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Table 5

Molecular column densities and fractional abundances.

Source N(o − H2D+) x(o − H2D+) N(C17O) x(C17O) N(N2H+) x(N2H+) N(N2D+) x(N2D+)
[1012 cm−2] [10−11] [1014 cm−2] [10−8] [1013 cm−2] [10−10] [1012 cm−2] [10−10]
IRAS 05399-0121 <1.4 <2.3 10.8 ± 1.1 2.7 ± 0.4 5.5 ± 0.8 10.7 ± 2.0 4.7 ± 0.3 1.1 ± 0.1
SMM 1 4.8 ± 0.8 11.5 ± 2.3 17.8 ± 1.0 7.4 ± 0.9 0.8 ± 0.1 3.1 ± 0.6 3.8 ± 0.4 1.6 ± 0.2
SMM 3 6.4 ± 1.0 5.9 ± 1.1 4.0 ± 0.6(a) 0.5 ± 0.1(a) 1.9 ± 0.2 1.6 ± 0.3 2.3 ± 0.5 0.3 ± 0.1
IRAS 05405-0117 <1.5 <9.7 3.2 ± 0.3 1.0 ± 0.2 0.5 ± 0.1 3.6 ± 0.6 0.3 ± 0.2 0.2 ± 0.1
SMM 6 (b) 8.4 ± 0.7 30.2 ± 5.6 2.0 ± 0.3 0.9 ± 0.2 0.6 ± 0.1 2.4 ± 0.4 3.1 ± 0.1 1.3 ± 0.2
3.0 ± 0.2 1.3 ± 0.2 1.0 ± 0.1 3.8 ± 0.7 3.5 ± 0.6 1.5 ± 0.3
SMM 7 4.8 ± 1.4 11.5 ± 3.7 16.0 ± 1.4 5.9 ± 0.9 2.2 ± 0.9 6.8 ± 2.9 <3.9(c) <1.5

Notes. (a) The column density and fractional abundance of the C18O isotopologue derived from observations towards the Spitzer 24 μm peak position (2.′′2 offset from the SABOCA peak) are (7.8 ± 1.0) × 1014 cm−2 and (9.6 ± 1.6) × 10−9, respectively (Miettinen 2016). (b) The values on the first row for SMM 6 refer to the SABOCA 350 μm peak position (Miettinen & Offner 2013b; their source SMM 6a), while those on the second row were derived towards our earlier target position (Miettinen et al. 2012).(c)The N2D+(3−2) line was not detected towards SMM 7 (Miettinen et al. 2012), and hence we estimated the column density upper limit from the 3σ line intensity upper limit and the N2H+(3−2) linewidth divided by the average Δv(N2H+(3−2))∕Δv(N2D+(3−2)) ratio (= 1.26) in our sample. All the quoted upper limits take the uncertainties into account.

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