However, it is likely that the 3C sample, although it makes finding galaxies at high redshift easy, is not a representative sample of high-redshift galaxies because the presence of powerful radio AGN affects the properties of the optical galaxy. Specifically, the discovery of UV-optical extended continuum (McCarthy et al. 1987) aligned with the radio axis is evidence for very strong interaction between the radio jet and the intragalactic medium. It has been claimed (Dunlop & Peacock 1993) that this alignment effect tends to disappear at radio powers only a factor 5-10 lower than the 3C survey. In this case we might expect to pick up passively evolving giant ellipticals by selecting lower-luminosity radio galaxies. There is, however, much debate about this point (e.g. Eales & Rawlings 1996).
These observations are part of an ongoing project
(Rhee et al. 1996;
hereafter Paper I)
to identify and study radio galaxies and quasars
from the 4C survey
(Pilkington & Scott 1965;
Gower et al. 1967)
between declinations
of and
.
The 4C survey is approximately a
factor of 5 deeper
than the 3C survey, and has a limiting
flux density of 2 Jy at 178 MHz.
In order to get
a complete sample, large enough to
study the properties of distant
galaxies, to
determine their space density and to
be able to compare the properties
of the steep
spectrum radio galaxies with those
of normal radio galaxies and quasars,
we selected
the 4C sources whose angular sizes are
smaller than 30 arcseconds using
the 365-MHz
Texas survey
(Douglas et al. 1980).
Our selection is independent of the radio spectral
index and the
complete radio sample will be published elsewhere.
The subset of the 4C sample whose
declinations are between
and
has a lot of radio observations,
providing good radio
spectral indices and has the advantage
of being observable from both
hemispheres. In this article,
we have concentrated on steep radio spectrum
objects which are not identified
on the Palomar Sky Survey in
order to improve positional information
for followup optical spectroscopy. The sources
have also been selected, as in Paper I, to have
angular sizes of less than 30
.Here we present radio maps of a
further 144 radio sources (19 of which are common
with Paper I). The sources were chosen
as far as possible to complete the mapping of
RA ranges according to the LST ranges at which
the observations were
scheduled. Hence most sources have
,
,
and
.
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