Mkn 1 (NGC 449) is a highly inclined SB0a galaxy at redshift z = 0.0159,
with 1'' corresponding to 460 pc projected distance in the sky. We show its B
band image in Fig. 1.
The [OIII] emission has radial extent 9'' (4
kpc) at PA = 83
, elongated along the major axis of the nuclear
continuum at PA = 87
(Mulchaey & Wilson 1995).
Although the profiles of optical emission lines of Mkn 1 show blue asymmetry (e.g. De Robertis & Shaw 1990), no asymmetry or evident broad wings are seen in the near-infrared (NIR; Veilleux et al. 1997). There is, therefore, no strong evidence for an obscured BLR in Mkn 1.
We show the B-I map of Mkn 1 in Fig. 2.
There are several blue regions in
the host galaxy to the E and SE of the nucleus, probably related to star
forming activity, and an arclike red region situated S of the nucleus. Closer
to the center, there is a blue elongated structure of 2.5'' (1.2 kpc
extent across the nucleus at PA = 290
). The nucleus is slightly
closer to the E end of this elongation. Although not closely parallel to the
axis of the [OIII] emission
(PA = 83
; Mulchaey & Wilson 1995), this
blue elongation may be caused by scattered light from the nucleus. We shall
discuss the origin of the detected structures in all the galaxies, in the
context of the unified models, in Sect. 4. The colours of the blue
elongation are given in Table 3.1. Note that in all the galaxies studied, these
colours include a contribution from the red underlying stellar population in
the nuclear region. Therefore, the real colours of the structures must be
even bluer than those reported here.
![]() |
Mkn 533 (NGC 7674, Arp 182) is an SBb spiral galaxy at z = 0.0289, with 1''
corresponding to 840 pc projected distance in sky. We show the B band image
of Mkn 533 in Fig. 3.
It has asymmetric arms and tidal connection to the
nearby compact elliptical, NGC 7675. Mkn 533 has a nuclear double radio
source, with diameter 0.75'' (630 pc) at PA = 117
(Kukula et al.1995). H
emission of Mkn 533
has polarised broad wings (Miller & Goodrich 1990;
Tran 1995a; Young et al.1996). The
nuclear polarisation
rises steeply to the blue, the polarised flux spectrum is much
bluer than the
total flux spectrum, and the polarisation PA
31
is independent
of wavelength, and perpendicular to the radio axis. All this indicates dust
scattering as the main polarisation mechanism.
The forbidden optical emission lines (e.g. [OIII]) in Mkn 533 have strong blue
wings (e.g. De Robertis & Shaw 1990; Veilleux 1991) and broad wings have been
found in the NIR HeI, Pa and Br
lines
(Ruiz et al. 1994; Veilleux et al.1997). Further evidence for an obscured central source
in Mkn 533 comes from the hard X-ray spectrum, which shows a prominent Fe K
line and a flat powerlaw continuum, well fitted by a steep intrinsic spectrum
reflected by optically thick cold matter (Malaguti et al.1998). The intrinsic
X-ray luminosity is at least one order of magnitude larger than what is
observed.
We present the B-I maps of Mkn 533 in Fig. 4
(the whole galaxy) and Fig. 5
(nuclear region).
The spiral structure, effects of dust reddening and star
forming regions are clearly visible in the disk of Mkn 533 (Fig. 4). In the
nuclear region (Fig. 5), there is a blue elongation from the nucleus to NW
(PA = 310) of 3.2'' (2.7 kpc) total extent. This structure is
aligned closely parallel to the radio axis and perpendicular to the
polarisation orientation, and probably represents scattered light from the
nucleus. Its colours are given in Table 3.1.
Mkn 607 (NGC 1320) is a nearly edge-on S0a galaxy at redshift z = 0.0090,
with 1'' corresponding to 260 pc projected distance in the sky. We show a B
band image of Mkn 607 in Fig. 6.
