Issue |
A&A
Volume 508, Number 3, December IV 2009
|
|
---|---|---|
Page(s) | 1253 - 1258 | |
Section | Extragalactic astronomy | |
DOI | https://doi.org/10.1051/0004-6361/200913055 | |
Published online | 04 November 2009 |
A&A 508, 1253-1258 (2009)
The core fundamental plane of B2 radio galaxies
D. Bettoni1 - R. Falomo1 - P. Parma2 - H. de Ruiter3,2 - R. Fanti2
1 - INAF - Osservatorio Astronomico di Padova,
Vicolo dell'Osservatorio, 5, 35122 Padova, Italy
2 - INAF - IRA Bologna, Italy
3 -
INAF - Osservatorio Astronomico di Bologna,
via Ranzani, 1, 40127 Bologna, Italy
Received 3 August 2009 / Accepted 3 October 2009
Abstract
Context. The photometric, structural and kinematical
properties of the centers of elliptical galaxies harbour important
information on the formation history of galaxies. In the case of
non-active elliptical galaxies, these properties are linked in a way
that surface brightness, break radius and velocity dispersion of the
core lie on a fundamental plane similar to that found for their global
properties.
Aims. We construct the core fundamental plane (CFP) for a
sizeable sample of low redshift radio galaxies and compare it with that
of non-radio ellipticals.
Methods. We combine data obtained from high resolution HST
images with medium resolution optical spectroscopy to derive the
photometric and kinematic properties of 40 low redshift radio galaxies.
Results. We found that the CFP of radio galaxies is
indistinguishable from that defined by non-radio elliptical galaxies of
similar luminosity. The characteristics of the CFP of radio galaxies
are also consistent (same slope) with those of the fundamental plane
(FP) derived from the global properties of radio (and non-radio)
elliptical galaxies. The similarity of CFP and FP for radio and
non-radio ellipticals suggests that the active phase of these galaxies
has minimal effects on the structure of the galaxies.
Key words: galaxies: active - galaxies: kinematics and dynamics
1 Introduction
The properties of the centers of massive elliptical galaxies are of strategic importance for the understanding of the complex processes of galaxy formation. The centers represent the bottom of the potential well of the galaxy, host massive black holes, and provide a record of the past history of the galaxies. Until a decade ago, the properties of the center of galaxies were very little studied because of the insufficient spatial resolution of the available instrumentation. Only with the use of the Hubble Space Telescope, and using future large ground based telescope, can such a study become feasible.
In the pioneering study on the nuclear properties of nearby early type galaxies (carried out with
HST images), Faber et al. (1997) were able to probe the inner regions of a number of nearby ellipticals. They point out
that the inner luminosity profiles can be parameterized by a core (or break) radius
and a
characteristic surface brightness within the break radius
.
They also showed that these parameters (
,
)
can be combined to form
a core fundamental plane (CFP) which is
analogous to the one found for the global properties of early type
galaxies (Faber et al. 1997). Assuming that the cores are in dynamical equilibrium and supported by random motion, and
that the velocity anisotropy does not vary too much from galaxy to galaxy, and if the core M/L is
a well-behaved function of any two variables
,
,
or
,
then one expects that the
cores of galaxies follow a law similar to that of the fundamental plane (FP).
The main reason to study global and core properties is that it allows one to probe the mechanism of galaxy formation. In the last decade a new tool has become available: the discovery of the presence of a massive black bole (BH) in the centers of virtually all galaxies (e.g. Ferrarese & Merritt 2000; Lauer et al. 2007). However, only a small fraction of these BHs exhibit associated nuclear activity (non-thermal nuclear emission, X-ray and radio emission). The BHs may play an important role in the formation and evolution of massive galaxies and are also a key component for the development of the nuclear activity. Therefore the comparison of the properties of active and inactive galaxies through the FP becomes a tool to investigate the interplay between galaxy formation and nuclear activity.
