The XMM-Newton Serendipitous Source Catalogue:
4XMM-DR13The XMM-Newton Serendipitous Source Catalogue:
4XMM-DR13| Release 1.40 | 12th June 2023 | Associated with Catalogue version 1.0 |
Prepared by the XMM-Newton Survey Science Centre Consortium |
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This User Guide refers directly to the full FITS and plain-text formats of the catalogue. Users interested in the details of changes to the data processing since the 4XMM-DR12 catalogue release, can refer directly to section 3. Information about the columns contained in the 4XMM-DR13 catalogue are presented in section 4. Brief summaries of some elements of the 4XMM-DR13 catalogue properties are provided in section 5 but a comprehensive evaluation of the catalogue is in Webb et al., (2020).
Should you use the catalogues 4XMM-DR13 or 4XMM-DR13s for your research and publish the results, please use the acknowledgement below and cite the relevant paper, either Webb et al., (2020) or Traulsen et al., (2020).
4XMM-DR13 is the fourth generation catalogue of serendipitous X-ray sources from the European Space Agency's (ESA) XMM-Newton observatory, and has been created by the XMM-Newton Survey Science Centre (SSC) on behalf of ESA. It is an incremental version of the the 4XMM catalogue and contains 531 more observations and 44678 more detections than the preceding 4XMM-DR12 catalogue, which was made public in July 2022. In addition, we provide spectra and lightcurves for more than 16762 more detections than in 4XMM-DR12.
The catalogue contains source detections drawn from a total of 13243 XMM-Newton EPIC observations made between 2000 February 1 and 2022 December 31; all datasets included were publicly available by 2022 December 31 but not all public observations are included in this catalogue. For net exposure time ≥ 1ksec, the net area of the catalogue fields taking account of the substantial overlaps between observations is ~ 1328 deg2.
4XMM-DR13 contains 983948 X-ray detections above the processing likelihood threshold of 6. These X-ray detections relate to 656997 unique X-ray sources. A significant fraction of sources (129133, 20%) have more than one detection in the catalogue (up to 90 repeat observations in the most extreme case).
The catalogue distinguishes between extended emission and point-like detections. Parameters of detections of extended sources are only reliable up to the maximum extent measure of 80 arcseconds. There are 91763 detections of extended emission, of which 20971 are 'clean' (in the sense that they were not flagged).
Due to intrinsic features of the instrumentation as well as some shortcomings of the source detection process, some detections are considered to be spurious or their parameters are considered to be unreliable. It is recommended to use a detection flag and an observation flag as filters to obtain what can be considered a 'clean' sample. There are 854095 out of 983948 detections that are considered to be clean (i.e., summary flag < 3).
For 353538 detections, EPIC time series and 353821 detections, EPIC spectra were automatically extracted during processing, and a χ2-variability test was applied to the time series. 8029 detections in the catalogue are considered variable, within the timespan of the specific observation, at a probability of 10-5 or less based on the null-hypothesis that the source is constant. Of these, 6039 have a summary flag < 3.
The median flux (in the total photon-energy band 0.2 - 12 keV) of the catalogue detections is ~ 2.2 × 10-14 erg/cm2/s; in the soft energy band (0.2 - 2 keV) the median flux is ~ 5.2 × 10-15, and in the hard band (2 - 12 keV) it is ~ 1.2 × 10-14. About 23% have fluxes below 1 × 10-14 erg/cm2/s. The flux values from the three EPIC cameras are, overall, in agreement to ~ 10% for most energy bands. The median positional accuracy of the catalogue point source detections is generally < 1.57 arcseconds (with a standard deviation of 1.43).
With 4XMM-DR13, we also release 4XMM-DR13s, a new version of the stacked catalogue built from 9796 4XMM-DR13 overlapping observations. 4XMM-DR13s contains 1688 stacks (or groups). Most of the stacks are composed of 2 observations and the largest has 372. The catalogue contains 401596 sources, of which 310478 have several contributing observations. Stacking observations allows yet fainter sources to be detected in sky regions observed more than once, increasing the number of detections and uncovering long-term variability on repeatedly observed objects. 4XMM-DR13s reaches a median depth of ~2.5E-15 and ~6.8E-15 erg/cm2/s in the soft (0.2-2 keV) and hard (2-12 keV) X-ray band, respectively.