The [OIII] emission is extended along the
major axis of the host galaxy (PA = 137) with
12'' (3.1 kpc)
radius (Mulchaey et al. 1996b). The PA of the innermost [OIII]
emission and that of the nuclear continuum emission is 132
(Mulchaey
& Wilson 1995; Mulchaey et al.1996b).
We show the B-I maps of Mkn 607 in Fig. 7
(the whole galaxy) and Fig. 8 (nuclear region). A red narrow dust lane at closest distance of 5.1'' (1.3
kpc) is visible along the whole SW side of the host galaxy (already seen in
the B band image; Fig. 6). Several blue star forming regions can be detected
in the host galaxy (Fig. 7). In the central region (Fig. 8), a red extended
region is visible on the SW side of the nucleus (at 1.2''; 310 pc),
probably related to the larger scale SW dust lane. In addition, there is a
faint blue elongated structure emanating from the nucleus toward NW (PA =
320) up to 0.9'' (230 pc) distance. Its orientation agrees
perfectly with the axis of the [OIII] emission, and possibly represents
scattered light from the nucleus. Its colours are given in Table 3.1.
Mkn 1066 (UGC 2456) is an inclined SB(s)0 galaxy at redshift z = 0.0121,
with
1'' corresponding to 350 pc projected distance on the sky. We show its B
band image in Fig. 9.
The nuclear continuum is aligned at
PA = 137 (Mulchaey et al.1996b). The radial extent of the [OIII] emission
is 6.5'' (2.3 kpc) at PA = 134
, with a double structure across the
nucleus separated by
3.3'' (1.2 kpc) at PA = 131
(Mulchaey et al.1996b). The innermost [OIII] gas is concentrated into a narrow
jet-like feature extending 1.4'' (490 pc) NW of the nucleus at
PA
, with much fainter emission up to 0.8'' (280 pc) SE at
PA
130
(Bower et al.1995). The [OIII] emission is thus parallel
to the axis of the linear triple radio source extending 2.8'' (1.0 kpc)
with bipolar jetlike morphology along PA = 134
(Ulvestad & Wilson 1989). No polarised or NIR broad lines have been detected in Mkn 1066
(Miller & Goodrich 1990; Kay 1994;
Veilleux et al.1997), and the UV continuum
polarisation is parallel to the radio axis, unlike in the Seyfert 2s with
evidence for scattered nuclear light.
We show the B-I map of Mkn 1066 in Fig. 10.
Note that the I band nucleus is
saturated, so the structure in the central few pixels is not real. The star
forming regions in the host galaxy are clearly visible in Fig. 10. There is a
very red region SW of the nucleus at 2.6'' (910 pc). Finally, there is a
blue elongated structure NW of the nucleus
(PA = 325) with total
extent 4.2'' (1.5 kpc). This structure agrees well with the axis of the
[OIII] and radio emission, and possibly represents scattered light from the
nucleus. Its colours are given in Table 3.1.
NGC 788 is an S0a galaxy at redshift z = 0.0136, with 1'' corresponding to
390 pc projected distance in the sky. We show its B band image of in
Fig. 11.
It shows faint spiral arms at 30'' (12 kpc) radius from the nucleus.
The [OIII] emission extends to 4.3'' (1.7 kpc) from the nucleus at
PA = 105
, while the major axis of the nuclear continuum is at PA =
112
(Mulchaey et al.1996b).
We show B-I maps of NGC 788 in Fig. 12
(the whole galaxy) and
Fig. 13
(nuclear region). The blue inclined ring of emission with 30'' (12
kpc) radius around the nucleus, tracing the faint spiral structure is clearly
visible in Fig. 12. The nucleus is situated between two blue
regions (Fig. 13), the less extended at 0.4'' (160 pc) S (PA = 170
) and the more
extended at 1.1'' (430 pc) NW (PA = 315
). There is also a red
extended region at 1.3'' (510 pc) S-SW of the nucleus. Although the axis
of the blue double structure (PA
150
) does not correspond well
with the axis of the [OIII] emission (PA = 105
), the blue maxima may
represent localized peaks in the scattered light from the nucleus. Their
colours are given in Table 3.1.
