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Table 1.

Parameters of the observations for each source.

Source Beam Noise level MRS
[FWHM and PA] [mJy/beam] [″]
GLMP 950 1 . 09 × 0 . 77 $ 1{{\overset{\prime\prime}{.}}}09 \times 0{{\overset{\prime\prime}{.}}}77 $/−6° 2.5 10.4
GLMP 953 1 . 00 × 0 . 78 $ 1{{\overset{\prime\prime}{.}}}00 \times 0{{\overset{\prime\prime}{.}}}78 $/−8° 2.5 9.8
AFGL 5385 1 . 19 × 0 . 63 $ 1{{\overset{\prime\prime}{.}}}19 \times 0{{\overset{\prime\prime}{.}}}63 $/−87° 1.9 9.8
HD 187885 0 . 93 × 0 . 78 $ 0{{\overset{\prime\prime}{.}}}93 \times 0{{\overset{\prime\prime}{.}}}78 $/−77° 1.9 8.0
Hen 3-1475 1 . 22 × 0 . 65 $ 1{{\overset{\prime\prime}{.}}}22 \times 0{{\overset{\prime\prime}{.}}}65 $/−84° 1.6 10.0
M1-92 1 . 10 × 0 . 77 $ 1{{\overset{\prime\prime}{.}}}10 \times 0{{\overset{\prime\prime}{.}}}77 $/−11° 2.2 10.3

Notes. The beam FWHM is an average value for the spectral window with lowest frequencies (between ∼219.44 GHz and ∼221.31 GHz) and the noise level in the spectral cube is given at a reference frequency of 221 GHz towards the position of the continuum peak.

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