Issue |
A&A
Volume 518, July-August 2010
Herschel: the first science highlights
|
|
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Article Number | A33 | |
Number of page(s) | 13 | |
Section | Extragalactic astronomy | |
DOI | https://doi.org/10.1051/0004-6361/201014400 | |
Published online | 27 August 2010 |
Radio polarimetry of 3C 119, 3C 318, and 3C 343 at milliarcsecond resolution
F. Mantovani1 - A. Rossetti1 - W. Junor2 - D. J. Saikia3,4 - C. J. Salter5
1 - Istituto di Radioastronomia - INAF, via Gobetti 101,
40129 Bologna, Italy
2 - Los Alamos National Laboratory, Los Alamos, NM 87545, USA
3 - National Centre for Radio Astrophysics, TIFR, Post Bag 3,
Ganeshkhind, Pune 411 007, India
4 - ICRAR, University of Western Australia, Crawley, WA 6009, Australia
5 - Arecibo Observatory, HC3 Box 53995, Arecibo, Puerto Rico 00612
Received 10 March 2010 / Accepted 4 May 2010
Abstract
Aims. We report new Very Long Baseline Array (VLBA)
polarimetric observations of the compact steep-spectrum (CSS) sources
3C 119, 3C 318, and 3C 343 at 5 and 8.4 GHz.
Methods. We analysed our VLBA observations and derived
milliarcsecond-resolution images of the total intensity, polarisation,
and rotation measure (RM) distributions.
Results. The CSS source 3C 119, associated with a possible quasar, has source rest-frame RM values up to 10 200 rad m-2 in a region that coincides with a change in the direction of the inner jet. This component is located
325 pc
from the core, which is a variable source with a peaked radio spectrum.
For 3C 318, which is associated with a galaxy, a rest-frame RM of
3030 rad m-2
was estimated for the brightest component contributing almost all
of the polarised emission. Two more extended components were detected,
that contain ``wiggles'' in the jet towards the southern side of the
source. The CSS source 3C 343 contains two peaks of emission and a
curved jet embedded in more diffuse emission. It exhibits complex field
directions close to the emission peaks, which are indicative of
rest-frame RM values in excess of
6000 rad m-2. The locations of the cores in 3C 318 and 3C 343 are unclear.
Conclusions. The available data about mas-scale rest-frame RM estimates for CSS sources show that these have a wide range of values extending up to 40 000 rad m-2 in the central region of OQ172, and may be located at projected distances from the core of up to
1600 pc, as in 3C 43 where this feature has a rest-frame RM of
14 000 rad m-2. The RM
estimates for the cores of core-dominated radio sources indicate that
in addition to responding to an overall density gradient of the
magneto-ionic medium, geometry, orientation, and modes of fuelling may
also play a significant role. In addition to these effects, the high
values of RM in CSS sources are possibly caused by dense clouds
of gas interacting with the radio jets. The observed distortions in the
radio structures of many CSS sources are consistent with this
interpretation.
Key words: polarization
1 Introduction
The number of compact steep-spectrum (CSS) sources with detailed polarimetric information available at milliarcsecond resolution remains small. Polarised radio emission from CSS radio galaxies is either very weak or below the detection limits at centimetre wavelengths. In contrast, CSS quasars have linear polarisation percentages of up to 10% above 1 GHz (Rossetti et al. 2008, and references therein). We have conducted a series of observations of CSS sources with significantly polarised emission and high values of rotation measure (RM) using the Very Long Baseline Array (VLBA).Table 1: VLBA+VLA1 observing parameters.
The CSS objects are young radio sources with ages <
yr.
They have linear sizes
20 kpc
and steep high-frequency radio spectra (
;
). Being subgalactic in size, CSS sources
reside deep within their host galaxies. Therefore, Faraday
rotation effects are to be expected when their polarised synchrotron
emission is observed through the host galaxy magneto-ionic
interstellar medium (ISM). The comparison of polarised emission
over a range of wavelengths is an important diagnostic of the physical
conditions within and around these compact radio sources (see Cotton
et al. 2003c, for an overview).
Existing subarcsec polarimetry has provided evidence in favour of the interaction of components of CSSs with dense clouds of gas, as seen for example in the CSS quasar 3C 147 (Junor et al. 1999).
Results for the first two CSS quasars observed in our ongoing program, B0548+165 and B1524-136, are available in Mantovani et al. (2002), while those for 3C 43 (B0127+233) are to be found in Mantovani et al. (2003). The results for 3C 147 (B0538+498) were presented by Rossetti et al. (2009). These sources have all been imaged with milliarcsecond resolution by means of full-Stokes VLBA observations.
In this paper, we report on multi-frequency VLBA, in addition to single Very Large Array (VLA) antenna, polarisation observations at 5 and 8.4 GHz for 3C 119 (B0429+415), 3C 318 (B1517+204), and 3C 343 (B1634+628).
In Sect. 2, we summarise the observations and data processing. Section 3 describes the new information obtained about the structural and polarisation properties of 3C 119, 3C 318, and 3C 343. Discussion and conclusions are presented in Sects. 4 and 5, respectively.
2 Observations and data reduction
Polarimetric observations of 3C 119, 3C 318, and
3C 343 using the VLBA and one VLA antenna were carried out
at 5 and 8.4 GHz as detailed in Table 1. The
data were recorded in both right- and left-circular polarisation in
four 8-MHz bands. At 5 GHz, these bands were spread across the
available bandwidth of 500 MHz, allowing us to obtain truly
simultaneous, independent, polarisation images. Only two of the
four sub-bands could make use of the VLA antenna in the array due to
limitations in the available VLA 5 GHz system. To
increase the sensitivity to polarised emission at 8.4 GHz, we chose
to use contiguous IFs for this band.
