XMM-Newton Science Analysis System


emldetect (emldetect-6.0.2) [xmmsas_20141104_1833-14.0.0]

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Description

For an input list of eboxdetect source locations, simultaneous maximum likelihood PSF fits to the source count distribution are performed in all energy bands of each EPIC instrument. A description of the main properties of the detection algorithm may be found in Cruddace, Hasinger, Schmitt (1988) and an overview of emldetect and its use in the XMM-Newton catalogue pipelines at http://xmmssc-www.star.le.ac.uk/Catalogue/2XMM/UserGuide_xmmcat.html#EmldetFit.

Fit parameters. Main free fit parameters are: the source location (image coordinates X_IMA, Y_IMA), source extent (Gaussian sigma or beta model core radius), and source count rates in each energy band for each telescope. The source location and source extent are constrained to the same best-fit value in all energy bands per EPIC instrument whereas the source count rates are adjusted to their individual best-fit value in each energy band per EPIC instrument. Derived parameters are: total source count rate, likelihood of detection (total and in each energy band), likelihood of source extent, and up to four hardness ratios (default: four).

Output source table. A summary of all the columns in the output source list can be found in Table 2 in Section 8 on the output files. For each detected source, the table contains one row for each energy band for each instrument. The individual source rows are identified through the column entries ID_INST and ID_BAND in the output table. ID_INST refers to the EPIC instrument ($1$: PN, $2$: MOS1, $3$: MOS2, $0$: summary row). ID_BAND is the energy band number as defined by the ordering of the energy bands, i.e.: the ordering of the input images given as command-line arguments to emldetect. The upper and lower bounds of each energy band are available in the header keywords aa_n_ELO and aa_n_EHI where aa stands for the EPIC camera (PN, M1, or M2) and n stands for the energy band number as given in the table column ID_BAND. Additional keywords N_INST and aa_BNDS specify the number of EPIC cameras and the number of energy bands for each EPIC camera. For the definition of the basic energy bands used in the pipeline processing, see
http://xmmssc-www.star.le.ac.uk/Catalogue/3XMM-DR4/UserGuide_xmmcat.html#TabBands.
An ID_BAND value of $0$ refers to the summary rows of each source, which list combined results per instrument and in total. The summary rows over the energy bands for each instrument contain sums of the entries in the individual energy bands where appropriate (counts, count rates, fluxes, and detection likelihoods). In the total summary row per source with ID_INST=0, those spatial parameters are repeated that are identical for all energy bands (positions and extent values). The other columns are set to NULL.

XID band. The XID energy band (0.5 - 4.5 keV) of the X-ray Follow-up & Identification Programme is marked by ID_BAND=9 and will be present if the input parameter withxidband has been set to true. The keyword XID_BND indicates whether XID band information is present in the source table. Note that the energy bands which constitute the XID band have to be specified for each instrument separately using the parameters xidpndef, xidm1def, xidm2def. Default values are the input bands $2$, $3$, and $4$, as defined in ID_BAND column.

From v4.42.5 on, an alternative method to treat the XID band has been introduced: With the parameter xidfixed set, emldetect can be run on one XID band image per instrument using an emldetect output list as input source list. Positions and source extent values will be kept fixed, and only fluxes and detection likelihoods are determined. In this case, the input images (science images, exposure maps, background images) for the desired band (e.g. 0.5 - 4.5 keV) have to be prepared beforehand. The parameters xidpndef, xidm1def, xidm2def determine which energy bands from the input source list are used to provide the start values for the fit. Note that when using this method, the parameter withxidband should be set to ``no'', and the parameter ecf is used to set the energy conversion factors (http://xmmssc-www.star.le.ac.uk/Catalogue/3XMM-DR4/UserGuide_xmmcat.html#TabNewECFs).

PSF fitting. Simultaneous fitting of data from different instruments (i.e., EPIC pn and MOS data) or different exposures is supported. The PSF fitting may either be performed in single-source or in multi-source mode. In multi-source mode, neighbouring sources with overlapping PSFs are fitted simultaneously. Detection likelihoods are optimized for all the overlapping sources simultaneously, and detection likelihoods per source are calculated and written to the column DET_ML of the output source table. Selection of sources for simultaneous fitting is controlled by the distance parameter scut and by the parameter nmaxfit that gives the maximum number of sources to be fit simultaneously ($1 \leq$ nmaxfit $\leq 10$). Sources fit simultaneously are identified in the output table through the ID_CLUSTER table column. It is also possible to fit several PSFs for each input source position by setting the parameter nmulsou to the corresponding value ($1 \leq$ nmulsou $\leq 3$, nmaxfit$*$nmulsou $\leq 10$).

