Given the low galactic latitude of IC 2602 (b=-4.9) it is to be expected that the stars selected using theoretical isochrones will be contaminated to a large extent by background stars. In order to gauge the scale of this contamination a similar selection process was applied to the photometry of the "offset'' field. The selection process yielded 43 "primary candidate members'' with V<18.5.
It should be noted that in using the offset field to gauge the background contamination we are assuming that the distribution of stars in it is representative of the background stars to be found in the cluster fields. This comparison suggests that nearly all of the stars selected are background stars. However, see the discussion in Sect. 6.2 (click here) for further comments on the location of the offset field.
In their study of IC 2602 using the ROSAT X-ray satellite,
Randich et al (1995)
detected 110 X-ray sources in an area,
68 of which they identify with at least one
optical counterpart. 4 of these X-ray sources lie in our field IC 2602a:
R64, R69, R76, R80.
No detected X-ray sources lie in our second cluster field. One X-ray source,
R25, lies in our offset field. Randich et al. identify 7 stars as
possible optical counterparts to these X-ray sources (6 in field
IC 2602a, 1 in our offset field) based on photometrically selected cluster
members and additional bright stars located close to the X-ray
position.
Table 4 (click here) shows the results of our photometry for the stars which Randich et al. indicate as optical counterparts. Photometry for the X-ray selected stars is taken from Prosser et al. (1996) where available. The X-ray source R80 is clearly identified with the bright star HD 308016 whose magnitude of V=10.66 places it beyond the bright limit of our photometry.
ID | V | V-R | V-I | Memb. |
R25 | 16.38 | -- | 2.75 | Y |
of-6078 | 16.15 | 1.00 | 2.67 | Y |
R64 | 16.53 | -- | 2.51 | Y? |
F41 | 16.66 | 0.93 | 2.62 | Y |
R69A | 18.0 | -- | 5.40 | ? |
f1-514 | 16.71 | 2.08 | 5.12 | N |
R69B | 14.12 | -- | 2.36 | N |
f1-10 | 14.20 | 1.11 | 2.42 | N |
R69C | 17.07 | -- | 2.87 | Y |
f1-738 | 17.16 | 1.04 | 2.94 | Y? |
R76 | 16.81 | -- | 2.97 | Y? |
F71 | 16.81 | 1.07 | 2.88 | Y |
Comparing the remaining 6 stars, there are differences in both the V
magnitude and the V-I colours
between the two sets of photometry somewhat larger than the errors in
Table 2 (click here).
Given that Randich et al.'s objects are active stars, however, they are
quite likely to be variable. van Leeuwen et al. (1987)
have found variable stars in the Pleiades with amplitudes of up to . Walter et al. (1992) have recorded
variability on a naked T-Tauri star of amplitude
,
. Thus a part of the discrepancy at least
might be reasonably attributed to such variability.
Since the majority of Randich et al.'s
photometry is unpublished we are unable to make a more
detailed comparison between the photometric datasets at this point.
The positions of the detected X-ray sources in the region of IC 2602 are shown in Fig. 7 (click here). The figure also shows the positions of our observed fields. It should be noted that there are no X-ray sources in the the field IC 2602b and that there are relatively few in the region surrounding it. This lack of X-ray sources is consistent with the lack of primary candidate members found from the photometry of that field. It should also be noted that the offset field contains one X-ray source, R25. Both our photometry and that of Randich et al. indicated that this star is a probable cluster member. If this star is a true cluster member then the offset field may be positioned too close to the cluster to give an accurate indication of the background contamination. If this is the case then we are over-estimating the level of background contamination as the "primary candidate members'' will contain real cluster members as well as background stars which lie in the appropriate areas of the colour-magnitude diagrams.
Figure 7: The region of IC 2602 showing X-ray sources corresponding to
photometric cluster members (filled circles) and non-members (open
circles) from Randich et al. (1995)
The Pleiades, by virtue of its proximity, is one of the most extensively
studied young (age Myr)
open clusters. Hambly & Jameson (1991) have studied
its mass-distribution and luminosity function. We may use their
results to independently examine the effects of
background contamination on our data.
By taking the star numbers for the inner radius of the
Pleiades as an approximate model for our region of IC 2602, and scaling to
allow for the different distance moduli and angular extents of the two
clusters, we should see roughly 22 cluster members in our cluster fields.
Insofar as this comparison is valid, this suggests that the level
of contamination is less than that suggested by the number of "primary
candidate members'' located in the offset field, assuming that the two
clusters have similar star densities and mass functions. We have made no
allowances for the differences in "richness'' between the two
clusters.
