Terzan 9 is also designated GCl B1758-268 and ESO521-SC11, and is located at
= 17
58
31.2
,
(
,
).
Malkan (1982)
derived
E(B-V)= 1.7 from
integrated infrared photometry, and
Zinn (1985)
based on the same data
estimated a metallicity
. Using near infrared integrated
spectroscopy, Armandroff & Zinn (1988)
derived
from CaII triplet lines, and
E(B-V)=1.25 from the interstellar band at 8621 Å.
By means of the
bright giants method
Webbink (1985)
estimated an horizontal branch level of
which, combined to a reddening of
E(B-V)=1.71 based on
Malkan's data, led to a distance from the Sun of
kpc.
Webbink (1985)
lists a metallicity
[M/H]=-0.45 for the cluster.
Liu et al. (1994)
reported an infrared Colour-Magnitude Diagram (CMD)
and derived
E(B-V)=1.8, a metallicity
and a distance from the Sun
kpc. More recently, by means of near-infrared integrated
spectroscopy,
Bica et al. (1998)
derived
E(B-V)=1.60 and
, and pointed out that Terzan 9 was one of the clusters
requiring deep photometry for more conclusive results, since bulge contamination might
be occurring in the integrated light.
Figure 3a shows the V vs. (V-I) CMD
for a pixel (
) extraction centered
on the cluster. The main features are a blue
disk main sequence (MS), and a red sequence corresponding
to the cluster plus bulge giants.
The best extraction for Terzan 9 is shown in Fig. 3b
corresponding to a radial extraction of 85 pixels (33)
centered on the cluster.
A vertical giant branch and a blue HB are present.
This CMD is very similar to that of Terzan 4 (Ortolani
et al. 1997a), an equally central cluster in the Galaxy
with blue HB. Overimposed on the Terzan 9 CMD is
the mean locus of M 30
(
,
Zinn 1985).
The mean locus of NGC 6752
(
,
Zinn 1985)
could be considered an acceptable fit, but not as good
as with M 30.
The mean loci of M 30 and NGC 6752 are from
Rosino et al. (1997).
Like in the case of Terzan 4, Terzan 9 is probably as
metal-poor as M 30.
Previous integrated methods where metallicities of
or higher were obtained, were
certainly contaminated by metal-rich
bulge field stars.
We show in Fig. 4 a pixel extraction
(
) corresponding to a field CMD located
at
east of the cluster (see Fig. 1a).
Besides the blue disk MS, the red HB of the bulge population
is clearly seen at
and
. The cluster RGB seen in Fig. 3a
corresponds to an underpopulated zone in Fig. 4.
On the other hand the bulge late type giants are seen as a curved
RGB extending to very red colours, similar to metal-rich globular clusters
such as NGC 6553 and NGC 6528,
as well as the Baade Window (Ortolani et al. 1995
and references therein). This extension is less clear in
the cluster field (Fig. 3a) because of a smaller area,
crowding in the cluster area, and possibly a higher extinction.
The brightest part of the
blue HB of Terzan 9 is located at .
We calculate the cluster reddening taking M 30 as reference.
By matching the overall sequences (Fig. 3b) we obtain
. Adopting
E(V-I)/E(B-V)=1.32 (Dean et al. 1978), this corresponds
to
, and assuming
E(B-V)=0.06 for M 30 (Barbuy et al. 1998a and references therein),
we get E(B-V)=1.95, which corresponds to
AV=6.24 (R=AV/E(B-V)=3.2).
Adopting an absolute magnitude of the HB for Terzan 9 like that of M 30,
MV=0.66
(Barbuy et al. 1998a and references therein),
we get the absolute distance
modulus . This corresponds to a
distance of
kpc for Terzan 9.
To derive the Galactocentric coordinates of the cluster,
we assume a distance of the
Sun to the Galactic center of kpc
(Reid 1993),
to be consistent with Barbuy et al. (1998a) - notice
however that Reid (1998), taking into account Hipparcos
data, pointed out that
could be as large
as 9.3 kpc. Terzan 9 galactocentric coordinates
are
X=-3.11
(X<0 refers to our side of the Galaxy),
Y=0.31 kpc and Z=-0.17 kpc.
The distance to the Galactic center is 3.13 kpc,
wherefrom we conclude that Terzan 9 is located
within the bulge.
We can calculate parameters for the offset field metal-rich bulge population and
compare it with those of the metal-poor cluster. The bulge red HB is located at
and
.
Using the metal-rich
template cluster NGC 6553 as reference
(Guarnieri et al. 1998) we get
, corresponding to
. Assuming
E(B-V)=0.73 for NGC 6553
(Barbuy et al. 1998a)
we derive
E(B-V)=1.79 for the field of Terzan 9, which corresponds to
AV=5.73 (R=3.2).
For this low Galactic latitude field
(
,
) the extinction is much higher than that
of the Baade Window
(Terndrup 1988).
Assuming MV=0.95 for a metal-rich HB
(Barbuy et al. 1998a), the distance
of the bulk of the population for this bulge field results to be 7.0 kpc.
However as pointed out by
Barbuy et al. (1998a and references therein) the total-to-selective
absorption ratio should increase with the metallicity
and a more appropriate value could be R=3.47 for this high metallicity field,
resulting in a distance of
kpc.
Considering that the distance to the Galactic center is of about 8-9 kpc
(Reid 1993, 1998), the possible interpretation is that we are observing
a relatively less reddened, foreground part of the bulge, where Terzan 9 would also
be embedded (Sect. 3.2).
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