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The XMM-Newton slew survey Source Catalogue:XMMSL1
User Guide to the Catalogue
This User Guide refers directly to the FITS format version of the catalogue. Most of the content is also applicable to the database-served format (from XSA), but there are some aspects that are not applicable to the latter. Conversely, there are aspects of the database implementations that are not covered by this User Guide, but by the Help information provided from the database user interfaces. The User Guide provides a detailed account of the production and contents of the catalogue. Contents
SummaryXMMSL1 is the first catalogue of X-ray sources found in slew data
taken from the European Space Agency's (ESA) XMM-Newton observatory,
and has been constructed by members of the XMM SOC and the EPIC
consortium on behalf of ESA. Version 1.5This version is an update to the existing catalogue. The update contains 131 extra slews taken between revolutions 1866 and 2011. An extra 2192 clean sources have been added with the update .This release is known as XMMSL1_Delta5. 1. IntroductionXMMSL1_Delta5 has been generated from 131 slews, executed between
revolutions 1866 and 2011. Not all slews made in this period have been
used; slews with particularly high background or which gave processing
problems have been rejected. A description of slew selection and
initial processing is given
T 2. Initial ProcessingThe XMM-Newton Slew Data Files (SDFs) for EPIC-pn were processed using the epchain package of the public xmmsas-6.1. For diagnostic reasons a few parameters were set to non-default values (e.g. keeping also events below 150 eV). For the Slew Survey catalogue only EPIC-pn exposures performed in Full Frame (FF), Extended Full Frame (eFF), and Large Window (LW) modes were selected, i.e. modes where all 12 CCDs are integrating (in LW mode only half of each CCD). The corresponding cycle times are 73.36 ms, 199.19 ms, and 47.66 ms, which converts to a scanned distance of 6.6 arcseconds, 17.9 arcseconds, and 4.3 arcseconds per cycle time, respectively. In the Small Window mode only the central CCD is operated and a window of 64 x 64 pixels is read out, i.e. only about 1/3 of a CCD. In the fast modes, Timing and Burst, only 1-dimensional spatial information for the central CCD is available and thus these three modes are not very well suited for source detection. Slews deemed to have a generally high background, with a mean 7.5 - 12 keV count rate greater than 5.5 c/s over the whole length of the slew, have been discarded3. ProcessingEvents are recorded initially in RAW or detector coordinates and
have to be transformed, using the satellite attitude history, into sky
coordinates. The tangential plane geometry commonly used to define a
coordinate grid for flat images is only valid for distances of 1-2
degrees from a reference position, usually placed at the centre of the
image. To avoid this limitation, slew datasets are divided into roughly
one square degree event files, attitude corrected and then converted
into images. 4. Combination of individual band surveysDetections in the three energy bands have been combined using a match radius of 30 arcseconds to identify sources detected in more than one band. The match radius is approximately 4 sigma and is reasonable for point sources because of the great scarcity of sources (0.8 detections per square degree on average) at the flux levels probed by the slew survey.5. Spurious flaggingSpurious detections are produced due to systematic effects with the instruments and detection software. These sources have been screened and flagged ('t' for 'true' or 'f' for 'false') in the different categories described below. When a source is flagged true the FLAG_COMMENT column gives a more detailed explanation of the problem for each particular source.VER_INEXT: This quality flag is used to ensure that only one source is quoted for extended objects; that with the highest det_ml. Two different cases have been found: - Large extended sources (mainly SNR) that often result in multiple detections of the same object. These have been identified by searching for images with a large number of sources - Other spurious sources (mainly due to Cluster of Galaxies) appear because the technique used for merging detections in the different energy bands is optimal for point-like sources. This consists of considering the same source if their centres lie within 30 arcsec of each other, but this offset has to be bigger for extended sources. This is expected to be fixed in a new version of the catalogue. VER_HALO: A halo of false detections is