Astron. Astrophys. 324, L5-L8 (1997)
5. Conclusion
The extinction map of the Chamaeleon I cloud has been significantly
improved for extinction greater than with
respect to previous maps obtained from star counts on Schmidt plates.
Four distinct maxima are detected and we reach 9 visual magnitudes of
extinction without degradation of the resolution. This result has been
obtained both by exploiting the massive star counts in the J
band provided by DENIS, and by applying a variant of the classical
star count method which is adapted to large variations of extinction
and a wavelet analysis of the extinction map. Moreover, DENIS give us
the opportunity to investigate the cloud at a larger scale than the
earlier investigations which were limited to small regions around the
visible reflection nebulae.
The comparison with the cold IRAS 100 is
striking. Each of the 3 most important extinction maxima corresponds
to a peak of cold IRAS emission. The IRAS flux is therefore a good
indicator of extinction. We plan further investigations of the
relation between the cold IRAS emission and extinction when new CO
observations at a comparable spatial resolution will be available.
Finally we stress the fact that our map has been derived from
J star counts converted to visual extinction with
. This value of 3.1 is the standard estimate for
diffuse interstellar medium, but it can reach 5.5 in dense molecular
cloud cores (Whittet et al., 1987). According to Cardelli et al.
(1989):
![[EQUATION]](img68.gif)
So, we obtain 0.282 for and 0.334 for
. This means that we overestimate the extinction
by a factor 1.18 if we choose rather than 5.5.
Extinction is generally expressed in visual magnitudes. This choice is
not the best because the extinction law in the visible range depends
on the composition of the medium. On the other hand, the extinction
law in the infrared seems universal. Therefore, it should be better to
refer the extinction to near infared magnitudes. Lastly, it appears
that J DENIS data with a detection limit of
magnitude are better adapted to investigate the
obscuration of regions where the extinction is larger than 4
magnitudes, rather than the Schmidt plate even at a usual detection
limit of magnitudes.
© European Southern Observatory (ESO) 1997
Online publication: May 26, 1998
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