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Table 3

Best-fit parameters of the C3 models in 27 sightlines.

Sightline(a) This work(b) Literature(c)


Tlow Thigh N FWHM voff T N Source
(K) (K) (1012 cm−2) (km s−1) (km s−1) (K) (1012 cm−2)
HD 23180(d) 127.3 ± 3.9 1.27 ± 0.13 A03
HD 24398(d) 132.0 ± 10.3 1.30 ± 0.35 A03
1.00 O03
50.0 1.37 R02
1.00 M01
HD 27778 1.20 ± 0.30 O03
HD 45314
HD 61827 (Comp.1)
HD 61827 (Comp.2)
HD 63804
HD 73882(d)
HD 80558(d) 1000.0
HD 144217(d) 100.0 <0.38 G02
HD 147683
HD 147888
HD 147889 tentative detection H95
HD 147933
HD 148184 3.10 ± 0.50 G02
HD 149404 (Comp.1)
HD 149404 (Comp.2)
HD 149757 1.60 ± 0.00 O03
2.01 ± 0.20 G02
1.83 ± 0.00 R02
1.60 ± 0.00 M01
HD 152248(d)
HD 154043(d)
HD 154368
HD 161056 (Comp.1)
HD 161056 (Comp.2) 100.0
HD 169454 1000.0 22.4 ± 1.0 6.61 ± 0.19 S14
23.4 ± 1.4 2.24 ± 0.66 A03
4.30 ± 0.50 O03
HD 179406 1.30 ± 0.70 O03
2.90 R02
2.00 M01
HD 185859(d)
HD 186745
HD 186841 (Comp.1)
HD 186841 (Comp.2)
HD 203532
HD 210121 1.90 ± 0.50 O03
4.56 R02

Notes. (a)Best-fit results are listed in separate entries for sightline harbouring multiple velocity components. (b)The Gaussian broadening factor FWHM has a lower boundary of 3.00 km s−1 to reflect instrumental profile; the fitting boundaries of the excitation temperature for the higher J-levels Thigh are between 100 and 1000 K; the velocity offset voff is relative to the barycentric frame. (c)Column densities from G02 and R02 have been converted to f000 = 0.016. The excitation temperature for the lower J-levels is listed if the reference uses double-temperature model. (d)Tentative detection, no individual transition exceeds the 3σ detection limit.

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