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FIRST - Faint Images of the Radio Sky at Twenty cm (FIRST) |
HEASARC Archive |
In this version of the catalog, images taken in the the new EVLA configuration have been re-reduced using shallower CLEAN thresholds in order to reduce the "CLEAN bias" in those images. Also, the EVLA images are not co-added with older VLA images to avoid problems resulting from the different frequencies and noise properties of the configurations. That leads to small gaps in the sky coverage at boundaries between the EVLA and VLA regions. As a result, the area covered by this release of the catalog is about 60 square degrees smaller than the earlier release of the catalog (13Jun05), and the total number of sources is reduced by nearly 25,000. The previous version of the catalog does have sources in the overlap regions, but their flux densities are considered unreliable due to calibration errors. The flux densities should be more accurate in this catalog, biases are smaller, and the incidence of spurious sources is also reduced.
Over most of the survey area, the detection limit is 1 mJy. A region along the equatorial strip (RA = 21.3 to 3.3 hrs, Dec = -1 to 1 deg) has a deeper detection threshold because two epochs of observation were combined. The typical detection threshold in this region is 0.75 mJy. There are approximately 4,500 sources below the 1 mJy threshold used for most previous versions of the catalog.
The format of this catalog is the same as releases since 13Jun05 but differs from earlier versions of the catalog. It contains two parameters which give information on the epoch of observation for each source (called mean_epoch and rms_epoch in this HEASARC version) which are described below. The P(S) parameter (called sidelobe_prob herein), which indicates the probability that the source is a sidelobe, replaces the previous binary sidelobe flag column. The parameters sdss_matches, sdss_first_offset, sdss_imag, sdss_class, twomass_matches, twomass_first_offset and twomass_kmag give information on counterparts to the FIRST source in the SDSS DR10 catalog and the 2MASS catalog, respectively. Other catalog parameters are common with FIRST catalog releases extending back over the past decade.
The co-added images are available online: see the FIRST page at http://sundog.stsci.edu/first/images.html for details. The source catalog presented here is derived from the images.
Data for the FIRST survey were collected in all VLA B-configurations from Spring 1993 through Spring 2004. For all data collected for the FIRST project, the raw u-v visibility data are placed in the VLA public archive on the day they are taken, and are available for use without restriction. Additional data in the southern Galactic cap were acquired in Spring 2009 and Spring 2011. The VLA was in a hybrid condition in 2009, with some new EVLA receivers and some old VLA receivers. The characteristics of those images are slightly different from the older data, but for most purposes they should be equivalent. In 2011 the EVLA receivers were available with an early version of the new EVLA data system, so there are a number of differences from the old data:
Date Frequencies Bandpass Integration Before 2011 1365, 1435 MHz 2x7 3-MHz channels 180 seconds 2011 1335, 1730 MHz 2x64 2-MHz channels 60 secondsNote particularly the frequency difference between the new and older data. The new data are in co-added fields with names ending with 'S' (and later letters in the alphabet) and are found entirely in the south Galactic cap.
The Last of FIRST: The Final Catalog and Source Identifications Helfand D.J., White R.L., Becker R.H. <Astrophys. J. 801, 26 (2015)> =2015ApJ...801...26H The FIRST Survey Catalog of 1.4GHz radio sources White R.L., Becker R.H., Helfand D.J., Gregg M.D. <Astrophys. J. 475, 479 (1997)> =1997ApJ...475..479WSee also:
http://sundog.stsci.edu/ : home page of the VLA FIRST Survey http://sundog.stsci.edu/first/catalogs/history.html : Version History http://sundog.stsci.edu/cgi-bin/searchfirst : the FIRST search engine http://third.ucllnl.org/cgi-bin/firstcutout : the FIRST cutout server http://www.cv.nrao.edu/first/ : FIRST page at NRAO
Survey Characteristic Percentage SDSS 1 or more counterparts < 8" 54.5% SDSS Counterpart < 1.5" 28.3% SDSS Covered by DR10 93.0% 2MASS 1 or more counterparts < 8" 11.6% 2MASS Counterpart < 1.5" 7.5%
Name
The full FIRST Source Designation (not part of the original catalog
as created by its authors): the source name was constructed by the HEASARC
according to the rule recommended by the CDS Dictionary of Nomenclature of
Celestial Objects and registered by the authors with the IAU, viz. the prefix
'FIRST J' followed by the truncated (not rounded) J2000.0 positional
coordinates.
