.
   
   If you are interested in learning how to extract the background spectra from blank fields event lists, please click here.
   From now onwards one does not need to use xmmselect any longer.


9. If you want to correct the source spectrum for Out-of-Time events, consult the Dealing with EPIC Out-of-Time (OoT) events Thread.


10. Generate a redistribution matrix
    
    Currently there are two possible approaches:
    
    a) use the SAS task rmfgen to create a redistribution matrix for your previously extracted spectrum:
    
    
    • rmfgen -d. The GUI launch interface will appear (see Fig.8)
    • define the following quantities:
      
      • spectrumset=PNsource_spectrum.fits
      • rmfset=PN.rmf
    
    NOTE: This can take long (>30 min) on low performance computers...
    
    
    
    Fig.8: The rmfgen launch GUI interface
    
    b) use the ready-made (canned) matrices available at the following URL: http://xmm2.esac.esa.int/external/xmm_sw_cal/calib/epic_files.shtml


11. Generate an ancillary file (for extended sources use extendedsource=yes detmaptype=flat or dataset)
    
    NOTE: arfgen reads in the pattern range from the DSS information in the spectrum dataset, and accumulates the quantum efficiency curves over those patterns, which is then combined to the other constituents of the ARF. Be aware that the entire range of allowed patterns are assumed if no pattern range is found in the DSS.
    
    
    • launch the arfgen GUI interface (see Fig.9)
      
       arfgen -d
      
      
    • define the following parameters
      
      • spectrumset=PNsource_spectrum.fits
      • arfset=PN.arf
      • withrmfset=yes (on calibration panel)
      • rmfset=PN.rmf (on calibration panel)
      • badpixlocation=PNclean.fits (on effects panel)
      • detmaptype=psf (on detector map panel)
    
    
    
    
    Fig.9: The arfgen launch GUI interface


12. Rebin the spectrum and link associated files. In the following example the spectrum is rebinned in order to have at least 25 counts for each background-subtracted spectral channel and not to oversample the intrinsic energy resolution by a factor larger then 3.
    
      specgroup spectrumset=PNsource_spectrum.fits mincounts=25 oversample=3 rmfset=PN.rmf \
        arfset=PN.arf backgndset=PNbackground_spectrum.fits
13. Fit the spectrum

Last Updated: 16 April 2010

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Caveats For bright sources and sources with narrow lines it might be better to extract two spectra and corresponding backgrounds, response and ancillary files: one set for single pixel events (PATTERN==0) and another set for doubles (PATTERN IN [1:4]). Fitting these two spectra simultaneously will show if there are any problems with pile-up (see also SAS thread on "How to evaluate the pile-up fraction") and - as the energy calibration for singles is slightly better than the one for doubles - will show the line features at highest energy resolution in the single events spectra. However, in case of PN Timing mode observations (where the rate of single to double events depends on the source position) one should always create and fit a spectrum of the combined single and double events. For details on the spectral analysis of data obtained in Timing and Burst mode, see again XMM-SOC-CAL-TN-0018.