THE EF-ERI GINGA DATA AND PHYSICAL MODELS FOR THE X-RAY-SPECTRA OF AM-HERCULIS SYSTEMS

Citation
C. Done et al., THE EF-ERI GINGA DATA AND PHYSICAL MODELS FOR THE X-RAY-SPECTRA OF AM-HERCULIS SYSTEMS, Monthly Notices of the Royal Astronomical Society, 276(2), 1995, pp. 483-494
Citations number
52
Categorie Soggetti
Astronomy & Astrophysics
ISSN journal
00358711
Volume
276
Issue
2
Year of publication
1995
Pages
483 - 494
Database
ISI
SICI code
0035-8711(1995)276:2<483:TEGDAP>2.0.ZU;2-#
Abstract
The Ginga hard X-ray spectrum of EF Eri is well fitted by a single-tem perature Raymond-Smith spectrum with kT similar to 14 keV with reduced iron abundance, together with its reflection from the white dwarf sur face. However, calculations of the shock structure indicate that the X -ray emission should consist of multitemperature components as the gas cools and settles on to the photosphere. We fit approximate models of such continua, together with their reflection, and find that, while t hese are not required by the data, they give as good a description of the spectrum as the single-temperature models. The maximum temperature material is derived to be at similar to 25 keV, close to that predict ed by strong shock models, but even with these more realistic models t he data still require that iron is a factor similar to 2 below solar a bundance. Radiation transfer in the hot shock is shown to be important , as the emission region is expected to be optically thick in the iron K alpha resonance lines, whilst remaining optically thin in the conti nuum. However, this is unlikely to be the cause of the low observed li ne equivalent width as there is no viable alternative decay path for t he Lyman alpha line in H- and He-like iron. The 6.4-keV iron line from fluorescence from the reflector is also smaller than expected by a fa ctor similar to 2, making a true underabundance of iron in this system the most likely explanation. We also calculate the absorption expecte d from the pre-shock material in the limit where the dense streams of material raining on to the surface to produce the soft X-rays are domi nant. The expected phase dependence of this absorption does not match well to that seen in EF Eri, but this may be due to non-circular or mu ltiple accretion sites or photoionization of the pre-shock column.