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Table 1.

Observed line parameters of HNC5 and HC4NC.

Transition (a) νrest(b) O−C (c) T A * dv $ \int T_{\rm A}^* dv $(d) Δv(e) T A $ T_{\mathrm{A}}^{*} $(f)
(MHz) (kHz) (mK km s−1) (km s−1) (mK)
HNC5
5–4 (g) 13 617.484 ± 0.002 0.4 ... ... ...
6–5 (g) 16 340.973 ± 0.002 −1.7 ... ... ...
7–6 (g) 19 064.462 ± 0.002 1.5 ... ... ...
12–11 32 681.784 ± 0.010 −4.7 1.21 ± 0.07 0.70 ± 0.04 1.63 ± 0.10
13–12 35 405.222 ± 0.010 −6.3 1.11 ± 0.13 0.75 ± 0.10 1.38 ± 0.11
14–13 38 128.657 ± 0.010 −0.6 1.27 ± 0.09 0.91 ± 0.08 1.31 ± 0.10
15–14 40 852.084 ± 0.010 8.0 0.68 ± 0.08 0.58 ± 0.08 1.11 ± 0.12
16–15 43 575.481 ± 0.010 −1.5 0.81 ± 0.15 0.73 ± 0.19 1.05 ± 0.17
17–16 46 298.876 ± 0.018 −0.4 0.14 ± 0.08 0.34 ± 0.15 0.40 ± 0.16

HC4NC
12–11 33 628.146 ± 0.010 0.4 3.16 ± 0.12 0.74 ± 0.03 4.03 ± 0.12
13–12 36 430.451 ± 0.010 2.5 2.58 ± 0.06 0.64 ± 0.02 3.77 ± 0.08
14–13 39 232.738 ± 0.010 −3.2 2.49 ± 0.13 0.59 ± 0.03 3.96 ± 0.14
15–14 42 035.028 ± 0.010 5.1 1.79 ± 0.09 0.56 ± 0.03 2.99 ± 0.10
16–15 44 837.284 ± 0.010 −8.8 1.87 ± 0.09 0.56 ± 0.03 3.11 ± 0.13
17–16 47 639.557 ± 0.010 6.8 1.76 ± 0.17 0.75 ± 0.09 2.21 ± 0.15

Notes.

(a)

Quantum numbers are J′−J″, where J′ denotes the upper and J″ the lower level.

(b)

Frequency of the observed transitions in TMC-1 assuming a local standard of rest velocity (vLSR) of 5.83 km s−1 (Cernicharo et al. 2020).

(c)

Observed minus calculated frequencies in kHz. The calculated frequencies were obtained from a merged fit to the TMC-1 and the laboratory data (see Table 2).

(d)

Integrated line intensity in mK km s−1.

(e)

Line width at half-intensity derived by fitting a Gaussian function to the observed line profile in km s−1.

(f)

Antenna temperature in milli Kelvin.

(g)

For the laboratory transitions J′−J″ = 5−4, 6−5, and 7−6, the observed frequencies correspond to the F′−F″ hyperfine components 6−5, 7−6, and 8−7, respectively.

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