often seen around bright slew sources due to the imperfect modelling of the PSF (as was also seen in the creation of the 1XMM Serendipitious Source Catalogue). Due to the reduced exposure time in slew observations this is only important for very bright sources rate>>10c/s. For flagging this category of spurious, the different sources detected in the same image and containing a very bright source have been inspected. If their centres lie within 30 arcsec but corresponding to the same object, the one with highest det_ml is taken as the non-spurious detection and the rest have been flagged 't'. VER_HIGHBGND: One of the characteristics of slew exposures is their low background (of average ~0.1 c/arcmin^2). Although high background slews taken at times of enhanced solar activity have been rejected for the processing, some high background sub-images have been detected in observations with a general rate below the threshold used for rejecting entire slews. These sources have been identified and flagged in this category looking for images with a large number of sources (without being included in the VER_INEXT category of spurious sources explained above). It has been checked that no other bright off-axis source could generate the detections. Rates for all images have also been computed. VER_NREDG: Some sources have been detected lying on the border of consecutive images of the same slew observation, so the position of both detections of the same object is unlikely to be accurate. These spurious sources have been identified by seaching for sources in consecutives images whose centres lie within 30 arcsec. VER_PSUSP: This quality flag is related to the astrometry performance and arises after a careful visual examination of the RAF files. The attitude reconstruction of some slews appears to be "turbulent" rather than smooth, so source positions lying in these poorly attitude reconstructed regions are likely to be inaccurate. VER_FALSE: This flag is related to spurious detections not included in the
other flags. Two sources (both are close to an SNR) which have been
discovered to lie outside the images they are supposed to belong to,
and hence have a calculated exposure time of zero, have this flag set
true. A further 27 detections, due to out of field-of-view reflections
from SCO X-1 also have this flag set. 6. SimulationsTo estimate the number of sources caused by statistical fluctuations in the background a series of simulations have been run to:1. Assess the effect of the number of photons in an image on the number of spurious detections as a function of detection likelihood. An average sized slew image was taken and a number of photons inserted at random positions. The number of false sources produced is a strong function of the number of photons in the image, with the peak appearing with a coverage of a few hundred photons over this size image. It is suspected that the peak in the curves is due to peculiarities of the background estimation technique which fits a spline-surface to the image. The majority of the slew images contain about 100 counts where the number of spurious sources produced by the background is small. 2. Equate the number of counts in an image with the measured background rate. The background rate in XMM images is traditionally measured by finding the count rate above 10 keV (PI>10000), where the contribution from celestial X-ray sources is expected to be very small. We see a strong correlation between this background estimator and the total number of source photons. 3. Estimate the total number of spurious sources in each energy band. There were 11449 images which have been searched for sources to form the original XMMSL1 catalogue. For each of these images, in each energy band, the position of the photons has been randomly reset and the images searched again using the same software. The table below gives, for different values of the minimum acceptable detection likelihood, false source numbers which are compared with the total number of sources detected in the catalogue. It can be seen that using a descriminator on the background count rate helps to reduce the fraction of spurious detections while maximising the number of real sources. The optimum extraction for the hard band and total band catalogues uses a likelihood limit of 10 for sources found in low background images [ (PI>1000) <= 3c/s ] and a limit of 14 for sources detected in images with a higher background. This selection has been used to form the "clean" catalogue which is the default selection within XSA. As can be seen from the Table , this is quite conservative for the soft band catalogue.
