At the present time 27 strong Class I methanol masers with a flux
50 Jy at 44 GHz are known. It is possible to observe 14 of them at
Onsala. Some well known masers were left out of our survey, such as Ori KL,
OMC-2, and DR21(OH), but some were included for comparison. Of the
remaining 11, only 7 were observed, because of weather conditions. The other
19 Class I methanol masers of our list have a lower flux at 44 GHz. We will
call a CS line with an integrated intensity > 10 K km s-1, i.e.
200 Jy km s-1, "strong''. Of 7 strong Class I methanol
masers (S235B, G30.80-0.10, W51 e1/e2, W75N, DR21-West, W33-Met,
L379IRS3) only one (G30.80-0.10) has a weak CS line (integrated intensity
less than 10 K km s-1). The others are stronger.
Class II methanol masers, on average, are more powerful than Class I methanol masers. Twenty-seven Class II methanol masers, detected by Menten (1991), have a flux higher than 100 Jy. It is possible to observe 21 sources of this list at Onsala. Eleven sources were observed in our survey and 6 out of them (S231, S252, G9.62+0.19, W33B, W51, W75 N) exhibit a strong CS line.
All observational data were reduced with the CLASS software package (Groupe
d'Astrophysique de Grenoble). The results of the
observations are presented in Table 1. Columns 1, 2, and 3 give the source
name, R.A. and Dec., respectively; Col. 4 gives the number of components
and type of lines (components of the C34S line are marked by a star),
and Cols. 5-8 give the Gaussian fitting parameters. In the last column
the sources are marked BO - bipolar outflow, MMI - Class I methanol
maser, MMII - Class II methanol maser. The list of sources with negative
results (emission with 0.03 K) is presented in Table 2. For
the positive results the CS(2-1) line was detected in 93% of the bipolar
outflows, in 100% of the Class I methanol masers and in 96% of the
Class II methanol masers. All sources observed in the C34S line
gave a positive result.
Spectra of sources detected in the CS line only are shown in Fig. i, and spectra of sources detected in both the CS and C34S lines are shown in Fig. ii (these figures are shown in the online version of the paper only).
A complex line shape was observed in 40% of the sources - one can approximate it as a sum of two Gaussians, a strong narrow and weak broader line. In these cases the parameters of both lines are given in Table 1. The shape of the lines is often asymmetrical and looks like a right or a left wing of the central component.
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