RA
The Right Ascension of the radio source in the selected equinox: this
was given in J2000 equatorial coordinates with a precision of 0.001 seconds
of time in the original catalog. The accuracy of the position depends
on the brightness and size of the source and the noise in the map. Point
sources at the detection limit of the catalog have positions accurate to
better than 1 arcsecond at 90% confidence; 2 mJy point sources in typically
noisy regions have positions good to 0.5 arcseconds.
An empirical expression for the positional accuracy, epsilon, is
epsilon(90% confidence) = Size * (1/SNR + 1/20) arcsecondswhere Size is either the major or minor axis fitted FWHM (fit_major_axis or fit_minor_axis) as given in the catalog and SNR is the peak flux density, Fpeak, signal-to-noise ratio given by SNR = (Fpeak - 0.25) / rms. The positional uncertainty is, of course, elliptical for elliptical sources. The best possible positional uncertainty is limited to about 0.1 arcseconds by the ability to fit source positions in maps with 1.8 arcsecond pixels and by various random calibration uncertainties. Systematic errors in the positions are smaller than 0.05 arcseconds.
Dec
The Declination of the radio source in the selected equinox: this
was given in J2000 equatorial coordinates with a precision of 0.01 arcseconds
in the original catalog. The accuracy of the position depends
on the brightness and size of the source and the noise in the map. Point
sources at the detection limit of the catalog have positions accurate to
better than 1 arcsecond at 90% confidence; 2 mJy point sources in typically
noisy regions have positions good to 0.5 arcseconds.
An empirical expression for the positional accuracy, epsilon, is
epsilon(90% confidence) = Size * (1/SNR + 1/20) arcsecondswhere Size is either the major or minor axis fitted FWHM (fit_major_axis or fit_minor_axis) as given in the catalog and SNR is the peak flux density, Fpeak (flux_20_cm in this table), signal-to-noise ratio given by SNR = (Fpeak - 0.25) / rms. The positional uncertainty is, of course, elliptical for elliptical sources. The best possible positional uncertainty is limited to about 0.1 arcsecond by the ability to fit source positions in maps with 1.8 arcsecond pixels and by various random calibration uncertainties. Systematic errors in the positions are smaller than 0.05 arcseconds.
LII
The Galactic Longitude of the radio source.
BII
The Galactic Latitude of the radio source.
Sidelobe_Prob
The probability P(S) that the radio source is spurious,
most commonly because it is a sidelobe of a nearby bright source.
Low values for this parameter mean the source is unlikely to be spurious.
Here is the distribution of P(S) values in this version of the catalog:
Probability Range Fraction of sources 0.00 < P(S) < 0.05 76.3% 0.05 < P(S) < 0.15 7.0% 0.15 < P(S) < 0.25 4.4% 0.25 < P(S) < 0.35 3.5% 0.35 < P(S) < 0.45 2.1% 0.45 < P(S) < 0.55 1.7% 0.55 < P(S) < 0.65 1.6% 0.65 < P(S) < 0.75 1.5% 0.75 < P(S) < 0.85 1.1% 0.85 < P(S) < 0.90 0.8%Sidelobe probabilities for this version of the catalog have been computed using an improved algorithm based on multiple voting oblique decision tree classifiers. The classifiers were trained using deep VLA fields that give reliable assessments of the reality of FIRST sources. The algorithm is described in detail in Section 4 of the 2015 reference paper on the final FIRST catalog cited above; the authors believe it is a substantial improvement over the previous sidelobe flagging approach. Nevertheless, they still recommend checking the images using the FIRST Cutout Server at http://third.ucllnl.org/cgi-bin/firstcutout if there is any doubt about the reality of particular sources.
