Up: V, I CCD photometry of 6553
Subsections
Figure 3 shows the V, (V-I) and I, (V-I) diagrams of all 40170
stars that were identified independently in both V
and I filters. The CMD shows the difficulties present in the
study of cluster NGC 6553. The field population dominates in the fainter stars
( 18) so much that the cluster sub-giant branch, MSTO region
and MS itself are not visible at all. In the brighter stars, typical features
of the field population in the direction of the Galactic centre and cluster
RGB are clearly visible. The RGB of NGC 6553 is marked as cluster
sequence in the Fig. 3. It turns over at about V = 15.3,
(V-I) = 2.9 in the V, (V-I) diagram. No such turnover is seen in the I,
(V-I) diagram.
To the blue side of this sequence, the MS of the young Galactic disk stars
can be easily identified while the older bulge populations are
present towards the redder side. Both cluster and field populations contain
a significant number of bright but very red stars with (V-I)
4.0. These stars should be taken into account in population synthesis
when interpreting red integrated colours of Galactic bulge populations.
Before discussing the features of cluster or field population any further
it is essential to determine the regions in sky where one dominates over the
other. In order to find out where the field population becomes dominant with
respect to the cluster population we determined the radial stellar density
profile of the region using stars brighter than V=20 mag. The (X,Y) pixel
coordinates of the eye-estimated cluster centre are (440, 645) with an accuracy
of few arcsec. The observed stellar density profile up to 7 from
the cluster centre is plotted in Fig. 4. The stellar densities
derived here are not corrected for data incompleteness. They are therefore
underestimated for inner regions (upto a radial distance of about 1), as
the plot shown by
Trager et al. (1995)
indicates that data completness could
be less than 50% in the central bin and reaches to 100% only at about
1. Since the cluster profiles from star counts are better than those
from integrated photometry in the outer regions, we have used the former for
determining outer boundary of the dominant regions of the cluster population.
The stellar density decreases strongly from cluster centre out to about a
radius of 3. Beyond that it becomes asymptotic at a level of about
150 stars arcmin-2. The profile given by
King (1962)
fits the observed
stellar density profile satisfactorily.
|
Figure 4:
This plot shows the observed stellar
density (logarithm of stars brighter than V=20 mag per square arcmin)
as a function of radius in arcmin. The length of the bar denotes the error in
density determination due to number statistics. The solid curve shows a
least square fit of the King profile. The cluster population is not
dominant beyond a radial distance of about |
The above analysis clearly indicates that the population of the cluster NGC 6553
is not dominant beyond a radial distance of and most of the stars
present in that part of the sky represent the field population. We
therefore considered stars with Y < 0 pixels (outside the cluster frame;
see Fig. 1), i.e., from the cluster centre as representative
of the field population. In order to maximise the percentage of cluster
members in the sample and to avoid the effects of strong stellar crowding on
the VI data, we consider only stars lying in an annular region (defined with
inner and outer radii of 17 to 100 arcsec respectively) as
representative of cluster population. The V, (V-I) diagrams
for the representatives of field and cluster populations are shown in
Fig. 5. Their respective numbers are about 14250 and 8500. The
corresponding areas are about 23.6 and 8.4 arcmin2. The dominance of one
population over other can be clearly seen in the both diagrams. With these
better defined features of the two populations contamination effects in the
CMDs stand out more clearly now. The limiting V mag of the field population
is about a magnitude fainter than that of the cluster even though the exposure
times are similar (see
Table 1). This illustrates the effect
of crowding on the limiting magnitude of the observations.
We will now analyse both populations separately.
|
Figure 5:
The V, (V-I) diagram for
the representatives of cluster and field populations. The regions
from where they were selected are listed. Dominance of one population
over other can be clearly seen in these diagrams |
We have carried out statistical field star subtraction. For this, we consider
only stars brighter than V = 20 mag in both cluster and field populations,
since the cluster HB and RGB are present there.
The field population used in the statistical subtraction has been selected
from a rectangular region with coordinates (in pixels) X=0 to 1000
and Y=-725 to -450. Thus the area is equal to that of the cluster region
but located at a radial distance of about 7 from the cluster centre.
At this radial distance, the cluster population will be negligible, as the
values of core and tidal radii for the cluster are about 0.6
and 8 respectively (cf.
Trager et al. 1995).
There are 3914 and 1317
stars brighter than V = 20 mag in the
chosen cluster and field regions respectively. The statistical field
star subtraction is done in the following manner. For each star of the
field population, the nearest star located within a box of size 0.5 mag
in V and 0.2 mag in (V-I) from the V, (V-I) position of the field
star in the CMD of the cluster region is deleted from the sample. This procedure
will remove statistically field stars from the selected cluster region.
However, precisely because of this we cannot completely rule out the presence
of some field stars in the cleaned sample or oversubtraction in the cluster
data. The lower part of the Fig. 6 shows the CMD of the cleaned
sample. The RGB and HB are very well defined in the diagram. Some field stars
mostly right side of the cluster SGB are still present in the diagram but they
will not affect the results.
Up: V, I CCD photometry of 6553
Copyright The European Southern Observatory (ESO)