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ATESP1P4GH - Australia Telescope ESO Slice Project 1.4-GHz Source Catalog |
HEASARC Archive |
This table contains the list of 6-sigma or more sources detected in the ATESP survey. For composite sources with multiple components, the individual components each have entries in this table, and there is also an entry for the entire source. Based on the numbers quoted above, this would imply that there should be (2960 + 2*168 + 3*19 + 4*2) = 3361 entries in this table. The HEASARC notes that there are actually 3370 entries in the CDS version of this table that the present table is based on, 169 of which are doubles, 19 triples and 2 quadruples, implying that this version has 2967 sources, slightly more than the number quoted in the reference paper.
The ATESP radio survey. II. The source catalogue. Prandoni I., Gregorini L., Parma P., De Ruiter H.R., Vettolani G., Wieringa M.H., Ekers R.D. <Astron. Astrophys. Suppl. Ser. 146, 41 (2000)> =2000A&AS..146...41P
Name
The source designation as given in the reference paper using the prefix
'ATESP' for Australia Telescope ESO Slace Project together with the J2000.0
equatorial coordinates of the source, e.g., 'ATESP JHHMMSS+DDMMSS(A,B,C,D)',
where the trailing letters A, B, C and D are used to refer to individual
components of multiple sources.
RA
The Right Ascension of the radio source or component in the selected
equinox. The RA was given in J2000.0 coordinates to a precision of 0.01 seconds
of time in the original table. Source positions for composite sources have
been defined as the flux-weighted average position of all the components
(source centroid). For sources with more than two components, the centroid
position has been replaced with the core position whenever the core is clearly
recognizable.
Dec
The Declination of the radio source or component in the selected
equinox. The RA was given in J2000.0 coordinates to a precision of 0.1
arcseconds in the original table. Source positions for composite sources have
been defined as the flux-weighted average position of all the components
(source centroid). For sources with more than two components, the centroid
position has been replaced with the core position whenever the core is clearly
recognizable.
LII
The Galactic Longitude of the radio source or component.
BII
The Galactic Latitude of the radio source or component.
Flux_1p4_GHz
The 1.4-GHz peak flux density of the radio source or
component, in milliJansky per beam (mJy/beam), on the Baars et al. (1977, A&AS,
61, 99) scale. The values given here are not corrected for the systematic
effects described in Section 4.2 of the reference paper.
Int_Flux_1p4_GHz
The 1.4-GHz integrated flux density of the radio source or
component, in milliJansky (mJy). Integrated total source flux densities for
composite sources are computed by summing all the component integrated fluxes.
Major_Axis
The intrinsic (deconvolved from the beam) major axis (FWHM) of the Gaussian
fit to the radio source or component, in arcseconds. Zero values refer to
unresolved sources (see Section 3.1 of the reference paper for more details).
For entries describing the summed components of composite sources (entries
with fit_quality_flag = 'M'), the total source angular size is given instead.
This is defined as the largest angular size (las: see Section 2.3 of the
reference paper) and it is computed as the maximum distance between the
source components.
Minor_Axis
The intrinsic (deconvolved from the beam) minor axis (FWHM) of
the Gaussian fit to the radio source or component, in arcseconds. Zero values
refer to unresolved sources (see Section 3.1 of the reference paper for more
details). This is left blank for entries describing the summed components of
composite sources
Position_Angle
The deconvolved position angle of the the Gaussian fit to
the radio source, in degrees, measured from North through East. Zero values
refer to unresolved sources (see Section 3.1 of the reference paper).
This is left blank for entries describing the summed components of
composite sources
Fit_Quality_Flag
This parameter contains a flag indicating the fitting
procedure and parametrization adopted for the source or source component (see
Sections 2.3 and 3.2 of the reference paper), coded as follows:
S refers to Gaussian fits, P refers to poor Gaussian fits, (changed from S* in the original table), E refers to non-Gaussian sources. M refers to multiple sources (see below).The parameters listed for non-Gaussian sources are defined as discussed in Section. 2.3 of the reference paper. For multiple sources, the table lists all of the components as separate entries (labeled 'A', 'B., etc.) and also has an entry (flagged as 'M') giving the position of the radio centroid, total flux density and overall angular size of the entire source. Source positions for composite sources have been defined as the flux-weighted average position of all the components (source centroid). For sources with more than two components, the centroid position has been replaced with the core position whenever the core is clearly recognizable. Integrated total source flux densities for composite sources are computed by summing all the component integrated fluxes. The total source angular size for composite sources is defined as the largest angular size (las: see Section 2.3 of the reference paper) and it is computed as the maximum distance between the source components.