Pointed observations with the XMM-Newton Observatory detect significant numbers of previously unknown 'serendipitous' X-ray sources in addition to the proposed target. Combining the data from many observations thus yields a serendipitous source catalogue which, by virtue of the large field of view of XMM-Newton and its high sensitivity, represents a significant resource. The serendipitous source catalogue enhances our knowledge of the X-ray sky and has the potential for advancing our understanding of the nature of various Galactic and extragalactic source populations.
The 4XMM-DR13 catalogue is the fifteenth publicly released XMM-Newton X-ray source catalogue produced by the XMM-Newton Survey Science Centre (SSC) consortium. It follows the 1XMM (released in April 2003), 2XMMp (July 2006), 2XMM (August 2007), 2XMMi (August 2008), 2XMMi-DR3 (April 2010), 3XMM-DR4 (July 2013), 3XMM-DR5 (April 2015), 3XMM-DR6 (July 2016), 3XMM-DR7 (June 2017) and 3XMM-DR8 (May 2018), 4XMM-DR9 (December 2019), 4XMM-DR10 (December 2020), 4XMM-DR11 (August 2021) and 4XMM-DR12 (July 2022) catalogues: 2XMMp was a preliminary version of 2XMM. 2XMMi and 2XMMi-DR3 are incremental versions of the 2XMM catalogue.
The 4XMM-DR13 catalogue is about 5% larger than the 4XMM-DR12 catalogue. In terms of the number of X-ray sources, combining the 4XMM-DR13 and 4XMM-DR13s catalogues gives a catalogue that is similar in size to the Chandra Source Catalogue but 4XMM-DR13+4XMM-DR13s contain twice as many individual sources as the current version of the Chandra catalogue. 4XMM-DR13+4XMM-DR13s complement deeper Chandra and XMM-Newton small area surveys, probing a large sky area at the flux limit where the bulk of the objects that contribute to the X-ray background lie. The 4XMM-DR13 catalogue provides a rich resource for generating large, well-defined samples for specific studies, utilizing the fact that X-ray selection is a highly efficient (arguably the most efficient) way of selecting certain types of object, notably active galaxies (AGN), clusters of galaxies, interacting compact binaries and active stellar coronae. The large sky area covered by the serendipitous survey, or equivalently the large size of the catalogue, also means that 4XMM-DR13+4XMM-DR13s is a superb resource for exploring the variety of the X-ray source population and identifying rare source types.
The production of the 4XMM-DR13 and 4XMM-DR13s catalogues has been undertaken by the XMM-Newton SSC consortium in fulfillment of one of its major responsibilities within the XMM-Newton project. The catalogue production process has been designed to fully exploit the capabilities of the XMM-Newton EPIC cameras and to ensure the integrity and quality of the resultant catalogue through rigorous screening of the data.
4XMM-DR13 and 4XMM-DR13s are based on the pipeline configurations 18 and 19. This pipeline version is the same as for the other versions of 4XMM, but contains many changes with respect to the pipeline used to make the previous major version of the catalogue, 3XMM-DR5. Changes include source spectra and light curves created for pn Timing mode and small window data, source detection on pn small window data, energy dependent Charge Transfer Inefficiencies (CTI) and double event energy corrections applied, time and pattern dependent corrections of the spectral energy resolution of pn data, X-ray loading and rate dependent energy (PHA) and CTI corrections for EPIC pn Timing and Burst modes, binning of MOS spectra changed from 15 eV to 5 eV and filtering with XMMEA_EM, which is a bit-wise selection expression, automatically removing “bad events” such as bad rows, edge effects, spoiled frames, cosmic ray events (MIPs), diagonal events, event beyond threshold, etc, instead of XMMEA_SM (which removed all flagged events except those flagged only as CLOSE_TO_DEADPIX), background regions for EPIC spectra and light curves selected from the same EPIC chip where the source is found, observations of solar system objects processed such that X-ray images and spectra correctly refer to the moving target, pileup diagnostic numbers for EPIC sources included, and footprints for EPIC observations based on combined EPIC exposure maps provided as ds9 region files. Other changes carried out specifically for the production of 4XMM include a revised systematic position error, the modelling of the EPIC background and finer binning of EPIC lightcurves. More information on these changes can be found in Webb et al., (2020). 141 observations containing pn timing data, that were already used for 4XMM-DR11 have been reprocessed for 4XMM-DR12 and subsequent catalogues using the pipeline version 19, to take into account an update to the pn effective area. The observations concerned can be found in this list.
