The scattering of radiation by free electrons is one of the dominant sources of continuous opacity in the atmospheres of hot white dwarfs. Most model atmosphere calculations adopt the classical Thomson isotropic scattering approach, whereby only the direction of photon propagation changes as the result of a scattering event. More rigorously, finite electron mass instead implies that both momentum and energy exchange should actually occur.
The effects of Compton scattering on white dwarf model
atmospheres was first investigated in detail by Madej (1994), who
found that pure hydrogen models with
temperatures of
K show a significant depression of the X-ray
continuum for wavelengths
Å. Effects for models containing
significant amounts of helium, or helium and heavier elements, were
found to be much smaller or negligible, in keeping with expectations
based on the relative importance of electron scattering as an opacity
source as opposed to photoelectric absorption.
In a later paper, Madej (1998) computed the effects of Compton
scattering for a model corresponding to the parameters of the DA white
dwarf HZ 43. Differences between Compton and Thomson scattering model
spectra are apparent for
Å, and grow to orders of
magnitude by 40 Å. While current X-ray
instrumentation is not sufficiently sensitive to study the spectra of
even the brightest DA white dwarfs in any detail at wavelengths
Å, the spectral differences implied by the more
rigorous Compton redistribution formalism will be of interest to more
sensitive future missions. Moreover, the Chandra Low Energy
Transmission Grating Spectrometer (LETG+HRC-S) effective area
calibration is based on observed spectra of HZ 43 and Sirius B at
wavelengths
Å (Pease et al., 2003). It is
therefore of current topical interest to re-examine the influence of
Compton scattering for these stars and determine whether any
significant differences might be discernible between Thomson and
Compton scattering in the LETGS bandpass.
In this paper, we perform two independent and rigorous tests of the influence of Compton Scattering on the emergent spectra of hot DA white dwarfs. Our methods of calculation are outlined in §2, while results and conclusions are briefly discussed in §§3 and 5.