Two parameters determine the image region on which a source fit is performed: The parameter ecut determines the size of the subimage around each source used for fitting. The parameter scut determines the radius around each source, in which other input sources are considered for multi-PSF fitting, if the parameter nmulsou is $>1$. Both ecut and scut are given as encircled energy fractions of the calibration PSF. The actual radii in pixel units therefore change slightly with energy band and source position. Alternatively, ecut and scut can be given as a fixed value in units of image pixels (if ecut or scut is $>1$). The actual value for the cutout radius of each source is listed in the column CUTRAD of the output source list.

Starting with SAS 10.0 and emldetect version 5.1, a full 2d parametrization of the EPIC PSF as a function of instrument, energy, and off-axis angle is introduced (Release Notes). The PSF model can be chosen via the parameter psfmodel. Up to version 5.17.1, the medium-accuracy PSF (psfmodel=medium) is used by default. The analytical 2d PSF (psfmodel=ellbeta) is the default PSF model from version 5.17.2 on. The slew-mode PSF for EPIC/pn (psfmodel=slew) has been introduced with emldetect-6.0 and cal-3.231.

Extent fitting. If the parameter fitextent is set to ``yes'', the point spread function will be convolved with a source extent model, that can be set to either a Gaussian profile or a $\beta$-model profile via the parameter extentmodel. In the case of extentmodel=beta, the surface brightness is calculated as

$$f(x,y)=\left(1+\frac{(x-x_0)^2+(y-y_0)^2}{r_c^2}\right)^{-3/2}$$

The value of the core radius $r_c$ is written to the column EXT of the output source list. In the case of a Gaussian extent model, $\sigma$ is written to the column EXT, instead. Note that the source extent can only be determined reliably for relatively bright objects. If the likelihood of the source extent falls below the threshold given via dmlextmin (default: $10.0$), point source parameters are derived.

From version 4.27 on, the extent likelihood values (EXT_ML) are corrected for the number of input images with the formalism described below in the paragraph on Detection likelihoods.

From version 4.32 on, the maximum value of the extent fit parameter can be given via the task parameter maxextent. The unit is image pixels. Large values of maxextent can lead to spurious detection of extended sources in some cases. With the parameter minextent, the minimum extent can be specified that is still considered to be significant. If the best fit extent is less than minextent, a point source model will be adopted for the source.

CPU saving. Since both multi-PSF fitting and extent fitting are CPU intensive, two methods exist to reduce the CPU requirements of an emldetect run using multi-PSF fitting. With the option withthreshold, the user can limit the application of multi-PSF fitting (as specified by nmulsou) to sources exceeding a certain threshold. The threshold is set by the parameter threshold. The corresponding input column is defined via the parameter threshcolumn, which can be LIKE, SCTS, or RATE.

The second method to save CPU time for combined extent and multi-PSF fitting is provided by the option withtwostage, which is used in combination with fitextent=''true'' and nmulsou $>1$. If withtwostage is set to ``true'', emldetect will perform the fit for each source in two stages: In the first stage, one extended source is fitted to the source. Only if the extent is significant, the second stage will be performed, and a multi-PSF fit with one extended source and nmulsou - 1 point sources is applied. The withtwostage option avoids misidentification of close pairs of point sources as extended sources in most cases and significantly reduces CPU time.

