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Table B.2

Integrated CH3 OH line intensities in units of Jy beam−1 km s−1 over each source position.

SVS 50 –40 E+ 51 –41 E 50 –40 A+ 51–41 E+ 52–42 E
SVS 4−2 0.66 ± 0.13 6.23 ± 1.24 7.98 ± 1.60 0.50 ± 0.10 0.19 ± 0.10
SVS 4−3 ... 0.69 ± 0.14 0.97 ± 0.20 ... ...
SVS 4−4 ... 1.73 ± 0.35 1.10 ± 0.22 ... ...
SVS 4–5 0.63 ± 0.13 3.82 ± 0.76 1.65 ± 0.50 0.41 ± 0.13 0.12 ± 0.05
SVS 4−6 0.50 ± 0.10 3.37 ± 0.67 3.89 ± 0.78 0.85 ± 0.17 0.92 ± 0.19
SVS 4−7 0.16 ± 0.05 2.74 ± 0.60 1.26 ± 0.45 0.43 ± 0.10 0.33 ± 0.07
SVS 4−8 ... 1.32 ± 0.26 1.32 ± 0.26 ... ...
SVS 4−9 0.30 ± 0.07 1.48 ± 0.30 1.97 ± 0.40 0.12 ± 0.04 ...
SVS 4−10 0.32 ± 0.07 1.12 ± 0.22 2.42 ± 0.48 ... ...
SVS 4−12 0.11 ± 0.04 4.29 ± 0.86 4.55 ± 0.91 0.19 ± 0.05 0.25 ± 0.07

Notes. Not provided numbers mean that the integrated intensities are below 5σ of the noise level.

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