next up previous
Next: About this document Up: Quiescent accretion disc Previous: Quiescent accretion disc

Research program

In collaboration with NASA/GSFC and the University of St Andrews, this research combines three disciplines.

Ground- and space-based observation: Quiescent accretion discs are hosted by white dwarf accretors in cataclysmic variables and black hole accretors in X-ray transients. We will acquire spectroscopic data of accretion discs with high time- and velocity-resolution over several energy bands, employing HST to detect the inner disc regions in the UV, and ground-based optical and IR instruments to detect the outer disc; e.g. the 4.2-m William Herschell Telescope on La Palma, the 3.9-m Anglo Australian Telescope in New South Wales and the 3.8-m UK IR Telescope on Hawaii. Several useful data sets from each of these instruments already exist.

Indirect accretion disc imaging: The accretion disc targets are too small to resolve directly, therefore we intend to use maximum entropy tomography techniques to spatially resolve disc spectra. We will construct maps of discs in velocity coordinates from orbital line profile variations and transform these to spatial coordinates by assuming a velocity field (Marsh & Horne 1988). Disc eclipses by the companion star will provide spectrally-resolved spatial maps more directly (Horne 1985). The advantage of the resolution provided by these techniques is that we can discriminate between contributions from the disc, stellar components and localized shocked material forming spots or waves. This fulfills one of the original scientific goals of disc tomography.

Disc atmosphere models: The discipline of disc atmosphere building has now reached a sophistication with which the physical state of discs can be realistically modelled. Our models can include the effects of external irradiation, vertical gravity gradients, finite optical depths, energy dissipation, turbulence and supersonic velocity gradients. Our current code has been used with notable success in probing the structure of absorption curtains in accretion discs and to investigate optically thick, steady-state atmospheres (Horne et al. 1994). A successful fit to synthetic data is provided in Fig. 3.

 


Figure 3: A synthetic optical disc spectrum in green constructed using atmosphere models and treated with noise. The black line is a fit. The three panels on the left present the run of (= 8000 K), (= 0.1g cm) and (= 100) as a function of R in green, and power-law fits in black. Consequently, even face-on accretion disc spectra yield potentially enough information to determine the radial runs of fundamental physical properties. From Still, Horne & Hubeny (1998).

References:
Horne K., 1985, MNRAS, 213, 129
Horne K., Marsh T.R., Cheng F.H., Hubeny I., Lanz T., 1994, ApJ, 426, 294
Marsh T.R., Horne K., 1988, MNRAS, 235, 269
Shakura N.I., Sunyaev R.A., 1973, A&A, 24, 337
Still M.D., Horne K., Hubeny I., 1998, in S.S. Holt, T. Kallman, eds., Proc. of the 8th Astrophysics Conference in Maryland, AIP
Wijers R., Pringle, J., 1998, MNRAS, in press.



next up previous
Next: About this document Up: Quiescent accretion disc Previous: Quiescent accretion disc


Martin Still (still@chunky.gsfc.nasa.gov)              Last modified: Thu May 13 13:53:56 EDT 1999