Free Access

Table 1

Line parameters of observed transitions.

Transition ν 0 a b E up a n crit c Telescope/Instrument
[GHz] [′′] [K] [cm-3]

12CO

J = 1 → 0 115.271 22.6 5.53 2 × 103 IRAM 30 m/EMIR
J = 2 → 1 230.538 11.3 16.60 7 × 103 IRAM 30 m/EMIR
J = 3 → 2 345.796 18.9 33.19 2 × 104 APEX/FLASH+
J = 4 → 3 461.041 14.1 55.32 4 × 104 APEX/FLASH+
J = 6 → 5 691.473 9.6 116.16 1 × 105 APEX/CHAMP+
J = 7 → 6 806.652 8.2 154.87 2 × 105 APEX/CHAMP+
J = 11 → 10 1267.014 24.2 364.97 8 × 105 SOFIA/GREAT
J = 12 → 11 1381.995 22.2 431.29 9 × 105 SOFIA/GREAT
J = 13 → 12 1496.923 20.9 503.13 1 × 106 SOFIA/GREAT
J = 16 → 15 1841.346 16.6 751.72 2 × 106 SOFIA/GREAT

13CO

J = 1 → 0 110.201 23.7 5.29 2 × 103 IRAM 30 m/EMIR
J = 2 → 1 220.399 11.8 15.87 1 × 104 IRAM 30 m/EMIR
J = 3 → 2 330.588 19.7 31.73 3 × 104 APEX/FLASH+
J = 6 → 5 661.067 10.0 111.05 3 × 105 APEX/CHAMP+
J = 13 → 12 1431.153 21.4 481.02 2 × 106 SOFIA/GREAT

HCN

J = 1 → 0 88.632 29.4 4.25 2 × 106 IRAM 30 m/EMIR
J = 3 → 2 265.886 24.9 25.52 1 × 107 APEX/HET230
J = 4 → 3 354.505 18.7 42.53 3 × 107 APEX/FLASH
J = 8 → 7 708.877 9.2 153.11 2 × 108 APEX/CHAMP+

HCN

J = 1 → 0 86.339 30.2 4.14 2 × 106 IRAM 30 m/EMIR
J = 3 → 2 259.012 25.2 24.86 5 × 107 APEX/HET230
J = 4 → 3 345.339 19.2 41.43 1 × 108 APEX/FLASH

HCO+

J = 1 → 0 89.189 29.2 4.28 2 × 105 IRAM 30 m/EMIR
J = 3 → 2 267.558 24.8 25.68 3 × 106 APEX/HET230
J = 4 → 3 356.734 18.6 42.80 6 × 106 APEX/FLASH
J = 9 → 8 802.458 8.1 192.58 9 × 107 APEX/CHAMP+

HCO+

J = 1 → 0 86.754 30.1 4.16 2 × 105 IRAM 30 m/EMIR
J = 3 → 2 260.255 25.1 24.98 3 × 106 APEX/HET230

Notes.

(a)

Rest frequencies and upper level energies are adopted from the Cologne Database for Molecular Spectroscopy (CDMS, Müller et al. 2005), and the Leiden Atomic and Molecular Database (LAMDA, Schöier et al. 2005).

(b)

Beam size (resolution) used to create the respective map. This beam is ~6% larger than the actual HPBW at the corresponding frequencies, as defined by the kernel used in the gridding algorithm of GILDAS/CLASS.

(c)

Critical densities for temperature ranges 40–300 K (12CO, 13CO) and 10–30 K (HCN, HCN, HCO+, HCO+). As the main collisional transitions for HCN occur with ΔJ = 2, the traditional two-level formula for the critical density is not appropriate here. This formula generally overestimates the critical density. This also applies to the other molecules where ΔJ = 2 transitions are at least comparable. A better estimate for the actual population of the molecule is obtained here by adding the coefficients for ΔJ = 1 and ΔJ = 2.

Current usage metrics show cumulative count of Article Views (full-text article views including HTML views, PDF and ePub downloads, according to the available data) and Abstracts Views on Vision4Press platform.

Data correspond to usage on the plateform after 2015. The current usage metrics is available 48-96 hours after online publication and is updated daily on week days.

Initial download of the metrics may take a while.