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Table 3.

FIR fine-structure emission line properties.

Line fobs ffit Lobs Lfit FWHM Beam PA S/N r.m.s.
[mJy
[Jy km s−1] [Jy km s−1] [109L] [109L] [km s−1] [″] [°] beam−1]
[OI]63 μm 20.6 ± 2.9 20.8 ± 4.4 32.4 ± 4.6 32.7 ± 6.9 679 ± 111 0.395 × 0.328 83.0 7.4 4.04
[OIII]88 μm < 1.38 < 1.61 0.363 × 0.309 88.7 1.96( * )
[NII]122 μm 6.27 ± 0.89 5.73 ± 1.26 5.12 ± 0.73 4.68 ± 1.03 801 ± 121 0.521 × 0.380 62.2 6.7 1.10
[OI]145 μm 5.07 ± 0.44 6.64 ± 1.33 3.47 ± 0.30 4.54 ± 0.91 677 ± 117 0.410 × 0.330 –83.6 11.6 1.47
[CII]158 μm 10.5 ± 0.4 11.1 ± 0.5 6.60 ± 0.26 6.98 ± 0.34 590 ± 23 0.385 × 0.355 48.5 26.3 0.58
[NII]205 μm 0.68 ± 0.08 0.70 ± 0.14 0.33 ± 0.04 0.34 ± 0.07 894 ± 140 0.517 × 0.440 –80.5 7.2 0.12
[CI]370 μm 0.41 ± 0.15 0.45 ± 0.22 0.11 ± 0.04 0.12 ± 0.06 368 ± 128 0.422 × 0.290 –49.8 3.3 0.20
[CI]609 μm < 0.08 < 0.01 0.365 × 0.315 –48.4 0.16( * )

Notes. Columns correspond to the line, flux and luminosity of both the data and the Gaussian fit, full width at half maximum (FWHM) of the Gaussian fit, size, and angle of the beam, signal-to-noise ratio (S/N) of the line, and depth (root mean square; r.m.s.) per channel. The channel width for all but [OIII]88 μm and [CI]609 μm FIR lines is 50 km s−1 while the channel width for those two lines (denoted by *) is 100 km s−1, in order to enhance the S/N and possible detection of the lines. The upper limits correspond to the integrated luminosity of a Gaussian assuming a FWHM of 600 km s−1 and a peak of 1σ detection.

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