Table: Numbers of sources, in the original XMMSL! catalogue, and estimated false sources (in brackets) for various selections of detection likelihood and background rate7. IdentificationsAll sources detected in the survey have been correlated with different catalogues in order to identify the XMM-Newton slew sources with previously known objects. The catalogues used for this aim comprises two astronomical databases, a catalogue of clusters of galaxies and nine other catalogues (some of them have been queried through the HEASARC astronomical database). Although the astrometric uncertainty of the slew sources was found to be 8 arcsec, the offset radius for the correlations was 30 arcsec (with a few exceptions described below) in order to include sources from catalogues with worse accuracy or truncated coordinates. For the EXOSAT CMA catalogue the offset radius was 45 arcsec, and for the Einstein IPC it was 2 arcmin, both due to their high uncertainty in source coordinates. A radius of 5 arcmin was chosen for the clusters catalogue due to the extension of this type of objects. As not all catalogues have the same astrometric accuracy distances are rounded to the nearest 0.1 arcmin in many cases. The identification process results in unidentified sources, sources with a single counterpart and sources with multiple matches. A hierarchical selection scheme has been applied for sources with different counterparts. A decision has been made to derive the most plausible identification candidate using the technique described below. Firstly, the SIMBAD and NED astronomical databases have been used for the cross-correlation and results from both databases have been compared in detail (SIMBAD has been queried in the frame of the Astronomical Virtual Observatory (AVO)).When a source has the same counterpart in both databases the one selected for the identification is that which gives more specification about the source category. When contradictory identification candidates have been found, the closest one has been chosen. These two databases provide the large majority (90%) of the total number of identifications. Then, a correlation with a clusters table (Abell and Zwicky Clusters of Galaxies ) has been performed. The final identification for those extended sources (ext>2.0) with a SIMBAD/NED and also a cluster correlation comes from the clusters table. The rest of catalogues used for the cross-match are listed below ordered in priority for the preferred identification. For sources with multiple matches in a catalogue, the identification was selected as the closest match. These catalogues are: All-Sky Optical Catalog of Radio/X-Ray Sources, Catalog of PSPC WGA Sources, Einstein IPC Sources Catalog, EXOSAT CMA Images/Lightcurves, ROSAT All-Sky Survey catalogue, ROSAT Results Archive Sources for the PSPC ROSAT Results Archive, Sources for the HRI RXTE Master Catalog, XMM-Newton Serendipitous Source Catalog, Version 1.1.0, INTEGRAL Bright Source Catalog. Identifications are offered for 70% of the sources. Results from the identification process appear in the final catalogue in the columns:IDENT: name of the source ALTIDENT: alternative name of the source ID_DIST: distance in arcmin between the slew source and the identification (distances are rounded in 0.1 arcmin). ID_CATEGORY: type of the identified source that, when existing, has been extract ed from the catalogues (it is not very homogeneous because type convention is different within the catalogues) RASSNAME: the closest RASS match RASSDIST: distance in arcsec to the closest RASS match All correlations can be summarized in roughly 50% identified slew sources. 8. AstrometryThe attitude information of the XMM-Newton satellite is provided by the Attitude and Orbit Control Subsystem (AOCS). A star tracker co-aligned with the telescopes allows up to a maximum of five stars to be continuously tracked giving accurate star position data every 0.5 seconds, which operates in addition to the Sun sensor that provides a precise Sun-line determination. Such information is processed resulting in an absolute accuracy of the reconstructed astrometry of typically 1 arcsecond during pointed observations. For the open-loop slews, large slews outside the star-tracker field of view of 3 x 4 degrees, the on-board software generates a three axis momentum reference profile and a two-axis (roll and pitch) Sun-sensor profile, both based on the ground slew