To avoid any confusion due to the complexity in both the photometry and the
kinematics of NGC 4621, we will use the following convention: the photometric
major axis of the galaxy (as measured by HST) defines the x-axis, the
negative values being in the SE quadrant, referred to as the left side of the
galaxy. The center (0,0) is defined as the center of the HST isophotes of
NGC 4621 within 1
,
excluding the central 0
1, the isophotes of
which exhibit a significant asymmetry (see next section). The centering and
rotation procedures of the HST frames have been performed using an algorithm
which minimizes the standard deviation of the recentered and rotated frame
subtracted by its flipped counterpart. This leads to accuracies of 0.1 degrees
and 0
005. All figures in this paper share a common orientation, as shown
in Fig. 3.
The OASIS stellar mean velocity and dispersion maps are presented in
Fig. 1. The datacubes have been centered and rotated in order to
match the HST data, using the center and angle provided by the PSF fitting
procedure mentioned in Sect. 2. The velocity field reveals a
clear counter-rotating core (CRC). The position of the zero-velocity curve is
used to measure the center and the size of the CRC: it is 1
7 (150 pc) in
diameter, and off-centered by
towards the SE. The total
velocity amplitude observed within the central 1
along the major axis
is 100 km s-1, while the peak-to-peak velocity amplitude of the CRC's is only
35 km s-1. The stellar velocity dispersion map peaks at
km s-1.
The dispersion map however exhibits high frequency substructures in the
central 0
5 (Fig. 1), the minor-axis dispersion profile even
having a local minimum at the centre. Considering the amplitude of these
structures and their spatial scales (comparable to the local FWHM), we should
wait for data with better signal to noise ratio to discuss these features.
The BSG94 data show no significant minor-axis rotation, and a maximum velocity
of 140 km s-1 at 30
(see BSG94 or Fig. 7). Besides
a relatively weak velocity amplitude in the innermost 4
(<60 km s-1), these data do not show any hint for the existence of the
counter-rotating core. We will use the BSG94 kinematics to constrain the
dynamical model outside the OASIS field of view.
The STIS velocities and dispersions are shown in Fig. 2. In
these data the size of the CRC is 0
7 (
60 pc) and its velocity
center is located at
(
4.5 pc). We have carefully
checked the centering of the STIS data with respect to
the reference WFPC2 images, and found that this offset is robust.
At STIS resolution the major-axis velocities of the CRC reach
75 km s-1with respect to the systemic. The maximum velocity
dispersion is
km s-1, at
.
These values are consistent with the OASIS data considering the
higher spatial resolution of the STIS data.
Both F555W and F814W images reveal a peculiar structure in the core. Indeed,
the luminosity peak is offset from the center of the outer isophotes by
0
01 towards the east. The photometric peak is located in the upper
left quadrant (Fig. 3). This feature does not seem to be an
artefact, as it is clearly visible on each individual HST frame, and in both
bands, and cannot be attributed to centering uncertainties (0
005).
The two HST frames were then PSF-crossconvolved and divided to obtain
a V - I colour image (Fig. 4). It reveals a central gradient (V-Iincreases towards the center) with a y-axis elongated structure
centered at (-0
02, 0
01) (see dashed line on
Fig. 3). The isochromes have slightly higher ellipticities than
the isophotes (
at 2
5 for V-I, vs. 0.4 for the V frame).
Copyright ESO 2002