NGC 5347 is an SBab galaxy at redshift z = 0.00778, with 1'' corresponding
to 230 pc projected distance in the sky. Its B band image is presented in
Fig. 14. It shows a bar enclosed by a ring structure at 25'' (5.8
kpc) radius, and faint spiral arms emerging from the ring at the ends of the
bar (see also Gonzalez-Delgado & Perez 1996). The bar is oriented roughly
parallel to the major axis of the galaxy. The [OIII] emission of NGC 5347 has
a double nuclear structure perpendicular to the bar (Pogge 1989). An
H
emission knot is located at 2.7'' (620 pc) NE at PA =
25
from the nucleus, perpendicular to the bar
(Gonzalez-Delgado & Perez 1996). The knot has high excitation spectrum and a large Ca triplet EW,
suggesting the presence of red supergiants associated with an old burst of
star formation. The emission line ratios of the knot, however, indicate
photoionisation by a hard AGN continuum (Gonzalez-Delgado
& Perez 1996). The
nuclear continuum emission is probably emitted anisotropically, as supported
by photon deficit arguments (Gonzalez-Delgado & Perez 1996).
We show the B-I map of NGC 5347 in Fig. 15. The blue star forming regions,
the ring structure and the spiral arms in the host galaxy are clearly
visible. There is also a red dust lane running S of the nucleus roughly E to
W at a closest distance of 3.3'' (760 pc), delineating the bar. In the
central region, the emission knot at 2.7'' (620 pc) at PA = 25 NE
of the nucleus is clearly seen. Even closer to the nucleus, there is a blue
elongated structure with total extent
1.3'' (300 pc) toward N of the
nucleus
(PA = 10
). These structures probably represent the brightest
localized peaks in the scattered light from the nucleus. Their colours are
given in Table 3.1.
NGC 5929 is an Sab pec galaxy interacting with the starburst galaxy NGC 5930,
together forming the galaxy pair Arp 90. The redshift of NGC 5929 is z =
0.00854, with 1'' corresponding to 250 pc projected distance in the sky.
The B band image of the system is shown in Fig. 16. NGC 5929 has a faint hard
X-ray spectrum, implying heavy absorption (Rush & Malkan 1996).
It has
triple radio structure extended along PA = 61, with total diameter
1.3'' (320 pc; Su et al.1996). The SW lobe is at 0.7'' (170 pc) distance
from the nucleus and is slightly stronger than the NE lobe at 0.6'' (150
pc) distance. The [OIII] emission resembles closely the radio morphology,
with two peaks straddling the nucleus at PA
60
(Bower et al.
1994). However, the [OIII] peaks are closer to the nucleus (1.1'' = 280 pc
separation). Also, the NE [OIII] component is bisected by a dust lane. The
[OIII] emission does not define a clear biconical morphology as in many other
Seyfert 2s. Also, there is no evidence for obscuration in the direct images,
except the dust lane, nor do energy balance considerations suggest anisotropy
of the nuclear radiation (Bower et al.1994).
We show the B-I maps of the whole system in Fig. 17 and of NGC 5929 in
Fig. 18. There is a blue stellar tail from the N part of NGC 5929 toward NGC 5930
and a red bridge between the galaxies, probably stellar emission reddened by
the disc of NGC 5930 (Fig. 17; see also Lewis & Bowen 1993). The nucleus of
NGC 5929 (Fig. 18) is situated between two blue maxima at opposite sides of
the nucleus, the closer and brighter at 0.8'' (200 pc) SW (PA =
225) and the more distant and fainter at 2.0'' NE (PA =
45
). Since the orientation of this structure agrees well with the
[OIII] and radio axes, and the peaks are only slightly further away from the
nucleus than the respective [OIII] and radio peaks, they possibly represent
extranuclear scattering mirrors of anisotropically escaping nuclear light.