The data were correlated with the National Radio Astronomy Observatory (NRAO)
VLBA processor at Socorro and
calibrated, imaged, and analysed using the AIPS package. The flux
density and polarisation calibrations were performed following the procedure
described in Rossetti et al. (2009) for the source 3C 147 observed using the
same system setup. The flux density calibration
uncertainty is .
The compact polarised sources
DA 193, 3C 345, and 3C 380 were used to
determine the instrumental polarisation (``D-term'') using the AIPS
task PCAL. The solution showed that the instrumental polarisation was
typically about of the order of
.
3 Results
3.1 3C 119
At different times, the radio source 3C 119 was optically identified as
either a galaxy or a quasar, as noted by Fanti
et al. (1990), who classified it as a quasar. Its light is
dominated by its nucleus, which has a morphology more typical of CSS quasars
(de Vries et al. 1997). It has a reasonably broad H
profile and we
presently classify it as a possible quasar. It has mv=20 and
z=1.023 (Eracleous & Halpern 1994), so that 1 mas corresponds to 8.086 pc.
A MERLIN polarimetric image of 3C 119 at 5 GHz was obtained by
Lüdke et al. (1998), who studied a sample of CSS sources. At their
resolution, it appears barely resolved. Lüdke et al. pointed out
that it exhibits extremely rapid depolarisation between 8.4 and 5 GHz.
This was confirmed by Mantovani et al. (2009), who detected
polarised emission of 8.8 and 5.9 % at 10.45 and 8.35 GHz
respectively, whereas at 4.85 GHz the polarisation was below the
detection limit (
110 mJy, corresponding to about 2.7%) of their
Effelsberg 100-m telescope observations.
The first VLBI images of 3C 119 with resolutions 10 mas were
acquired by Fanti et al. (1986) at 18 and 6 cm. They found at least four
components embedded in a complex, spiral, filamentary structure
suggesting that the low brightness emission was distributed in
filaments surrounding the brighter components. Global VLBI observations
at 18 cm were also performed by Nan et al. (1991a). These observations,
combined with MERLIN data taken at the same time, confirmed the
existence of the four components found by Fanti et al. (1986). These were
labelled A, B, C, and D, by Nan et al. (1991a) and we adopt the
same nomenclature here. An additional three, extended components of low
surface brightness, E, F and G, were also found by Nan et al. (1991a).
Together, these components account for 90% of the total flux density
of the source.
VLBI polarimetry of 3C 119 was first performed by Nan et al. (1999) using the VLBA at three widely-separated frequencies in the 8.4 GHz band. The brightest jet component they found, component C, has a smooth rotation measure gradient of 2300 rad m-2 mas-1, which is indicative of a collision between the VLBI jet and a dense interstellar cloud.
3C 119 is included in the MOJAVE (Lister & Homan 2009, Monitoring Of Jets in Active galactic nuclei with VLBA Experiments) monitoring project at 15.4 GHz. Four images from 2002, 2006, 2008, and 2009 are available in their data archive. At this frequency, components A, B, and C are detected, while the low brightness emission detected by Nan et al. (1991a), is completely resolved out.
Our total intensity image of 3C 119 at 4.8 GHz, compiled using all four C-band IFs, and the image at 8.4 GHz, are presented in Fig. 1. The source exhibits a core-jet structure with four of the seven components, (A-D), being detected. The three brightest components are not aligned, but lie along a jet contain ``wiggles''. Components B and C are surrounded by a ``halo'' of spots, reminiscent of the low brightness emission in which the jet itself is embedded.
Component A is almost point-like in the available VLBI images. Using
its flux density estimates for almost the same epoch at
frequencies from 1.6 to 15.4 GHz, we find a spectrum (see
Fig. 2) typical of a giga-peaked spectrum (GPS)
source with a peak flux density around 5 GHz. In
Fig. 2, the flux density measurements at frequencies
>4.5 GHz were taken over a narrow range of dates. The measurement
at 1.6 GHz (Nan et al. 1991a) was adopted assuming negligible temporal
variability at that frequency. Component A is not detected at 50 cm
(Nan et al. 1991b) with an upper limit of 40 mJy, which is consistent with
its inverted spectrum at low frequencies. We note that the flux
density at 8.4 GHz for this component declined from 117 to 70 mJy
between December 1994 (Nan et al. 1999)
and December 2001 (present work).
The observations performed by MOJAVE at 15.4 GHz also indicate
that the
flux densities rose from 45 mJy in October 2002 to
116 mJy in March 2006, 149 mJy in May 2008, and
173 mJy in July 2009. This component clearly
appears to be a variable GPS source. Variability in a small
fraction of GPS sources was found by Jauncey et al. (2003).
Therefore, component A is almost certainly the core of 3C 119.
![]() |
Figure 1:
(Left) The total intensity
image of 3C 119 at 4.8 GHz made by combining all four
C-band IFs, and (right) the total intensity 8.4 GHz image of
3C 119. The restoring beams are
|
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![]() |
Figure 2: Spectral index plot for component A made using flux density measurements taken almost at the same epoch for frequencies >4.5 GHz. The measurement at 1.6 GHz (Nan et al. 1991a) was adopted assuming negligible flux density variability at that frequency. |
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Mantovani et al. (2009) found total flux densities for 3C 119 of 4722 and 2677 mJy at 4.8 and 8.4 GHz, respectively, from their Effelsberg 100-m observations. The total flux density in our 4.8 GHz combined-IF image is 2838 mJy. At 8.4 GHz, we obtain 1531 mJy. The peak flux density is located in component C, being 987 and 660 mJy at 4.8 and 8.4 GHz, respectively.
