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Table A.1

Summary of the ATLASGAL sources used to compute the o-H2D+ detection limits.

ATLASGAL-ID Tdust N(H2) rms noise (a) N(o-H2 D+) (b) X(o-H2D+) (b) Class
(K) log10(cm−2) (K) log10(cm−2) log10(N[o-H2D+]/N[H2])
G30.85-0.08 (c) 16.7 22.72 0.07 <12.77 <−9.95 ± 0.14 70w
G320.88-0.40 (c) 16.8 22.69 0.09 <12.86 <−9.83 ± 0.13 70w
G337.28+0.01 (c) 10.7 22.92 0.09 <13.07 <−9.86 ± 0.12 70w
G338.07+0.01 (c) 18.5 22.51 0.07 <12.75 <−9.76 ± 0.15 70w
G338.78+0.48 (c) 12.2 22.85 0.07 <12.90 <−9.95 ± 0.13 70w
G351.13+0.77 (c) 18.6 22.49 0.06 <12.69 <−9.80 ± 0.14 70w
G351.57+0.76 (c) 17.0 22.67 0.03 <12.40 <−10.27 ± 0.14 70w
G353.42-0.08 (c) 17.1 22.38 0.04 <12.49 <−9.89 ± 0.14 70w

G08.68-0.37 (c) 24.2 22.94 0.07 <12.67 <−10.27 ± 0.16 IRw
G10.45-0.02 (c) 20.7 22.70 0.05 <12.58 <−10.12 ± 0.15 IRw
G18.73-0.23 (c) 21.9 22.90 0.06 <12.66 <−10.24 ± 0.15 IRw
G18.89-0.47 (c) 14.4 23.17 0.02 <12.25 <−10.92 ± 0.13 IRw
G23.21-0.38 (c) 22.1 23.20 0.03 <12.36 <−10.84 ± 0.15 IRw
G24.63+0.17 (c) 18.1 22.57 0.06 <12.71 <−9.86 ± 0.14 IRw
G317.87-0.15 (c) 19.3 23.03 0.06 <12.68 <−10.35 ± 0.14 IRw
G318.78-0.14 (c) 24.9 22.60 0.07 <12.68 <−9.92 ± 0.15 IRw
G331.71+0.60 (c) 21.0 22.88 0.05 <12.56 <−10.32 ± 0.15 IRw
G335.79+0.17 (c) 24.7 23.18 0.06 <12.61 <−10.57 ± 0.16 IRw
G337.26-0.10 (c) 21.7 22.72 0.06 <12.62 <−10.10 ± 0.16 IRw
G338.92+0.56 (c) 24.2 23.48 0.07 <12.68 <−10.80 ± 0.16 IRw
G340.78-0.10 (c) 26.2 22.82 0.08 <12.70 <−10.12 ± 0.16 IRw
G342.48+0.18 (c) 23.6 22.82 0.05 <12.50 <−10.32 ± 0.16 IRw
G343.75-0.16 (c) 24.3 23.30 0.06 <12.57 <−10.73 ± 0.16 IRw
G351.45+0.66 (c) 21.4 23.88 0.03 <12.34 <−11.54 ± 0.16 IRw

G19.88-0.54 (c) 24.2 23.12 0.03 <12.30 <−10.82 ± 0.16 IRb
G34.41+0.23 (c) 26.1 23.25 0.05 <12.50 <−10.75 ± 0.16 IRb
G37.55+0.20 (c) 28.4 22.73 0.05 <12.50 <−10.23 ± 0.16 IRb
G53.14+0.07 (c) 25.4 22.90 0.04 <12.42 <−10.48 ± 0.16 IRb
G332.09-0.42 (c) 30.8 22.94 0.05 <12.46 <−10.48 ± 0.16 IRb
G333.31+0.11 (c) 25.9 22.76 0.04 <12.44 <−10.32 ± 0.16 IRb
G341.22-0.21 (c) 27.0 22.86 0.06 <12.55 <−10.31 ± 0.16 IRb
G351.16+0.70 (c) 21.9 23.67 0.06 <12.62 <−11.05 ± 0.15 IRb
G351.25+0.67 (c) 32.5 23.34 0.06 <12.56 <−10.78 ± 0.16 IRb

G10.62-0.38 (c) 34.5 23.57 0.08 <12.67 <−10.90 ± 0.17 HII
G12.81-0.20 (c) 35.1 23.56 0.07 <12.60 <−10.96 ± 0.17 HII
G14.33-0.64 (d) 21.6 23.51 0.06 <12.65 <−10.86 ± 0.15 HII
G31.41+0.31 (c) 26.3 23.57 0.06 <12.62 <−10.95 ± 0.16 HII
G34.26+0.15 (c) 31.0 23.85 0.07 <12.66 <−11.19 ± 0.16 HII
G34.40+0.23 (c) 22.8 23.11 0.06 <12.63 <−10.48 ± 0.15 HII
G330.95-0.18 (c) 33.0 23.76 0.04 <12.37 <−11.39 ± 0.16 HII
G333.13-0.43 (c) 35.2 23.40 0.05 <12.50 <−10.90 ± 0.16 HII
G333.28-0.39 (c) 30.4 23.24 0.05 <12.51 <−10.73 ± 0.16 HII
G333.60-0.21 (c) 41.1 23.49 0.07 <12.60 <−10.89 ± 0.17 HII
G337.40-0.40 (c) 31.8 23.36 0.07 <12.70 <−10.65 ± 0.16 HII
G337.70-0.02 (c) 25.6 23.35 0.08 <12.66 <−10.70 ± 0.16 HII
G343.13-0.06 (c) 30.9 23.39 0.05 <12.48 <−10.91 ± 0.16 HII

Notes. Derived physical properties of the sample of massive clumps used to derive the o-H2 D+ detection limits described in Sect. 4.1. The sources are separated, from top to bottom, into their evolutionary classes. The error associated with N(H2) is 20% for each source. (a)The temperatures are reported on the main-beam temperature scale; (b) derived in this work. (c) Tdust, N(H2), and Class from Giannetti et al. (2017). (d) Tdust, N(H2), and Class from Urquhart et al. (2018).

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