Flux_20_cm
The peak flux density at 1.4 GHz, in milliJanskies per beam (mJy/beam).
The peak and integrated flux densities are derived by fitting an elliptical
Gaussian model to the source. To correct for the "CLEAN bias" effect,
0.25 mJy has been added to the peak flux density and the integrated flux
density has been multiplied by (1+0.25/Fpeak) (see the published papers
for more details).
The uncertainty in the peak flux density is given by the rms noise at the source position, while the uncertainty in the integrated flux density can be considerably greater, depending on the source size and morphology. For bright sources the accuracies of the peak and integrated flux densities are limited to about 5% by systematic effects.
Int_Flux_20_cm
The integrated flux density at 1.4 GHz, in milliJanskies (mJy). The peak and
integrated flux densities are derived by fitting an elliptical Gaussian model
to the source. To correct for the 'CLEAN bias' effect, 0.25 mJy has been
added to the peak flux density and the integrated flux density has been
multiplied by (1+0.25/Fpeak) (see the published papers for more details).
The uncertainty in the peak flux density is given by the rms noise at the source position, while the uncertainty in the integrated flux density can be considerably greater, depending on the source size and morphology. For bright sources the accuracies of the peak and integrated flux densities are limited to about 5% by systematic effects. Note that, for sources that are not well-described by an elliptical Gaussian model, the integrated flux density calculated as above is not an accurate measure of the actual integrated flux density.
Flux_20_cm_Error
The estimated error in the flux density, in milliJanskies per beam
(mJy/beam), is a local rms noise estimate at the source position. The rms is
computed by combining the measured noise from all grid pointing images
contributing to this co-added map position. Note that the significance of
detection for a source is (Fpeak - 0.25)/rms, not Fpeak / rms, because of
the CLEAN bias correction to the peak flux density, Fpeak. The catalog
includes only sources brighter than 5 times the rms.
FITS images giving the rms noise as a function of position on the sky are available for the northern and the southern areas at http://sundog.stsci.edu/first/catalogs/coverage-north-3arcmin-14dec17.fits and http://sundog.stsci.edu/first/catalogs/coverage-south-3arcmin-14dec17.fits, respectively. These images give the rms in mJy/beam tabulated on a ~3 arcmin grid in RA and Declination. If there is no source in the catalog at a given position, the source peak flux density (before CLEAN bias correction) is less than 5 times the coverage map rms value at that position. The coverage in the southern Galactic cap is ragged (and discontiguous) at the northern edge because poor weather and equipment failures prevented the planned survey area from being filled in there. Small gaps can be seen around the edges of the area observed using the EVLA configuration in 2011, as noted in the Overview above.
Major_Axis
The major axis FWHM, in arcseconds. The parameters major_axis, minor_axis,
and position_angle (measured in degrees, east of north) are derived from the
elliptical Gaussian model for the source. The major_axis and minor_axis are
the values after deconvolution to remove blurring by the elliptical Gaussian
point-spread function. (The fitted parameters before deconvolution are given
in the fit_major_axis, fit_minor_axis, and fit_position_angle parameter). In
the north, the beam is circular, with a 5.4 arcsec FWHM, south of declination
+4 degrees 33' 21", the beam is elliptical, with a 6.4" x 5.4" FWHM, with the
major axis running north-south, while in the southern Galactic cap (RA = 21
hrs to 3 hrs), the elliptical beam size increases further to 6.8" x 5.4"
south of declination -2 degrees 30' 25".
Noise can cause the fitted values of the major and minor axes (before deconvolution) to be smaller than the beam. The corresponding deconvolved size is given as zero in those cases.
The uncertainties in the deconvolved sizes depend on both the brightness and the sizes. Objects at the catalog flux density limit have uncertainties of about 2 arcsec in their sizes (so faint objects with major_axis <2 arcsec are consistent with point sources). A simple empirical estimate of the uncertainty is Sigma(Size) = 10 arcsec * (1/SNR + 1/75), where SNR is the signal-to-noise ratio defined as SNR = (Fpeak - 0.25) / rms.