![]() |
Figure 3:
The total intensity contours for 3C 119 A-C
for the four C-band IFs with the polarisation |
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3.1.1 Polarised emission from the inner jet of 3C 119
To compare the 5 and 8.4 GHz results, the images of 3C 119 were convolved to a resolution of

Figure 3 shows the total intensity and polarisation
structure of the jet at C-band for the four individual IFs, while
Fig. 4 shows the jet structure at X-band. The
parameters derived from these images are listed in
Table 2. Flux densities were determined using the AIPS
task IMEAN on the same region of the P and I images. In
Table 2, the total and peak flux densities, S, the
rms noises, the polarised integrated flux densities,
and its
rms noise, the percentage polarisation, m, and the electric vector
position angle (EVPA),
,
are listed for the four C-band IFs and
X-band. For the core component A, which appears unresolved, we
listed the values at the pixel of maximum total intensity.
Plots of
against wavelength squared for components B and C are shown in Fig. 5. These were derived as
follows. The median values and associated errors were computed for a
box of five-by-five pixels around the peaks of polarised emission.
At 15.4 GHz, the EVPA for both components was derived from the image
made available by the MOJAVE archive from observations taken in 2002.
These values have an accuracy of better than 5
(Lister & Homan 2005).
Both components show high values for the rotation measure. We derive RM = 884 rad m-2 (3618 rad m-2 in the source rest frame) for component B, whereas component C yields RM = 1373 rad m-2(5620 rad m-2 in the source rest frame). We note that the EVPAs reported by Nan et al. (1999) for component C in the three sub-bands of their VLBA X-band observations are in close agreement with the linear fit in Fig. 5. They did not detect polarised emission in the region close to the peak of emission for component B, in contrast to our more sensitive observations. Polarised emission was detected by both sets of observations for the region immediately to the south west of compact component B, where almost the same values were found for the EVPAs.
![]() |
Figure 4:
The total intensity contours for 3C 119 A-C
at X-band with the polarisation |
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Table 2: Polarimetric parameters for the inner jet of 3C 119.
![]() |
Figure 5:
Plots of the observed |
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![]() |
Figure 6:
The derived distribution of RM for 3C 119 C
as a grey scale plot
(left) and as a contour plot (right).
The range of RM in the left panel is from 500 to 3000 rad m-2,
and the distribution is overlaid on the continuum image at 4619.2 MHz.
The continuum contour levels
are -2, 2, 8, 32, 128, and 512 mJy beam-1. In the right panel,
the RM contour levels are
|
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We have also plotted the distribution of RM around the emission peak in component C (Fig. 6). These plots were produced using the AIPS task RM, which requires EVPAs for up to four frequencies to compute the RM values. In this case, we selected frequencies of 4619, 4854, 5094, and 8421 MHz for which we have images available. Figure 6 shows that in a small area close to the peak of polarised emission, there are values of about 1400 rad m-2 (see Fig. 5). This area is surrounded by a region with much higher RMs lying in the range 2300 to 2500 rad m-2 (9400-10 200 rad m-2 in the source rest frame). This region coincides with a change in the direction of the inner jet of 3C 119. The value of RM reported for the integrated emission of 3C 119 by Mantovani et al. (2009) is 1928 rad m-2. Clearly, C is the dominant component, strongly influencing the polarimetric parameters of the source.
Figure 6 (left) shows in grey scale the RM
distribution for 3C 119 derived from the four frequencies (4619,
4854, 5094, and 8421 MHz) overlaid on the total-intensity contour
image, while the panel on the right shows the RM contours. No
redshift corrections were applied, so the RMs in the
rest frame of the source will be higher by a factor of
.
3.2 3C 318
3C 318 is a radio galaxy at a redshift of 1.574 (1 mas = 8.554 pc).
Single-dish observations of the object were recently made by
Mantovani et al. (2009) who measured flux densities of 764 mJy at
4.8 GHz and 417 mJy at 8.4 GHz. The source is 3.4% and 6.6%
polarised at 4.8 and 8.4 GHz, respectively. At lower frequencies,
the polarisation drops below the detection limit of these Effelsberg
observations. The RM derived by Mantovani et al. is 498 rad m-2. Using the measurements of Tabara & Inoue (1980), we derive an
RM of 342 rad m-2. A similar value for the brightest
component (420 rad m-2) is reported by Taylor et al. (1992) from VLA
observations with angular resolution of 0.4
.
Taylor et al. found a
polarisation percentage of
10% at 8.4 GHz.
A higher resolution L-band image of 3C 318 was obtained by Spencer et al. (1991)
using combined MERLIN and EVN observations at a resolution of
mas2. The component B detected by Akujor et al. (1991) with
MERLIN at 5 GHz was resolved out, while the two northern components were
found to show considerable structure and bright peaks. The total flux density
detected by Akujor et al. (1991) was 543 mJy. Akujor & Garrington (1995) performed
polarimetric observations of 3C 318 at 8.4 GHz with the VLA, and
detected polarised emission (
10%) mainly from the two
northern components. VLA observations were also made by
van Breugel et al. (1992) at 15 and 22 GHz. They found the northern
region, in which the two components merge, to be 17%
polarised. Additional polarimetric observations were performed by
Lüdke et al. (1998) with MERLIN who found the brightest component to be
3.6% polarised at 5 GHz. In this image, 3C 318 shows a core-jet
structure on one side and a lobe on the other. It is suggested that
component K2 (Spencer et al. 1991) might be the core, although it
appears resolved and does not have a flat spectrum.
