1999
DOI: 10.1086/312280
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CO Depletion in the Starless Cloud Core L1544

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Cited by 492 publications
(590 citation statements)
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References 27 publications
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“…This case is extremely unlikely as it requires typical densities of ∼10 6 cm −3 over a size of 20 (3200 AU). The depletion factor would also be a factor of ∼2 smaller if the central temperature is taken to be 11 K instead of 7.5 K. These results considerably extend the previous works on depletion in pre-stellar cores by Kramer et al (1999), Caselli et al (1999) and more recently by Tafalla et al (2002). The latter report similar depletion factors for L1544 and 4 other pre-stellar cores in the Taurus molecular cloud.…”
Section: Discussionsupporting
confidence: 85%
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“…This case is extremely unlikely as it requires typical densities of ∼10 6 cm −3 over a size of 20 (3200 AU). The depletion factor would also be a factor of ∼2 smaller if the central temperature is taken to be 11 K instead of 7.5 K. These results considerably extend the previous works on depletion in pre-stellar cores by Kramer et al (1999), Caselli et al (1999) and more recently by Tafalla et al (2002). The latter report similar depletion factors for L1544 and 4 other pre-stellar cores in the Taurus molecular cloud.…”
Section: Discussionsupporting
confidence: 85%
“…modified thermal balance or contraction by ambipolar diffusion induced by a decreased abundance of the molecule. CO depletion in dense cores has already been discussed by Kramer et al (1999), Willacy et al (1998), and Caselli et al (1999, 2002a, 2002b who focussed on L1544, a core similar to the ones we discuss in this work. Here, we studied the distribution and abundance of CO via its rarer isotopes C 17 O(1-0) and C 18 O(1-0), and of N 2 H + (1-0) in a sample of pre-stellar cores, using the 1.3 mm continuum as a tracer of the H 2 column density.…”
Section: Introductionsupporting
confidence: 79%
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“…Such a structure in the low-mass protostars has already been inferred for several molecules like CO and H 2 CO Jørgensen et al 2004Jørgensen et al , 2005. The raising of the abundance in the outermost regions of the envelope is explained by a longer depletion timescale than the lifetime of the protostars (∼10 4 −10 5 years) for H 2 densities lower than ∼10 4 −10 5 cm −3 (e.g., Caselli et al 1999;Jørgensen et al 2004). On the other hand, Hollenbach et al (2009) have shown that, at the edge of molecular clouds, the icy mantles are photodesorbed by the UV photons, giving rise to an extended layer with a higher water abundance for a visual extinction A V ∼ 1-4 mag (for G 0 = 1).…”
Section: Determination Of the Hdo Abundancementioning
confidence: 55%
“…In undepleted gas, reaction (9) represents a minor loss for H + 3 , however, as other species begin to freeze onto grain surfaces, reaction with HD becomes the dominant loss mechanism for H + 3 . As this produces H 2 D + , the This theoretical expectation, first predicted by Brown & Millar (1989), has recently been confirmed observationally by the detection of large [DCO + ]/[HCO + ] ratios in L1544 in clumps in which CO is significantly depleted (Caselli et al 1999). It may also prove important in explaining the large molecular D/H ratios observed towards IRAS 16293 and L134N.…”
Section: The Chemical Modelsmentioning
confidence: 70%