Astron. Astrophys. 341, 44-57 (1999)
2. The GPS source B1144+352
The GPS nature of the radio source B1144+352 was first recognized
by Snellen et al. (1995, hereafter S95), who find that the radio
spectrum peaks at 2.4 GHz, with a spectral index of
in the optical thick (low frequency) part of
the radio spectrum, and a spectral index of -0.56 in the optical thin
part. These values should be treated with care, however, because of
the variability of the central source (see also Sect. 4.1) and the
large time spanned by the observations used in obtaining them.
The radio source has been identified with the galaxy CGCG 186-048
(Zwicky et al. 1960-1968). The Gunn r-band magnitude of the
host galaxy is (Snellen et al. 1996) and it has
a redshift of 0.0630 (Colla et al. 1975a; Hewitt & Burbidge 1991).
This makes it one of the nearest GPS galaxies known. The absolute
magnitude in the Gunn r-band is , using the
K-correction as given in Snellen et al. (1996). The optical spectrum
shows bright narrow emission lines, typical for powerful radio
sources, on top of a starlight dominated continuum (Marcha et al.
1996). There is no hint of a non-thermal continuum or of broad Balmer
emission lines, hence the classification as a GPS galaxy. An optical
R-band CCD image can be found in Snellen et al. (1996). Fig. 1
presents a contour plot of the host galaxy from the Digitized Sky
Survey (DSS). The host galaxy appears to have a small companion galaxy
at a projected distance of kpc
( ) to the west. This is close to the median
distance at which apparent companions were found in a sample of GPS
galaxies by O'Dea et al. (1996a). From the DSS it is apparent that
CGCG 186-048 is the brightest galaxy within a radius of at least
1 Mpc ( ). There is no indication that it is
a member of a rich cluster, although there are several fainter (R-band
magn. ) galaxies within a radius of a few
hundred kpc. More likely, it is situated in a poor group of
galaxies.
![[FIGURE]](img30.gif) |
Fig. 1.
Contourplot of the host galaxy of the GPS source B1144+352 from the DSS. The contours are drawn at logarithmic intervals of , starting at three times the background noise level. The cross at the center of the host galaxy gives the position of the GPS source. Its size is not related to the positional uncertainty which is only .
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VLA maps of the GPS source at 1.4 GHz are presented by Parma et al.
(1986) and S95. Both were obtained using the same configuration and
have a resolution of arcsec. The GPS source
appears as a strong unresolved point-source. However, the maps also
show a long weak jet-like feature emanating
from the radio core, and a shorter ( ) and
somewhat weaker counter-jet. The total linear size of this extended
system is kpc. S95 note that the flux density
from the 20-cm Green Bank survey (White & Becker 1992) is higher
(by mJy) than that from their VLA observations.
Since the Green Bank survey has a beamsize of
(FWHM), they attribute this difference to a radio source component
extending even beyond the observed jet-like feature. The fractional
polarization of the core, obtained from high resolution 8.4-GHz VLA
observations, is 3% at a -level (Marcha et al.
1996).
A VLBI map of the central source is presented by Henstock et al.
(1995). It shows a pc large double radio
structure, with one well resolved bright radio lobe-like component and
an unresolved second component. The position angle of the radio axis
is , counted counter-clockwise (CCW) from the
North. Giovannini et al. (1995) find that the two components are
separating from each other superluminally with an apparent velocity of
. This is surprising since GPS galaxies in
general do not show superluminal motion (Stanghellini et al.
1997).
Giovannini et al. (1990) report that the flux density of the peak
in the radio spectrum (the peak flux density) has continuously
increased from mJy in 1974 to
mJy in 1990. S95 and Snellen et al. (1998)
claim that it has decreased again somewhat thereafter. Snellen et al.
(1998) further state that the brightest (eastern) VLBI component,
which has a radio lobe-like morphology, must be largely responsible
for the observed change in the peak flux density. Variability in the
flux density has been found in other GPS sources, but mostly in GPS
quasars (e.g. Stanghellini et al. 1998).
© European Southern Observatory (ESO) 1999
Online publication: November 26, 1998
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