In our 4.8 GHz VLBA observations, 3C 318 appears to be clearly resolved.
Fringes were not detected at 8.4 GHz. Our 5 GHz image
was made using the full bandwidth and, to be able to compare with
previous VLBI observations, with a convolution beam of
mas2 in PA 46
(Spencer et al. 1991). 3C 318 appears
elongated in roughly the north south direction, the southern side
contain a ``wiggling'' structure (Fig. 7). We follow
the nomenclature of Spencer et al. (1991), who found four components
named K1, K2, K3, and A. About 61% of the flux density found by
Lüdke et al. (1998) is recovered here. The source parameters derived from
our image are summarised in Table 3, the flux density
values having been obtained using the AIPS task TVSTAT.
![]() |
Figure 7:
The VLBA image of 3C 318 at 4.8 GHz. Contour levels are -0.35,
0.35, 0.7, 1, 2, 4, 8, 16, 32, 64, and 128 mJy/beam.
A vector of 1 mas corresponds to 0.1 mJy/beam of polarised emission.
The convolution beam is
|
Open with DEXTER |
In our image, we find two other extended components, which we designate K4 and K5. These were not detected by the less sensitive observations of Spencer et al. (1991).
The brightest component, K2, is responsible for almost all of the
polarised emission from 3C 318, and the magnetic field orientation appears
to be almost constant over the region. A similar behaviour, but with
different position angles, is presented by all available
polarimetric images. Thus, we can derive the values of the rotation
measure from these interferometric observations made at different
frequencies. Values of the EVPA are taken from Lüdke et al. (1998) at
4996 MHz, Akujor & Garrington (1995) at 8414 MHz, Taylor et al. (1992) at
8515 MHz, and van Breugel et al. (1992) at 15 GHz, as well as from the
present work, and are plotted in Fig. 8.
The EVPA accuracies of these observations were not given, and values of
have been assumed for both MERLIN and VLA EVPA determinations.
The RM computed is
457 rad m-2, not far from
the values of 420 rad m-2 derived by Taylor et al. (1992), and
498 rad m-2 derived by Mantovani et al. (2009). We are again
dealing with a CSS showing a very high RM of
3030 rad m-2 in the source rest frame at sub-arcsecond resolution.
3.3 3C 343
3C 343 is associated with a quasar at z=0.988 (1 mas = 8.017 pc). From their single dish observations, Mantovani et al. (2009) reported the detection of polarised flux density for this source only at 10.45 GHz at a level of 1.4%. A low level of polarised emission (0.8%) was also reported by Lüdke et al. (1998) from their MERLIN observations at 5 GHz in which the source appears barely resolved with a total flux density of 1434 mJy. Polarised emission is detected only in its eastern extension. Previous VLBI observations were performed by Fanti et al. (1985) and Nan et al. (1991b) at 1.6 GHz and 608 MHz, respectively. The mas structure of the source is quite peculiar, resembling a ``fried egg''.
Our total-intensity VLBA images of 3C 343 for the different C-band
IFs are shown in Fig. 9, while the VLBA image at
8.4 GHz is shown in Fig. 10. The wide-band 5 GHz
VLBA system allowed us to use four 8 MHz IF channels separated well in
frequency. Only C-band IFs 1 and 3 contain data from the VLA antenna
which was included in the observing array. Two bright, compact
components, A and B, are surrounded by weak, diffuse emission. The two
images made from data including the VLA antenna detected only diffuse
emission, while the two images lacking baselines to the VLA antenna
show the two prominent components, A and B, and the ridge of emission
that resembles a curved radio jet. Both A and B have steep spectral
indices between 4.8 and 8.4 GHz. The flux densities of these
components were obtained with the AIPS task JMFIT, and component A
(the eastern one) has
(1.3 using the peak flux
densities), while component B has
(0.8 using the
peak flux densities). Polarised emission is detected for both of
these components and along the emission region between them. This
all implies that either A or B is unlikely to be the core of
3C 343.
Table 3:
Parameters for 3C 318 at 4.8 GHz with a
resolution of
mas2 at 46
.
From the 8.4 GHz image, we note that a new compact component is
clearly visible directly to the east of component A. This feature,
which we label C in Fig. 10, is well separated from the brighter
component A. Using the AIPS task JMFIT, we obtain total and peak flux
densities of 7.7 and 3.5 mJy, respectively, for component C. It is not
detected in any of the C-band images of the same resolution, including that
made by combining all four IFs to produce a 3
upper limit peak flux
density of 1 mJy. This corresponds to an inverted spectrum
for C between 4.8 and 8.4 GHz, making it a candidate for being the core
of 3C 343. Moreover, component C is situated nicely on the curved
track of the jet as seen in Figs. 9b and d.
![]() |
Figure 8:
A plot of the observed |
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The parameters for components A and B are summarised in Table 4. The component peak and total flux densities, along with their deconvolved angular dimensions, were obtained using the AIPS task JMFIT. The degree of polarisation was estimated close to the peaks of emission in A and B. However, there appears to be large changes in the EVPAs close to the peaks of emission. Therefore, we have not quoted a single value in Table 4 but refer the reader to the distributions of EVPAs in Fig. 9.
Table 4: Polarimetric parameters for the components A and B of 3C 343.
The total flux density detected in a combined C-band image is 1274 mJy, about 89% of the flux density detected by MERLIN (Lüdke et al. 1998) and 85% of the flux density detected with the Effelsberg 100-m telescope by Mantovani et al. (2009). The polarisation percentage is estimated to be 0.96%, close to the value of 0.8% measured with MERLIN (Lüdke et al. 1998).