Minor_Axis
The minor axis FWHM, in arcseconds. The parameters major_axis, minor_axis,
and position_angle (measured in degrees, east of north) are derived from the
elliptical Gaussian model for the source. The major_axis and minor_axis are
the values after deconvolution to remove blurring by the elliptical Gaussian
point-spread function. (The fitted parameters before deconvolution are given
in the fit_major_axis, fit_minor_axis, and fit_position_angle parameter). In
the north, the beam is circular, with a 5.4 arcsec FWHM, south of declination
+4 degrees 33' 21", the beam is elliptical, with a 6.4" x 5.4" FWHM, with the
major axis running north-south, while in the southern Galactic cap (RA = 21
hrs to 3 hrs), the elliptical beam size increases further to 6.8" x 5.4"
south of declination -2 degrees 30' 25".
Noise can cause the fitted values of the major and minor axes (before deconvolution) to be smaller than the beam. The corresponding deconvolved size is given as zero in those cases.
The uncertainties in the deconvolved sizes depend on both the brightness and the sizes. Objects at the catalog flux density limit have uncertainties of about 2 arcsec in their sizes (so faint objects with major_axis <2 arcsec are consistent with point sources). A simple empirical estimate of the uncertainty is Sigma(Size) = 10 arcsec * (1/SNR + 1/75), where SNR is the signal-to-noise ratio defined as SNR = (Fpeak - 0.25) / rms.
Position_Angle
The position angle of the major axis, in degrees, measured in an eastwards
direction from north. The parameters major_axis, minor_axis, and
position_angle (measured in degrees, east of north) are derived from the
elliptical Gaussian model for the source. The major_axis and minor_axis are
the values after deconvolution to remove blurring by the elliptical Gaussian
point-spread function. (The fitted parameters before deconvolution are given
in the fit_major_axis, fit_minor_axis, and fit_position_angle parameter). In
the north, the beam is circular, with a 5.4 arcsec FWHM, south of declination
+4 degrees 33' 21", the beam is elliptical, with a 6.4" x 5.4" FWHM, with the
major axis running north-south, while in the southern Galactic cap (RA = 21
hrs to 3 hrs), the elliptical beam size increases further to 6.8" x 5.4"
south of declination -2 degrees 30' 25".
Noise can cause the fitted values of the major and minor axes (before deconvolution) to be smaller than the beam. The corresponding deconvolved size is given as zero in those cases.
The uncertainties in the deconvolved sizes depend on both the brightness and the sizes. Objects at the catalog flux density limit have uncertainties of about 2 arcsec in their sizes (so faint objects with major_axis < 2 arcsec are consistent with point sources). A simple empirical estimate of the uncertainty is Sigma(Size) = 10 arcsec * (1/SNR + 1/75), where SNR is the signal-to-noise ratio defined as SNR = (Fpeak - 0.25) / rms.
Fit_Major_Axis
The fitted major axis before deconvolution, in arcseconds. fit_major_axis,
fit_minor_axis, and fit_position_angle give the major and minor axes (FWHM in
arcsec) and position angle (in degrees, measured eastwards from the north)
derived from the elliptical Gaussian model for the source. These are the
fitted sizes measured directly from the image; the elliptical point-spread
function has not been deconvolved.
Fit_Minor_Axis
The fitted minor axis before deconvolution, in arcseconds. fit_major_axis,
fit_minor_axis, and fit_position_angle give the major and minor axes (FWHM in
arcsec) and position angle (in degrees, measured eastwards from the north)
derived from the elliptical Gaussian model for the source. These are the
fitted sizes measured directly from the image; the elliptical point-spread
function has not been deconvolved.
Fit_Position_Angle
The position angle of the fitted major axis, in degrees measured eastwards
from the north. fit_major_axis, fit_minor_axis, and fit_position_angle give
the major and minor axes (FWHM in arcsec) and position angle derived from the
elliptical Gaussian model for the source. These are the fitted sizes measured
directly from the image; the elliptical point-spread function has not been
deconvolved.
