2004
DOI: 10.1051/0004-6361:20041063
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Origin of diffuse C II 158 micron and Si II 35 micron emission in the Carina nebula

Abstract: 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.

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Cited by 30 publications
(28 citation statements)
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“…We have emphasized that the chemistry of our dust models is consistent with observed abundances in the CNO-processed nebula, supported by analysis of 12 CO and 13 CO lines that indicates a subsolar abundance ratio of CO/H 2 and an enhancement of 13 C. Some caution is needed about the isotopic abundance ratio, however, since chemical fractionation of carbon driven by the reaction 13 C + + CO  12 C + + 13 CO + 34.8 K can occur in dense photodissociation regions (PDRs; Langer et al 1984;Gerin et al 1998; (Mizutani et al 2004) formed at the interface between the HII region and molecular cloud mapped out in CO (Brooks et al 1998;Zhang et al 2001; see also Cox 1995;Smith et al 2000;Brooks et al 2003, for reviews of the large-scale structure of the Carina cloud). Our PACS spectroscopy shows significant emission in the vicinity of the Homunculus, the strongest being in the direct sightline.…”
Section: The Carbon Isotope Ratio and The Question Of C + In The Homusupporting
confidence: 76%
“…We have emphasized that the chemistry of our dust models is consistent with observed abundances in the CNO-processed nebula, supported by analysis of 12 CO and 13 CO lines that indicates a subsolar abundance ratio of CO/H 2 and an enhancement of 13 C. Some caution is needed about the isotopic abundance ratio, however, since chemical fractionation of carbon driven by the reaction 13 C + + CO  12 C + + 13 CO + 34.8 K can occur in dense photodissociation regions (PDRs; Langer et al 1984;Gerin et al 1998; (Mizutani et al 2004) formed at the interface between the HII region and molecular cloud mapped out in CO (Brooks et al 1998;Zhang et al 2001; see also Cox 1995;Smith et al 2000;Brooks et al 2003, for reviews of the large-scale structure of the Carina cloud). Our PACS spectroscopy shows significant emission in the vicinity of the Homunculus, the strongest being in the direct sightline.…”
Section: The Carbon Isotope Ratio and The Question Of C + In The Homusupporting
confidence: 76%
“…Since the [C II] 158 μm/[N II] 122 μm ratio largely depends on the electron density, 16−91% of the observed [C II] intensity comes from the ionized gas for the range of n e = 16−977 cm −3 . The contribution of the ionized gas to the [C II] 158 μm emission has been investigated in some star-forming regions: 27% or 20 ± 10% in the Carina nebula (Oberst et al 2006;Mizutani et al 2004), 20−70% in S171 (Okada et al 2003), and 30−80% in the σ Sco region (Okada et al 2006). Model calculations indicate that it is at least 10% and up to 50−60% according to Abel (2006), and ∼10% for Kaufman et al (2006).…”
Section: Resultsmentioning
confidence: 99%
“…Although great strides have been made in understanding heating and cooling in nearby galaxies with the best techniques and spatial resolution available (Brauher et al 2008;Rubin et al 2009), the use of global values can make it difficult to ensure that emission averaged together arises from similar physical environments. Contursi et al (2002) noted that the integrated far-IR emission measured in global studies appears to be dictated by relatively few active regions that dominate the signal within the beam, whereas Mizutani et al (2004) showed that overlapping photodissociation regions (PDRs) within an aperture lead to discrepant far-IR diagnostics. It has also been shown that the observed [C ii] line deficit is increased if emission that does not originate from the dense gas around massive stars (e.g., non-PDR emission) is present (Luhman et al 2003).…”
Section: Heating the Ismmentioning
confidence: 99%