SIMBAD references

We present a possible interpretation for the increase of the angular diameter of the Mira variables {omi} Cet, R Leo, and χ Cyg from the K band to the 11µm region revealed by the recent interferometric observations using narrow bandpasses where no salient spectral feature is present (Weiner et al., 2003ApJ...588.1064W and 2003ApJ...589..976W). A simple two-layer model consisting of hot and cool H₂O layers for the warm water vapor envelope, whose presence in Mira variables was revealed by previous spectroscopic observations, can reproduce the angular diameters observed with Infrared Spatial Interferometer as well as the high-resolution TEXES spectra obtained in the 11µm region. The warm water vapor layers are optically thick in the lines, and therefore, strong absorption due to H₂O can be expected from such a dense water vapor envelope. However, the absorption lines are filled in by emission from the extended part of the envelope, and this results in the high-resolution 11µm spectra which exhibit only weak, fine spectral features, masking the spectroscopic evidences of the dense, warm water vapor envelope. On the other hand, the presence of the warm water vapor envelope manifests itself as the larger angular diameters in the 11µm region as compared to those measured in the near-infrared. Furthermore, comparison of the visibilities predicted in the near-infrared (1.5-3.8µm) with observational results available in the literature demonstrates that our two-layer model for the warm water vapor envelope can also reproduce the observed near-infrared visibilities and angular diameters, and suggests that the wavelength dependence of the angular size of Mira variables in the infrared largely reflects the H₂O opacity. The radii of the hot H₂O layers in the three Mira variables are derived to be 1.5-1.7 R_* with temperatures of 1800-2000K and H₂O column densities of (1-5)x10²¹cm^–2, while the radii of the cool H₂O layers are derived to be 2.2-2.5R_* with temperatures of 1200-1400K and H₂O column densities of (1-7)x10²¹cm^–2.