The origin of the rebrightening in soft X-ray transient outbursts
Mon.Not.Roy.Astron.Soc. 337 (2002) 1329 We present a model of an outburst of the soft X-ray transient A0620-003. A two-dimensional time-dependent smoothed particle hydrodynamics scheme is used to simulate the evolution of the accretion disc through a complete outburst. The scheme includes the full t...
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Main Authors | , , , |
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Format | Journal Article |
Language | English |
Published |
29.08.2002
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Subjects | |
Online Access | Get full text |
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Summary: | Mon.Not.Roy.Astron.Soc. 337 (2002) 1329 We present a model of an outburst of the soft X-ray transient A0620-003. A
two-dimensional time-dependent smoothed particle hydrodynamics scheme is used
to simulate the evolution of the accretion disc through a complete outburst.
The scheme includes the full tidal potential of the binary and a simple
treatment of the thermal-viscous disc instability.
In the case where the mass accretion rate onto the primary determines the
fraction of the disc that can be kept in a hot, high viscosity state by the
resulting X-ray emission, we find that the shape of the X-ray light curve is
ultimately determined by the relative sizes of the irradiated and unirradiated
parts of the disc and the growth time-scale of the tidal instability.
The model accounts for the rebrightening that has been observed in the light
curves of A0620-003 and several other transients. The primary maximum and
subsequent decline are due to the accretion of gas within the irradiated
portion of the disc, while the secondary maximum is caused by the accretion of
gas in the outer part of the disc that is initially shadowed from the central
X-rays, but subject to tidal forces. We propose that tidal effects at the disc
edge can be sufficient to drive accretion on a time-scale shorter than that
expected for a standard alpha-viscosity disc.
The final decay is subsequently controlled by the gradual retreat of the
irradiated portion of the disc. If the entire disc is kept in the
high-viscosity state by the irradiation, no rebrightening is possible. |
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DOI: | 10.48550/arxiv.astro-ph/0208527 |