2023ApJ...952..102G -
Astrophys. J., 952, 102 (2023/August-1)
Structure of the W3A Low-density Foreground Region.
GOLDSMITH P.F., LANGER W.D., SEO Y., PINEDA J., STUTZKI J., GUEVARA C., ALADRO R. and JUSTEN M.
Abstract (from CDS):
We present analysis of [O I] 63 μm and CO J = 5 - 4 and 8 - 7 multiposition data in the W3A region and use it to develop a model for the extended low-density foreground gas that produces absorption features in the [O I] and J = 5 - 4 CO lines. We employ the extinction to the exciting stars of the background H II region to constrain the total column density of the foreground gas. We have used the Meudon photodissociation region code to model the physical conditions and chemistry in the region employing a two-component model with a high-density layer near the H II region responsible for the fine-structure line emission and an extended low-density foreground layer. The best-fitting total proton density, constrained largely by the CO lines, is n(H) = 250 cm–3 in the foreground gas and 5 × 105 cm–3 in the material near the H II region. The absorption is distributed over the region mapped in W3A and is not restricted to the foreground of either the embedded exciting stars of the H II region or the protostar W3 IRS5. The low-density material associated with regions of massive-star formation, based on an earlier study by Goldsmith et al., is quite common, and we now see that it is extended over a significant portion of W3A. It thus should be included in modeling of fine-structure line emission, including interpreting low-velocity-resolution observations made with incoherent spectrometer systems, in order to use these lines as accurate tracers of massive-star formation.
Abstract Copyright:
© 2023. The Author(s). Published by the American Astronomical Society.
Journal keyword(s):
Star formation - Photodissociation regions - Giant molecular clouds - Submillimeter astronomy
Simbad objects:
13
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