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Table 2.

CO line pointed observations of the MIR-selected sample and Gaussian fits to detected lines.

ID I1−0 I2−1 V1−0 V2−1 W1−0 W2−1 P1−0 P2−1 rms1−0 rms2−1
... mK km s−1 mK km s−1 km s−1 km s−1 km s−1 km s−1 mK mK mK mK
s537 <77 <49 ... ... ... ... ... ... 4.8 3.1
s542 <93 <70 ... ... ... ... ... ... 5.8 4.3
s555 <75 <75 ... ... ... ... ... ... 4.7 4.7
s555−o1 <140 <117 ... ... ... ... ... ... 8.7 7.3
s631 <75 <43 ... ... ... ... ... ... 4.7 2.7
s672 <97 <80 ... ... ... ... ... ... 6.1 5.0
s771 <83 <83 ... ... ... ... ... ... 5.2 5.2
s787 <77 <57 ... ... ... ... ... ... 4.8 3.6
s799 408 ± 45 (467) 202 ± 19 (227) −179.1 −179.5 3.7 2.4 104 79 8.8 4.8
s854 <87 <89 ... ... ... ... ... ... 5.4 5.6
s892 150 ± 23 (149) 179 ± 11 (171) −272.4 −272.8 2.2 3.0 65 57 6.1 4.5
s892−o1 <171 <128 ... ... ... ... ... ... 10.7 8.0
s892−o2 <134 <140 ... ... ... ... ... ... 8.4 8.7
s892−o3 <158 <132 ... ... ... ... ... ... 9.9 8.3
s892−o4 <144 <146 ... ... ... ... ... ... 9.0 9.1
s892−o5 <205 <131 ... ... ... ... ... ... 12.8 8.2
s905 <101 <63 ... ... ... ... ... ... 6.3 3.9
s907 <85 <61 ... ... ... ... ... ... 5.3 3.8

Notes. The ID of the MIR source in each pointed observation is given in Col. 1. In Cols. 2 and 3 we show I, the integrated line brightness per beam of the J = 1−0 and J = 2−1 detected lines, respectively (in parentheses we add the values obtained by summing the flux in each channel) or their upper limits. In Cols. 4 and 5 we display the mean velocity V of the detected lines, in Cols. 6 and 7 we list the relative line widths W, and in Cols. 8 and 9 the peak intensity values P. In the last two columns we show the rms noise level for the CO J = 1−0 and J = 2−1 spectra smoothed at 2 km s−1 resolution.

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