In a previous work, using photometrical and dynamical data for 73 low red-shift (z<0.2) radio galaxies (RG), we (Bettoni et al. 2001) were able to compare the FP of RG with the one defined by inactive ellipticals (Jørgensen et al. 1996, JFK96). We showed that the same FP holds for both radio and non-radio ellipticals with radio galaxies occupying the region of the most luminous and large galaxies.
Until very recently little data have been available on the optical nuclear properties
of radio galaxies. One of the best optical sets of data is the study of
the B2 sample of low luminosity radio galaxies (Fanti et al. 1987; Capetti et al. 2000). For 60 radio galaxies WFPC2 HST imaging is
available in the F555W (approximately V) and F814W (approximately I) filters. A similar set of data is also available for a sample of powerful 3C radio sources.
These studies revealed the presence of new and interesting features, some of them
almost exclusively associated with low luminosity FR I radio galaxies.
In particular, the HST observations have shown the presence of dust in a
large fraction of weak (FR I) radio galaxies which takes the form of
extended nuclear disks (Jaffe et al. 1993; De Koff et al. 1996; De Juan et al. 1996; Verdoes Kleijn et al. 1999; de Ruiter et al. 2002).
Such structures have been naturally identified with the reservoir of material which will ultimately
accrete into the central black hole. The symmetry axis of the nuclear
disk may be a useful indicator of the rotation axis of the central
black hole (see e.g. Capetti & Celotti 1999), although the precise relationship between these two axes remains uncertain.
In this paper we investigate the CFP for a sample of low redshift radio galaxies and to
compare it with that for radio quiet galaxies. The plan of the paper is as follows. In Sect. 2 we
discuss our observations and data reduction methods. In Sect. 3 we present the CFP for our sample
of RG. The implications of those observations are then discussed in Sect. 4. Throughout this paper
we use the Concordance Cosmological Model, with H0=70 km s-1 Mpc-1, and
.
Table 1: The sample of low redshift B2 radio galaxies with velocity dispersion measurements.
2 The sample of radio galaxies
One of the most complete and well studied samples of nearby radio galaxies in the northern
hemisphere is the B2 sample (Fanti et al. 1987). This sample consists of 100 early-type galaxies
and was extensively studied at radio wavelengths, especially since the 1980s (see Fanti et al. 1987;
Parma et al. 1987; de Ruiter et al. 1990; Morganti et al. 1997). The sample is complete down to 0.25 Jy at 408 MHz
and down to (roughly)
mv = 16.5 and should be essentially unbiased for orientation. The objects
span the radio power range between 1023 and
at 1.4 GHz with a pronounced peak around
.
Therefore they give an excellent representation of the radio source types encountered below and
around the break of the radio luminosity function.
We considered here the sub sample of the B2 sample (100 objects) of 57 low redshift (z<0.20) radio galaxies, for which photometric and structural data of the core are available from HST observations in the F814W band (de Ruiter et al. 2002; Capetti et al. 2000). As described in Capetti et al. 2000
there is no bias in the selection of the 57 objects observed with HST
(they were chosen randomly as far as their radio and optical properties
are concerned). In comparing various parameters of this observed
sub-sample with those of the sources that were not observed by HST they
found that no significant differences emerged. The HST observations are
complete at the level of
57% and therefore constitute an unbiased sub sample.
3 Summary of previous results on the core properties of radio galaxies
In de Ruiter et al. (2002) the dust properties of radio cores were analysed. About half of the sources have
significant amounts of dust in the nuclear region, mostly in the form of disks or lanes, and if
radio jets are present they tend to be perpendicular to the dusty disk or lane, at least in the low
power sources (
at 1.4 GHz). There is also a (broad) correlation between
total dust mass of the disks and the radio power.
Based on high resolution HST images it was found that elliptical galaxies come in two flavours, one with ``core'' radial brightness profiles and one with power law profiles (see e.g. Faber et al. 1997). This distinction is seen also for other properties: rotation, isophote shape and presence of X-ray emission (see for a recent discussion Kormendy et al. 2009).