Users of the 4XMM catalogue should be aware that the DETID and SRCID values bear no relation to those in the previous 2XMM series of catalogues. However, a cross-matching is provided in 4XMM-DR13 via the DR3DETID and DR3SRCID columns.
The extensive User Guide (UG) for the 2XMM catalogue still describes many of the details of the data processing and compilation approach applicable to the 4XMM-DR13 catalogue. However, a significant number of changes to the processing have been implemented for 4XMM and these are described in the 4XMM-DR9 documentation and the Section 3 below. For convenience, Table 1, which gives the energy band definitions, is repeated here.
| Basic energy bands: | 1 | = | 0.2 - 0.5 keV | ||
| 2 | = | 0.5 - 1.0 keV | |||
| 3 | = | 1.0 - 2.0 keV | |||
| 4 | = | 2.0 - 4.5 keV | |||
| 5 | = | 4.5 - 12.0 keV | |||
| Broad energy bands: | 6 | = | 0.2 - 2.0 keV | soft band, no images made | |
| 7 | = | 2.0 - 12.0 keV | hard band, no images made | ||
| 8 | = | 0.2 - 12.0 keV | total band | ||
| 9 | = | 0.5 - 4.5 keV | XID band | ||
XMM-Newton observations considered for inclusion in the 4XMM-DR13 catalogue were those with ODFs available for processing up to 2022 December 31 and all were publicly available as of 2022 December 31. After allowing for a small number of observations which failed in processing for a variety of reasons, Table 2.1 gives the list of the final 13243 observations which are included in the 4XMM-DR13 catalogue.
Starting in 3XMM-DR5, the procedure for attributing the detection identification number (DETID) and the unique source identification number (SRCID), both being unique to each detection and each unique source respectively, has been modified. Previously, identification numbers were re-computed for each catalogue version leading to supplementary columns added to the catalogue with the DETID and SRCID from previous releases.
The DETID is now constructed from the OBS_ID, which always remains the same for an observation, coupled with the source number SRC_NUM (SRC_NUM is the source number in the individual source list for a given observation; Sources are numbered in decreasing order of count rate (i.e. the brightest source has SRC_NUM = 1)) as follow:
DETID = 1 + OBS_ID + SRC_NUM
where the '+' sign indicates string concatenation and where SRC_NUM is zero-padded to form a 4 digit number. The SRCID of a unique source is then determined from the first DETID attributed to that source (i.e. in the observation where the source was first detected) and replacing the first digit '1' by '2'.
Despite the new naming convention that aims at preserving SRCID numbers across catalogue versions, a certain number of SRCID can disappear from one catalogue version to another. This is a normal consequence of the algorithm that groups detections together into unique sources (see section 6 of Rosen et al. 2016). When new data are added and statistics are improved, the algorithm might find a better association of detections into unique sources. As an example, a total of 134 SRCIDs listed in 3XMM-DR7 are absent in 3XMM-DR8.
