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Table 2.

Molecular transitions detected.

Molecule Resolved quantum numbers ν (GHz) Rel. Intensity
CCH N = 1 → 0 F = 2 → 1 87.317
F = 1 → 1 87.402
HCN J = 1 → 0 F = 0 → 1 88.630 0.3333
F = 2 → 1 88.632 0.5555
F = 1 → 1 88.634 0.1111
HCO+ J = 1 → 0 89.189
HNC(a) J = 1 → 0 90.664
13CO J = 1 → 0 110.201
CN N = 1→0 113.170
113.191
113.491
12CO J = 1 → 0 115.271
HCN J = 2 → 1 F = 2 → 2 177.260 0.0833
F = 1 → 0 177.260 0.1111
F = 2 → 1 177.261 0.2500
F = 3 → 2 177.261 0.4667
F = 1 → 2 177.262 0.0056
F = 1 → 1 177.263 0.0833
HCO+ J = 2 → 1 178.375
HNC J = 2 → 1 181.325
12CO J = 2 → 1 230.538
HCN J = 3 → 2 265.886
HCO+ J = 3 → 2 267.558
HNC J = 3 → 2 271.981

Notes. Line frequencies and relative intensities were measured in the laboratory and published in Müller et al. (2001) and Müller et al. (2005). Frequencies of HCN transitions (and their hyperfine components) were established by Mullins et al. (2016).

(a)

The hyperfine structure of HNC (J = 1 → 0) is unresolved in these observations.

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