The colours of the blue maxima are given in Table 3.1. A very red region,
probably due to dust emission, is located 3.4'' (850 pc) S of the nucleus
(PA = 166
).
NGC 5953 is an S0/a pec spiral galaxy at redshift z = 0.00655, with 1'' corresponding to 190 pc projected distance in the sky. It interacts with the late-type spiral NGC 5954, and together they form the galaxy pair Arp 91 (VV 244). We show a B band image of the system in Fig. 19. While NGC 5954 has pronounced spiral arms, faint emission to N and W of its disk and a stellar bridge extending toward NGC 5953, the latter appears relatively smooth. HI maps (Chengalur et al. 1995) show a long plume of emission to NW of NGC 5953, corresponding to faint optical stellar emission (Fig. 19), and probably associated to the S stellar bridge of NGC 5954.
From long-slit spectroscopy, Yoshida et al.(1993) detected an inclined ring
of giant star forming regions around the nucleus of NGC 5953, with ring
diameter 15'' (2.9 kpc). More recently, the circumnuclear star
forming properties of NGC 5953 were studied by [OIII] and H
imaging
(Gonzalez-Delgado & Perez 1997) and by UV imaging
(Colina et al.1997). The
UV continuum is concentrated in several compact circumnuclear knots in a ring
with similar morphology to H
. Yoshida et al.(1993)
detected also a
high-ionisation region 4'' (760 pc) NE from the nucleus at
PA
. Its location agrees well with radio morphology (PA =
40
; Jenkins 1984), and it is probably ionised by an anisotropic
nuclear continuum. Yoshida et al.estimate that the flux seen by the ENLR is
an order of magnitude higher than that directly observed. The lack of similar
emission region on the opposite (SW) side of the nucleus is probably due to
obscuration and/or the torus inclination.
We show the B-I maps of the whole system in Fig. 20 and of NGC 5953 in
Fig. 21. The overall features already visible in the direct B band image
(Fig. 19), such as the stellar bridge between the galaxies, and the long plume of
emission to NW of NGC 5953, are even more clearly visible in the B-I map
(Fig. 20). In NGC 5953, the B-I map (Fig. 21) clearly shows the inclined
star forming ring oriented roughly N-S with diameter 8''
(
kpc). There is a red arc around the nucleus E-N-W with two main peaks at
1.6'' (300 pc) at PA = 320
, and at 1.8'' (340 pc) at PA =
60
, inside the star forming ring. Finally, there is a faint narrow
blue elongated structure of 0.5'' (100 pc) extent at PA = 220
. This
elongation is at similar orientation to the [OIII] and radio axes and
probably represent scattered light from the nucleus. Its colours are given in
Table 3.1.
NGC 7212 is in a pair of interacting galaxies. Its redshift is z = 0.0266,
with 1'' corresponding to 770 pc projected distance in the sky. We
show the B band image of NGC 7212 in Fig. 22. Polarised spectra of NGC 7212
show broad components to H
and H
, and this polarisation is
higher than that in the continuum (Tran et al. 1992;
Tran 1995a), an
indication of a hidden BLR. Most likely, the polarisation arises from
scattering by dust (Tran 1995a), because the spectrum is very red, the
continuum polarisation rises smoothly to the blue, and the polarised flux
spectrum is bluer than total flux spectrum. The [OIII] emission of NGC 7212
shows a jet-like high-ionisation feature extending up to 10'' (7.7 kpc)
from the nucleus at PA = 10
(Tran 1995a). This jet is exactly
parallel to the axis of the small scale double radio source (0.7''
separation; Falcke et al. 1998), and roughly perpendicular to the
optical polarisation (PA = 93
), suggesting that the jet is collimated
radiation from the hidden nucleus obscured by a torus. The line ratios of the
jet indicate photoinisation by the nuclear continuum. There is a faint broad
base to H
, probably the BLR reflected from the obscured nucleus by an
offnuclear scattering mirror. However, no obvious BLR component to NIR lines
was found by Veilleux et al.(1997).
