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A&A 386, 1074-1102 (2002)
DOI: 10.1051/0004-6361:20020362
CO and H
O vibrational emission toward Orion Peak 1 and Peak 2
E. González-Alfonso1, 2, C. M. Wright3, 4, J. Cernicharo1, D. Rosenthal5, A. M. S. Boonman3 and E. F. van Dishoeck3
1 CSIC, IEM, Dpto. Física Molecular, Serrano 123, 28006 Madrid, Spain
2 Universidad de Alcalá de Henares, Departamento de Física, Campus Universitario, 28871 Alcalá de Henares, Madrid, Spain
3 Leiden Observatory, PO Box 9513, 2300 RA Leiden, The Netherlands
4 School of Physics, University College, Australian Defence Force Academy, University of New South Wales, Canberra ACT 2600, Australia
5 Max-Planck-Institut für Extraterrestrische Physik, Giessenbachstrasse, 85741 Garching, Germany
(Received 4 December 2001 / Accepted 4 March 2002)
Abstract
ISO/SWS observations of Orion Peak 1 and Peak 2 show strong emission in the
ro-vibrational lines of CO
v=1-0 at 4.45-4.95
m and of H
2O
at 6.3-7.0
m. Toward Peak 1 the total flux in both
bands is, assuming isotropic emission,
2.4 and
0.53 ,
respectively. This corresponds to
14 and
3% of the
total luminosity in the same beam. Two temperature components are
found to contribute to the CO emission from Peak 1/2: a
warm component, with
-400 K, and a hot component with
K. At Peak 2 the CO flux from the
warm component is similar to that observed at Peak 1, but the hot
component is a factor of
2 weaker.
The band is
25% stronger toward Peak 2,
and seems to arise only in the warm component.
The
P-branch emission of both bands from the warm component is
significantly stronger than the
R-branch, indicating that the
line emission is optically thick.
Neither thermal collisions with nor with H I seem capable of explaining
the strong emission from the warm component. Although the emission arises
in the postshock gas, radiation from the most prominent mid-infrared
sources in Orion BN/KL is most likely pumping the excited vibrational
states of CO and . CO column densities along the line of sight
of
-
are required to explain the band shape,
the flux, and the , and beam-filling is invoked to reconcile this high
N(CO) with the upper limit inferred from the emission. CO is
more abundant than by a factor of at least 2. The density of the
warm component is estimated from the emission to be
~
.
The CO emission from the hot component is neither satisfactorily explained
in terms of non-thermal (streaming) collisions, nor by
resonant scattering. Vibrational excitation through collisions with for
densities of ~
or, alternatively, with atomic hydrogen,
with a density of at least
107 cm3, are invoked to explain
simultaneously the emission from the hot component and that from the high
excitation lines in the same beam.
A jump shock is most probably responsible for this emission.
The emission from the warm component could in principle be explained
in terms of a
C-shock. The underabundance of relative
to CO could be the consequence of photodissociation, but may also
indicate some contribution from a jump shock to the CO warm emission.
Key words: shock waves -- ISM: abundances -- ISM: individual objects: Orion
Offprint request: E. González-Alfonso, gonzalez@isis.iem.csic.es
SIMBAD Objects
© ESO 2002
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