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Table 5

Fractional abundances.

Source XSiO XH13CO +  XHN13C XHNCO XCS XH13CN NH2 Chemistry References
(×10-9) (×1022 cm-2)

SW CND 1.3 0.4 0.12 1.0 10 ... 1.5 PDR + Shock
20 GMC 2.4 0.25 1.3 19 10 ... 2.5 Shock

Galactic sources
Orion Bar { (20′′, −20′′) 0.03 0.05 .../0.014  ≤ 0.015 23 .../0.07 6.5 } PDR } 1, 2
(60′′, −60′′) ... .../0.08 .../0.08  ≤ 0.3 5 .../0.04 0.3
IC 443−G 0.8  ≤ 0.1/0.05 .../0.015 ... 3 .../0.12 1.2 Shock 3
Orion KL−Plateau 22 ... ... 7 11 ... 21 Shock } 4, 5, 6
Orion KL−Hot Core 3 ... ... 14 50 ... 42 Hot Core
TMC−1  ≤ 6  ×  10-4 0.18 0.20 1.5 4 0.17 1 Ion-molecule 7

Extragalactic sources
NGC 253 0.13 0.04 0.025 1.6 6 0.13 6.7 SB 8
NGC 4945  ≤ 0.13 0.10 0.3 4 4 0.20 6.4 AGN + SB ring 8, 9
M 82 { Southwest  ≤ 0.12 0.12 ...  ≤ 9 2.3 ... 3.8 } Evolved SB } 8, 10, 11
Center ... .../0.06  ≤ 0.3/0.04  ≤ 9 7  ≤ 0.24/0.09 3.8
Northeast ... ... ...  ≤ 0.12 4 ... 2.4
IC 342 { Center ... .../0.04 .../0.06 3 4 .../0.14 1.3 Normal−nucleus
North  ≤ 0.9 0.4 ... 5 6  ≤ 1.1 1.1 Normal−arm
IC 342 { A 0.16 0.12 .../0.08  ≤ 4 .../(30–80) .../0.22 2.3 Normal−nucleus } 12, 13, 14
D 0.4 0.06 .../0.04 5 .../ ≤ (8–23) .../0.14 1.7 } Normal−arm
(interf.) D′ ... ... .../0.03 8 .../ ≤ (6–16) ... 2.0

References. (1) Jansen et al. (1995); (2) Schilke et al. (2001); (3) van Dishoeck et al. (1993); (4) Marcelino et al. (2009); (5) Tercero et al. (2010); (6) Tercero et al. (in prep.); (7) Marcelino (2007); (8) Martín et al. (2006); (9) Wang et al. (2004); (10) Martín et al. (2009a); (11) Bayet et al. (2009); (12) Downes et al. (1992); (13) Meier & Turner (2005); (14) Usero et al. (2006).

Notes. Galactic sources: The second value of the H13CO+, HN13C, and H13CN abundances has been derived from the main isotope assuming a 12C/13C isotopic ratio of 65 for the Orion Bar and the SNR IC 443−G. Extragalactic sources: a source size of 20′′ (Martín et al. 2006; Wang et al. 2004) has been assumed in our column density estimations of M 82 and IC 342 from single-dish observations, as well as optically thin emission and the LTE approximation. For that purpose, integrated intensities have been taken from the compilation made by Martín et al. (2006) plus additional data taken from Martín et al. (2009a) and Bayet et al. (2009). The second values of the H13CO+, HN13C, and H13CN abundances have been derived from the main isotopes assuming 12C/13C  ≃  40 (Henkel et al. 1998). Interferometric IC 342 abundances have been derived from the parameters of the line profiles taken from Usero et al. (2006), Meier & Turner (2005), and Downes et al. (1992), assuming a source size of 6′′, optically thin emission, and the LTE approximation. CS abundance has been derived from C34S assuming 32S/34S  ~  8−23 (Meier & Turner 2005).

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