telecommanding. During slew manoeuvring a momentum correction is superimposed onto the reference momentum profile and, as there are no absolute measurements for the yaw axis, a residual yaw attitude error exists at the end of each slew that may be corrected in the final closed-loop slew. To process slew data, attitude information is taken from a Raw Attitude File (RA F) which stores attitude points every 40-60 seconds. The times quoted in the RAF are offset from spacecraft time by 0.75 seconds, which has to be corrected in the software, otherwise a 1 arcminute offset in source positions is seen along the slew direction. Initially the correction was performed in the slew specific software but from SAS 7.0 has been included in the general SAS software. The SAS astrometry software interpolates between the rather sparse RAF points using a curve fit. Five RAFs have been found to contain one bad attitude point which is sufficient to totally corrupt the attitude solution over a considerable section of the slew. In these cases affected sources have been removed from the CLEAN catalogue and the error on their position has been set to 120 arcseconds. In a further 7 slews a part or all of the attitude seems to be turbulent rather than smooth. It is not known why this occurs and no attempt to fix it has been made. Sources affected by this attitude problem have a position suspect (VER_PSUSP) flag set to true. The error introduced in the source positions can be of the order of 1 arcminute. A sample of point sources from the catalogue with matches in the SIMBAD catalogue have been analysed and show that 68% lie within 8 arcseconds of the SIMBAD position and 90% within 17 arcseconds.9. Column DescriptionsUNIQUE_SRCNAMEThis is the official name for sources detected in the XMM-Newton
slew survey. It starts with the prefix, XMMSL1, the IAU registered
designator, and then encodes the J2000 sky position, e.g. XMMSL1
J010537.6+364858 The name is assigned in two passes. When the three
independent energy band source lists are combined to form one catalogue
the source name is set using the position in the band where the DET_ML
likelihood is the highest. A second pass is then performed such that
sources which have been observed in more than one slew are given the
same name. Again, priority is given depending on the detection
likelihood. Note that the combination of UNIQUE_SRCNAME and observation
number (OBSID) is unique. Detections are deemed to be from the same
source if their centres lie within 30 arcseconds of each other. Note
that the statistical position error (RADEC_ERR) calculated by the
source search software is not used in this calculation. This is because
the mean error on the slew attitude reconstruction of 8" dominates the
error budget. Given the scarcity of slew sources (0.8 detections per
square degree) on the sky, 30" was found to be a reasonably robust
match radius for point sources. It is not so good for extended sources
and the catalogue may contain multiple detections of the same extended
source with different names. Please note that no attempt has been made to assign a UNIQUE_SRCNAME
from the original XMMSL1 catalogue to sources added in the subsequent
delta increment(s). OBSID This is the observation number assigned to the slew by the satellite scheduling system. Slew observations always begin with a 9 to distinguish them from pointed observations, followed by a 4 digit satellite orbit number and a 5 digit slew designator, e.g. 9031400004, refers to the second slew of revolution 314. SOURCENUM This is a number which uniquely identifies each detection in an observation. RA, DEC The J2000 right ascension and declination of the source. Units: Degrees In the event of a detection in more than one energy band, the coordinates are taken from the band with the highest detection likelihood. RADEC_ERR The statistical error on the source position as returned by the source detection software. Units: arcseconds LII, BII The galactic coordinates of the source. Units: Degrees HR1 The hardness ratio, defined as HR1 = (rate_b4-rate_b5)/(rate_b4+rate_b5) where rate_b4 is the hard band count rate and rate_b5 is the soft band count rate. This has been calculated for the 168 sources which have a positive detection in both bands (see hratios.ps) HR1_ERR Error on the hardness ratio calculated as: sqrt(rate_b4_err*rate_b4_err + rate_b5_err*rate_b5_err) /(rate_b4+rate_b5) where rate_b4_err and