The astrometry of the X-ray detections is improved by using the catcorr task to cross-correlate the X-ray detections with the USNO B1.0, 2MASS or SDSS (DR8) optical/IR catalogues. However, where catcorr fails to obtain a statistically reliable result (poscorrok=false), a systematic error of 1.5′′ was used to create the 3XMM catalogue. To check this value, we cross-matched SDSS quasars with the detection catalogue where poscorrok=false, out to r=30 arcsecs, filtering the latter with SUM_FLAG=0 and EP_EXTENT=0, to keep only the cleanest sample of secure point-like X-ray sources. For more information about what was done, see Webb et al. (2020). We define the combined positional error as σ=(Δ S2+Δ X2/2)0.5, where Delta; X = POSERR and Δ S is the radially-averaged uncertainty in the SDSS positions to which we had already added a systematic 0.1'' in quadrature, and x = r / σ. Our final filtering retained only the 157 QSO-X-ray pairs with x<5.
The expected probability density distribution of x should follow the Rayleigh distribution P(x) = x e-x2. Since this was not the case for the 157 pairs of sources found above, we added an additional positional uncertainty, σ, in quadrature, so that the total positional uncertainty is now σ = (σ2 + Σ2)0.5, looking for the value of Σ that minimizes the difference between the distribution of the x' = r/σ' and the Rayleigh distribution. For 4XMM-DR10 we found Σ = 1.90 +/- 0.01 arcsec, where the uncertainty (1 σ) has been calculated by bootstrap with replacement. This value was then used to replace the 1.5 arcsec systematic error when poscorrok=false.
As of 4XMM we provide three new columns (PN_PILEUP, M1_PILEUP and M2_PILEUP) quantifying whether each detection may be affected by pile-up in any instrument. A value below 1 corresponds to negligible pile-up (less than a few % flux loss) while values larger than 10 denote heavy pile-up. Pile-up is dependent on time for variable sources. We neglect that here, but note that a variable source is more piled-up than a constant one for the same average count rate, so our pile-up level can be viewed as a lower limit. We also neglect the slight dependence on the source spectrum due to the event grade dependence of pile-up.
Our pile-up levels are not based on a fit of the full images using a pile-up model (Ballet 1999). For point sources, they are based on the measured count rates reported in the catalogue over the full energy band, transformed into counts per frame. The thresholds (at which the pile-up level is set to 1) are set to 1.3 cts/frame for MOS and 0.15 cts/frame for PN.
Some pileup values for extended sources were deemed to be erroneous and therefore all pileup values for extended sources were NULL in the 4XMM-DR10, 4XMM-DR11 and 4XMM-DR12 versions. Starting from pipeline version 20.08 (SAS version 20.0), emldetect (v.7.7) introduces a vignetting correction to the pileup estimate of extended sources. Since the observations processed with older version of the pipeline could not benefit from this correction and in order to keep pileup values consistent across the catalogue, we applied an analytic calculation method to the older data for the pileup which closely matches the results produced by the new version of emldetect. Therefore pileup values for extended sources in 4XMM-DR13 are now accurate.
Warm pixels on a CCD (at a few counts per exposure) are too faint to be detected as such by the automatic processing, but can either push faint sources above detection level, or create spurious sources when combined with statistical fluctuations. This is an intrinsically random process, not visible over a short period of time, but which creates hot areas when projecting all sources detected over 18 years onto the detector plane.
We addressed this by projecting all sources onto CCD coordinates PN/M1/M2_RAWX/Y, keeping only sources above the detection threshold with the current instrument alone. In that way, we can distinguish hot areas coming from different instruments. We proceeded to detect hot pixels or columns in each CCD, using a similar method to the SAS task embadpixfind. For more information see Webb et al. (2020). Many of warm pixels were not present at the beginning of the mission, and some appear for a short amount of time. So we tested each hot area for variability using revolution number, and the same KS-based algorithm used to detect segments of bright columns, compared to the reference established over all sources on all CCDs and all instruments. This resulted in a revolution interval for each hot area.
