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Table 4

Fitresults of the 2Π1∕2 OH J = 3/2–1/2 line.

Source σrms Δv(b)
(K) (K) (K) (km s−1) (km s−1)
G10.47+0.03 5.49 0.06 1.2 ± 0.2 64.3 ± 0.4 4.3 ± 1.1
− 0.8 ± 0.1 49.5 ± 1.7 26.9 ± 3.0
G34.26+0.15(†) 8.66 0.14 1.6 ± 0.2 58.1 ± 0.3 4.2 ± 0.7
− 1.1 ± 0.3 62.5 ± 0.3 1.5 ± 0.6
G35.20−0.7 2.02 0.15 2.1 ± 0.2 34.5 ± 0.4 9.7 ± 0.9
W28A 6.80 0.11 5.7 ± 2.1 26.0 ± 6.2 34.2 ± 8.5
4.0 ± 1.5 12.4 ± 1.3 13.7 ± 5.8
W31C 8.79 0.12 3.5 ± 0.3 −3.3 ± 0.5 7.8 ± 1.0
2.0 ± 0.3 4.2 ± 1.2 14.9 ± 2.9
W33A 2.32 0.13 1.5 ± 0.1 40.7 ± 0.4 16.3 ± 1.2
W49N 12.35 0.07 4.8 ± 0.4 19.8 ± 0.4 10.2 ± 1.1
3.8 ± 0.3 6.7 ± 1.2 12.8 ± 1.2
2.9 ± 0.2 13.9 ± 3.8 68.6 ± 3.8
G327.29−0.6 5.53 0.06
G351.58−0.4 6.17 0.10 0.7 ± 0.2 − 86.0 ± 1.9 15.9 ± 3.9

Notes. (a) Main-beam brightness temperature of the single-sideband continuum at 1.838 THz (Rayleigh-Jeans scale). The velocity resolution is 0.75 km s−1. (b) The errors are constrained by the fitting procedure inCLASS. (†)The hfs fit is for the 1834.8 GHz component of the Λ-doublet from the image band.

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