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Table 2.

Observed line parameters for HC3N+.

J′−J F 1 F 1 $ F_1^\prime - F_1 $ F′−F νrest (a) (o-c) (b) T A d v $ \int T_{\rm A}^* {\rm d}v $ (c) Δv (d) T A $ T_{\rm A}^* $ (e) Notes
(MHz) (MHz) (mK km s−1) (km s−1) (mK)
7/2–5/2 4–5 3–4 31621.877 ± 0.010 0.002 1.53 ± 0.08 1.07 ± 0.07 1.33 ± 0.10
7/2–5/2 3–4 2–3 31623.173 ± 0.010 –0.000 1.05 ± 0.07 0.90 ± 0.01 1.16 ± 0.10
7/2–5/2 4–4 3–3 31626.161 ± 0.010 0.001 1.07 ± 0.13 0.75 ± 0.08 1.34 ± 0.13 A
7/2–5/2 3–3 2–2 31627.170 ± 0.010 0.005 0.91 ± 0.13 0.99 ± 0.18 0.87 ± 0.10
7/2–5/2 4–3 3–2 31629.665 ± 0.010 0.000 0.92 ± 0.13 0.92 ± 0.18 0.94 ± 0.10 B
7/2–5/2 3–2 2–1 31630.840 ± 0.020 –0.006 0.88 ± 0.13 0.95 ± 0.23 0.61 ± 0.10
9/2–7/2 5–6 4–5 C
9/2–7/2 4–5 3–4 40659.446 ± 0.010 0.002 1.37 ± 0.08 0.97 ± 0.07 1.33 ± 0.09
9/2–7/2 5–5 4–4 40660.934 ± 0.010 0.001 1.44 ± 0.08 0.81 ± 0.05 1.67 ± 0.09
9/2–7/2 4–4 3–3 40661.701 ± 0.010 0.009 1.45 ± 0.09 0.98 ± 0.07 1.39 ± 0.09
9/2–7/2 5–4 4–3 40662.912 ± 0.010 –0.004 0.92 ± 0.07 0.72 ± 0.06 1.20 ± 0.09
9/2–7/2 4–3 3–2 40663.761 ± 0.010 –0.008 0.90 ± 0.09 1.10 ± 0.09 0.76 ± 0.09
11/2–9/2 6–7 5–6 49694.811 ± 0.050 –0.049 2.41 ± 0.24 1.51 ± 0.18 1.51 ± 0.25
11/2–9/2 5–6 4–5 49695.446 ± 0.050 0.037 1.00 ± 0.19 0.69 ± 0.17 1.38 ± 0.25
11/2–9/2 6–6 5–5 49696.225 ± 0.050 –0.020 1.21 ± 0.19 0.83 ± 0.14 1.43 ± 0.25
11/2–9/2 5–5 4–4 49696.847 ± 0.050 0.008 1.65 ± 0.21 0.85 ± 0.13 1.82 ± 0.25 B
11/2–9/2 6–5 5–4 49697.548 ± 0.050 0.026 0.98 ± 0.22 1.01 ± 0.30 0.91 ± 0.25
11/2–9/2 5–4 4–3 D

Notes.

(a)

Rest frequency assuming a vLSR of 5.83 km s−1 (Cernicharo et al. 2020c).

(b)

Observed frequency minus calculated frequency from the fit.

(c)

Integrated intensity (in mK km s−1).

(d)

Line width (in km s−1).

(e)

Antenna temperature (in mK).

(A)

Data only from the set of data with frequency switching throw of 8 MHz.

(B)

Partially blended with a U feature.

(C)

The line is fully blended with a strong line of CH2CN.

(D)

Affected by a negative feature produced in the folding of the frequency switching data.

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