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This article has an erratum: [https://doi.org/10.1051/0004-6361/202245659e]


Table 1.

HNCO and SiO transitions used in this work.

Species Transition (a) Rest frequency Eu Aul gu mJy beam−1 to K (b)
[GHz] [K] [s−1]
HNCO 40,4–30,3 87.9252 10.55 9.024e−06 9 0.062
50,5–40,4 109.9057 15.82 1.803e−05 11 0.040
60,6–50,5 131.8857 22.15 3.163e−05 13 0.027
70,7–60,6 153.8651 29.54 5.078e−05 15 0.020
80,8–70,7 175.8437 37.98 7.643e−05 17 0.015
90,9–80,8 197.8215 47.47 1.095e−04 19 0.012
100,10–90,9 219.7983 58.02 1.51e−04 21 0.010
120,12–110,11 263.7486 82.28 2.631e−04 25 0.007
130,13–120,12 285.7220 95.99 3.355e−04 27 0.006
140,14–130,13 307.6939 110.76 4.201e−04 29 0.005
150,15–140,14 329.6644 126.58 5.178e−04 31 0.004

SiO 2–1 86.847 6.25 2.927e−05 5 0.063
3–2 130.269 12.50 1.058e−04 7 0.028
4–3 173.688 20.84 2.602e−04 9 0.015
5–4 217.105 31.26 5.197e−04 11 0.010
6–5 260.518 43.76 9.118e−04 13 0.007
7–6 303.927 58.35 1.464e−03 15 0.005

Notes. We use HNCO and SiO molecular data from Niedenhoff et al. (1995), Sahnoun et al. (2018), Balança et al. (2018) via the LAMDA database (Schöier et al. 2005).

(a)

The transition quantum number labeling and the rest frequency data are from the Cologne Database for Molecular Spectroscopy (CDMS) catalog https://cdms.astro.uni-koeln.de/ (Müller et al. 2001, 2005; Endres et al. 2016).

(b)

The conversion factor from [mJy beam−1] to [K] described in Sect. 3 in each transition is provided.

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