We show the B-I maps of NGC 7212 in Fig. 23 (the whole system) and
Fig. 24 (NGC 7212). The nucleus of NGC 7212 is very blue and an extended fan-shaped
blue emission region extends from the nucleus to S (PA = 165) with
total extent 2.3'' (1.8 kpc). This blue region is bisected by a red dust
lane. A much redder narrow dust lane is situated on the other side of the
nucleus, at closest distance 3.7'' (2.8 kpc) at PA = 280
. Although
the orientation of the blue elongation does not correspond perfectly with the
[OIII] emission, it may represent scattered light from the nucleus. Its
colours are given in Table 3.1.
NGC 7319 (Arp 319) is an SBb galaxy belonging to the Stephen's Quintet
compact group of galaxies. Its redshift is z = 0.0225, with 1''
corresponding to 650 pc projected distance in the sky. We show the B band
image of NGC 7319 in Fig. 25. In the radio (van der Hulst & Rots 1981), NGC
7319 shows a jet-like feature SW to the nucleus at PA =
207 extending
6'' (3.9 kpc). The X-ray emission from
Stephan's Quintet consists of two components: the soft X-ray emission
probably arises from hot intracluster gas
(Sulentic et al. 1995),
while the hard X-ray emission, peaked on NGC 7319, is consistent with an
absorbed powerlaw, and exhibits a strong Fe K line, providing strong evidence
for an obscured nucleus in NGC 7319 (Awaki et al.1997).
The [OIII] emission of NGC 7319 extends for 10'' (6.5 kpc) toward
S-SW, possibly in the form of an ionisation cone (Aoki et al.1996). The
[OIII] morphology and PA agree well with the radio, however, the [OIII] peak
is closer to the nucleus than the radio peak. The kinematics of the extended
[OIII] emission indicates a high velocity outflow up to
9'' (5.8 kpc)
from the nucleus, mainly photoionised by the nuclear
radiation (Aoki et al.1996). The number of ionising photons required to ionise the ENLR is over 10
times higher than the number of photons in our line of sight, strongly
indicating an anisotropic nuclear radiation field (Aoki et al.1996).
We show the B-I map of NGC 7319 in Fig. 26. To the S of the nucleus (PA =
210) there is a very red region at 0.7'' (460 pc), continuing
further S as a more extended red region. The bluest region is situated
1.1'' (720 pc) N of the nucleus (PA = 10
). The orientation of the
blue elongation agrees well with the [OIII] and radio axes, and probably
represents scattered light from the nucleus. Its colours are given in
Table 3.1.
![]() |
Figure 3:
The B band image of Mkn 533. The size of the image is
![]() ![]() |
![]() |
Figure 5:
The B-I map of the
innermost ![]() ![]() |
![]() |
Figure 8:
The B-I map of the innermost ![]() ![]() ![]() |
![]() |
Figure 12:
The B-I map of NGC 788. The size of the image is
![]() ![]() ![]() ![]() ![]() |
![]() |
Figure 13:
The B-I map of the innermost ![]() ![]() |
![]() |
Figure 16:
The B band image of NGC 5929/5930. The size of the
image is ![]() ![]() |
![]() |
Figure 18:
The B-I map of the innermost ![]() ![]() |
![]() |
Figure 19:
The B band image of NGC 5953/5954. The size of the
image is ![]() ![]() |
![]() |
Figure 21:
The B-I map of the innermost ![]() ![]() |
![]() |
Figure 24:
The B-I map of the innermost ![]() ![]() |
![]() |
Figure 25:
The B band image of NGC 7319. The size of the image
is ![]() ![]() |
Copyright The European Southern Observatory (ESO)