Detection likelihoods. All detection likelihoods are transformed to equivalent likelihoods $L_2$ (column DET_ML of the output source table), corresponding to the case of two free parameters to allow comparison between detection runs with different numbers of free parameters (i.e., when different numbers of input images are used):

$$L_2 = -\ln (1-P(\frac{\nu}{2},L')) \;\;\; {\rm with} \;\;\; L' = \sum_{i=1}^n L_i$$

where $P$ is the incomplete Gamma function, $n$ is the number of energy bands involved, $\nu$ is the number of degrees of freedom of the fit ($\nu = 3+n$ if task parameter fitextent=yes, and $\nu = 2+n$ otherwise), and $L_i = C_i/2$ with $C$ as defined by Cash (1979). Note that $n$ is 1 for the individual energy-band detection likelihoods that are listed in source table rows with ID_BAND $>$ 0, and $n$ is equal to the total number of energy bands in the ID_BAND=0 summary rows. The equivalent detection likelihoods obey the simple relationship $L_2 = - \ln(p)$, where $p$ is the probability for a random Poissonian fluctuation to have caused the observed source counts. This is in agreement with the equivalent detection likelihoods as defined in task eboxdetect (column SIGMA of eboxdetect source lists). Note that for very small numbers of source counts (less than $\approx 9$ counts, Cash 1979), this relation has to be treated with caution. Therefore, it will only give a rough estimate of the number of expected spurious sources.

OOT correction. All EPIC PN source count rates and fluxes written to the emldetect source list are corrected for photons that arrive during readout of the PN CCDs and therefore are not detected on the nominal source position (out-of-time events).
emldetect v4.5 to 4.27: Correction factors of 1.0626 for PrimeFullWindow mode and of 1.0223 for the PrimeFullWindowExtended mode are applied by emldetect. Data taken in other observing modes are left uncorrected.
emldetect v4.28 onwards: From eexpmap v3.31 on, the OOT events correction is applied to the exposure maps in all observing modes. emldetect reads the keyword OOTCORR from the FITS header of the exposure maps. If OOTCORR is existing and set to ``true'', no further correction is applied by emldetect.

Table 1: Default band assignments of hardness ratios HRi for the EPIC instruments and default energy intervals during pipeline processing (cf. 3XMM-DR4 catalogue description).

$i$	$n$	$m$	Pipeline energy bands [keV]
1	1	2	0.2 - 0.5        0.5 - 1.0
2	2	3	0.5 - 1.0        1.0 - 2.0
3	3	4	1.0 - 2.0        2.0 - 4.5
4	4	5	2.0 - 4.5        4.5 - 12.0

Hardness ratios. If detection over several energy bands is performed, up to four hardness ratios HRi are calculated from the source count rates in the individual bands (default: four). The hardness ratios are defined as follows:

$$\index{Columns!HR{\it i}}{\tt HR{\it i}} = \frac{B_m - B_n}{B_m + B_n}$$

where $B$ denotes the count rates in energy bands $n$ and $m$, respectively. The energy bands $n$ and $m$ used to calculate the hardness ratios can be specified for each instrument via the parameters hrpndef, hrm1def, and hrm2def. The default band assignments (identical for all instruments) are given in Table 1. The band numbers $n$ and $m$ are assigned to the individual bands by numbering the corresponding input images in the order in which they are given on the command line. It is therefore important that the ordering of the input images is consistent with the contents of hrdef to obtain meaningful hardness ratios.

Position errors. The final stage of the source detection process is done via ML-fitting of the PSF-shape at the given detector position to the observed photon distribution utilizing the $C$-statistics. The best fitting X-ray position is determined at the minimum value of $C$, and the $1\sigma$ errors in right ascension and declination are derived at $C=C_\mathrm{min}+1$. The two-dimensional positional error RADEC_ERR, written to the output source list, is calculated as square root of the quadratic sum of the errors in R.A. and Dec. It translates into a one-dimensional $\sigma=$RADEC_ERR$/\sqrt{2}$, if symmetric errors in R.A. and Dec are assumed. Individual position errors in image coordinates can be accessed via the X_IMA_ERR and Y_IMA_ERR columns in the output source list.

Mosaic images. From version 5.0 onward, the parameter imagebuffersize is implemented. The main purpose of this parameter is to make the processing of mosaic-pointings more efficient, where the mosaicked sky image will contain large areas without photon data. The value of imagebuffersize characterizes the memory that is allocated for each individual image and is given in image pixels: imagebuffersize is (at least) the size of the sub-image per pointing that contains non-zero pixels (Fig. 1). Its default is $640$, which is the side length of a typical pipeline-produced EPIC image with a bin size of $4$arcsec.

Figure 1: Use of parameter imagebuffersize.