This dichotomy extends also to radio properties. Radial brightness
profiles of sources with a moderate content of nuclear dust (de Ruiter
et al. 2005) are of core type. This has been confirmed by Balmaverde & Capetti (2006) & Capetti & Balmaverde (2006).
Observations suggest that there is a class of early-type galaxies that
will never harbour a classical radio source of the Fanaroff-Riley type
I or II.
These galaxies have steep power law inner profiles, with a slope (inner
Nuker law)
.
On the other hand galaxies with a core profile (
)
may or may not possess a nuclear radio source. This difference seems
genuine and not induced by selection effects. The absolute magnitudes
of core and power law galaxies overlap and the power law galaxies are
never associated with classical radio sources.
This result is consistent with the dichotomy described above and
suggests that AGN activity in core galaxies can be very pronounced and
that the dichotomy is the result of strong or weak AGN feedback
respectively (Kormendy et al. 2009).
4 Stellar velocity dispersion
To derive the CFP we need, together with the photometric data, the central velocity dispersion of
the galaxy. For 11 galaxies in the sample, we found measurements of the stellar velocity dispersion in the
literature, using the Lyon-Meudon Extragalactic Database (LEDA Paturel et al. 1997). These measurements
of
were corrected to a circular aperture with a metric diameter of 1.19 h-1 kpc ,
equivalent to 3.4
at the distance of the Coma cluster. To derive
for
the remaining sources, we carried out spectroscopic observations. We
were able to observe 27
out of the remaining 46 galaxies. One object (0648+27) was not included
in the final sample to derive the CFP, as explained in Appendix A1. For
this reason the final sample considered in this study is composed of 37
objects.
4.1 Spectroscopic observations
Optical spectroscopy in the range
Å and 4600-6500 Å
was obtained in service mode in two observing runs in 2005 and 2006 with the
Telescopio Nazionale Galileo (TNG). We used the spectrograph DOLORES
equipped with a Loral CCD with
pixels of 15
.
In 2005 we used the HRV Grism #6 with a slit of 1.0 arcsec, this yields a velocity dispersion
resolution
.
In 2006 we used the grism VHR-V with a slit of 1.0 arcsec,
this yields a
.
The plate scale across the dispersion is 0.275 arcsec/pix. In
addition to the radio galaxy spectra, we secured spectra of bright
stars of spectral type
from G8III to K1III with low rotational velocity, (
). These spectra
were used as templates of zero velocity dispersion. During the second observing run an early-
type galaxy (NGC 3377), as standard for the measurement of
,
was also observed. The slit was oriented
along the apparent major axis for all the galaxies in our sample except in the cases of galaxies
with multiple nuclei, where the slit was aligned along the two nuclei. All the spectra were bias and
flat-field corrected, trimmed and wavelength calibrated using standard procedures available in the
IRAF package. The accuracy of the latter procedure was checked with measurements of the night sky
Å emission line. The systemic velocity, corrected to the Sun, and the
velocity dispersion
were determined using the Fourier Quotient method (Sargent et al. 1977;
Bertola et al. 1994). The Fourier Quotient method was applied, using all the template stars, to all
spectra to obtain the radial velocity and the velocity dispersion. The rms of the determinations
obtained with different template stars turned out to be less than
for
and
for the systemic radial velocity
both for the sample of radio galaxies
than for the template galaxy. For NGC 3377 we found
in agreement with
the value of 139 km s-1 reported in LEDA. The average values of individual determinations were
adopted as final values of
and
.
In order to improve the S/N ratio of the spectra, we
co-added the central spectra within an aperture of 6
.
Since early-type galaxies
exhibit some gradients in the radial velocity and velocity dispersion, the derived central parameter
depends
on the distance of the galaxies and on the size of the aperture used
for the observation. In order to compare our velocity dispersions with
the data available in the literature, we applied aperture corrections
according to the procedure given by Jørgensen et al. (1996). The
individual measurements of
are corrected to a circular aperture with a metric diameter of 1.19 h-1 kpc , equivalent to 3.4
at the distance of the Coma cluster of galaxies.