rate_b5_err are the errors on the hard and soft band count rates respectively. DATE_OBS, DATE_END The start and end times of the slew containing this source. Format is: Year-Month-dayThours:minutes:seconds, e.g. 2004-07-12T14:23:16 SCTS_B0 The number of background subtracted counts, in the total energy band (0.2-12 keV). Units: counts This number has been corrected for photons scattered outside the source region due to the Point Spread Function (PSF). SCTS_B0_ERR Statistical 1 sigma error on the total band source counts. SCTS_B4 The number of background subtracted counts, in the hard energy band (2-12 keV), corrected for the PSF. Units: counts SCTS_B4_ERR Statistical 1 sigma error on the hard band source counts. SCTS_B5 The number of background subtracted counts, in the soft energy band (0.2-2 keV), corrected for the PSF. Units: counts SCTS_B5_ERR Statistical 1 sigma error on the soft band source counts. X_IMA_B0, Y_IMA_B0 The X and Y position of the source in the total band image in image pixels. Units: 4.1"x4.1" pixels X_IMA_B4, Y_IMA_B4 The X and Y position of the source in the hard band image in image pixels. Units: 4.1"x4.1" pixels X_IMA_B5, Y_IMA_B5 The X and Y position of the source in the soft band image in image pixels. Units: 4.1"x4.1" pixels EXT_B0 The spatial extension of the source in the total energy band. Units: 4.1"x4.1" image pixels This measures the deviation from a point source of the spatial distribution of the source counts. It is defined as the sigma of a Gaussian which would need to be convolved with the point spread function (PSF) to produce the observed counts distribution. The software (emldetect) fits sources out to a maximum extent of 20 pixels. EXT_B0_ERR Statistical one sigma error on the total band extension parameter. EXT_B4 Spatial extension of the source in the hard energy band. Units: 4.1"x4.1" image pixels EXT_B4_ERR Statistical one sigma error on the hard band extension parameter. EXT_B5 Spatial extension of the source in the soft energy band. Units: 4.1"x4.1" image pixels EXT_B5_ERR Statistical one sigma error on the soft band extension parameter. DET_ML_B0 The detection likelihood in the total (0.2-12 keV) energy band. DET_ML_B4 The detection likelihood in the hard (2-12 keV) energy band. DET_ML_B5 The detection likelihood in the soft (0.2-2 keV) energy band. EXT_ML_B0 Likelihood of the source being extended in the total band. EXT_ML_B4 Likelihood of the source being extended in the hard band. EXT_ML_B5 Likelihood of the source being extended in the soft band. BG_MAP_B0 Background value for the total band. Units: Counts per pixel BG_MAP_B4 Background value for the hard band. Units: Counts per pixel BG_MAP_B5 Background value for the soft band. Units: Counts per pixel EXP_MAP_B0 The effective on-axis exposure time in the total energy band. EXP_MAP_B4 The effective on-axis exposure time in the hard energy band. EXP_MAP_B5 The effective on-axis exposure time in the soft energy band. FLUX_B0 The source flux in the total energy (0.2-12 keV) band. Units: 10^-12 ergs/s/cm2 Derived for an absorbed power-law spectrum of slope 1.7 and Nh=3.0E20 cm-2 FLUX_B0_ERR The error on the total band source flux FLUX_B4 The source flux in the hard energy (0.2-12 keV) band. Units: 10^-12 ergs/s/cm2 Derived for an absorbed power-law spectrum of slope 1.7 and Nh=3.0E20 cm-2 FLUX_B4_ERR The error on the hard band source flux. FLUX_B5 The source flux in the soft energy (0.2-12 keV) band. Units: 10^-12 ergs/s/cm2 Derived for an absorbed power-law spectrum of slope 1.7 and Nh=3.0E20 cm-2 FLUX_B5_ERR The error on the soft band source flux. RATE_B0 The total band count rate Units: counts/second RATE_B0_ERR The error on the total band count rate RATE_B4 The hard band count rate Units: counts/second RATE_B4_ERR The error on the hard band count rate RATE_B5 The soft band count rate Units: counts/second RATE_B5_ERR The error on the soft band count rate RA_B0, DEC_B0 The J2000 celestial position of the total band source. RADEC_B0_ERR The statistical error on the total band position. RA_B4, DEC_B4 The J2000 celestial position of the hard band source. RADEC_B4_ERR The statistical error on the hard band position. RA_B5, DEC_B5 The J2000 celestial position of the soft band source. RADEC_B5_ERR The statistical error on the soft band position. LII_B0, BII_B0 The galactic position of the total band source. LII_B4, BII_B4 The galactic position of the hard band source.
