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Astron. Astrophys. 355, 979-993 (2000) 1. IntroductionInterstellar and circumstellar maser emission from the water
molecule has been detected in a large number of objects (cataloged by
Cesaroni et al. 1988; Brand et al. 1994). The most extensively studied
H2O masers are the Chapman & Cohen (1986) concluded from their study of the supergiant VX Sgr that the SiO, H2O, and OH masers form a natural sequence at increasing radii from the star. Several authors have found that, in a few objects, the H2O maser emission is consistent with the expanding shell models (Spencer et al. 1979; Lane et al. 1987 on IK Tau; Diamond et al. 1987). This was also reported by Reid & Menten (1990), who were able to detect as well the photosphere of W Hya, providing the stellar radius and, for the first time, could locate the circumstellar maser emission with respect to the central star. Nevertheless, in other objects there is evidence of non-spherical geometric distributions, where the standard expanding shell model fails to fit the H2O maser data (Johnston et al. 1985; Lane et al. 1987; Bowers et al. 1993; Bowers & Johnston 1994; Yates & Cohen 1994). Careful mapping of the position and velocity of the individual maser features is necessary to illuminate this point, and new approaches of data analysis are needed particularly for studies with instruments of moderate angular resolution like the VLA. It is also important to know whether the extent of the masing
region increases with mass-loss rate, as this is predicted by model
pumping calculations (Cooke & Elitzur 1985). Water maser regions
have been reported to show sizes in the range
Most of the mentioned studies, however cannot provide information
on the sizes of individual spots due to lack of angular resolution
(the VLA is unable to resolve the spots, as its minimum fringe spacing
is An interesting problem that remains to be solved is to establish where the H2O masers appear in the expanding circumstellar envelope. The existing data suggest that the distance from the star at which these masers arise is smaller than the distance at which dust is formed (measured by infrared interferometers, or by the thermal emission of SiO). This can be explained if the density is large enough inside the dust formation point, and it is compatible with the moderate velocities seen in these masers.
© European Southern Observatory (ESO) 2000 Online publication: March 21, 2000 ![]() |