Sources on a hot area for a particular instrument and within the corresponding revolution interval are flagged with flag 12. The updated table for the 12 flags is given below.
| 1 | Low detector coverage | ca_MASKFRAC < 0.5 |
| 2 | Near other source | R ≤ 65 * SQRT (EP_RATE); R(min) = 10", R(max) =
400" |
| 3 | Within extended emission | R ≤ 3 * EP_EXTENT; R(max) = 200" |
| 4 | Possible spurious extended source near bright source | Flag 2 is set and EP_CTS(min) = 1000 for the causing
source |
| 5 | Possible spurious extended source within extended emission | R ≤ 160" and fraction of rate wrt causing source is 0.4 |
| 6 | Possible spurious extended source due to unusal large single-band DET_ML | Fraction of ca_b_DET_ML wrt the sum of all
≥ 0.9 |
| 7 | Possible spurious extended source | At least one of the flags 4, 5, 6 is set |
| 8 | On bright MOS-1 corner or bright low gain PN column | |
| 9 | Near bright MOS-1 corner | R ≤ CUTRAD = 60" of a bright pixel the corner |
| 10 | Detection whose centre lies on any masked column or row due OoT and RGA features. | 11 | Within region where spurious detections occur | Manual flag | 12 | Detection on hot area |
The default value of every flag is F for False. When a flag was set it means it has been changed to T for True.
The task dpssflag sets all flags except the camera-specific flags (i.e., flags 2,3,4,5,6,7) on the summary row (EPIC band 8) which are then propagated backwards to the individual cameras and bands. Flag 12 is not propagated into the SUM_FLAG in 4XMM.
This section summarises the organisation of the catalogue and gives details of all the columns. Known problems with parameters presented in the catalogue or with products associated with it are listed in Sec. 6.
There are 336 columns in the catalogue; they are grouped together and explained in the links below.
For each observation there are up to three cameras with one or more exposures which were merged when the filter and submodes were the same (2XMM UG, Sec. 2.2). The data in each exposure are accumulated in several distinct energy bands (Table 1). Camera-level measurements can further be combined into observation-level parameters. Consequently, the source parameters can refer to some or all of these levels: on the observation level there are the final mean parameters of the source (prefix 'EP'); on the camera level the data for each of the three cameras (where available) are given (prefix 'PN', 'M1', or 'M2'), and on the energy band level the energy-dependent details of the source parameters are given (indicated by a 'b' in the column name where b = 1,2,3,4,5,8,9). Finally, on a meta-level, some parameters of sources that were detected more than once (prefix 'SC') were combined, see 2XMM UG, Sec. 3.2.4.
The column name is given in capital letters, the FITS data format in brackets and the unit in square brackets. If the column originates from a SAS task, the name of the task is given to the right hand side and a link is set to the SAS package documentation with which the data in the 4XMM-DR9 catalogue was processed. It should be pointed out that the SAS used for the bulk reprocessing (for 4XMM) was from manifest pipeline version 18, which is based on SAS 18. A description of the column and possible cross-references follow.
Entries with NULL are given when no detection was made
with the respective camera, that is, ca_MASKFRAC < 0.15 or
NULL (i.e., a camera was not used in an observation).
| Part 1: | 14 columns: Identification of the source |
|---|---|
| This includes the basic static identifiers, IAU name, together with cross-references to the (spatially) nearest detection and source ID in the previous 3XMM-DR4 and 2XMMi-DR3 catalogues, where relevant, including information about the spatial displacements and the number of 'nearby' matches. Five columns (introduced in 3XMM-DR7) are used to provide this information. | |
| Part 2: | 11 columns: Details of the observation and exposures |
| Part 3: | 20 columns: Coordinates |
| The external equatorial and Galactic coordinates and the internal equatorial coordinates as derived from the SAS tasks catcorr and emldetect are given together with the error estimates. Two columns convey information about the absolute astrometric catalogue used for field rectification and whether the field was successfully rectified | |
| Part 4: | 228 columns: Source parameters |
| The parameters of the source detection as derived from the SAS tasks emldetect and srcmatch are given here. | |
| Part 5: | 8 columns: Detection flags |
| This part lists the flags to qualify the detections. The summary flag, which gives an overall assessment for the detection, is followed by particular flags for each camera. A flag each is given if there exists at least one time series or one spectrum for this source. One column is added at the end of the catalogue to provide information about detections arising in fields with high background levels. However, since 4XMM, thanks to the improved data reduction, the high background is eliminated more efficiently and this column is redundant. | |
| Part 6: | 13 columns: Detection variability |
| This part gives variability information for those detections for which time series were extracted. This includes six columns which provide measures of the fractional variance of the timeseries | |
| Part 7: | 42 columns: Unique source parameters |
| This part lists the source parameters for the unique sources across all observations (using the prefix 'SC'); these are coordinates, fluxes, hardness ratios, likelihoods, extent information and a variability and a summary flag. The number of detections is given also. Of six columns introduced for 3XMM, two of these relate to a fractional variance measure (and error). The other four provide information about the maximum and minimum measured fluxes from constituent detections (and errors). Two further columns relating to the epochs of the first and last observations contributing to a unique source, replace two columns in 2XMMi-DR3 |
Table 6 lists the 45 columns in the 4XMM-DR13 'slimline' version of the catalogue, all of which are explained in Part 1 or Part 7 of the 4XMM-DR13 column description, except the WEBPAGE_URL column which is described at the end of the table.
