Table A.1
Line intensities integrated with a linear baseline fit outside the line, except for 110 − 101 where the frequency switch observing mode leads to optical standing waves that had to be corrected by a fouth order polynom.
Transition | Pol. | HPBW (a) | ηmb (a) | RA−Dec (b) | ΔVint (c) | ∫ TmbdV | ΔVLine (d) | Ω (e) | Cal. (f) | ||
---|---|---|---|---|---|---|---|---|---|---|---|
(″) | (″) | (km s−1) | (K km s−1) | (km s−1) | (%) | ||||||
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110−101-a | H | 37.15 | 0.622 ± 0.07 | 1.6 | 4.8 | [6.7–14.5] | 21.02 ± 0.22 | 4.3 ± 0.3 | 0.74 ± 0.11 | 5.8 |
V | 37.49 | 0.616 ± 0.07 | −0.2 | −1.6 | [6.7–14.5] | 22.58 ± 0.23 | 4.6 ± 0.3 | 0.79 ± 0.10 | 5.8 | ||
110−101-b | H | 37.15 | 0.622 ± 0.07 | 0.9 | 3.4 | [6.7–14.5] | 20.37 ± 0.24 | 4.6 ± 0.5 | 0.75 ± 0.11 | 5.3 | |
V | 37.49 | 0.616 ± 0.07 | −2.7 | −2.2 | [6.7–14.5] | 20.56 ± 0.25 | 4.3 ± 0.8 | 0.80 ± 0.09 | 5.3 | ||
111−000 | H | 18.88 | 0.632 ± 0.08 | −1.0 | 1.5 | [6.7–14.5] | 9.63 ± 0.44 | 4.4 ± 0.8 | 0.78 ± 0.09 | 5.4 | |
V | 18.71 | 0.636 ± 0.08 | 2.2 | 0.0 | [6.7–14.5] | 10.93 ± 0.45 | 4.3 ± 0.5 | 0.85 ± 0.05 | 5.8 | ||
212−101-a | H | 12.58 | 0.593 ± 0.07 | 0.2 | 0.8 | [7.2–14.0] | 10.41 ± 0.46 | 5.2 ± 0.4 | 0.78 ± 0.07 | 7.1 | |
V | 12.41 | 0.572 ± 0.07 | 0.4 | 0.1 | [7.2–14.0] | 10.10 ± 0.47 | 4.9 ± 1.1 | 0.82 ± 0.07 | 6.9 | ||
212−101-b | H | 12.58 | 0.593 ± 0.07 | −1.9 | −0.3 | [7.2–14.0] | 6.76 ± 1.33 | 4.9 ± 1.4 | 0.80 ± 0.06 | 5.1 | |
V | 12.41 | 0.572 ± 0.07 | −2.0 | 0.5 | [7.2–14.0] | 8.38 ± 1.77 | 4.0 ± 0.3 | 0.76 ± 0.08 | 4.8 | ||
202−111 | H | 21.28 | 0.634 ± 0.08 | −1.2 | 2.0 | [7.7–13.5] | 6.47 ± 0.28 | 2.9 ± 0.8 | 0.78 ± 0.09 | 5.4 | |
V | 21.09 | 0.637 ± 0.08 | 1.8 | 0.1 | [7.7–13.5] | 9.64 ± 0.38 | 3.0 ± 0.8 | 0.84 ± 0.06 | 5.7 | ||
211−202 | H | 28.00 | 0.640 ± 0.09 | −0.4 | 3.0 | [8.2–13.0] | 6.51 ± 0.26 | 2.6 ± 0.6 | 0.77 ± 0.11 | 5.5 | |
V | 27.91 | 0.659 ± 0.09 | 0.9 | −1.3 | [8.2–13.0] | 9.13 ± 0.22 | 2.4 ± 0.4 | 0.82 ± 0.08 | 5.7 | ||
221−212 | H | 12.65 | 0.579 ± 0.07 | 0.2 | 10.8 | [8.2–13.0] | 2.04 ± 0.45 | 1.4 ± 1.0 | 0.78 ± 0.07 | 7.1 | |
V | 12.48 | 0.572 ± 0.07 | 0.4 | 0.1 | [8.2–13.0] | 3.20 ± 0.55 | 2.4 ± 0.5 | 0.82 ± 0.07 | 6.9 | ||
312−303 | H | 19.16 | 0.632 ± 0.08 | −1.0 | 1.5 | [9.2–12.0] | 1.43 ± 0.24 | 2.1 ± 0.6 | 0.78 ± 0.09 | 5.4 | |
V | 18.98 | 0.636 ± 0.08 | 2.2 | 0.0 | [9.2–12.0] | 2.27 ± 0.23 | 1.9 ± 0.6 | 0.85 ± 0.05 | 5.8 | ||
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110−101 | H | 37.77 | 0.622 ± 0.07 | −0.7 | −1.5 | [8.2–13.0] | 0.31 ± 0.02 | 1.9 ± 0.5 | 0.79 ± 0.10 | 5.2 |
V | 38.12 | 0.616 ± 0.07 | 1.9 | 4.6 | [8.2–13.0] | 0.26 ± 0.01 | 1.9 ± 0.3 | 0.74 ± 0.11 | 5.3 | ||
111−000 | H | 19.08 | 0.632 ± 0.08 | −1.0 | 1.5 | [8.2–13.0] | 0.43 ± 0.30 | 0.78 ± 0.09 | 5.4 | ||
V | 18.91 | 0.636 ± 0.08 | 2.2 | 0.0 | [8.2–13.0] | 0.25 ± 0.30 | 0.85 ± 0.05 | 5.8 |
Notes. See Table 1 for the definition of a and b labeled transitions. (a) Half-power beam width and main-beam efficiency of the Herschel telescope at the water line frequency (Mueller et al. 2014). (b) Right ascension and declination offsets from the CO+ peak (α2000 = 05h35m20.61s, δ2000 = −05°25′14.0′′). (c) Integration velocity range. (d) Observed full width at half maximum of the lines. (e)Beam coupling factor. (f)Absolute calibration uncertainty.
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