![]() |
Figure 9:
The total intensity contours for 3C 343 A-C
for the four C-band IFs with the |
Open with DEXTER |
The total flux density detected in the VLBA image at 8.4 GHz (Fig. 10) is 553 mJy, 69% of the flux density detected by Mantovani et al. (2009). The polarised emission detected is 7.2 mJy, corresponding to 1.3%. The percentage polarisation drops by a factor of 0.73 between 8.4 and 4.8 GHz.
We detect polarised emission at all five observing frequencies.
However, because of both the low level of polarisation and the lower
sensitivity of the observations without the VLA antenna, mapping the
RM distribution of 3C 343 is more difficult. It is clear
from Fig. 9 that there may be changes of up
to 90
in the orientation of the EVPAs close to the peaks
of emission in components A and B. Significant polarisation is also not always
detected from the same physical region of a component, possibly due
to a combination of both varying sensitivity in the different IFs and
varying RM across the source. These aspects have made it difficult
to construct a reliable RM map. However, changes in the EVPAs between
two neighbouring IFs, say IF2 and IF3, by of more than
30
in some regions are indicative of RM values higher than
1500 rad m-2 in the observer's frame.
While more sensitive observations are required to produce a reliable RM
map, a preliminary one using the present data seems to indicate similarly
high values of RM.
4 Discussion
4.1 Comments on the three sources
The three CSSs we present here have mutually very different structures when imaged with mas resolution. The source 3C 119, which is associated with a possible quasar, has a complex shape when observed at low resolution, but has strong core-jet structure on resolutions of a few mas. We suggest that component A, which exhibits a convex spectrum, flux density variability, and either no, or at best marginal, polarisation above the detection limits, is the core. The jet contains ``wiggles''. From published images at sub-mas resolution, 3C 119 appears to maintain its collimation while presenting an overall spiral-like shape. Two bright, polarised blobs are seen along the jet. The brighter of these has a high rotation measure and strong depolarisation between 8.4 and 5 GHz, which we interpret as an indication of a strong interaction between the jet and a cloud in the ISM, possibly a dense narrow-line region (NLR) cloud. Although this interaction does not disrupt the jet, the jet does seem to change direction. The jet may also be bent close to our line of sight and move at apparent superluminal speed. We do not detect a counter-jet. The apparent speed of the two bright blobs (components B and C) along the approaching jet is most likely to be measured by the MOJAVE monitoring project, and this could possibly place constraints on the orientation of the ejection axis.
The source 3C 318 has an elongated jet with ``wiggles'' along its
southern part.
It is associated with a galaxy. Although the cores in
quasars are often at the end of the jet, this need not be the case for
a galaxy. In the present observations, we are unable to
identify the exact core. Component K2, suggested by Spencer et al. (1991)
to be the core, has a steep spectrum (
)
and
has a percentage polarisation of
3.4% at 4.8 GHz.
It also has a high rotation measure, often visible in term of jets in CSS
sources.
This component is unlikely to be the radio core.
Among the three sources observed, 3C 343, which is associated with a quasar, presents the most unusual structure. The two brightest polarised components are embedded in a diffuse region of weak emission. It is unlikely that either is the core of the source. We propose that the component clearly visible to the east of component A in the X-band image, instead, is the possible core candidate. The C-band images without the VLA antenna do not detect the extended diffuse emission but show the two prominent components, A and B, and a ridge of emission that resembles a strongly curved jet.
The structures of all three CSS sources discussed in this paper exhibit
large deviations from a collinear structure that are indicative of interactions
of the jets with clouds in the interstellar medium of the host galaxy.
Although two of the sources, 3C 119 and 3C 343, are associated with quasars,
their cores are either weak or undetected, suggesting that projection
effects caused by a small angle of inclination may not be important. However,
jets may be bent towards the line of sight after collisions with clouds.
Systematic monitoring of the knots or peaks of emission may help us to clarify
whether this is indeed the case. The detection of high RMs towards
the components in the radio jet/structure in both 3C 119 and 3C 343, as well
as in 3C 318, supports the possibility of interaction of the jets with
dense clouds. For an electron density of 103 cm-3, which
is a reasonable estimate for the NLR clouds (e.g., Osterbrock 1989;
Peterson 1997),
and cloud sizes of
20 to 100 pc, the highest value of RM for
3C 119 yields magnetic field strengths in the range
of
0.1 to 0.6
G. The lower value of the cloud size was assumed to
roughly correspond to the size of the radio components. The corresponding
values of field strength for 3C 318 and 3C 343 are in the range of
0.04-0.2 and 0.07-0.4
G, respectively. These values are similar
to those of, for example, Zavala & Taylor (2002). For a less dense medium
with a thermal electron
density of
1 cm-3 and a screen thickness of
1 kpc, as adopted
by Mantovani et al. (2002), the magnetic field strenghts are in the range from
3.7 to 12.6
G. These are similar to those estimated by Mantovani et al. (2002) for the CSS quasars B0548+165 and B1524-136, which also
have high values of RM and bends in their radio structures.
4.2 A discussion of CSS quasars
To date, few CSSs have been imaged with polarimetric VLBI observations.
