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Table 1.

Observed line parameters of HMgCCCN and NaCCCN towards IRC +10216.

Transition νobs(a) νobs − νcal(b) dv(c) (horn) (d) (centre) (e) Notes
Ju − Jl (MHz) (MHz) (mK km s−1) (mK) (mK)
HMgCCCN

12-11 31 672.704±0.050 0.0569 39.84 1.48 1.31 (A)
13-12 34 311.875±0.050 −0.0304 38.53 1.45 1.26
14-13 36 951.092±0.050 −0.0407 42.28 1.59 1.39
15-14 39 590.327±0.020 (B)
16-15 42 229.489±0.050 0.0040 53.36 2.06 1.72 (C)
17-16 44 868.617±0.050 0.0118 50.25 2.22 1.48
18-17 47 507.686±0.050 0.0010 72.11 3.06 2.19
19-18 50 146.722±0.040 ≤3.5, (D)

NaCCCN

12-11 31 705.51±0.20 −0.0447 13.25 0.49 0.44
13-12 34 347.56±0.30 0.0147 11.35 0.43 0.37 (E)
14-13 36 989.38±0.20 −0.1235 12.17 0.46 0.40
15-14 39 631.36±0.20 −0.0667 11.35 0.44 0.37
16-15 42 273.31±0.20 −0.0024 10.64 0.41 0.34
17-16 44 915.22±0.40 0.0619 17.38 0.77 0.51 (F)
18-17 47 556.89±0.40 −0.0709 17.67 0.75 0.54

Notes.

(a)

Observed frequency assuming a VLSR = −26.5 km s−1.

(b)

Observed minus calculated frequencies in MHz.

(c)

Integrated line intensity in mK km s−1. The total uncertainty is assumed to be dominated by the calibration uncertainties of 10%.

(d)

Antenna temperature at the terminal velocity (horn) in mK.

(e)

Antenna temperature at line centre in mK.

(A)

Line partially blended with a weak hyperfine component of CC13CH. Frequency and line parameters can be correctly estimated adopting the observed intensities of the other hyperfine components of CC13CH (see top panel of Fig. 1).

(B)

Line fully blended with C3N. Frequency and line parameters cannot be estimated. The quoted frequency corresponds to the predicted one.

(C)

Line partially blended with c − C3H2. Frequency and line parameters can still be estimated.

(D)

Line not detected. The upper limit in antenna temperature corresponds to 3σ. The quoted frequency corresponds to the predicted one.

(E)

Line partially blended with an unknown feature. Frequency and line parameters can still be estimated.

(F)

Line blended with an unknown feature and with a line from HC9N in the 3ν19 state. Frequency and line parameters are very uncertain.

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