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Table 1

Parameters for the observed HDO, H2O, O, and HD18O lines1.

Species Frequency J Ka,Kc Eup/k A ij Telescope Beam F eff B eff rms2 FWHM Ref.3
(GHz) (K) (s-1) size (″) (mK) (K km s-1) (km s-1)

HDO 481.7795 31,2−31,3 168 4.74  ×  10-5 HIFI 1a 44.0 0.96 0.76 15  ≤ 0.12 a
HDO 490.5966 20,2−11,1 66 5.25  ×  10-4 HIFI 1a 43.9 0.96 0.76 9 0.60 4.9 a
HDO 509.2924 11,0−10,1 47 2.32  ×  10-3 HIFI 1a 42.3 0.96 0.76 9 1.08 5.8 a
HDO 599.9267 21,1−20,2 95 3.45  ×  10-3 HIFI 1b 35.9 0.96 0.75 9 0.83 4.9 a
HDO 753.4112 31,2−30,3 168 5.90  ×  10-3 HIFI 2b 28.6 0.96 0.75 22 0.27 4.3 a
HDO 848.9618 21,2−11,1 84 9.27  ×  10-4 HIFI 3a 25.4 0.96 0.75 20 0.54 5.3 a
HDO 893.6387 11,1−00,0 43 8.35  ×  10-3 HIFI 3b 24.1 0.96 0.74 18 0.40 5.2 a
HDO 919.3109 20,2−10,1 66 1.56  ×  10-3 HIFI 3b 23.4 0.96 0.74 25 0.93 5.8 a
HDO 995.4115 30,3−21,2 131 7.04  ×  10-3 HIFI 4a 21.7 0.96 0.74 32 1.10 7.0 a
HDO 1009.9447 21,1−11,0 95 1.56  ×  10-3 HIFI 4a 21.0 0.96 0.74 29 0.38 6.5 a
HDO 1507.2610 31,2−21,1 168 6.58  ×  10-3 HIFI 6a 14.1 0.96 0.72 257  ≤ 2.04 a
HDO 1625.4081 31,3−20,2 144 4.49  ×  10-2 HIFI 6b 13.0 0.96 0.71 238  ≤ 1.89 a

HDO 80.5783 11,0−11,1 47 1.32  ×  10-6 IRAM-30 m 31.2 0.95 0.78 14 0.54 6.0 b,d
HDO 225.8967 31,2−22,1 168 1.32  ×  10-5 IRAM-30 m 11.1 0.91 0.54 34 2.15 7.4 b,d
HDO 241.5616 21,1−21,2 95 1.19  ×  10-5 IRAM-30 m 10.4 0.91 0.51 23 2.27 6.8 b
HDO 464.9245 10,1−00,0 22 1.69  ×  10-4 JCMT 10.8 0.55 63 5.50 5.9 c

p-H2O 745.3202 21,1−20,2 136 6.83  ×  10-3 HIFI 2b 28.4 0.96 0.75 18 0.34 5.2 a
p-H2O 970.2720 42,2−33,1 452 6.71  ×  10-4 HIFI 4a 21.9 0.96 0.74 31  ≤ 0.23 a
p-H2O 994.6751 20,2−11,1 101 6.02  ×  10-3 HIFI 4a 21.3 0.96 0.74 35 0.81 7.0 a
p-H2O 1101.6983 11,1−00,0 53 1.79  ×  10-2 HIFI 4b 19.2 0.96 0.74 44 0.63 5.3 a
p-H2O 1188.8631 42,2 − 41,3 452 2.73  ×  10-2 HIFI 5a 17.8 0.96 0.64 125  ≤ 0.92 a
p-O 1199.0056 22,0−21,1 194 1.76  ×  10-2 HIFI 5a 17.7 0.96 0.64 90  ≤ 0.66 a
p-O 1605.9625 41,3 − 40,4 395 3.71  ×  10-2 HIFI 6b 13.2 0.96 0.71 339  ≤ 2.49 a

o-O 489.0543 42,3−33,0 4304 6.89  ×  10-5 HIFI 1a 43.4 0.96 0.76 14  ≤ 0.10 a
o-O 547.6764 11,0−10,1 604 3.29  ×  10-3 HIFI 1a 38.7 0.96 0.75 8 0.98 7.0 a
o-O 1095.6274 31,2−30,3 2494 1.62  ×  10-2 HIFI 4b 19.4 0.96 0.74 49 0.38 3.0 a
o-O 1136.7036 32,1−31,2 3034 2.15  ×  10-2 HIFI 5a 18.7 0.96 0.64 103  ≤ 0.76 a
o-O 1181.3940 31,2−22,1 2494 2.89  ×  10-3 HIFI 5a 17.9 0.96 0.64 108  ≤ 0.79 a
o-O 1633.4836 22,1−21,2 1924 2.91  ×  10-2 HIFI 6b 13.0 0.96 0.71 264  ≤ 1.94 a
o-O 1655.8676 21,2−10,1 1144 5.46  ×  10-2 HIFI 6b 12.8 0.96 0.71 226  ≤1.66 a
o-O 1719.2502 30,3−21,2 1964 5.12  ×  10-2 HIFI 7a 12.3 0.96 0.71 277  ≤2.04 a

p-O 1107.1669 11,1−00,0 53 1.81  ×  10-2 HIFI 4b 19.1 0.96 0.74 47  ≤0.34 a
o-O 552.0210 11,0−10,1 614 3.37  ×  10-3 HIFI 1a 38.4 0.96 0.75 11 0.58 7.1 a

HD18O 883.1894 11,1−00,0 42 7.96  ×  10-3 HIFI 3b 24.0 0.96 0.75 22  ≤ 0.16 a

Notes. 

(1)

The frequencies, the upper state energies (Eup), and the Einstein coefficients (Aij) of HDO and O come from the spectroscopic catalog JPL (Pickett et al. 1998). The ortho/para separation of O was carried out in the CASSIS database.

(2)

The rms is computed for a spectral resolution of 0.7 km s-1 for the HDO transitions and 0.6 km s-1 for the O, O, and HD18O transitions.

(3)

References: a) this work; b) Caux et al. (2011); c) Stark et al. (2004); d) Parise et al. (2005).

(4)

The o-O and o-O upper energy levels quoted in the table assume that the fundamental 11,0−10,1 level lies at 34 K and not at 0 K.

(5)

This value corresponds to the ratio between the beam efficiency and the forward efficiency.

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