Field_Name
This is the name of the co-added image containing the source. Note that the
field name encodes the position of the field center: thus, field hhmmm+ddmmm
is centered at RA=hh mm.m, Dec=+dd mm.m. The images are available from
several archives and through the FIRST Cutout Server at
http://third.ucllnl.org/cgi-bin/firstcutout. All field names in the current
catalog end with a letter E through X, depending on the date of the last
catalog release in which the image was modified. The W and X fields are new
in this catalog, while sources extracted from the E-T fields are essentially
identical to those in the previous version of the catalog. The W fields
include contributions from EVLA data taken in Spring 2011 and have both a
slightly different central frequency (1.335 GHz instead of 1.400 GHz) and
typically higher noise levels than the older images. The X fields are images
that neighbor the EVLA fields but differ from the previous release in that
they omit nearby EVLA observations from the co-adding of overlapping grid
images.
SDSS_Matches
The number of potential optical counterparts to the radio source in the Sloan
Digital Sky Survey (SDSS) DR10 within a fiducial radius of 8 arcseconds. The
SDSS matches were found using the SDSS-III CasJobs web interface at
http://skyservice.pha.jhu.edu/casjobs/. A count of zero indicates there are
no sources within this radius (which is also indicated by a null value for
the corresponding offset and a classification of '-'). A count of -1
indicates that the FIRST source falls outside the SDSS DR10 survey area so
that no SDSS data are available. The SDSS catalog has multiple wavebands
available; the given magnitude herein is for the i band. An SDSS i magnitude
of -1 indicates that the magnitude in the DR10 catalog was given as -9999.
SDSS_FIRST_Offset
The angular offset or separation of the nearest matching SDSS source from the
FIRST radio source, in arcseconds.
SDSS_Imag
The i magnitude of the nearest matching SDSS source. A magnitude of -1
indicates that the magnitude in the DR10 catalog was given as -9999.
SDSS_Class
The morphological classification of the nearest matching SDSS source, where
's' stands for stellar and 'g' for non-stellar/galaxy.
TwoMASS_Matches
The number of potential infrared counterparts to the radio source in the
2MASS Catalog within a fiducial radius of 8 arcseconds. The 2MASS matches
were found using the SDSS-III CasJobs web interface at
http://skyservice.pha.jhu.edu/casjobs/. A count of zero indicates there are
no sources within this radius (which is also indicated by a null value for
the corresponding offset and a classification of '-'). The 2MASS catalog has
multiple wavebands available; the given magnitude herein is for the K band.
TwoMASS_FIRST_Offset
The angular offset or separation of the nearest matching 2MASS source from
the FIRST radio source, in arcseconds.
TwoMASS_Kmag
The K magnitude of the nearest matching 2MASS source.
Mean_Epoch
The mean epoch of the FIRST flux density measurement of the source. The FIRST
survey consists of 3-minute integrations at a grid of points on the sky. But
the catalogs are derived from co-added images that use a weighted sum of the
individual pointing maps to achieve nearly uniform sensitivity. (See the
FIRST survey papers for more details.) That means that each measurement is a
weighted sum of multiple observations. The mean_epoch give the weighted mean
of all the contributing pointing epochs at the position of the source.
RMS_Epoch
The rms of the FIRST flux density measurement of the source, in days.
This parameter gives the weighted rms of the pointing epochs at the source
position. It is a measure of the spread in epochs that contribute to the
measurement. Many sources have small rms values of only a few minutes
(dominated by a single 3-minute pointings or by 2 adjacent pointings), but
values of days to weeks are also common (for sources observed in the overlap
between declination strips), and some objects have rms values of years (for
sources observed at the edges of regions in different observing seasons or
that were observed multiple times due to data problems). The largest epoch
rms in the survey is 6.8 years.
The epoch rms should be used as a guide to identify objects that do not have well-defined epochs. The table below gives an indication of the frequency of different epoch rms values in the catalog:
Epoch rms range Fraction < 5 minutes 5% 5 min - 1 day 29% 1 - 10 days 44% 10 - 100 days 11% 100 days - 1 yr 7% 1 - 2 yrs 1% 2 - 5 yrs 2% > 5 yrs 0.3%