Astron. Astrophys. 358, 708-716 (2000)
5. Conclusions
We obtained a rather complete view of the infrared emission of the
Orion nebula and its interface with the adjacent molecular cloud. The
most interesting results are the observation of amorphous, and
possibly crystalline, silicates in emission over the entire
H II region and in an extended region around the
bright O9.5Vpe star Ori A. We have
fitted the mid-IR continuum of the H II region
and around Ori A with the emission
from amorphous silicate and amorphous carbon grains at the equilibrium
temperatures predicted for the grains in the given radiation field.
This shows that both types of grains can survive in the harsh
conditions of the H II region. A number of bands
(the 9.6 µm bump seen in Fig. 6; the excess
14 µm emission indicated in Figs. 4 and 10)
suggest emission from crystalline silicates (essentially forsterite)
in the H II region. Crystalline silicates may
also exist around Ori A, but further,
longer wavelength observations are required to confirm their
presence.
Do the observed crystalline silicates result from processing of
amorphous silicates in the H II region or in the
environment of Ori A? Silicate
annealing into a crystalline form requires temperatures of the order
of 1000 K for extended periods (Hallenbeck et al. 1998).
The dust temperatures observed in the H II
region and around Ori A are
considerably lower than this annealing temperature. One might however
invoke grain heating following grain-grain collisions in the shock
waves that are likely to be present in the H II
region. However, grain fragmentation rather than melting is the
more likely outcome of such collisions (Jones et al. 1996). It
is probable that the crystalline silicates observed here were already
present in the parent molecular cloud, and probably originate from
oxygen-rich red giants.
Emission by both amorphous and crystalline silicates has been
observed with ISO around evolved stars (Waters et al. 1996;
Voors et al. 1998). The crystalline silicates there must have
been produced locally by annealing of amorphous silicates. Gail &
Sedlmayr (1999) have shown that this is possible, and that both
amorphous and crystalline forms can be released into the interstellar
medium. However, there is no evidence for absorption by crystalline
silicates in the general interstellar medium in front of the deeply
embedded objects for which amorphous silicate absorption is very
strong (Demyk et al. 1999; Dartois et al. 1998).
Consequently, crystalline silicates represent only a minor fraction
compared to amorphous silicates. It would be difficult to detect the
emission from a small crystalline component of dust in the diffuse
interstellar medium because the dust is too cool
(T K) to emit strongly in the
m wavelength region. Observations of
H II regions and bright stars provide the
opportunity of observing this emission due to the strong heating of
dust. Emission from amorphous and crystalline silicates is seen around
young stars (Waelkens et al. 1996; Malfait et al. 1998) as
well as in comets (Crovisier et al. 1998). There are also
silicates in meteorites, but their origin is difficult to determine
because of secondary processing in the solar system. Crystalline
silicates in comets, and perhaps in interplanetary dust particles
believed to come from comets (Bradley et al. 1992), must be
interstellar since the material in comets never reached high
temperatures. However, the silicates probably experienced changes
during their time in the interstellar medium. It is interesting to
note that while very small grains of carbonaceous material exist,
there seem to be no very small silicate grains in the interstellar
medium (Désert et al. 1986).
© European Southern Observatory (ESO) 2000
Online publication: June 8, 2000
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