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Table 3

Results from the Gaussian fits of the emission lines of 13CO and C18O towards the 12 positions where they are detected.

Pos. 13CO (1−0) 13CO (2−1) C18O (1−0) C18O (2−1)
v0 W Tpeak Δv v0 W Tpeak Δv v0 W Tpeak Δv v0 W Tpeak Δv

First dominant velocity component
N1 20.7 17.4 5.3 3.1 20.5 15.1 4.1 3.5 20.9 2.7 1.0 2.4 21.1 1.5 0.8 1.9
N5 20.6 15.7 5.0 3.0 20.5 15.0 4.7 3.0 20.8 2.8 1.3 2.1 20.7 2.6 1.0 2.4
N6 21.2 23.9 7.4 3.0 21.1 24.2 7.0 3.3 21.2 5.5 2.0 2.5 21.1 6.2 2.3 2.5
N2 21.1 59.6 12.6 4.5 21.5 57.4 9.6 5.6 21.1 14.7 4.5 3.0 21.0 25.0 7.9 3.0
N7 22.5 15.3 5.8 2.5 22.4 13.9 4.8 2.7 22.3 3.6 1.7 1.9 22.3 3.4 1.5 2.1
N8 18.4 15.4 4.0 3.6 18.2 9.7 2.5 3.6 18.6 2.4 1.3 1.7 18.6 1.3 0.9 1.4
N3 16.8 17.3 4.4 3.7 16.6 11.6 2.8 3.9 16.8 5.3 1.9 2.6 16.7 4.6 1.9 2.3
N4 18.9 15.2 4.9 2.9 19.0 11.3 3.3 3.2 18.9 2.2 1.5 1.4 18.8 1.4 1.6 0.8
SE1 15.0 34.3 9.9 3.3 15.1 39.7 8.7 4.3 15.3 6.7 2.1 3.0 15.0 7.5 3.0 2.4
SE2 16.3 5.8 2.0 2.7 16.3 5.6 1.6 3.2 16.9 0.8 0.3 2.5 16.9 0.6 0.3 1.9
SW2 9.6 10.5 7.0 1.4 9.5 13.2 7.4 1.7 9.7 1.3 1.1 1.1 9.7 2.2 1.8 1.2
SW4 8.9 14.7 4.7 3.0 7.8 18.6 6.4 2.7 7.5 3.4 2.4 1.4 7.6 4.6 3.1 1.4

Second dominant velocity component
N1 11.7 5.6 1.5 3.6 11.8 5.7 2.2 2.5 11.9 0.3 0.2 1.8 11.9 0.5 0.2 2.1
N5 10.4 8.0 2.3 3.3 10.4 7.3 2.1 3.3 10.4 0.6 0.2 3.2 10.1 0.8 0.3 3.0
N6 9.0 8.3 3.7 2.1 9.0 8.1 3.9 2.0 9.0 0.6 0.4 1.5 9.0 1.0 0.7 1.4
N7 18.6 10.0 3.9 2.4 18.3 9.1 3.2 2.7 18.7 1.8 1.0 1.8 18.6 1.6 0.8 1.9
N8 22.3 4.5 2.2 1.9 21.3 3.0 1.6 1.8 22.3 0.9 0.3 2.3 22.1 0.8 0.2 3.3
N4 16.0 12.4 4.5 2.6 15.8 8.3 3.4 2.3 16.3 2.3 0.8 2.6 16.1 1.5 0.5 2.5
SE1 17.3 10.4 4.6 2.1 17.2 1.9 2.6 0.7 17.0 1.6 1.9 0.8 17.0 3.0 4.3 0.7
SE2 18.6 4.3 2.2 1.9 18.8 3.0 1.9 1.5 18.5 0.3 0.2 1.5 18.8 0.4 0.3 1.1
SW2 7.6 9.1 5.3 1.6 7.5 8.0 6.2 1.2 7.6 0.6 0.4 1.3 7.5 1.0 1.0 0.9
SW4 7.3 11.8 6.9 1.6 10.4 12.7 7.9 1.5 10.5 2.5 1.9 1.2

Notes. The fit parameters are: the centre line velocity v0 (in km s-1, in the local standard of rest), the integrated intensity W (in K km s-1), the peak temperature Tpeak (in K), and the full width at half maximum Δv (in km s-1). In case of non-detections, upper limits are given at the 1σ level. Uncertainties are dominated by calibration (~20%). Integrated intensities and peak temperatures are given on the main-beam temperature scale.

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