![]() |
Figure 1:
The
|
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All these data are listed in Table 1, in which we also give
photometric data derived from HST images in the F814W
filter (all taken with an exposure time of 300 s): as described in
de Ruiter et al. (2002) the one-dimensional brightness profiles
determined with the IRAF task ELLIPSE were fitted with a Nuker law,
thus obtaining
for each galaxy, in the F814W (I) filter, the core radius
in arcsecs and the average surface brightness
(in mag/arcsec2) within the core radius.
For some galaxies the S/N is high enough to study the inner part of the rotation curve (see Fig. A.1). In Appendix A, comments on some individual objects are reported.
5 The CFP of radio and normal ellipticals
To complete our data-set we decided to collect all the available data
in the literature for the core properties of E galaxies. We added to
the RG data the core photometric data and the velocity dispersion for
two sets of data of non-radio galaxies. The first set is from the
classical work of Faber et al. (1997) which include data for 24 normal core
galaxies. To compare these measurements with our data for RG (derived in the R band) we applied a
mean color correction V-R=0.60. The second set is taken from the
recently published HST photometric data (Hyde et al. 2008) and the corresponding central
velocity dispersion
(Bernardi et al. 2008) for the core of 13 nearby non-radio massive galaxies.
The data of Hyde et al. (2008) were obtained using the high resolution channel (HRC) of the ACS in the iband, thus we transformed their CTPS to mag/sq/arcs using the zero point for the i filter ZP =
25.654 (AB mag). Then we applied a correction
to transform the data to the Vega
magnitude system. In Fig. 1 we plot the
projection of the CFP for our sample of radio galaxies, and for a
combined sample of non-radio ellipticals (Faber et al. 1997; Bernardi et al. 2008), we confirm the same correlation already found by Faber et al. (1997).
In order to derive the parameters (,
and
)
describing the CFP in the following relation:
![]() |
(1) |
we minimized the root square of the residual perpendicular to the plane. In Table 2 we report the coefficients obtained using this fitting procedure for the CFP of both radio galaxies and normal ones; for comparison we report also the coefficients for the FP for radio and normal galaxies (Bettoni et al. 2001).
Table 2: Coefficients of the best fit for the core fundamental plane and the global fundamental plane of low redshift radio galaxies (see Eq. (1)) and of normal galaxies.
In Fig. 2 we show the comparison of the CFP plotted with the coefficients of our best fit and with the coefficients of the best fit of FP (Bettoni et al. 2001). The two planes are very similar and almost parallel (see also Table 2). We note a slight tendency of CFP to show a curvature at low luminosity; this is similar to what was pointed out by Desroches et al. (2007, for the FP).
In Fig. 3 we compare the whole CFP with the FP derived from the global properties of a different sample of radio and non-radio ellipticals (see Bettoni et al. 2001, for details). Again the CFP and FP are closely parallel, as suggested by Faber et al. (1997): whatever differences exist among core galaxies these are not so large as to erase the appearance of a two-parameter family of self-gravitating cores that is similar to the 2-dimensional family of isothermal spheres.