The galactic position of the soft band source. VAL_FLAG A text string which is set to 'CLEAN_SAMPLE' if this source is included in the clean subset. Otherwise the string is set to 'XXXXXXXXXXXX' SRCNAME_B0 The source name defined in the total band list. The format is 'xs' followed by the revolution number, the observation ID and the source position, e.g. xs0841_9084100002_12:57:07.5+01:50:42 SRCNAME_B4 The source name defined in the hard band list. The format is 'xs' followed by the revolution number, the observation ID and the source position, e.g. xs0841_9084100002_12:57:07.5+01:50:42 SRCNAME_B5 The source name defined in the soft band list. The format is 'xs' followed by the revolution number, the observation ID and the source position, e.g. xs0841_9084100002_12:57:07.5+01:50:42 XIMNAME_B0 The name of the image containing the total band detection. XIMNAME_B4 The name of the image containing the hard band detection. XIMNAME_B5 The name of the image containing the soft band detection. VER_INEXT If set true, this flag notes that a detection has been found within an extended source and is probably false. This flag is used to ensure that only one source is quoted for the large supernova remnants. VER_HALO If set true, this flag indicates that a detection lies within the point spread function, or halo, of a very bright source and is probably spurious. VER_HIBGND If set true, this flag indicates that the source lies within a bright region, caused by high background, and is probably spurious. VER_NREDG If set true, this flag indicates that the source has been detected in two consecutive images of the same slew. This can occur if the source lies on the border between slews and implies that the position of the source is unlikely to be accurate. VER_PSUSP This flag indicates that the quoted position of the source is likely to be inaccurate. In a few slews the attitude reconstruction is poor and in these cases the actual position of the source is difficult to determine and can be wrong by an arcminute. VER_FALSE This is a catch-all for problems not included in the other flags. In
the catalogue 29 sources have this flag set true, in two cases it is
because the exposure time has been calculated as zero and in the other
cases the detections are due to reflection from a close, but out of the
field-of-view SCO X-1. FLAG_COMMENT A comment which explains why a particular source flag has been set to true. IDENT Cross-correlations of the positions of the slew sources with astronomical databases and catalogues have been performed (see section on IDs). This column gives the catalogue name of the best match. ALTIDENT An alternative name for the best match source. RASSNAME The name of the closest Rosat All Sky Survey (RASS) source. ID_CATEGORY The source type as returned by SIMBAD, NED and the other resources used in the cross-matching process. This is directly taken from the catalogue in question and no attempt has been made to rationalise the values. ID_RESOURCE The astronomical database or catalogue from which the best match has been selected. e.g. SIMBAD, NED, etc. ID_DIST The distance in arcminutes between the best match candidate and the slew survey source. Units: arcminutes RASS_DIST The distance from the best match ROSAT source and the slew source. Units: arcseconds MODE_ID Observing mode of the EPIC-pn camera. FF= Full frame mode eFF = extended full frame mode LW = large window mode IMAGE_BG_RATE Peak background count rate in the image from which the source was extracted. This is measured as the count rate, over the whole image, for events with energy > 10 keV (PI>10000). Units: counts/second It is quoted to a resolution of 0.1 c/s and is used to determine the overall background environment in which a source was detected. This value is used in the creation of a clean subsample of the catalogue (see top level description). Generally, the higher this value, the greater the probability that the source is spurious. This is especially true if the detection likelihood of the source is less than 14. The value has been tabulated for images with a background rate greater than 2 c/s. For quieter images the value has been artifically set to 1.9 c/s. 10 Detection LimitsThe minimum detectable count rate for a given band is ~0.4 c/s, for a source which passes through the centre of the detector and for typical background levels. A rough flux upper limit is then available by multiplying this count rate by the conversion factors specified below. This is for each band:-
11 Flux ConversionSource fluxes have been calculated from count rates based on energy conversion factors assuming a spectral model of an absorbed power-law with Nh = 3.0 * 10^20 cm2 and slope = 1.7 (see XMM science survey centre memo, SSC-LUX TN-0059 for a general description of the technique) The energy conversion factors used here are:
and convert between the source count rate (c/s) to flux in these energy bands in units of 10E-12 ergs/s/cm2 12 Reference"The first XMM-Newton slew survey catalogue: XMMSL1" R.D. Saxton, A.M. Read, P. Esquej, M.J. Freyberg, B. Altieri, D. Bermejo, 2008, A&A 480, 611
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