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Figure 1:
Short-exposure image of the MWC 297 signal on the AMBER
detector. X-axis corresponds to the spatial extension of the beams
and Y-axis to the wavelength. First column (Dk) corresponds to
the dark, the second (P1) and third (P2) ones are the beams from
the first and second telescope resp., and finally the last column
(IF) shows the fringes obtained by superposition of the two beams.
The bright row is the
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Figure 2:
Spectral dependence of the visibility as measured with
AMBER for MWC 297 around the
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Figure 3:
Comparison of
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Figure 4: Sketch of the model including an optically thick disk and an outflowing wind (edge-on view). The receding part of the wind is only partly visible because of the screen made by the optically thick disk. |
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Figure 5: Result from the optically thick disk model. Left panel: observed and modeled SED for MWC 297. The full dots are the continuum measurements taken from Pezzuto et al. (1997), also included are the ISO SWS/LWS spectra. Dotted line is the star, dashed line the accretion disk, and the full line the resulting total flux of the model. Right panel: resulting best-fit model radial squared visibilities compared with continuum squared visibilities observed with AMBER, IOTA and PTI. Full line and IOTA data are in the H-band, dashed line and AMBER/PTI are in the K-band. PTI values are upper limits. |
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Figure 6:
Double peaked
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Figure 7: The visibility observed with AMBER (points with error bars) and the one obtained from the outflowing wind model (full line). |
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Figure 8:
Edge-on intensity maps of the wind in the computed
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Figure 9: Continuum H-band squared visibilities obtained with the disk model compared to the IOTA visibilities observed during the transit of the object over the sky with the IOTA S15N35 baseline. |
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Figure 10:
Pole-on intensity maps of the wind
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