Table 1

Spectral properties of the observed lines.

Species Quantum numbers Frequency s(a) Noise(b)

Simplified Complete [MHz] # [K]
12CO (1–0) J = 1 → 0 115 271.202 1 0.11
13CO (1–0) J = 1 → 0 110 201.354 1 0.04
C18O (1–0) J = 1 → 0 109 782.173 1 0.04
C17O (1–0) J = 1 → 0 112 358.982 1 0.06
H2CO (1–0) 10,1 → 00,0 72 837.948 3 0.11
HCO+ (1–0) J = 1 → 0 89 188.525 3 0.05
HC13O+ (1–0) J = 1 → 0 86 754.288 3 0.06
HCN (1–0) J = 1 → 0, F = 2 → 1 88 631.848 3 0.06
HNC (1–0) J = 1 → 0 90 663.568 3 0.06
12CN (1–0) N = 1 → 0, J = 3∕2 → 1∕2, F = 5∕2 → 3∕2 113 490.970 1 0.07
12CS (2–1) J = 2 → 1 97 980.953 1 0.04
32SO (3–2) J = 3 → 2, N = 2 → 1 99 299.870 1 0.04
CCH (1–0) N = 1 → 0, J = 3∕2 → 1∕2, F = 2 → 1 87 316.898 2 0.05
c-C3H2 (2–1) 21,2 → 10,1 85 338.890 2 0.04
N2H+ (1–0) J = 1 → 0, F1 = 2 → 1, F = 3 → 2 93 173.764 3 0.05
CH3OH (2–1) J = 2 → 1, K = 0 → 0, (A+) 96 741.375 1 0.04
SiO (2–1) J = 2 → 1 86 846.985 1 0.06
H+ 40α 40α recombination line 99 022.953 1 0.02

Notes. (a) Number of the IRAM-30 m tuning setup the line was observed with (see Sect. 2.1 for details). (b) Typical noise level in channels of 0.5 km s−1 measured on the cubes that were smoothed at an angular resolution of 40″.

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