1983
DOI: 10.1086/160619
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Dense cores in dark clouds. I - CO observations and column densities of high-extinction regions

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Cited by 227 publications
(165 citation statements)
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“…Rieke & Lebofsky (1985) derive A V = Si % 17 for grains in the interstellar medium. This would indicate A V ¼ 10 30 for the present Class I objects, to compare with the general extinction determined toward Taurus association stars of A V ¼ 1 5 and the total extinction through the densest Taurus molecular-cloud cores of A V ¼ 2 20 ( Myers et al 1983). Only one of our targets ( IRAS 04108+2803B) lies near a cloud core ( L1495) dense enough that its silicate feature could be explained by a location on the far side and absorption by the intervening cloud; even if this were the case, the 15.2 m CO 2 ice feature would still be unusually strong.…”
Section: Analysis and Conclusionmentioning
confidence: 63%
“…Rieke & Lebofsky (1985) derive A V = Si % 17 for grains in the interstellar medium. This would indicate A V ¼ 10 30 for the present Class I objects, to compare with the general extinction determined toward Taurus association stars of A V ¼ 1 5 and the total extinction through the densest Taurus molecular-cloud cores of A V ¼ 2 20 ( Myers et al 1983). Only one of our targets ( IRAS 04108+2803B) lies near a cloud core ( L1495) dense enough that its silicate feature could be explained by a location on the far side and absorption by the intervening cloud; even if this were the case, the 15.2 m CO 2 ice feature would still be unusually strong.…”
Section: Analysis and Conclusionmentioning
confidence: 63%
“…Compared to the broad, supersonic 12 CO and 13 CO line profiles, roughly equal contributions of thermal and non-thermal motions are found in the observed C 18 O linewidths in nearby clouds (Myers et al 1983;Vilas-Boas et al 1994;Onishi et al 1996). Originally thought to be restricted to cores at scales of 0.1 pc (Goodman et al 1998), constant (tran-)sonic-like C 18 O linewidths have been found to be characteristic of filaments and fibers at scales of 0.5 pc (Hacar & Tafalla 2011;Arzoumanian et al 2013;Hacar et al 2013).…”
Section: Introductionmentioning
confidence: 92%
“…Assuming similar and uniform local termodynamic equilibrium (LTE) conditions along the line of sight, the opacities of a given J transition for the different CO lines can be estimated by their relative abundances as τ(A) X(A/B) · τ(B) (e.g., Myers et al 1983). Characteristic values of τ(C 18 O) between 0.2 and 0.6 based on the study of the C 18 O (1−0) transition are found in different studies of dark clouds (Myers et al 1983;Vilas-Boas et al 1994Onishi et al 1996). Assuming typical relative abundances for the main three CO isotopologues in the local ISM (i.e., X(C 18 O):X( 13 CO):X( 12 CO) = 1:7.3:560 Wilson & Rood 1994) these opacities translate into characteristic line opacities ranging between τ( 13 CO) ∼ 1.5-4.4 and τ( 12 CO) ∼ 110-340 for the J = 1−0 transitions of the most abundant CO isotopologue (e.g., Phillips et al 1979;Wong et al 2008).…”
Section: Co Linewidths: Differential Opacity Broadeningmentioning
confidence: 99%
“…However, for several molecules with large abundances, we observe the corresponding transitions of their main and rare isotopologues, e.g., OCS (J = 19 → 18) − O 13 CS (19 → 18), 13 CO (2 → 1) − CO (2 → 1) − C 18 O (2 → 1) and CH 13 3 CN (12 2 → 11 2 )−CH 3 CN (12 2 → 11 2 ). By measuring the ratio between main beam brightness temperature of the main line T B, α,0 and its rare isotopologue T B, β,0 , we can estimate the optical depth at line centre of a given transition τ α,0 (Myers et al 1983 where α is the intrinsic abundance of the main isotope (e.g., 12 C) compared to its rare isotope (e.g., 13 C) in the ISM (Table 4, e.g., Wilson & Rood 1994;Chin et al 1996). …”
Section: Molecular Column Densitiesmentioning
confidence: 99%