Issue |
A&A
Volume 423, Number 2, August IV 2004
|
|
---|---|---|
Page(s) | 579 - 592 | |
Section | Interstellar and circumstellar matter | |
DOI | https://doi.org/10.1051/0004-6361:20041063 | |
Published online | 06 August 2004 |
Origin of diffuse C II 158 micron and Si II 35 micron emission in the Carina nebula *,**
1
Department of Astronomy, Graduate School of Science, University of Tokyo, Tokyo 113-0033, Japan e-mail: onaka@astron.s.u-tokyo.ac.jp
2
Division of Particle and Astrophysical Science, Graduate School of Science, Nagoya University, Nagoya 464-8602, Japan
3
Institute of Advanced Research (IAR), Nagoya University, Nagoya 464-8602, Japan
Received:
26
August
2003
Accepted:
11
May
2004
We present the results of mapping observations with ISO of
[] 63 μm, 145 μm, [
] 122 μm,
[
] 158 μm, [
] 35 μm, and
H2 9.66 μm line emissions for
the Carina nebula, an active star-forming region in the Galactic plane.
The observations were made for the central
area
of the
nebula, including the optically bright
region and molecular
cloud lying in front of the ionized gas.
Around the center of the observed area is the interface between the
region and the molecular cloud which creates a typical
photodissociation region (PDR).
The [
] 158 μm emission shows a good correlation with the
[
] 63 μm emission and peaks around the
-molecular region interface. The correlated component has the
ratio of [
] 158 μm to [
] 63 μm of about 2.8.
We estimate from the correlation that about 80% of [
]
emission comes from the PDR in the Carina nebula.
The photoelectric heating efficiency estimated from the ratio of the
([
] 158 μm + [
] 63 μm) intensity to the total
far-infrared intensity ranges from 0.06 to 1.2%.
[
] 145 μm is detected marginally at 10 positions.
The average ratio of [
] 145 μm to [
] 63 μm
of these positions is about
and is larger than model
predictions.
The observed [
] 158 μm to [
] 63 μm ratio
indicates a relatively low temperature (<500 K) of the gas, while the large
[
] 145 μm to 63 μm ratio suggests a high temperature
(~
K).
This discrepancy cannot be accounted for consistently by the latest
PDR model with the efficient photoelectric
heating via polycyclic aromatic hydrocarbons (PAHs)
even if absorption
of [
] 63 μm by foreground cold gas is taken into
account. We suggest that absorption of [
] 158 μm
together with [
] 63 μm by overlapping PDRs, in which
the heating via PAHs is suppressed due to the charge-up effect, may resolve the
discrepancy.
Quite strong [
] 35 μm emission has been detected
over the observed area.
It shows a good correlation with [
] 122 μm, but the
correlation with [
] 63 μm is very weak, indicating that
[
] 35 μm comes mainly from the diffuse ionized gas
rather than the PDR.
The ratio of [
] 35 μm to [
] 122 μm is about 8 and Si of
about 50% of the solar abundance relative to N should be present in the gas phase.
The present results suggest that efficient dust
destruction takes place and a large fraction of Si returns to the gas
in the Carina star-forming region.
Key words: infrared: ISM / ISM: abundances / ISM: individual objects: Carina nebula / ISM: lines and bands / ISM: dust, extinction
© ESO, 2004
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