6 Conclusions
![]() |
Figure 2: Upper panel: the best fit of the CFP for the B2 radio galaxies (black circles) compared with a sample of nearby (non radio) early type galaxies ([red] squares Faber et al. 1997; [green] triangles Bernardi et al. 2008), using the CFP fit in the y-axis. The solid line represents CFP relation. Lower panel: The same data as in the upper panel, but using the coefficient of the global FP fit of Bettoni et al. (2001) with a shift in the y-axis to take into account the different units on the x-axis (from kpc to pc); the solid line is the corresponding FP relation. The blue dashed line reports the fit to the core data with a shift of 0.23 dex. |
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![]() |
Figure 3:
The CFP of B2 radio galaxies (black circles) and
nearby (non radio) early-type galaxies ([red] squares
Faber et al. 1997; [green] triangles Bernardi et al. 2008)
compared to the Fundamental Plane of normal small black dots (Jørgensen et al. 1996) and
radio galaxies light-blue squares (Bettoni et al. 2001). The solid line represents the FP for
a sample of RG (Bettoni et al. 2001) while the dashed
line yields the fit to the core data. Note that we plot |
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We have presented the photometric, structural and kinematic properties of the centers of a sample of 38 low redshift radio galaxies galaxies and have shown that the conventional parameters characterizing the centers (the break radius, its surface brightness and the central velocity dispersion) are well represented in a plane (the core fundamental plane) which is indistinguishable from that of elliptical galaxies that do not exhibit radio emission.
A similar result was found from the comparison of the global properties of a sample of 72 radio galaxies and local ellipticals using the standard fundamental plane description (Bettoni et al. 2001). The comparison of the properties of the FP that refer to the whole galaxy with those concering the centers (the CFP) shows that the slopes of the two planes are very similar and suggest that the same mechanism is responsible for the link between the involved quantities.
The remarkable similarity of the properties of radio and non radio elliptical galaxies in the description of both the fundamental plane and the core fundamental plane indicates that the active phase of the galaxy connected with the strong emission at radio frequencies likely has an inconsequential effect on the structure of the whole galaxy. Moreover these results suggest that the two type of galaxies (radio and non-radio) have had a similar history of formation and evolution.
Appendix A: Notes on individual galaxies
B2 0648+27 - This galaxy shows a typical E+A spectrum indicating the presence of a young stellar population (Emonts et al. 2006; Emonts et al. 2008).
In this case the measured velocity dispersion is only indicative having been measured using an imperfect stellar template.
This galaxy was not used to construct the CFP of RG. The spectrum show the [OII] 3727 Å
emission line. For this object we were able to measure the rotation
curve (both for gas and stars) and the velocity dispersion profile in
the inner
,
these are shown in Fig. A.1. We found a
km s-1 for both components.
B2 0908+37 - As noted by Capetti et al. (2000) a fainter companion galaxy is located
to the SW.
Our spectrum crosses on the faint companion for which we were able to measure a redshift
,
very close to the redshift of the radio galaxy.
B2 0924+30 - For this galaxy we measure a rotation
km s-1 in the inner
(see Fig. A.1).
B2 1113+24 - For this galaxy we measure a rotation
km s-1 in the inner
(see Fig. A.1).
B2 1204+34 - This galaxy show strong emission lines in the spectrum i.e [O III]
5007 Å and
.
We measured the gas rotation curve, and after subtraction of the
emission component, also the stellar rotation curve (see Fig. A.1).
The gas is more extended in the NE direction and show a
200 km s-1.
B2 1322+36 - NGC 5141 - This S0 galaxy has a nuclear dust lane and the gas exhibits a regular rotation profile as measured by Noel-Storr et al. (2003).
Here we measure, for the first time, a regular rotation curve for the stellar component with a
km s-1 at
(see Fig. A.1).
Our spectra are in the region
3800-4800 Å where only a very faint
3727 [OII] line is visible; the gas and stellar components are co-rotating.
![]() |
Figure A.1: Rotation curves and velocity dispersion profiles for selected low redshift radio galaxies (full squares stars, open squares gas). |
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B2 1422+26B - This galaxy show the presence in the spectrum of the [O II]
3727 Å line.
B2 1450+28 - This galaxy is a well known dumbbell system in the center of the cluster Abell 1984. The radio
galaxy is associated with the southern galaxy of the pair. To obtain our spectrum, the slit was oriented at PA = 0
and crosses both galaxies.
In Table 1 we report the velocity dispersion for both objects. In Table 1 the non-radio galaxy is labelled with an asterisk and was excluded from the fit.
