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Astron. Astrophys. 327, 1023-1038 (1997) 3. The reconstruction methodThe eclipse mapping method (Horne 1985) employs the maximum
entropy fitting package MEMSYS (Skilling et al. 1984) to interprete
observed eclipse light curves in terms of intensity and brightness
temperature maps of accretion disks. A cartesian two dimensional grid,
located in the orbital plane and centered on the white dwarf undergoes
an eclipse by the secondary star to produce an artificial lightcurve,
whereby all pixels are assumed to have the same brightness at all
phases. The intensities of the pixels are adjusted until the
artificial light curve fits the observed one within a maximum allowed
The eclipse mapping method used by us is different with respect to the adopted geometry for the reconstructions. Instead of a flat grid, a three dimensional disk with a constant disk opening angle and an outward facing "ribbon" at a certain disk radius was used. Our improved method addresses two specific problems with the original eclipse mapping method. First, light curve variations due to anisotropic light sources like the so called "hump" which is caused by the hot spot where the gas stream hits the disk rim cannot be mapped due to the assumed isotropic radiation of the pixels. Second, there is only one-dimensional information available from the observed light curve for the reconstruction of the two-dimensional disk. Therefore additional constraints have to be introduced. This is done by manipulating the default image in a special manner, leading to the fact that the final result depends on the default image and the way it is created. For further details see Appendix A and B. ![]() ![]() ![]() ![]() © European Southern Observatory (ESO) 1997 Online publication: April 6, 1998 ![]() |