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LD7C151MHZ - 7C 151-MHz Low-Declination Survey Catalog |
HEASARC Archive |
The 7C Survey of Radio Sources at 151 MHz - a region covering RA 9h to 16h and Dec 20 deg to 35 deg. Waldram E.M., Yates J.A., Riley J.M., Warner P.J. <Mon. Not. R. Astron. Soc. 282, 779 (1996)> =1996MNRAS.282..779W
Name
The source designation adopted by the HEASARC, viz., '7C
HHMMSS.s+DDMMSS', where the numerical part of the name is the B1950.0
beam-fitted position of the radio source. Sometimes, a truncated version of
this naming convention, viz., '7C HHMM+DDMMa' has been used, but the HEASARC
has adopted the higher precision position-based naming convention that is
now recommended for the primary 7C catalog.
RA
The Right Ascension of the beam-fitted position of the radio source in
the selected
equinox. This was given in B1950.0 equatorial coordinates in the original table
to a precision of 0.1 seconds of time. The rms (1-sigma) accuracy of the
beam-fitted RA is approximately sqrt[22 + (40/SNR)2] arcseconds,
where the 2 arseconds part is the error introduced by random phase errors,
and the (40/SNR) part is the error due to source confusion and noise.
Dec
The Declination of the beam-fitted position of the radio source in the
selected
equinox. This was given in B1950.0 equatorial coordinates in the original table
to a precision of 1 arcsecond. The rms (1-sigma) accuracy of the
beam-fitted Dec is approximately 1.3 cosec(Dec) times the rms error in
RA: the dependence on Declination increases more rapidly than the expected
factor of cosec(Dec) because of the effects of the distortion of the beam
shape and confusion.
LII
The Galactic Longitude of the beam-fitted position of the radio source.
BII
The Galactic Latitude of the beam-fitted position of the radio source
Centroid_RA
The Right Ascension of the centroid position of the radio
source in the selected
equinox. This was given in B1950.0 equatorial coordinates in the original table
to a precision of 0.1 seconds of time. Multiple peaks which have been
integrated together have the same centroid position.
Centroid_Dec
The Declination of the centroid position of the radio
source in the selected
equinox. This was given in B1950.0 equatorial coordinates in the original table
to a precision of 1 arcsecond. Multiple peaks which have been
integrated together have the same centroid position.
Flux_151_MHz
The beam-fitted flux density Sbf of the radio source at 151
MHz, in mJy/beam (converted by the HEASARC from the Jy/beam units used in the
original table). Monte Carlo analysis showed that, in the absence of phase
errors, the fractional errors in Sbf are given by the inverse of the
signal-to-noise ratio, 1/SNR. The effects of random phase errors limit the
accuracy fo high-SNR (>= 40) sources to 2-3 percent.
Int_Flux_151_MHz
The integrated flux density Sin of the radio source at
151 MHz, in mJy (converted by the HEASARC from the Jy units used in the
original table). The errors in Sin are a factor of ~ 1.5 times larger than
those of the beam-fitted flux values; this factor increases to ~ 3 for the
lowest Declinations mainly because of the effects of confusion. A conservative
estimate of the integrated flux density errors for the sources with SNR > 15
is around 10 per cent.
SNR
The signal-to-noise ratio SNR of the radio source as defined by
Waldram and Riley (1993, MNRAS, 265, 853), i.e., the interpolated peak
height of the source on the map (after subtraction of the local zero
level), divided by the local noise. The minimum SNR value for sources
in this table is 5.5.
Source_Extent
The extent of the source size in units of the local beam
area. This estimate is influenced by residual ionospheric smearing of the
synthesized beam. Another measure of whether a source is resolved
or not is the ratio of the integrated to beam-fitted flux densities,
Sin/Sbf. The flux density calibration is performed in
such a way as to ensure that the median value of this ratio for
unresolved sources is unity. Thus, any source with this ratio >> 1 is
resolved, and, for this survey, a ratio of Sin/Sbf >= 1.3 is a more
robust indication that the source is resolved.
Num_Local_Max
The number m of individual peaks that were included in the
flux integration. For multiple sources, each peak has a separate
entry in this source list, with its own beam-fitted flux density and
position, although the integrated flux, the centroid position, the source
extent and m are the same for each such entry.