B2 1502+26 - 3C 310 - This galaxy shows a boxy elliptical galaxy approximately
SW, the slit for our spectrum was oriented at
PA =
and crosses both galaxies, for the fainter companion we measure the same redshift
z = 0.0540 and a velocity dispersion
km s-1.
B2 1527+30 - in Abell 2083; this galaxy show a strong velocity gradient
km s-1 in the inner
(see Fig. A.1).
We thanks the anonymous referee whose comments helped us to improve our manuscript. This research made use of Vizier service (Ochsenbein et al. 2000) and 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. We have made use of the LEDA (http://leda.univ-lyon1.fr) and Hypercat database.
References
- Balmaverde, B., & Capetti, A. 2006, A&A, 447, 97 [NASA ADS] [EDP Sciences] [CrossRef]
- Bernardi, M., Hyde, J. B., Fritz, A., et al. 2008, MNRAS, 391, 1191 [NASA ADS] [CrossRef]
- Bettoni, D., Falomo, R., Fasano, G., et al. 2001, A&A, 380, 471 [NASA ADS] [EDP Sciences] [CrossRef]
- Bertola F., Bettoni, D., Rusconi, L., & Sedmak, G. 1994, AJ, 89, 356 [NASA ADS] [CrossRef]
- Capetti, A., & Balmaverde, B. 2006, A&A, 453, 27 [NASA ADS] [EDP Sciences] [CrossRef]
- Capetti, A., & Celotti, A. 1999, MNRAS, 304, 434 [NASA ADS] [CrossRef]
- Capetti, A., de Ruiter, H. R., & Fanti, R. 2000, A&A, 362, 871 [NASA ADS]
- Colla, G., Fanti, C., Fanti, R., et al. 1975, A&AS, 20, 1 [NASA ADS]
- Desroches, L.-B., Quataert, E., Ma, C.-P., & West, A. A. 2007, MNRAS, 377, 402 [NASA ADS] [CrossRef]
- De Koff, S., Baum, S. A., Sparks, W. B., et al. 1996, ApJS, 107, 621 [NASA ADS] [CrossRef]
- De Juan, L., Colina, L., & Golombek, D. 1996, A&A, 305, 776 [NASA ADS]
- de Ruiter, H. R., Parma, P., Fanti, C., & Fanti, R. 1990, A&A, 227, 351 [NASA ADS]
- de Ruiter, H., Parma, P., Capetti, A., Fanti, R., & Morganti, R. 2002, A&A, 396, 857 [NASA ADS] [EDP Sciences] [CrossRef]
- de Ruiter, H. R., Parma, P., & Capetti, A. 2005, A&A, 439, 487 [NASA ADS] [EDP Sciences] [CrossRef]
- Emonts, B. H. C., Morganti, R., Tadhunter, C. N., et al. 2006, A&A, 454, 125 [NASA ADS] [EDP Sciences] [CrossRef]
- Emonts, B. H. C., Morganti, R., van Gorkom, J. H., et al. 2008, A&A, 488, 519 [NASA ADS] [EDP Sciences] [CrossRef]
- Faber, S. M., Tremaine, S., Ajhar, E. A., et al. 1997, ApJ, 114, 5
- Fanti, R., Gioia, I., Lari, C., & Ulrich, M. H. 1978, A&AS, 34, 341 [NASA ADS]
- Fanti, C., Fanti, R., De Ruiter, H. R., & Parma, P. 1987, A&AS, 69, 57 [NASA ADS]
- Ferrarese, L., & Merritt, D. 2000, ApJ, 539, L9 [NASA ADS] [CrossRef]
- González-Serrano, J. I., & Carballo, R. 2000, A&AS, 142, 353 [NASA ADS] [EDP Sciences] [CrossRef]
- González-Serrano, J. I., Carballo, R., & Perez-Fournon 1993, AJ, 105, 1710 [NASA ADS] [CrossRef]
- Jaffe, W., Ford, H. C., Ferrarese, L., Van den Bosch, F., & O'Connell, R.W. 1993, Nature, 364, 213 [NASA ADS] [CrossRef]
- Jørgensen, I., Franx, M., & Kjaergaard, P. 1996, MNRAS, 280, 167 [NASA ADS]
- Hyde, J. B., Bernardi, M., Sheth, R. K., & Nichol, R. C. 2008, MNRAS, 391, 1559 [NASA ADS] [CrossRef]