Most of those that have are quasars. At present, 12 out of 24 quasars
in the list of CSSs from the 3C and PW catalogues (Fanti et al. 1990) have
published polarimetric VLBI data. Almost all of these show core-jet
structures. Polarised emission is detected along the jets. Cores are
usually weak and polarisation is not detected, in contrast to flat
spectrum quasars. CSSs for which mas-scale values of RM have
been derived are even rarer. Table 5 summarises
parameters derived from existing observations. Except for
3C 287, whose low RM has been estimated from only two nearby
frequencies, and 3C 286, which possibly has a low RM given its
low integrated value but whose RM has not been determined with
mas resolution, the remaining 12 sources have absolute rest-frame
values of RM ranging from 1600 to
rad m-2. In the case of OQ172, which also has the highest
RM, the region of high RM is close to the core with the
highest values occurring within
20 pc of the peak of emission
in the core. This is also the case for the quasar 3C 309.1, which
has a prominent radio core, the region of highest RM
being situated in the vicinity of the radio core. For the remaining
sources, the component of highest RM is distinct from the core,
wherever a radio core could be identified. The distance from the core
to the component with the highest RM varies from
37 to 1600 pc, the median separation being
400 pc. The regions of high RM are clearly within the NLR of the host galaxy.
The fractional polarisation usually tends to decrease with decreasing
frequency. For the sources listed in Table 5, the
components with the highest RM in 3C 119 and 3C 309.1 are
strongly depolarised with DP values of 0.1 or less (beetween 5.0 and 8.4 GHz and 8.4 and 15 GHz respectively), while those
in 3C 216 and OR-140 (B1524-136) exhibit hardly any
depolarisation. While a high RM without depolarisation may be
due to an external screen, a high RM along with depolarisation
may be caused by unresolved structures in the screen and/or
thermal plasma mixed with the radio-emitting material. Several examples
of high RM with little or no significant depolarisation imply
that the RM is due to a foreground Faraday screen, the NLR
contributing to the observed RM. In all cases examined, a
law is closely followed over the observed frequency range.
The jets are often distorted and this is interpreted in terms of
jet-cloud interactions, although projection effects can also affect the
observed structure if the jet is bent close to the line of sight. In
many core-jet CSS quasars, high integrated Faraday rotation occurs
where bends in the jet are found, suggesting that jet-cloud
interactions play a significant role in the observed high RMs of
these components. For example, amongst the 10 sources in Table 5
where a core or possible core has been identified, the highest values
of RM occur at distances from the core ranging from
20 pc
for OQ 172 to
1600 pc for 3C 43, excluding 3C 309.1 where
the highest value is for the core. The median separation in
the region of highest RM from the core is
300 pc. The axes
of radio emission in these sources bend significantly after the region
of highest RM. The PA of the latter differs from the axis defined
by the core and the region of highest RM by
20 to 90
,
the more extreme cases being 3C 43, 3C 119, 4C 16.14, and 3C 216. In
the case of OQ 172, the region of highest RM is within
20
pc of the nucleus, and the jet shows a large deviation very close to
the nucleus.
![]() |
Figure 10:
The VLBA image of 3C 343 at 8.4 GHz using data from the
full bandwidth. Contour levels increase by a factor of two from
0.75 mJy/beam. A vector of 1 mas corresponds to 0.1 mJy/beam of polarised
emission. The convolution beam is |
Open with DEXTER |
Table 5: Polarisation parameters of CSSs from mas-resolution observations.
4.3 Comparison with pc-scale RMs in other AGNs
Apart from a few radio galaxies with either strong cores
or jets, such as 3C 111, 3C 120, and M 87, most of the pc-scale
RM estimates for other AGNs have been made for either
core-dominated quasars or BL Lac objects. Early measurements with
subarcsec resolution using the VLA inferred low core RMs at long
wavelengths, the RMs increasing at shorter wavelengths as
one probed deeper into the radio core (e.g., Saikia et al. 1998, and
references therein). Subsequent mas-resolution observations with the
VLBA have revealed a wealth of information on core RMs (e.g.,
Zavala & Taylor 2003,2004,2002, and references therein; O'Sullivan & Gabuzda 2009, and references therein). A systematic study of the
mas-scale RM properties of 40 quasars, radio galaxies, and BL Lac
objects by Zavala & Taylor (2003,2004) demostrated that the rest-frame
core RM for quasars ranges up to 104 rad m-2 with a
median value of
1860 rad m-2 within
10 pc of the core.
For BL Lac objects, their core RM values are usually within
1000 rad m-2 with a median value of
440 rad m-2. The RMs of pc-scale jets decreases rapidly, the
median values of the rest-frame RM for the jets being
460
and 260 rad m-2 for quasars and BL Lacs, respectively (Zavala & Taylor 2004). The few radio galaxies that have been studied exhibit
evidence of moderate to high values of RM. For example, the core
of 3C 111 is not significantly polarised, while the jet
exhibits an RM of -750 rad m-2 3 mas (2.8 pc) east of the
core, decreasing further to -200 rad m-2 5 mas (4.7 pc) east
of the core. For 3C 120, while Zavala & Taylor (2002, 2003)
estimate a core RM of 2080 rad m-2, decreasing to
100 rad m-2 about 1 pc from the core, Gomez et al. (2008)
find a localised region of high RM
3 to 4 mas (2-2.6 pc) from the core with a peak RM of
6000 rad m-2.
The RM values for M 87 could be determined from 18 to 27 mas
(
1.5 to 2 pc) west of the core, and the values varied from
-5000 to 104 rad m-2 (Zavala & Taylor 2003,2002).
We noted that M 87 is in a cooling core cluster and that RM
values as high as
8000 rad m-2 have been seen towards its
2-kpc radio lobes (Owen et al. 1990).
In comparison, the median value of RM for the CSS sources listed
in Table 5 is 5000 rad m-2, and values higher than
10 000 rad m-2 are seen to occur at distances from the core
ranging from
300 to 1600 pc. This is quite unlike the
regions of RM discussed earlier, almost all of which are very
close to the radio core. For CSS objects, this implies
the jets are often interacting with dense clouds of gas in the
circumnuclear region of the host galaxy.
