A FIR luminosity limited sample of IRAS sources revealed also a spatial
dependence in the SiO detection rate. For sources with the detection rate in the galactic longitude range
is roughly twice as high as in the other two
equal intervals of longitude. About 90% of the sources in the mentioned
longitude range are located between the galactocentric radii 3 and 7 kpc.
The full widths above two sigma of the SiO lines vary from 2 to 103 km s-1 and they always have a single peak. The latter characteristic implies that bow-shocks do not provide a generally applicable model for the SiO emission regions. A better agreement with the observations is obtained by the model of turbulent wakes behind bow-shocks by Raga & Cabrit (1993), where the FWZI and the line asymmetry depends on the viewing angle. However, the number of narrow and symmetric line profiles suggests that the SiO formation also takes place in relatively quiescent gas, perhaps due to grain mantle evaporation and subsequent chemical processing aided by ionizing radiation from shocks. The higher detection rate in the inner 7 kpc of the Galaxy may be partly due to the latter processes. It is possible that in this region, where the molecular gas surface density is large and the star formation rate is high (e.g. Blitz 1997; Bronfman 1992), the dense cores are warmer and have higher column or volume densities, and thereby provide appropriate conditions for the production and excitation of SiO.
The data provide a basis for further investigation of shocks associated with massive young stars. In a subsequent paper we shall study the velocities of H2O, OH and CH3OH masers with respect to the observed SiO line profiles, utilizing the existing interferometric maps of the spatial distribution of masers and UC HII regions.
The excitation temperatures derived from the SiO data towards three sources are subthermal and do not show variation in velocity ranges of about 20 kms-1. This agrees with the results of Acord et al. (1997) towards the massive outflow source G5.89-0.39 and indicates that the determination of kinetic temperature of shocked gas is not possible with the aid of two transitions of SiO only.
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