The boundary layer of VW Hydri in quiescence

In this short paper, we suggest that the missing boundary layer luminosity of dwarf novae in quiescence is released mainly in the ultraviolet (UV) as the second component commonly identified in the far-UV as the ‘accretion belt’. We present the well-studied SU UMa-type system VW Hyi in detail as a p...

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Bibliographic Details
Published inMonthly notices of the Royal Astronomical Society Vol. 361; no. 3; pp. 809 - 812
Main Authors Godon, P., Sion, E. M.
Format Journal Article
LanguageEnglish
Published Oxford, UK Blackwell Science Ltd 11.08.2005
Blackwell Science
Oxford University Press
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Summary:In this short paper, we suggest that the missing boundary layer luminosity of dwarf novae in quiescence is released mainly in the ultraviolet (UV) as the second component commonly identified in the far-UV as the ‘accretion belt’. We present the well-studied SU UMa-type system VW Hyi in detail as a prototype for such a scenario. We consider detailed multiwavelength observations and in particular the recent Far Ultraviolet Spectroscopic Explorer (FUSE) observations of VW Hyi in quiescence, which confirm the presence of a second component (the ‘accretion belt’) in the far-UV spectrum. The temperature (≈ 50 000 K) and rotational velocity (≈ 3000 km s −1) of this second component are entirely consistent with the optically thick region (τ ≈ 1) located just at the outer edge of optically thin boundary layer in the simulations of Popham. This second component contributes about 20 per cent of the far-UV flux. Using geometrical assumptions and taking into account the X-ray luminosity, we find that the total boundary layer luminosity sums up to LBL= (0.53 ± 0.25) Ldisc, while the theory (Kluzniak) predicts, for the rotation rate of VW Hyi's white dwarf, LBL≈ (0.76 ± 0.03)Ldisc. About one-fifth of the boundary layer energy is emitted in the X-ray and the remaining is emitted in the UV. This scenario is consistent with the recent simultaneous X-ray and UV observations of VW Hyi by Pandel, Córdova & Howell, from which we deduce here that the viscosity in the boundary layer region must be of the order of ν ≈ 1013–1014 cm2 s −1, depending on the white dwarf mass and the size of the boundary layer.
Bibliography:Visiting at the Space Telescope Science Institute, Baltimore, MD, USA.
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istex:1CB6916DC61FE1FE943276DE5A0311F7C902DFAE
ISSN:0035-8711
1365-2966
DOI:10.1111/j.1365-2966.2005.09209.x