This section summarises the main properties of the catalogue but does not provide a detailed analysis. A comprehensive evaluation of the catalogue is presented in the 4XMM catalogue papers Webb et al., (2020) or Traulsen et al., (2020).
The catalogue contains source detections drawn from 13243 XMM-Newton EPIC observations made between 2000 February 3 and 2022 December 31 and which were publicly available by 2022 December 31. Net exposure times in these observations range from < 1000 up to ~130000 seconds (that is, a full orbit of the satellite). Figure 5.1 shows the distribution of fields on the sky.
The sky area of the catalogue observations corrected for field overlaps with effective exposure > 1 ks ~1328 deg2.
The catalogue contains 983948 X-ray detections with total-band (0.2 -12 keV) likelihood values ≥ 6. These are detections of 656997 unique X-ray sources, that is, 129133 X-ray sources have multiple detections in separate observations (up to 90 detections). Of the 983948 X-ray detections, 91763 are classified as extended with 20971 of these being in regions considered to be 'clean' (SUM_FLAG < 1).
As part of extensive quality evaluation for the catalogue, each field has been visually screened. Regions where there were obvious deficiencies with the automatic source detection and parameterization process were identified and all detections within those regions were flagged (cf. 2XMM UG, Sec. 3.2.6 but importantly, note Section 3.11). Such flagged detections include clearly spurious detections as well as detections where the source parameters may be unreliable. Each XMM-Newton field is also evaluated to assess the fractional area of the observation that is affected by flagged detections, as reflected by the OBS_CLASS parameter. For most uses of the catalogue it is recommended to use a detection flag (SUM_FLAG, EP_FLAG or SC_SUM_FLAG) and an observation flag (OBS_CLASS) as a filter to obtain what can be considered a 'clean' sample.
Note that no attempt is made to flag spurious detections arising from statistical fluctuations in the background. An updated analysis of the false detection rate is presented in the 4XMM catalogue paper Webb et al., (2020).
Figure 5.4 presents, for each of the three cameras, the distributions of flux for energy bands 1 to 5 and also for the combined (EPIC) data. These give an indication of the limiting flux available in the catalogues for each of the bands.
Comparing the astrometry between 3 and 4XMM shows very similar results. A more detailed analysis of these issues are presented in the 4XMM catalogue paper Webb et al., (2020).
Please read the Watchouts section of the 4XMM-DR13 documentation for the latest information on 4XMM-DR13 catalogue issues.
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This project has received funding from the European Union's
Horizon 2020 research and innovation programme under grant
agreement n°101004168, the XMM2ATHENA project.
| Release No. | Release Date | Comments |
| 1.40 | 12th June 2023 | First release for 4XMM-DR13 |
| 1.30 | 28th July 2022 | First release for 4XMM-DR12 |
| 1.20 | 18th August 2021 | First release for 4XMM-DR11 |
| 1.10 | 10 December 2020 | First release for 4XMM-DR10 |
| 1.0 | 18 December 2019 | First release for 4XMM |
List of observations ('fields').