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Table 2

HC3N 2-1 spectral measurements.

Source On-time RMS δV ΔV V0 I(HC3N) S(HC3N)
(min) (mK) (km s-1) (km s-1) (km s-1) (K km s-1) (Jy km s-1)
(1) (2) (3) (4) (5) (6) (7) (8) (9)

NGC 660 28 4.2 32.2 260.7 (90.6) 825 (36) 1.47 (0.40) 0.86 (0.24) ~0.034a
IC 342 20 6.5 20.1 52.0 (12.9) 45 (6) 0.77 (0.18) 0.45 (0.11) ~0.005b
M 66 18 7.0 20.1 44.8 (17.7) 775 (7) 0.68 (0.21) 0.4 (0.12) ~0.114c
NGC 520 14 5.7 ... ... ... <1.02 <0.6 <0.087d
NGC 891 30 2.3 ... ... ... <0.26 <0.15 <0.033e
NGC 972 33 3.8 ... ... ... <0.61 <0.36 ...
NGC 1068 25 4.0 ... ... ... <0.73 <0.43 <0.013f
UGC 2855 23 4.9 ... ... ... <0.76* <0.45 ...
UGC 2866 22 3.6 ... ... ... <0.56* <0.33 ...
NGC 1569 33 3.0 ... ... ... <0.31 <0.18 ...
NGC 2146 24 3.4 ... ... ... <0.67 <0.39 <0.021e
NGC 2403 30 3.2 ... ... ... <0.33 <0.19 ...
M 82 26 5.5 ... ... ... <0.73 <0.43 <0.011e
NGC 3079 19 5.5 ... ... ... <1.17 <0.69 <0.225e
NGC 3310 36 2.3 ... ... ... <0.29 <0.17 ...
IC 694+NGC3690 47 4.2 ... ... ... <0.72 <0.42 <0.158g
Mrk 231 44 6.4 ... ... ... <0.91 <0.54 <0.191g
Arp 220 26 4.5 ... ... ... <0.94 <0.55 <0.069h
NGC 6946 28 5.1 ... ... ... <0.64 <0.38 <0.018e

Notes. All the temperature scales are Tmb. The columns are: (1) galaxy name; (2) on-source time for each galaxy; (3) RMS noise of the smoothed spectrum; (4) velocity resolution of the smoothed spectrum; (5) line width (FWHM) of the Gaussian fit of the line (if available); (6) HC3N emission line center; (7) integrated intensity (and errors) of HC3N 21 emission. For those non-detections, 2σ upper limits are presented (see text in Sect. 3.1); (8) integrated flux density, and (9) flux density ratio between HC3N 21 and HCN 10. HCN 10 data from:

(*)

The upper limits of the two galaxies are derived assuming a 200 km s-1 line width.

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