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Table B.1

Beam coupling corrections and C2H line intensities toward the SDLS position (Fig. 1 left).

Species Frequency Telescope HPBW Icorra$I_{\text{corr}}^{a}$
[GHz] /Receiver [arcsec] fb (single-dish) fb (ALMA) fb (total) [K km s−1]
C2H N = 1–0 87.3 IRAM30m/E0 28.2 0.76 0.89 0.67 13.5
C2H N = 2–1 174.7 IRAM 30m/E1 14.1 0.93 0.89 0.83 28.4
C2H N = 3–2 262.0 IRAM 30m/E2 9.4 0.99 0.89 0.88 38.7
C2H N = 4–3 349.3 IRAM 30m/E3 8.0 1.00 0.89 0.89 37.0
C2H N = 6–5 524.0 Herschel/HIFI 40.5 0.66 0.89 0.59 13.7
C2H N = 7–6 611.3 Herschel/HIFI 34.7 0.70 0.89 0.62 8.7
C2H N = 8–7 698.5 Herschel/HIFI 30.4 0.74 0.89 0.66 4.7
C2H N = 9–8 785.8 Herschel/HIFI 27.0 0.77 0.89 0.68 3.6
C2H N = 10–9 873.1 Herschel/HIFI 24.3 0.80 0.89 0.71 3.6

Notes. In this work we correct the observed C2H line intensities obtained with the IRAM 30 m and Herschel telescopes toward the SDLS position as Icorr = Iobs/fb (total), with fb (total) = fb (single-dish) ⋅ fb (single-dish). Iobs (IRAM) are taken from Cuadrado et al. (2015). Iobs (HIFI) are taken from Table A.1 of Nagy et al. (2017). aAdding the intensities of all individual fine-structure and hyperfine-structure C2H lines.

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