In summary, the evidence suggests that the level of contamination due to background stars lies somewhere between 50%, as suggested by Pleiades mass functions, and 73% as suggested by comparing the "offset'' field with field IC 2602a, although it is likely to be well below the latter figure, given that the "offset'' field appears to be located within the cluster. Such levels of contamination might well be expected given the location of the cluster, and the broad selection limits used.
In Fig. 8 (click here), which shows the distribution of primary candidate members with V magnitude, several features are apparent. Firstly, for 12<V<14 there is a clear excess of cluster members in field IC 2602a in comparison with cluster field IC 2602b and the offset field. This excess is not apparent in the range 14<V<16 where an effectively similar number of primary candidate members was selected in each cluster field. A larger number of stars were selected in the offset field in this magnitude range. In each colour-manitude diagram there is an obvious field-giant branch with 1.4<V-I<1.9. This may be a cause of contamination in the candidate list for V<14.5, but a reason why this should be worse in the offset field in comparison with the other two fields is unclear. There is a sharp falloff in stars in all fields in the range 16<V<19. Because of the likely high level of field contamination, further dicussion of the cluster luminosity function is not appropriate at this time.
Figure 8: The distribution of primary candidate members in IC 2602a (
solid line), IC 2602b (dashed line) and the offset field (dotted
line) with magnitude
Given
that the filter had a passband of 70 Å, that the equivalent
width of
in an active late-M dwarf is
Å and that the
equivalent width in absorption for an inactive M dwarf is
Å, we
would expect a
magnitude difference between active and inactive
stars of
mag, assuming that cluster late-type stars are
similar to solar neighbourhood M dwarfs.
This magnitude difference is comparable to both the scatter in the plot and
the errors in
.
Thus, we were unable to make any further selection on the basis of the
magnitudes.
We were able to determine magnitudes for 20 of the 45
photometrically selected stars in cluster field IC 2602a (the rest being too
bright). 13 of the 20 stars lie to the
bright side of
the mean
level, 7 of these more than
from the
mean level (
Å). Of the stars that lie below the mean,
none are more than
from the mean.
Similarly, for cluster field IC 2602b we have determined
magnitudes for 18 of the 33 primary candidate members. The scatter in the
data is much larger (
Å), and so only two stars lie more
than
from the mean, both in emission. The
data for the primary candidate members are shown in Table 5 (click here).
ID | R | R-![]() | ![]() | ID | R | R-![]() |
![]() |
F1 | 14.55 | -6.79 | -0.36 | F36 | 14.78 | -6.13 | 2.92 |
F2 | 14.22 | -6.74 | 2.92 | F38 | 14.47 | -6.24 | -4.11 |
F4 | 14.34 | -6.82 | -2.26 | F41 | 15.73 | -5.83 | 25.25 |
F6 | 13.70 | -6.87 | -3.50 | F42 | 17.01 | -5.92 | 19.30 |
F7 | 14.25 | -6.81 | -1.63 | F46 | 16.12 | -5.88 | 20.96 |
F8 | 17.02 | -6.85 | -7.65 | F49 | 14.46 | -6.23 | -3.50 |
F9 | 14.88 | -6.72 | 3.60 | F53 | 14.79 | -6.16 | 0.93 |
F10 | 14.55 | -6.80 | -1.00 | F54 | 16.92 | -5.91 | 20.13 |
F13 | 14.49 | -6.80 | -1.00 | F57 | 16.89 | -5.98 | 14.50 |
F14 | 13.80 | -6.87 | -3.50 | F59 | 14.17 | -6.18 | -0.36 |
F16 | 14.95 | -6.74 | 2.92 | F60 | 15.09 | -6.10 | 4.28 |
F18 | 14.27 | -6.65 | 9.22 | F61 | 16.88 | -5.79 | 28.82 |
F19 | 16.48 | -6.40 | 24.37 | F62 | 15.00 | -6.18 | -0.36 |
F20 | 14.41 | -6.59 | 13.72 | F64 | 14.53 | -6.19 | -1.00 |
F22 | 13.97 | -6.68 | 9.22 | F66 | 14.45 | -6.22 | -2.88 |
F24 | 14.14 | -6.81 | -1.63 | F67 | 14.09 | -6.15 | 2.25 |
F30 | 14.04 | -6.78 | 2.25 | F69 | 14.67 | -6.16 | 0.93 |
F32 | 14.23 | -6.66 | 8.50 | F70 | 14.06 | -6.12 | 4.28 |
F34 | 13.58 | -6.24 | -3.50 | F71 | 15.74 | -5.84 | 24.37 |
For field IC 2602a the data reinforces the likelyhood of a
significant fraction of the photometrically selected star being true cluster
members; 35% of those stars with
magnitudes being well in emission.
For field IC 2602b the results are also consistent with the reduced number
of photometrically selected stars, and the lack of any X-ray detections in
that field.