4.4 Environmental versus orientation effects
For quite some time, it has been apparent that the degree of core polarisation correlates with AGN classification. From subarcsec scale measurements with the VLA, it was pointed out quite early on that quasar cores tend to be more polarised than galaxy cores (Saikia et al. 1985,1987). Milliarcsec-scale polarisation measurements also showed a similar trend, with the cores in BL Lac objects being slightly more polarised than the quasar cores (Cawthorne et al. 1993). Gabuzda et al. (1992) also demonstrated that the cores of BL Lacs are more polarised than quasars, a result also obtained for a larger sample of AGNs by Pollack et al. (2003). From arcsec-scale polarisation data, Saikia (1999) showed that BL Lac objects and core-dominated quasars had higher levels of core polarisation than lobe-dominated quasars and radio galaxies, and suggested that this might related to an orientation effect. Here, the low polarisation of the cores of radio galaxies, and perhaps the lobe-dominated quasars as well, were attributed by the authors to depolarisation by the obscuring torus. However, the observed degree of polarisation may also reflect the contribution of a small-scale jet, which may be more strongly polarised and contribute more significantly at smaller angles to the line of sight.
Taylor (2000) suggested that the RM values for BL Lac objects
may be smaller than those of quasars, because their jets are believed
to be inclined at smaller angles to the line of sight. This could arise
if the relativistic jets cleared out the magneto-ionic material
responsible for the Faraday rotation. Similar ideas were suggested by
Saikia et al. (1998) to explain the low RM values for quasar
cores determined from long-wavelength polarimetric observations with
arcsec resolution. Although individual RM values in BL Lac
objects are known to exceed thousands of rad m-2, the median
value of rest-frame RM for quasars is larger than that for the BL
Lac objects by a factor of 4, consistent with the expectation of
Taylor (2000). It appears that for quasars the long-wavelength
measurements probe the outer regions of the nuclear jets on scales of
tens of pc yielding low RM values as these are seen through
regions that have been at least partially cleared of the
magneto-ionic medium by the relativistic jets. Shorter wavelength
observations with mas resolution probe deeper into the base of the
jet, and yield high RMs indicating denser gas and/or higher
magnetic fields than on the larger scales. It is relevant to note
that O'Sullivan & Gabuzda (2009) find the core RM to
systematically increase with frequency, this being well described by
a power law, providing information about the power law fall off of
electron density and/or magnetic field with distance from the nucleus.
In the scheme where
orientation effects play a role, the cores of radio galaxies and any
emission in their immediate vicinity would be expected to have high
values of RM because of the effects of the obscuring torus.
An interesting characteristic of extragalactic radio sources is that there appear to be significant differences between the host galaxy and emission-line properties of Fanaroff-Riley class I and II sources (Fanaroff & Riley 1974), which may be related to the fuelling mechanism. While a significant fraction of high-luminosity radio sources have peculiar optical morphologies and high-excitation emission lines, reminiscent of gas-rich galaxy mergers, the low-luminosity radio sources do not share the same optical properties and have weak, low-excitation emission lines (Baum et al. 1995,1992; Heckman et al. 1986). Hubble Space Telescope observations show that the low-power radio sources lack evidence of an obscuring torus and significant emission from a classical accretion disc (Chiaberge et al. 1999), and may be fuelled by quasi-spherical Bondi accretion of circum-galactic gas rather than gas-rich galaxy mergers (Hardcastle et al. 2007). The finding by Baldi & Capetti (2008) that high-excitation radio galaxies almost always show evidence of star formation, unlike their low-luminosity counterparts, is consistent with this trend. In our case, BL Lac objects are usually hosted by galaxies with low-excitation emission lines, while quasars are hosted in galaxies with high-excitation emission lines. This difference is also likely to affect the observed RMs of BL Lac objects and quasars, with the former expected to have smaller values.
For CSS sources, although orientation is also expected to play a
role (e.g. Saikia et al. 1995), the cores are either weak or not clearly
identified making it impossible to either determine their RMs or place
robust limits on their degrees of polarisation. Amongst the sources listed
in Table 5, the cores are strong enough for their RMs to be
estimated in 3C 309.1 and OQ172, the values being -1600
and 40 000 rad m-2, respectively. While 3C 309.1 exhibits a large
misalignment between the mas-scale and arcsec-scale structures, the jet
in OQ 172 bends sharply west of the nucleus and the RM of the jet
falls to less than 100 rad m-2 only 10 mas (
74 pc) from the
nucleus (Udomprasert et al. 1997). Although the high values of RM may be partly due to these observations probing close to the nuclear
region, the large
bends in these sources imply that collisions with dense
clouds of gas are also a significant factor. For the remaining CSS
objects, where the regions of large RM occur at large distances
from the nucleus, these large values are most likely to be caused by
interactions of the jets with dense clouds of gas, some of which may
also be fuelling the AGN activity.
5 Summary and conclusions
We have presented multi-frequency VLBA polarisation observations of
three CSS sources, namely 3C 119, 3C 318, and 3C 343 to estimate
their RM values. The radio source 3C 119 is associated with a
possible quasar, and its RM in the source rest-frame has been found
to be as high as 10 200 rad m-2 in a region that coincides
with a change in direction of the inner jet. This component is located
at a projected distance of
325 pc from the core, which is
almost point-like, variable, has a peaked radio spectrum and is at best
marginally polarised. The source 3C 318 is associated with a radio galaxy
and its
rest-frame RM has been found to reach a maximum of
3030 rad m-2 for the brightest component, which contributes almost all
of the polarised emission. These observations are more sensitive than
those of Spencer et al. (1991) and have detected two more extended
components, which trace ``wiggles'' in the jet towards the
southern side of the source. Of the three, the CSS source 3C 343
has perhaps the most complex structure. It contains two peaks of
emission and a curved jet embedded in more diffuse emission. It
exhibits complex field directions near the peaks of emission, which
indicate rest-frame RM values in excess of
4000 rad m-2. The varying sensitivity of the different frequencies and
the complex field patterns near the peaks of emission make it
difficult to construct a reliable RM image for this source.
