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Table 1

Observed line parameters.

ν 0 HPBW η δv τ
Molecule Transition (GHz) (″) (km s-1) (K)

p-NH3 (1,1) 23.694506 33 0.80 0.08 6.4
(2,2) 23.722634 33 0.80 0.08 0.3
p-15NH3 (1,1) 22.624929 33 0.80 0.08 7.53 0.02
o-NH2D 11,1s − 10,1a 85.926278 29 0.80 0.14 6.4
o-15NH2D 11,1s − 10,1a 86.420128 29 0.80 0.13 5.04 0.02

N2H+ 1−0 93.173772 27 0.79 0.13 8.3
3−2 279.511858 9 0.57 0.08 5.7
N2D+ 1−0 77.109622 32 0.83 0.08 1.7
3−2 231.321857 10 0.60 0.05 2.3
15NNH+ 1−0 90.263833 28 0.80 0.13 0.03
N15NH+ 1−0 91.205741 28 0.80 0.13 0.03

HCN 1−0 88.631847 29 0.79 0.13 55.6
2−1 177.261222 14 0.69 0.07 89.7
3−2 265.886499 9 0.57 0.05 36.9
H13CN 1−0 86.340163 29 0.79 0.14 4.2
2−1 172.677956 14 0.69 0.07 3.2
3−2 259.011866 9 0.60 0.18 0.4
HC15N 1−0 86.054966 29 0.79 0.14 0.9
2−1 172.107957 14 0.69 0.07 0.6
3−2 258.156996 9 0.60 0.05 0.1
DCN 1−0 72.414933 34 0.84 0.08 3.3
2−1 144.828111 17 0.69 0.08 4.9
3−2 217.238612 11 0.64 0.05 1.4
D13CN 3−2 213.519936 12 0.66 0.11 0.8

HNC 1−0 90.663568 28 0.79 0.13 8.6
3−2 271.981142 9 0.60 0.09 11.7
HN13C 1−0 87.090850 29 0.79 0.13 0.8
2−1 174.179408 14 0.69 0.13 1.2
3−2 261.263310 9 0.60 0.05 0.3
H15NC 1−0 88.865717 28 0.79 0.13 0.2
2−1 177.729094 14 0.69 0.13 0.3
3−2 266.587800 9 0.60 0.18 0.06
DNC 2−1 152.609737 16 0.69 0.08 6.98 7.0
3−2 228.910489 11 0.66 0.05 5.06 5.0
DN13C 2−1 146.734002 17 0.69 0.16 3.96 0.4
3−2 220.097238 11 0.66 0.05 3.92 0.1

CN 1−0 113.490982 21 0.79 0.20 34.5
2−1 226.874781 11 0.66 0.11 47.6
13CN 1−0 108.780203 21 0.79 0.21 1.6
2−1 217.467150 11 0.64 0.11 0.8
C15N 1−0 110.024590 21 0.79 0.11 0.3

Notes. Summary of the nitrogen containing species observed at the IRAM telescope (except for the NH3 isotopologues that were observed at the Green Bank Telescope). The NH3 and NH2D isotopologue observations are respectively taken from Lis et al. (2010) and Gérin et al. (2009). All the observations were obtained at a single position except for N2H+J = 1 − 0 and NH2D, for which we obtained maps. For each line, we indicate the central frequency of the line (ν0) as well as the quantum numbers of the corresponding transition. The HPBW and efficiency (η) of the telescope at this frequency and the spectral resolution (δv) of the observations are also indicated. The last two columns indicate the averaged excitation temperature and the opacity of the rotational lines (summed over the hyperfine components), as derived from the results of the radiative transfer modelling. The upper/lower subscripts for indicate the highest/lowest excitation temperatures found when considering all the hyperfine components. These quantities are zero when all the hyperfine components are described by the same excitation temperature. In the case of the DNC isotopologues, we neglected the hyperfine structure and the subscripts are thus absent.

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