[C II]-deficit caused by self-absorption in an ionized carbon-filled bubble in RCW79

Recent spectroscopic observations of the [C II ] 158 μm fine-structure line of ionized carbon (C + ), using the Stratospheric Observatory for Infrared Astronomy (SOFIA), have revealed expanding [C II ] shells in Galactic H II regions. We report the discovery of a bubble-shaped source (S144 in RCW79 in the GLIMPSE survey), associated with a compact H II region, excited by a single O7.5–9.5V/III star, which is consistent with a scenario that the bubble is still mostly “filled” with C + . This indicates most likely a very early evolutionary state, in which the stellar wind has not yet blown material away as it has in more evolved H II regions. Using the SimLine non-local thermodynamic equilibrium radiative transfer code, the [C II ] emission can be modeled to originate from three regions: first, a central H II region with little C + in the fully ionized phase, followed by two layers with a gas density around 2500 cm −3 of partially photodissociated gas. From these two layers, the second layer is a slowly expanding [C II ] shell with an expansion velocity of ∼2.6 km s −1 that corresponds approximately to a bright ring at 8 μm. The outermost layer exhibits a temperature and velocity gradient that produces the observed self-absorption features in the optically thick [C II ] line ( τ ∼ 4), leading to an apparent deficit in [C II ] emission and a low ratio of [C II ] to total far-infrared (FIR) emission. We developed a procedure to reconstruct the missing [C II ] flux and find a linear correlation between [C II ] and FIR without a [C II ]-deficit after incorporating the missing [C II ] flux. This example demonstrates that at least some of the [C II ]-deficit found in Galactic H II bubbles can be attributed to self-absorption, although a broader sample of these objects needs to be studied to fully constrain the range of conditions in which [C II ]-deficits can be explained by this process.

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Publication Details

Journal
Astronomy and Astrophysics
Published
2025-04-14
DOI
https://doi.org/10.1051/0004-6361/202453445
Citations
2
Primary Topic
Astrophysics and Star Formation Studies
Type
article
Field-Weighted Citation Impact
2.31

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article

[C II]-deficit caused by self-absorption in an ionized carbon-filled bubble in RCW79

L. Bonne, A. Zavagno, M. Röllig, R. Simon et al.
2 citations
Astronomy and Astrophysics
Astrophysics and Star Formation Studies
2.31
article

[C II]-deficit caused by self-absorption in an ionized carbon-filled bubble in RCW79

L. Bonne, A. Zavagno, M. Röllig, R. Simon, Dominik A. Riechers, Eduard Keilmann, P. F. Goldsmith, V. Ossenkopf-Okada, J. L. Verbena, A. G. G. M. Tielens, N. Schneider, R. Güsten, S. Kabanovic, Simon Dannhauer, J. Stutzki
article en
2 citations

Abstract

Recent spectroscopic observations of the [C II ] 158 μm fine-structure line of ionized carbon (C + ), using the Stratospheric Observatory for Infrared Astronomy (SOFIA), have revealed expanding [C II ] shells in Galactic H II regions. We report the discovery of a bubble-shaped source (S144 in RCW79 in the GLIMPSE survey), associated with a compact H II region, excited by a single O7.5–9.5V/III star, which is consistent with a scenario that the bubble is still mostly “filled” with C + . This indicates most likely a very early evolutionary state, in which the stellar wind has not yet blown material away as it has in more evolved H II regions. Using the SimLine non-local thermodynamic equilibrium radiative transfer code, the [C II ] emission can be modeled to originate from three regions: first, a central H II region with little C + in the fully ionized phase, followed by two layers with a gas density around 2500 cm −3 of partially photodissociated gas. From these two layers, the second layer is a slowly expanding [C II ] shell with an expansion velocity of ∼2.6 km s −1 that corresponds approximately to a bright ring at 8 μm. The outermost layer exhibits a temperature and velocity gradient that produces the observed self-absorption features in the optically thick [C II ] line ( τ ∼ 4), leading to an apparent deficit in [C II ] emission and a low ratio of [C II ] to total far-infrared (FIR) emission. We developed a procedure to reconstruct the missing [C II ] flux and find a linear correlation between [C II ] and FIR without a [C II ]-deficit after incorporating the missing [C II ] flux. This example demonstrates that at least some of the [C II ]-deficit found in Galactic H II bubbles can be attributed to self-absorption, although a broader sample of these objects needs to be studied to fully constrain the range of conditions in which [C II ]-deficits can be explained by this process.

Astronomy and AstrophysicsVol. 697
Ames Research Center (US), Jet Propulsion Laboratory (US), University of Cologne (DE), Institut Universitaire de France (FR), Aix-Marseille Université (FR), Medizinisch Wissenschaftliche Verlagsgesellschaft (Germany) (DE), Max Planck Institute for Radio Astronomy (DE), Leiden Observatory, University of Maryland, College Park (US)
National Aeronautics and Space Administration, California Institute of Technology, Universities Space Research Association, Deutsche Forschungsgemeinschaft, Deutsches Zentrum für Luft- und Raumfahrt, Universität Stuttgart, International Max Planck Research School for Advanced Methods in Process and Systems Engineering
Openalex Percentile: Top 12%
Astrophysics and Star Formation Studies
2.31
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