We have compiled the available data on mas-scale RM estimates for
CSS sources. They exhibit a wide range of values with indications of a
low RM for 3C 287 that needs to be confirmed from observations
with a larger number of frequencies, to values as high as
40 000 rad m-2 in the central region of OQ172
(Udomprasert et al. 1997). The components with high RM may also
occur at considerable distances from the core, e.g., in 3C 43 where
the component with an RM of
14 000 rad m-2 is located
at a projected distance of
1600 pc (Cotton et al. 2003a). The RM estimates for flat-spectrum cores in largely core-dominated radio
sources appear to increase with frequency (see O'Sullivan & Gabuzda 2009), suggesting that as one probes deeper into the core or unresolved
base of the jet, one samples regions of higher density and/or magnetic
field in the magneto-ionic medium. On larger scales, the jet RMs
tend to be low because these objects are observed along a line of sight
where the magneto-ionic medium may have been swept out by the
relativistic jets (e.g., Taylor 2000; Zavala & Taylor 2004; Saikia et al. 1998). The CSS objects for which RM values have been
estimated are almost entirely quasars. While the effects of an overall
density gradient in the magneto-ionic medium, along with effects of
geometry, orientation, and modes of fuelling of the AGN, are likely
to play a significant role, the
high RM values in many of these CSS sources appear to be caused by dense
clouds of gas interacting with the radio jets. They usually also
exhibit large structural bends and distortions, consistent with the
possibility of jet-cloud interactions in the interstellar medium of the
host galaxy. Some of these gas clouds may also be responsible for
fuelling the AGN activity.
We thank an anonymous referee for his/her very helpful comments and suggestions, and for a careful reading of the manuscript of this paper. The VLBA is operated by the U.S. National Radio Astronomy Observatory which is a facility of the National Science Foundation operated under a cooperative agreement by Associated Universities, Inc. This research has made use of data from the MOJAVE database that is maintained by the MOJAVE team (Lister et al. 2009, AJ, 137, 3718). This research has made use of the NASA/IPAC Extragalactic Database (NED) which is operated by the Jet Propulsion Laboratory, California Institute of Technology, under contract with the National Aeronautics and Space Administration. F.M. likes to thank Prof. Anton Zensus, Director, for the kind hospitality at the Max-Planck-Institut für Radioastronomie, Bonn, for a period during which part of this work has been done.
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Footnotes
All Tables
Table 1: VLBA+VLA1 observing parameters.
Table 2: Polarimetric parameters for the inner jet of 3C 119.
Table 3:
Parameters for 3C 318 at 4.8 GHz with a
resolution of
mas2 at 46
.
Table 4: Polarimetric parameters for the components A and B of 3C 343.
Table 5: Polarisation parameters of CSSs from mas-resolution observations.
All Figures
![]() |
Figure 1:
(Left) The total intensity
image of 3C 119 at 4.8 GHz made by combining all four
C-band IFs, and (right) the total intensity 8.4 GHz image of
3C 119. The restoring beams are
|
Open with DEXTER | |
In the text |
![]() |
Figure 2: Spectral index plot for component A made using flux density measurements taken almost at the same epoch for frequencies >4.5 GHz. The measurement at 1.6 GHz (Nan et al. 1991a) was adopted assuming negligible flux density variability at that frequency. |
Open with DEXTER | |
In the text |
![]() |
Figure 3:
The total intensity contours for 3C 119 A-C
for the four C-band IFs with the polarisation |
Open with DEXTER | |
In the text |
![]() |
Figure 4:
The total intensity contours for 3C 119 A-C
at X-band with the polarisation |
Open with DEXTER | |
In the text |
![]() |
Figure 5:
Plots of the observed |
Open with DEXTER | |
In the text |
![]() |
Figure 6:
The derived distribution of RM for 3C 119 C
as a grey scale plot
(left) and as a contour plot (right).
The range of RM in the left panel is from 500 to 3000 rad m-2,
and the distribution is overlaid on the continuum image at 4619.2 MHz.
The continuum contour levels
are -2, 2, 8, 32, 128, and 512 mJy beam-1. In the right panel,
the RM contour levels are
|
Open with DEXTER | |
In the text |
![]() |
Figure 7:
The VLBA image of 3C 318 at 4.8 GHz. Contour levels are -0.35,
0.35, 0.7, 1, 2, 4, 8, 16, 32, 64, and 128 mJy/beam.
A vector of 1 mas corresponds to 0.1 mJy/beam of polarised emission.
The convolution beam is
|
Open with DEXTER | |
In the text |
![]() |
Figure 8:
A plot of the observed |
Open with DEXTER | |
In the text |
![]() |
Figure 9:
The total intensity contours for 3C 343 A-C
for the four C-band IFs with the |
Open with DEXTER | |
In the text |
![]() |
Figure 10:
The VLBA image of 3C 343 at 8.4 GHz using data from the
full bandwidth. Contour levels increase by a factor of two from
0.75 mJy/beam. A vector of 1 mas corresponds to 0.1 mJy/beam of polarised
emission. The convolution beam is |
Open with DEXTER | |
In the text |
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