- Kormendy, J., Fisher, D. B., Cornell, M. E., & Bender, R. 2009, ApJS, 182, 21 [NASA ADS] [CrossRef]
- Lauer, T. R., Faber, S. M., Richstone, D., et al. 2007, ApJ, 662, 808 [NASA ADS] [CrossRef]
- Massaglia, S., Trussoni, E., Caucino, S., et al. 1996, A&A, 309, 75 [NASA ADS]
- Morganti, R., Fanti, R., Gioia, I. M., et al. 1988, A&A, 189, 11 [NASA ADS]
- Morganti, R., Parma, P., Capetti, A., et al. 1997, A&AS, 126, 335 [NASA ADS] [EDP Sciences] [CrossRef]
- Noel-Storr, J., Baum, S. A., Verdoes Kleijn, G., et al. 2003, ApJS, 148, 419 [NASA ADS] [CrossRef]
- Ochsenbein, F., Bauer, P., & Marcout, J. 2000, A&ASS, 143, 23 [NASA ADS] [CrossRef]
- Parma, P., Fanti, C., Fanti, R., Morganti, R., & De Ruiter, H. R. 1987, A&A, 181, 244 [NASA ADS].
- Paturel, G., Andernach, H., Bottinelli, L., et al. 1997, A&AS, 124, 109 [NASA ADS] [EDP Sciences] [CrossRef]
- Sargent, W. L. W., Schechter, P. L., Boksenberg, A., & Shortridge, K. 1977, ApJ, 212, 326 [NASA ADS] [CrossRef]
- Trussoni, E., Massaglia, S., Ferrari, R., et al. 1997, A&A, 327, 27 [NASA ADS]
- Verdoes Kleijn, G. A., Baum, S. A., de Zeeuw, P. T., & O'Dea, C. P. 1999, AJ, 118, 2592 [NASA ADS] [CrossRef]
All Tables
Table 1: The sample of low redshift B2 radio galaxies with velocity dispersion measurements.
Table 2: Coefficients of the best fit for the core fundamental plane and the global fundamental plane of low redshift radio galaxies (see Eq. (1)) and of normal galaxies.
All Figures
![]() |
Figure 1:
The
|
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In the text |
![]() |
Figure 2: Upper panel: the best fit of the CFP for the B2 radio galaxies (black circles) compared with a sample of nearby (non radio) early type galaxies ([red] squares Faber et al. 1997; [green] triangles Bernardi et al. 2008), using the CFP fit in the y-axis. The solid line represents CFP relation. Lower panel: The same data as in the upper panel, but using the coefficient of the global FP fit of Bettoni et al. (2001) with a shift in the y-axis to take into account the different units on the x-axis (from kpc to pc); the solid line is the corresponding FP relation. The blue dashed line reports the fit to the core data with a shift of 0.23 dex. |
Open with DEXTER | |
In the text |
![]() |
Figure 3:
The CFP of B2 radio galaxies (black circles) and
nearby (non radio) early-type galaxies ([red] squares
Faber et al. 1997; [green] triangles Bernardi et al. 2008)
compared to the Fundamental Plane of normal small black dots (Jørgensen et al. 1996) and
radio galaxies light-blue squares (Bettoni et al. 2001). The solid line represents the FP for
a sample of RG (Bettoni et al. 2001) while the dashed
line yields the fit to the core data. Note that we plot |
Open with DEXTER | |
In the text |
![]() |
Figure A.1: Rotation curves and velocity dispersion profiles for selected low redshift radio galaxies (full squares stars, open squares gas). |
Open with DEXTER | |
In the text |
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